Silica-containing substrates with vias having an axially variable sidewall taper and methods for forming the same

Information

  • Patent Grant
  • 11972993
  • Patent Number
    11,972,993
  • Date Filed
    Friday, May 14, 2021
    3 years ago
  • Date Issued
    Tuesday, April 30, 2024
    21 days ago
Abstract
Silica-containing substrates including vias with a narrow waist, electronic devices incorporating a silica-containing substrate, and methods of forming vias with narrow waist in silica-containing substrates are disclosed. In one embodiment, an article includes a silica-containing substrate including greater than or equal to 85 mol % silica, a first surface, a second surface opposite the first surface, and a via extending through the silica-containing substrate from the first surface toward the second surface. The via includes a first diameter at the first surface wherein the first diameter is less than or equal to 100 μm, a second diameter at the second surface wherein the first diameter is less than or equal to 100 μm, and a via waist between the first surface and the second surface. The via waist has a waist diameter that is less than the first diameter and the second diameter such that a ratio between the waist diameter and each of the first diameter and the second diameter is less than or equal to 75%.
Description
BACKGROUND
Field

The present disclosure generally relates to silica-containing substrates with vias. In particular, the present disclosure is directed to silica-containing substrates comprising at least 75 mol % silica with vias having an axially variable sidewall taper, electronic devices incorporating silica-containing substrates with vias, and methods for forming vias having an axially variable sidewall taper in silica-containing substrates.


Technical Background

Substrates, such as silicon, have been used as an interposer disposed between electrical components (e.g., printed circuit boards, integrated circuits, and the like). Metalized through-substrate vias provide a path through the interposer for electrical signals to pass between opposite sides of the interposer. Glass substrates are attractive materials that are highly advantageous for electrical signal transmission, as they have excellent thermal dimensional stability due to a low coefficient of thermal expansion (CTE), as well as very good low electrical loss at high frequencies electrical performance, and the possibility of being formed at thickness as well as at large panel sizes. In particular, high silica content substrates, such as fused silica, are even more attractive then generic glasses, as the CTE of fused silica can be extremely low (˜0.5 ppm/deg C.), and the electrical loss tangent can be even lower than in glasses that often contain significant fractions of non-silica material. However, through-via formation and metallization in high silica content substrates presents significant challenges.


Vias may be filled by an electroplating process wherein electrically conductive material (e.g., copper) is deposited on the sidewalls of the via and continuously built up until the via is hermetically sealed. Electroplating vias require an hourglass shape having a narrow waist that provides a metal “bridge” for the electrically conductive material to be initially deposited. The electrically conductive material is continuously deposited on both sides of this bridge until the via is filled.


Small-diameter vias conducive to providing electrical connections in glass interposers of electronic devices may be formed by a laser-damage-and-etch process. In this process, a damage track is initially formed in the glass substrate by using a laser to modify the glass material along the damage track. An etching solution is then applied to the glass substrate. The glass substrate is thinned by the etching solution. Because the etching rate of the glass material is faster at the damage track, the damage track is preferentially etched so that a via is opened through the glass substrate. In most glass materials, the shape of the via is preferentially an hourglass-shape conducive to electroplating. However, in silica-containing substrates with high silica content, such as fused silica, the resulting via is cylindrically shaped without a narrow waist for providing a metal bridge during the electroplating process. Such straight-walled vias in fused silica cannot be electroplated.


Accordingly, a need exists for alternative methods of forming vias with an axially variable sidewall taper (e.g., hourglass shape) in silica-containing substrates, as well as silica-containing substrates incorporating such vias.


SUMMARY

In one embodiment, a method for processing a substrate including silica, a first surface, and a second surface opposite the first surface, includes forming, using a laser beam, a damage track through the substrate from the first surface to the second surface, wherein a level of modification of the substrate along the damage track decreases in a first direction starting from the first surface toward a bulk of the substrate, and the level of modification of the substrate decreases in a second direction starting from the second surface toward the bulk of the substrate. The damage track includes a first modified segment proximate the first surface, a second modified segment proximate the second surface, and a third modified segment disposed between the first highly modified segment and the second highly modified segment, wherein a level of modification of the third modified segment is less than a level of modification of the first modified segment and the second modified segment. The method further includes etching, using an etching solution, the substrate to form a via having a first diameter at the first surface, a second diameter at the second surface, and a via waist having a waist diameter between the first surface and the second surface, wherein the waist diameter is less than the first diameter and is less than the second diameter.


In another embodiment, an article includes a silica-containing substrate including greater than or equal to 85 mol % silica, a first surface, a second surface opposite the first surface, and a via extending through the silica-containing substrate from the first surface toward the second surface. The via includes a first diameter at the first surface having a diameter of less than or equal to 100 μm, a second diameter at the second surface having a diameter of less than or equal to 100 μm, and a via waist between the first surface and the second surface. The via waist has a waist diameter that is less than the first diameter and the second diameter such that a ratio between the waist diameter and each of the first diameter and the second diameter is less than or equal to 75%.


In yet another embodiment, an electronic device includes a silica-containing substrate including greater than or equal to 85 mol % silica, a first surface, a second surface opposite the first surface, and a via extending through the silica-containing substrate from the first surface toward the second surface. The via includes a first diameter at the first surface having a diameter of less than or equal to 100 μm, a second diameter at the second surface having a diameter of less than or equal to 100 μm, and a via waist between the first surface and the second surface, wherein the via waist has a waist diameter that is less than the first diameter and the second diameter such that a ratio between the waist diameter and each of the first diameter and the second diameter is less than or equal to 75%. The electronic device further includes a semiconductor device coupled to the silica-containing substrate, wherein the semiconductor device is electrically coupled to the via.


In yet another embodiment, a substrate includes greater than or equal to 85 mol % silica, a first surface, a second surface opposite the first surface, and a damage track through the substrate from the first surface to the second surface. A level of modification of the substrate along the damage track decreases in a first direction starting from the first surface toward a bulk of the substrate, and the level of modification of the substrate decreases in a second direction starting from the second surface toward the bulk of the substrate. The damage track includes a first modified segment proximate the first surface, a second modified segment proximate the second surface, and a third modified segment disposed between the first highly modified segment and the second highly modified segment.


In yet another embodiment, an article includes a silica-containing substrate including greater than or equal to 85 mol % silica, a first surface, a second surface opposite the first surface, and a via extending through the silica-containing substrate from the first surface toward the second surface. The via includes a first diameter at the first surface having a diameter of less than or equal to 100 μm, a second diameter at the second surface having a diameter of less than or equal to 100 μm, and a via waist between the first surface and the second surface. The via waist has a waist diameter that is less than the first diameter and the second diameter such that a ratio of the difference between the first diameter and the waist diameter to one-half a thickness of the silica-containing substrate is greater than or equal to 1/15.


Additional features and advantages of the embodiments described herein 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 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 describe various embodiments and are intended to provide an overview or framework for understanding the nature and character of the claimed subject matter. The accompanying drawings are included to provide a further understanding of the various embodiments, and are incorporated into and constitute a part of this specification. The drawings illustrate the various embodiments described herein, and together with the description serve to explain the principles and operations of the claimed subject matter.





BRIEF DESCRIPTION OF THE DRAWINGS

The embodiments set forth in the drawings are illustrative and exemplary in nature and are not intended to limit the subject matter defined by the claims. The following detailed description of the illustrative embodiments can be understood when read in conjunction with the following drawings, where like structure is indicated with like reference numerals and in which:



FIG. 1 schematically depicts a partial perspective view of a silica-containing substrate as an interposer according to one or more embodiments described and illustrated herein;



FIG. 2 schematically depicts an example electronic device comprising a silica-containing substrate as an interposer disposed between electronic devices according to one or more embodiments described and illustrated herein;



FIG. 3 schematically depicts dimensional characteristics of an example via through a silica-containing substrate according to one or more embodiments described and illustrated herein;



FIGS. 4A-4E schematically depict an evolution of the formation of an example via through a silica-containing substrate according to one or more embodiments described and illustrated herein;



FIG. 5 schematically depicts a method of forming a damage track within a silica-containing substrate by scanning a laser spot through a bulk of the silica-containing substrate while modulating the intensity of the laser spot according to one or more embodiments described and illustrated herein;



FIG. 6 schematically depicts a method of forming a damage track within a silica-containing substrate by using a pulsed laser beam focused into a laser beam focal line positioned within a bulk of the silica-containing substrate according to one or more embodiments described and illustrated herein;



FIGS. 7 and 8 schematically depict sub-pulses of the pulsed laser beam depicted in FIG. 6 according to one or more embodiments described and illustrated herein;



FIGS. 9A-9C graphically depict an intensity profile of a Gauss-Bessel laser beam focal line of FIG. 6 with a maximum intensity positioned at various locations within a silica-containing substrate according to one or more embodiments described and illustrated herein;



FIGS. 10A and 10B graphically depict two different intensity profiles on the laser beam focal line depicted in FIG. 6 according to one or more embodiments described and illustrated herein;



FIGS. 11A-11C depict digital images of damage tracks within a silica-containing substrate according to one or more embodiments described and illustrated herein;



FIG. 12 depicts a digital image of a via having an hourglass shape within a silica-containing substrate formed by a laser-damage-and-etch process according to one or more embodiments described and illustrated herein;



FIGS. 13A-13C graphically depict histograms showing the distribution of a first diameter, a second diameter, and a waist diameter of vias within a silica-containing substrate formed by a laser-damage-and-etch process according to one or more embodiments described and illustrated herein;



FIGS. 14A-14C graphically depict histograms showing the distribution of circularity for a first diameter, a second diameter, and a waist diameter of vias within a silica-containing substrate formed by a laser-damage-and-etch process according to one or more embodiments described and illustrated herein;



FIGS. 15A and 15B graphically depict histograms showing waist defect and total defect for samples laser processed using a laser beam focal line at four different burst energies and three different focus settings according to one or more embodiments described and illustrated herein; and



FIGS. 16A-16C graphically depict histograms showing the via waist variation across samples laser processed using a laser beam focal line at four different burst energies and three different focus settings according to one or more embodiments described and illustrated herein.





DETAILED DESCRIPTION

Referring generally to the figures, embodiments of the present disclosure are generally related to articles comprising silica-containing substrates having vias (e.g., holes) which allow for successful downstream processing including, but not limited to, via metallization/electroplating and application of redistribution layers (RDL). The article may be for use in semiconductor devices, radio-frequency (RF) devices (e.g., antennae, electronic switches, and the like), interposer devices, microelectronic devices, optoelectronic devices, microelectronic mechanical system (MEMS) devices and other applications where vias may be leveraged.


Embodiments of the present disclosure are also generally related to methods for creating vias in silica-containing substrates. In some embodiments, the vias have geometries that facilitate electroplating the vias. Silica-containing substrates include glass and glass-ceramics. As used herein, the term “silica-containing substrate” means silica-containing substrates comprises a silica (SiO2) content greater than or equal to 75 mol %, greater than or equal to 80 mol %, greater than or equal to 85 mol %, greater than or equal to 90 mol %, greater than or equal to 91 mol %, greater than or equal to 92 mol %, greater than or equal to 93 mol %, greater than or equal to 94 mol %, greater than or equal to 95 mol %, greater than or equal to 96 mol %, greater than or equal to 97 mol %, greater than or equal to 98 mol %, greater than or equal to 99 mol %, or greater than or equal to 99.9 mol %. In some embodiments, the silica-containing substrate may be fused silica. Example silica-containing substrates include, but are not limited to, HPFS® fused silica sold by Corning Incorporated of Corning, N.Y. under glass codes 7980, 7979, and 8655. In one example, the silica-containing substrate is a substrate comprising unintentionally doped silica. The phrase “unintentionally doped” means that no additional ingredients are intentionally added to the silica prior to melting the silica.


Properties of silica make it a desirable substrate as an interposer in electronic devices. The term “interposer” generally refers to any structure that extends or completes an electrical connection through the structure, for example but not limited to, between two or more electronic devices disposed on opposite surfaces of the interposer. The two or more electronic devices may be co-located in a single structure or may be located adjacent to one another in different structures such that the interposer functions as a portion of an interconnect nodule or the like. As such, the interposer may contain one or more active areas in which vias and other interconnect conductors (such as, for example, power, ground, and signal conductors) are present and formed. The interposer may also include one or more active areas in which blind vias are present and formed. When the interposer is formed with other components, such as dies, underfill materials, encapsulants, and/or the like, the interposer may be referred to as an interposer assembly. Also, the term “interposer” may further include a plurality of interposers, such as an array of interposers or the like.


The low coefficient of thermal expansion (CTE) of silica minimizes expansion and movement of the silica-containing substrate due to the application of heat flux, such as heat flux generated by a semiconductor device that is coupled to the silica-containing substrate acting as an interposer. Expansion of the interposer due to CTE mismatch between the interposer and a semiconductor device (or other electronic component) may cause the bond between the interposer and the semiconductor to fail and result in separation or other damage.


Additionally, silica-containing substrates provide desirable RF properties over other substrates such as silicon. Desirable RF properties may be important in high frequency applications, such as high-speed data communications applications.


Thus, silica-containing substrates comprising greater than or equal to 75 mol %, 80 mol %, 85 mol %, 90 mol %, 95 mol %, or 99 mol % silica (SiO2) may be a desired material in an interposer in particular electronics devices. However, use of silica-containing substrates presents challenges when particular geometries of the via are desired, including but not limited to, hourglass-shaped vias. Hourglass-shaped vias facilitate metalizing the vias by an electroplating process. During the electroplating process, electrically conductive material (e.g., copper, silver, aluminum, titanium, gold, platinum, nickel, tungsten, magnesium, or any other suitable material) is deposited within a via. An hourglass-shaped via has a narrow waist having a diameter that is less than a diameter of openings at the surfaces of the interposer. In the electroplating process, deposited metal forms a metal bridge at the waist location first, and then metal is deposited on the bridge to finish filling the via to enable a void-free hermetic filling of via.


Laser-damage-and-etch techniques may be utilized to form vias in silica-containing materials. However, conventional laser-damage-and-etch techniques used to form vias within silica-containing substrates as defined herein result in substantially cylindrical vias (i.e., vias with substantially straight walls). Therefore, electroplating of vias formed in silica-containing substrates may not be possible using conventional techniques because of the lack of a narrow waist and the ability for the formation of a metal bridge. The inability to produce vias having a narrow waist in silica-containing substrates may be due to the low etch rate of in hydrofluoric acid, and that the etching process results in no non-soluble by-products which clog or inhibit etching within the middle of the substrate and lead to a differential etch rate between the hole at the surface versus deep inside the silica-containing substrates. It is noted that the methods disclosed herein are not limited to silica-containing substrate comprising greater than or equal to 75 mol % silica (SiO2). The methods disclosed herein may also be used on glass or glass-ceramic substrates having less than 75 mol % silica. For example, the methods described herein may also be utilized to form narrow-waist vias in glass or glass-ceramic substrates having less than 75 mol % silica (SiO2), such as Eagle XG® glass and Gorilla® Glass sold by Corning Incorporated.


Embodiments described herein are directed to methods and articles comprising silica-containing substrates having vias formed by a laser-damage-and-etch process that include a particular interior wall geometry, such as an interior wall having a plurality of regions that each have a distinctive angle thereby defining an “hourglass” shape. Embodiments provide for high quality hourglass-shaped vias in silica-containing substrates that are formed practically and reliably. Various embodiments of articles, semiconductor packages, and methods of forming a via with a narrow waist in a substrate are described in detail below.


Referring now to FIG. 1, an example article comprising a silica-containing substrate 100 is schematically depicted in a partial perspective view. The silica-containing substrate 100 comprises a first surface 102 and a second surface 104 opposite from the first surface 102. A plurality of vias 110 extends through the bulk of the silica-containing substrate 100 from the first surface 102 to the second surface 104. It should be understood that any number of vias 110 may extend through the silica-containing substrate 100 in any arrangement. The thickness t of the silica-containing substrate 100 may be any appropriate thickness depending on the application. As non-limiting examples, the thicknesses t of the silica-containing substrate is within the range of 50 μm and 1 mm including endpoints, within a range of 100 μm and 700 μm including endpoints, within a range of 100 μm and 500 μm including endpoints, or within a range of 250 μm to 500 μm including endpoints.


