Glass articles exhibiting improved fracture performance

Abstract
A glass-based article having an amorphous phase and a crystalline phase, and a first surface and a second surface opposing the first surface thereby defining a thickness (t) of the glass-based article. The glass-based article having a stress profile with a surface compressive stress (CS) and a maximum central tension (CT). The maximum CT is greater than or equal to 50 MPa and less than or equal to 200 MPa and is positioned within the glass-based article at a range from greater than or equal to 0.4·t and less than or equal to 0.6·t. The surface CS is greater than or equal to 200 MPa and less than or equal to 500 MPa, and a depth of compression (DOC) is from greater than or equal to 0.14·t and less than or equal to 0.25·t.
Description
BACKGROUND

The disclosure relates to glass articles exhibiting improved fracture performance, and more particularly to glass articles exhibiting improved fracture patterns and dicing behavior.


Consumer electronics devices, including handheld devices such as smart phones, tablets, electronic-book readers and laptops often incorporate chemically strengthened glass articles for use as cover glass. As cover glass is directly bonded to a substrate like a touch-panel, display or other structures, when strengthened glass articles fracture, such articles may eject small fragments or particles from the free surface due to the stored energy created by a combination of surface compressive stresses and tensile stresses beneath the surfaces of the glass. As used herein, the term fracture includes cracking and/or the formation of cracks. These small fragments are a potential concern to the device user, especially when fracture occurs in a delayed manner close to the users face (i.e. eyes and ears), and when the user continues to use and touch the fractured surface and is, thus, susceptible to minor cuts or abrasions, especially when crack distances are relatively long and fragments with sharp corners and edges are present.


Accordingly, there is a need for glass articles that exhibit a modified fragmentation behavior so that when such articles fracture, they exhibit an enhanced dicing behavior, such as, for example, a dicing effect generating short crack lengths and fewer ejected particles. Moreover, there is also a need for glass articles that, when fractured, eject fewer fragments and fragments with less kinetic energy and momentum.


SUMMARY

A first aspect of this disclosure pertains to a strengthened glass article including a first surface and a second surface opposing the first surface defining a thickness (t) of about 1.1 mm or less, and a compressive stress layer extending from the first surface to a depth of compression (DOC) of greater than about 0.11·t. In some embodiments, after the glass article fractures, the glass article includes a plurality of fragments, wherein at least 90% of the plurality of fragments have an aspect ratio of about 5 or less, the glass article fractures into the plurality of fragments in 1 second or less, as measured by a Frangibility Test.


In some embodiments, the strengthened glass article exhibiting a equibiaxial flexural strength of about 20 kgf or greater, after being abraded with 90-grit SiC particles at a pressure of 25 psi for 5 seconds. In some embodiments, the strengthened glass article may, after the glass article fractures, comprises fractures such that 50% or more of the fractures extend only partially through the thickness.


A third aspect of this disclosure pertains to a device including a strengthened glass substrate, as described herein, a containment layer; and a support, wherein the device comprises a tablet, a transparent display, a mobile phone, a video player, an information terminal device, an e-reader, a laptop computer, or a non-transparent display.


A fourth aspect of this disclosure pertains to a consumer electronics product including a housing having a front surface, electrical components provided at least partially internal to the housing, the electrical components including at least a controller, a memory, and a display; and a cover glass disposed at the front surface of the housing and over the display, the cover glass comprising a strengthened glass article as described herein.


Additional features and advantages will be set forth in the detailed description which follows, and in part will be readily apparent to those skilled in the art from that description or recognized by practicing the embodiments as described herein, including the detailed description which follows, the claims, as well as the appended drawings.


It is to be understood that both the foregoing general description and the following detailed description are merely exemplary, and are intended to provide an overview or framework to understanding the nature and character of the claims. The accompanying drawings are included to provide a further understanding, and are incorporated in and constitute a part of this specification. The drawings illustrate one or more embodiment(s), and together with the description serve to explain principles and operation of the various embodiments.





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1A is a side view of a glass article according to one or more embodiments;



FIG. 1B is a side view of the glass article of FIG. 1A after fracture;



FIG. 2 is a cross-sectional view across a thickness of a known thermally tempered glass-based article;



FIG. 3 is a cross-sectional view across a thickness of a known chemically strengthened glass-based article;



FIG. 4 is a cross-sectional view across a thickness of a strengthened glass-based article according to one or more embodiments;



FIG. 5 is a is a schematic cross-sectional view of a ring-on-ring apparatus;



FIG. 6 is a schematic cross-sectional view of an embodiment of the apparatus that is used to perform the inverted ball on sandpaper (IBoS) test described in the present disclosure;



FIG. 7 is a schematic cross-sectional representation of the dominant mechanism for failure due to damage introduction plus bending that typically occurs in glass-based articles that are used in mobile or hand held electronic devices;



FIG. 8 is a flow chart for a method of conducting the IBoS test in the apparatus described herein; and



FIG. 9A is a side view of the glass article of FIG. 1A including a containment layer;



FIG. 9B is a side view the glass article of FIG. 9A including a second containment layer;



FIG. 10 is a front plan view of an electronic device incorporating one or more embodiments of the glass articles described herein.



FIG. 11 is a graph showing AROR test results for Example 1;



FIG. 12 is a graph showing drop test results for Example 2;



FIG. 13 is a plot showing the concentration of K2O as a function of ion exchange depth for Example 4;



FIG. 14 is a plot showing the stress profile of Example 4G;



FIGS. 15A-15D are fracture images of Example 5;



FIGS. 16A-16D are images showing the readability of Example 6 after fracture at different viewing angles;



FIG. 17 is a plot of calculated stored tensile energy as a function of ion-exchange time, for Example 7; and



FIG. 18 is a plot of calculated central tension as a function of ion-exchange time, for Example 7; and



FIG. 19 is a plot showing the stress profile of Example 6, with compressive and tensile stress plotted as function of depth.





DETAILED DESCRIPTION

Reference will now be made in detail to various embodiments, examples of which are illustrated in the accompanying drawings. Referring to the drawings in general, it will be understood that the illustrations are for the purpose of describing particular embodiments and are not intended to limit the disclosure or appended claims thereto. The drawings are not necessarily to scale, and certain features and certain views of the drawings may be shown exaggerated in scale or in schematic in the interest of clarity and conciseness.


In the following description, like reference characters designate like or corresponding parts throughout the several views shown in the figures. It is also understood that, unless otherwise specified, terms such as “top,” “bottom,” “outward,” “inward,” and the like are words of convenience and are not to be construed as limiting terms. In addition, whenever a group is described as comprising at least one of a group of elements and combinations thereof, it is understood that the group may comprise, consist essentially of, or consist of any number of those elements recited, either individually or in combination with each other. Similarly, whenever a group is described as consisting of at least one of a group of elements or combinations thereof, it is understood that the group may consist of any number of those elements recited, either individually or in combination with each other. Unless otherwise specified, a range of values, when recited, includes both the upper and lower limits of the range as well as any ranges therebetween. As used herein, the indefinite articles “a,” “an,” and the corresponding definite article “the” mean “at least one” or “one or more,” unless otherwise specified. It also is understood that the various features disclosed in the specification and the drawings can be used in any and all combinations.


It is noted that the terms “substantially” and “about” may be utilized herein to represent the inherent degree of uncertainty that may be attributed to any quantitative comparison, value, measurement, or other representation. These terms are also utilized herein to represent the degree by which a quantitative representation may vary from a stated reference without resulting in a change in the basic function of the subject matter at issue.


As used herein, the term “glass article” is used in its broadest sense to include any object made wholly or partly of glass. Glass articles include laminates of glass and non-glass materials, laminates of amorphous and crystalline materials, and glass-ceramics (including an amorphous phase and a crystalline phase). Unless otherwise specified, all compositions are expressed in terms of mole percent (mol %).


As will be discussed herein, embodiments of the glass articles may include strengthened glass or glass ceramic materials that exhibit improved mechanical performance and reliability compared to known glass articles, especially known cover glass articles. Embodiments of the glass articles described herein may exhibit fragmentation behaviors that are not exhibited by known cover glass articles. In this disclosure glass-based substrates are generally unstrengthened and glass-based articles generally refer to glass-based substrates that have been strengthened (by, for example, ion exchange).


A first aspect of this disclosure pertains to a strengthened glass article that exhibits the ability to fracture into a dense fracture pattern with a dicing effect that is analogous to fully, thermally tempered glass used in shower panels or automobile window panels. In some embodiments, the fragments are intended to be less injurious to humans. Such articles exhibit this behavior despite being chemically strengthened and having thicknesses significantly less than achievable by current known thermal tempering processes. In some embodiments, the fragments are even smaller or finer than those observed with known thermally tempered glass. For example, embodiments of the glass articles exhibit a “dicing” effect in that, when the glass article is fractured, the “diced” fragments have a small aspect ratio and the fracture generated surface and the as-formed surface form larger angles (i.e., fewer blade-like or knife-like angles), such that the fragments resemble cubes more than splinters, as described in more detail below with respect to FIG. 1A. In some instances, the diced fragments are limited by a maximum or longest dimension of 2 millimeters (mm) or less in any direction of the major plane of the glass article. In some instances, when fractured or after the glass article fractures, the glass article includes a plurality of fragments having an average aspect ratio of about 10 or less, or about 5 or less (e.g., about 4.5 or less, about 4 or less, about 3.5 or less, about 3 or less, about 2.5 or less, about 2 or less). In some embodiments, the average aspect ratio of the plurality of fragments is in the range from about 1 to about 2. In some instances, about 90% or greater, or about 80% or greater of the plurality of fragments exhibits the average aspect ratios described herein. As used herein, the term “aspect ratio” refers to the ratio of the longest or maximum dimension of a fragment to the shortest or minimum dimension of the fragment. The term “dimension” can include a length, width, diagonal, or thickness. Glass articles that exhibit such fragments after being fractured may be characterized herein as exhibiting “dicing” behavior.


Referring to FIGS. 1A and 1B, in one or more embodiments, the glass articles 10 described herein may have a sheet configuration with opposing major surfaces 12, 14 and opposing minor surfaces 16, 18. At least one major surface 12 forms an “as-formed” surface of the glass article. When fractured, a new surface generated by the fracture of the glass article, is formed (i.e., a “fracture-generated” surface), indicated by reference number 19 in FIG. 1B. The angle α between a fracture generated surface and the as-formed surface (after the glass article is fractured) are in the range from about 85 degrees to about 95 degrees or about 88 degrees to about 92 degrees. In one or more embodiments, about 90% or more of the plurality of fragments in glass article exhibit the angles between the as-formed surface and all of the fracture generated surfaces, after the glass article is fractured.


In one or more embodiments, at least 50% (e.g., about 60% or more, about 70% or more, about 80% or more, or about 90% or more) of the plurality of fragments have a maximum dimension that is less than or equal to 5·t, less than or equal to 3·t, or less than or equal to 3·t. In some instances, at least 50% (e.g., about 60% or more, about 70% or more, about 80% or more, or about 90% or more) of plurality of fragments comprise a maximum dimension that is less than 2 times the minimum dimension. In some embodiments, the maximum dimension is about 1.8 times the minimum dimension or less, about 1.6 times the minimum dimension or less, about 1.5 times the minimum dimension or less, about 1.4 times the minimum dimension or less, about 1.2 times the minimum dimension or less, or about equal to the minimum dimension.


In one or more embodiments, at least 50% (e.g., about 60% or more, about 70% or more, about 80% or more, or about 90% or more) of the plurality of fragments comprises a volume of less than or equal to about 10 mm3. In some embodiments, the volume may be less than or equal to about 8 mm3, less than or equal to about 5 mm3, or less than or equal to about 4 mm3. In some embodiments, the volume may be in the range from about 0.1 mm3 to about 1.5 mm3.


As used herein, the phrase “strengthened articles” includes articles that are chemically strengthened, or chemically strengthened and thermally strengthened, but exclude articles that are only thermally strengthened. As shown in FIG. 4, the strengthened glass article exhibits a stress profile that can be characterized in terms of a surface compressive stress (CS), a central tension (CT) and a depth of compression (DOC).


The stress profile exhibited by the strengthened glass articles of one or more embodiments may be distinguished between the stress profiles exhibited by known thermally tempered glass articles and known chemically strengthened glass articles. Traditionally, thermally tempered glass has been used to prevent failures where such flaws may be introduced to the glass because thermally tempered glass often exhibits large CS layers (e.g., approximately 21% of the total thickness of the glass), which can prevent flaws from propagating and thus, failure. An example of a stress profile generated by thermal tempering is shown in FIG. 2. In FIG. 2, the thermally treated glass article 100 includes a first surface 101, a thickness t1, and a surface CS 110. The glass article 100 exhibits a CS that decreases from the first surface 101 to a DOC 130, as defined herein, at which depth the stress changes from compressive to tensile stress and reaches a CT 120.


Thermal tempering is currently limited to thick glass articles (i.e., glass articles having a thickness t1 of about 3 millimeters or greater) because, to achieve the thermal strengthening and the desired residual stresses, a sufficient thermal gradient must be formed between the core of such articles and the surface. Such thick articles are undesirable or not practical in many applications such as displays (e.g., consumer electronics, including mobile phones, tablets, computers, navigation systems, and the like), architecture (e.g., windows, shower panels, countertops etc.), transportation (e.g., automotive, trains, aircraft, sea craft, etc.), appliances, packaging, or any application that requires superior fracture resistance but thin and light-weight articles.


Known chemically strengthened glass articles do not exhibit the stress profile of thermally tempered glass articles, although chemical strengthening is not limited by the thickness of the glass article in the same manner as thermally tempering. An example of a stress profile generated by chemical strengthening (e.g., by ion exchange process), is shown in FIG. 3. In FIG. 3, the chemically strengthened glass article 200 includes a first surface 201, a thickness t2 and a surface CS 210. The glass article 200 exhibits a CS that decreases from the first surface 201 to a DOC 230, as defined herein, at which depth the stress changes from compressive to tensile stress and reaches a CT 220. As shown in FIG. 3, such profiles exhibit a flat CT region or CT region with a constant or near constant tensile stress and, often, a lower CT value, as compared to the CT value shown in FIG. 2.


The glass articles of one or more embodiments of this disclosure exhibit a thickness t of less than about 3 mm (e.g., about 2 mm or less, about 1.5 mm or less, or about 1.1 mm or less) and a compressive stress layer extending from the first surface to a DOC of about 0.1·t or greater. As used herein, DOC refers to the depth at which the stress within the glass article changes compressive to tensile stress. At the DOC, the stress crosses from a positive (compressive) stress to a negative (tensile) stress (e.g., 130 in FIG. 2) and thus exhibits a stress value of zero.


According to the convention normally used in the art, compression is expressed as a negative (<0) stress and tension is expressed as a positive (>0) stress. Throughout this description, however, CS is expressed as a positive or absolute value—i.e., as recited herein, CS=|CS|.


In particular, the glass articles described herein are thin and exhibit stress profiles that are typically only achievable through tempering thick glass articles (e.g., having a thickness of about 2 mm or 3 mm or greater). In some cases, the glass articles exhibit a greater surface CS than tempered glass articles. In one or more embodiments, the glass articles exhibit a larger depth of the compression layer (in which the CS decreases and increases more gradually than known chemically strengthened glass articles) such that the glass article exhibits substantially improved fracture resistance, even when the glass article or a device including the same is dropped on a hard, rough surface. The glass articles of one or more embodiments exhibit a greater CT value than some known chemically strengthened glass substrates.


CS is measured by surface stress meter (FSM) using commercially available instruments such as the FSM-6000, manufactured by Orihara Industrial Co., Ltd. (Japan). Surface stress measurements rely upon the accurate measurement of the stress optical coefficient (SOC), which is related to the birefringence of the glass. SOC in turn is measured according to a modified version of Procedure C described in ASTM standard C770-98 (2013), entitled “Standard Test Method for Measurement of Glass Stress-Optical Coefficient,” the contents of which are incorporated herein by reference in their entirety. The modification includes using a glass disc as the specimen with a thickness of 5 to 10 mm and a diameter of 12.7 mm, wherein the disc is isotropic and homogeneous and core drilled with both faces polished and parallel. The modification also includes calculating the maximum force, Fmax to be applied. The force should be sufficient to produce at least 20 MPa compression stress. Fmax is calculated as follows:

Fmax=7.854*D*h


Where:


Fmax=Force in Newtons


D=the diameter of the disc


h=the thickness of the light path


For each force applied, the stress is computed as follows:

σMPa=8F/(π*D*h)


Where:


F=Force in Newtons


D=the diameter of the disc


h=the thickness of the light path


CT values are measured using a scattered light polariscope (“SCALP”, supplied by Glasstress Ltd., located in Tallinn, Estonia, under model number SCALP-04) and techniques known in the art. SCALP can also be used to measure the DOC, as will be described in more detail below.


In some embodiments, the glass article may also exhibit a depth of penetration of potassium ions (“Potassium DOL”) that is distinct from the DOC. The degree of difference between DOC and Potassium DOL depends on the glass substrate composition and the ion exchange treatment that generates the stress in the resulting glass article. Where the stress in the glass article is generated by exchanging potassium ions into the glass article, FSM (as described above with respect to CS) is used to measure Potassium DOL. Where the stress is generated by exchanging sodium ions into the glass article, SCALP (as described above with respect to CT) is used to measure DOC and the resulting glass article will not have a Potassium DOL since there is no penetration of potassium ions. Where the stress in the glass article is generated by exchanging both potassium and sodium ions into the glass, the exchange depth of sodium indicates the DOC, and the exchange depth of potassium ions indicates a change in the magnitude of the compressive stress (but not the change in stress from compressive to tensile); in such embodiments, the DOC is measured by SCALP, and Potassium DOL is measured by FSM. Where both Potassium DOL and DOC are present in a glass article, the Potassium DOL is typically less than the DOC.


Refracted near-field (RNF) method or SCALP may be used to measure the stress profile in the glass articles described herein (regardless of whether the stress is generated by sodium ion exchange and/or potassium ion exchange). When the RNF method is utilized, the CT value provided by SCALP is utilized. In particular, the stress profile measured by RNF is force balanced and calibrated to the CT value provided by a SCALP measurement. The RNF method is described in U.S. Pat. No. 8,854,623, entitled “Systems and methods for measuring a profile characteristic of a glass sample”, which is incorporated herein by reference in its entirety. In particular, the RNF method includes placing the glass-based article adjacent to a reference block, generating a polarization-switched light beam that is switched between orthogonal polarizations at a rate of between 1 Hz and 50 Hz, measuring an amount of power in the polarization-switched light beam and generating a polarization-switched reference signal, wherein the measured amounts of power in each of the orthogonal polarizations are within 50% of each other. The method further includes transmitting the polarization-switched light beam through the glass sample and reference block for different depths into the glass sample, then relaying the transmitted polarization-switched light beam to a signal photodetector using a relay optical system, with the signal photodetector generating a polarization-switched detector signal. The method also includes dividing the detector signal by the reference signal to form a normalized detector signal and determining the profile characteristic of the glass sample from the normalized detector signal.


In one or more embodiments in which the stress in a glass article is generated by only potassium ion exchange and Potassium DOL is equivalent to DOC, the stress profile may also be obtained by the methods disclosed in U.S. patent application Ser. No. 13/463,322, entitled “Systems And Methods for Measuring the Stress Profile of Ion-Exchanged Glass (hereinafter referred to as “Roussev I”),” filed by Rostislav V. Roussev et al. on May 3, 2012, and claiming priority to U.S. Provisional Patent Application No. 61/489,800, having the same title and filed on May 25, 2011. Roussev I discloses methods for extracting detailed and precise stress profiles (stress as a function of depth) of chemically strengthened glass using FSM. Specifically, the spectra of bound optical modes for TM and TE polarization are collected via prism coupling techniques, and used in their entirety to obtain detailed and precise TM and TE refractive index profiles nTM(z) and nTE(z). The contents of the above applications are incorporated herein by reference in their entirety. The detailed index profiles are obtained from the mode spectra by using the inverse Wentzel-Kramers-Brillouin (IWKB) method, and fitting the measured mode spectra to numerically calculated spectra of pre-defined functional forms that describe the shapes of the index profiles and obtaining the parameters of the functional forms from the best fit. The detailed stress profile S(z) is calculated from the difference of the recovered TM and TE index profiles by using a known value of the stress-optic coefficient (SOC):

S(z)=[nTM(z)−nTE(z)]/SOC  (2).


Due to the small value of the SOC, the birefringence nTM(z)−nTE(z) at any depth z is a small fraction (typically on the order of 1%) of either of the indices nTM(z) and nTE(z). Obtaining stress profiles that are not significantly distorted due to noise in the measured mode spectra requires determination of the mode effective indices with precision on the order of 0.00001 RIU. The methods disclosed in Roussev I further include techniques applied to the raw data to ensure such high precision for the measured mode indices, despite noise and/or poor contrast in the collected TE and TM mode spectra or images of the mode spectra. Such techniques include noise-averaging, filtering, and curve fitting to find the positions of the extremes corresponding to the modes with sub-pixel resolution.


As stated above, the glass articles described herein may be chemically strengthened by ion exchange and exhibit stress profiles that are distinguished from those exhibited by known strengthened glass. In this process, ions at or near the surface of the glass article are replaced by—or exchanged with—larger ions having the same valence or oxidation state. In those embodiments in which the glass article comprises an alkali aluminosilicate glass, ions in the surface layer of the glass and the larger ions are monovalent alkali metal cations, such as Li+ (when present in the glass article), Na+, K+, Rb+, and Cs+. Alternatively, monovalent cations in the surface layer may be replaced with monovalent cations other than alkali metal cations, such as Ag+ or the like.


Ion exchange processes are typically carried out by immersing a glass article in a molten salt bath (or two or more molten salt baths) containing the larger ions to be exchanged with the smaller ions in the glass article. It should be noted that aqueous salt baths may also be utilized. In addition, the composition of the bath(s) may include more than one type of larger ion (e.g., Na+ and K+) or a single larger ion. It will be appreciated by those skilled in the art that parameters for the ion exchange process, including, but not limited to, bath composition and temperature, immersion time, the number of immersions of the glass article in a salt bath (or baths), use of multiple salt baths, additional steps such as annealing, washing, and the like, are generally determined by the composition of the glass article (including the structure of the article and any crystalline phases present) and the desired DOC and CS of the glass article that result from the strengthening operation. By way of example, ion exchange of a glass articles may be achieved by immersion of the glass articles in at least one molten bath containing a salt such as, but not limited to, nitrates, sulfates, and chlorides of the larger alkali metal ion. Typical nitrates include KNO3, NaNO3, LiNO3, NaSO4 and combinations thereof. The temperature of the molten salt bath typically is in a range from about 380° C. up to about 450° C., while immersion times range from about 15 minutes up to about 100 hours depending on glass thickness, bath temperature and glass diffusivity. However, temperatures and immersion times different from those described above may also be used.


In one or more embodiments, the glass articles may be immersed in a molten salt bath of 100% NaNO3 having a temperature from about 370° C. to about 480° C. In some embodiments, the glass substrate may be immersed in a molten mixed salt bath including from about 5% to about 90% KNO3 and from about 10% to about 95% NaNO3. In some embodiments, the glass substrate may be immersed in a molten mixed salt bath including Na2SO4 and NaNO3 and have a wider temperature range (e.g., up to about 500° C.). In one or more embodiments, the glass article may be immersed in a second bath, after immersion in a first bath. Immersion in a second bath may include immersion in a molten salt bath including 100% KNO3 for 15 minutes to 8 hours.


The ion exchange conditions may be modified based on the glass composition and thickness of the glass substrate. For example, a glass substrate having a nominal composition as shown in Example 1 below having a thickness of 0.4 mm may be immersed in a molten salt bath of 80-100% KNO3 (with the balance NaNO3) having a temperature of about 460° C. for a duration from about 10 hours to about 20 hours. The same substrate having a thickness of about 0.55 mm may be immersed in a molten salt bath of 70-100% KNO3 (with the balance NaNO3) having a temperature of about 460° C. for a duration of from about 20 hours to about 40 hours. The same substrate having a thickness of about 0.8 mm may be immersed in a molten salt bath of 60-100% KNO3 (with the balance NaNO3) having a temperature of about 460° C. for a duration of from about 40 hours to about 80 hours.


In one or more embodiments, the glass-based substrate may be immersed in a molten, mixed salt bath including NaNO3 and KNO3 (e.g., 49%/51%, 50%/50%, 51%/49%) having a temperature less than about 420° C. (e.g., about 400° C. or about 380° C.). for less than about 5 hours, or even about 4 hours or less.


Ion exchange conditions can be tailored to provide a “spike” or to increase the slope of the stress profile at or near the surface of the resulting glass-based article. This spike can be achieved by single bath or multiple baths, with the bath(s) having a single composition or mixed composition, due to the unique properties of the glass compositions used in the glass-based articles described herein.


As illustrated in FIG. 4, the glass article 300 of one or more embodiments includes a first surface 302 and a second surface 304 opposing the first surface, defining a thickness t. In one or more embodiments, the thickness t may be less than about 3 mm, about 2 mm or less, about 1.5 mm or less, about 1.1 mm or less, or 1 mm or less (e.g., in the range from about 0.01 mm to about 1.5 mm, from about 0.1 mm to about 1.5 mm, from about 0.2 mm to about 1.5 mm, from about 0.3 mm to about 1.5 mm, from about 0.4 mm to about 1.5 mm, in the range from about 0.01 mm to about 1.1 mm, from about 0.1 mm to about 1.1 mm, from about 0.2 mm to about 1.1 mm, from about 0.3 mm to about 1.1 mm, from about 0.4 mm to about 1.1 mm, from about 0.01 mm to about 1.4 mm, from about 0.01 mm to about 1.2 mm, from about 0.01 mm to about 1.1.1 mm, from about 0.01 mm to about 1 mm, from about 0.01 mm to about 0.9 mm, from about 0.01 mm to about 0.8 mm, from about 0.01 mm to about 0.7 mm, from about 0.01 mm to about 0.6 mm, from about 0.01 mm to about 0.5 mm, from about 0.1 mm to about 0.5 mm, or from about 0.3 mm to about 0.5 mm.)



