Patent Application
20240337890
An electrophoretic display (EPD) changes color by modifying the position of a charged colored particle with respect to a light-transmissive viewing surface. Such electrophoretic displays are typically referred to as “electronic paper” or “ePaper” because the resulting display has high contrast and is sunlight-readable, much like ink on paper. Electrophoretic displays have enjoyed widespread adoption in eReaders, such as the AMAZON KINDLE® because the electrophoretic displays provide a book-like reading experience, use little power, and allow a user to carry a library of hundreds of books in a lightweight handheld device.
For many years, electrophoretic displays included only two types of charged color particles, black and white. (To be sure, “color” as used herein includes black and white.) The white particles are often of the light scattering type, and comprise, e.g., titanium dioxide, while the black particle are absorptive across the visible spectrum, and may comprise carbon black, or an absorptive metal oxide, such as copper chromite. In the simplest sense, a black and white electrophoretic display only requires a light-transmissive electrode at the viewing surface, a back electrode, and an electrophoretic medium including oppositely charged white and black particles. When a voltage of one polarity is provided, the white particles move to the viewing surface, and when a voltage of the opposite polarity is provided the black particles move to the viewing surface. If the back electrode includes controllable regions (pixels)—either segmented electrodes or an active matrix of pixel electrodes controlled by transistors—a pattern can be made to appear electronically at the viewing surface. The pattern can be, e.g., the text to a book.
More recently, a variety of color option have become commercially available for electrophoretic displays, including three-color displays (black, white, red; black white, yellow), and four color displays (black, white, red, yellow). Similar to the operation of black and white electrophoretic displays, electrophoretic displays with three or four reflective particles operate similar to the simple black and white displays because the desired color particle is driven to the viewing surface. The driving schemes are far more complicated than only black and white, but in the end, the optical function of the particles is the same.
Advanced Color electronic Paper (ACeP™) also included four particles, but the cyan, yellow, and magenta particles are subtractive rather than reflective, thereby allowing thousands of colors to be produced at each pixel. The color process is functionally equivalent to the printing methods that have long been used in offset printing and ink-jet printers. A given color is produced by using the correct ratio of cyan, yellow, and magenta on a bright white paper background. In the instance of ACeP, the relative positions of the cyan, yellow, magenta and white particles with respect to the viewing surface will determine the color at each pixel. While this type of electrophoretic display allows for thousands of colors at each pixel, it is critical to carefully control the position of each of the (50 to 500 nanometer-sized) pigments within a working space of about 10 to 20 micrometers in thickness. Obviously, variations in the position of the particles will result in incorrect colors being displayed at a given pixel. Accordingly, exquisite voltage control is required for such a system. More details of this system are available in the following U.S. Patents, all of which are incorporated by reference in their entireties: U.S. Pat. Nos. 9,361,836; 9,921,451; 10,276,109; 10,353,266; 10,467,984; and 10,593,272.
The term gray state is used herein in its conventional meaning in the imaging art to refer to a state intermediate two extreme optical states of a pixel, and does not necessarily imply a black-white transition between these two extreme states. For example, several of the E Ink patents and published applications referred to below describe electrophoretic displays in which the extreme states are white and deep blue, so that an intermediate gray state would actually be pale blue. Indeed, as already mentioned, the change in optical state may not be a color change at all. The terms black and white may be used hereinafter to refer to the two extreme optical states of a display, and should be understood as normally including extreme optical states which are not strictly black and white, e.g. the aforementioned white and dark blue states.
The terms bistable and bistability are used herein in their conventional meaning in the art to refer to displays comprising display elements having first and second display states differing in at least one optical property, and such that after any given element has been driven, by means of an addressing pulse of finite duration, to assume either its first or second display state, after the addressing pulse has terminated, that state will persist for at least several times, e.g., at least four times, the minimum duration of the addressing pulse required to change the state of the display element. It is shown in U.S. Pat. No. 7,170,670 that some particle-based electrophoretic displays capable of gray scale are stable not only in their extreme black and white states but also in their intermediate gray states, and the same is true of some other types of electro-optic displays. This type of display is properly called multi-stable rather than bistable, although for convenience the term bistable may be used herein to cover both bistable and multi-stable displays.
The term impulse, when used to refer to driving an electrophoretic display, is used herein to refer to the integral of the applied voltage with respect to time during the period in which the display is driven.