A pitch of the vias 110, which is the center-to-center spacing between adjacent vias 110, may be any dimension according to the desired application, such as, without limitation, about 10 μm to about 2,000 μm, including about 10 μm, about 50 μm, about 100 μm, about 250 μm, about 1,000 μm, about 2,000 μm, or any value or range between any two of these values (including endpoints). In some embodiments, the pitch may vary between vias 110 on the same silica-containing substrate 100 (i.e., the pitch between a first via and a second via may be different from a pitch between the first via and a third via). In some embodiments, the pitch may be a range, such as about 10 μm to about 100 μm, about 25 μm to about 500 μm, about 10 μm to about 1,000 μm, or about 250 μm to about 2,000 μm.


The silica-containing substrate 100 may be an interposer of an electronic device 200 as schematically illustrated in FIG. 2. The non-limiting electronic device 200 schematically illustrated in FIG. 2 comprises a first electrical component 201 coupled to the first surface 102 of the silica-containing substrate 100 and a second electrical component 203 coupled to a second surface 104 of the silica-containing substrate 100. The first electrical component 201 and the second electronic device 203 may be configured as any type of electrical component, such as, without limitation, a semiconductor device, a substrate, a power source, or an antenna. The silica-containing substrate 100 includes a plurality of metalized vias 110 that electrically couple the first electrical component 201 to the second electrical component 203 such that electrical signals and/or electrical power may pass therebetween.


An example electrically conductive via 110 through a silica-containing substrate 100 having an hourglass-shaped profile is schematically depicted in FIG. 3. The via 110 has a first diameter D1 at the first surface 102, and a second diameter D2 at the second surface 104. The example via 110 further includes a longitudinal axis LA along a length of the via 110, an interior wall 111, and a waist w having a waist diameter Dw that is the smallest diameter of the via 110. Thus, the waist diameter Dw is smaller than both the first diameter D1 and the second diameter D2. As non-limiting examples, the profile of the via 110 is such that the waist diameter dw is less than 75%, less than 65%, less than 60%, less than 55%, less than 50%, less than 50%, less than 45%, less than 40%, less than 35%, less than 30%, less than 25%, less than 20%, less than 15%, less than 10%, or less than 5% of each of the first diameter D1 and the second diameter D2. Furthermore, if the etching time is reduced, then the holes from the two surfaces will fail to connect, leading to “blind” vias, which are vias that terminate in the bulk of the substrate. As non-limiting examples, post etching, the first diameter D1 and the second diameter D2 are within the range of 5 μm to 150 μm including end points, 5 μm to 100 μm including end points, 20 μm to 150 μm including endpoints, 30 μm to 60 μm including endpoints, or 40 μm to 50 μm including endpoints. In some embodiments, the first diameter D1 and the second diameter D2 are less than or equal to 100 μm, 90 μm, 80 μm, 70 μm, 60 μm, 50 μm, 40 μm, 30 μm, 20 μm, or 10 μm. The first diameter D1 may or may not be equal to the second diameter D2.


The example via 110 of FIG. 3 has four distinct tapered regions: a first tapered region 112, a second tapered region 113, a third tapered region 118 and a fourth tapered region 119. The example via 110 has four different taper angles: a first angle θ1, a second angle θ2, a third angle θ3, and a fourth angle θ4 corresponding to the first tapered region 112, the second tapered region 113, the third tapered region 118, and the fourth tapered region 119, respectively. The example via 110 is further characterized by four segments lengths: a first segment length L1 extending from the first surface 102 to the transition to the second tapered region 113, a second segment length L2 extending from the transition between the first tapered region 112 and the second tapered region 113 to the waist w, a third segment length L3 extending from the waist w to the transition between the third tapered region 118 and the fourth tapered region 112, and a fourth segment length L4 extending from the transition between the third tapered region 118 and the fourth tapered region 119 and the second surface 104.


The first through fourth segment lengths L1-L4 may be any appropriate lengths and are not limited by this disclosure. In the example of FIG. 3, each of the four segment lengths is different from one another. However, embodiments are not limited thereto. For example, the first segment length L1 may be equal to the fourth segment length L4 and/or the second segment length L2 may be equal to the third segment length L3.


It is noted that the taper angles shown in FIG. 3 are measured between respective reference lines parallel to the longitudinal axis LA and the interior wall 111 of the via 110. The first angle θ1 is measured from the interior wall 111 of the first tapered region 112 to the longitudinal axis LA. The second angle θ2 is measured from the interior wall 111 of the second tapered region 113 to the longitudinal axis LA. The third angle θ3 is measured from the interior wall 111 of the third tapered region 118 to the longitudinal axis LA. The fourth tapered angle θ4 is measured from the interior wall 111 of the fourth tapered region 112 to the longitudinal axis LA.


The angles of the via 110 with respect to the longitudinal axis LA may be determined by forming a traced line TL that matches the contour of the interior wall 111 of the particular tapered region. The traced line may then be analyzed to determine the slope of one or more portions of the interior wall 111 (including the various tapered regions 112, 113, 118, 119). For example, as depicted in FIG. 3, the traced line TL is graphically depicted and the computer software described herein is used to determine one or more linear regions of the traced line TL. A linear region is defined as follows: (1) the length of the region is no less than 5 μm, and may generally be greater than 10 μm; (2) the region can be fit to a linear function (y=a+bx) wherein y is the radius of the hole and x is the depth of the substrate, with the absolute value of the fit residual less than 1 μm; and (3) the slope of the fit function for any adjacent region should be different by at least 0.01, which translates to a 0.57 degree difference in terms of tapered angle. A region meeting all of the criteria described above is referred to as a region having a constant slope (i.e., a linear region). As shown in FIG. 3, the traced line TL has four distinct linear regions: the region between points A and B, the region between points B and C, the region between points C and D, and the region between points D and E. As such, the slope of the regions between points A and B, between points B and C, between points C and D, and between points D and E is constant. However, there may be areas of the traced line TL surrounding each points A, B, C, D, and E that have non-constant slope. These areas may be transition areas between the areas of constant slope, as described in greater detail herein. Such areas may occur where there is a gradual transition between tapered regions.


The transition area between the slope of each of the tapered regions may occur in any instance where a region of constant slope of the interior wall 111 ends. Referring briefly to FIG. 12, a via 510 formed within a silica-containing substrate that comprises a first tapered region 512 between points A and B, a second tapered region 513 between points C and D, a third tapered region 518 between points E and F, and a fourth tapered region 519 between points G and H is graphically depicted. The example via 510 has transition areas with non-constant slope that are the regions of the traced line 1415 between points B and C, between points D and E, and between points F and G. In some embodiments, the slope of the transition area varies from the slope of the region of constant slope by greater than or equal to about 0.57 degrees, greater than or equal to about 1 degree, greater than or equal to about 2 degrees, greater than or equal to about 3 degrees, greater than or equal to about 4 degrees, or greater than or equal to about 5 degrees.


As noted above, the constant slope of each tapered region may be defined by an angle relative to the longitudinal axis LA of the via, which is generally perpendicular to the first surface 102 and/or the second surface 104. Referring once again to FIG. 3, each of the first angle θ1 and the fourth angle θ4 is smaller than each of the second angle θ2 and the third angle θ3 due to the strongly modified material proximate the first surface 102 and the second surface 104 of the silica-containing substrate 100, and the more weakly modified material in the bulk region of the silica-containing substrate 100. As an example and not a limitation, each of the first angle θ1 and the fourth angle θ4 is less than 5 degrees, for example in a range from greater than 0 degrees and 5 degrees, greater than 0 degrees and 4 degrees, greater than 0 degrees and 3 degrees, greater than 0 degrees and 2 degrees, 1 degree and 5 degrees, 1 degree and 4 degrees, 1 degree and 3 degrees, 1 degree and 2 degrees, 2 degrees and 5 degrees, 2 degrees and 4 degrees, 2 degrees and 3 degrees, or 4 degrees, 3 degrees, 2 degrees, or 1 degree. In the example of FIG. 3, each of the tapered angles is different from one another. However, embodiments are not limited thereto. For example, the first angle θ1 and the fourth angle θ4 may be equal to one another, and/or the second angle θ2 and the third angle θ4 may be equal to one another.


As noted above, waist w is the region of the via having the smallest diameter (D). The vias 110 through substrates described herein may be characterized by a ratio of the difference between the first diameter (or the second diameter) and the waist diameter to one-half a thickness of the silica-containing substrate is greater than or equal to 1/15, as provided in the following relationship:









d
1

-

d
w



1
/

2
t






1
15

.





The via 110 may be filled with an electrically conductive material by any known or yet-to-be-developed process, such as sputter, electroplating or paste filling. The electrically conductive material may be any suitable material, such as, without limitation, copper, silver, aluminum, titanium, gold, platinum, nickel, tungsten, or magnesium.


Referring now to FIGS. 4A-4E, a laser-damage-and-etch process and an evolution of the fabrication of a via 110 with an axially variable sidewall taper in a silica-containing substrate 100 having an initial thickness ti are schematically illustrated. Referring to FIG. 4A, a damage track 120 is formed using a laser beam through a bulk of the silica-containing substrate 100 from the first surface 102 to the second surface 104. As an example and not a limitation the damage track 120 has a diameter that is less than or equal to 1 μm. The laser beam modifies the material along the damage track 120. As used herein, the terms “modify” or “modification” with respect to the silica-containing substrate means a change in refractive index, a change in material density, melting, compacting, ablation, or chemical alteration of the material. The modification may also include cracking of the material to create microscopic fissures or voids that can facilitate the penetration of gaseous or liquid etchant. The laser beam forms the damage track 120 such that the damage track 120 has segments providing different etching properties. A level of modification of the silica-containing substrate 100 is strongest proximate the first surface 102 and the second surface 104, and the level of modification decreases in a direction into the bulk of the silica-containing substrate 100 along the damage track 120. The level of modification affects the etching rate of the silica-containing substrate 100. The higher the level of modification, the faster the etch rate of the silica-containing substrate 100. In embodiments described herein, a level of modification is determined by evaluating the damage track 120 under a microscope in the presence of backlighting. In the presence of backlighting, the darker the material along the damage track 120 the higher the level of modification. In embodiments, the damage track 120 appears darker near the surfaces of the silica-containing substrate 100 (i.e., the damage track has a high level of modification in these segments), and appears lighter near the middle of the silica-containing substrate 100 (i.e., the damage track has a low level of modification in these segments as compared to the segments proximate the surfaces). FIG. 11A, which is described in more detail below, illustrates the appearance of varying levels of material modification of damage tracks 120, 120′, 120″ in a backlit silica-containing substrate 100 under a microscope.


In the example of FIG. 4A, the damage track 120 includes four segments each having a different level of modification and therefore different etching properties: a first modified segment 120A, a second modified segment 120B, a third modified segment 120C, and a fourth modified segment 120D. It should be understood that the level of modification between the various segments may not be discrete. Rather, the level of modification may gradually vary along damage track 120. Thus, the level of modification may vary within the individual segments of the damage track 120.


As noted above, the damage track 120 is configured such that the highest level of modification occurs proximate the first surface 102 and the second surface 104 of the silica-containing substrate 100. Therefore, the first modified segment 120A and the fourth modified segment 120D are highly modified segments. The second modified segment 120B and the third modified segment 120C are minimally modified segments in that they have a level of modification that is less than that of the first segment 120A and the fourth segment 120D. Although the second segment 120B and the third segment 120C are illustrated as individual segments, in some embodiments, the second segment 120B and the third segment 120C are a single, minimally modified segment having a level of modification that is less than the level of modification of first modified segment 120A and fourth modified segment 120D.


Details regarding laser beam properties utilized to form the damage track are discussed below with respect to FIGS. 5-8.


After forming the damage track 120, the silica-containing substrate 100 is etched by application of an etching solution. In an example, the silica-containing substrate 100 is disposed in a bath of etching solution. Alternatively, the etching solution may be sprayed onto the silica-containing substrate 100. The type of etching solution is not limited by this disclosure. Any known or yet-to-be-developed etching solution capable of etching silica-containing substrates may be utilized. In one example, the etching solution comprises hydrofluoric acid (HF) or sodium/potassium hydroxide. As a particular example, an etching solution for etching fused silica includes 20% HF by volume or 20% HF with 12% HCl by volume at about 47 degrees Celsius provides an etch rate of about 0.005 μm/second. Temperature adjustments (e.g., 10 degrees Celsius to 50 degrees Celsius) and acid concentration adjustments may be made to change the etch rate. Other mineral acids may be substituted for HCl, such as nitric acid (HNO3). It is also possible to use hydroxide etchants, such as sodium hydroxide (NaOH) and potassium hydroxide (KOH).


The etching solution etches away material at each of the first surface 102 and the second surface 104 of the silica-containing substrate 100 by an amount Δs as shown in FIG. 4B. The material damaged within the strongly modified first segment 120A and fourth segment 120D of the damage track 120 are etched at a faster rate than the non-damaged regions outside of the damage track 120. This faster etch rate due to the damaged material causes a first pilot hole 115 to open at the first surface 102 and extend through a bulk of the silica-containing substrate 100 along the first segment 120A of the damage track, and a second pilot hole 117 to open at the second surface 104 and extend through the bulk of the silica-containing substrate 100 along the fourth segment 120D of the damage track 120. As shown in FIG. 4C, the first pilot hole 115 and the second pilot hole 117 extend deeper into the bulk of the silica-containing substrate 100, and the silica-containing substrate 100 is further thinned by an increased amount Δs.


Referring now to FIG. 4D, the continued etching of the silica-containing substrate 100 causes a diameter of the first pilot hole 115 to increase and open into a first tapered region 112, and a diameter of the second pilot hole 117 to increase and open into a fourth tapered region 119. The first surface 102 and the second surface 104 of the silica-containing substrate 100 is further thinned by an increased amount Δs. By this time, the etching solution reaches the second segment 120B and the third segment 120C of the damage track 120. The second segment 120B opens into a second tapered region 113, and the third segment 120C opens into a third tapered region 118. Because the level of modification of the material is lower in the second segment 120B and the third segment 120C than the first segment 120A and the fourth segment 120D, the etch rate is slower in the second segment 120B and the third segment 120C than the first segment 120A and the fourth segment 120D. As shown in FIG. 4D, the differences in the level of modification along the damage track 120 causes the angle of the second tapered region 113 and the third tapered region 118 with respect to the longitudinal axis LA to be larger than the angle of the first tapered region 112 and the fourth tapered region 119.


The second tapered region 113 and the third tapered region 118 meet at a waist w. The waist w is the narrowest region of the via 110, and is the location where a metal bridge forms during the electroplating process. Referring now to FIG. 4E, a completed example via 110 within a fused substrate having a final thickness tF is shown. As shown, the via 110 has an axially variable sidewall taper that results in distinct segments, as well as a narrow waist w providing a location for a metal bridge to form during the electroplating process.


The damage tracks 120 described herein having varying levels of modification of the silica-containing substrate 100 may be formed by a variety of laser processes. In an example illustrated by FIG. 5, the damage track 120 is formed in the silica-containing substrate 100 by scanning a focused laser spot LS of a laser beam 150 through the thickness t of the silica-containing substrate 100 in a direction z, with the power of the laser beam being modulated during the scan as shown by graph 152 to create different levels of material modification (i.e., damage) at different depths from the surfaces of the silica-containing substrate 100. The laser power is lower when the focused laser spot LS is within a bulk of the silica-containing substrate 100 (i.e., near the middle) than when the focused laser spot LS is positioned close to the first surface 102 and the second surface 104 of the silica-containing substrate 100. However, this method would require many sequential laser exposures to form the damage track 120 through the full thickness of the silica-containing substrate 100, which may make the process slow.