FIG. 4, is a cross-sectional illustration of the stress profile of a chemically strengthened glass article 300 along its thickness 330 (depicted along the x-axis). The magnitude of the stress is illustrated on the y-axis with the line 301 representing a zero stress.


The stress profile 312 includes a CS layer 315 (with a surface CS value 310) that extends from one or both the first major surface 302 and the second major surface 304 to a DOC 330, and a CT layer 325 (with a CT 320) that extends from DOC 330 to the central portion of the article.


As used herein, DOC refers to the depth at which the stress within the glass article changes compressive to tensile. At the DOC, the stress crosses from a positive (compressive) stress to a negative (tensile) stress (e.g., 330 in FIG. 5) and thus exhibits a stress value of zero.


The CS layer has an associated depth or length 317 extending from a major surface 302, 304 to the DOC 330. The CT layer 325 also has an associated depth or length 327 (CT region or layer).


The surface CS 310 may be about 150 MPa or greater or about 200 MPa or greater (e.g., about 250 MPa or greater, about 300 MPa or greater, about 400 MPa or greater, about 450 MPa or greater, about 500 MPa or greater, or about 550 MPa or greater). The surface CS 310 may be up to about 900 MPa, up to about 1000 MPa, up to about 1100 MPa, or up to about 1200 MPa. In one or more embodiments, the surface CS 310 may be in a range from about 150 MPa to about 1200 MPa, from about 200 MPa to about 1200 MPa, from about 250 MPa to about 1200 MPa, from about 300 MPa to about 1200 MPa, from about 350 MPa to about 1200 MPa, from about 400 MPa to about 1200 MPa, from about 450 MPa to about 1200 MPa, from about 500 MPa to about 1200 MPa, from about 200 MPa to about 1100 MPa, from about 200 MPa to about 1000 MPa, from about 200 MPa to about 900 MPa, from about 200 MPa to about 800 MPa, from about 200 MPa to about 700 MPa, from about 200 MPa to about 600 MPa, from about 200 MPa to about 500 MPa, from about 300 MPa to about 900 MPa, or from about 400 MPa to 600 MPa.


The CT 320 may be about 25 MPa or greater, about 50 MPa or greater, about 75 MPa or greater, or about 85 MPa or greater, or about 100 MPa or greater (e.g., about 150 MPa or greater, about 200 MPa or greater, 250 MPa or greater, or about 300 MPa or greater). In some embodiments, the CT 320 may be in the range from about 50 MPa to about 400 MPa, (e.g., from about 75 MPa to about 400 MPa, from about 100 MPa to about 400 MPa, from about 150 MPa to about 400 MPa, from about 50 MPa to about 350 MPa, from about 50 MPa to about 300 MPa, from about 50 MPa to about 250 MPa, from about 50 MPa to about 200 MPa, from about 100 MPa to about 400 MPa, from about 100 MPa to about 300 MPa, from about 150 MPa to about 250 MPa). As used herein, CT is the greatest magnitude of the central tension in the glass article.


It should be noted that any one or more of surface CS 310 and CT 320 may be dependent on the thickness of the glass article. For example, glass articles having at thickness of about 0.8 mm may have a CT of about 100 MPa or greater. In one or more embodiment, glass articles having at thickness of about 0.4 mm may have a CT of about 130 MPa or greater. In some embodiments, the CT may be expressed in terms of thickness t of the glass article. For example, in one or more embodiment CT may be about (100 MPa)/√(t/1 mm), or greater, where t is thickness is mm. In some embodiments, CT may be about (105 MPa)/√(t/1 mm) or greater, (110 MPa)/√(t/1 mm) or greater, (115 MPa)/√(t/1 mm) or greater, (120 MPa)/√(t/1 mm) or greater, or (125 MPa)/√(t/1 mm) or greater.


The CT 320 may be positioned at a range from about 0.3·t to about 0.7·t, from about 0.4·t to about 0.6·t or from about 0.45·t to about 0.55·t. It should be noted that any one or more of surface CS 310 and CT 320 may be dependent on the thickness of the glass-based article. For example, glass-based articles having at thickness of about 0.8 mm may have a CT of about 75 MPa or less. When the thickness of the glass-based article decreases, the CT may increase. In other words, the CT increases with decreasing thickness (or as the glass-based article becomes thinner).


The Young's modulus of the glass article can influence the CT of the strengthened glass articles described herein. Specifically, as the Young's modulus of a glass article decreases, the glass article may be strengthened to have a lower CT, for a given thickness, and still exhibit the fracture behavior described herein. For example, when comparing a 1 mm glass article having a relatively lower Young's modulus than another 1 mm-thick glass article having a higher Young's modulus, the lower Young's modulus glass article may be strengthened to a lesser degree (i.e., to a relatively lower CT value) and still exhibit the same fracture behavior as the higher Young's modulus glass (which would have a higher CT compared to the CT glass article).


In some embodiments, the ratio of the CT 320 to the surface CS in the range from about 0.05 to about 1 (e.g., in the range from about 0.05 to about 0.5, from about 0.05 to about 0.3, from about 0.05 to about 0.2, from about 0.05 to about 0.1, from about 0.5 to about 0.8, from about 0.0.5 to about 1, from about 0.2 to about 0.5, from about 0.3 to about 0.5). In known chemically strengthened glass articles, the ratio of the CT 320 to the surface CS is 0.1 or less. In some embodiments, surface CS may be 1.5 times (or 2 times or 2.5 times) the CT or greater. In some embodiments, the surface CS may be up to about 20 times the CT.


In one or more embodiments, the stress profile 312 comprises a maximum CS, which is typically the surface CS 310 and can be found at one or both of the first surface 302 and the second surface 304. In one or more embodiments, the CS layer or region 315 extends along a portion of the thickness to the DOC 317 and a CT 320. In one or more embodiments, the DOC 317 may be about 0.1·tor greater. For example, the DOC 317 may be about 0.12·t or greater, about 0.14·t or greater, about 0.15·t or greater, about 0.16·t or greater, 0.17·t or greater, 0.18·t or greater, 0.19·t or greater, 0.20·t or greater, about 0.21·t or greater, or up to about 0.25·t. In some embodiments, the DOC 317 is less than the maximum chemical depth 342. The maximum chemical depth 342 may be about 0.4·t or greater, 0.5·t or greater, about 55·t or greater, or about 0.6·t or greater.


In one or more embodiments, the glass-based article comprises a Potassium DOL in the range from about 6 micrometers to about 20 micrometers. In some embodiments, the Potassium DOL may be expressed as a function of the thickness t of the glass-based article. In one or more embodiments, Potassium DOL may be in the range from about 0.005t to about 0.05t. In some embodiments, the Potassium DOL may be in the range from about 0.005t to about 0.05t, from about 0.005t to about 0.045t, from about 0.005t to about 0.04t, from about 0.005t to about 0.035t, from about 0.005t to about 0.03t, from about 0.005t to about 0.025t, from about 0.005t to about 0.02t, from about 0.005t to about 0.015t, from about 0.005t to about 0.01t, from about 0.006t to about 0.05t, from about 0.008t to about 0.05t, from about 0.01t to about 0.05t, from about 0.015t to about 0.05t, from about 0.02t to about 0.05t, from about 0.025t to about 0.05t, from about 0.03t to about 0.05t, or from about 0.01t to about 0.02t.


In one or more embodiments, the compressive stress value at the Potassium DOL depth may be in the range from about 50 MPa to about 300 MPa. In some embodiments, the compressive stress value at the Potassium DOL depth may be in the range from about 50 MPa to about 280 MPa, from about 50 MPa to about 260 MPa, from about 50 MPa to about 250 MPa, from about 50 MPa to about 240 MPa, from about 50 MPa to about 220 MPa, from about 50 MPa to about 200 MPa, from about 60 MPa to about 300 MPa, from about 70 MPa to about 300 MPa, from about 75 MPa to about 300 MPa, from about 80 MPa to about 300 MPa, from about 90 MPa to about 300 MPa, from about 100 MPa to about 300 MPa, from about 1100 MPa to about 300 MPa, from about 120 MPa to about 300 MPa, from about 130 MPa to about 300 MPa, or from about 150 MPa to about 300 MPa.


In one or more embodiments, the glass article exhibits the combination of a surface CS in a range from about 450 MPa to about 600 MPa, a CT in a range from about 200 to 300 MPa, and a thickness in a range from about 0.4 mm to 0.5 mm. In some embodiments, the DOC of the glass article is in a range from about 0.18t to about 0.21t.


In one or more embodiments, the glass article exhibits the combination of a surface CS in a range from about 350 MPa to about 450 MPa, a CT in a range from about 150 to 250 MPa, and a thickness in a range from about 0.4 mm to 0.5 mm. In some embodiments, the DOC of the glass article is in a range from about 0.18t to about 0.21t.


In one or more embodiments, the glass articles exhibits a maximum chemical depth of about 0.4·t or greater, 0.5·t or greater, about 55·t or greater, or about 0.6·t or greater. As used herein, the term “chemical depth” means the depth at which an ion of the metal oxide or alkali metal oxide (e.g., the metal ion or alkali metal ion) diffuses into the glass article and the depth at which the concentration of that ion reaches a minimum value, as determined by Electron Probe Micro-Analysis (EPMA). The ion is the ion diffused into the chemically strengthened glass article as a result of ion exchange. Maximum chemical depth refers to the maximum diffusion depth of any ion exchanged into the chemically strengthened glass article by ion exchange process. For example, where a molten salt bath having more than one diffusing ionic species (i.e., a molten salt bath of both NaNO3 and KNO3), the different ionic species may diffuse to different depths into the chemically strengthened glass articles. The maximum chemical depth is the greatest diffusion depth of all the ionic species ion exchanged into the chemically strengthened glass article.


In one or more embodiments, the stress profile 312 may be described as parabolic-like in shape. In some embodiments, the stress profile along the region or depth of the glass-based article exhibiting tensile stress exhibits a parabolic-like shape. In one or more specific embodiments, the stress profile 312 is free of a flat stress (i.e., compressive or tensile) portion or a portion that exhibits a substantially constant stress (i.e., compressive or tensile). In some embodiments, the CT region exhibits a stress profile that is substantially free of a flat stress or free of a substantially constant stress. In one or more embodiments, all points of the stress profile 312 between a thickness range from about 0·t up to about 0.2·t and greater than 0.8·t (or from about 0·t to about 0.3·t and greater than 0.7·t) comprise a tangent that is less than about −0.1 MPa/micrometers or greater than about 0.1 MPa/micrometers. In some embodiments, the tangent may be less than about −0.2 MPa/micrometers or greater than about 0.2 MPa/micrometers. In some more specific embodiments, the tangent may be less than about −0.3 MPa/micrometers or greater than about 0.3 MPa/micrometers. In even more specific embodiments, the tangent may be less than about −0.5 MPa/micrometers or greater than about 0.5 MPa/micrometers. In other words, the stress profile of one or more embodiments along these thickness ranges (i.e., 0·t up to about 2·t and greater than 0.8t, or from about 0·t to about 0.3·t and 0.7·t or greater) exclude points having a tangent, as described herein. Without being bound by theory, known error function or quasi-linear stress profiles have points along these thickness ranges (i.e., from about 0·t up to about 2·t and greater than 0.8·t, or from about 0·t to about 0.3·t and 0.7·t or greater) that have a tangent that is in the range from about −0.1 MPa/micrometers to about 0.1 MPa/micrometers, from about −0.2 MPa/micrometers to about 0.2 MPa/micrometers, from about −0.3 MPa/micrometers to about 0.3 MPa/micrometers, or from about −0.5 MPa/micrometers to about 0.5 MPa/micrometers (indicating a flat or zero slope stress profile along such thickness ranges, as shown in FIG. 3, 220). The glass-based articles of one or more embodiments of this disclosure do not exhibit such a stress profile having a flat or zero slope stress profile along these thickness ranges, as shown in FIG. 4.


In one or more embodiments, the glass-based article exhibits a stress profile in a thickness range from about 0.1·t to 0.3·t and from about 0.7·t to 0.9·t that comprises a maximum tangent and a minimum tangent. In some instances, the difference between the maximum tangent and the minimum tangent is about 3.5 MPa/micrometers or less, about 3 MPa/micrometers or less, about 2.5 MPa/micrometers or less, or about 2 MPa/micrometers or less.


In one or more embodiments, the glass-based article includes a stress profile 312 that is substantially free of any linear segments that extend in a depth direction or along at least a portion of the thickness t of the glass-based article. In other words, the stress profile 312 is substantially continuously increasing or decreasing along the thickness t. In some embodiments, the stress profile is substantially free of any linear segments in a depth direction having a length of about 10 micrometers or more, about 50 micrometers or more, or about 100 micrometers or more, or about 200 micrometers or more. As used herein, the term “linear” refers to a slope having a magnitude of less than about 5 MPa/micrometer, or less than about 2 MPa/micrometer along the linear segment. In some embodiments, one or more portions of the stress profile that are substantially free of any linear segments in a depth direction are present at depths within the glass-based article of about 5 micrometers or greater (e.g., 10 micrometers or greater, or 15 micrometers or greater) from either one or both the first surface or the second surface. For example, along a depth of about 0 micrometers to less than about 5 micrometers from the first surface, the stress profile may include linear segments, but from a depth of about 5 micrometers or greater from the first surface, the stress profile may be substantially free of linear segments.


In some embodiments, the stress profile may include linear segments at depths from about 0·t up to about 0.1t and may be substantially free of linear segments at depths of about 0.1t to about 0.4t. In some embodiments, the stress profile from a thickness in the range from about 0·t to about 0.1t may have a slope in the range from about 20 MPa/microns to about 200 MPa/microns. As will be described herein, such embodiments may be formed using a single ion-exchange process by which the bath includes two or more alkali salts or is a mixed alkali salt bath or multiple (e.g., 2 or more) ion exchange processes.


In one or more embodiments, the glass-based article may be described in terms of the shape of the stress profile along the CT region (327 in FIG. 4). For example, in some embodiments, the stress profile along the CT region (where stress is in tension) may be approximated by equation. In some embodiments, the stress profile along the CT region may be approximated by Equation (1):

Stress(x)=MaxT−(((CTn·(n+1))/0.5n)·|(x/t)−0.5|n)  (1)

In Equation (1), the stress (x) is the stress value at position x. Here the stress is positive (tension). In Equation (1), MaxT is the maximum tension value and CTn is the tension value at n and is less than or equal to MaxT. Both MaxT and CTn as positive values in MPa. The value x is position along the thickness (t) in micrometers, with a range from 0 to t; x=0 is one surface (302, in FIG. 4), x=0.5t is the center of the glass-based article, stress(x)=MaxCT, and x=t is the opposite surface (304, in FIG. 4). MaxT used in Equation (1) is equivalent to the CT, which may be less than about 71.5/√(t). In some embodiments, the MaxT used in Equation (1) may be in the range from about 50 MPa to about 80 MPa (e.g., from about 60 MPa to about 80 MPa, from about 70 MPa to about 80 MPa, from about 50 MPa to about 75 MPa, from about 50 MPa to about 70 MPa, or from about 50 MPa to about 65 MPa), and n is a fitting parameter from 1.5 to 5 (e.g., 2 to 4, 2 to 3 or 1.8 to 2.2) or from about 1.5 to about 2. In one or more embodiments, n=2 can provide a parabolic stress profile, exponents that deviate from n=2 provide stress profiles with near parabolic stress profiles. FIG. 5 is a graph illustrating various stress profiles according to one or more embodiments of this disclosure, based on changes in the fitting parameter n.


In one or more embodiments, CTn may be less than MaxT where there is a compressive stress spike on one or both major surfaces of the glass-based article. In one or more embodiments, CTn is equal to MaxT when there is no compressive stress spike on one or both major surfaces of the glass-based article.


In some embodiments, the stress profile may be modified by heat treatment. In such embodiments, the heat treatment may occur before any ion-exchange processes, between ion-exchange processes, or after all ion-exchange processes. In some embodiments, the heat treatment may result reduce the slope of the stress profile at or near the surface. In some embodiments, where a steeper or greater slope is desired at the surface, an ion-exchange process after the heat treatment may be utilized to provide a “spike” or to increase the slope of the stress profile at or near the surface.


In one or more embodiments, the stress profile 312 (and/or estimated stress profile 340) is generated due to a non-zero concentration of a metal oxide(s) that varies along a portion of the thickness. The variation in concentration may be referred to herein as a gradient. In some embodiments, the concentration of a metal oxide is non-zero and varies, both along a thickness range from about 0·t to about 0.3·t. In some embodiments, the concentration of the metal oxide is non-zero and varies along a thickness range from about 0·t to about 0.35·t, from about 0·t to about 0.4·t, from about 0·t to about 0.45·t or from about 0·t to about 0.48·t. The metal oxide may be described as generating a stress in the glass-based article. The variation in concentration may be continuous along the above-referenced thickness ranges. Variation in concentration may include a change in metal oxide concentration of about 0.2 mol % along a thickness segment of about 100 micrometers. This change may be measured by known methods in the art including microprobe, as shown in Example 1. The metal oxide that is non-zero in concentration and varies along a portion of the thickness may be described as generating a stress in the glass-based article.


The variation in concentration may be continuous along the above-referenced thickness ranges. In some embodiments, the variation in concentration may be continuous along thickness segments in the range from about 10 micrometers to about 30 micrometers. In some embodiments, the concentration of the metal oxide decreases from the first surface to a point between the first surface and the second surface and increases from the point to the second surface.


The concentration of metal oxide may include more than one metal oxide (e.g., a combination of Na2O and K2O). In some embodiments, where two metal oxides are utilized and where the radius of the ions differ from one or another, the concentration of ions having a larger radius is greater than the concentration of ions having a smaller radius at shallow depths, while the at deeper depths, the concentration of ions having a smaller radius is greater than the concentration of ions having larger radius. For example, where a single Na− and K− containing bath is used in the ion exchange process, the concentration of K+ ions in the glass-based article is greater than the concentration of Na+ ions at shallower depths, while the concentration of Na+ is greater than the concentration of K+ ions at deeper depths. This is due, in part, due to the size of the ions. In such glass-based articles, the area at or near the surface comprises a greater CS due to the greater amount of larger ions (i.e., K+ ions) at or near the surface. This greater CS may be exhibited by a stress profile having a steeper slope at or near the surface (i.e., a spike in the stress profile at the surface).


The concentration gradient or variation of one or more metal oxides is created by chemically strengthening a glass-based substrate, as previously described herein, in which a plurality of first metal ions in the glass-based substrate is exchanged with a plurality of second metal ions. The first ions may be ions of lithium, sodium, potassium, and rubidium. The second metal ions may be ions of one of sodium, potassium, rubidium, and cesium, with the proviso that the second alkali metal ion has an ionic radius greater than the ionic radius than the first alkali metal ion. The second metal ion is present in the glass-based substrate as an oxide thereof (e.g., Na2O, K2O, Rb2O, Cs2O or a combination thereof).


In one or more embodiments, the metal oxide concentration gradient extends through a substantial portion of the thickness t or the entire thickness t of the glass-based article, including the CT layer 327. In one or more embodiments, the concentration of the metal oxide is about 0.5 mol % or greater in the CT layer 327. In some embodiments, the concentration of the metal oxide may be about 0.5 mol % or greater (e.g., about 1 mol % or greater) along the entire thickness of the glass-based article, and is greatest at the first surface 302 and/or the second surface 304 and decreases substantially constantly to a point between the first surface 302 and the second surface 304. At that point, the concentration of the metal oxide is the least along the entire thickness t; however the concentration is also non-zero at that point. In other words, the non-zero concentration of that particular metal oxide extends along a substantial portion of the thickness t (as described herein) or the entire thickness t. In some embodiments, the lowest concentration in the particular metal oxide is in the CT layer 327. The total concentration of the particular metal oxide in the glass-based article may be in the range from about 1 mol % to about 20 mol %.


In one or more embodiments, the glass-based article includes a first metal oxide concentration and a second metal oxide concentration, such that the first metal oxide concentration is in the range from about 0 mol % to about 15 mol % along a first thickness range from about 0·t to about 0.5t, and the second metal oxide concentration is in the range from about 0 mol % to about 10 mol % from a second thickness range from about 0 micrometers to about 25 micrometers (or from about 0 micrometers to about 12 micrometers); however, the concentration of one or both the first metal oxide and the second metal oxide is non-zero along a substantial portion or the entire thickness of the glass-based article. The glass-based article may include an optional third metal oxide concentration. The first metal oxide may include Na2O while the second metal oxide may include K2O.


The concentration of the metal oxide may be determined from a baseline amount of the metal oxide in the glass-based article prior to being modified to include the concentration gradient of such metal oxide.


In some embodiments, the stress profile may be modified by heat treatment. In such embodiments, the heat treatment may occur before any ion-exchange processes, between ion-exchange processes, or after all ion-exchange processes. In some embodiments, the heat treatment may result reduce the slope of the stress profile at or near the surface. In some embodiments, where a steeper or greater slope is desired at the surface, an ion-exchange process after the heat treatment may be utilized to provide a “spike” or to increase the slope of the stress profile at or near the surface.


In one or more embodiments, the stress profile 312 is generated due to a non-zero concentration of a metal oxide(s) that varies along a portion of the thickness. The variation in concentration may be referred to herein as a gradient. In some embodiments, the concentration of a metal oxide is non-zero and varies, both along a thickness range from about 0·t to about 0.3·t. In some embodiments, the concentration of the metal oxide is non-zero and varies along a thickness range from about 0·t to about 0.35·t, from about 0·t to about 0.4·t, from about 0·t to about 0.45·t or from about 0·t to about 0.48·t. The metal oxide may be described as generating a stress in the glass-based article. The variation in concentration may be continuous along the above-referenced thickness ranges. Variation in concentration may include a change in metal oxide concentration of about 0.2 mol % along a thickness segment of about 100 micrometers. This change may be measured by known methods in the art including microprobe, as shown in Example 1. The metal oxide that is non-zero in concentration and varies along a portion of the thickness may be described as generating a stress in the glass-based article.


The variation in concentration may be continuous along the above-referenced thickness ranges. In some embodiments, the variation in concentration may be continuous along thickness segments in the range from about 10 micrometers to about 30 micrometers. In some embodiments, the concentration of the metal oxide decreases from the first surface to a point between the first surface and the second surface and increases from the point to the second surface.


The concentration of metal oxide may include more than one metal oxide (e.g., a combination of Na2O and K2O). In some embodiments, where two metal oxides are utilized and where the radius of the ions differ from one or another, the concentration of ions having a larger radius is greater than the concentration of ions having a smaller radius at shallow depths, while the at deeper depths, the concentration of ions having a smaller radius is greater than the concentration of ions having larger radius. For example, where a single Na− and K− containing bath is used in the ion exchange process, the concentration of K+ ions in the glass-based article is greater than the concentration of Na+ ions at shallower depths, while the concentration of Na+ is greater than the concentration of K+ ions at deeper depths. This is due, in part, due to the size of the ions. In such glass-based articles, the area at or near the surface comprises a greater CS due to the greater amount of larger ions (i.e., K+ ions) at or near the surface. This greater CS may be exhibited by a stress profile having a steeper slope at or near the surface (i.e., a spike in the stress profile at the surface).


The concentration gradient or variation of one or more metal oxides is created by chemically strengthening a glass-based substrate, as previously described herein, in which a plurality of first metal ions in the glass-based substrate is exchanged with a plurality of second metal ions. The first ions may be ions of lithium, sodium, potassium, and rubidium. The second metal ions may be ions of one of sodium, potassium, rubidium, and cesium, with the proviso that the second alkali metal ion has an ionic radius greater than the ionic radius than the first alkali metal ion. The second metal ion is present in the glass-based substrate as an oxide thereof (e.g., Na2O, K2O, Rb2O, Cs2O or a combination thereof).


In one or more embodiments, the metal oxide concentration gradient extends through a substantial portion of the thickness t or the entire thickness t of the glass-based article, including the CT layer 327. In one or more embodiments, the concentration of the metal oxide is about 0.5 mol % or greater in the CT layer 327. In some embodiments, the concentration of the metal oxide may be about 0.5 mol % or greater (e.g., about 1 mol % or greater) along the entire thickness of the glass-based article, and is greatest at the first surface 302 and/or the second surface 304 and decreases substantially constantly to a point between the first surface 302 and the second surface 304. At that point, the concentration of the metal oxide is the least along the entire thickness t; however the concentration is also non-zero at that point. In other words, the non-zero concentration of that particular metal oxide extends along a substantial portion of the thickness t (as described herein) or the entire thickness t. In some embodiments, the lowest concentration in the particular metal oxide is in the CT layer 327. The total concentration of the particular metal oxide in the glass-based article may be in the range from about 1 mol % to about 20 mol %.


In one or more embodiments, the glass-based article includes a first metal oxide concentration and a second metal oxide concentration, such that the first metal oxide concentration is in the range from about 0 mol % to about 15 mol % along a first thickness range from about 0·t to about 0.5t, and the second metal oxide concentration is in the range from about 0 mol % to about 10 mol % from a second thickness range from about 0 micrometers to about 25 micrometers (or from about 0 micrometers to about 12 micrometers); however, the concentration of one or both the first metal oxide and the second metal oxide is non-zero along a substantial portion or the entire thickness of the glass-based article. The glass-based article may include an optional third metal oxide concentration. The first metal oxide may include Na2O while the second metal oxide may include K2O.


The concentration of the metal oxide may be determined from a baseline amount of the metal oxide in the glass article prior to being modified to include the concentration gradient of such metal oxide.