A particle that absorbs, scatters, or reflects light, either in a broad band or at selected wavelengths, is referred to herein as a colored or pigment particle. Various materials other than pigments (in the strict sense of that term as meaning insoluble colored materials) that absorb or reflect light, such as dyes or photonic crystals, etc., may also be used in the electrophoretic media and displays of the present invention.
Particle-based electrophoretic displays have been the subject of intense research and development for a number of years. In such displays, a plurality of charged particles (sometimes referred to as pigment particles) move through a fluid under the influence of an electric field. Electrophoretic displays can have attributes of good brightness and contrast, wide viewing angles, state bistability, and low power consumption when compared with liquid crystal displays. Nevertheless, problems with the long-term image quality of these displays have prevented their widespread usage. For example, particles that make up electrophoretic displays tend to settle, resulting in inadequate service-life for these displays.
As noted above, electrophoretic media require the presence of a fluid. In most prior art electrophoretic media, this fluid is a liquid, but electrophoretic media can be produced using gaseous fluids; see, e.g., Kitamura, T., et al., Electrical toner movement for electronic paper-like display, IDW Japan, 2001, Paper HCS1-1, and Yamaguchi, Y., et al., Toner display using insulative particles charged triboelectrically, IDW Japan, 2001, Paper AMD4-4). See also U.S. Pat. Nos. 7,321,459 and 7,236,291. Such gas-based electrophoretic media appear to be susceptible to the same types of problems due to particle settling as liquid-based electrophoretic media, when the media are used in an orientation which permits such settling, e.g., in a sign where the medium is disposed in a vertical plane. Indeed, particle settling appears to be a more serious problem in gas-based electrophoretic media than in liquid-based ones, since the lower viscosity of gaseous suspending fluids as compared with liquid ones allows more rapid settling of the electrophoretic particles.
Numerous patents and applications assigned to or in the names of the Massachusetts Institute of Technology (MIT) and E Ink Corporation describe various technologies used in encapsulated electrophoretic and other electro-optic media. Such encapsulated media comprise numerous small capsules, each of which itself comprises an internal phase containing electrophoretically-mobile particles in a fluid medium, and a capsule wall surrounding the internal phase. Typically, the capsules are themselves held within a polymeric binder to form a coherent layer positioned between two electrodes. The technologies described in these patents and applications include:
Many of the aforementioned patents and applications recognize that the walls surrounding the discrete microcapsules in an encapsulated electrophoretic medium could be replaced by a continuous phase, thus producing a so-called polymer-dispersed electrophoretic display, in which the electrophoretic medium comprises a plurality of discrete droplets of an electrophoretic fluid and a continuous phase of a polymeric material, and that the discrete droplets of electrophoretic fluid within such a polymer-dispersed electrophoretic display may be regarded as capsules or microcapsules even though no discrete capsule membrane is associated with each individual droplet; see e.g., U.S. Pat. No. 6,866,760. Accordingly, for purposes of the present application, such polymer-dispersed electrophoretic media are regarded as sub-species of encapsulated electrophoretic media.
A related type of electrophoretic display is a so-called microcell electrophoretic display. In a microcell electrophoretic display, the charged particles and the fluid are not encapsulated within microcapsules but instead are retained within a plurality of cavities formed within a carrier medium, typically a polymeric film. See, e.g., U.S. Pat. Nos. 6,672,921 and 6,788,449.
Although electrophoretic media are often opaque (since, e.g., in many electrophoretic media, the particles substantially block transmission of visible light through the display) and operate in a reflective mode, many electrophoretic displays can be made to operate in a so-called shutter mode in which one display state is substantially opaque and one is light-transmissive. Sec, e.g., U.S. Pat. Nos. 5,872,552; 6,130,774; 6,144,361; 6,172,798; 6,271,823; 6,225,971; and 6,184,856. Dielectrophoretic displays, which are similar to electrophoretic displays but rely upon variations in electric field strength, can operate in a similar mode; see U.S. Pat. No. 4,418,346. Other types of electro-optic displays may also be capable of operating in shutter mode. Electro-optic media operating in shutter mode can be used in multi-layer structures for full color displays; in such structures, at least one layer adjacent the viewing surface of the display operates in shutter mode to expose or conceal a second layer more distant from the viewing surface.