Referring to FIG. 6, in another example, the damage track 120 is formed by a pulsed laser beam 302a that is focused into a laser beam focal line 302b that is positioned through the bulk of the silica-containing substrate 100. The laser beam focal line generates an induced multi-photon absorption within the silica-containing substrate 100. The multi-photon induced absorption produces a material modification within the silica-containing substrate along the laser beam focal line 302b, thereby forming the damage track 120. The laser beam focal line 302b is created by optics 306, which as a non-limiting example depicted in FIG. 6, is a conical lens (i.e., an axicon). Additional description of methods for generating and using a laser beam focal line for drilling glass substrates is provided in U.S. Pat. No. 9,517,963, which is incorporated by reference herein in its entirety.


The optics 306 form the laser beam into an extended focus, or quasi-non-diffracting beam resulting in a Bessel-like or Gauss-Bessel beam. Because of the quasi-non-diffracting nature of the beam, the light maintains a tight focused intensity over a much longer range than is achieved with more commonly used Gaussian beams, allowing the full thickness t of the glass substrate to be damaged by a single burst pulse or a closely timed burst train of laser pulses.


To modify the silica-containing substrate and create the damage track, the wavelength of the pulsed laser beam should be transparent to the silica-containing substrate material. The pulse duration and intensity should be short enough to achieve the multi-photon absorption effect described above. Ultra-short pulse lasers may be utilized, such as picosecond or femtosecond laser sources. In some embodiments, a ˜10 picosecond pulsed laser may be utilized. As an example and not a limitation, with a line focus of between about 1 mm and about 3 mm extent, and a ˜10 picosecond pulsed laser that produces output power of greater than about 50 W at a repetition rate of 200 kHz (250 μJ/pulse), then the optical intensities in the line region can be high enough to create non-linear absorption in the silica-containing substrate.


Note that the operation of such a picosecond laser described herein creates a “pulse burst” 5 sub-pulses 5a. FIG. 7 depicts three sub-pulses 5a, 5a′, and 5a″ (collectively “5a”). Producing pulse bursts is a type of laser operation where the emission of pulses is not in a uniform and steady stream but rather in tight clusters of sub-pulses. Each pulse burst contains multiple individual sub-pulses 5a (such as, without limitation, at least 2 sub-pulses, at least 3 sub-pulses, at least 4 sub-pulses, at least 5 sub-pulses) of very short duration. That is, a pulse bust 5 is a “pocket” of sub-pulses 5a, and the pulse bursts 5 are separated from one another by a longer duration than the separation of individual adjacent pulses within each burst. Referring to FIG. 8, which plots laser emission against time for sub-pulse 5a of FIG. 7, sub-pulses have may have a pulse duration Td of up to 100 psec (for example, 0.1 psec, 5 psec, 10 psec, 15 psec, 18 psec, 20 psec, 22 psec, 25 psec, 30 psec, 50 psec, 75 psec, or therebetween). These individual sub-pulses (e.g., sub-pulses 5a, 5a′, and 5a″) within a single pulse burst 5 are referred to as sub-pulses herein to denote the fact that they occur within a single pulse burst. The energy or intensity of each individual sub-pulse 5a. 5a′, 5a″ within the pulse burst 5 may not be equal to that of other sub-pulses within the pulse burst, and the intensity distribution of the multiple sub-pulses within a pulse burst often follows an exponential decay in time governed by the laser design.


Each sub-pulse (e.g., sub-pulses 5a, 5a′, 5a″) within the pulse burst 5 of the exemplary embodiments described herein are separated in time from the subsequent sub-pulse in the burst by a duration tp from 1 nsec to 50 nsec (e.g. 10-50 nsec, or 10-30 nsec, with the time often governed by the laser cavity design). For a given laser, the time separation tp between each sub-pulses (sub-pulse-to-sub-pulse separation) within a pulse burst 5 is relatively uniform (±10%). For example, in some embodiments, each sub-pulse within a pulse burst may be separated in time from the subsequent sub-pulse by approximately 20 nsec (50 MHz). For example, for a laser that produces a sub-pulse separation tp of about 20 nsec, the sub-pulse-to-sub-pulse separation tp within a pulse burst is maintained within about ±10%, or is about ±2 nsec.


It has been observed that too many sub-pulses results in a cylindrically shaped via. Particularly, a fifteen sub-pulse burst providing 80 μJ of energy produced a cylindrically shaped via, while a five sub-pulse burst providing 50 μJ produced an hourglass shaped via. The former has a lesser energy per sub-pulse, but will create a very uniform damage track through the thickness of the silica-containing substrate, whereas the latter has a greater energy per sub-pulse but will create a more non-uniform damage track through the thickness of the silica-containing substrate, with stronger damage being observed near the glass surfaces and weaker damage being observed near the middle of the silica-containing substrate.


The laser beam focal line 302b typically has a uniform intensity. However, in the embodiments described herein, the amount of energy and the number of laser beam bursts are controlled to provide for non-uniform levels of modification along the desired damage track 120. In other words, the damage pattern as a function of depth within the silica-containing substrate 100 is not uniform. What is observed is that the amount of material modification near the surfaces of the silica-containing substrate 100, in particular within 100 μm of each surface, is significantly different and stronger than the damage in the middle (center) of the silica-containing substrate 100. As observed under a microscope with back-lighting, the regions near the surfaces of the silica-containing substrate 100 typically appear very dark, indicating greater optical scattering and material modification, whereas the regions near the center of the silica-containing substrate 100 appear as light colored or broken up dark regions, indicating less light scattering and hence weaker or less spatially consistent material modification. In addition, the regions near the surfaces of the silica-containing substrate 100 will often exhibit actual holes, or regions where material has been ejected/ablated from the substrate, which can provide an easy path for chemical etchant to penetrate.


This effect of stronger damage near the surfaces is particularly evident as the laser energy of the laser beam focal line 302b is reduced to just above the threshold need to modify the silica-containing substrate 100, such as within 60% above the threshold, within 65% above the threshold, within 55% above the threshold, within 50% above the threshold, within 45% above the threshold, within 40% above the threshold, within 35% above the threshold, within 30% above the threshold, within 25% above the threshold, within 20% above the threshold, within 15% above the threshold, or within 10% above the threshold. As used herein, the term “threshold” means a minimum energy needed to create surface damage on the substrate using a laser beam focal line. In such a situation, the regions closest to the surfaces will still exhibit dark damage regions, but the middle of the silica-containing substrate will in some cases show no obvious damaged or modified regions at all. As described above, this differential damage effect as a function of depth observed with non-diffracting beams may be taken advantage of to form tapered vias in silica-containing substrate where such vias shapes are not otherwise possible. As non-limiting examples, an operating range of the pulsed laser beam is within a range of 40 μJ to 55 μJ including endpoints, or within 45 μJ to 50 μJ including endpoints for five sub-pulses.


It is possible to shift the location of the waist w of the via by altering the position of the maximum intensity of the laser beam focal line. FIG. 9A plots the intensity 305 of the laser beam focal line through the silica-containing substrate 100, and illustrates resulting vias 410 in an example silica-containing substrate 400. As shown in FIG. 9A, positioning the maximum intensity 305 at the center of the silica-containing substrate 100 results in vias 410 have a waist in the center of the silica-containing substrate 400 after the etching process.



FIG. 9B graphically illustrates a shift of the maximum intensity 305 of the laser beam focal line to the first surface 102 of the silica-containing substrate 100. FIG. 9B further illustrates an example silica-containing substrate 400′ with vias 410′ following an etching process having a waist that is closer to the second surface 404 than the first surface 402. FIG. 9C graphically illustrates a shift of the maximum intensity 305 of the laser beam focal line to the second surface 104 of the silica-containing substrate 100. FIG. 9C further illustrates an example silica-containing substrate 400″ with vias 410″ following an etching process having a waist that is closer to the first surface 402 than the second surface 404. Shifting the waist w leads to an asymmetrical via about a plane through a center of the silica-containing substrate 100.


It is noted that it is not required to make the optical intensity of the quasi-non-diffracting beam (e.g., the laser beam focal line 302b) stronger near the surfaces of the silica-containing substrate 100. However, it is possible to design optics, such as waxicon-like elements, which create custom optical energy distributions along the beam propagation direction. In such a case, the optical intensity of the laser beam focal line 302b may be enhanced near the fused substrate surfaces, while creating a lower intensity region in the middle of the silica-containing substrate. Example optics for customizing the energy distribution of a laser beam focal line are described in U.S. Pat. Appl. No. 62/381,345.



FIGS. 10A and 10B graphically depict manipulation of the intensity profiles of two laser beam focal lines through a silica-containing substrate 100. In FIG. 10A, the intensity profile 305′ of the laser beam focal line has rectangular, “top hat” shape. This intensity profile 305′ may be formed by waxicon optics, for example, and may result in stronger modification proximate the surfaces of the silica-containing substrate than the Gaussian profile depicted in FIGS. 9A-9C. In the intensity profile 305″ depicted in FIG. 10B has two maximum peaks proximate the first surface 102 and the second surface 104 of the silica-containing substrate 100, which results in stronger modification proximate the first surface 102 and the second surface 104 than in the middle of the silica-containing substrate. The laser beam focal line of FIG. 10B has a greater intensity at a first end of the laser beam focal line and a second end of the laser beam focal line than a center region of the laser beam focal line. Custom optics may be employed to create the intensity profile 305″ depicted in FIG. 10B.


Other approaches to enhance the laser damage/modification near the surfaces of the silica-containing substrates include heating or cooling the surfaces to have a temperature gradient, such as through application of hot air flow, and thus in turn to have differential laser/glass interaction through the glass thickness.


Example

A 50 mm×50 mm Corning code 7980 fused silica substrate with 0.36 mm thickness was laser damaged using a system equipped with a Coherent Hyper-Rapid-50 picosecond laser operating at 532 nm wavelength. The beam delivery optics were configured to create a Gauss-Bessel laser beam focal line, with an optical intensity distribution along the beam propagation axis of 0.74 mm full-width half maximum, and a spot size of 1.2 μm in diameter, as measured by the diameter of the first nulls or intensity minimums in the Bessel-like cross sectional profile of the beam. Each damage track was formed by exposing the silica-containing substrate to a 50 μJ laser burst that contained five laser pulses, each had a duration of 7.2 psec and the time interval between the pulses inside each burst was 20 ns. The laser-processed silica-containing substrate was then etched in a static (no physical agitation, no ultrasound) bath with 20% HF (vol %) and 12% HCl (vol %) at 47° C. The bulk etch rate was 0.0046 μm/s-0.005 μm/s.



FIG. 11A show images of the resulting damage tracks 120, 120′ and 120″ made in the 0.36 mm thick fused silica substrate at low magnification with the sample under back lighting prior to etching. The lateral spacing (i.e., pitch) of the damage tracks in the image of FIG. 11A is 150 μm. It is clear from the optical microscope image of FIG. 11A that each damage track has more strongly modified sections (the darker linear features in the optical microscope image, above and below the two horizontal dash lines) near the first surface 102 (a first modified section) and the second surfaced 104 (a second modified section), and a weaker third modified section in the middle of the glass (the lighter linear features in the optical microscope image, between the two horizontal dash lines). Thus the level of modification for the third modified section is less than the level of modification for the first modified section and the second modified section. The differences are more clearly revealed in the high magnification images of FIG. 11B (first surface 102) and of FIG. 11C (second surface 104).


The damage tracks 120, 120′, 120″ each have at least a first segment 120A, 120A′, 120A″, a second segment 120B, 120B′, 120B″, and a third segment 120C, 120C′, 120C″.


It is noted that the differences in the damage track intensity are not explained by optical intensity differences created by the quasi-non-diffracting beam (Gauss-Bessel) forming optics. The focal line intensity was measured using a high NA microscope objective and a CCD camera scanned along the optical axis, and shown to closely follow a Gauss-Bessel intensity profile. The position of the focus was set to achieve near maximum intensity near the center of the silica-containing substrate, with slightly diminished intensity near each of the surfaces. The expected intensity variation for this focal line through depth of the 0.35 mm thick glass is approximately 6-8%.



FIG. 12 shows a side view optical microscopy image of an etched via 510 following the etching process of the example. As shown, the via 110 has an hourglass shape with a narrow waist w. The via 510 has an interior wall profile similar to example via 110 schematically depicted in FIG. 5. Referring to FIGS. 5 and 12, the via 510 has the following interior wall profile: θ14=10, θ23=8°; L1=L4=62 μm, L2=L3=88 μm; first diameter D1=49.5 μm; second diameter D2=51.2 μm; and Dw=25.7 μm. In this case, the damage track is approximately symmetric about the middle plane of the fused substrate thickness and results in a symmetrical via about a horizontal centerline, as oppose to the case illustrated in FIG. 3.


The silica-containing substrate made with this process exhibited very low via-to-via variation at the part level. This indicates the process is stable and not unduly influenced by any small variations in laser energy or system focus. Both the diameter and the circularity are very well controlled for top, waist and bottom of 10000 vias, as shown in FIGS. 13A-13C and 14A-14C. FIG. 13A is a histogram showing the first diameter, FIG. 13B is a histogram showing the second diameter, and FIG. 13C is a histogram showing the waist diameter for a number of holes as indicated in each graph. Dimensional control is shown to be better than +/−1% for first diameter, +/−2.5% for second diameter, and +/−6% for waist diameter.


Another metric for via quality is circularity, which may be measured for the first diameter (FIG. 14A), the second diameter (FIG. 14B), and the waist diameter (FIG. 14C) of each via. As used herein, circularity is determined by fitting a circle to a microscope image of the via. Taking H={h1, h2, . . . , hn) to be a collection of points hi=(xi, yi) identified along the edge of the via at the first diameter, second diameter, or waist diameter as viewed from above (e.g., from a microscope image of the via at the respective diameters). The points may be, without limitation, at a resolution of approximately 1 μm per pixel. Exactly one least squares fit circle can be evaluated. The center point of this circle C=(xc, yc) and its radius R minimize the quantity












i
=
1

n




(





(


x
c

-

x
i


)

2

+


(


y
c

-

y
i


)

2



-

R
2


)

.






Given the set of distances (diameters) di=dist(hi, C), a minimum value dmin and a maximum value dmax can be found. The difference dmax−dmin is referred to here as circularity. Thus, a theoretically perfect circle, for which all distances d, are equal, will have equivalent values of dmin and dmax leading to a circularity value of zero. Larger values of circularity are indicative of less round holes.



FIG. 15A is a histogram of waist defect for samples with four different burst energies. A via with too large a circularity is a via that is too elliptical or poorly formed. FIG. 15B is a histogram for total defects (blind vias, vias with greater than 5 μm entrance or second diameters, or waist circularity greater than 5 μm) for samples with four different burst energies. FIG. 16A (mean) and FIG. 16B (standard deviation) are histograms showing via waist variation across a part for samples made with different burst energies and focus conditions. FIG. 16C is a histogram showing a ratio between waist diameter and first diameter for different burst energies and focus conditions.


As shown in FIGS. 15A and 15B and FIGS. 16A-16C, as defined by the percentage of vias that have circularities exceeding 5 μm, parts made by this process also have extremely low defect rate, within a reasonable process window (FIGS. 15A and 15B), and the waist opening only has a small variation within a process window (FIGS. 16A-16C), both indicating that the process is stable. Additionally, FIGS. 16A-16C show that a 35%-45% waist diameter/first diameter ratio can be achieved using 5 μJ energy and 100 μm process window.


It should now be understood that embodiments described herein provide a methods and articles providing hourglass-shaped vias in silica-containing substrates, such as high purity silica-containing substrates. The hourglass-shaped vias may be metalized using an electroplating process, for example. The hourglass-shaped vias are formed by a laser-damage-and-etch process by which a customized damage track in formed in the silica-containing substrate prior to etching. The damage track has stronger material modification proximate the surfaces of the silica-containing substrate than in the bulk/middle of the silica-containing substrate. The customized damage track results in an etched via having tapered regions defining a waist. The waist may act as a metal bridge to grow an interior metal layer within the via. Silica-containing substrates with hourglass-shaped vias may be used as interposers in electronic devices, such as high-frequency electronic devices.