The glass articles described herein may exhibit a stored tensile energy in the range from greater than 15 J/m2 or greater (e.g., from about 15 J/m2 to about 50 J/m2). For example, in some embodiments, the stored tensile energy may be in the range from about 20 J/m2 to about 150 J/m2. In some instances, the stored tensile energy may be in the range from about 25 J/m2 to about 150 J/m2, from about 30 J/m2 to about 150 J/m2, from about 35 J/m2 to about 150 J/m2, from about 40 J/m2 to about 150 J/m2, from about 45 J/m2 to about 150 J/m2, from about 50 J/m2 to about 150 J/m2, from about 55 J/m2 to about 150 J/m2, from about 60 J/m2 to about 150 J/m2, from about 65 J/m2 to about 150 J/m2, from about 25 J/m2 to about 140 J/m2, from about 25 J/m2 to about 130 J/m2, from about 25 J/m2 to about 120 J/m2, from about 25 J/m2 to about 110 J/m2, from about 30 J/m2 to about 140 J/m2, from about 35 J/m2 to about 130 J/m2, from about 40 J/m2 to about 120 J/m2 or from about 40 J/m2 to about 100 J/m2. The thermally and chemically strengthened glass-based articles of one or more embodiments may exhibit a stored tensile energy of about 40 J/m2 or greater, about 45 J/m2 or greater, about 50 J/m2 or greater, about 60 J/m2 or greater, or about 70 J/m2 or greater.


Stored tensile energy is calculated using the following Equation (2):

stored tensile energy (J/m2)=[1−ν]/E∫σ{circumflex over ( )}2dt  (2)

where ν is Poisson's ratio, E is the Young's modulus and the integration is computed for the tensile region only. Equation (2) is described in Suresh T. Gulati, Frangibility of Tempered Soda-Lime Glass Sheet, GLASS PROCESSING DAYS, The Fifth International Conference on Architectural and Automotive Glass, 13-15 Sep. 1997, as equation number 4.


The glass articles of some embodiments exhibit superior mechanical performance as demonstrated by device drop testing or component level testing, as compared to known strengthened glass articles. In one or more embodiments, the glass articles exhibit improved surface strength when subjected to abraded ring-on-ring (AROR) testing. The strength of a material is defined as the stress at which fracture occurs. The AROR test is a surface strength measurement for testing flat glass specimens, and ASTM C1499-09 (2013), entitled “Standard Test Method for Monotonic Equibiaxial Flexural Strength of Advanced Ceramics at Ambient Temperature,” serves as the basis for the ring-on-ring abraded ROR test methodology described herein. The contents of ASTM C1499-09 are incorporated herein by reference in their entirety. In one embodiment, the glass specimen is abraded prior to ring-on-ring testing with 90 grit silicon carbide (SiC) particles that are delivered to the glass sample using the method and apparatus described in Annex A2, entitled “abrasion Procedures,” of ASTM C158-02 (2012), entitled “Standard Test Methods for Strength of Glass by Flexure (Determination of Modulus of Rupture). The contents of ASTM C158-02 and the contents of Annex 2 in particular are incorporated herein by reference in their entirety.


Prior to ring-on-ring testing a surface of the glass article is abraded as described in ASTM C158-02, Annex 2, to normalize and/or control the surface defect condition of the sample using the apparatus shown in Figure A2.1 of ASTM C158-02. The abrasive material is typically sandblasted onto the surface 110 of the glass article at a load or pressure of 15 psi or greater using an air pressure of 304 kPa (44 psi). In some embodiments, the abrasive material may be sandblasted onto the surface 110 at a load of 20 psi, 25 psi or even 45 psi. After air flow is established, 5 cm3 of abrasive material is dumped into a funnel and the sample is sandblasted for 5 seconds after introduction of the abrasive material.


For the ring-on-ring test, a glass article having at least one abraded surface 112 as shown in FIG. 5 is placed between two concentric rings of differing size to determine equibiaxial flexural strength or failure load (i.e., the maximum stress that a material is capable of sustaining when subjected to flexure between two concentric rings), as also shown in FIG. 5. In the abraded ring-on-ring configuration 10, the abraded glass article 110 is supported by a support ring 120 having a diameter D2. A force F is applied by a load cell (not shown) to the surface of the glass article by a loading ring 130 having a diameter D1.


The ratio of diameters of the loading ring and support ring D1/D2 may be in a range from about 0.2 to about 0.5. In some embodiments, D1/D2 is about 0.5. Loading and support rings 130, 120 should be aligned concentrically to within 0.5% of support ring diameter D2. The load cell used for testing should be accurate to within 1% at any load within a selected range. In some embodiments, testing is carried out at a temperature of 23±2° C. and a relative humidity of 40±10%.


For fixture design, the radius r of the protruding surface of the loading ring 430, h/2≤r≤3h/2, where h is the thickness of glass article 110. Loading and support rings 130, 120 are typically made of hardened steel with hardness HRc>40. ROR fixtures are commercially available.


The intended failure mechanism for the ROR testis to observe fracture of the glass article 110 originating from the surface 130a within the loading ring 130. Failures that occur outside of this region—i.e., between the loading rings 130 and support rings 120—are omitted from data analysis. Due to the thinness and high strength of the glass article 110, however, large deflections that exceed % of the specimen thickness h are sometimes observed. It is therefore not uncommon to observe a high percentage of failures originating from underneath the loading ring 130. Stress cannot be accurately calculated without knowledge of stress development both inside and under the ring (collected via strain gauge analysis) and the origin of failure in each specimen. AROR testing therefore focuses on peak load at failure as the measured response.


The strength of glass article depends on the presence of surface flaws. However, the likelihood of a flaw of a given size being present cannot be precisely predicted, as the strength of glass is statistical in nature. A probability distribution can therefore generally be used as a statistical representation of the data obtained.


In some embodiments, the strengthened glass articles described herein exhibits a equibiaxial flexural strength or failure load of 20 kgf or greater and up to about 45 kgf as determined by AROR testing using a load of 25 psi or even 45 psi to abrade the surface. In other embodiments, the surface strength is at least 25 kgf, and in still other embodiments, at least 30 kgf.


In some embodiments, the strengthened glass articles may exhibit improved drop performance. As used herein, the drop performance is evaluated by assembling the glass article to a mobile phone device. In some instances, a number of glass articles may be assembled to identical mobile phone devices and tested identically. The mobile phone device with the glass article assembled thereto is then dropped onto an abrasive paper (which may include Al2O3 particles or other abradant) for successive drops starting at a height of 50 cm. As each sample survives the drop from a height, the mobile phone device with the sample is dropped again from an increase height until the glass article fracture, at which point the failure height of that sample is recorded as a maximum failure height.


In some embodiments, the glass articles exhibit a maximum failure height of about 100 cm or greater, when having a thickness of about 1 mm. In some embodiments, the glass articles exhibit a maximum failure height of about 120 cm or greater, about 140 cm or greater, about 150 cm or greater, about 160 cm or greater, about 180 cm or greater or about 200 cm or greater, at a thickness of about 1 mm. The glass articles of one or more embodiments exhibit a diced fracture pattern after failing at the failure height. The diced fracture pattern includes exhibiting the aspect ratio described herein.


In one or more embodiments, the glass articles herein exhibit fracture behavior such that, when the glass article is directly bonded to a substrate (i.e. a display unit), after the glass article fractures, 50% or more of the cracks are sub-surface cracks (where cracks extend only partially through the thickness and arrest below surface. For example, in some instances, the cracks may extend partially through the thickness t of the glass article, for example, from 0.05t to 0.95t. The percentage of cracks in the glass article that extend only partially through the thickness t may be 50% greater, 60% or greater, 70% or greater, 80% or greater or 90% or greater.


In some embodiments, the strengthened glass-based articles described herein may be described in terms of performance in an inverted ball on sandpaper (IBoS) test. The IBoS test is a dynamic component level test that mimics the dominant mechanism for failure due to damage introduction plus bending that typically occurs in glass-based articles that are used in mobile or hand held electronic devices, as schematically shown in FIG. 6. In the field, damage introduction (a in FIG. 7) occurs on the top surface of the glass-based article. Fracture initiates on the top surface of the glass-based article and damage either penetrates the glass-based article (b in FIG. 7) or the fracture propagates from bending on the top surface or from the interior portions of the glass-based article (c in FIG. 7). The IBoS test is designed to simultaneously introduce damage to the surface of the glass and apply bending under dynamic load. In some instances, the glass-based article exhibits improved drop performance when it includes a compressive stress than if the same glass-based article does not include a compressive stress.


An IBoS test apparatus is schematically shown in FIG. 6. Apparatus 500 includes a test stand 510 and a ball 530. Ball 530 is a rigid or solid ball such as, for example, a stainless steel ball, or the like. In one embodiment, ball 530 is a 4.2 gram stainless steel ball having diameter of 10 mm. The ball 530 is dropped directly onto the glass-based article sample 518 from a predetermined height h. Test stand 510 includes a solid base 512 comprising a hard, rigid material such as granite or the like. A sheet 514 having an abrasive material disposed on a surface is placed on the upper surface of the solid base 512 such that surface with the abrasive material faces upward. In some embodiments, sheet 514 is sandpaper having a 30 grit surface and, in other embodiments, a 180 grit surface. The glass-based article sample 518 is held in place above sheet 514 by sample holder 515 such that an air gap 516 exists between glass-based article sample 518 and sheet 514. The air gap 516 between sheet 514 and glass-based article sample 518 allows the glass-based article sample 518 to bend upon impact by ball 530 and onto the abrasive surface of sheet 514. In one embodiment, the glass-based article sample 218 is clamped across all corners to keep bending contained only to the point of ball impact and to ensure repeatability. In some embodiments, sample holder 514 and test stand 510 are adapted to accommodate sample thicknesses of up to about 2 mm. The air gap 516 is in a range from about 50 μm to about 100 μm. Air gap 516 is adapted to adjust for difference of material stiffness (Young's modulus, Emod), but also includes the Young's modulus and thickness of the sample. An adhesive tape 520 may be used to cover the upper surface of the glass-based article sample to collect fragments in the event of fracture of the glass-based article sample 518 upon impact of ball 530.


Various materials may be used as the abrasive surface. In a one particular embodiment, the abrasive surface is sandpaper, such as silicon carbide or alumina sandpaper, engineered sandpaper, or any abrasive material known to those skilled in the art for having comparable hardness and/or sharpness. In some embodiments, sandpaper having 30 grit may be used, as it has a surface topography that is more consistent than either concrete or asphalt, and a particle size and sharpness that produces the desired level of specimen surface damage.


In one aspect, a method 600 of conducting the IBoS test using the apparatus 500 described hereinabove is shown in FIG. 8. In Step 610, a glass-based article sample (218 in FIG. 6) is placed in the test stand 510, described previously and secured in sample holder 515 such that an air gap 516 is formed between the glass-based article sample 518 and sheet 514 with an abrasive surface. Method 600 presumes that the sheet 514 with an abrasive surface has already been placed in test stand 510. In some embodiments, however, the method may include placing sheet 514 in test stand 510 such that the surface with abrasive material faces upward. In some embodiments (Step 610a), an adhesive tape 520 is applied to the upper surface of the glass-based article sample 518 prior to securing the glass-based article sample 518 in the sample holder 510.


In Step 520, a solid ball 530 of predetermined mass and size is dropped from a predetermined height h onto the upper surface of the glass-based article sample 518, such that the ball 530 impacts the upper surface (or adhesive tape 520 affixed to the upper surface) at approximately the center (i.e., within 1 mm, or within 3 mm, or within 5 mm, or within 10 mm of the center) of the upper surface. Following impact in Step 520, the extent of damage to the glass-based article sample 518 is determined (Step 630). As previously described hereinabove, herein, the term “fracture” means that a crack propagates across the entire thickness and/or entire surface of a substrate when the substrate is dropped or impacted by an object.


In method 600, the sheet 518 with the abrasive surface may be replaced after each drop to avoid “aging” effects that have been observed in repeated use of other types (e.g., concrete or asphalt) of drop test surfaces.


Various predetermined drop heights hand increments are typically used in method 600. The test may, for example, utilize a minimum drop height to start (e.g., about 10-20 cm). The height may then be increased for successive drops by either a set increment or variable increments. The test described in method 600 is stopped once the glass-based article sample 518 breaks or fractures (Step 631). Alternatively, if the drop height h reaches the maximum drop height (e.g., about 100 cm) without fracture, the drop test of method 300 may also be stopped, or Step 520 may be repeated at the maximum height until fracture occurs.


In some embodiments, IBoS test of method 600 is performed only once on each glass-based article sample 518 at each predetermined height h. In other embodiments, however, each sample may be subjected to multiple tests at each height.


If fracture of the glass-based article sample 518 has occurred (Step 631 in FIG. 7), the IBoS test according to method 600 is ended (Step 640). If no fracture resulting from the ball drop at the predetermined drop height is observed (Step 632), the drop height is increased by a predetermined increment (Step 634)—such as, for example 5, 10, or 20 cm—and Steps 620 and 630 are repeated until either sample fracture is observed (631) or the maximum test height is reached (636) without sample fracture. When either Step 631 or 636 is reached, the test according to method 600 is ended.


When subjected to the inverted ball on sandpaper (IBoS) test described above, embodiments of the glass-based article described herein have at least about a 60% survival rate when the ball is dropped onto the surface of the glass from a height of 100 cm. For example, a glass-based article is described as having a 60% survival rate when dropped from a given height when three of five identical (or nearly identical) samples (i.e., having approximately the same composition and, when strengthened, approximately the same compressive stress and depth of compression or compressive stress layer, as described herein) survive the IBoS drop test without fracture when dropped from the prescribed height (here 100 cm). In other embodiments, the survival rate in the 100 cm IBoS test of the glass-based articles that are strengthened is at least about 70%, in other embodiments, at least about 80%, and, in still other embodiments, at least about 90%. In other embodiments, the survival rate of the strengthened glass-based articles dropped from a height of 100 cm in the IBoS test is at least about 60%, in other embodiments, at least about 70%, in still other embodiments, at least about 80%, and, in other embodiments, at least about 90%. In one or more embodiments, the survival rate of the strengthened glass-based articles dropped from a height of 150 cm in the IBoS test is at least about 60%, in other embodiments, at least about 70%, in still other embodiments, at least about 80%, and, in other embodiments, at least about 90%.


To determine the survivability rate of the glass-based articles when dropped from a predetermined height using the IBoS test method and apparatus described hereinabove, at least five identical (or nearly identical) samples (i.e., having approximately the same composition and, if strengthened, approximately the same compressive stress and depth of compression or layer) of the glass-based articles are tested, although larger numbers (e.g., 10, 20, 30, etc.) of samples may be subjected to testing to raise the confidence level of the test results. Each sample is dropped a single time from the predetermined height (e.g., 100 cm or 150 cm) or, alternatively, dropped from progressively higher heights without fracture until the predetermined height is reached, and visually (i.e., with the naked eye) examined for evidence of fracture (crack formation and propagation across the entire thickness and/or entire surface of a sample). A sample is deemed to have “survived” the drop test if no fracture is observed after being dropped from the predetermined height, and a sample is deemed to have “failed (or “not survived”) if fracture is observed when the sample is dropped from a height that is less than or equal to the predetermined height. The survivability rate is determined to be the percentage of the sample population that survived the drop test. For example, if 7 samples out of a group of 10 did not fracture when dropped from the predetermined height, the survivability rate of the glass would be 70%.


In one or more embodiments, the glass articles exhibit a lower delayed fracture rate (i.e., the glass articles, when fractured, fracture quickly or even immediately). In some embodiments, this fracture rate may be attributed to the deep DOC and high level of CT. Specifically, there is a lower probability that the glass article will break spontaneously, well after the insult to the glass article that induces fracture or failure occurs. In one or more embodiments, when the glass article fractures, it fractures into a plurality of fragments within 2 seconds or 1 second or less after impact measured by the “Frangibility Test”, as described Z. Tang, et al. Automated Apparatus for Measuring the Frangibility and Fragmentation of Strengthened Glass. Experimental Mechanics (2014) 54:903-912. The Frangibility Test utilizes a drop height of the stylus of 50 mm and a stylus with a tungsten carbide tip (available from Fisher Scientific Industries, under the trademark TOSCO® and manufacturer identifying number #13-378, with a 60 degree coni-spherical tip), having a weight of 40 g. In some embodiments, a primary fracture (or the first fracture visible to the naked eye that creates 2 fragments) occurs immediately or within zero seconds or 0.1 seconds after an impact that causes the glass article to fracture. In one or more embodiments, the probability of the primary fracture occurring within the time periods described herein, as measured by the Frangibility Test, is about 90% or greater In some embodiments, secondary fracture(s) occur within 5 seconds or less (e.g., 4 seconds or less, 3 seconds or less, 2 seconds or less or about 1 second or less). As used herein, “secondary fracture” means a fracture that occurs after the primary fracture. In one or more embodiments, the probability of the secondary fracture(s) occurring within the time periods described herein, as measured by the Frangibility Test, is about 90% or greater.


In one or more embodiments, upon fracturing, the glass article ejects fewer and smaller fragments that are of potential concern to a user than is exhibited by known glass articles currently being used on mobile electronic devices. As used herein, the term “ejects” or “ejected” refers to fragments that move from their original position or placement in the glass article after the glass article is fractured. In some embodiments, after the glass article is fractured and a plurality of fragments is formed, about 10% or less (e.g., about 8% or less, about 6% or less, or about 5% or less) of the plurality of fragments is ejected. In some embodiments, after the glass article is fractured and a plurality of fragments is formed, about 50% of more of the ejected portion of the plurality of fragments has a maximum dimension less than 0.5 mm. In some embodiments, the number or amount of ejected fragments may be characterized by weight, in relation to the glass article before and after fracture. For example, the difference between the weight of the glass article prior to fracture (including the total weight of the ejected portion of the plurality of fragments and the non-ejected portion of fragments, after fracture) and the weight of the non-ejected portion of fragments, may be less than about 1% or less of the weight prior to impact. In some instances, difference between the weight of the glass article prior to fracture (including the total weight of the ejected portion of the plurality of fragments and the non-ejected portion of fragments, after fracture) and the weight of the non-ejected portion of fragments, may be less than about 0.0005 g (e.g., 0.0004 g or less, 0.0003 g or less, 0.0002 g or less, or 0.0001 g or less). To determine the weight of the non-ejected portion.


In one or more embodiments, the glass article exhibits a high degree of dicing in a more uniform pattern across the surface and volume thereof. In some embodiments, this high degree of dicing and uniformity is exhibited where the glass article has a non-uniform thickness (i.e., is shaped to have a three-dimensional or 2.5 dimensional shape). Without being bound by theory, this enables the thinnest portion of the glass article to be strengthened to a sufficient degree, without having some portions of the glass article exhibiting frangibility while other portions are non-frangible, as defined by current industry norms.


In one or more embodiments, the glass article (directly bonded to the substrate, i.e., a display unit) exhibits a haze after being fractured, due to the dense fracture pattern. The readability of depends on viewing angle and the thickness of the glass-based article. At a viewing angle of 90 degrees to a major surface of the glass article or at normal incidence, the fractured glass article exhibits a low haze such that an underlying image or text is visible to the naked eye. At a viewing angle of 70 degrees or less to a major surface of the glass article (or 30 degrees or more away from normal incidence), the fractured glass article exhibits a haze that prevents the underlying image or text from being visible to the naked eye. It should be understood that such haze is present when the fragments of the glass article are still held together or when less than 10% of the fragments are ejected from the glass article. Without being bound by theory, it is believed that the glass article after fracture may provide privacy screen functionality due to its low haze at 90 degrees and the high haze at smaller viewing angles.


In some embodiments, at least one major surface of the glass article has a low surface roughness after the glass article is fractured. This attribute is desirable where the glass article may be used or touched by a user even after the glass article is fractured so that cuts and abrasions to the user are minimized or eliminated.


In one or more embodiments, the glass articles described herein may be combined with a containment layer. The containment layer is a material that can contain the fragments of the glass article, when fractured. For example, the containment layer may include a polymeric material. In one or more embodiments, the containment layer may include an adhesive material (such as a pressure-sensitive adhesive material). In one or more embodiments, the containment layer may have a Young's modulus in the range from about 0.5 to about 1.2 MPa. In one or more embodiments, the containment layer may include a filled epoxy, an unfilled epoxy, a filled urethane or an unfilled urethane.


An example of a filled epoxy includes a UV induced catiltic epoxy from the polymerization product of 70.69 wt % Nanopox C620 colloidal silica sol (40% silica nanoparticles in cycloaliphatic epoxy resin), 23.56 wt % Nanopox C680 (50% wt silica nanoparticles in 3-ethyl-3-hydroxymethyl-oxetane), 3 wt % Coatosil MP-200 epoxy functional silane (adhesion promoter), 2.5 wt % Cyracril UVI-6976 (cationic photoinitiator, including triarylsulfonium hexaflouroantimonate salts in propylene carbonate), 0.25 wt % Tinuvine 292 amine stabilizer (bis(1,2,2,6,6-pentamethyl-4-piperidinyl)-sebacate and 1-(methyl)-8-(1,2,2,6,6-pentamethyl-4-piperidinyl)-sebacate),


An example of an unfilled epoxy material includes 48 wt % Synasia S06E cycloaliphatic epoxy, 48 wt % Synasia S-101 (3-ethyl-3-oxetanemethanol), 1 wt % UVI-6976 (cationic photoinitiator), and 3 wt % Silquest A-186 (epoxy functionalized silane).


In some embodiments, a low modulus urethane acrylate can be used in the containment layer. In some embodiments, this material may include silica filling. An example of a low modulus urethane acrylate includes 31.5 wt % Doublemer 554 (aliphatic urethane diacrylate resin), 1.5 wt % Genomer 4188/M22 (monofunctional urethane acrylate), 20 wt % NK Ester A-SA (beta-acryloyl oxyethyl hydrogen succinate), 10 wt % Sartomer SR339 2 (phenoxyethyl acrylate), 4 wt % Irgacure 2022 (photoinitiator, acyl phosphine oxide/alpha hydroxy ketone), 3 wt % adhesion promoter (e.g., Silquest A-189, gamma-mercaptopropyltrimethoxysilane). To form a filled urethane, 4 wt % silica powder (such as Hi Sil 233) may be added.


In one or more embodiments, the glass article may be combined with a containment layer with or without being adhered thereto. In some embodiments, the glass articles may be disposed on and adhered to a containment layer. The glass article may be temporarily adhered or permanently adhered to a containment layer. As shown in FIG. 9A, the containment layer 20 is disposed on at least one major surface (e.g., 12, 14, in FIG. 1A) of the glass article. In FIG. 9A, the containment layer 20 is not disposed on any portion of the minor surfaces 16, 18; however, the containment layer 20 may extend from the major surface to at least partially along one or both minor surfaces (16, 18) or along the entire length of one or both minor surfaces (16, 18). In such embodiments, the containment layer may be formed from the same material. In one or more alternative embodiments, the containment layer formed on the major surface may be different from the containment layer formed on any portion of the minor surface(s). FIG. 9B illustrates an embodiment in which the containment layer 20 is disposed on the major surface 14 and a second containment layer 22 is disposed on both minor surfaces 16, 18. In one or more embodiment, the containment layer 20 differs compositionally from the second containment layer 22.


In one or more embodiments, the glass article may include a stress profile including a spike, as described herein, such that the surface CS is in the range from about 400 MPa to about 1200 MPa and includes an containment material 20 on one major surface 14, and a second containment material 22 on both minor surfaces 16, 18 (as shown in FIG. 9B). In one or more embodiments, the glass article may include a stress profile without a spike, such that the surface CS is in the range from about 150 MPa to about 500 MPa, and includes only containment material 20 on major surface 14 (as shown in FIG. 9A). The glass articles described herein may be incorporated into various products and articles such as in consumer electronics products or devices (e.g., cover glass for mobile electronic devices and touch-enabled displays). The glass articles may also be used in displays (or as display articles) (e.g., billboards, point of sale systems, computers, navigation systems, and the like), architectural articles (walls, fixtures, panels, windows, etc.), transportation articles (e.g., in automotive applications, trains, aircraft, sea craft, etc.), appliances (e.g., washers, dryers, dishwashers, refrigerators and the like), packaging (e.g., pharmaceutical packaging or containers) or any article that requires some fracture resistance.


As shown in FIG. 10, an electronic device 1000 may include a glass-based article 100 according to one or more embodiments described herein. The device 100 includes a housing 1020 having front 1040, back 1060, and side surfaces 1080; electrical components (not shown) that are at least partially inside or entirely within the housing and including at least a controller, a memory, and a display 1120 at or adjacent to the front surface of the housing. The glass-based article 100 is shown as a cover disposed at or over the front surface of the housing such that it is over the display 1120. In some embodiments, the glass-based article may be used as a back cover.


In some embodiments, the electronic device may include a tablet, a transparent display, a mobile phone, a video player, an information terminal device, an e-reader, a laptop computer, or a non-transparent display.


In one or more embodiments, the glass articles described herein may be used in packaging. For example, the packaging may include glass articles in the form of bottles, vials or containers that hold a liquid, solid or gas material. In one or more embodiments, the glass articles are vials that include chemicals such as pharmaceutical materials. In one or more embodiments, the packaging includes a housing including an opening, an exterior surface and an interior surface defining an enclosure. The housing may be formed from the glass articles described herein. The glass article includes a containment layer. In some embodiments, the enclosure is filled with a chemical or pharmaceutical material. In one or more embodiments, the opening of the housing may be closed or sealed by a cap. In other words, the cap may be disposed in the opening to close or seal the enclosure.


The glass article may include an amorphous substrate, a crystalline substrate or a combination thereof (e.g., a glass-ceramic substrate). The glass article may include an alkali aluminosilicate glass, alkali containing borosilicate glass, alkali aluminophosphosilicate glass or alkali aluminoborosilicate glass. In one or more embodiments, the glass article substrate (prior to being chemically strengthened as described herein) may include a glass having a composition, in mole percent (mole %), including: SiO2 in the range from about 40 to about 80, Al2O3 in the range from about 10 to about 30, B2O3 in the range from about 0 to about 10, R2O in the range from about 0 to about 20, and RO in the range from about 0 to about 15. In some instances, the composition may include either one or both of ZrO2 in the range from about 0 mol % to about 5 mol % and P2O5 in the range from about 0 to about 15 mol %. TiO2 can be present from about 0 mol % to about 2 mol %.