An encapsulated electrophoretic display typically does not suffer from the clustering and settling failure mode of traditional electrophoretic devices and provides further advantages, such as the ability to print or coat the display on a wide variety of flexible and rigid substrates. (Use of the word printing is intended to include all forms of printing and coating, including, but without limitation: pre-metered coatings such as patch die coating, slot or extrusion coating, slide or cascade coating, curtain coating; roll coating such as knife over roll coating, forward and reverse roll coating; gravure coating; dip coating; spray coating; meniscus coating; spin coating; brush coating; air knife coating; silk screen printing processes; electrostatic printing processes; thermal printing processes; ink jet printing processes; electrophoretic deposition (See U.S. Pat. No. 7,339,715); and other similar techniques.) Thus, the resulting display can be flexible. Further, because the display medium can be printed (using a variety of methods), the display itself can be made inexpensively.
As indicated above most simple prior art electrophoretic media essentially display only two colors. Such electrophoretic media either use a single type of electrophoretic particle having a first color in a colored fluid having a second, different color (in which case, the first color is displayed when the particles lie adjacent the viewing surface of the display and the second color is displayed when the particles are spaced from the viewing surface), or first and second types of electrophoretic particles having differing first and second colors in an uncolored fluid (in which case, the first color is displayed when the first type of particles lie adjacent the viewing surface of the display and the second color is displayed when the second type of particles lie adjacent the viewing surface). Typically the two colors are black and white. If a full color display is desired, a color filter array may be deposited over the viewing surface of the monochrome (black and white) display. Displays with color filter arrays rely on area sharing and color blending to create color stimuli. The available display area is shared between three or four primary colors such as red/green/blue (RGB) or red/green/blue/white (RGBW), and the filters can be arranged in one-dimensional (stripe) or two-dimensional (2×2) repeat patterns. Other choices of primary colors or more than three primaries are also known in the art. The three (in the case of RGB displays) or four (in the case of RGBW displays) sub-pixels are chosen small enough so that at the intended viewing distance they visually blend together to a single pixel with a uniform color stimulus (‘color blending’). The inherent disadvantage of area sharing is that the colorants are always present, and colors can only be modulated by switching the corresponding pixels of the underlying monochrome display to white or black (switching the corresponding primary colors on or off). For example, in an ideal RGBW display, each of the red, green, blue and white primaries occupy one fourth of the display arca (one sub-pixel out of four), with the white sub-pixel being as bright as the underlying monochrome display white, and each of the colored sub-pixels being no lighter than one third of the monochrome display white. The brightness of the white color shown by the display as a whole cannot be more than one half of the brightness of the white sub-pixel (white areas of the display are produced by displaying the one white sub-pixel out of each four, plus each colored sub-pixel in its colored form being equivalent to one third of a white sub-pixel, so the three colored sub-pixels combined contribute no more than the one white sub-pixel). The brightness and saturation of colors is lowered by area-sharing with color pixels switched to black. Arca sharing is especially problematic when mixing yellow because it is lighter than any other color of equal brightness, and saturated yellow is almost as bright as white. Switching the blue pixels (one fourth of the display area) to black makes the yellow too dark.
U.S. Pat. Nos. 8,576,476 and 8,797,634 describe multicolor electrophoretic displays having a single back plane comprising independently addressable pixel electrodes and a common, light-transmissive front electrode. Between the back plane and the front electrode is disposed a plurality of electrophoretic layers. Displays described in these applications are capable of rendering any of the primary colors (red, green, blue, cyan, magenta, yellow, white and black) at any pixel location. However, there are disadvantages to the use of multiple electrophoretic layers located between a single set of addressing electrodes. The electric field experienced by the particles in a particular layer is lower than would be the case for a single electrophoretic layer addressed with the same voltage. In addition, optical losses in an electrophoretic layer closest to the viewing surface (e.g., caused by light scattering or unwanted absorption) may affect the appearance of images formed in underlying electrophoretic layers.
Two other types of electrophoretic display systems provide a single electrophoretic medium capable of rendering any color at any pixel location. Specifically, U.S. Pat. No. 9,697,778 describes a display in which a dyed solvent is combined with a white (light-scattering) particle that moves in a first direction when addressed with a low applied voltage and in the opposite direction when addressed with a higher voltage. When the white particles and the dyed solvent are combined with two additional particles of opposite charge to the white particle, it is possible to render a full-color display. However, the color states of the '778 patent are not acceptable for applications such as a text reader. In particular, there will always be some of the dyed fluid separating the white scattering particle from the viewing surface, which leads to a tint in the white state of the display.