It will be apparent to those skilled in the art that various modifications and variations can be made to the embodiments described herein without departing from the spirit and scope of the claimed subject matter. Thus it is intended that the specification cover the modifications and variations of the various embodiments described herein provided such modification and variations come within the scope of the appended claims and their equivalents.

Claims
  • 1. An article comprising: a silica-containing substrate comprising greater than or equal to 75 mol % silica, a first surface, a second surface opposite the first surface and at least one via extending through the silica-containing substrate from a first opening at the first surface a second opening at the second surface, the at least one via comprising: a first opening diameter at the first surface less than 100 μm;a second opening diameter at the second surface less than 100 μm;a longitudinal axis along a length of the via;an interior wall;a via waist between the first surface and the second surface, wherein the via waist has a waist diameter than is less than the first opening diameter and the second opening diameter such that a ratio between the waist diameter and each of the first opening diameter and the second opening diameter is less than or equal to 75%;a first tapered region extending from proximate the first opening at the first surface toward the via waist and comprising a first axial length, the first tapered region comprising a substantially constant slope having a first angle measured between the interior wall within the first tapered region and a line intersecting the interior wall within the first tapered region and parallel to the longitudinal axis;a second tapered region extending from proximate the first tapered region to proximate the via waist and comprising a second axial length, the second tapered region comprising a substantially constant slope having a second angle measured between the interior wall within the second tapered region and a line intersecting the interior wall within the second tapered region and parallel to the longitudinal axis;a third tapered region extending from proximate the via waist toward the second surface and comprising a third axial length, the third tapered region comprising a substantially constant slope having a third angle measured between the interior wall within the third tapered region and a line intersecting the interior wall within the third tapered region and parallel to the longitudinal axis; anda fourth tapered region extending from proximate the third tapered region to proximate the second opening at the second surface and comprising a fourth axial length, the fourth tapered region comprising a substantially constant slope having a fourth angle measured between the interior wall within the fourth tapered region and a line intersecting the interior wall within the fourth tapered region and parallel to the longitudinal axis,wherein each of the first angle and the fourth angle is greater than 0 degrees and less than or equal to 5 degrees,wherein each of the first angle and fourth angle is less than each of the second angle and the third angle, andwherein the first angle is different from the fourth angle such that the first axial length is less than the fourth axial length and the second angle is different from the third angle such that the third axial length is less than the second axial length.
  • 2. The article of claim 1, wherein the silica-containing substrate comprises at least 90 mol % silica.
  • 3. The article of claim 2, wherein the silica-containing substrate comprises at least 99 mol % silica.
  • 4. The article of claim 1, wherein the at least one via has an asymmetric hourglass shape.
  • 5. The article of claim 1, wherein the via waist is located closer to one of the first opening at the first surface and the second opening at the second surface than the other.
  • 6. The article of claim 1, wherein the ratio between the waist diameter and each of the first opening diameter and the second opening diameter is less than or equal to 55%.
  • 7. The article of claim 6, wherein the ratio between the waist diameter and each of the first opening diameter and the second opening diameter is less than or equal to about 50%.
  • 8. The article of claim 7, wherein the ratio between the waist diameter and the first opening diameter and/or the second opening diameter is greater than or equal to 35% and less than or equal to 45%.
  • 9. The article of claim 1, wherein the first opening diameter is equal to the second opening diameter.
  • 10. The article of claim 1, wherein the third angle is greater than the second angle.
  • 11. The article of claim 1, wherein the first angle is less than the fourth angle.
  • 12. The article of claim 1, wherein the at least one via is part of a plurality of vias through the silica-containing substrate.
  • 13. The article of claim 12, wherein a center-to-center spacing between adjacent vias of the plurality of vias is about 10 μm to about 2,000 μm the first angle is equal to the fourth angle.
  • 14. The article of claim 1, wherein the at least one via is electroplated with an electrically conductive material.
  • 15. An article comprising: a silica-containing substrate comprising greater than or equal to 75 mol % silica, a first surface, a second surface opposite the first surface and at least one via extending through the silica-containing substrate from a first opening at the first surface a second opening at the second surface, the at least one via comprising: a first opening diameter at the first surface less than 100 μm;a second opening diameter at the second surface less than 100 μm;a longitudinal axis along a length of the via;an interior wall;a via waist between the first surface and the second surface, wherein the via waist has a waist diameter than is less than the first opening diameter and the second opening diameter such that a ratio of a difference between the first opening diameter and the waist diameter and a difference between the second opening diameter and the waist diameter to one-half a thickness of the silica-containing substrate are each greater than or equal to 1/15, and that a ratio between the waist diameter and each of the first opening diameter and the second opening diameter is less than or equal to 60%;a first tapered region extending from proximate the first opening at the first surface toward the via waist and comprising a first axial length, the first tapered region comprising a substantially constant slope having a first angle measured between the interior wall within the first tapered region and a line intersecting the interior wall within the first tapered region and parallel to the longitudinal axis;a second tapered region extending from proximate the first tapered region to proximate the via waist and comprising a second axial length, the second tapered region comprising a substantially constant slope having a second angle measured between the interior wall within the second tapered region and a line intersecting the interior wall within the second tapered region and parallel to the longitudinal axis;a third tapered region extending from proximate the via waist toward the second surface and comprising a third axial length, the third tapered region comprising a substantially constant slope having a third angle measured between the interior wall within the third tapered region and a line intersecting the interior wall within the third tapered region and parallel to the longitudinal axis; anda fourth tapered region extending from proximate the third tapered region to proximate the second opening at the second surface and comprising a fourth axial length, the fourth tapered region comprising a substantially constant slope having a fourth angle measured between the interior wall within the fourth tapered region and a line intersecting the interior wall within the fourth tapered region and parallel to the longitudinal axis,wherein each of the first angle and the fourth angle is less than each of the second angle and the third angle, each of the first angle and the fourth angle is greater than 0 degrees and less than 5 degrees, and each of the second angle and the third angle is greater than 5 degrees and less than about 10 degrees such that the at least one via is an hourglass-shaped via that is substantially symmetric about a horizontal centerline.
  • 16. The article of claim 15, wherein the silica-containing substrate comprises at least 90 mol % silica.
  • 17. The article of claim 16, wherein the silica-containing substrate comprises at least 99 mol % silica.
  • 18. The article of claim 15, wherein each the first and fourth angles are 1 degree and the second and third angles are 8 degrees, wherein the ratio between the waist diameter and each of the first opening diameter and the second opening diameter is about 50%, andwherein each of the first axial length and the fourth axial length are less than each of the second axial length and the third axial length.
  • 19. The article of claim 15, wherein transition areas from the substantially constant slope of the first tapered region to the substantially constant slope of the second tapered region, from the substantially constant slope of the second tapered region to the substantially constant slope of the third tapered region, and from the substantially constant slope of the third tapered region to the substantially constant slope of the fourth tapered region each comprise a slope that varies from the substantially constant slope by greater than or equal to about 1 degree.
  • 20. The article of claim 15, wherein the at least one via is part of a plurality of vias having dimensional control of better than ±1% for the first opening diameter, ±2.5% for the second opening diameter, and ±6% for the waist diameter based on histograms for each thereof.
Parent Case Info

This application is a divisional and claims the benefit of priority under 35 U.S.C. § 120 of U.S. patent application Ser. No. 15/978,430, filed on May 14, 2018, which claims the benefit of priority under 35 U.S.C. § 119 of U.S. Provisional Application Ser. No. 62/510,957, filed on May 25, 2017 and 62/588,615, filed on Nov. 20, 2017, the contents of both are relied upon and incorporated herein by reference in their entirety.