In some embodiments, the glass composition may include SiO2 in an amount, in mol %, in the range from about 45 to about 80, from about 45 to about 75, from about 45 to about 70, from about 45 to about 65, from about 45 to about 60, from about 45 to about 65, from about 45 to about 65, from about 50 to about 70, from about 55 to about 70, from about 60 to about 70, from about 70 to about 75, or from about 50 to about 65.


In some embodiments, the glass composition may include Al2O3 in an amount, in mol %, in the range from about 5 to about 28, from about 5 to about 26, from about 5 to about 25, from about 5 to about 24, from about 5 to about 22, from about 5 to about 20, from about 6 to about 30, from about 8 to about 30, from about 10 to about 30, from about 12 to about 30, from about 14 to about 30, from about 16 to about 30, from about 18 to about 30, or from about 18 to about 28.


In one or more embodiments, the glass composition may include B2O3 in an amount, in mol %, in the range from about 0 to about 8, from about 0 to about 6, from about 0 to about 4, from about 0.1 to about 8, from about 0.1 to about 6, from about 0.1 to about 4, from about 1 to about 10, from about 2 to about 10, from about 4 to about 10, from about 2 to about 8, from about 0.1 to about 5, or from about 1 to about 3. In some instances, the glass composition may be substantially free of B2O3. As used herein, the phrase “substantially free” with respect to the components of the composition means that the component is not actively or intentionally added to the composition during initial batching, but may be present as an impurity in an amount less than about 0.001 mol %.


In some embodiments, the glass composition may include one or more alkali earth metal oxides, such as MgO, CaO and ZnO. In some embodiments, the total amount of the one or more alkali earth metal oxides may be a non-zero amount up to about 15 mol %. In one or more specific embodiments, the total amount of any of the alkali earth metal oxides may be a non-zero amount up to about 14 mol %, up to about 12 mol %, up to about 10 mol %, up to about 8 mol %, up to about 6 mol %, up to about 4 mol %, up to about 2 mol %, or up about 1.5 mol %. In some embodiments, the total amount, in mol %, of the one or more alkali earth metal oxides may be in the range from about 0.1 to 10, from about 0.1 to 8, from about 0.1 to 6, from about 0.1 to 5, from about 1 to 10, from about 2 to 10, or from about 2.5 to 8. The amount of MgO may be in the range from about 0 mol % to about 5 mol % (e.g., from about 2 mol % to about 4 mol %). The amount of ZnO may be in the range from about 0 to about 2 mol %. The amount of CaO may be from about 0 mol % to about 2 mol %. In one or more embodiments, the glass composition may include MgO and may be substantially free of CaO and ZnO. In one variant, the glass composition may include any one of CaO or ZnO and may be substantially free of the others of MgO, CaO and ZnO. In one or more specific embodiments, the glass composition may include only two of the alkali earth metal oxides of MgO, CaO and ZnO and may be substantially free of the third of the earth metal oxides.


The total amount, in mol %, of alkali metal oxides R2O in the glass composition may be in the range from about 5 to about 20, from about 5 to about 18, from about 5 to about 16, from about 5 to about 15, from about 5 to about 14, from about 5 to about 12, from about 5 to about 10, from about 5 to about 8, from about 5 to about 20, from about 6 to about 20, from about 7 to about 20, from about 8 to about 20, from about 9 to about 20, from about 10 to about 20, from about 6 to about 13, or from about 8 to about 12.


In one or more embodiments, the glass composition includes Na2O in an amount in the range from about 0 mol % to about 18 mol %, from about 0 mol % to about 16 mol % or from about 0 mol % to about 14 mol %, from about 0 mol % to about 10 mol %, from about 0 mol % to about 5 mol %, from about 0 mol % to about 2 mol %, from about 0.1 mol % to about 6 mol %, from about 0.1 mol % to about 5 mol %, from about 1 mol % to about 5 mol %, from about 2 mol % to about 5 mol %, or from about 10 mol % to about 20 mol %.


In some embodiments, the amount of Li2O and Na2O is controlled to a specific amount or ratio to balance formability and ion exchangeability. For example, as the amount of Li2O increases, the liquidus viscosity may be reduced, thus preventing some forming methods from being used; however, such glass compositions are ion exchanged to deeper DOC levels, as described herein. The amount of Na2O can modify liquidus viscosity but can inhibit ion exchange to deeper DOC levels.


In one or more embodiments, the glass composition may include K2O in an amount less than about 5 mol %, less than about 4 mol %, less than about 3 mol %, less than about 2 mol %, or less than about 1 mol %. In one or more alternative embodiments, the glass composition may be substantially free, as defined herein, of K2O.


In one or more embodiments, the glass composition may include Li2O in an amount about 0 mol % to about 18 mol %, from about 0 mol % to about 15 mol % or from about 0 mol % to about 10 mol %, from about 0 mol % to about 8 mol %, from about 0 mol % to about 6 mol %, from about 0 mol % to about 4 mol % or from about 0 mol % to about 2 mol %. In some embodiments, the glass composition may include Li2O in an amount about 2 mol % to about 10 mol %, from about 4 mol % to about 10 mol %, from about 6 mol % to about 10 mol, or from about 5 mol % to about 8 mol %. In one or more alternative embodiments, the glass composition may be substantially free, as defined herein, of Li2O.


In one or more embodiments, the glass composition may include Fe2O3. In such embodiments, Fe2O3 may be present in an amount less than about 1 mol %, less than about 0.9 mol %, less than about 0.8 mol %, less than about 0.7 mol %, less than about 0.6 mol %, less than about 0.5 mol %, less than about 0.4 mol %, less than about 0.3 mol %, less than about 0.2 mol %, less than about 0.1 mol % and all ranges and sub-ranges therebetween. In one or more alternative embodiments, the glass composition may be substantially free, as defined herein, of Fe2O3.


In one or more embodiments, the glass composition may include ZrO2. In such embodiments, ZrO2 may be present in an amount less than about 1 mol %, less than about 0.9 mol %, less than about 0.8 mol %, less than about 0.7 mol %, less than about 0.6 mol %, less than about 0.5 mol %, less than about 0.4 mol %, less than about 0.3 mol %, less than about 0.2 mol %, less than about 0.1 mol % and all ranges and sub-ranges therebetween. In one or more alternative embodiments, the glass composition may be substantially free, as defined herein, of ZrO2.


In one or more embodiments, the glass composition may include P2O5 in a range from about 0 mol % to about 10 mol %, from about 0 mol % to about 8 mol %, from about 0 mol % to about 6 mol %, from about 0 mol % to about 4 mol %, from about 0.1 mol % to about 10 mol %, from about 0.1 mol % to about 8 mol %, from about 4 mol % to about 8 mol %, or from about 5 mol % to about 8 mol %. In some instances, the glass composition may be substantially free of P2O5.


In one or more embodiments, the glass composition may include TiO2. In such embodiments, TiO2 may be present in an amount less than about 6 mol %, less than about 4 mol %, less than about 2 mol %, or less than about 1 mol %. In one or more alternative embodiments, the glass composition may be substantially free, as defined herein, of TiO2. In some embodiments, TiO2 is present in an amount in the range from about 0.1 mol % to about 6 mol %, or from about 0.1 mol % to about 4 mol %. In some embodiments, the glass may be substantially free of TiO2.


In some embodiments, the glass composition may include various compositional relationships. For example, the glass composition may include a ratio of the amount of Li2O (in mol %) to the total amount of R2O (in mol %) in the range from about 0.5 to about 1. In some embodiments, the glass composition may include a difference between the total amount of R2O (in mol %) to the amount of Al2O3 (in mol %) in the range from about −5 to about 0. In some instances the glass composition may include a difference between the total amount of RxO (in mol %) and the amount of Al2O3 in the range from about 0 to about 3. The glass composition of one or more embodiments may exhibit a ratio of the amount of MgO (in mol %) to the total amount of RO (in mol %) in the range from about 0 to about 2.


In some embodiments, the compositions used for the glass substrate may be batched with 0-2 mol % of at least one fining agent selected from a group that includes Na2SO4, NaCl, NaF, NaBr, K2SO4, KCl, KF, KBr, and SnO2. The glass composition according to one or more embodiments may further include SnO2 in the range from about 0 to about 2, from about 0 to about 1, from about 0.1 to about 2, from about 0.1 to about 1, or from about 1 to about 2. The glass compositions disclosed herein may be substantially free of As2O3 and/or Sb2O3.


In one or more embodiments, the composition may specifically include 62 mol % to 75 mol % SiO2; 10.5 mol % to about 17 mol % Al2O3; 5 mol % to about 13 mol % Li 20; 0 mol % to about 4 mol % ZnO; 0 mol % to about 8 mol % MgO; 2 mol % to about 5 mol % TiO2; 0 mol % to about 4 mol % B2O3; 0 mol % to about 5 mol % Na2O; 0 mol % to about 4 mol % K2O; 0 mol % to about 2 mol % ZrO2; 0 mol % to about 7 mol P2O5; 0 mol to about 0.3 mol % Fe2O3; 0 mol % to about 2 mol % MnOx; and 0.05 mol % to about 0.2 mol % SnO2.


In one or more embodiments, the composition may include 67 mol % to about 74 mol % SiO2; 11 mol % to about 15 mol % Al2O3; 5.5 mol % to about 9 mol % Li 20; 0.5 mol % to about 2 mol % ZnO; 2 mol % to about 4.5 mol % MgO; 3 mol % to about 4.5 mol % TiO2; 0 mol % to about 2.2 mol % B2O3; 0 mol % to about 1 mol % Na2O; 0 mol % to about 1 mol % K2O; 0 mol % to about 1 mol % ZrO2; 0 mol % to about 4 mol P2O5; 0 mol to about 0.1 mol % Fe2O3; 0 mol % to about 1.5 mol % MnOx; and 0.08 mol % to about 0.16 mol % SnO2.


In one or more embodiments, the composition may include 70 mol % to 75 mol % SiO2; 10 mol % to about 15 mol % Al2O3; 5 mol % to about 13 mol % Li 20; 0 mol % to about 4 mol % ZnO; 0.1 mol % to about 8 mol % MgO; 0 mol % to about 5 mol % TiO2; 0.1 mol % to about 4 mol % B2O3; 0.1 mol % to about 5 mol % Na2; 0 mol % to about 4 mol % K2O; 0 mol % to about 2 mol % ZrO2; 0 mol % to about 7 mol % P2O5; 0 mol % to about 0.3 mol % Fe2O3; 0 mol % to about 2 mol % MnOx; and 0.05 mol % to about 0.2 mol % SnO2.


In one or more embodiments, the composition may include 52 mol % to about 63 mol % SiO2; 11 mol % to about 15 mol % Al2O3; 5.5 mol % to about 9 mol % Li 20; 0.5 mol % to about 2 mol % ZnO; 2 mol % to about 4.5 mol % MgO; 3 mol % to about 4.5 mol % TiO2; 0 mol % to about 2.2 mol % B2O3; 0 mol % to about 1 mol % Na2O; 0 mol % to about 1 mol % K2O; 0 mol % to about 1 mol % ZrO2; 0 mol % to about 4 mol P2O5; 0 mol to about 0.1 mol % Fe2O3; 0 mol % to about 1.5 mol % MnOx; and 0.08 mol % to about 0.16 mol % SnO2.


In some embodiments, the composition may be substantially free of any one or more of B2O3, TiO2, K2O and ZrO2.


In one or more embodiments, the composition may include at least 0.5 mol % P2O5, Na2O and, optionally, Li2O, where Li2O (mol %)/Na2O (mol %)<1. In addition, these compositions may be substantially free of B2O3 and K2O. In some embodiments, the composition may include ZnO, MgO, and SnO2.


In some embodiments, the composition may comprise: from about 58 mol % to about 65 mol % SiO2; from about 11 mol % to about 19 mol % Al2O3; from about 0.5 mol % to about 3 mol % P2O5; from about 6 mol % to about 18 mol % Na2O; from 0 mol % to about 6 mol % MgO; and from 0 mol % to about 6 mol % ZnO. In certain embodiments, the composition may comprise from about 63 mol % to about 65 mol % SiO2; from 11 mol % to about 17 mol % Al2O3; from about 1 mol % to about 3 mol % P2O5; from about 9 mol % to about 20 mol % Na2O; from 0 mol % to about 6 mol % MgO; and from 0 mol % to about 6 mol % ZnO.


In some embodiments, the composition may include the following compositional relationships R2O (mol %)/Al2O3 (mol %)<2, where R2O=Li2O+Na2O. In some embodiments, 65 mol %<SiO2 (mol %)+P2O5 (mol %)<67 mol %. In certain embodiments, R2O (mol %)+R′O (mol %)−Al2O3 (mol %)+P2O5 (mol %)>−3 mol %, where R2O=Li2O+Na2O and R′O is the total amount of divalent metal oxides present in the composition.


Other exemplary compositions of glass articles prior to being chemically strengthened, as described herein, are shown in Table 1.









TABLE 1





Exemplary compositions prior to chemical strengthening.





















Mol %
Ex. A
Ex. B
Ex. C
Ex. D
Ex. E
Ex. F





SiO2
71.8
69.8
69.8
69.8
69.8
69.8


Al2O3
13.1
13
13
13
13
13


B2O3
2
2.5
4
2.5
2.5
4


Li2O
8
8.5
8
8.5
8.5
8


MgO
3
3.5
3
3.5
1.5
1.5


ZnO
1.8
2.3
1.8
2.3
2.3
1.8


Na2O
0.4
0.4
0.4
0.4
0.4
0.4


TiO2
0
0
0
1
1
1


Fe2O3
0
0
0
0.8
0.8
0.8


SnO2
0.1
0.1
0.1
0.1
0.1
0.1


















Mol %
Ex. G
Ex. H
Ex. I
Ex. J
Ex. K
Ex. L
Ex. M
Ex. N





SiO2
70.18
70.91
71.28
71.65
71.65
71.65
74.77
72.00


Al2O3
12.50
12.78
12.93
13.07
13.07
13.07
10.00
12.50


B2O3
1.91
1.95
1.98
2.00
2.00
2.00
1.99
2.00


Li2O
7.91
7.95
7.96
7.98
6.98
5.00
6.13
6.00


Na2O
4.43
2.43
1.42
0.41
1.41
3.40
3.97
0.50


MgO
2.97
2.98
2.99
3.00
3.00
3.00
2.94
2.10


ZnO
0.00
0.89
1.34
1.80
1.80
1.80
0.00
0.00


CaO
0.00
0.00
0.00
0.00
0.00
0.00
0.05
4.90


SnO2
0.10
0.10
0.10
0.10
0.10
0.10
0.10
0.10


Li2O/R2O
0.64
0.77
0.85
0.95
0.83
0.60
0.61
0.92


R2O—Al2O3
−0.16
−2.41
−3.54
−4.68
−4.68
−4.67
0.10
−6.00


RxO—Al2O3
2.81
1.47
0.79
0.12
0.12
0.13
3.09
1.00


MgO/RO
1.00
0.77
0.69
0.63
0.63
0.63
1.00
1.00


R2O
12.34
10.38
9.39
8.39
8.39
8.40
10.10
6.50


RO
2.97
3.88
4.34
4.79
4.79
4.79
2.99
7.00









Other exemplary compositions of glass-based articles prior to being chemically strengthened, as described herein, are shown in Table 1A. Table 1B lists selected physical properties determined for the examples listed in Table 1A. The physical properties listed in Table 1B include: density; low temperature and high temperature CTE; strain, anneal and softening points; 1011 Poise, 35 kP, 200 kP, liquidus, and zircon breakdown temperatures; zircon breakdown and liquidus viscosities; Poisson's ratio; Young's modulus; refractive index, and stress optical coefficient. In some embodiments, the glass-based articles and glass substrates described herein have a high temperature CTE of less than or equal to 30 ppm/° C. and/or a Young's modulus of at least 70 GPa and, in some embodiments, a Young's modulus of up to 80 GPa.









TABLE 1A





Exemplary compositions prior to chemical strengthening.






















Composition









(mol %)
Ex. 1
Ex. 2
Ex. 3
Ex. 4
Ex. 5
Ex. 6
Ex. 7





SiO2
63.77
64.03
63.67
63.91
64.16
63.21
63.50


Al2O3
12.44
12.44
11.83
11.94
11.94
11.57
11.73


P2O5
2.43
2.29
2.36
2.38
1.92
1.93
1.93


Li2O
0.00
0.00
0.00
0.00
0.00
0.00
0.00


Na2O
16.80
16.81
16.88
16.78
16.80
17.63
16.85


ZnO
0.00
4.37
0.00
4.93
0.00
5.59
5.93


MgO
4.52
0.02
5.21
0.02
5.13
0.02
0.01


SnO2
0.05
0.05
0.05
0.05
0.05
0.05
0.05


R2O/Al2O3
1.35
1.35
1.43
1.41
1.41
1.52
1.44


Li2O/Na2O
0.00
0.00
0.00
0.00
0.00
0.00
0.00


(R2O +
6.45
6.46
7.89
7.40
8.07
9.74
9.14


RO)—Al2O3—P2O5





Composition









(mol %)
Ex. 8
Ex. 9
Ex. 10
Ex. 11
Ex. 12
Ex. 13
Ex. 14





SiO2
63.37
63.43
63.56
63.58
63.66
63.62
63.67


Al2O3
11.72
12.49
12.63
12.59
12.91
12.85
12.89


P2O5
2.00
2.32
2.46
2.46
2.43
2.45
2.47


Li2O
0.00
0.00
1.42
2.87
0.00
1.42
2.92


Na2O
16.84
17.16
15.45
14.04
16.89
15.48
13.92


ZnO
6.00
4.54
4.43
4.41
4.04
4.12
4.06


MgO
0.02
0.02
0.02
0.02
0.02
0.02
0.02


SnO2
0.05
0.04
0.05
0.05
0.05
0.05
0.05


R2O/Al2O3
1.44
1.37
1.34
1.34
1.31
1.31
1.31


Li2O/Na2O
0.00
0.00
0.09
0.20
0.00
0.09
0.21


(R2O +
9.14
6.90
6.22
6.29
5.62
5.72
5.57


RO)—Al2O3—P2O5





Composition









(mol %)
Ex. 15
Ex. 16
Ex. 17
Ex. 18
Ex. 19
Ex. 20
Ex. 21





SiO2
63.55
63.80
63.76
63.88
63.74
64.03
63.68


Al2O3
12.92
12.90
12.95
13.48
13.37
13.26
13.19


P2O5
2.35
2.34
2.37
2.31
2.34
2.29
2.46


Li2O
0.00
1.47
2.94
0.00
1.48
2.94
0.00


Na2O
17.97
16.36
14.85
17.20
15.96
14.37
16.84


ZnO
0.00
0.00
0.00
0.00
0.00
0.00
3.77


MgO
3.17
3.08
3.09
3.08
3.08
3.06
0.02


SnO2
0.05
0.04
0.05
0.05
0.04
0.04
0.05


R2O/Al2O3
1.39
1.38
1.37
1.28
1.30
1.31
1.28


Li2O/Na2O
0.00
0.09
0.20
0.00
0.09
0.20
0.00


(R2O +
5.87
5.67
5.56
4.48
4.81
4.83
4.98


RO)—Al2O3—P2O5





Composition









(mol %)
Ex. 22
Ex. 23
Ex. 24
Ex. 25
Ex. 26
Ex. 27
Ex. 28





SiO2
63.66
63.76
63.67
63.73
63.73
63.64
63.76


Al2O3
14.15
15.31
13.87
14.82
12.93
16.62
16.59


P2O5
2.47
2.44
2.47
2.43
2.48
2.47
2.47


Li2O
1.49
2.98
1.50
2.96
0.00
2.52
4.91


Na2O
15.31
13.79
15.36
13.93
16.83
14.68
12.20


ZnO
2.85
1.64
0.00
0.00
2.98
0.00
0.00


MgO
0.03
0.03
3.09
2.08
1.00
0.03
0.03


SnO2
0.05
0.04
0.05
0.05
0.05
0.05
0.05


R2O/Al2O3
1.19
1.10
1.22
1.14
1.30
1.03
1.03


Li2O/Na2O
0.10
0.22
0.10
0.21
0.00
0.17
0.40


(R2O +
3.05
0.70
3.61
1.72
5.40
−1.86
−1.92


RO)—Al2O3—P2O5





Composition









(mol %)
Ex. 29
Ex. 30
Ex. 31
Ex. 32
Ex. 33
Ex. 34
Ex. 35





SiO2
63.89
63.92
63.77
63.73
63.70
63.65
63.87


Al2O3
16.55
15.29
15.27
15.30
15.27
15.22
15.29


P2O5
2.47
2.24
2.31
2.39
2.40
2.48
2.37


Li2O
7.27
3.46
2.98
4.02
4.46
4.96
5.39


Na2O
9.74
13.46
13.99
12.91
12.51
11.99
11.44


ZnO
0.00
1.56
1.61
1.57
1.58
1.63
1.57


MgO
0.03
0.02
0.02
0.03
0.03
0.02
0.02


SnO2
0.04
0.04
0.04
0.05
0.04
0.05
0.04


R2O/Al2O3
1.03
1.11
1.11
1.11
1.11
1.11
1.10


Li2O/Na2O
0.75
0.26
0.21
0.31
0.36
0.41
0.47


(R2O +
−1.98
0.97
1.01
0.84
0.90
0.91
0.76


RO)—Al2O3—P2O5





Composition









(mol %)
Ex. 36
Ex. 37
Ex. 38
Ex. 39
Ex. 40
Ex. 41
Ex. 42





SiO2
63.69
63.75
63.70
63.62
63.74
63.77
63.77


Al2O3
15.26
15.30
15.27
15.23
15.27
15.27
15.33


P2O5
2.45
2.42
2.45
2.46
2.47
2.46
2.44


Li2O
2.96
2.98
3.94
3.98
4.93
4.93
2.91


Na2O
13.50
13.46
12.54
12.57
11.49
11.50
13.94


ZnO
2.06
2.01
2.03
2.06
2.03
2.00
0.00


MgO
0.02
0.03
0.02
0.03
0.03
0.03
1.57


SnO2
0.05
0.04
0.04
0.05
0.04
0.05
0.04


R2O/Al2O3
1.08
1.08
1.08
1.09
1.08
1.08
1.10


Li2O/Na2O
0.22
0.22
0.31
0.32
0.43
0.43
0.21


(R2O +
0.83
0.77
0.80
0.95
0.73
0.73
0.66


RO)—Al2O3—P2O5





Composition









(mol %)
Ex. 43
Ex. 44
Ex. 45
Ex. 46
Ex. 47
Ex. 48
Ex. 49





SiO2
63.69
63.81
63.65
63.71
63.62
63.65
63.62


Al2O3
15.25
15.26
15.33
15.32
15.24
15.68
15.67


P2O5
2.43
2.41
2.46
2.44
2.47
2.44
2.48


Li2O
4.00
4.89
2.96
4.01
4.91
6.07
6.06


Na2O
13.01
12.03
13.29
12.25
11.42
10.93
10.53


ZnO
0.00
0.00
2.24
2.20
2.27
1.17
1.57


MgO
1.57
1.56
0.03
0.03
0.02
0.02
0.02


SnO2
0.05
0.04
0.05
0.04
0.05
0.04
0.05


R2O/Al2O3
1.12
1.11
1.06
1.06
1.07
1.08
1.06


Li2O/Na2O
0.31
0.41
0.22
0.33
0.43
0.56
0.58


(R2O +
0.90
0.81
0.73
0.73
0.91
0.08
0.04


RO)—Al2O3—P2O5





Composition









(mol %)
Ex. 50
Ex. 51
Ex. 52
Ex. 53
Ex. 54
Ex. 55
Ex. 56





SiO2
63.60
63.89
63.84
63.90
63.88
64.74
60.17


Al2O3
15.65
16.09
16.47
16.87
16.97
15.25
18.58


P2O5
2.46
2.42
2.43
2.43
2.42
0.98
1.90


Li2O
6.13
6.80
7.84
8.75
9.78
5.28
5.16


Na2O
10.29
9.97
8.96
7.99
6.88
12.09
12.58


ZnO
1.81
0.78
0.39
0.00
0.00
1.61
1.55


MgO
0.02
0.02
0.02
0.02
0.02
0.02
0.02


SnO2
0.04
0.04
0.04
0.04
0.04
0.03
0.03


R2O/Al2O3
1.05
1.04
1.02
0.99
0.98
1.14
0.96


Li2O/Na2O
0.60
0.68
0.87
1.10
1.42
0.44
0.41


(R2O +
0.14
−0.94
−1.68
−2.54
−2.70
2.78
−1.16


RO)—Al2O3—P2O5





Composition






















(mol %)
Ex. 57
Ex. 58
Ex. 59
Ex. 60
Ex. 61
Ex. 62
Ex. 63
Ex. 64





SiO2
58.32
63.3
63.3
63.3
63.3
63.3
63.3
63.46


Al2O3
18.95
15.25
15.65
16.2
15.1
15.425
15.7
15.71


P2O5
2.42
2.5
2.5
2.5
2.5
2.5
2.5
2.45


Li2O
4.96
6
7
7.5
6
7
7.5
6.37


Na2O
13.74
10.7
9.7
9.45
10.55
9.475
8.95
10.69


ZnO
1.56
1.2
0.8
0
2.5
2.25
2
1.15


MgO
0.02
1
1
1
0
0
0
0.06


SnO2
0.03
0.05
0.05
0.05
0.05
0.05
0.05
0.04


R2O/Al2O3
0.99
1.10
1.07
1.05
1.10
1.07
1.05
1.09


Li2O/Na2O
0.36
0.56
0.72
0.79
0.57
0.74
0.84
0.6


(R2O +
−1.09
1.15
0.35
−0.75
1.45
0.80
0.25
−1.1


RO)—Al2O3—P2O5
























TABLE 1B





Selected physical properties of the glasses listed in Table 1B.