A second form of electrophoretic medium capable of rendering any color at any pixel location is described in U.S. Pat. No. 9,921,451. In the '451 patent, the electrophoretic medium includes four particles: white, cyan, magenta and yellow, in which two of the particles are positively-charged and two negatively charged. However displays of the '451 patent also suffer from color mixing with the white state. Because one of the particles has the same charge as the white particle, some quantity of the same-charge particle moves with the white toward the viewing surface when the white state is desired. While it is possible to overcome this unwanted tinting with complex waveforms, such waveforms greatly increase the update time of the display and in some instances, result in unacceptable “flashing” between images.
A color electrophoretic display providing an improved black optical state in accordance with one aspect of the invention includes a light-transmissive electrode layer at a viewing surface, a back electrode layer, and an electrophoretic medium disposed therebetween. The electrophoretic medium comprises a non-polar fluid and a multi-pigment particle system comprising five types of charged electrophoretic pigment particles dispersed in the non-polar fluid. The five types of charged electrophoretic pigment particles comprise: a first type of particle having a first optical property and a first charge polarity; a second type of particle having a second optical property, and having a second charge polarity with a first charge magnitude, said second charge polarity being opposite to the first charge polarity a third type of particle having a third optical property, and having the second charge polarity with a second charge magnitude smaller than the first charge magnitude; a fourth type of particle having a fourth optical property, and having the second charge polarity with a third charge magnitude smaller than the second charge magnitude; and a fifth type of particle having a fifth optical property, and having the second charge polarity with a fourth charge magnitude greater than the first charge magnitude. The first type of particle is white, the fifth type of particle is black, and the second, third, and fourth types of particles are each a different one of cyan, magenta, and yellow.
In one or more embodiments, the second, third, and fourth types of particles are cyan, magenta, and yellow, respectively.
In one or more embodiments, the first charge polarity is negative and the second charge polarity is positive.
As is well known in the art of electrophoresis, the charge magnitude (i.e., charge density per unit area of the pigment particle surface) is roughly proportional to the zeta potential (the electrical potential at the shear plane for electrophoretic motion) given a constant Debye length and dielectric constant. The values provided below to characterize charge magnitude (i.e., charge density) are zeta potentials measured in a hydrocarbon solvent in the presence of a surfactant (charge control agent).
In one or more embodiments, the first charge magnitude is about 80 mV to about 100 mV.
In one or more embodiments, the second charge magnitude is about 40 m V to about 50 mV.
In one or more embodiments, the third charge magnitude is about-5 mV to about 5 mV.
In one or more embodiments, the fourth charge magnitude is about 100 mV.
In one or more embodiments, the first type of particle has a charge magnitude of about-55 mV to about-70 m V.
In one or more embodiments, the back electrode layer includes an array of thin film transistors coupled to pixel electrodes. Each thin film transistor comprises a layer of a metal oxide semiconductor.
In one or more embodiments, the metal oxide semiconductor is indium gallium zinc oxide (IGZO).
In one or more embodiments, the thin film transistors comprising the layer of metal oxide semiconductor enable switching of control voltages greater than 25V and less than-25V while the light-transmissive electrode layer is held at constant voltage for changing optical states of pixels of the electrophoretic display.
In one or more embodiments, the black particles include a polymer shell grafted on a surface of the particles.
In one or more embodiments, the third type of particle is magenta and includes a polymer shell coated on the particles by dispersion polymerization.
Additional details of one or more embodiments of the subject matter described in this specification are set forth in the accompanying drawings and the description below. Other features, aspects, and advantages of the subject matter will become apparent from the descriptions contained herein and the accompanying drawings. It should be stressed that the accompanying drawings are schematic and not to scale. In particular, for ease of illustration, the thicknesses of the various layers in the drawings do not correspond to their actual thicknesses. Also, the thicknesses of the various layers are out of scale relative to their lateral dimensions. Generally, elements of similar structures are annotated with like reference numerals for illustrative purposes throughout the drawings. However, the specific properties and functions of elements in different embodiments may not be identical. Further, the drawings are only intended to facilitate the description of the subject matter. The drawings do not illustrate every aspect of the described embodiments and do not limit the scope of the present disclosure or claims.