US Referenced Citations (657)
Number Name Date Kind
108387 Pike. Oct 1870 A
208387 George. Sep 1878 A
237571 Messier. Feb 1881 A
1790397 Woods et al. Jan 1931 A
2682134 Stanley Jun 1954 A
2749794 O'Leary Jun 1956 A
3647410 Heaton et al. Mar 1972 A
3695497 Dear Oct 1972 A
3695498 Dear Oct 1972 A
3713921 Fleischer et al. Jan 1973 A
3729302 Heaton Apr 1973 A
3775084 Heaton Nov 1973 A
3798013 Hasegawa et al. Mar 1974 A
4226607 Domken Oct 1980 A
4395271 Beall et al. Jul 1983 A
4441008 Chan Apr 1984 A
4546231 Gresser et al. Oct 1985 A
4547836 Anthony Oct 1985 A
4564579 Morita et al. Jan 1986 A
4646308 Kafka et al. Feb 1987 A
4764930 Bille et al. Aug 1988 A
4891054 Bricker et al. Jan 1990 A
4907586 Bille et al. Mar 1990 A
4918751 Pessot et al. Apr 1990 A
4929065 Hagerty et al. May 1990 A
4948941 Altman et al. Aug 1990 A
5022959 Itoh et al. Jun 1991 A
5035918 Vyas Jul 1991 A
5040182 Spinelli et al. Aug 1991 A
5089062 Pavlik et al. Feb 1992 A
5102498 Itoh et al. Apr 1992 A
5104210 Tokas Apr 1992 A
5108857 Kitayama et al. Apr 1992 A
5112722 Tsujino et al. May 1992 A
5114834 Nachshon May 1992 A
5166493 Inagawa et al. Nov 1992 A
5208068 Davis et al. May 1993 A
5265107 Delfyett, Jr. Nov 1993 A
5314522 Kondo et al. May 1994 A
5374291 Yabe et al. Dec 1994 A
5400350 Galvanauskas Mar 1995 A
5434875 Rieger et al. Jul 1995 A
5436925 Lin et al. Jul 1995 A
5457836 Wiedeck Oct 1995 A
5493096 Koh Feb 1996 A
5553093 Ramaswamy et al. Sep 1996 A
5574597 Kataoka Nov 1996 A
5575291 Hayakawa et al. Nov 1996 A
5575936 Goldfarb Nov 1996 A
5586138 Yokoyama Dec 1996 A
5696782 Harter et al. Dec 1997 A
5736709 Neiheisel Apr 1998 A
5745236 Haga Apr 1998 A
5746884 Gupta et al. May 1998 A
5776220 Allaire et al. Jul 1998 A
5844200 Leader et al. Dec 1998 A
5879424 Nishii et al. Mar 1999 A
5909284 Nakamura Jun 1999 A
5919607 Lawandy Jul 1999 A
5933230 Imaino et al. Aug 1999 A
5965043 Noddin et al. Oct 1999 A
6016223 Suzuki et al. Jan 2000 A
6016324 Rieger et al. Jan 2000 A
6055829 Witzmann et al. May 2000 A
6072624 Dixon et al. Jun 2000 A
6078599 Everage et al. Jun 2000 A
6120131 Murthy et al. Sep 2000 A
6140243 Wallace et al. Oct 2000 A
6143382 Koyama et al. Nov 2000 A
6156030 Neev Dec 2000 A
6160835 Kwon Dec 2000 A
6186384 Sawada Feb 2001 B1
6210401 Lai Apr 2001 B1
6224713 Hembree et al. May 2001 B1
6234755 Bunker et al. May 2001 B1
6256328 Delfyett et al. Jul 2001 B1
6259151 Morrison Jul 2001 B1
6259512 Mizouchi Jul 2001 B1
6272156 Reed et al. Aug 2001 B1
6301932 Allen et al. Oct 2001 B1
6308055 Welland et al. Oct 2001 B1
6319867 Chacon et al. Nov 2001 B1
6322958 Hayashi Nov 2001 B1
6338901 Veerasamy Jan 2002 B1
6339208 Rockstroh et al. Jan 2002 B1
6344242 Stolk et al. Feb 2002 B1
6373565 Kafka et al. Apr 2002 B1
6381391 Islam et al. Apr 2002 B1
6391213 Homola May 2002 B1
6396856 Sucha et al. May 2002 B1
6399914 Troitski Jun 2002 B1
6407360 Choo et al. Jun 2002 B1
6420088 Angelopoulos et al. Jul 2002 B1
6438996 Cuvelier Aug 2002 B1
6445491 Sucha et al. Sep 2002 B2
6449301 Wu et al. Sep 2002 B1
6484052 Visuri et al. Nov 2002 B1
6489589 Alexander Dec 2002 B1
6501578 Bernstein et al. Dec 2002 B1
6537937 Nishizawa et al. Mar 2003 B1
6552301 Herman et al. Apr 2003 B2
6563079 Umetsu et al. May 2003 B1
6573026 Aitken et al. Jun 2003 B1
6592703 Habeck et al. Jul 2003 B1
6635849 Okawa et al. Oct 2003 B1
6635850 Amako et al. Oct 2003 B2
6720519 Liu et al. Apr 2004 B2
6729161 Miura et al. May 2004 B1
6737345 Lin et al. May 2004 B1
6744009 Xuan et al. Jun 2004 B1
6754429 Borrelli et al. Jun 2004 B2
6787732 Xuan et al. Sep 2004 B1
6794605 Park et al. Sep 2004 B2
6800237 Yamamoto et al. Oct 2004 B1
6800831 Hoetzel Oct 2004 B1
6906795 Goto et al. Jun 2005 B2
6958094 Ohmi et al. Oct 2005 B2
6990285 Schroeder et al. Jan 2006 B2
6992026 Fukuyo et al. Jan 2006 B2
6992030 Paulson Jan 2006 B2
7008817 Kim et al. Mar 2006 B2
7009138 Amako et al. Mar 2006 B2
7019257 Stevens Mar 2006 B2
7033519 Taylor et al. Apr 2006 B2
7043072 Goto et al. May 2006 B2
7057135 Li Jun 2006 B2
7084073 Lee et al. Aug 2006 B2
7211899 Taniguchi et al. May 2007 B2
7337540 Kurosawa Mar 2008 B2
7353829 Wachter et al. Apr 2008 B1
7407889 Tsunetomo et al. Aug 2008 B2
7511886 Schultz et al. Mar 2009 B2
7528967 Okawauchi et al. May 2009 B2
7534734 Ellison May 2009 B2
7535634 Savchenkov et al. May 2009 B1
7626665 Koike Dec 2009 B2
7633033 Thomas et al. Dec 2009 B2
7642483 You et al. Jan 2010 B2
7649153 Haight et al. Jan 2010 B2
7683370 Kugimiya et al. Mar 2010 B2
7726532 Gonoe Jun 2010 B2
7749809 How et al. Jul 2010 B2
7763559 Kurachi et al. Jul 2010 B2
7772115 Hiatt Aug 2010 B2
7777275 Lee Aug 2010 B2
7836727 Nishiyama Nov 2010 B2
7880117 Li et al. Feb 2011 B2
7981810 Subramonium et al. Jul 2011 B1
7994503 Hino et al. Aug 2011 B2
8007913 Coppola et al. Aug 2011 B2
8021950 Abadeer et al. Sep 2011 B1
8104385 Hayashi et al. Jan 2012 B2
8118971 Hori et al. Feb 2012 B2
8119462 Takasawa et al. Feb 2012 B2
8132427 Brown et al. Mar 2012 B2
8163649 Koike et al. Apr 2012 B2
8168514 Garner et al. May 2012 B2
8245539 Lu et al. Aug 2012 B2
8245540 Abramov et al. Aug 2012 B2
8257603 Logunov et al. Sep 2012 B2
8269138 Garner et al. Sep 2012 B2
8283595 Fukuyo et al. Oct 2012 B2
8292141 Cox et al. Oct 2012 B2
8296066 Zhao et al. Oct 2012 B2
8303754 Higuchi Nov 2012 B2
8307672 Hidaka et al. Nov 2012 B2
8327666 Harvey et al. Dec 2012 B2
8338957 Nilsson Dec 2012 B2
8341976 Dejneka et al. Jan 2013 B2
8347651 Abramov et al. Jan 2013 B2
8358888 Ramachandran Jan 2013 B2
8384083 Mori et al. Feb 2013 B2
8411459 Yu et al. Apr 2013 B2
8444906 Lee et al. May 2013 B2
8448471 Kumatani et al. May 2013 B2
8455378 Yanase et al. Jun 2013 B2
8482189 Goto et al. Jul 2013 B2
8518280 Hsu et al. Aug 2013 B2
8531679 Scheiner Sep 2013 B2
8533942 Ohashi et al. Sep 2013 B2
8535997 Kawakami et al. Sep 2013 B2
8549881 Brown et al. Oct 2013 B2
8584354 Cornejo et al. Nov 2013 B2
8584490 Garner et al. Nov 2013 B2
8592716 Abramov et al. Nov 2013 B2
8604380 Howerton et al. Dec 2013 B2
8607590 Glaesemann et al. Dec 2013 B2
8616024 Cornejo et al. Dec 2013 B2
8635887 Black et al. Jan 2014 B2
8643129 Laming et al. Feb 2014 B2
8670182 Tanida et al. Mar 2014 B2
8680489 Martinez et al. Mar 2014 B2
8685838 Fukuyo et al. Apr 2014 B2
8697228 Carre et al. Apr 2014 B2
8699037 Cox Apr 2014 B2
8720228 Li May 2014 B2
8742588 Nilsson et al. Jun 2014 B2
8796165 Ellison et al. Aug 2014 B2
8826696 Brown et al. Sep 2014 B2
8835335 Murata et al. Sep 2014 B2
8852698 Fukumitsu Oct 2014 B2
8871641 Nilsson Oct 2014 B2
8873067 Lee et al. Oct 2014 B2
8887529 Lu et al. Nov 2014 B2
8916798 Pluss Dec 2014 B2
8943855 Gomez et al. Feb 2015 B2
8971053 Kariya et al. Mar 2015 B2
8980727 Lei et al. Mar 2015 B1
8993465 Ellison et al. Mar 2015 B2
8999179 Yu et al. Apr 2015 B2
9023421 Nakashima May 2015 B2
9024443 Inaba et al. May 2015 B2
9093381 Barriere et al. Jul 2015 B2
9138913 Arai et al. Sep 2015 B2
9140539 Scheiner Sep 2015 B2
9227868 Matsumoto et al. Jan 2016 B2
9232652 Fushie et al. Jan 2016 B2
9263300 Tsai et al. Feb 2016 B2
9278886 Boek et al. Mar 2016 B2
9285593 Laskin et al. Mar 2016 B1
9290407 Barefoot et al. Mar 2016 B2
9296066 Hosseini et al. Mar 2016 B2
9296646 Burket et al. Mar 2016 B2
9305470 Miki et al. Apr 2016 B2
9321680 Chuang et al. Apr 2016 B2
9324791 Tamemoto Apr 2016 B2
9327381 Lee et al. May 2016 B2
9346706 Bazemore et al. May 2016 B2
9377583 Giaretta et al. Jun 2016 B2
9425125 Shen Aug 2016 B2
9442377 Ongayi et al. Sep 2016 B1
9446590 Chen et al. Sep 2016 B2
9481598 Bergh et al. Nov 2016 B2
9517963 Marjanovic et al. Dec 2016 B2
9676046 Hamada et al. Jun 2017 B2
9745220 Burket et al. Aug 2017 B2
9758876 Shorey et al. Sep 2017 B2
9760986 Ramamurthy et al. Sep 2017 B2
9815730 Marjanovic et al. Nov 2017 B2
9832868 Wright et al. Nov 2017 B1
9850160 Marjanovic et al. Dec 2017 B2
9953912 Goers Apr 2018 B2
10144093 Marjanovic et al. Dec 2018 B2
10203476 Cui Feb 2019 B2
20010009250 Herman et al. Jul 2001 A1
20020005805 Ogura et al. Jan 2002 A1
20020041946 Abe Apr 2002 A1
20020046997 Nam et al. Apr 2002 A1
20020051563 Goto et al. May 2002 A1
20020052125 Shaffer et al. May 2002 A1
20020062563 Koide et al. May 2002 A1
20020082466 Han Jun 2002 A1
20020097486 Yamaguchi et al. Jul 2002 A1
20020110639 Bruns Aug 2002 A1
20020137344 Jordan et al. Sep 2002 A1
20020180015 Yamaguchi et al. Dec 2002 A1
20020182871 Lu et al. Dec 2002 A1
20030006221 Hong et al. Jan 2003 A1
20030007772 Borrelli et al. Jan 2003 A1
20030045420 Koyama et al. Mar 2003 A1
20030137056 Taniguchi et al. Jul 2003 A1
20030150839 Kobayashi et al. Aug 2003 A1
20030206651 Goto et al. Nov 2003 A1
20030217568 Koyo et al. Nov 2003 A1
20030235385 Taylor et al. Dec 2003 A1
20040000534 Lipinski Jan 2004 A1
20040013951 Wang Jan 2004 A1
20040022487 Nagasaka et al. Feb 2004 A1
20040058476 Enquist et al. Mar 2004 A1
20040061705 Yoon et al. Apr 2004 A1
20040092105 Lee et al. May 2004 A1
20040094524 Stevens May 2004 A1
20040152229 Najafi et al. Aug 2004 A1
20040188393 Li et al. Sep 2004 A1
20040214423 Marxsen et al. Oct 2004 A1
20040217455 Shiono et al. Nov 2004 A1
20040221615 Postupack et al. Nov 2004 A1
20040223704 Fujii et al. Nov 2004 A1
20040256619 Nomura et al. Dec 2004 A1
20050009315 Kim et al. Jan 2005 A1
20050023246 McEntee et al. Feb 2005 A1
20050024743 Camy-Peyret Feb 2005 A1
20050029238 Chen Feb 2005 A1
20050033184 Christoph Feb 2005 A1
20050079650 Mancini et al. Apr 2005 A1
20050098458 Gruetzmacher et al. May 2005 A1
20050098548 Kobayashi et al. May 2005 A1
20050106874 Matsui et al. May 2005 A1
20050112506 Czech et al. May 2005 A1
20050115938 Sawaki et al. Jun 2005 A1
20050142364 Aitken Jun 2005 A1
20050142812 Kurosawa Jun 2005 A1
20050158538 Li et al. Jul 2005 A1
20050199592 Ri et al. Sep 2005 A1
20050202683 Wang et al. Sep 2005 A1
20050266320 Amemiya Dec 2005 A1
20050274690 Park et al. Dec 2005 A1
20050274702 Deshi Dec 2005 A1
20060011593 Fukuyo et al. Jan 2006 A1
20060012766 Klosner et al. Jan 2006 A1
20060019814 Baik et al. Jan 2006 A1
20060039160 Cassarly et al. Feb 2006 A1
20060109874 Shiozaki et al. May 2006 A1
20060127679 Gulati et al. Jun 2006 A1
20060151450 You et al. Jul 2006 A1
20060192978 Laguarta et al. Aug 2006 A1
20060194916 Zhong et al. Aug 2006 A1
20060207976 Bovatsek et al. Sep 2006 A1
20060219676 Taylor et al. Oct 2006 A1
20060227440 Gluckstad Oct 2006 A1
20060270232 Kawamura et al. Nov 2006 A1
20060289410 Morita et al. Dec 2006 A1
20060290232 Fujita et al. Dec 2006 A1
20060292877 Lake Dec 2006 A1
20070045779 Hiatt Mar 2007 A1
20070051706 Bovatsek et al. Mar 2007 A1
20070111390 Komura et al. May 2007 A1
20070111480 Maruyama et al. May 2007 A1
20070117044 Ogihara et al. May 2007 A1
20070119831 Kandt May 2007 A1
20070132977 Komatsuda Jun 2007 A1
20070138151 Tanaka et al. Jun 2007 A1
20070177116 Amako Aug 2007 A1
20070181543 Urairi et al. Aug 2007 A1
20070190340 Coppola et al. Aug 2007 A1
20070202619 Tamura et al. Aug 2007 A1
20070232028 Lee et al. Oct 2007 A1
20070298529 Maeda et al. Dec 2007 A1
20080000884 Sugiura et al. Jan 2008 A1
20080099444 Misawa et al. May 2008 A1
20080194109 Ishibashi et al. Aug 2008 A1
20080206690 Kennedy et al. Aug 2008 A1
20080212185 Fuse Sep 2008 A1
20080245109 Flemming et al. Oct 2008 A1
20080314883 Juodkazis et al. Dec 2008 A1
20090013724 Koyo et al. Jan 2009 A1
20090029189 Moriwaki et al. Jan 2009 A1
20090032510 Ando et al. Feb 2009 A1
20090075087 Xu et al. Mar 2009 A1
20090098351 Kishi Apr 2009 A1
20090151996 Mishima et al. Jun 2009 A1
20090176034 Ruuttu et al. Jul 2009 A1
20090183764 Meyer Jul 2009 A1
20090219491 Williams et al. Sep 2009 A1
20090242528 Howerton et al. Oct 2009 A1
20090250446 Sakamoto Oct 2009 A1
20090286091 Danielson et al. Nov 2009 A1
20090294419 Abramov et al. Dec 2009 A1
20090294422 Lubatschowski et al. Dec 2009 A1
20090324899 Feinstein et al. Dec 2009 A1
20100000259 Ukrainczyk et al. Jan 2010 A1
20100015439 Buether et al. Jan 2010 A1
20100015454 Anderson et al. Jan 2010 A1
20100025387 Arai et al. Feb 2010 A1
20100029460 Shojiya et al. Feb 2010 A1
20100032087 Takahashi et al. Feb 2010 A1
20100050692 Logunov et al. Mar 2010 A1
20100068453 Imai et al. Mar 2010 A1
20100080961 Okamura et al. Apr 2010 A1
20100086741 Bovatsek et al. Apr 2010 A1
20100086870 Ogihara et al. Apr 2010 A1
20100089631 Sakaguchi et al. Apr 2010 A1
20100089882 Tamura Apr 2010 A1
20100102042 Garner et al. Apr 2010 A1
20100119808 Li et al. May 2010 A1
20100119846 Sawada May 2010 A1
20100129603 Blick et al. May 2010 A1
20100133697 Nilsson Jun 2010 A1
20100147813 Lei et al. Jun 2010 A1
20100178732 Wu et al. Jul 2010 A1
20100206008 Harvey et al. Aug 2010 A1
20100252540 El et al. Oct 2010 A1
20100252959 Lei et al. Oct 2010 A1
20100276505 Smith Nov 2010 A1
20100279067 Sabia et al. Nov 2010 A1
20100279509 Kim et al. Nov 2010 A1
20100284027 Scheiner Nov 2010 A1
20100287991 Brown et al. Nov 2010 A1
20100289115 Akiyama et al. Nov 2010 A1
20100289186 Longo et al. Nov 2010 A1
20100291353 Dejneka et al. Nov 2010 A1
20100292068 Takaya et al. Nov 2010 A1
20100294748 Garner et al. Nov 2010 A1
20100307809 Noda et al. Dec 2010 A1
20100320179 Morita et al. Dec 2010 A1
20100326138 Kumatani et al. Dec 2010 A1
20110003619 Fujii Jan 2011 A1
20110032467 Koike Feb 2011 A1
20110045239 Takaya et al. Feb 2011 A1