Ex. 1
Ex. 2
Ex. 3
Ex. 4
Ex. 5
Ex. 6
Ex. 7





Density (g/cm3)
2.434
2.493
2.434
2.504
2.44
2.514
2.519


Low
8.9
8.62
8.95
8.6
8.82
8.71
8.54


temperature









CTE









25-300° C.









(ppm/° C.)









High
17.67
19.1
17.16
21
18.12
20
20.11


temperature









CTE (ppm/° C.)









Strain pt. (° C.)
630
591
612
580
605
580
589


Anneal pt. (° C.)
683
641
662
628
651
629
639


1011 Poise
770
725
748
710
734
711
721


temperature









(° C.)









Softening pt.
937
888
919
873
909
868
874


(° C.)









T35 kP (° C.)



1167
1180
1158
1160


T200 kP (° C.)



1070
1083
1061
1064


Zircon

1205

1220
1170
1185
1205


breakdown









temperature









(° C.)









Zircon



1.56 × 104
4.15 × 104
2.29 × 104
1.74 × 104


breakdown









viscosity (P)









Liquidus

980

990
975
990
1000


temperature









(° C.)









Liquidus



1.15 × 106
2.17 × 106
9.39 × 105
7.92 × 105


viscosity (P)









Poisson's ratio
0.200
0.211
0.206
0.214
0.204
0.209
0.211


Young's
69.2
68.8
69.4
68.5
69.6
68.3
69.0


modulus (GPa)









Refractive
1.4976
1.5025
1.4981
1.5029
1.4992
1.5052
1.506


index at 589.3









nm









Stress optical
2.963
3.158
3.013
3.198
2.97
3.185
3.234


coefficient









(nm/mm/MPa)






Ex. 8
Ex. 9
Ex. 10
Ex. 11
Ex. 12
Ex. 13
Ex. 14





Density (g/cm3)
2.516
2.501
2.498
2.493
2.493
2.492
2.486


Low
8.35
8.67
8.87
8.49
8.65
8.71
8.49


temperature









CTE









25-300° C.









(ppm/° C.)









High
20.11
20.6
20.94

19.52
20.77



temperature









CTE (ppm/° C.)









Strain pt. (° C.)
590
589
591
584
600
579
588


Anneal pt.
641
639
640
628
652
620
630


(° C.)









1011 Poise
726
724
720
704
738
695
704


temperature









(° C.)









Softening pt.
888
890
865
857
900
867
860


(° C.)









T35 kP (° C.)
1170
1176
1159
1139
1197
1169



T200 kP (° C.)
1073
1080
1061
1041
1099
1070



Zircon
1195
1195
1210
1225
1195
1195
1220


breakdown









temperature









(° C.)









Zircon
2.33 × 104
2.58 × 104
1.60 × 104
9.94 × 103
3.63 × 104
2.35 × 104



breakdown









viscosity (P)









Liquidus
1005
990
990
980
990
980
980


temperature









(° C.)









Liquidus
8.69 × 104
1.48E+06
9.02E+05
7.10E+05
2.19E+06
1.33E+06



viscosity (P)









Poisson's ratio
0.211
0.205
0.208
0.209
0.209
0.210
0.217


Young's
69.0
68.7
71.4
73.5
68.4
71.6
74.0


modulus (GPa)









Refractive
1.506
1.5036
1.505
1.5063
1.5026
1.5041
1.5052


index at 589.3









nm









Stress optical
3.234
3.194
3.157
3.131
3.18
3.156
3.131


coefficient









(nm/mm/MPa)






Ex. 15
Ex. 16
Ex. 17
Ex. 18
Ex. 19
Ex. 20
Ex. 21





Density (g/cm3)
2.433
2.429
2.426
2.431
2.428
2.433
2.486


Low
9.15
9.16
8.83
8.97
8.97
8.79
8.45


temperature









CTE









25-300° C.









(ppm/° C.)









High
20
20
21
17.3
20




temperature









CTE (ppm/° C.)









Strain pt. (° C.)
615
606
599
633
616
611
602


Anneal pt. (° C.)
662
659
653
684
670
665
653


1011 Poise
747
745
741
771
758
751
739


temperature









(° C.)









Softening pt.
935
903
901
943
918
905
910


(° C.)









T35 kP (° C.)
1182
1166
1152
1221
1185
1167
1207


T200 kP (° C.)
1083
1066
1051
1122
1084
1066
1108


Zircon









breakdown









temperature









(° C.)









Zircon









breakdown









viscosity (P)









Liquidus









temperature









(° C.)









Liquidus









viscosity (P)









Poisson's ratio
0.203
0.207
0.205
0.209
0.199

0.207


Young's
68.9
71.2
72.7
69.4
70.9

68.1


modulus (GPa)









Refractive
1.4964
1.4981
1.4991
1.4965
1.4984
1.5006
1.5019


index at 589.3









nm









Stress optical
2.994
3.022
2.982
2.979
2.99
0
3.173


coefficient









(nm/mm/MPa)






Ex. 22
Ex. 23
Ex. 24
Ex. 25
Ex. 26
Ex. 27
Ex. 28





Density (g/cm3)
2.468
2.448
2.434
2.428
2.47
2.419
2.414


Low
8.6
8.23
8.91
8.25
8.66
8.52
8.17


temperature









CTE









25-300° C.









(ppm/° C.)









High
19.52

19.49



19.47


temperature









CTE (ppm/° C.)









Strain pt. (° C.)
596
595
638
616
608
640
620


Anneal pt.
644
649
695
656
654
700
677


(° C.)









1011 Poise
728
741
785
732
736
798
771


temperature









(° C.)









Softening pt.
905
922
941
925
911
978
946


(° C.)









T35 kP (° C.)
1217
1227
1209
1215
1209
1283
1249


T200 kP (° C.)
1115
1125
1109
1115
1107
1184
1150


Zircon
1185
1185
1180
1185


1185


breakdown









temperature









(° C.)









Zircon
5.86E+04
6.91E+04
5.59E+04
5.72E+04


1.05E+05


breakdown









viscosity (P)









Liquidus
975
980
1080
1025


940


temperature









(° C.)









Liquidus
4.14E+06
4.52E+06
3.56E+05
1.27E+06


2.92E+07


viscosity (P)









Poisson's ratio
0.210

0.204
0.210
0.212

0.213


Young's
71.4

71.6
73.5
68.8

76.9


modulus (GPa)









Refractive
1.502
1.5025
1.4996
1.5008
1.5006
1.4987
1.5014


index at 589.3









nm









Stress optical
3.123
3.03
3.001
3.021
3.148
3.039
3.015


coefficient









(nm/mm/MPa)






Ex. 29
Ex. 30
Ex. 31
Ex. 32
Ex. 33
Ex. 34
Ex. 35





Density (g/cm3)
2.408
2.446
2.448
2.446
2.445
2.443
2.442


Low
7.86
8.29
8.38
8.17
8.14
8.04
7.97


temperature









CTE









25-300° C.









(ppm/° C.)









High
18.57




19.71



temperature









CTE (ppm/° C.)









Strain pt. (° C.)
610
591
595
585
580
574
577


Anneal pt.
665
645
649
638
633
627
629


(° C.)









1011 Poise
755
736
740
726
722
717
717


temperature









(° C.)









Softening pt.
924
915
919
894
894
895
890


(° C.)









T35 kP (° C.)
1216
1223
1227
1216
1210
1203
1196


T200 kP (° C.)
1120
1122
1126
1114
1108
1102
1095


Zircon
1210
1175
1180
1190
1195
1210
1205


breakdown









temperature









(° C.)









Zircon
3.86E+04
7.72E+04
7.55E+04
5.29E+04
4.43E+04
3.14E+04
3.04E+04


breakdown









viscosity (P)









Liquidus
1080
990
975
975
975
975
980


temperature









(° C.)









Liquidus
4.55E+05
3.28E+06
5.43E+06
3.80E+06
3.33E+06
3.02E+06
2.29E+06


viscosity (P)









Poisson's ratio
0.211
0.206
0.202
0.21
0.204
0.204
0.203


Young's
75.0
73.91
73.02
74.60
74.67
75.15
75.43


modulus (GPa)









Refractive
1.5053
1.503
1.5025
1.5035
1.5041
1.5046
1.5053


index at 589.3









nm









Stress optical
3.002
3.074
3.083
3.071
3.059
3.016
3.053


coefficient









(nm/mm/MPa)






Ex. 36
Ex. 37
Ex. 38
Ex. 39
Ex. 40
Ex. 41
Ex. 42





Density (g/cm3)
2.453
2.453
2.452
2.451
2.449
2.449
2.425


Low
8.17
8.14
7.97
8.01
7.79
7.9
8.54


temperature









CTE









25-300° C.









(ppm/° C.)









High




20.56




temperature









CTE (ppm/° C.)









Strain pt. (° C.)
595
595
584
587
578
584
617


Anneal pt. (° C.)
649
649
638
640
630
637
663


1011 Poise
740
741
729
730
718
726
746


temperature









(° C.)









Softening pt.
918
921
905
907
894
901
929


(° C.)









T35 kP (° C.)
1229
1232
1212
1219
1200
1204
1232


T200 kP (° C.)
1128
1131
1111
1118
1100
1103
1132


Zircon
1185

1200

1210




breakdown









temperature









(° C.)









Zircon
7.20E+04

4.26E+04

3.00E+04




breakdown









viscosity (P)









Liquidus
995

990

965




temperature









(° C.)









Liquidus
3.33E+06

2.51E+06

3.71E+06




viscosity (P)









Poisson's ratio
0.208

0.206

0.206




Young's
73.70

74.67

75.50




modulus (GPa)









Refractive
1.5032

1.5042

1.5054

1.5005


index at 589.3









nm









Stress optical
3.093

3.071

3.072

3.033


coefficient









(nm/mm/MPa)



















Ex. 43
Ex. 44
Ex. 45
Ex. 46
Ex. 47
Ex. 48
Ex. 49
Ex. 50





Density (g/cm3)
2.424
2.422
2.455
2.454
2.454
2.434
2.439
2.443


Low
8.48
8.34
8.03
7.88
7.76
7.87
7.71
7.63


temperature










coefficient of










thermal










expansion










25-300° C.










(ppm/° C.)










High










temperature










coefficient of










thermal










expansion










(ppm/° C.)










Strain pt.
614
594
595
586
579
580
581
579


temperature










(° C.)










Anneal pt.
659
640
649
639
630
633
633
632


temperature










(° C.)










1011 Poise
739
722
740
729
718
722
721
721


temperature










(° C.)










Softening pt.
912
899
918
909
898
892
893
895


temperature










(° C.)










35 kP
1216
1204

1212
1200
1203
1203
1203


temperature










(° C.)










200 kP
1116
1102

1113
1099
1105
1102
1103


temperature










(° C.)










Zircon










breakdown










temperature










(° C.)










Zircon










breakdown










viscosity (P)










Liquidus


985

965
1005
1010
1030


temperature










(° C.)










Liquidus




 4.E+06
1.78E+06
1.34E+06
8.98E+05


viscosity (P)










Poisson's ratio





0.211
0.21
0.213


Young's





76.32
76.60
76.81


modulus (GPa)










Refractive
1.5014
1.5026
1.5036
1.5047
1.5061
1.505
1.5059
1.5064


index at 589.3










nm










Stress optical
2.965
2.981
3.082
3.057
3.063
3.025
3.004
3.046


coefficient










(nm/mm/MPa)


















Ex. 51
Ex. 52
Ex. 53
Ex. 54
Ex. 55
Ex. 56
Ex. 57





Density (g/cm3)
2.424
2.431
2.403
2.4
2.45
2.462
2.468


Low
77.1
76.1
74.3
73.1
80.2
79.7
83.6


temperature









CTE









25-300° C.









(ppm/° C.)









High









temperature









CTE (ppm/° C.)









Strain pt. (° C.)
588
599
611
612
580
611
597


Anneal pt.
640
651
665
665
631
663
649


(° C.)









1011 Poise
728
738
753
752
718
750
735


temperature









(° C.)









Softening pt.
900.4
907.5
916
912.5
892.2
915.6
899.4


(° C.)









T35 kP (° C.)
1204
1209
1209
1202
1206
1205
1184


T200 kP (° C.)
1106
1113
1113
1106
1102
1111
1093















Zircon










breakdown










temperature










(° C.)










Zircon










breakdown










viscosity (P)










Liquidus
1060
1115
1160
1205






temperature










(° C.)










Liquidus
5.11E+05
1.90E+05
8.18E+04
3.32E+04






viscosity (P)










Poisson's ratio
0.211
0.212
0.208
0.214






Young's
77.01
78.05
77.57
78.74






modulus (GPa)










Refractive
1.5054
1.5055
1.5059
1.5072






index at 589.3










nm










Stress optical
3.011
2.98
2.982
2.964






coefficient










(nm/mm/MPa)
















Ex. 64









Density (g/cm3)
2.428






CTE 25-300° C. (ppm/° C.)
7.8






Strain pt. (° C.)
571






Anneal pt. (° C.)
622






1011 Poise temperature (° C.)







Softening pt. (° C.)
881.4






T35 kP (° C.)







T200 kP (° C.)
1645






Zircon breakdown temperature (° C.)







Zircon breakdown viscosity (P)







Liquidus temperature (° C.)
1000






Liquidus viscosity (P)
1524280






Poisson's ratio
0.211






Young's modulus (GPa)
76.3






Refractive index at 589.3 nm
1.51






Stress optical coefficient (nm/mm/MPa)
3.02









Where the glass article includes a glass-ceramic, the crystal phases may include β-spodumene, rutile, gahnite or other known crystal phases and combinations thereof.


The glass article may be substantially planar, although other embodiments may utilize a curved or otherwise shaped or sculpted substrate. In some instances, the glass article may have a 3D or 2.5D shape. The glass article may be substantially optically clear, transparent and free from light scattering. The glass article may have a refractive index in the range from about 1.45 to about 1.55. As used herein, the refractive index values are with respect to a wavelength of 550 nm.


Additionally or alternatively, the thickness of the glass article may be constant along one or more dimension or may vary along one or more of its dimensions for aesthetic and/or functional reasons. For example, the edges of the glass article may be thicker as compared to more central regions of the glass article. The length, width and thickness dimensions of the glass article may also vary according to the article application or use.


The glass article may be characterized by the manner in which it is formed. For instance, where the glass article may be characterized as float-formable (i.e., formed by a float process), down-drawable and, in particular, fusion-formable or slot-drawable (i.e., formed by a down draw process such as a fusion draw process or a slot draw process).


A float-formable glass article may be characterized by smooth surfaces and uniform thickness is made by floating molten glass on a bed of molten metal, typically tin. In an example process, molten glass that is fed onto the surface of the molten tin bed forms a floating glass ribbon. As the glass ribbon flows along the tin bath, the temperature is gradually decreased until the glass ribbon solidifies into a solid glass article that can be lifted from the tin onto rollers. Once off the bath, the glass article can be cooled further and annealed to reduce internal stress. Where the glass article is a glass ceramic, the glass article formed from the float process may be subjected to a ceramming process by which one or more crystalline phases are generated.


Down-draw processes produce glass articles having a uniform thickness that possess relatively pristine surfaces. Because the average flexural strength of the glass article is controlled by the amount and size of surface flaws, a pristine surface that has had minimal contact has a higher initial strength. When this high strength glass article is then further strengthened (e.g., chemically), the resultant strength can be higher than that of a glass article with a surface that has been lapped and polished. Down-drawn glass articles may be drawn to a thickness of less than about 2 mm. In addition, down drawn glass articles have a very flat, smooth surface that can be used in its final application without costly grinding and polishing. Where the glass article is a glass ceramic, the glass article formed from the down draw process may be subjected to a ceramming process by which one or more crystalline phases are generated.


The fusion draw process, for example, uses a drawing tank that has a channel for accepting molten glass raw material. The channel has weirs that are open at the top along the length of the channel on both sides of the channel. When the channel fills with molten material, the molten glass overflows the weirs. Due to gravity, the molten glass flows down the outside surfaces of the drawing tank as two flowing glass films. These outside surfaces of the drawing tank extend down and inwardly so that they join at an edge below the drawing tank. The two flowing glass films join at this edge to fuse and form a single flowing glass article. The fusion draw method offers the advantage that, because the two glass films flowing over the channel fuse together, neither of the outside surfaces of the resulting glass article comes in contact with any part of the apparatus. Thus, the surface properties of the fusion drawn glass article are not affected by such contact. Where the glass article is a glass ceramic, the glass article formed from the fusion process may be subjected to a ceramming process by which one or more crystalline phases are generated.


The slot draw process is distinct from the fusion draw method. In slow draw processes, the molten raw material glass is provided to a drawing tank. The bottom of the drawing tank has an open slot with a nozzle that extends the length of the slot. The molten glass flows through the slot/nozzle and is drawn downward as a continuous glass article and into an annealing region. Where the glass article is a glass ceramic, the glass article formed from the slot draw process may be subjected to a ceramming process by which one or more crystalline phases are generated.


In some embodiments, the glass article may be formed using a thin rolling process, as described in U.S. Pat. No. 8,713,972, entitled “Precision Glass Roll Forming Process and Apparatus”, U.S. Pat. No. 9,003,835, entitled “Precision Roll Forming of Textured Sheet Glass”, U.S. Patent Publication No. 20150027169, entitled “Methods And Apparatus For Forming A Glass Ribbon”, and U.S. Patent Publication No. 20050099618, entitled “Apparatus and Method for Forming Thin Glass Articles”, the contents of which are incorporated herein by reference in their entirety. More specifically the glass article may be formed by supplying a vertical stream of molten glass, forming the supplied stream of molten glass or glass-ceramic with a pair of forming rolls maintained at a surface temperature of about 500° C. or higher or about 600° C. or higher to form a formed glass ribbon having a formed thickness, sizing the formed ribbon of glass with a pair of sizing rolls maintained at a surface temperature of about 400° C. or lower to produce a sized glass ribbon having a desired thickness less than the formed thickness and a desired thickness uniformity. The apparatus used to form the glass ribbon may include a glass feed device for supplying a supplied stream of molten glass; a pair of forming rolls maintained at a surface temperature of about 500° C. or higher, the forming rolls being spaced closely adjacent each other defining a glass forming gap between the forming rolls with the glass forming gap located vertically below the glass feed device for receiving the supplied stream of molten glass and thinning the supplied stream of molten glass between the forming rolls to form a formed glass ribbon having a formed thickness; and a pair of sizing rolls maintained at a surface temperature of about 400° C. or lower, the sizing rolls being spaced closely adjacent each other defining a glass sizing gap between the sizing rolls with the glass sizing gap located vertically below the forming rolls for receiving the formed glass ribbon and thinning the formed glass ribbon to produce a sized glass ribbon having a desired thickness and a desired thickness uniformity.


In some instances, the thin rolling process may be utilized where the viscosity of the glass does not permit use of fusion or slot draw methods. For example, thin rolling can be utilized to form the glass articles when the glass exhibits a liquidus viscosity less than 100 kP.


The glass article may be acid polished or otherwise treated to remove or reduce the effect of surface flaws.


Another aspect of this disclosure pertains to a method of forming a fracture-resistant glass article. The method includes providing a glass substrate having a first surface and a second surface defining a thickness of about 1 millimeter or less and generating a stress profile in the glass substrate, as described herein to provide the fracture-resistant glass article. In one or more embodiments, generating the stress profile comprises ion exchanging a plurality of alkali ions into the glass substrate to form an alkali metal oxide concentration gradient comprising a non-zero concentration of alkali metal oxide extending along the thickness. In one example, generating the stress profile includes immersing the glass substrate in a molten salt bath including nitrates of Na+, K+, Rb+, Cs+ or a combination thereof, having a temperature of about 350° C. or greater (e.g., about 350° C. to about 500° C.). In one example, the molten bath may include NaNO3 and may have a temperature of about 485° C. In another example, the bath may include NaNO3 and have a temperature of about 430° C. The glass substrate may be immersed in the bath for about 2 hours or more, up to about 48 hours (e.g., from about 12 hours to about 48 hours, from about 12 hours to about 32 hours, from about 16 hours to about 32 hours, from about 16 hours to about 24 hours, or from about 24 hours to about 32 hours).


In some embodiments, the method may include chemically strengthening or ion exchanging the glass substrate in more than one step using successive immersion steps in more than one bath. For example, two or more baths may be used successively. The composition of the one or more baths may include a single metal (e.g., Ag+, Na+, K+, Rb+, or Cs+) or a combination of metals in the same bath. When more than one bath is utilized, the baths may have the same or different composition and/or temperature as one another. The immersion times in each such bath may be the same or may vary to provide the desired stress profile.


In one or more embodiments, a second bath or subsequent baths may be utilized to generate a greater surface CS. In some instances, the method includes immersing the glass material in the second or subsequent baths to generate a greater surface CS, without significantly influencing the chemical depth of layer and/or the DOC. In such embodiments, the second or subsequent bath may include a single metal (e.g., KNO3 or NaNO3) or a mixture of metals (KNO3 and NaNO3). The temperature of the second or subsequent bath may be tailored to generate the greater surface CS. In some embodiments, the immersion time of the glass material in the second or subsequent bath may also be tailored to generate a greater surface CS without influencing the chemical depth of layer and/or the DOC. For example, the immersion time in the second or subsequent baths may be less than 10 hours (e.g., about 8 hours or less, about 5 hours or less, about 4 hours or less, about 2 hours or less, about 1 hour or less, about 30 minutes or less, about 15 minutes or less, or about 10 minutes or less).


In one or more alternative embodiments, the method may include one or more heat treatment steps which may be used in combination with the ion-exchanging processes described herein. The heat treatment includes heat treating the glass article to obtain a desired stress profile. In some embodiments, heat treating includes annealing, tempering or heating the glass material to a temperature in the range from about 300° C. to about 600° C. The heat treatment may last for 1 minute up to about 18 hours. In some embodiments, the heat treatment may be used after one or more ion-exchanging processes, or between ion-exchanging processes.


EXAMPLES

Various embodiments will be further clarified by the following examples.


Example 1

Glass articles according to Examples 1A-1B and Comparative Examples 1C-1G were made by providing glass substrates having a nominal glass composition of 58 mol % SiO2, 16.5 mol % Al2O3, 17 mol % Na2O, 3 mol % MgO, and 6.5 mol P2O5. The glass substrates had a thickness of 0.4 mm and length and width dimensions of 50 mm. The glass substrates were chemically strengthened by an ion exchange process that included immersing in a molten salt bath of 80% KNO3 and 20% NaNO3 having a temperature of about 420° C. for the durations shown in Table 2. The resulting glass articles were then subjected to AROR testing as described above and by abrading a major surface of each of the samples using 90 grit SiC particles at a pressure of 5 psi, 15 psi or 25 psi, as also shown in Table 2. Table 2 shows the average equibiaxial flexural strength or failure load of the glass articles.









TABLE 2







Chemical strengthening conditions


and AROR results for Example 1.













At 5 psi
15 psi
25 psi



Ion Exchange
Average kgf
Average kgf
Average kgf


Ex.
Conditions
(stdev)
(stdev)
(stdev)





1C
420° C./4 hours 
49.4 (7.1)
17.4 (7.2)
 0.3 (0.9)


1D
420° C./8 hours 
49.9 (7.1)
36.5 (6.7)
19.3 (6.4)


1A
420° C./16 hours
47.5 (6.0)
38.3 (2.8)
30.0 (5.4)


1B
420° C./32 hours
36.9 (4.3)
30.9 (3.1)
26.2 (2.8)


1E
420° C./64 hours
18.7 (1.5)
15.3 (0.9)
13.5 (1.2)


1F
 420° C./128 hours
 5.9 (0.5)
 5.4 (0.3)
 4.5 (0.3)









The average equibiaxial flexural strength or failure load of the Examples after abrasion at 15 psi and 25 psi are plotted in FIG. 11. As shown in FIG. 11, Examples 1A and 1B exhibited the greatest average equibiaxial flexural strength after being abraded at 25 psi. Accordingly, the AROR performance of Examples 1A and 1B demonstrate that these glass articles exhibit a highly diced fracture pattern, which indicates improved retained strength, especially for deeper abrasion depths that result from higher abrasion pressures.


Example 2

Glass articles according to Examples 2A-2C and Comparative Examples 2D-2F were made by providing glass substrates and chemically strengthening the glass substrates. The glass substrates used for Examples 2A-2C and Comparative 2E-2F had a nominal glass composition of 69.2 mol % SiO2, 12.6 mol % Al2O3, 1.8 mol % B2O3, 7.7 mol % Li2O, 0.4 mol % Na2O, 2.9 mol % MgO, 1.7 mol % ZnO, 3.5 mol % TiO2 and 0.1 mol % SnO2. The substrate used for Comparative Example 2D had the same composition as Example 1.


The glass substrates had a thickness of 1 mm and length and width dimensions permitting assembly with a known mobile device housing. The glass substrates were chemically strengthened by the ion exchange processes shown in Table 3. The CT and DOC values for Examples 2A-2C were measured by SCALP and are also shown in Table 3.









TABLE 3







Ion exchange conditions and drop testing results for Example 2.














Molten Bath
Immersion





Molten Bath
Temperature
Time
CT
DOC


Example
Composition
(° C.)
(hours)
(MPa)
(μm)















Ex. 2A
100% NaNO3
430
24
128
160


Ex. 2B
100% NaNO3
430
29
153
200


Ex. 2C
100% NaNO3
430
33
139
200


Comp.