Various embodiments disclosed herein relate to a five-particle electrophoretic medium in a display device providing an improved, more saturated black optical state at the device viewing surface.
U.S. Pat. No. 11,686,989, the content of which is incorporated by reference herein in its entirety, discloses a four-particle electrophoretic medium, including a first particle of a first polarity, and three other particles having the opposite polarity, but having different magnitudes of charge. Typically, such a system includes a negatively-charged white particle and positively-charged yellow, magenta, and cyan particles having subtractive primary colors. Additionally, some particles may be engineered so that their electrophoretic mobility is non-linear with respect to the strength of the applied electric field. Accordingly, one or more particles will experience a decrease in electrophoretic mobility with the application of a high electric field (e.g., 20V or greater) of the correct polarity. Such a four-particle system is shown schematically in
As shown in
The viewing surface of the
More specifically, when the cyan, magenta, and yellow particles lie below the white particles (Situation [A] in
It is possible that one subtractive primary color could be rendered by a particle that scatters light, so that the display would comprise two types of light-scattering particle, one of which would be white and another colored. In this case, however, the position of the light-scattering colored particles with respect to the other colored particles overlying the white particle would be important. For example, in rendering the color black (when all three colored particles lie over the white particles) the scattering colored particle cannot lie over the non-scattering colored particles (otherwise they will be partially or completely hidden behind the scattering particle and the color rendered will be that of the scattering colored particle, not black).
As standard with electrophoretic displays, the first surface 13 includes a common electrode 11, which is light-transmissive, e.g., constructed from a sheet of PET with indium tin oxide (ITO) disposed thereon. On the second surface 14, there is an electrode layer 12, which includes a plurality of pixel electrodes 15. Such pixel electrodes are described in U.S. Pat. No. 7,046,228, the content of which is incorporated herein by reference in its entirety. It is noted that while active matrix driving with a thin film transistor (TFT) backplane is mentioned for the layer of pixel electrodes, the scope of the present invention encompasses other types of electrode addressing as long as the electrodes serve the desired functions. For example, the top and bottom electrodes can be contiguous. Additionally, pixel electrode backplanes different from those described in the '228 patent are also suitable, and may include active matrix backplanes capable of providing higher driving voltages than typically found with amorphous silicon thin-film-transistor backplanes.
Newly-developed active matrix backplanes may include thin film transistors incorporating metal oxide materials, such as tungsten oxide, tin oxide, indium oxide, zinc oxide or more complex metal oxides such as indium gallium zirconium oxide. In these applications, a channel formation region is formed for each transistor using such metal oxide materials, allowing faster switching of higher voltages. Such metal oxide transistors also allow for less leakage in the “off” state of the thin-film transistor (TFT) than can be achieved by, e.g., amorphous silicon TFTs. In a typical scanning TFT backplane comprising n lines, the transistor will be in the “off” state for approximately a proportion (n−1)/n of the time required to refresh every line of the display. Any leakage of charge from the storage capacitors associated with each pixel would result in degradation of the electro-optical performance of the display. TFTs typically include a gate electrode, a gate-insulating film (typically SiO2), a metal source electrode, a metal drain electrode, and a metal oxide semiconductor film over the gate-insulating film, at least partially overlapping the gate electrode, source electrode, and drain electrode. Such backplanes are available from manufacturers such as Sharp/Foxconn, LG, and BOE. Such backplanes are able to provide driving voltages of +30V (or more). In some embodiments, intermediate voltage drivers are included so that the resulting driving waveforms may include five levels, or seven levels, or nine levels, or more.
One preferred metal oxide material for such applications is indium gallium zinc oxide (IGZO). IGZO-TFT has 20-50 times the electron mobility of amorphous silicon. By using IGZO TFTs in an active matrix backplane, it is possible to provide voltages of greater than 30V via a suitable display driver. Furthermore, a source driver capable of supplying at least five, and preferably seven levels provides a different driving paradigm for a four-particle electrophoretic display system. In an embodiment, there will be two positive voltages, two negative voltages, and zero volts. In another embodiment, there will be three positive voltages, three negative voltages, and zero volts. In an embodiment, there will be four positive voltages, four negative voltages, and zero volts. These levels may be chosen within the range of about-27V to +27V, without the limitations imposed by top plane switching as described above.