20110049764 Lee et al. Mar 2011 A1
20110049765 Li et al. Mar 2011 A1
20110088324 Wessel Apr 2011 A1
20110100401 Fiorentini May 2011 A1
20110123787 Tomamoto et al. May 2011 A1
20110132881 Liu Jun 2011 A1
20110132883 Sheng et al. Jun 2011 A1
20110183116 Hung et al. Jul 2011 A1
20110187025 Costin, Sr. Aug 2011 A1
20110189847 Tsai et al. Aug 2011 A1
20110195360 Flemming et al. Aug 2011 A1
20110201197 Nilsson et al. Aug 2011 A1
20110204528 Matsutani et al. Aug 2011 A1
20110229687 Gu et al. Sep 2011 A1
20110240611 Torbjoern Oct 2011 A1
20110248405 Li et al. Oct 2011 A1
20110256344 Ono et al. Oct 2011 A1
20110259373 Hotta et al. Oct 2011 A1
20110259860 Bass et al. Oct 2011 A1
20110277507 Lu et al. Nov 2011 A1
20110300908 Grespan et al. Dec 2011 A1
20110308942 Liu et al. Dec 2011 A1
20110316561 Tinsley et al. Dec 2011 A1
20110318555 Bookbinder et al. Dec 2011 A1
20110318561 Murata et al. Dec 2011 A1
20120013196 Kim et al. Jan 2012 A1
20120017642 Teranishi et al. Jan 2012 A1
20120047951 Dannoux et al. Mar 2012 A1
20120047956 Li Mar 2012 A1
20120048604 Cornejo et al. Mar 2012 A1
20120050692 Gollier Mar 2012 A1
20120052302 Matusick et al. Mar 2012 A1
20120061440 Roell Mar 2012 A1
20120064306 Kang et al. Mar 2012 A1
20120092681 Cox Apr 2012 A1
20120103018 Lu et al. May 2012 A1
20120105095 Bryant et al. May 2012 A1
20120111057 Barefoot et al. May 2012 A1
20120125892 Shimoi et al. May 2012 A1
20120125893 Shimoi et al. May 2012 A1
20120129359 Shimoi et al. May 2012 A1
20120130004 Xu et al. May 2012 A1
20120131958 Shimoi et al. May 2012 A1
20120131962 Mitsugi et al. May 2012 A1
20120135177 Cornejo et al. May 2012 A1
20120135195 Glaesemann et al. May 2012 A1
20120135607 Shimoi et al. May 2012 A1
20120135608 Shimoi et al. May 2012 A1
20120135852 Ellison et al. May 2012 A1
20120135853 Amin et al. May 2012 A1
20120141668 Nakashima Jun 2012 A1
20120142136 Horning et al. Jun 2012 A1
20120145331 Gomez et al. Jun 2012 A1
20120168412 Hooper Jul 2012 A1
20120196071 Cornejo et al. Aug 2012 A1
20120205356 Christoph Aug 2012 A1
20120211923 Garner et al. Aug 2012 A1
20120214006 Chen et al. Aug 2012 A1
20120234049 Bolton Sep 2012 A1
20120234807 Sercel et al. Sep 2012 A1
20120235969 Burns et al. Sep 2012 A1
20120241919 Mitani Sep 2012 A1
20120255935 Kakui et al. Oct 2012 A1
20120261697 Margalit et al. Oct 2012 A1
20120276483 Ogihara et al. Nov 2012 A1
20120276743 Won et al. Nov 2012 A1
20120299203 Sugo et al. Nov 2012 A1
20120299219 Shimoi et al. Nov 2012 A1
20120302139 Darcangelo et al. Nov 2012 A1
20120308803 Dejneka et al. Dec 2012 A1
20130019637 Sol et al. Jan 2013 A1
20130029092 Wakioka Jan 2013 A1
20130034688 Koike et al. Feb 2013 A1
20130044371 Rupp et al. Feb 2013 A1
20130050226 Shenoy et al. Feb 2013 A1
20130061636 Imai et al. Mar 2013 A1
20130068736 Mielke et al. Mar 2013 A1
20130075480 Yokogi et al. Mar 2013 A1
20130078891 Lee et al. Mar 2013 A1
20130089701 Hooper et al. Apr 2013 A1
20130091897 Fujii et al. Apr 2013 A1
20130105213 Hu et al. May 2013 A1
20130118793 Teshima et al. May 2013 A1
20130122264 Fujii et al. May 2013 A1
20130126573 Hosseini et al. May 2013 A1
20130129947 Harvey et al. May 2013 A1
20130133367 Abramov et al. May 2013 A1
20130135745 Tanida et al. May 2013 A1
20130143416 Norval Jun 2013 A1
20130149434 Oh et al. Jun 2013 A1
20130149494 Koike et al. Jun 2013 A1
20130163801 Ha et al. Jun 2013 A1
20130167590 Teranishi et al. Jul 2013 A1
20130174607 Wootton et al. Jul 2013 A1
20130174610 Teranishi et al. Jul 2013 A1
20130180285 Kariya Jul 2013 A1
20130180665 Gomez et al. Jul 2013 A2
20130189806 Hoshino Jul 2013 A1
20130192305 Black et al. Aug 2013 A1
20130193585 Lin et al. Aug 2013 A1
20130205835 Giaretta et al. Aug 2013 A1
20130209731 Nattermann et al. Aug 2013 A1
20130210245 Jackl Aug 2013 A1
20130213467 Nattermann et al. Aug 2013 A1
20130220982 Thomas et al. Aug 2013 A1
20130221053 Zhang Aug 2013 A1
20130224439 Zhang et al. Aug 2013 A1
20130224492 Bookbinder et al. Aug 2013 A1
20130228918 Chen et al. Sep 2013 A1
20130247615 Boek et al. Sep 2013 A1
20130255779 Aitken et al. Oct 2013 A1
20130266757 Giron et al. Oct 2013 A1
20130270240 Kondo Oct 2013 A1
20130280495 Matsumoto Oct 2013 A1
20130288010 Akarapu et al. Oct 2013 A1
20130291598 Saito et al. Nov 2013 A1
20130312460 Kunishi et al. Nov 2013 A1
20130323469 Abramov et al. Dec 2013 A1
20130330515 Oh et al. Dec 2013 A1
20130334185 Nomaru Dec 2013 A1
20130337599 Yun Dec 2013 A1
20130340480 Nattermann et al. Dec 2013 A1
20140015121 Koizumi et al. Jan 2014 A1
20140027951 Srinivas et al. Jan 2014 A1
20140034374 Cornejo et al. Feb 2014 A1
20140034730 Gun-Hong Feb 2014 A1
20140042202 Lee Feb 2014 A1
20140044143 Clarkson et al. Feb 2014 A1
20140047957 Wu Feb 2014 A1
20140054618 Li Feb 2014 A1
20140102146 Saito et al. Apr 2014 A1
20140110040 Cok Apr 2014 A1
20140113797 Yamada et al. Apr 2014 A1
20140116091 Chuang et al. May 2014 A1
20140133119 Kariya et al. May 2014 A1
20140141217 Gulati et al. May 2014 A1
20140147623 Shorey et al. May 2014 A1
20140147624 Streltsov et al. May 2014 A1
20140154439 Demartino et al. Jun 2014 A1
20140165652 Saito Jun 2014 A1
20140166199 Bellman et al. Jun 2014 A1
20140170378 Bellman et al. Jun 2014 A1
20140174131 Saito et al. Jun 2014 A1
20140199519 Schillinger et al. Jul 2014 A1
20140216108 Wiegel et al. Aug 2014 A1
20140231390 Nukaga et al. Aug 2014 A1
20140235796 Ogihara et al. Aug 2014 A1
20140242375 Mauro et al. Aug 2014 A1
20140254004 Wooder et al. Sep 2014 A1
20140290310 Green Oct 2014 A1
20140300728 Drescher et al. Oct 2014 A1
20140312506 Hayashi et al. Oct 2014 A1
20140320947 Egerton et al. Oct 2014 A1
20140333929 Sung et al. Nov 2014 A1
20140339207 Sugiyama et al. Nov 2014 A1
20140340730 Bergh et al. Nov 2014 A1
20140342897 Amin et al. Nov 2014 A1
20140347083 Bryant et al. Nov 2014 A1
20140361463 Desimone et al. Dec 2014 A1
20140376006 Scheiner Dec 2014 A1
20150021513 Kim et al. Jan 2015 A1
20150027757 Shin et al. Jan 2015 A1
20150036065 Yousefpor et al. Feb 2015 A1
20150037553 Mauro Feb 2015 A1
20150038313 Hosseini Feb 2015 A1
20150051060 Ellison et al. Feb 2015 A1
20150054136 Ebefors et al. Feb 2015 A1
20150060402 Burkett et al. Mar 2015 A1
20150075221 Kawaguchi et al. Mar 2015 A1
20150075222 Mader Mar 2015 A1
20150093908 Reddy et al. Apr 2015 A1
20150102498 Enicks et al. Apr 2015 A1
20150110442 Zimmel et al. Apr 2015 A1
20150118522 Hosseini Apr 2015 A1
20150136743 Hosseini May 2015 A1
20150140241 Hosseini May 2015 A1
20150140299 Ellison et al. May 2015 A1
20150151380 Hosseini Jun 2015 A1
20150158120 Courvoisier et al. Jun 2015 A1
20150165548 Marjanovic et al. Jun 2015 A1
20150165560 Hackert et al. Jun 2015 A1
20150165562 Marjanovic et al. Jun 2015 A1
20150165563 Manley et al. Jun 2015 A1
20150166391 Marjanovic et al. Jun 2015 A1
20150166393 Marjanovic et al. Jun 2015 A1
20150166394 Marjanovic et al. Jun 2015 A1
20150166395 Marjanovic et al. Jun 2015 A1
20150166396 Marjanovic et al. Jun 2015 A1
20150166397 Marjanovic et al. Jun 2015 A1
20150173191 Takahashi Jun 2015 A1
20150183679 Saito Jul 2015 A1
20150232369 Marjanovic et al. Aug 2015 A1
20150239775 Amin et al. Aug 2015 A1
20150274583 An et al. Oct 2015 A1
20150299018 Bhuyan et al. Oct 2015 A1
20150306847 Bellman et al. Oct 2015 A1
20150329415 Bellman et al. Nov 2015 A1
20150360991 Grundmueller et al. Dec 2015 A1
20150367442 Bovatsek et al. Dec 2015 A1
20150368145 Senshu et al. Dec 2015 A1
20150376050 Nakamura et al. Dec 2015 A1
20160008927 Grundmueller et al. Jan 2016 A1
20160009066 Nieber et al. Jan 2016 A1
20160016257 Hosseini Jan 2016 A1
20160023922 Addiego et al. Jan 2016 A1
20160026842 Withers et al. Jan 2016 A1
20160031745 Ortner et al. Feb 2016 A1
20160035587 Keech et al. Feb 2016 A1
20160059359 Krueger et al. Mar 2016 A1
20160060156 Krueger et al. Mar 2016 A1
20160102009 Boek et al. Apr 2016 A1
20160107925 Burket et al. Apr 2016 A1
20160145149 Burket et al. May 2016 A1
20160152516 Bazemore et al. Jun 2016 A1
20160166395 Weiman Jun 2016 A9
20160199944 Hosseini Jul 2016 A1
20160200621 N'Gom et al. Jul 2016 A1
20160201474 Slavens et al. Jul 2016 A1
20160204126 Amano Jul 2016 A1
20160208387 Liu et al. Jul 2016 A1
20160219704 Vandemeer et al. Jul 2016 A1
20160237571 Liu et al. Aug 2016 A1
20160276257 Kuramochi Sep 2016 A1
20160280580 Bohme Sep 2016 A1
20160282584 Cui Sep 2016 A1
20160289669 Fan et al. Oct 2016 A1
20160290791 Buono et al. Oct 2016 A1
20160305764 Cui et al. Oct 2016 A1
20160311717 Nieber et al. Oct 2016 A1
20160312365 Cordonier et al. Oct 2016 A1
20160322291 Goers Nov 2016 A1
20160327744 Giaretta et al. Nov 2016 A1
20160334203 Cui et al. Nov 2016 A1
20160351410 Fu et al. Dec 2016 A1
20160352023 Dang et al. Dec 2016 A1
20160362331 Castle et al. Dec 2016 A1
20160365275 Chang et al. Dec 2016 A1
20160368100 Marjanovic et al. Dec 2016 A1
20160370680 Geerlings et al. Dec 2016 A1
20160376186 Gross Dec 2016 A1
20170002601 Bergh et al. Jan 2017 A1
20170008122 Wieland et al. Jan 2017 A1
20170011914 Sumant et al. Jan 2017 A1
20170029957 Moon et al. Feb 2017 A1
20170036419 Adib et al. Feb 2017 A1
20170103249 Jin et al. Apr 2017 A1
20170119891 Lal et al. May 2017 A1
20170160077 Featherstone et al. Jun 2017 A1
20170169847 Tamaki Jun 2017 A1
20170228884 Yoshida Aug 2017 A1
20170252859 Kumkar et al. Sep 2017 A1
20170276951 Kumkar et al. Sep 2017 A1
20170358447 Tsunetomo et al. Dec 2017 A1
20170363417 Cui et al. Dec 2017 A1
20170372899 Yang et al. Dec 2017 A1
20180005922 Levesque et al. Jan 2018 A1
20180033128 Sobieranski et al. Feb 2018 A1
20180057390 Hackert et al. Mar 2018 A1
20180062342 Comstock et al. Mar 2018 A1
20180068868 Jaramillo et al. Mar 2018 A1
20180093914 Akarapu et al. Apr 2018 A1
20180215647 Ortner et al. Aug 2018 A1
20180340262 Hiranuma Nov 2018 A1
20180342450 Huang et al. Nov 2018 A1
20180342451 Dahlberg et al. Nov 2018 A1
20190012514 Jin et al. Jan 2019 A1
20190185373 Hu et al. Jun 2019 A1
20200156990 Sakade et al. May 2020 A1
Foreign Referenced Citations (393)
Number Date Country
2004276725 Apr 2005 AU
2011101310 Nov 2011 AU
2530607 Apr 2005 CA
1096936 Jan 1995 CN
1196562 Oct 1998 CN
2388062 Jul 2000 CN
1473087 Feb 2004 CN
1485812 Mar 2004 CN
1200793 May 2005 CN
1619778 May 2005 CN
1636912 Jul 2005 CN
1657220 Aug 2005 CN
1735568 Feb 2006 CN
1761378 Apr 2006 CN
1845812 Oct 2006 CN
1283409 Nov 2006 CN
1967815 May 2007 CN
101048255 Oct 2007 CN
101238572 Aug 2008 CN
101386466 Mar 2009 CN
101427427 May 2009 CN
101438397 May 2009 CN
100494879 Jun 2009 CN
101502914 Aug 2009 CN
100546004 Sep 2009 CN
100555601 Oct 2009 CN
101602148 Dec 2009 CN
101610870 Dec 2009 CN
201357287 Dec 2009 CN
101631739 Jan 2010 CN
101637849 Feb 2010 CN
201471092 May 2010 CN
101722367 Jun 2010 CN
101862907 Oct 2010 CN
101965242 Feb 2011 CN
102046545 May 2011 CN
102060437 May 2011 CN
102246292 Nov 2011 CN
102300820 Dec 2011 CN
102304323 Jan 2012 CN
102319960 Jan 2012 CN
102326232 Jan 2012 CN
102343631 Feb 2012 CN
102356049 Feb 2012 CN
102356050 Feb 2012 CN
102428047 Apr 2012 CN
102458754 May 2012 CN
102485405 Jun 2012 CN
102540474 Jul 2012 CN
102574246 Jul 2012 CN
102585696 Jul 2012 CN
102596830 Jul 2012 CN
102649199 Aug 2012 CN
102672355 Sep 2012 CN
102795596 Nov 2012 CN
102898014 Jan 2013 CN
102916081 Feb 2013 CN
102923939 Feb 2013 CN
102958642 Mar 2013 CN
103013374 Apr 2013 CN
103079747 May 2013 CN
103143841 Jun 2013 CN
103159401 Jun 2013 CN
203021443 Jun 2013 CN
103237771 Aug 2013 CN
103273195 Sep 2013 CN
103316990 Sep 2013 CN
103359947 Oct 2013 CN
103359948 Oct 2013 CN
103460368 Dec 2013 CN
103531414 Jan 2014 CN
103534216 Jan 2014 CN
103746027 Apr 2014 CN
203509350 Apr 2014 CN
104344202 Feb 2015 CN
104897062 Sep 2015 CN
105246850 Jan 2016 CN
105392593 Mar 2016 CN
105693102 Jun 2016 CN
106132627 Nov 2016 CN
108191258 Jun 2018 CN
2231330 Jan 1974 DE
10322376 Dec 2004 DE
102006035555 Jan 2008 DE
102010003817 Oct 2011 DE
102011000768 Aug 2012 DE
102012010635 Nov 2013 DE
102012110971 May 2014 DE
102013103370 Oct 2014 DE
102013223637 May 2015 DE
102014113339 Mar 2016 DE
0247993 Dec 1987 EP
0270897 Jun 1988 EP
0280918 Sep 1988 EP
0393381 Oct 1990 EP
0938946 Sep 1999 EP
1043110 Oct 2000 EP
1159104 Dec 2001 EP
1164113 Dec 2001 EP
1412131 Apr 2004 EP
1449810 Aug 2004 EP
1609559 Dec 2005 EP
1614665 Jan 2006 EP
1651943 May 2006 EP
1714730 Oct 2006 EP
1990125 Nov 2008 EP
2020273 Feb 2009 EP
2133170 Dec 2009 EP
2202545 Jun 2010 EP
2253414 Nov 2010 EP
2398746 Dec 2011 EP
2543065 Jan 2013 EP
2574983 Apr 2013 EP
2600397 Jun 2013 EP
2754524 Jul 2014 EP
2781296 Sep 2014 EP
2783784 Oct 2014 EP
2831913 Feb 2015 EP
2859984 Apr 2015 EP
2922793 Sep 2015 EP
3166372 May 2017 EP
3288906 Mar 2018 EP
2989294 Oct 2013 FR
1242172 Aug 1971 GB
2481190 Dec 2011 GB
201102390 Mar 2013 IN
55-130839 Oct 1980 JP
56-129261 Oct 1981 JP
56-160893 Dec 1981 JP
60-220340 Nov 1985 JP
64-077001 Mar 1989 JP
01-179770 Jul 1989 JP
03-252384 Nov 1991 JP
04-349132 Dec 1992 JP
06-079486 Mar 1994 JP
06-318756 Nov 1994 JP
09-106243 Apr 1997 JP
10-263873 Oct 1998 JP
11-197498 Jul 1999 JP
11-269683 Oct 1999 JP
11-297703 Oct 1999 JP
11-330597 Nov 1999 JP
11-347758 Dec 1999 JP
2000-010289 Jan 2000 JP
2000-301372 Oct 2000 JP
2000-302488 Oct 2000 JP
2001-105398 Apr 2001 JP
2001-106545 Apr 2001 JP
2001-138083 May 2001 JP
2002-028799 Jan 2002 JP