Ex. 2D







Comp.
100% NaNO3
390
3.5




Ex. 2E







Comp.
100% NaNO3
430
48




Ex. 2F









Comparative Example 2D was ion exchanged to exhibit an error function stress profile with a DOC exceeding 75 micrometers (as measured by Roussev I applying IWKB analysis). The resulting glass articles were then retrofitted to identical mobile device housings and subjected to drop testing as described above onto 30 grit sand paper. FIG. 12 shows the maximum failure height for the Examples. As shown in FIG. 12, Examples 2A-2C exhibited significantly greater maximum failure heights (i.e., 212 cm, 220 cm, and 220 cm, respectively) and exhibited dicing behavior. Example 2F, which has the same composition, did not exhibit the same dicing behavior and exhibited a lower maximum failure height, as compared to Examples 2A-2C.


Example 3

Glass articles according to Examples 3A-3K and Comparative Examples 3L-3X were made by providing glass substrates and strengthening the glass substrates. The substrates used for Examples 3A-3D had the same composition as Example 1 and the substrates used for Examples 3L-3X had a nominal glass composition of 69 mol % SiO2, 10.3 mol % Al2O3, 15.2 mol % Na2O, 5.4 mol % MgO, and 0.2 mol % SnO2.


The glass substrates had a thickness of 0.4 mm and length and width dimensions of 50 mm by 50 mm. The glass substrates were chemically strengthened by ion exchange. Examples 3A-3K were ion exchanged in a molten salt bath of 80% KNO3 and 20% NaNO3 having a temperature of 460° C. for 12 hours. Comparative Examples 3L-3X were ion exchanged such that each resulting glass article exhibits a surface CS of 912 MPa and a DOC of 37 μm, as measured by FSM.


The resulting glass articles were then subjected to fracture by impacting one major surface of each article with a tungsten carbide conospherical scribe for a single strike from a drop distance (as indicated in Tables 4 and 5) and assessing the breakage or fracture pattern in terms of how many fragments resulted, whether the glass article fractured immediately or did not fracture at all, and the frangibility of the glass article.









TABLE 4







Failure characteristics and fracture mechanics of Examples 3A-3K.













Strike
Fragment Count
Frangible
Drop Distance
Time to


Ex.
Count
(#)
(Y/N)
(inches)
fracture





3A
1
100+
Yes
0.611
Instant


3B
1
DNB
DNB
0.561
DNB


3C
1
DNB
DNB
0.511
DNB


3D
1
DNB
DNB
0.461
DNB


3E
1
DNB
DNB
0.411
DNB


3F
1
DNB
DNB
0.361
DNB


3G
1
DNB
DNB
0.311
DNB


3H
1
100+
Yes
0.261
Instant


3I
1
DNB
DNB
0.211
DNB


3J
1
DNB
DNB
0.161
DNB


3K
1
DNB
DNB
0.111
DNB





* DNB = did not break













TABLE 5







Failure characteristics and fracture mechanics


of Comparative Examples 3L-3X.













Strike
Fragment Count
Frangible
Drop Distance
Time to


Ex.
Count
(#)
(Y/N)
(inches)
fracture





3L
1
9
No
0.226
Instant


3M
1
7
No
0.221
Instant


3N
1
5
Yes
0.216
30 seconds


3O
1
6
Yes
0.211
30 seconds


3P
1
2
No
0.206
30 seconds


3Q
1
7
Yes
0.201
1 minute


3R
1
DNB
DNB
0.196
DNB


3S
1
5
Yes
0.191
30 seconds


3T
1
6
Yes
0.186
10 seconds


3U
1
9
Yes
0.181
10 seconds


3V
1
6
Yes
0.176
15 seconds


3W
1
10+
Yes
0.171
10 seconds


3X
1
8
Yes
0.111
30 seconds





* DNB = did not break






As shown in Tables 4-5, it is clear that glass articles chemically strengthened to a condition near the frangibility limit (i.e., Comparative Examples 3L-3X) are much more likely to experience a delayed failure, when compared to glass articles that were chemically strengthened to a condition a high degree of dicing/fragmentation occurs upon fracture (i.e., Examples 3A-3K). Specifically, more than 80% of Comparative Examples 3L-3X failed in a delayed manner, while the samples in Table 4 either failed immediately, or did not break. Moreover, Comparative Examples 3L-3X exhibited fewer, larger, more splintered fragments than Examples 3A-4K, which failed with a high degree of dicing and exhibited fragments with low aspect ratios.


Example 4

Glass articles according to Examples 4A-4B and Comparative Examples 4C-4F were made by providing glass substrates having the same nominal composition as Example 1 and strengthening the glass substrates. The glass substrates had a thickness of 0.4 mm and were chemically strengthened by an ion exchange process in which the glass substrates were immersed in a molten salt bath of 80% KNO3 and 20% NaNO3 having a temperature of 430° C. for the durations shown in Table 6.









TABLE 6







Ion exchange durations for Example 5.










Example
Immersion time (hours)













Example 4A
16



Example 4B
32



Comparative Ex. 4C
4



Comparative Ex. 4D
8



Comparative Ex. 4E
64



Comparative Ex. 4F
128









The concentration of K2O in the glass articles was measured using Glow-Discharge Optical Emission Spectroscopy (GDOES). In FIG. 13, the mol % (expressed as K2O) of the larger K+ ion that is replacing the smaller Na+ in the glass substrate is represented on the vertical axis, and plotted as a function of ion-exchange depth. Examples 4A and 4B exhibited a higher stored tensile energy (and central tension) than the other profiles, and maximize the DOC as well as the magnitude of the surface compression.



FIG. 14 shows the stress profile, as measured by Roussev I applying IWKB analysis, of Example 4G which was formed by providing the same substrate as Examples 4A and 4B but and immersing in a molten salt bath of 70% KNO3 and 30% NaNO3 having a temperature of 460° C. for 12 hours.


Example 5

Glass articles according to Examples 5A-5D (with Examples B and C being comparative) were made by providing glass substrates having the same nominal composition as Example 2A-2C and strengthening the glass substrates. The glass substrates were chemically strengthened by the ion exchange processes shown in Table 7.









TABLE 7







Ion exchange conditions for Example 5.












Molten Bath
Immersion



Molten Bath
Temperature
duration


Example
Composition
(° C.)
(hours)













5A
80% KNO3/20% NaNO3
460
12


Comparative 5B
65% KNO3/35% NaNO3
460
12


Comparative 5C
100% NaNO3
430
4


5D
100% NaNO3
430
16









Example 5A and Comparative Example 5B were adhered to a transparent substrate using a pressure sensitive adhesive supplied by 3M under the tradename 468MP, applied in the same manner and identical thicknesses. Example 5A and Comparative Example 5B were fractured and the resulting fractured glass articles were evaluated. FIGS. 15A and 15B show fracture images of Example 5A and Comparative Example 5B, respectively. As shown in FIG. 15A, Example 5A exhibited higher dicing behavior and resulted in fragments having an aspect ratio of less than about 2. As shown in FIG. 15B, Comparative Example 5B resulted in fragments having a higher aspect ratio.


Comparative Example 5C and Example 5D were not constrained by an adhesive and were fractured. The resulting fractured glass articles were evaluated. FIGS. 15C and 15D show fracture images of Comparative Example 5C and Example 5D, respectively. As shown in FIG. 15C, Comparative Example 5C exhibited larger fragments. As shown in FIG. 15D, Example 5D resulted in fragments indicating dicing. It is believed that the sub-fragments (not shown) did not extend through the thickness of the glass article.


Example 6

A glass article according to Example 6 was made by providing a glass substrate having the same nominal composition as Examples 3A-3K and strengthened in the same manner. Example 6 was evaluated for haze or readability after fracture, at different viewing angles. After fracture, Example 6 exhibited a high degree of dicing but still exhibited good readability at a 90° viewing angle, relative to the surface plane or major surface of the glass article. The readability drops as the viewing angle decreases, as illustrated by the images of FIGS. 16A-16D. FIG. 16A demonstrates text placed behind Example 6 is still visible and readable at a viewing angle of 90 degrees relative to the surface plane or major surface of the glass article. FIG. 16B shows the test is somewhat visible and readable at a viewing angle of about 67.5 degrees. The text is not clear or readable at viewing angles of 45 degrees and 22.5 degrees relative to the surface plane or major surface of the glass article, according to FIGS. 16C-16D. Accordingly, Example 6 can function as a privacy screen when used in a display such that only the viewer may read or see the display clearly, while others beside the viewer would not be able to read the display clearly.


Example 7

Glass articles according to Examples 7A-7C were made by providing glass substrates having a 2.5-dimensional shape but each having a different thickness (i.e., Example 7A had a thickness of 1 mm, Example 7B had a thickness of 0.8 mm and Example 7C had a thickness of 0.5 mm). A 2.5-dimensional shape includes a flat major surface and an opposite curved major surface. The composition of the glass substrates was the same as Examples 2A-2C. The stored tensile energy of each substrate was calculated as a function of ion exchange time using a molten bath having a temperature of 430° C. Stored tensile energy was calculated using the total amount of stress over the CT region (327 in FIG. 4) measured by SCALP. The calculated stored tensile energy was plotted as a function of ion exchange time in FIG. 17. For purposes of illustration, a dotted line at a stored tensile energy value of 10 J/m2 has been drawn to represent an approximate threshold for frangibility. The highlighted area represents the ion-exchange conditions for a single part having a thickness range from 0.5-1.0 mm that exhibit the behaviors described herein. Specifically, this range enables optimized mechanical performance and a similar degree of dicing across the area of the part, when and if the part fractures.


If known frangibility limits are used to determine the ion exchange parameters for various thicknesses, at Time A the ion exchange time where the stored tensile energy reaches below 10 J/m2, a glass substrate having a thickness of 1 mm would be non-frangible, and a glass substrate with a thickness of 0.5 mm would have low CS. At time C, a glass substrate having a thickness of 0.5 mm is non-frangible, and a glass substrate having a thickness between 1 mm and 0.8 mm regions would be considered frangible. Accordingly, when using the current definition of frangibility, FIG. 17 shows that one would choose an ion-exchange time in a given bath at a designated temperature that is significantly longer for a relatively thick part, or region of a non-uniformly thick part, than one would choose for a thinner part, or a thinner region, of an intentionally non-uniformly thick part. In order to provide a fully-finished 2.5D part that has substantially improved drop performance and reliability, and a relatively uniform degree of fragmentation, or dicing, it may be desirable to ion-exchange the part for a shorter period of time in order to install a higher degree of stored tensile energy than would choose to limit the degree of fragmentation or dicing.



FIG. 18 represents the samples shown in FIG. 17, except that the installed tensile energy represented in 11 is now represented as central tension (CT), which has been used as a more common descriptor of the tensile energy in the central region of the ion-exchanged specimens.


Example 8

Example 8 included a glass article made by providing a glass substrate having the same nominal composition as Example 1 and strengthening the glass substrate. The glass substrate had a thickness of 0.4 mm and was chemically strengthened by a two-step ion exchange process in which the glass substrate was first immersed in a first molten salt bath of 80% KNO3 and 20% NaNO3 having a temperature of 460° C. for 12 hours, removed from the first molten salt bath and immersed in a second molten salt bath of 100% KNO3 having a temperature of 390° C. for 12 minutes. The resulting glass article had a surface compressive stress of 624.5 MPa, a DOC of about 83.3 micrometers (which is equivalent to 0.208t) and a max CT of about 152.6 MPa, measured by Roussev I applying IWKB analysis. FIG. 19 shows the compressive stress (shown as negative values) and tensile stress (shown as positive values) as a function of depth in micrometers.


Aspect (1) of this disclosure pertains to a strengthened glass article comprising: a first surface and a second surface opposing the first surface defining a thickness (t) of about 1.1 mm or less; a compressive stress layer extending from the first surface to a depth of compression (DOC) of greater than about 0.11·t; wherein, after the glass article fractures according to a Frangibility Test, the glass article includes a plurality of fragments, wherein at least 90% of the plurality of fragments have an aspect ratio of about 5 or less.


Aspect (2) of this disclosure pertains to the strengthened glass article of Aspect (1), wherein the glass article fractures into the plurality of fragments in 1 second or less, as measured by the Frangibility Test.


Aspect (3) of this disclosure pertains to the strengthened glass article of Aspect (1) or Aspect (2), wherein at least 80% of the plurality of fragments have a maximum dimension that is less than or equal to 3·t.


Aspect (4) of this disclosure pertains to the strengthened glass article of any one of Aspects (1) through Aspect (3), wherein at least 50% of plurality of fragments comprises an aspect ratio of 2 or less.


Aspect (5) of this disclosure pertains to the strengthened glass article of anyone of Aspects (1) through Aspect (4), wherein at least 50% of the plurality of fragments comprises a volume of less than or equal to about 10 mm3.


Aspect (6) of this disclosure pertains to the strengthened glass article of any one of Aspects (1) through Aspect (5), wherein the plurality of fragments comprises an ejected portion of fragments, wherein the ejected portion of fragments comprises 10% or less of the plurality of fragments.


Aspect (7) of this disclosure pertains to the strengthened glass article of any one of Aspects (1) through Aspect (6), wherein the glass article comprises a first weight prior to fracture and the wherein the plurality of fragments comprises an ejected portion of fragments and a non-ejected portion of fragments, the non-ejected portion of fragments having a second weight, and the difference between the first weight and the second weight is 1% of the first weight.


Aspect (8) of this disclosure pertains to the strengthened glass article of any one of Aspects (1) through Aspect (7), wherein the probability of the glass article fracturing into the plurality of fragments within 1 second or less, as measured by a Frangibility Test, is 99% or greater.


Aspect (9) of this disclosure pertains to the strengthened glass article of any one of Aspects (1) through Aspect (8), wherein the glass article comprises a stored tensile energy of 20 J/m2 or greater.


Aspect (10) of this disclosure pertains to the strengthened glass article of anyone of Aspects (1) through Aspect (9), wherein the glass article comprises a surface compressive stress and a central tension, wherein the ratio of central tension to surface compressive stress is in the range from about 0.1 to about 1.


Aspect (11) of this disclosure pertains to the strengthened glass article of Aspect (10), wherein the central tension is 100 MPa/(t/1 mm) or greater (in units of MPa), wherein t is in mm.


Aspect (12) of this disclosure pertains to the strengthened glass article of anyone of Aspect (10) through Aspect (11), wherein the central tension is 50 MPa or greater.


Aspect (13) of this disclosure pertains to the strengthened glass article of anyone of Aspect (10) through Aspect (12), wherein the surface compressive stress is 150 MPa or greater.


Aspect (14) of this disclosure pertains to the strengthened glass article of anyone of Aspect (10) through Aspect (13), wherein the surface compressive stress is 400 MPa or greater.


Aspect (15) of this disclosure pertains to the strengthened glass article of anyone of Aspect (10) through Aspect (14), wherein the DOC comprises about 0.2t or greater.


Aspect (16) of this disclosure pertains to the strengthened glass article of anyone of Aspect (1) through Aspect (15), wherein the glass article comprises an alkali aluminosilicate glass, alkali containing borosilicate glass, an alkali aluminophosphosilicate glass or alkali aluminoborosilicate glass.


Aspect (17) of this disclosure pertains to the strengthened glass article of anyone of Aspect (1) through Aspect (16), wherein the glass article is disposed on a containment layer.


Aspect (18) of this disclosure pertains to a strengthened glass article comprising: a first surface and a second surface opposing the first surface defining a thickness (t) of about 1.1 mm or less; a compressive stress layer extending from the first surface to a depth of compression (DOC) of about greater than about 0.11·t, wherein the glass article exhibits a load to failure of about 10 kgf or greater, after being abraded with 90-grit SiC particles at a pressure of 25 psi for 5 seconds.


Aspect (19) of this disclosure pertains to the strengthened glass article of Aspect (18), wherein the glass article comprises a stored tensile energy of 20 J/m2 or greater.


Aspect (20) of this disclosure pertains to the strengthened glass article of any one of Aspect (18) or Aspect (19), The strengthened glass article of claim 18 or claim 19, wherein the glass article comprises a surface compressive stress and a central tension, wherein the ratio of central tension to surface compressive stress is in the range from about 0.1 to about 1.


Aspect (21) of this disclosure pertains to the strengthened glass article of Aspect (20), wherein the central tension (CT) is 50 MPa or greater.


Aspect (22) of this disclosure pertains to the strengthened glass article of Aspect (20) or Aspect (21), wherein the surface compressive stress is 150 MPa or greater.


Aspect (23) of this disclosure pertains to the strengthened glass article of any one of Aspect (20) through Aspect (22), wherein the surface compressive stress is 400 MPa or greater.


Aspect (24) of this disclosure pertains to the strengthened glass article of any one of Aspect (20) through Aspect (23), wherein the DOC comprises about 0.2t or greater.


Aspect (25) of this disclosure pertains to the strengthened glass article of any one of Aspect (18) through Aspect (24), wherein the glass article comprises an alkali aluminosilicate glass, alkali containing borosilicate glass, alkali aluminophosphosilicate glass or alkali aluminoborosilicate glass.


Aspect (26) of this disclosure pertains to the strengthened glass article of any one of Aspect (20) through Aspect (25), wherein the glass article is adhered to a substrate.


Aspect (27) of this disclosure pertains to a device comprising: a strengthened glass substrate; a containment layer; and a support, wherein the strengthened glass substrate comprises a first surface and a second surface opposing the first surface defining a thickness (t) of about 1.1 mm or less, a compressive stress layer extending from the first surface to a depth of compression (DOC) of greater than about 0.11·t and, and a central tension (CT) of 50 MPa or greater, wherein the device comprises a tablet, a transparent display, a mobile phone, a video player, an information terminal device, an e-reader, a laptop computer, or a non-transparent display.


Aspect (28) pertains to the device of Aspect (27), wherein, after the glass article fractures according to a Frangibility Test, the glass article includes a plurality of fragments having an aspect ratio of about 5 or less.


Aspect (29) pertains to the device of Aspect (27) or Aspect (28), wherein the glass article fractures into the plurality of fragments in 1 second or less, as measured by the Frangibility Test.


Aspect (30) pertains to the device of Aspect (28) or Aspect (29), wherein at least 80% of the plurality of fragments have a maximum dimension that is less than or equal to 5·t.


Aspect (31) pertains to the device of anyone of Aspects (28) through Aspect (30), wherein at least 50% of plurality of fragments each comprise an aspect ratio of 2 or less.


Aspect (32) pertains to the device of any one of Aspects (28) through Aspect (31), wherein at least 50% of the plurality of fragments comprises a volume of less than or equal to about 10 mm3.


Aspect (33) pertains to the device of anyone of Aspects (28) through Aspect (32), wherein the plurality of fragments comprises an ejected portion of fragments, wherein the ejected portion of fragments comprises 10% or less of the plurality of fragments.


Aspect (34) pertains to the device of anyone of Aspects (28) through Aspect (33), wherein the glass article comprises a first weight prior to fracture and the wherein the plurality of fragments comprises an ejected portion of fragments and a non-ejected portion of fragments, the non-ejected portion of fragments having a second weight, and the difference between the first weight and the second weight is 1% of the first weight.


Aspect (35) pertains to the device of anyone of Aspects (28) through Aspect (34), wherein the probability of the glass article fracturing into the plurality of fragments within 1 second or less, as measured by the Frangibility Test, is 99% or greater.


Aspect (36) pertains to the device of anyone of Aspects (28) through Aspect (35), wherein the glass article comprises a stored tensile energy of 20 J/m2 or greater.


Aspect (37) pertains to the device of anyone of Aspects (27) through Aspect (36), wherein the glass article comprises a surface compressive stress and a central tension, wherein the ratio of central tension to surface compressive stress is in the range from about 0.1 to about 1.


Aspect (38) pertains to the device of Aspect (37), wherein the surface compressive stress is 150 MPa or greater.


Aspect (39) pertains to the device of anyone of Aspects (27) through Aspect (38), The device of any one of claims 27-38, wherein the DOC comprises about 0.2t or greater.


Aspect (40) pertains to the device of any one of Aspects (27) through Aspect (39), wherein the glass article comprises an alkali aluminosilicate glass, alkali containing borosilicate glass, alkali aluminophosphosilicate glass or alkali aluminoborosilicate glass.


Aspect (41) pertains to the device of anyone of Aspects (27) through Aspect (40), wherein the glass article is disposed on a containment layer.


Aspect (42) pertains to a strengthened glass article comprising: a first surface and a second surface opposing the first surface defining a thickness (t) of about 1.1 mm or less; a compressive stress layer extending from the first surface to a depth of compression (DOC) of greater than about 0.11·t; wherein, after the glass article is laminated to a containment layer and is fractured according to a Frangibility Test, the glass article comprises fractures, and wherein at least 5% of the fractures extend only partially through the thickness.


Aspect (43) pertains to the strengthened glass article of Aspect (42), wherein the glass article fractures into the plurality of fragments in 1 second or less, as measured by the Frangibility Test.


Aspect (44) pertains to the strengthened glass article of Aspect (42) or Aspect (43), wherein the glass article comprises a stored tensile energy of 20 J/m2 or greater.


Aspect (45) pertains to the strengthened glass article of any one of Aspect (42) through Aspect (44), wherein the glass article comprises a surface compressive stress and a central tension, wherein the ratio of central tension to surface compressive stress is in the range from about 0.1 to about 1.


Aspect (46) pertains to the strengthened glass article of Aspect (45), wherein the central tension is 50 MPa or greater.


Aspect (47) pertains to the strengthened glass article of Aspect (45) or Aspect (46), wherein the surface compressive stress is 150 MPa or greater.


Aspect (48) pertains to the strengthened glass article of any one of Aspect (42) through Aspect (47), wherein the DOC comprises about 0.2t or greater.


Aspect (49) pertains to the strengthened glass article of any one of Aspect (42) through Aspect (48), wherein the glass article comprises an alkali aluminosilicate glass, alkali containing borosilicate glass or alkali aluminoborosilicate glass.


Aspect (50) pertains to the strengthened glass article of any one of Aspect (42) through Aspect (49), wherein the glass article is disposed on a containment layer.


Aspect (51) pertains to a consumer electronic product comprising: a housing having a front surface; electrical components provided at least partially internal to the housing, the electrical components including at least a controller, a memory, and a display; and a cover glass disposed at the front surface of the housing and over the display, the cover glass comprising a strengthened glass article, wherein the strengthened glass article comprises: a first surface and a second surface opposing the first surface defining a thickness (t) of about 1.1 mm or less; a compressive stress layer extending from the first surface to a depth of compression (DOC) of greater than about 0.11·t; and a central tension (CT) of about 50 MPa or greater.


Aspect (52) pertains to the consumer electronics device of Aspect (51), wherein, after the glass article fractures according to a Frangibility Test, the glass article includes a plurality of fragments having an aspect ratio of about 5 or less, and


Aspect (53) pertains to the consumer electronics device of Aspect (52), wherein the glass article fractures into the plurality of fragments in 1 second or less, as measured by the Frangibility Test.


Aspect (54) pertains to the consumer electronics device of Aspect (52) or Aspect (53), wherein at least 80% of the plurality of fragments have a maximum dimension that is less than or equal to 2·t.


Aspect (55) pertains to the consumer electronics device of any one of Aspect (52) through Aspect (54), wherein at least 50% of plurality of fragments each comprise an aspect ratio of 2 or less.


Aspect (56) pertains to the consumer electronics device of any one of Aspect (52) through Aspect (55), wherein at least 50% of the plurality of fragments comprises a volume of less than or equal to about 10 mm3.


Aspect (57) pertains to the consumer electronics device of any one of Aspect (52) through Aspect (56), wherein the plurality of fragments comprises an ejected portion of fragments, wherein the ejected portion of fragments comprises 10% or less of the plurality of fragments.


Aspect (58) pertains to the consumer electronics device of any one of Aspect (52) through Aspect (57), wherein the glass article comprises a first weight prior to fracture and the wherein the plurality of fragments comprises an ejected portion of fragments and a non-ejected portion of fragments, the non-ejected portion of fragments having a second weight, and the difference between the first weight and the second weight is 1% of the first weight.


Aspect (59) pertains to the consumer electronics device of any one of Aspect (53) through Aspect (58), wherein the probability of the glass article fracturing into the plurality of fragments within 1 second or less, as measured by the Frangibility Test, is 99% or greater.


Aspect (60) pertains to the consumer electronics device of anyone of Aspect (51) through Aspect (59), wherein the glass article comprises a stored tensile energy of 20 J/m2 or greater.


Aspect (61) pertains to the consumer electronics device of anyone of Aspect (51) through Aspect (60), wherein the glass article comprises a surface compressive stress and a central tension, wherein the ratio of central tension to surface compressive stress is in the range from about 0.1 to about 1.


Aspect (62) pertains to the consumer electronics device of Aspect (61), wherein the surface compressive stress is 150 or greater.


Aspect (63) pertains to the consumer electronics device of anyone of Aspect (51) through Aspect (62), wherein the DOC comprises about 0.2t or greater.


Aspect (64) pertains to the consumer electronics device of anyone of Aspect (51) through Aspect (63), wherein the glass article comprises an alkali aluminosilicate glass, alkali containing borosilicate glass, alkali aluminophosphosilicate or alkali aluminoborosilicate glass.


Aspect (65) pertains to the consumer electronics device of anyone of Aspect (51) through Aspect (64), wherein the glass article is disposed on a containment layer.


Aspect (66) pertains to the consumer electronics device of anyone of Aspect (51) through Aspect (65), wherein the consumer electronic product comprises a tablet, a transparent display, a mobile phone, a video player, an information terminal device, an e-reader, a laptop computer, or a non-transparent display.


Aspect (67) pertains to a package product comprising: a housing comprising an opening, an exterior surface and an interior surface defining an enclosure; wherein the housing comprises a strengthened glass article, wherein the strengthened glass article comprises: a first surface and a second surface opposing the first surface defining a thickness (t) of about 1.1 mm or less; a compressive stress layer extending from the first surface to a depth of compression (DOC) of greater than about 0.11·t; and a central tension (CT) of 50 MPa or greater.


Aspect (68) pertains to the package product of Aspect (67), wherein, after the glass article fractures according to a Frangibility Test, the glass article includes a plurality of fragments having an aspect ratio of about 5 or less, and wherein the glass article fractures into the plurality of fragments in 1 second or less, as measured by the Frangibility Test.