In one example, the first particle (negative) is white and scattering. The second particle (positive, medium charge magnitude) is magenta and absorptive. The third particle (positive, low charge magnitude) is yellow and absorptive. The fourth particle (positive, high charge magnitude) is cyan and absorptive. Table 1 below shows the diffuse reflectance of exemplary yellow, magenta, cyan and white particles useful in electrophoretic media, together with the ratio of their absorption and scattering coefficients according to the Kubelka-Munk analysis of these materials as dispersed in a poly (isobutylene) matrix.
The electrophoretic medium may be in any of the forms discussed above. Thus, the electrophoretic medium may be unencapsulated, encapsulated in discrete capsules surrounded by capsule walls, encapsulated in sealed microcells, or in the form of a polymer-dispersed medium. The pigments are described in detail elsewhere, such as in U.S. Pat. Nos. 9,697,778 and 9,921,451. Briefly, white particle W1 is a silanol-functionalized light-scattering pigment (titanium dioxide) to which a polymeric material comprising lauryl methacrylate (LMA) monomers has been attached as described in U.S. Pat. No. 7,002,728. White particle W2 is a polymer-coated titania produced substantially as described in Example 1 of U.S. Pat. No. 5,852,196, with a polymer coating comprising an approximately 99:1 ratio of lauryl methacrylate and 2,2,2-trifluoroethyl methacrylate. Yellow particle Y1 is C.I. Pigment Yellow 180, used without coating and dispersed by attrition in the presence of Solsperse 19000, as described generally in U.S. Pat. No. 9,697,778. Yellow particle Y2 is C.I. Pigment Yellow 155 used without coating and dispersed by attrition in the presence of Solsperse 19000, as described generally in in U.S. Pat. No. 9,697,778. Yellow particle Y3 is C.I. Pigment Yellow 139, used without coating and dispersed by attrition in the presence of Solsperse 19000, as described generally in in U.S. Pat. No. 9,697,778. Yellow particle Y4 is C.I. Pigment Yellow 139, which is coated by dispersion polymerization, incorporating trifluoroethyl methacrylate, methyl methacrylate and dimethylsiloxane-containing monomers as described in Example 4 of U.S. Pat. No. 9,921,451. Magenta particle M1 is a positively-charged magenta material (dimethylquinacridone, C.I. Pigment Red 122) coated using vinylbenzyl chloride and LMA as described in U.S. Pat. No. 9,697,778 and in Example 5 of U.S. Pat. No. 9,921,451.
Magenta particle M2 is a C.I. Pigment Red 122 which is coated by dispersion polymerization, methyl methacrylate and dimethylsiloxane-containing monomers as described in Example 6 of U.S. Pat. No. 9,921,451. Cyan particle C1 is a copper phthalocyanine material (C.I. Pigment Blue 15:3) that is coated by dispersion polymerization, incorporating methyl methacrylate and dimethylsiloxane-containing monomers as described in Example 7 of U.S. Pat. No. 9,921,451. In some embodiments, it has been found that the color gamut is improved by using Ink Jet Yellow 4GC (Clariant) as the core yellow pigment, with incorporation of methyl methacrylate surface polymers. The zeta potential of this yellow pigment can be tuned with the addition of 2,2,2-trifluoroehtyl methacrylate (TFEM) monomers and monomethacrylate terminated poly (dimethylsiloxane). Black particles may be formed from CI pigment black 26 or 28 or the like (e.g., manganese ferrite black spinel or copper chromite black spinel) or carbon black.
The charge polarity of any of the above particles, as well as the charge magnitude, can be engineered using a variety of surface treatments. Additionally, the surface treatment may improve compatibility of the core particles to the monomer in a reaction medium, or chemical bonding with the monomer, in forming the shell of the composite color particles. As an example, the surface treatment may be carried out with an organic silane having functional groups, such as acrylate, vinyl, —NH2, —NCO—, —OH or the like. These functional groups may undergo chemical reaction with the monomers. The color core particles may also be surface treated with an inorganic material, such as silica, aluminum oxide, zinc oxide or the like or a combination thereof. Sodium silicate or tetraethoxysilane may be used as a common precursor for silica coating. In case of an inorganic treatment, the structure of the coating may be porous to reduce density. To increase the negative charge on a particle, a variety of fluorinated acrylates or fluorinated methacrylates (especially 2,2,2-trifluoroethyl methacrylate, hereinafter abbreviated as “TFEM”) may be incorporated into the polymer shell, or incorporated during the production of, e.g., a composite organic pigment particle. Other fluorinated monomers (namely 2,2,3,4,4,4-hexafluorobutyl acrylate and 3,3,4,4,5,5,6,6,7,7,8,8,8-tridecafluorooctyl acrylate) may also be used to adjust the zeta potential of the particles.