2002-154846 May 2002 JP
2002-210730 Jul 2002 JP
2002-228818 Aug 2002 JP
2003-017503 Jan 2003 JP
2003-062756 Mar 2003 JP
2003-114400 Apr 2003 JP
2003-148931 May 2003 JP
2003-154517 May 2003 JP
2003-181668 Jul 2003 JP
2003-197811 Jul 2003 JP
2003-238178 Aug 2003 JP
2004-190043 Jul 2004 JP
2004-209675 Jul 2004 JP
2004-255562 Sep 2004 JP
2004-330236 Nov 2004 JP
2004-351494 Dec 2004 JP
2004-363212 Dec 2004 JP
2005-000952 Jan 2005 JP
2005-019576 Jan 2005 JP
2005-074663 Mar 2005 JP
2005-104819 Apr 2005 JP
2005-121417 May 2005 JP
2005-144622 Jun 2005 JP
2005-205440 Aug 2005 JP
2005-257339 Sep 2005 JP
2005-279755 Oct 2005 JP
2005-288503 Oct 2005 JP
2005-306702 Nov 2005 JP
2006024652 Jan 2006 JP
2006-130691 May 2006 JP
3775250 May 2006 JP
3775410 May 2006 JP
2006-161124 Jun 2006 JP
2006-248885 Sep 2006 JP
3823108 Sep 2006 JP
2006-290630 Oct 2006 JP
2007-021548 Feb 2007 JP
2007-042741 Feb 2007 JP
2007-067031 Mar 2007 JP
2007-196277 Aug 2007 JP
2007-253203 Oct 2007 JP
2007-260896 Oct 2007 JP
2008-094641 Apr 2008 JP
2008-156200 Jul 2008 JP
2008-522950 Jul 2008 JP
2008-247639 Oct 2008 JP
2008-273783 Nov 2008 JP
2008-288577 Nov 2008 JP
2009-200356 Sep 2009 JP
4349132 Oct 2009 JP
4418282 Feb 2010 JP
2010-046761 Mar 2010 JP
2010-074017 Apr 2010 JP
2010-539288 Dec 2010 JP
4592855 Dec 2010 JP
2011-011212 Jan 2011 JP
2011-037707 Feb 2011 JP
2011-049398 Mar 2011 JP
4672689 Apr 2011 JP
2011-517299 Jun 2011 JP
2011-143434 Jul 2011 JP
2011-178642 Sep 2011 JP
2011-228517 Nov 2011 JP
2011-251872 Dec 2011 JP
2012-024782 Feb 2012 JP
2012-028533 Feb 2012 JP
2012-031018 Feb 2012 JP
4880820 Feb 2012 JP
2012-506837 Mar 2012 JP
2012-159749 Aug 2012 JP
2012-517957 Aug 2012 JP
2012-187618 Oct 2012 JP
2013-007842 Jan 2013 JP
2013-031879 Feb 2013 JP
2013-043808 Mar 2013 JP
2013-075802 Apr 2013 JP
2013-091578 May 2013 JP
2013-121908 Jun 2013 JP
5274085 Aug 2013 JP
2013-178371 Sep 2013 JP
2013-187247 Sep 2013 JP
2013-536081 Sep 2013 JP
5300544 Sep 2013 JP
2013-203630 Oct 2013 JP
2013-203631 Oct 2013 JP
2013-220958 Oct 2013 JP
2013-223886 Oct 2013 JP
5318748 Oct 2013 JP
2013-245153 Dec 2013 JP
2014078720 May 2014 JP
2014-127701 Jul 2014 JP
2014-214036 Nov 2014 JP
2015-501531 Jan 2015 JP
2015-030040 Feb 2015 JP
2015-129076 Jul 2015 JP
2015-519722 Jul 2015 JP
2015-146410 Aug 2015 JP
2016-508069 Mar 2016 JP
2016049542 Apr 2016 JP
2016063114 Apr 2016 JP
2016-213253 Dec 2016 JP
2017-059669 Mar 2017 JP
2017-510531 Apr 2017 JP
10-2002-0038707 May 2002 KR
10-2002-0066005 Aug 2002 KR
10-2009-0057161 Jun 2009 KR
2010-0120297 Nov 2010 KR
10-1020621 Mar 2011 KR
2011-0046953 May 2011 KR
2011-0121637 Nov 2011 KR
10-2012-0015366 Feb 2012 KR
10-1120471 Mar 2012 KR
10-1159697 Jun 2012 KR
10-2012-0074508 Jul 2012 KR
2012-0102675 Sep 2012 KR
2013-0031380 Mar 2013 KR
10-1259349 Apr 2013 KR
10-1269474 May 2013 KR
2013-0079395 Jul 2013 KR
10-2013-0111269 Oct 2013 KR
10-2013-0124646 Nov 2013 KR
10-1344368 Dec 2013 KR
10-2014-0022980 Feb 2014 KR
10-2014-0022981 Feb 2014 KR
10-2014-0064220 May 2014 KR
10-1423338 Jul 2014 KR
10-2014-0112652 Sep 2014 KR
2015-0016176 Feb 2015 KR
200423242 Nov 2004 TW
200842313 Nov 2008 TW
200842345 Nov 2008 TW
201027601 Jul 2010 TW
201041027 Nov 2010 TW
201041118 Nov 2010 TW
201212755 Mar 2012 TW
201226345 Jul 2012 TW
201303259 Jan 2013 TW
201311592 Mar 2013 TW
201317622 May 2013 TW
201331136 Aug 2013 TW
201339111 Oct 2013 TW
201340272 Oct 2013 TW
201429897 Aug 2014 TW
201610602 Mar 2016 TW
201621267 Jun 2016 TW
8902877 Apr 1989 WO
9821154 May 1998 WO
9929243 Jun 1999 WO
9963900 Dec 1999 WO
0051778 Sep 2000 WO
0133621 May 2001 WO
2002081142 Oct 2002 WO
2003007370 Jan 2003 WO
0311522 Feb 2003 WO
0321004 Mar 2003 WO
2004110693 Dec 2004 WO
2005031300 Apr 2005 WO
2005033033 Apr 2005 WO
2005034594 Apr 2005 WO
2006073098 Jul 2006 WO
2006112822 Oct 2006 WO
2007094160 Aug 2007 WO
2007094233 Aug 2007 WO
2007096958 Aug 2007 WO
2008012186 Jan 2008 WO
2008080182 Jul 2008 WO
2008102848 Aug 2008 WO
2008110061 Sep 2008 WO
2008128612 Oct 2008 WO
2009072810 Jun 2009 WO
2009114375 Sep 2009 WO
2010035736 Apr 2010 WO
2010087483 Aug 2010 WO
2010096359 Aug 2010 WO
2010111609 Sep 2010 WO
2010129459 Nov 2010 WO
2011025908 Mar 2011 WO
2011056781 May 2011 WO
2011109648 Sep 2011 WO
2012006736 Jan 2012 WO
2012011230 Jan 2012 WO
2012027220 Mar 2012 WO
2012060277 May 2012 WO
2012075072 Jun 2012 WO
2012108052 Aug 2012 WO
2012161317 Nov 2012 WO
2012166753 Dec 2012 WO
2013008344 Jan 2013 WO
2013016157 Jan 2013 WO
2013022148 Feb 2013 WO
2013030848 Mar 2013 WO
2013043173 Mar 2013 WO
2013084877 Jun 2013 WO
2013084879 Jun 2013 WO
2013130718 Sep 2013 WO
2013134237 Sep 2013 WO
2013138802 Sep 2013 WO
2013147694 Oct 2013 WO
2013150990 Oct 2013 WO
2013153195 Oct 2013 WO
WO-2013160994 Oct 2013 WO
2014010490 Jan 2014 WO
2014012125 Jan 2014 WO
2014028022 Feb 2014 WO
2014038326 Mar 2014 WO
2014064492 May 2014 WO
2014079478 May 2014 WO
2014079570 May 2014 WO
2014085660 Jun 2014 WO
2014085663 Jun 2014 WO
2014111385 Jul 2014 WO
2014111794 Jul 2014 WO
2014121261 Aug 2014 WO
2014148020 Sep 2014 WO
2014161535 Oct 2014 WO
2014161534 Nov 2014 WO
2014205301 Dec 2014 WO
2015029286 Mar 2015 WO
2015077113 May 2015 WO
2015094898 Jun 2015 WO
2015095088 Jun 2015 WO
2015095090 Jun 2015 WO
2015095146 Jun 2015 WO
2015095151 Jun 2015 WO
2015100056 Jul 2015 WO
2015113023 Jul 2015 WO
2015127583 Sep 2015 WO
2015157202 Oct 2015 WO
2016005455 Jan 2016 WO
2016010954 Jan 2016 WO
2016010991 Jan 2016 WO
2016069821 May 2016 WO
2016089844 Jun 2016 WO
2016118683 Jul 2016 WO
2016154284 Sep 2016 WO
2016176171 Nov 2016 WO
2016178966 Nov 2016 WO
2016201027 Dec 2016 WO
2017038075 Mar 2017 WO
2017062798 Apr 2017 WO
2017127489 Jul 2017 WO
2017210376 Dec 2017 WO
2018162385 Sep 2018 WO
Non-Patent Literature Citations (140)
Entry
Machine Translation of WO-2013160994-A1, Oct. 2013 (Year: 2013).
Machine Translation of JP-2016063114-A, Apr. 2016 (Year: 2016).
“EagleEtch” Product Brochure, EuropeTec USA Inc., pp. 1-8, Aug. 1, 2014.
“Etched Laser Filament Tracks in Glasses and Polymers”, E. Uzgiris and R. Fleischer. (1973) Phys. Rev. A 7, 734-740.
“Micro-machinability of silver-sodium ion-exchanged glass by UV nanosecond laser”, A. Matsusaka and T. Watanabe (2008). J. Materials Processing Technology, 514-520.
“Micromachining of glass by the third harmonic of nanosecond Nd:YVO4 laser”, A. Ramil, J. Lamas, J.C. Alvarez, A.J. Lopez, E. Saavedra, and A. Yanez (2009). Applied Surface Science 255, 5557-5560.
“PHAROS High-power femtosecond laser system” product brochure; Light Conversion, Vilnius, LT; Apr. 18, 2011, pp. 1-2.
“Projection ablation of glass-based single and arrayed microstructures using excimer laser”, Y-T Chen, K-J Ma, A.A. Tseng, and P.H. Chen. (2005) Optics and Laser Technology 37, 271-280.
“TruMicro 5000” Product Manual, Trumpf Laser GmbH + Co. KG, pp. 1-4, Aug. 2011.
“What is the difference between Ra and RMS?”; Harrison Electropolishing LP; (http://www.harrisonep.com/electropolishingra.html), Accessed Aug. 8, 2016.
Abakians et al. “Evaporative Cutting of a Semitransparent Body With a Moving CW Laser”, J. Heat Transfer 110(4a), 924-930 (Nov. 1, 1988) (7 pages) doi:10.1115/1.3250594.
Abramov et al., “Laser separation of chemically strengthened glass”; Physics Procedia 5 (2010) 285-290, Elsevier.; doi: 10.1016/j.phpro.2010.08.054.
Ahmed et al. “Display glass cutting by femtosecond laser induced single shot periodic void array” Applied Physics A: Materials Science and Proccessing vol. 93 No. 1 (2008) pp. 189-192.
Arimoto et al., “Imaging properties of axicon in a scanning optical system”; Applied Optics, Nov. 1, 1992, vol. 31, No. 31, pp. 6653-6657.
ASTM standard C770-16, entitled “Standard Test Method for Measurement of Glass Stress-Optical Coefficient,” downloaded Jan. 4, 2017.
Bagchi et al. “Fast ion beams from intense, femtosecond laser irradiated nanostructured surfaces” Applied Physics B 88 (2007) p. 167-173.
Benjamin et al.; “The Adhesion of Evaporated Metal Films on Glass” ; Proc. Roy. Soc. A., vol. 261, (1962); pp. 516-531.
Bhuyan et al. “Laser micro- and nanostructuring using femtosecond Bessel beams”, Eur. Phys. J. Special Topics 199 (2011) p. 101-110.
Bhuyan et al. “Single shot high aspect ratio bulk nanostructuring of fused silica using chirp-controlled ultrafast laser Bessel beams” Applied Physics Letters 104 (2014) 021107.
Bhuyan et al. “Ultrafast Bessel beams for high aspect ratio taper free micromachining of glass” Proc. Of SPIE vol. 7728 77281V-1.
Bhuyan et al., “Femtosecond non-diffracting Bessel beams and controlled nanoscale ablation” by IEEE (2011).
Bhuyan et al., “High aspect ratio nanochannel machining using single shot femtosecond Bessel beams”; Applied Physics Letters 97, 081102 (2010); doi: 10.1063/1.3479419.
Bhuyan et al., “High aspect ratio taper-free microchannel fabrication using femtosecond Bessel beams”; Optics Express (2010) vol. 18, No. 2, pp. 566-574.
Borghi et al.; “M2 Factor of Bessel-Gauss Beams” ; Optics Letters; vol. 22, No. 5; (1997) pp. 262-264.
Case Design Guidelines for Apple Devices Release R5 (https://web.archive.org/web/20131006050442/https://developer.apple.com/resources/cases/Case-Design-Guidelines. pdf; archived on Oct. 6, 2013).
Chen et al. “Development of an AOI system for chips with a hole on backside based on a frame imager” Proc. of SPIE vol. 9903, 2016. 6 pgs. (Jan. 26, 2016).
Chen et al. “Projection ablation of glass-based single and arrayed microstructures using excimer laser”, (2005) Optics and Laser Technology 37, 271-280.
Chiao et al. 9. “Self-trapping of optical beams,” Phys. Rev. Lett, vol. 13, No. 15, p. 479 (1964).
Corning Inc., “Corning(Registered) Eagle2000 TM AMLCD Glass Substrates Material Information”, issued Apr. 2005.
Corning Inc., “Corning(Registered) 1737 AM LCD Glass Substrates Material Information”, issued Aug. 2002.
Corning, “Properties of VYCOR Code 7913 96% Silica High Temperature Glass,” Apr. 2014.
Couairon et al. “Femtosecond filamentation in transparent media” Physics Reports 441 (2007) pp. 47-189.
Courvoisier et al. “Applications of femtosecond Bessel beams to laser ablation” Applied Physics A (2013) 112, p. 29-34.
Courvoisier et al. “Surface nanoprocessing with non-diffracting femtosecond Bessel beams” Optics Letters vol. 34 No 20, (2009) p. 3163-3165.
Cubeddu et al., “A compact time-resolved reflectance system for dual-wavelength multichannel assessment of tissue absorption and scattering”; Part of the SPIE Conference on Optical Tomography and Spectroscopy of Tissue III, San Jose, CA (Jan. 1999), SPIE vol. 3597, 0277-786X/99, pp. 450-455.
Cubeddu et al., “Compact tissue oximeter based on dual-wavelength multichannel time-resolved reflectance”; Applied Optics, vol. 38, No. 16, Jun. 1, 1999, pp. 3670-3680.
Ding et al., “High-resolution optical coherence tomography over a large depth range with an axicon lens”; Optic Letters, vol. 27, No. 4, pp. 243-245, Feb. 15, 2002, Optical Society of America.
Dong et al. “On-axis irradiance distribution of axicons illuminated by spherical wave”, Optics & Laser Technology 39 (2007) 1258-1261.
Dumin. “Exact solutions for nondiffracting beams I. The scaler theory” J. Opt. Soc. Am. A. 4(4) pp. 651-654.
Duocastella et al. “Bessel and annular beams for material processing”, Laser Photonics Rev. 6, 607-621, 2012.
Durnin. “Exact solutions for nondiffracting beams I. The scaler theory” J. Opt. Soc. Am. A. 4(4) pp. 651-654.
Eaton et al. “Heat accumulation effects in femtosecond laser written waveguides with variable repetition rates”, Opt. Exp. 5280, vol. 14, No. 23, Jun. 2006.
Gattass et al. “Micromachining of bulk glass with bursts of femtosecond laser pulses at variable repetition rates” Opt. Exp. 5280, vol. 14, No. 23, Jun. 2006.
Girkin et al., “Macroscopic multiphoton biomedical imaging using semiconductor saturable Bragg reflector modelocked Lasers”; Part of the SPIE Conference on Commercial and Biomedical Applications of Ultrafast Lasers, San Jose, CA (Jan. 1999), SPIE vol. 3616, 0277-786X/99, pp. 92-98.
Glezer et al., “Ultrafast-laser driven micro-explosions in transparent materials”; Applied Physics Letters, vol. 71 (1997), pp. 882-884.
Golub, I., “Fresnel axicon”; Optic Letters, vol. 31, No. 12, Jun. 15, 2006, Optical Society of America, pp. 1890-1892.
Gori et al. “Analytical derivation of the optimum triplicator” Optics Communications 157 (1998) pp. 13-16.
Handbook of Adhesives (3rd edition, Edited by Irving Skeist).
Herman et al., “Laser micromachining of 'transparent' fused silica with 1-ps pulses and pulse trains”; Part of the SPIE Conference on Commercial and Biomedical Applications of Ultrafast Lasers, San Jose, CA (Jan. 1999), SPIE vol. 3616, 0277-786X/99, pp. 148-155.
Honda et al. “A Novel Polymer Film that Controls Light Transmission”, Progress in Pacific Polymer Science 3, 159-169 (1994).
http://www.gtat.com/Collateral/Documents/English-US/Sapphire/12-21-12_GT_TouchScreen_V3_web.pdf.
Hu et al. “5-axis laser cutting interference detection and correction based on STL model” (2009) Zhongguo Jiguang/Chinese Journal of Lasers, 36 (12), pp. 3313-3317.
Huang et al., “Laser etching of glass substrates by 1064 nm laser irradiation”, Applied Physics, Oct. 2008, vol. 93, Issue 1, pp. 159-162.