Aspect (69) pertains to the package product of Aspect (68), wherein at least 80% of the plurality of fragments have a maximum dimension that is less than or equal to 2·t.


Aspect (70) pertains to the consumer electronics device of Aspect (68) or Aspect (69), wherein at least 50% of plurality of fragments each comprise an aspect ratio of 2 or less.


Aspect (71) pertains to the package product of anyone of Aspect (68) through Aspect (70), wherein at least 50% of the plurality of fragments comprises a volume of less than or equal to about 10 mm3.


Aspect (72) pertains to the package product of any one of Aspect (68) through Aspect (71), wherein the plurality of fragments comprises an ejected portion of fragments, wherein the ejected portion of fragments comprises 10% or less of the plurality of fragments.


Aspect (73) pertains to the package product of any one of Aspect (68) through Aspect (72), wherein the glass article comprises a first weight prior to fracture and the wherein the plurality of fragments comprises an ejected portion of fragments and a non-ejected portion of fragments, the non-ejected portion of fragments having a second weight, and the difference between the first weight and the second weight is 1% of the first weight.


Aspect (74) pertains to the package product of any one of Aspect (68) through Aspect (73), wherein the probability of the glass article fracturing into the plurality of fragments within 1 second or less, as measured by the Frangibility Test, is 99% or greater.


Aspect (75) pertains to the package product of any one of Aspect (67) through Aspect (74), wherein the glass article comprises a stored tensile energy of 20 J/m2 or greater.


Aspect (76) pertains to the package product of any one of Aspect (67) through Aspect (75), wherein the glass article comprises a surface compressive stress and a central tension, wherein the ratio of central tension to surface compressive stress is in the range from about 0.1 to about 1.


Aspect (77) pertains to the package product of Aspect (76), wherein the surface compressive stress is 150 or greater.


Aspect (78) pertains to the package product of any one of Aspect (67) through Aspect (77), wherein the DOC comprises about 0.2t or greater.


Aspect (79) pertains to the package product of any one of Aspect (67) through Aspect (78), wherein the glass article comprises an alkali aluminosilicate glass, alkali containing borosilicate glass, alkali aluminophosphosilicate or alkali aluminoborosilicate glass.


Aspect (80) pertains to the package product of any one of Aspect (67) through Aspect (72), wherein the glass article is disposed on a containment layer.


Aspect (82) pertains to the package product of any one of Aspect (67) through Aspect (80), further comprising a pharmaceutical material.


Aspect (83) pertains to the package product of any one of Aspect (67) through Aspect (81), further comprising a cap disposed in the opening.


It will be apparent to those skilled in the art that various modifications and variations can be made without departing from the spirit or scope of the invention.

Claims
  • 1. A glass-based article comprising: greater than or equal to 40 mol % and less than or equal to 80 mol % SiO2;greater than or equal to 0 mol % and less than or equal to 5 mol % Na2O;less than 2 mol % K2O;a first surface and a second surface opposing the first surface thereby defining a thickness (t) of the glass-based article;a ratio of Li2O (mol %) to R2O (mol %) in the glass-based article is greater than or equal to 0.5 and less than or equal to 1.0, wherein R2O is the sum of Li2O, Na2O, and K2O in the glass-based article;a stress profile comprises a surface compressive stress (CS) and a maximum central tension (CT), wherein: the maximum CT is greater than or equal to 50 MPa and less than or equal to 200 MPa;the maximum CT is positioned within the glass-based article at a range from greater than or equal to 0.4·t and less than or equal to 0.6·t;the surface CS is greater than or equal to 200 MPa and less than or equal to 500 MPa; anda depth of compression (DOC) is from greater than or equal to 0.14·t and less than or equal to 0.25·t, andwherein the glass-based article is a glass-ceramic comprising an amorphous phase and a crystalline phase.
  • 2. The glass-based article of claim 1, wherein the glass-based article is strengthened by an ion exchange process resulting in the stress profile.
  • 3. The glass-based article of claim 1, wherein the glass-based article comprises less than or equal to 1 mol % Na2O.
  • 4. The glass-based article of claim 1, wherein the ratio of Li2O (mol %) to R2O (mol %) in the glass-based article is greater than or equal to 0.85 and less than or equal to 1.0.
  • 5. The glass-based article of claim 1, wherein the glass-based article comprises a maximum CT greater than or equal to 50 MPa and less than or equal to 100 MPa.
  • 6. The glass-based article of claim 1, wherein the glass-based article comprises a surface CS greater than or equal to 200 MPa and less than or equal to 400 MPa.
  • 7. The glass-based article of claim 1, wherein the glass-based article comprises a ratio of CT to CS in a range from 0.05 to 1.00.
  • 8. The glass-based article of claim 1, wherein the glass-based article comprises a thickness of about 1 mm or less.
  • 9. The glass-based article of claim 1, wherein the glass-based article comprises greater than or equal to 0 mol % and less than or equal to 5 mol % ZrO2.
  • 10. The glass-based article of claim 1, where the glass-based article comprises greater than or equal to 67 mol % and less than or equal to 74 mol % SiO2.
  • 11. A glass-based article comprising: an amorphous phase and a crystalline phase;a first surface and a second surface opposing the first surface thereby defining a thickness (t) of the glass-based article;a stress profile comprises a surface compressive stress (CS) and a maximum central tension (CT), wherein: the maximum CT is greater than or equal to 50 MPa and less than or equal to 200 MPa;the maximum CT is positioned within the glass-based article at a range from greater than or equal to 0.4·t and less than or equal to 0.6·t;the surface CS is greater than or equal to 200 MPa and less than or equal to 500 MPa; anda depth of compression (DOC) is from greater than or equal to 0.14·t and less than or equal to 0.25·t.
  • 12. The glass-based article of claim 11, wherein the glass-based article comprises a ratio of Li2O (mol %) to R2O (mol %) in the glass-based article is greater than or equal to 0.5 and less than or equal to 1.0, wherein R2O is the sum of Li2O, Na2O, and K2O in the glass-based article.
  • 13. The glass-based article of claim 11, wherein the glass-based article is strengthened by an ion exchange process resulting in the stress profile.
  • 14. The glass-based article of claim 11, wherein the glass-based article comprises less than or equal to 1 mol % Na2O.
  • 15. The glass-based article of claim 11, wherein the glass-based article comprises less than 1 mol % K2O.
  • 16. The glass-based article of claim 11, wherein the ratio of Li2O (mol %) to R2O (mol %) in the glass-based article is greater than or equal to 0.85 and less than or equal to 1.0.
  • 17. The glass-based article of claim 11, wherein the glass-based article comprises a maximum CT greater than or equal to 50 MPa and less than or equal to 100 MPa.
  • 18. The glass-based article of claim 11, wherein the glass-based article comprises a surface CS greater than or equal to 200 MPa and less than or equal to 400 MPa.
  • 19. The glass-based article of claim 11, wherein the glass-based article comprises a ratio of CT to CS in a range from 0.05 to 1.00.
  • 20. The glass-based article of claim 11, wherein the glass-based article comprises a thickness of about 1 mm or less.
CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation of and claims the benefit of priority under 35 U.S.C. § 120 of U.S. application Ser. No. 16/804,271 filed on Feb. 28, 2020, which is a divisional of and claims the benefit of priority under 35 U.S.C. § 120 of U.S. application Ser. No. 15/214,602 filed on Jul. 20, 2016 and issued as U.S. Pat. No. 10,579,106 on Mar. 3, 2020, which in turn, claims the benefit of priority under 35 U.S.C. § 119 of U.S. Provisional Application Ser. No. 62/343,320 filed on May 31, 2016 and U.S. Provisional Application Ser. No. 62/194,984 filed on Jul. 21, 2015, the content of which is relied upon and incorporated herein by reference in its entirety.