Electrophoretic media additives and surface treatments for facilitating differential electrophoretic mobility, as well as proposed mechanisms for interaction between the surface treatment and surrounding charge control agents and/or free polymers, are discussed in detail in U.S. Pat. No. 9,697,778, incorporated by reference in its entirety. In such electrophoretic media, one way of controlling the interactions among the various types of particles is by controlling the kind, amount, and thickness of polymeric coatings on the particles. For example, to control the particle characteristics such that the particle-particle interactions are less between the second type of particles and the third and fourth types of particles than between, e.g.,, the third type of particles and the fourth type of particles of the third species, the second type of particle may bear a polymeric surface treatment, while the third and fourth types of particles bear either no polymeric surface treatment or a polymeric surface treatment having a lower mass coverage per unit area of the particle surface than the second type of particles. More generally, the Hamaker constant (which is a measure of the strength of the Van der Waals interaction between two particles, the pair potential being proportional to the Hamaker constant and inversely proportional to the sixth power of the distance between the two particles) and/or the interparticle spacing need(s) to be adjusted by judicious choice of the polymeric coating(s) on the three species of particles.
As discussed in U.S. Pat. No. 9,921,451, different types of polymers may include different types of polymer surface treatment. For example, Coulombic interactions may be weakened when the closest distance of approach of oppositely-charged particles is maximized by a steric barrier (typically a polymer grafted or adsorbed to the surface of one or both particles). The polymer shell may be a covalently-bonded polymer made by grafting processes or chemisorption as is well known in the art, or may be physisorbed onto the particle surface. For example, the polymer may be a block copolymer comprising insoluble and soluble segments. Alternatively, the polymer shell may be dynamic in that it is a loose network of free polymer from the electrophoretic medium that is complexed with a pigment particle in the presence of an electric field and a sufficient amount and kind of charge control agent (CCA-discussed below). Thus, depending upon the strength and polarity of the electric field, a particle may have more associated polymer, which causes the particle to interact differently with the container (e.g., microcapsule or microcell) and the other particles. [The extent of the polymer shell is conveniently assessed by thermal gravimetric analysis (TGA), a technique in which the temperature of a dried sample of the particles is raised and the mass loss due to pyrolysis is measured as a function of temperature. Using TGA, the proportion of the mass of the particle that is polymer can be measured, and this can be converted to a volume fraction using the known densities of the core pigments and the polymers attached to them.] Conditions can be found in which the polymer coating is lost but the core pigment remains (these conditions depend upon the precise core pigment particle used). A variety of polymer combinations can be made to work as described below with respect to
The fluid 17, in which the four types of particles are dispersed, is clear and colorless. The fluid contains the charged electrophoretic particles, which move through the fluid under the influence of an electric field. A preferred suspending fluid has a low dielectric constant (about 2), high volume resistivity (about 1015 Ohm·cm), low viscosity (less than 5 mPas), low toxicity and environmental impact, low water solubility (less than 10 parts per million (ppm), if traditional aqueous methods of encapsulation are to be used; note however that this requirement may be relaxed for non-encapsulated or certain microcell displays), a high boiling point (greater than about 90° C.), and a low refractive index (less than 1.5). The last requirement arises from the use of scattering (typically white) pigments of high refractive index, whose scattering efficiency depends upon a mismatch in refractive index between the particles and the fluid.
Organic solvents such as saturated linear or branched hydrocarbons, silicone oils, halogenated organic solvents, and low molecular weight halogen-containing polymers are some useful fluids. The fluid may comprise a single component or may be a blend of more than one component in order to tune its chemical and physical properties. Reactants or solvents for the microencapsulation process (if used), such as oil soluble monomers, can also be contained in the fluid.