Iijima et al.; “Resistivity Reduction By External Oxidation of Cu-Mn Alloy Films for Semiconductor Interconnect Application”; Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures Processing, Measurement, and Phenomena, 27, 1963-1968 (2009.
Integrace: “Borosilicate glass: Technical Glass by Pulles & Hanique: Duran & Pyrex”, Mar. 15, 2012 (Mar. 15, 2012) XP055524680, Retrived from the Internet: URL: https://web.archive.org/web/20120315092729/http://www.pulleshanique.com/02_borosilicate-glass.htm.
International Search Report and Written Opinion of the International Searching Authority; PCT/US2018/033814; dated Nov. 30, 2018; 10 Pages; European Patent Office.
Jaramillo et al., Wet etching of hydrogenated amorphous carbon films, Mar. 7, 2001, Diamond and Related Materials, vol. 10, Issues 3-7, pp. 976-979 (Year: 2001).
Juodkazis S. et al. Laser induced microexplosion confined in the bulk of a sapphire crystal: evidence of multimegabar pressures., Phys. Rev. Lett. 96, 166101, 2006.
Karlsson et al. “The technology of chemical glass strengthening - a review” Glass Technol: Eur. J. Glass Sci. Technol. A (2010) 51 (2) pp. 41-54.
Kiyama et al.; “Examination of Etching Agent and Etching Mechanism On Femtosecond Laser Microfabrication of Channels Inside Vitreous Silica Substrates”; J. Phys. Chem. C, 2009, 113, pp. 11560-11566.
Koike et al.; “P-33: Cu-Mn Electrodes For a-Si TFT and Its Electrical Characteristics” ; SID Symposium Digest of Technical Papers, 41:1, 1343-1346 (2010).
Koike et al.; “Self-Forming Diffusion Barrier Layer In Cu-Mn Alloy Metallization”; Appl Phys. Lett. 87, 041911-1-041911-3 (2005).
Kondo et al., Three-Dimensional Microdrilling of Glass by Multiphoton Process and Chemical Etching, 1999, Japanese Journal of Applied Physics, vol. 38, Part 2, No. 10A (Year: 1999).
Kosareva et al., “Formation of extended plasma channels in a condensed medium upon axicon focusing of a femtosecond laser pulse”; Quantum Electronics 35 (11) 1013-1014 (2005), Kvantovaya Elektronika and Turpion Ltd.; doi: 10.1070/QE2005v035n11ABEH013031.
Koyama et al. “Laser-micromachining for Ag lon Exchanged Glasses,” Second International Symposium on Laser Precision Microfabrication, Proc. SPE vol. 4426 (2002) 162-165.
Kruger et al. “UV laser drilling of SiC for semiconductor device fabrication,” J_Physics:Conference Series 59 (2007) 740-744.
Kruger et al., “Femtosecond-pulse visible laser processing of transparent materials”; Applied Surface Science 96-98 (1996) 430-438.
Kruger et al., “Laser micromachining of barium aluminium borosilicate glass with pluse durations between 20 fs and 3 ps”; Applied Surface Science 127-129 (1998) 892-898.
Kruger et al., “Structuring of dielectric and metallic materials with ultrashort laser pulses between 20 fs and 3 ps”; SPIE vol. 2991, 0277-786X/97, pp. 40-47.
Lapczyna et al., “Ultra high repetition rate (133 MHZ) laser ablation of aluminum with 1.2-ps pulses”; Applied Physics A 69 [Suppl.], S883-S886, Springer-Verlag (1999); doi: 10.1007/s003399900300.
Levy et al. “Design, fabrication, and characterization of circular Dammann gratings based on grayscale lithography,” Opt. Lett vol. 35, No. 6, p. 880-882 (2010).
Li et al. “Thick Polymer cover layers for laser micromachining of fine holes,” Applied Physics A, Sep. 2005, vol. 81, Issues 4, pp. 753-758.
Liu X et al. “laser ablation and micromachining with ultrashort laser pulses”, IEEE J. Quantum Electronics, 22, 1706-1716, 1997.
Machine Translation of J P-2004363212-A, Dec. 2004 (Year: 2004).
Machine Translation of J P-2011178642-A, Sep. 2011 (Year: 2011).
Machine Translation of J P-2015146410-A, Aug. 2015 (Year: 2015).
Machine Translation of J P-2008094641-A, Apr. 2008 (Year: 2008).
Machine Translation of JP-2008288577-A, Nov. 2008 (Year: 2008).
Machine Translation of WO 2005034594 A1/JP 4702794 B2, Jun. 2011 (Year: 2011).
Machine Translation of WO 2018162385 A1, Sep. 2018 (Year: 2018).
Madehow.com, Liquid Crystal Display {LCD), Jan. 29, 2006, https:/fweb.archive.org/web/20060129092154/http://www.madehow.comNolume-1/Liquid-Crystal-Display-LCD.html; pp. 1-6.
Maeda et al. “Optical performance of angle-dependent light-control glass”, Proc. SPIE 1536, Optical Materials Technology for Energy Efficiency and Solar Energy Conversion X, 138 (Dec. 1, 1991).
Matsusaka et al. “Micro-machinability of silversodium ion-exchanged glass by UV nanosecond laser,” J. Materials Processing Technology 202 (2008) 514-520.
Mbise et al. “Angular selective window coatings: theory and experiments” J. Phys. D: Appl. Phys. 30 2103 (1997).
McGloin et al. “Bessel beams: diffraction in a new light” Contemporary Physics, vol. 46 No. 1 (2005) pp. 15-28.
Merola et al. “Characterization of Bessel beams generated by polymeric microaxicons” Meas. Sci. Technol. 23 (2012) 10 pgs.
Microchemicals, “Silicon Wafers, Quartz Wafers, Glass Wafers,” Product Specifications: Brochure. 2014, 28 pgs.
Miranda et al. (Ultraviolet-induced crosslinking of poly(vinyl alcohol) evaluated by principal component analysis of FTIR spectra, Polym Int 50:1068-1072(2001)).
Mirkhalaf, M. et al., Overcoming the brittleness of glass through bio-inspiration and micro-achitecture, Nature Communications, 5:3166/ncomm4166(2014).
Mukhina L.; “Laser Pulse Damage On the Surface of Ion Exchange Treated Glass”; Soviet Journal of Glass Physics and Chemistry; vol. 19; No. 3; pp. 269-272; (1993.
Ogutu et al.; “Superconformal Filling of High Aspect Ratio Through Glass Vias (TGV) for Interposer Applications Using TNBT and NTBC Additives”; Journal of the Electrochemical Society, 162 (9), D457-D464 (2015).
Perry et al., “Ultrashort-pulse laser machining of dielectric materials”; Journal of Applied Physics, vol. 85, No. 9, May 1, 1999, American Institute of Physics, pp. 6803-6810.
Perry et al., “Ultrashort-pulse laser machining”; UCRL-1D-132159, Sep. 1998, pp. 1-38.
Perry et al., “Ultrashort-pulse laser machining”; UCRL-JC-132159 Rev 1., Jan. 22, 1999, pp. 1-24.
Pie Scientific, Photoresist stripping and descum organic contamination removal for silicon wafer, Feb. 2016 (Year: 2016).
Polavka et al. “Crosslinking of polymers by the effect of ultraviolet radiation crosslinking of poly(vinyl alcohol) in the presence oflerephthalic aldehyde”; 1980.
Polynkin et al., “Extended filamentation with temporally chirped femtosecond Bessel-Gauss beams in air”; Optics Express, vol. 17, No. 2, Jan. 19, 2009, OSA, pp. 575-584.
Ramil et al. “Micromachining of glass by the third harmonic of nanosecond Nd:YV04 laser”, Applied Surface Science 255 (2009) p. 5557-5560.
Romero et al. “Theory of optimal beam splitting by phase gratings. Il. Square and hexagonal gratings” J. Opt. Soc. Am. A/vol. 24 No. 8 (2007) pp. 2296-2312.
Salleo A et al., Machining of transparent materials using IR and UV nanosecond laser pulses, Appl. Physics A 71, 601-608, 2000.
Serafetinides et al., “Polymer ablation by ultra-short pulsed lasers” Proceedings of SPIE vol. 3885 (2000) http://proceedings.spiedigitallibrary.org/.
Serafetinides et al., “Ultra-short pulsed laser ablation of polymers”; Applied Surface Science 180 (2001) 42-56.
Shah et al. “Micromachining with a high repetition rate femtosecond fiber laser”, Journal of Laser Micro/Nanoengineering vol. 3 No. 3 (2008) pp. 157-162.
Shealy et al. “Geometric optics-based design of laser beam shapers”, Opt. Eng. 42(11), 3123-3138 (2003). doi:10.1117/1.1617311.
Shorey et al.; “Progress and Application of Through Glass via (TGV) Technology” ; 2016 Pan Pacific Microelectronis Symposium, SMTA, Jan. 25, 2016; pp. 1-6.
Shorey; “Leveraging Glass for Advanced Packaging and loT” ; Apr. 21, 2016, Retrieved Form the Internet: URL:http://www.corning.com/media/worldwide/cdt/documents/iMAPs%20-%20Corn- ing%20Overview%20-%204-21-16%20FINALpptx.pdf.
Siegman; “New Development in Laser Resonators” ; SPIE, vol. 1227, Optical Resonators (1990) pp. 2-14.
Smedskjaer et al.; “Impact Of ZnO On the Structure and Properties of Sodium Aluminosilicate Glasses: Comparison With Alkaline Earth Oxides,” Journal of Non- Crystalline Solids 381, 58-64 (2013).
Stoian et al. “Spatial and temporal laser pulse design for material processing on ultrafast scales” Applied Physics A (2014) 114, p. 119-127.
Sundaram et al., “Inducing and probing non-thermal transitions in semiconductors using femtosecond laser pulses”; Nature Miracles, vol. 1, Dec. 2002, Nature Publishing Group (2002), pp. 217-224.
Swift Glass, Quartz/Fused Silica, Mar. 2016 (Year: 2016).
Thiele; “Relation Between Catalytic Activity and Size of Particle” ; Industrial and Engineering Chemistry, vol. 31, No. 7; (1939) pp. 916-920.
Tom Christiansen, Tami Erickson; Standard Operating Procedure: Spin-on-Glass, Surface Level Characterization (2000),.
Topper et al.; “3-D Thin Film Interposer Based On TGV (Through Glass Vias): an Alternative To Si-Interposer”; IEEE, Electronic Components and Technology Conference; 2010; pp. 66-73.
Toytman et al. “Optical breakdown in transparent media with adjustable axial length and location”, Optics Express vol. 18 No 24, 24688-24698 (2010).
Tsai et al. “Investigation of underwater laser drilling for brittle substrates,” J. Materials Processing technology 209 (2009) 2838-2846.
U.S. Appl. No. 62/846,059; Cai et al. “Silicate Glass Compositions Useful for the Efficient Production of Through Glass Vias” , Filed May 10, 2019, 43 pgs.
U.S. Appl. No. 62/846, 102; Guo et al. “High Silicate Glass Articles Possessing Through Glass Vias and Methods of Making and Using Thereof” , Filed May 10, 2019, 36 pgs.
Uzgiris et al. “Etched Laser Filament Tracks in Glasses and Polymers”, (1973) Phys. Rev. A 7, 734-740.
Vanagas et al., “Glass cutting by femtosecond pulsed irradiation”; J. Micro/Nanolith. MEMS MOEMS. 3(2), 358-363 (Apr. 1, 2004); doi: 10.1117/1.1668274.
Varel et al., “Micromachining of quartz with ultrashort laser pulses”; Applied Physics A 65, 367-373, Springer-Verlag (1997).
Velpula et al.. “Ultrafast imaging of free carriers: controlled excitation with chirped ultrafast laser Bessel beams”, Proc. Of SPIE vol. 8967 896711-1 (2014).
Wakayama et al. “Small size probe for inner profile measurement of pipes using optical fiber ring beam device” Proc. of SPIE vol. 8563, 2012. 7 pgs.
Wang et al., “Investigation on CO2 laser irradiation inducing glass strip peeling for microchannel formation”, BIOMICROFLUIDICS 6, 012820 (2012).
West et al., Optimisation of photoresist removal from silicon wafers using atmosphericpressure plasma jet effluent, Jul. 2015, 22nd International Symposium on Plasma Chemistry (Year: 2015).
Wlodarczyk et al. “The Impact of Graphite Coating and Wavelength on Picosecond Laser Machining of Optical Glasses,” , 31st ICALEO Program Notes (2012). Paper M#309.
Wu et al., “A Study on Annealing Mechanisms With Different Manganese Contents in CuMn Alloy”; Journal of Alloys and Compounds, vol. 542, 2012, pp. 118-123.
Wu et al. “Optimal orientation of the cutting head for enhancing smoothness movement in three-dimensional laser cutting” (2013) Zhongguo Jiguang/Chinese Journal of Lasers, 40 (1), art. No. 0103005.
Xu et al. “Optimization of 3D laser cutting head orientation based on the minimum energy consumption” (2014) International Journal of Advanced Manufacturing Technology, 74 (9-12), pp. 1283-1291.
Yan et al. “Fiber structure to convert a Gaussian beam to higher-order optical orbital angular momentum modes” Optics Letters vol. 37 No. 16 (2012) pp. 3294-3296.
Yun et al.; “p. 23:The Contact Properties and TFT Structures of A-IGZO TFTS Combined With Cu—Mn Alloy Electrodes”; SID Symposium Digest of Technical Papers 42:1, 1177-1180.
Zavyalov; “3D Hole Inspection Using Lens With High Field Curvature”; Measurement Science Review; vol. 15, No. 1; 2015; pp. 52-57.
Zeng et al. “Characteristic analysis of a refractive axicon system for optical trepanning”; Optical Engineering 45(9), 094302 (Sep. 2006), pp. 094302-1-094302-10.
Zhang et al., “Design of diffractive-phase axicon illuminated by a Gaussian-profile beam”; Acta Physica Sinica (overseas edition), vol. 5, No. 5 (May 1996) Chin. Phys. Soc., 1004-423X/96/05050354-11, pp. 354-364.
Taiwanese Patent Application No. 107117314, Office Action, dated Aug. 16, 2022, 1 page; Taiwanese Patent Office.
Korean Patent Application No. 10-2019-7038257, Korean Office Action, dated Nov. 1, 2022, 6 pages (3 pages of English Translation and 3 pages of Original copy); Korean Patent Office.
Bhuyan et al. “Ultrafast Bessel beams for high aspect ratio taper free micromachining of glass” Proc. Of SPIE vol. 7728 77281V-1, Apr. 30, 2010, pp. 1-8.
Chinese Patent Application No. 201880034479.7, Office Action, dated Feb. 24, 2023, 5 pages Chinese Patent Office.
Durnin. “Exact solutions for nondiffracting beams I. The scaler theory” J. Opt. Soc. Am. A. 4(4), Apr. 1, 1987, pp. 651-654.
Kruger et al., “Structuring of dielectric and metallic materials with ultrashort laser pulses between 20 fs and 3 ps”; SPIE vol. 2991, 0277-786X/97, May 9, 1997, pp. 40-47.
Related Publications (1)
Number Date Country
20210269357 A1 Sep 2021 US
Provisional Applications (2)
Number Date Country
62588615 Nov 2017 US
62510957 May 2017 US
Divisions (1)
Number Date Country
Parent 15978430 May 2018 US
Child 17320646 US