US Referenced Citations (342)
Number Name Date Kind
1960121 Moulton May 1934 A
3107196 Acloque Oct 1963 A
3357876 Rinehart Dec 1967 A
3380818 Smith Apr 1968 A
3404015 Dumbaugh, Jr. Oct 1968 A
3410673 Marusak Nov 1968 A
3433611 Saunders et al. Mar 1969 A
3464880 Rinehart Sep 1969 A
3489097 Gemeinhardt Jan 1970 A
3490984 Petticrew et al. Jan 1970 A
3625718 Petticrew Dec 1971 A
3639198 Plumat et al. Feb 1972 A
3656923 Garfinkel et al. Apr 1972 A
3660060 Spanoudis May 1972 A
3673049 Giffen et al. Jun 1972 A
3737294 Dumbaugh et al. Jun 1973 A
3746526 Giffon Jul 1973 A
3765855 Larrick Oct 1973 A
3798013 Hasegawa et al. Mar 1974 A
3811855 Stockdale et al. May 1974 A
3844754 Grubb et al. Oct 1974 A
3879183 Carlson Apr 1975 A
3907577 Kiefer et al. Sep 1975 A
3931438 Beall et al. Jan 1976 A
3936287 Beall et al. Feb 1976 A
3958052 Galusha et al. May 1976 A
3959000 Nakagawa et al. May 1976 A
4042405 Krohn et al. Aug 1977 A
4053679 Rinehart Oct 1977 A
4055703 Rinehart Oct 1977 A
4102664 Dumbaugh, Jr. Jul 1978 A
4130437 Mazeau et al. Dec 1978 A
4148661 Kerko et al. Apr 1979 A
4156755 Rinehart May 1979 A
4190451 Hares et al. Feb 1980 A
4192688 Babcock Mar 1980 A
4214886 Shay et al. Jul 1980 A
4240836 Borrelli et al. Dec 1980 A
4242117 van Ass Dec 1980 A
4358542 Hares et al. Nov 1982 A
4407966 Kerko et al. Oct 1983 A
4468534 Boddicker Aug 1984 A
4471024 Pargamin et al. Sep 1984 A
4483700 Forker et al. Nov 1984 A
4537612 Borrelli et al. Aug 1985 A
4608349 Kerko et al. Aug 1986 A
4702042 Herrington et al. Oct 1987 A
4726981 Pierson et al. Feb 1988 A
4757162 Dumora et al. Jul 1988 A
4857485 Brennan et al. Aug 1989 A
5270269 Hares et al. Dec 1993 A
5273827 Francis Dec 1993 A
5322819 Araujo et al. Jun 1994 A
5342426 Dumbaugh, Jr. Aug 1994 A
5350607 Tyson et al. Sep 1994 A
5559060 Dumbaugh et al. Sep 1996 A
5763343 Brix et al. Jun 1998 A
5773148 Charrue et al. Jun 1998 A
5804317 Charrue Sep 1998 A
5895768 Speit Apr 1999 A
5972460 Tachiwana Oct 1999 A
6111821 Bach Aug 2000 A
6187441 Takeuchi et al. Feb 2001 B1
6333286 Kurachi et al. Dec 2001 B1
6376402 Pannhorst et al. Apr 2002 B1
6413892 Koyama et al. Jul 2002 B1
6440531 Kurachi et al. Aug 2002 B1
6472068 Glass et al. Oct 2002 B1
6514149 Yoon Feb 2003 B2
6516634 Green et al. Feb 2003 B1
6518211 Bradshaw et al. Feb 2003 B1
6528440 Vilato et al. Mar 2003 B1
6537938 Miyazaki Mar 2003 B1
6607999 Hachitani Aug 2003 B2
6689704 Ota et al. Feb 2004 B2
6846760 Siebers et al. Jan 2005 B2
7007512 Kamada et al. Mar 2006 B2
7091141 Horsfall et al. Aug 2006 B2
7176528 Couillard et al. Feb 2007 B2
7476633 Comte et al. Jan 2009 B2
7514149 Bocko et al. Apr 2009 B2
7531475 Kishimoto et al. May 2009 B2
7619283 Gadkaree Nov 2009 B2
7666511 Ellison et al. Feb 2010 B2
7687419 Kawai Mar 2010 B2
7727917 Shelestak et al. Jun 2010 B2
7838136 Nakashima et al. Nov 2010 B2
7891212 Isono Feb 2011 B2
8007913 Coppola et al. Aug 2011 B2
8075999 Barefoot et al. Dec 2011 B2
8099982 Takagi et al. Jan 2012 B2
8143179 Aitken et al. Mar 2012 B2
8158543 Dejneka et al. Apr 2012 B2
8193128 Hellmann et al. Jun 2012 B2
8232218 Dejneka et al. Jul 2012 B2
8252708 Morena et al. Aug 2012 B2
8312739 Lee et al. Nov 2012 B2
8312789 Beck Nov 2012 B2
8327666 Harvey et al. Dec 2012 B2
8347651 Abramov et al. Jan 2013 B2
8349455 Kondo et al. Jan 2013 B2
8415013 Barefoot et al. Apr 2013 B2
8431502 Dejneka et al. Apr 2013 B2
8561429 Allan et al. Oct 2013 B2
8580411 Endo et al. Nov 2013 B2
8586492 Barefoot et al. Nov 2013 B2
8623776 Dejneka et al. Jan 2014 B2
8652978 Dejneka et al. Feb 2014 B2
8656734 Zou et al. Feb 2014 B2
8691711 Nakashima et al. Apr 2014 B2
8697592 Ikenishi et al. Apr 2014 B2
8713972 Lakota et al. May 2014 B2
8756262 Zhang Jun 2014 B2
8759238 Chapman et al. Jun 2014 B2
8765262 Gross Jul 2014 B2
8778820 Gomez et al. Jul 2014 B2
8783063 Osakabe et al. Jul 2014 B2
8802581 Dejneka et al. Aug 2014 B2
8854623 Fontaine et al. Oct 2014 B2
8932510 Li et al. Jan 2015 B2
8943855 Gomez et al. Feb 2015 B2
8946103 Dejneka et al. Feb 2015 B2
8950215 Rappoport et al. Feb 2015 B2
8951927 Dejneka et al. Feb 2015 B2
8957374 Liu et al. Feb 2015 B2
8969226 Dejneka et al. Mar 2015 B2
8975374 Kimura Mar 2015 B2
9003835 Lock Apr 2015 B2
9007878 Matsumoto et al. Apr 2015 B2
9139469 Comte et al. Sep 2015 B2
9140543 Allan et al. Sep 2015 B1
9145329 Drake et al. Sep 2015 B2
9156724 Gross Oct 2015 B2
9193625 Bookbinder et al. Nov 2015 B2
9212288 Fujiwara et al. Dec 2015 B2
9272945 Smith Mar 2016 B2
9290407 Barefoot et al. Mar 2016 B2
9290413 Dejneka et al. Mar 2016 B2
9346703 Bookbinder et al. May 2016 B2
9359251 Bookbinder et al. Jun 2016 B2
9487434 Amin et al. Nov 2016 B2
9498822 Brandt et al. Nov 2016 B2
9499431 Barefoot et al. Nov 2016 B2
9593042 Hu et al. Mar 2017 B2
9604876 Gy et al. Mar 2017 B2
9701569 Demartino et al. Jul 2017 B2
9751802 Allan et al. Sep 2017 B2
9908811 Gross et al. Mar 2018 B2
9977470 Demartino et al. May 2018 B2
10017417 Dejneka et al. Jul 2018 B2
10144670 Akatsuka et al. Dec 2018 B2
10160688 Amin et al. Dec 2018 B2
10239784 Oram et al. Mar 2019 B2
10259746 Hu et al. Apr 2019 B2
10570059 Dejneka et al. Feb 2020 B2
10579106 Demartino et al. Mar 2020 B2
20020023463 Siebers et al. Feb 2002 A1
20050090377 Shelestak et al. Apr 2005 A1
20050099618 DiFoggio et al. May 2005 A1
20050143247 Siebers Jun 2005 A1
20050221044 Gaume et al. Oct 2005 A1
20050250639 Siebers et al. Nov 2005 A1
20060127679 Gulati et al. Jun 2006 A1
20060279217 Peuchert et al. Dec 2006 A1
20070060465 Varshneya et al. Mar 2007 A1
20070122580 Krall May 2007 A1
20070123410 Morena et al. May 2007 A1
20070218262 Degand et al. Sep 2007 A1
20080026927 Monique Comte Jan 2008 A1
20080128953 Nagai et al. Jun 2008 A1
20080241603 Isono Oct 2008 A1
20080286548 Ellison et al. Nov 2008 A1
20090142568 Dejneka et al. Jun 2009 A1
20090197088 Murata Aug 2009 A1
20090215607 Dejneka et al. Aug 2009 A1
20090220761 Dejneka et al. Sep 2009 A1
20090286091 Danielson et al. Nov 2009 A1
20100009154 Allan et al. Jan 2010 A1
20100028607 Lee et al. Feb 2010 A1
20100029460 Shojiya et al. Feb 2010 A1
20100035038 Barefoot Feb 2010 A1
20100035745 Murata Feb 2010 A1
20100087307 Murata et al. Apr 2010 A1
20100112341 Takagi et al. May 2010 A1
20100119846 Sawada May 2010 A1
20100190038 Osakabe et al. Jul 2010 A1
20100200804 Woodruff et al. Aug 2010 A1
20100210442 Abramov et al. Aug 2010 A1
20100215996 Wendling et al. Aug 2010 A1
20100291353 Dejneka et al. Nov 2010 A1
20100326657 Hellmann et al. Dec 2010 A1
20110014475 Murata Jan 2011 A1
20110064951 Fujiwara et al. Mar 2011 A1
20110067447 Zadesky et al. Mar 2011 A1
20110092353 Amin et al. Apr 2011 A1
20110165393 Bayne et al. Jul 2011 A1
20110201490 Barefoot et al. Aug 2011 A1
20110226832 Bayne et al. Sep 2011 A1
20110281093 Gulati et al. Nov 2011 A1
20110293942 Cornejo et al. Dec 2011 A1
20110294648 Chapman et al. Dec 2011 A1
20110294649 Gomez et al. Dec 2011 A1
20110312483 Nakashima et al. Dec 2011 A1
20120015150 Suzuki Jan 2012 A1
20120021898 Elam et al. Jan 2012 A1
20120040146 Garner et al. Feb 2012 A1
20120048604 Cornejo et al. Mar 2012 A1
20120052271 Gomez Mar 2012 A1
20120052275 Hashimoto et al. Mar 2012 A1
20120083401 Koyama et al. Apr 2012 A1
20120114955 Almoric et al. May 2012 A1
20120135153 Osakabe et al. May 2012 A1
20120135226 Bookbinder et al. May 2012 A1
20120135848 Beall et al. May 2012 A1
20120171497 Koyama et al. Jul 2012 A1
20120189843 Chang et al. Jul 2012 A1
20120194974 Weber et al. Aug 2012 A1
20120196110 Murata et al. Aug 2012 A1
20120216565 Allan et al. Aug 2012 A1
20120216569 Allan et al. Aug 2012 A1
20120219792 Yamamoto et al. Aug 2012 A1
20120236526 Weber Sep 2012 A1
20120264585 Ohara et al. Oct 2012 A1
20120297829 Endo et al. Nov 2012 A1
20120308827 Boek et al. Dec 2012 A1
20120321898 Meinhardt et al. Dec 2012 A1
20130004758 Dejneka et al. Jan 2013 A1
20130007458 Wakita et al. Jan 2013 A1
20130017380 Murata et al. Jan 2013 A1
20130045375 Gross Feb 2013 A1
20130050992 Schneider et al. Feb 2013 A1
20130101596 Demartino et al. Apr 2013 A1
20130101798 Hashimoto Apr 2013 A1
20130122260 Liang May 2013 A1
20130122284 Gross May 2013 A1
20130183512 Gy Jul 2013 A1
20130186139 Tanii Jul 2013 A1
20130189486 Wang et al. Jul 2013 A1
20130202868 Barefoot et al. Aug 2013 A1
20130203583 Zhang et al. Aug 2013 A1
20130219966 Hasegawa et al. Aug 2013 A1
20130224492 Bookbinder et al. Aug 2013 A1
20130236666 Bookbinder et al. Sep 2013 A1
20130236699 Prest et al. Sep 2013 A1
20130240025 Bersano et al. Sep 2013 A1
20130260154 Allan et al. Oct 2013 A1
20130274085 Beall et al. Oct 2013 A1
20130288001 Murata et al. Oct 2013 A1
20130288010 Akarapu et al. Oct 2013 A1
20130309613 O'Malley et al. Nov 2013 A1
20130323444 Ehemann et al. Dec 2013 A1
20140023865 Comte et al. Jan 2014 A1
20140050911 Mauro et al. Feb 2014 A1
20140063393 Zhong et al. Mar 2014 A1
20140087159 Cleary et al. Mar 2014 A1
20140087193 Cites et al. Mar 2014 A1
20140087194 Dejneka et al. Mar 2014 A1
20140090864 Paulson Apr 2014 A1
20140092377 Liu et al. Apr 2014 A1
20140093702 Kitajima Apr 2014 A1
20140106141 Bellman et al. Apr 2014 A1
20140106172 Dejneka et al. Apr 2014 A1
20140109616 Varshneya Apr 2014 A1
20140113141 Yamamoto et al. Apr 2014 A1
20140134397 Amin et al. May 2014 A1
20140139978 Kwong May 2014 A1
20140141226 Bookbinder et al. May 2014 A1
20140147576 Lewis et al. May 2014 A1
20140150525 Okawa et al. Jun 2014 A1
20140151370 Chang et al. Jun 2014 A1
20140154661 Bookbinder et al. Jun 2014 A1
20140170380 Murata et al. Jun 2014 A1
20140193606 Kwong Jul 2014 A1
20140220327 Adib et al. Aug 2014 A1
20140227523 Dejneka et al. Aug 2014 A1
20140227524 Ellison et al. Aug 2014 A1
20140227525 Matsuda et al. Aug 2014 A1
20140248495 Matsuda et al. Sep 2014 A1
20140308526 Chapman et al. Oct 2014 A1
20140321124 Schneider et al. Oct 2014 A1
20140329660 Barefoot et al. Nov 2014 A1
20140335330 Bellman et al. Nov 2014 A1
20140356576 Dejneka et al. Dec 2014 A1
20140356605 Adib et al. Dec 2014 A1
20140364298 Ohara et al. Dec 2014 A1
20140370264 Ohara et al. Dec 2014 A1
20140370302 Amin et al. Dec 2014 A1
20150004390 Kawamoto et al. Jan 2015 A1
20150011811 Pavone et al. Jan 2015 A1
20150027169 Fredholm Jan 2015 A1
20150030834 Morey et al. Jan 2015 A1
20150030838 Sellier et al. Jan 2015 A1
20150037543 Keegan et al. Feb 2015 A1
20150037586 Gross Feb 2015 A1
20150044473 Murata et al. Feb 2015 A1
20150052949 Bayne et al. Feb 2015 A1
20150060401 Chang et al. Mar 2015 A1
20150064472 Gross et al. Mar 2015 A1
20150064474 Dejneka et al. Mar 2015 A1
20150074974 Pesansky et al. Mar 2015 A1
20150079398 Amin Mar 2015 A1
20150093581 Murata et al. Apr 2015 A1
20150111030 Miyasaka et al. Apr 2015 A1
20150132563 O'Malley et al. May 2015 A1
20150140325 Gross et al. May 2015 A1
20150144291 Brandt et al. May 2015 A1
20150147574 Allan et al. May 2015 A1
20150147575 Dejneka et al. May 2015 A1
20150147576 Bookbinder et al. May 2015 A1
20150152003 Kawamoto et al. Jun 2015 A1
20150157533 Demartino et al. Jun 2015 A1
20150166401 Yamamoto Jun 2015 A1
20150166407 Varshneya et al. Jun 2015 A1
20150175469 Tabe Jun 2015 A1
20150183680 Barefoot et al. Jul 2015 A1
20150239775 Amin et al. Aug 2015 A1
20150239776 Amin et al. Aug 2015 A1
20150251947 Lestrigant et al. Sep 2015 A1
20150259244 Amin et al. Sep 2015 A1
20150261363 Shah et al. Sep 2015 A1
20150274585 Rogers et al. Oct 2015 A1
20150329413 Beall et al. Nov 2015 A1
20150329418 Murata et al. Nov 2015 A1
20150368148 Duffy et al. Dec 2015 A1
20150368153 Pesansky et al. Dec 2015 A1
20160083291 Dogimont et al. Mar 2016 A1
20160102011 Hu et al. Apr 2016 A1
20160102014 Hu et al. Apr 2016 A1
20160107924 Yamamoto et al. Apr 2016 A1
20160122239 Amin et al. May 2016 A1
20160122240 Oram et al. May 2016 A1
20160187994 La et al. Jun 2016 A1
20160318796 Masuda Nov 2016 A1
20170022093 Demartino et al. Jan 2017 A1
20170158556 Dejneka et al. Jun 2017 A1
20170166478 Gross et al. Jun 2017 A1
20170197869 Beall et al. Jul 2017 A1
20170197870 Finkeldey et al. Jul 2017 A1
20170291849 Dejneka et al. Oct 2017 A1
20170295657 Gross et al. Oct 2017 A1
20170305786 Roussev et al. Oct 2017 A1
20190208652 Gross et al. Jul 2019 A1
Foreign Referenced Citations (205)
Number Date Country
6452265 Oct 1965 AU
2011212982 Aug 2012 AU
1312582 Sep 2001 CN
1693247 Nov 2005 CN
1759074 Apr 2006 CN
1886348 Dec 2006 CN
101316799 Dec 2008 CN
101578240 Nov 2009 CN
101583576 Nov 2009 CN
101679106 Mar 2010 CN
101689376 Mar 2010 CN
102026929 Apr 2011 CN
102089252 Jun 2011 CN
102131740 Jul 2011 CN
102149649 Aug 2011 CN
102363567 Feb 2012 CN
102393289 Mar 2012 CN
102531384 Jul 2012 CN
102690059 Sep 2012 CN
102791646 Nov 2012 CN
102815860 Dec 2012 CN
102887650 Jan 2013 CN
102898022 Jan 2013 CN
102958855 Mar 2013 CN
103058506 Apr 2013 CN
103058507 Apr 2013 CN
103068759 Apr 2013 CN
103097319 May 2013 CN
103282318 Sep 2013 CN
103338926 Oct 2013 CN
103569015 Feb 2014 CN
103648996 Mar 2014 CN
103946166 Jul 2014 CN
104379522 Feb 2015 CN
104736496 Jun 2015 CN
105753314 Jul 2016 CN
108046589 May 2018 CN
0132751 Feb 1985 EP
0163873 Dec 1985 EP
0700879 Mar 1996 EP
0931028 Jul 1999 EP
1291631 Mar 2003 EP
1314704 May 2003 EP
1593658 Nov 2005 EP
2263979 Dec 2010 EP
2397449 Dec 2011 EP
2415724 Feb 2012 EP
2531459 Dec 2012 EP
2540682 Jan 2013 EP
2594536 May 2013 EP
2609047 Jul 2013 EP
2646243 Oct 2013 EP
2666756 Nov 2013 EP
2695734 Feb 2014 EP
2736855 Jun 2014 EP
2762459 Aug 2014 EP
2762460 Aug 2014 EP
3204338 Aug 2017 EP
1012367 Dec 1965 GB
1026770 Apr 1966 GB
1089912 Nov 1967 GB
1334828 Oct 1973 GB
47-004192 Sep 1972 JP
54-083923 Jul 1979 JP
62-187140 Aug 1987 JP
02-293345 Dec 1990 JP
07-263318 Oct 1995 JP
11-328601 Nov 1999 JP
2000-203872 Jul 2000 JP
2000-327365 Nov 2000 JP
2001-076336 Mar 2001 JP
2001-354446 Dec 2001 JP
2002-115071 Apr 2002 JP
2002-174810 Jun 2002 JP
2002-358626 Dec 2002 JP
2003-505327 Feb 2003 JP
2003-283028 Oct 2003 JP
2004-099370 Apr 2004 JP
2004-259402 Sep 2004 JP
2005-062592 Mar 2005 JP
2005-139031 Jun 2005 JP
2005-519997 Jul 2005 JP
2005-206406 Aug 2005 JP
2005-289683 Oct 2005 JP
2005-289685 Oct 2005 JP
2005-320234 Nov 2005 JP
2006-228431 Aug 2006 JP
2007-527354 Sep 2007 JP
2007-252589 Oct 2007 JP
2007-255139 Oct 2007 JP
2007-255319 Oct 2007 JP
2007-314521 Dec 2007 JP
2008-007384 Jan 2008 JP
2008-094713 Apr 2008 JP
2008-115071 May 2008 JP
2009-084076 Apr 2009 JP
2009-099239 May 2009 JP
2009-107878 May 2009 JP
2009-274902 Nov 2009 JP
2009-280478 Dec 2009 JP
2010-202514 Sep 2010 JP
2011-057504 Mar 2011 JP
2011-213576 Oct 2011 JP
2011-527661 Nov 2011 JP
2011-530470 Dec 2011 JP
2012-066995 Apr 2012 JP
2012-232882 Nov 2012 JP
2013-502371 Jan 2013 JP
2013-028512 Feb 2013 JP
2013-518800 May 2013 JP
2013-529172 Jul 2013 JP
2013-536155 Sep 2013 JP
2013-542159 Nov 2013 JP
2014-501214 Jan 2014 JP
2014-073953 Apr 2014 JP
5483923 May 2014 JP
2014-136751 Jul 2014 JP
2014-141363 Aug 2014 JP
2014-522798 Sep 2014 JP
2015-511537 Apr 2015 JP
10-2012-0128657 Nov 2012 KR
10-1302664 Sep 2013 KR
1302664 Sep 2013 KR
10-2013-0135840 Dec 2013 KR
10-2014-0131558 Nov 2014 KR
10-1506378 Mar 2015 KR
10-2016-0080048 Jul 2016 KR
2127711 Mar 1999 RU
187326 Feb 2013 SG
1677028 Sep 1991 SU
200911718 Mar 2009 TW
201040118 Nov 2010 TW
201313635 Apr 2013 TW
201331148 Aug 2013 TW
201335092 Sep 2013 TW
201350449 Dec 2013 TW
201402490 Jan 2014 TW
201520178 Jun 2015 TW
9906334 Feb 1999 WO
2000047529 Aug 2000 WO
0107374 Feb 2001 WO
2005042423 May 2005 WO
2005091021 Sep 2005 WO
2005093720 Oct 2005 WO
2009041348 Apr 2009 WO
2009041618 Apr 2009 WO
2010002477 Jan 2010 WO
2010005578 Jan 2010 WO
2010016928 Feb 2010 WO
2010147650 Dec 2010 WO
2011022661 Feb 2011 WO
2011041484 Apr 2011 WO
2011069338 Jun 2011 WO
2011077756 Jun 2011 WO
2011085190 Jul 2011 WO
2011097314 Aug 2011 WO
2011103798 Sep 2011 WO
2011103799 Sep 2011 WO
2011104035 Sep 2011 WO
2011149740 Dec 2011 WO
2011149811 Dec 2011 WO
2011149812 Dec 2011 WO
2012027660 Mar 2012 WO
2012074983 Jun 2012 WO
2012126394 Sep 2012 WO
2013016157 Jan 2013 WO
2013018774 Feb 2013 WO
2013027651 Feb 2013 WO
2013028492 Feb 2013 WO
2013032890 Mar 2013 WO
2013047679 Apr 2013 WO
2013082246 Jun 2013 WO
2013088856 Jun 2013 WO
2013110721 Aug 2013 WO
2013116420 Aug 2013 WO
2013120721 Aug 2013 WO
2013130653 Sep 2013 WO
2013130665 Sep 2013 WO
2013130721 Sep 2013 WO
2013136013 Sep 2013 WO
2013184205 Dec 2013 WO
2014042244 Mar 2014 WO
2014052229 Apr 2014 WO
2014097623 Jun 2014 WO
2014100432 Jun 2014 WO
2014175144 Oct 2014 WO
2014180679 Nov 2014 WO
2015057552 Apr 2015 WO
2015057555 Apr 2015 WO
2015077179 May 2015 WO
2015080043 Jun 2015 WO
2015127483 Aug 2015 WO
2015175595 Nov 2015 WO
2015195419 Dec 2015 WO
2015195465 Dec 2015 WO
2016014937 Jan 2016 WO
2016028554 Feb 2016 WO
2016057787 Apr 2016 WO
2016070048 May 2016 WO
2016174825 Nov 2016 WO
2016185934 Nov 2016 WO
2017030736 Feb 2017 WO
2017100646 Jun 2017 WO
2017177109 Oct 2017 WO
2017177114 Oct 2017 WO
Non-Patent Literature Citations (136)
Entry
European Patent Application No. 16823100.9 Office Action dated Jul. 23, 2020; 9 Pages; European Patent Office.
European Patent Application No. 16823100.9 Office Action dated Mar. 29, 2019; 6 Pages; European Patent Office.
European Patent Application No. 17719103.8 Observations by third parties dated Aug. 26, 2020; 10 Pages; European Patent Office.
European Patent Office First Office Action EP11799531.6-1355 dated May 2, 2014, 2 Pgs.
European Patent Office First Office Action EP11802990.9 dated Mar. 6, 2014, 6 Pgs.
European Patent Office; International Search Report; dated Aug. 27, 2013; pp. 1-3.
Extended European Search Report and Search Opinion; 19217082.7; dated Aug. 12, 2020; 14 pages; European Patent Office.
F.V. Tooley; “The Handbook of Glass Manufacture, vol. II”; China Architecture & Building Press, First Edition, Feb. 1983, pp. 304-305.
Fu, et al, “Preparation of alumina films from a new sol-gel route” Thin Solid films 348, pp. 99-102 (1999).
Glover et al; “The interactive whiteboard: a literature survey”; Technology, Pedagogy and Education (14) 2: 155-170.
Glover, D., Miller, D., Averts, D., Door, V. (2005) “The interactive whiteboard: a literature survey”. Technology, Pedagogy and Education (vol. 14) 2005, Issue 2: 155-170.
Greaves et al; “Inorganic Glasses, glass-forming liquids and amorphizing solids” Advances in Physics; vol. 56, No. 1; 2007 pp. 1-166.
Greaves et al; “Inorganic Glasses, Glass-Forming Liquids and Amorphizing Solids”, Advances in Physics; vol. 56, No. 1, Jan.-Feb. 2007, 1166.
Green; “Section 2. Residual stress, brittle fracture and damage; Critical parameters in the processing of engineered stress profile glasses”; Journal of Non-Crystalline Solids, 316 (2003) 35-41.
Gulati, “Frangibility of tempered soda-lime glass sheet” Glass Processing Days, Sep. 13-15, 1997. pp. 72-76.
Gulati, Frangibility of Tempered Soda-Lime Glass Sheet, Glass Processing Days, The Fifth International Conference on Architectural and Automotive Glass, Sep. 13-15, 1997.
Hampshire; “Oxynitride glasses, their properties and crystallization—a review”; Journal of Non-Crystalline Solids; vol. 316, 2003; pp. 64-73.
Hampshire; “Section 3. Oxynitride Glasses; Oxynitride Glasses, Their Properties and Crystallisation—A Review”, Journal of Non-Crystalline Solids 316 (2003) pp. 64-73.
Hauk “Sol-gel preparation of scratch-resistant Al2O3 coatings on float glass”, Glass Science and Technology Glastechnische Berichte, 72(12), pp. 386, 1999.
Indian Patent Application No. 202018006461 office Action dated Sep. 22, 2020; 6 Pages; Indian Patent Office.
Indian Patent Application No. 201817021369; First Examination Report dated Dec. 24, 2019; India Patent Office; 7 Pgs.
International Search Report and the Written Opinoin of the International Searching Authority; PCT/US2015/035448; dated Sep. 18, 2015; 11 Pages.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2015/023507; dated Oct. 19, 2015; 19 Pages.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2015/034996 dated Jan. 4, 2016; 13 Pages.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2015/054681; dated Apr. 6, 2016; 16 Pages; European Patent Office.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2015/058322 dated Jan. 8, 2016; 14 Pages.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2015/058919;dated Jan. 11, 2016; 11 Pages.
International Search Report and Written Opinion of the International Searching Authority; PCTUS2015041976; dated Oct. 29, 2015; 11 Pages.
International Search Report and Written Opinion PCT/US2011/062288 dated Feb. 28, 2012.
International Search Report and Written Opinion PCT/US2011/062354 dated Mar. 15, 2012.
International Search Report and Written Opinion PCT/US2013/028079 dated Aug. 27, 2013.
International Search Report and Written Opinion PCT/US2016/034634 dated Nov. 2, 2016.
International Search Report and Written Opinion PCT/US2016/043610 dated Feb. 1, 2017.
International Search Report and Written Opinion PCT/US2016/085932 dated Apr. 5, 2017.
International Search Report and Written Opinion PCT/US2017/026554 dated Jul. 10, 2017.
International Search Report and Written Opinion PCT/US2017/026561 dated Jun. 19, 2017; 13 Pages; European Patent Office.
International Searching Authority Invitation to Pay Additional Fees PCT/US2016/043610 dated Dec. 8, 2016.
Japanese Patent Application No. 2018-073075 Decision to Grant dated Sep. 2, 2020; 5 Pages; Japanese Patent Office.
Japanese Patent Application No. 2018529948; Machine Translation of the Office Action dated Dec. 18, 2019; Japan Patent Office; 8 Pgs.
Japanese Patent Application No. 2018540470; Machine Translation of the Office Action dated Feb. 12, 2020; Japan Patent Office; 7 Pgs.
Japanese Patent Application No. 2019-005651 Notice of Reasons for Refusal dated Sep. 30, 2020; 18 Pages; Japanese Patent Office.
Japanese Patent Application No. 2019-005651; Office Action dated Nov. 8, 2019; Japan Patent Office; 4 Pgs.
Japanese Patent Application No. 2019-184641 Notice of Reasons for Refusal dated Oct. 7, 2020; 7 Pages; Japanese Patent Office.
JP2017518941 Notice of Allowance dated Feb. 20, 2019, Japan Patent Office, 3 Pgs.
JP2018073075 Office Action dated May 8, 2019, Japan Patent Office.
JP2019005650 Office Action dated Feb. 13, 2019, Japan Patent Office.
Kim; “Glass Engineering”; Glass Technology 3rd Edition; (2009) 8 Pages.
Kitaigorodskii et al, In: Sb.Nauchn.Rabot Belor.Politekhn.Inst.,Khimiya, Tekhnologiya i Istoriya Stekla i Keramiki, 1960, No. 86, p. 38. (The Synthesis of Thermo-stable glasses) Abstract Only.
Kitaigorodskii I.I. ‘Sentyurin G.G.’ ‘Egorova L.S.’, In: Sb.Nauchn.Rabot Belor.Politekhn.Inst.,Khimiya, Tekhnologiya Istoriya Stekla i Keramiki, 1960, No. 86, p. 38. (The Synthesis of Thermo-stable glasses) Abstract Only.
Le Bourhis; “Glass Mechanics and Technology”; Wiley-Vch, Second Edition; (2014) 8 Pages.
Le Bourhis; “Hardness”; Glass Mechanics and Technology; 2008; pp. 170-174.
Liu et al, “Common Knowledge Evidence: Inorganic Non-Metallic Materials Technology”, China University of Science and Technology Press, Sep. 2015, 1st edition.
Nagashima; “Chemical Strengthening of Glass”; Surface Technology; vol. 64, No. 8; (2013) pp. 434-438.
Oram et al; U.S. Appl. No. 14/932,411, filed Nov. 4, 2015, Titled “Deep Non-Frangible Stress Profiles and Methods of Making”.
Patent Cooperation Treaty International Notification of Invitation to pay additional fees; international application No. PCT/US2015/054681: dated Dec. 14, 2015, 7 pages.
Patent Cooperation Treaty, Partial International Search Report for International Application No. PCT/US2015/054681, dated Nov. 11, 2015, 7 pages.
Peitl et al; “Thermal Shock Properties of Chemically Toughened Borosilicate Glass”; Journal of Non-Crystallin Solids, 247, (1999) pp. 39-49.
Pflitsch et al; “Sol-gel deposition of chromium doped aluminum oxide films (Ruby) for surface temperature sensor application”, Chem. Mater., vol. 20, pp. 2773-2778, 2008.
Poumellec et al; “Surface topography change induced by poling in Ge doped silica glass films”; 2003 OSA/BGPP 2003 MD 38.
Reddy et al. “Fracture Toughness Measurement of Glass and Ceramic Materials Using Chevron-Notched Specimens” J. Am. Ceram. Soc. 71 (6) C-310-C313 (1988).
Reddy, K.P.R. et al, “Fracture Toughness Measurement of Glass and Ceramic Materials Using Chevron-Notched Specimens,” J. Am. Ceram. Soc., 71 [6], C-310-C-313 (1988).
Rusan et al; “A New Method for Recording Phase Optical Structures in Glasses”; Glass Physics and Chemistry, 2010, vol. 36, No. 4, pp. 513-516.
Russian Patent Application No. 2018105921; Russian Office Action and Search Report dated Sep. 19, 2019; Russia Patent Office; 4 Pgs.
Sglavo & Green, “Flaw-insensitive ion-exchanged glass: 11, Production and mechanical performance” J. Am. Ceram. Soc. 84(8) pp. 1832-1838 (2001).
Sglavo et al. “procedure for residual stress profile determination by vurbature measurements” Mechanics of Materias, 2005, 37(8) pp. 887-898.
Shen et al; “Control of concentration profiles in two step ion exchanged glasses”; Phys. Chem. Glasses, 2003 44 (4), 284-92.
Shen et al; “Variable-temperature ion-exchanged engineered stress profile (ESP) glasses”; J. Am. Ceram. Soc., 86 [11] 1979-81 (2003).
Smedskjaer “Effect of thermal history and chemical composition on hardness of silicate glasses”; Journal of Non-Crystalline Solids 356 (2010); pp. 893-897.
Stosser et al “Magnetic Resonance investigation of the process of corundum formation starting from sol-gel precursors”, J Am. Ceram. Soc, vol. 88, No. 10, pp. 2913-2922, 2005.
Taiwan First Office Action and Search Report TW100143769 Tsai, Lee and Chen. dated Apr. 29, 2016, 3 Pgs.
Takagi et al; “Electrostatic Imprint Process for Glass”; Applied Physics Express 1 (20008) 024003.
Tang et al. “Methods for measurement and statistical analysis of the frangibility of strengthened glass” Frontiers in Materials, 2015 vol. 2, article 50. 8 pgs.
Tang, et al., “Automated Apparatus for Measuring the Frangibility and Fragmentation of Strengthened Glass”, Experimental Mechanics (Jun. 2014) vol. 54 pp. 903-912.
Varshneya; “Fundamentals of Inorganic Glasses”; 2nd edition, Society of Glass Technology, 2006, pp. 513-521, XP002563094.
Varshneya; “Microhardness vs. Glass Composition”; Fundamentals of Inorganic Glasses; 2006; p. 208, paragraph 7.
Yong-Hwan; “Chemical Tempered Glass for Mobile Displays”; Korea Institute of Science and Technology; Date Unknown; 6 Pages.
Zheng et al; “Effect of Y2O3 addition on viscosity and crystallizationof the lithium aluminosilicate glasses”; Thermochimica Acta 456 (2007) 69-74.
Zheng et al; “Structure and Properties of the Lithium Aluminosilicate Glasses with Yttria Addition”; vol. 22, No. 2 Wuhan University of Technology—(Abstract).
Zimmer, “Thin Glasses for Touch Display Technologies” Schott: glass made of ideas. Emerging Display Technologies Conference, Aug. 16-17, 2011. 17 slides.
European Patent Application No. 13709022.1 Observations by third parties dated Dec. 16, 2020; 4 Pages; European Patent Office.
Abrams et al; “Fracture behavior of engineered stress profile soda lime silicate glass”; Journal of Non-Crystalline Solids; 321, (2003) 10-19.
Aegerter et al “Sol-gel technologies for glass producers and users—Chapter 4.1 8—Scratch resistant coatings (G. Helsch and G. H. Frischat)”, pp. 217-221, Kluwer Academic Publishers, 2004.
Amin et al; U.S. Appl. No. 14/926,425, filed Oct. 29, 2015, titled “Strengthened Glass With Ultra-Deep Depth of Compression”.
ASTM C1279-13 “Standard Test Method for Non-Destructive Photoelastic Measurement of Edge and Surface Stresses in Annealed, Heat-Strengthened, and Fully Tempered Flat Glass”.
ASTM C1422/C1422M—10 “Standard Specification for Chemically Strengthened Flat Glass”.
ASTM C158-02(2012), Standard Test Methods for Strength of Glass by Flexure (Determination of Modulus of Rupture), ASTM International, West Conshohocken, PA, 2012, 9 pages.
Bahlawane “Novel sol-gel process depositing a-AI2O3 for the improvement of graphite oxidation-resistance”—Thin Solid Films, vol. 396, pp. 126-130, 2001.
Bansal et al; “Chapter 10: Elastic Properties” Handbook of Glass Properties; Elsevier; (1986) pp. 306-336.
Bansal et al; “Handbook of Glass Properties”; Elsevier; (1986) 2 pages.
Bouyne eil al; “Fragmentation of thin chemically tempered glass plates”; Glass Technol., 2002, 43C, 300-2.
Brandt et al; “Mechanics of Ceramics, Active Materials, Nanoscale Materials, Composites, Glass, and Fundamentals”; Proceedings of the 8th International Symposium on Fracture Mechanics of Ceramics, (2003); 11 Pages.
Brunkov et al; “Submicron-Resolved Relief Formation in Poled Glasses and Glass-Metal Nanocomposites”; Technical Physics Letters, 2008, vol. 34, No. 12 pp. 1030-1033.
Bubsey, R.T. et al, “Closed-Form Expressions for Crack-Mouth Displacement and Stress Intensity Factors for Chevron-Notched Short Bar and Short Rod Specimens Based on Experimental Compliance Measurements,” NASA Technical Memorandum 83796, pp. 1-30 (Oct. 1992).
ChemCor Product Specification.
Chinese First Office Action CN201180057659.5 dated Dec. 24, 2014, Shanghai Patent and Trademark Office, 9 Pgs.
Chinese Office Action CN201180066244.4 dated Aug. 6, 2014, Shanghai Patent and Trademark Law Office, LLC. 20 Pgs.
Chinese Patent Application No. 201611141439.1 Second Office Action dated Jun. 28, 2020; 30 Pages; Chinese Patent Office.
Chinese Patent Application No. 201810008016.5, Office Action dated Oct. 19, 2020; 20 pages (12 pages of English Translation and 8 pages of Original Document); Chinese Patent Office.
Chinese Patent Application No. 201811009613 First Office Action dated Sep. 3, 2020; 19 Pages; Chinese Patent Office.
Chinese Search Report; 201710228902.4; dated Jun. 10, 2020; 4 Page; Chinese Patent Office.
Chinese Search Report; 201810008010.8; dated Jun. 1, 2020; 5 Pages; Chinese Patent Office.
Chinese Search Report; 201811009613.6; dated Aug. 25, 2020; 4 Page; Chinese Patent Office.
CN201510895444.0 Second Office Action dated Apr. 10, 2018, China Patent Office.
CN201510895444.0 Second Office Action dated Aug. 17, 2018, China Patent Office.
Corning Incorporated, “What Makes CHEMCOR Glass Work?” ChemCor Product Specification, Feb. 1990, 2 pgs.
Corning leads $62M Investment in ‘smart’ glass maker view, Jun. 19, 2013; http://optics.org/news/4/6/27.
Corning, “Nook—Stress Profile Measurement”, Corning Incorporated, 2019, 4 slides.
Declaration of Rostislav V. Roussev; 9 Pages; Aug. 11, 2019.
Dessler et al; “Differences between films and monoliths of sol-gel derived aluminas”, Thin Solid Films, vol. 519, pp. 42-51, 2010.
Donald “Review Methods for Improving the Mechanical Properties of Oxide Glasses”; Journal of Materials Science 24 (1989) 4177-4208.
English Translation of CN201510895444.0 Notice of First Office Action dated Dec. 11, 2017; 6 Pages; Chinese Patent Office.
English Translation of CN201580044744.6 Office Action dated Jan. 22, 2019; 19 Pages; Chinese Patent Office.
English Translation of CN201611141439.1 Notice of Second Office Action dated Oct. 19, 2018; 10 Pages; Chinese Patent Office.
English Translation of CN2018100080625 Search Report dated May 9, 2020; 2 Pages; Chinese Patent Office.
English Translation of CN201810903093.7 Office Action dated Apr. 25, 2019; 14 Pages; Chinese Patent Office.
English Translation of JP2014559996 Office Action dated Feb. 7, 2017, Japan Patent Office.
English Translation of JP2017157071 Office Action dated Nov. 21, 2017, Japan Patent Office, 6 Pgs.
English Translation of KR1020177012502 Office Action dated Jun. 28, 2018, Korean Intellectual Property Office, 3 Pgs.
English Translation of KR1020197037663 Office Action dated May 2, 2020; 3 Pages; Korean Patent Office.
English Translation of TW105123002 Search Report dated May 14, 2018, Taiwan Patent Office, 1 Pg.
English Translation of TW106111688 Search Report dated Apr. 26, 2019; 1 Page; Taiwan Patent Office.
English Translation of TW107106081 Search Report dated Jun. 22, 2018, Taiwan Patent Office.
English Translation of TW107106082 Search Report dated Jun. 21, 2018, Taiwan Patent Office.
English Translation of TW108142075 Office Action dated Apr. 6, 2020; 2 Pages; Taiwan Patent Office.
European Patent Application No. 13709022.1 Office Action dated Apr. 12, 2016; 5 Pages; European Patent Office.
European Patent Application No. 15784527.2 Observations by third parties dated Feb. 18, 2020; 21 Pages European Patent Office.
European Patent Application No. 15784527.2 Observations by third parties dated Jan. 9, 2020; 1 Pages European Patent Office.
European Patent Application No. 15784527.2 Office Action dated May 10, 2019; 5 Pages; European Patent Office.
European Patent Application No. 16823100.9 Observations by third parties dated Mar. 17, 2020; 10 Pages; European Patent Office.
European Patent Application No. 16823100.9 Observations by third parties dated May 5, 2020; 10 Pages; European Patent Office.
Dusil J et al., “Black Colored Glass Ceramics Based on Beta-Quartz Solid Solutions,” Glass 1977: proceedings of the 11th International Congress on Glass, Prague, Czechoslovakia, Jul. 4-8, 1977, vol. 2, pp. 139-149.
Guo et al., “Nucleation and Crystallization Behavior of Li2O—Al2O3—SiO2 System Glass-Ceramic Containing Little Fluorine and No-Fluorine”, J.Non-Cryst.Solids, 2005, vol. 351, No. 24-26, pp. 2133-2137.
European Patent Application No. 15784527.2 Summons to attend oral proceedings pursuant to Rule 115(1) EPC dated Dec. 8, 2020; 22 Pages; European Patent Office.
Sglavo et al. “procedure for residual stress profile determination by curvature measurements” Mechanics of Materias, 2005, 37(8) pp. 887-898.
“Building Materials”, Co-edited by Xi'an University of Architecture and Technology, China Construction Industry Press, Edition 3, Apr. 30, 2004, 5 pages.
Rukmani et al., “Effects of V and Mn Colorants on the Crystallization Behavior and Optical Properties of Ce-Doped Li-Disilicate Glass”, In Journal of American Ceramic Society, vol. 90, 2007, pp. 706-711.
Related Publications (1)
Number Date Country
20210004059 A1 Jan 2021 US
Provisional Applications (2)
Number Date Country
62343320 May 2016 US
62194984 Jul 2015 US
Divisions (1)
Number Date Country
Parent 15214602 Jul 2016 US
Child 16804271 US
Continuations (1)
Number Date Country
Parent 16804271 Feb 2020 US
Child 17025602 US