The fluid preferably has a low viscosity and a dielectric constant in the range of about 2 to about 30, preferably about 2 to about 15 for high particle mobility. Examples of suitable dielectric fluids include hydrocarbons such as Isopar®, decahydronaphthalene (DECALIN), 5-ethylidene-2-norbornene, fatty oils, paraffin oil, silicon fluids, aromatic hydrocarbons such as toluene, xylene, phenylxylylethane, dodecylbenzene or alkylnaphthalene, halogenated solvents such as perfluorodecalin, perfluorotoluene, perfluoroxylene, dichlorobenzotrifluoride, 3,4,5-trichlorobenzotri fluoride, chloropentafluoro-benzene, dichlorononane or pentachlorobenzene, and perfluorinated solvents such as FC-43, FC-70 or FC-5060 from 3M Company, St. Paul MN, low molecular weight halogen containing polymers such as poly (perfluoropropylene oxide) from TCI America, Portland, Oregon, poly (chlorotrifluoro-ethylene) such as Halocarbon Oils from Halocarbon Product Corp., River Edge, NJ, perfluoropolyalkylether such as Galden from Ausimont or Krytox Oils and Greases K-Fluid Series from DuPont, Delaware, polydimethylsiloxane based silicone oil from Dow-corning (DC-200).
The electrophoretic media typically also include one or more charge control agents (CCA), and may also include a charge director. CCA and charge directors typically comprise low molecular weight surfactants, polymeric agents, or blends of one or more components and serve to stabilize or otherwise modify the sign and/or magnitude of the charge on the electrophoretic particles. The CCA is typically a molecule comprising ionic or other polar groupings, hereinafter referred to as head groups. At least one of the positive or negative ionic head groups is preferably attached to a non-polar chain (typically a hydrocarbon chain) that is hereinafter referred to as a tail group. It is thought that the CCA forms reverse micelles in the internal phase and that it is a small population of charged reverse micelles that leads to electrical conductivity in the very non-polar fluids typically used as electrophoretic fluids.
The addition of CCAs provides for the production of reverse micelles including a highly polar core that may vary in size from 1 nm to tens of nanometers (and may have spherical, cylindrical, or other geometry) surrounded by the non-polar tail groups of the CCA molecule. In electrophoretic media, three phases may typically be distinguished: a solid particle having a surface, a highly polar phase that is distributed in the form of extremely small droplets (reverse micelles), and a continuous phase that comprises the fluid. Both the charged particles and the charged reverse micelles may move through the fluid upon application of an electric field, and thus there are two parallel pathways for electrical conduction through the fluid (which typically has a vanishingly small electrical conductivity itself).
The polar core of the CCA is thought to affect the charge on surfaces by adsorption onto the surfaces. In an electrophoretic display, such adsorption may be onto the surfaces of the electrophoretic particles or the interior walls of a microcapsule (or other solid phase, such as the walls of a microcell) to form structures similar to reverse micelles, these structures hereinafter being referred to as hemi-micelles. When one ion of an ion pair is attached more strongly to the surface than the other (e.g., by covalent bonding), ion exchange between hemi-micelles and unbound reverse micelles can lead to charge separation in which the more strongly bound ion remains associated with the particle and the less strongly bound ion becomes incorporated into the core of a free reverse micelle.
It is also possible that the ionic materials forming the head group of the CCA may induce ion-pair formation at the particle (or other) surface. Thus the CCA may perform two basic functions: charge-generation at the surface and charge-separation from the surface. The charge-generation may result from an acid-base or an ion-exchange reaction between some moiety present in the CCA molecule or otherwise incorporated into the reverse micelle core or fluid, and the particle surface. Thus, useful CCA materials are those which are capable of participating in such a reaction, or any other charging reaction as known in the art.
Non-limiting classes of charge control agents that are useful in the media of the present invention include organic sulfates or sulfonates, metal soaps, block or comb copolymers, organic amides, organic zwitterions, and organic phosphates and phosphonates. Useful organic sulfates and sulfonates include, but are not limited to, sodium bis (2-ethylhexyl) sulfosuccinate, calcium dodecylbenzenesulfonate, calcium petroleum sulfonate, neutral or basic barium dinonylnaphthalene sulfonate, neutral or basic calcium dinonylnaphthalene sulfonate, dodecylbenzenesulfonic acid sodium salt, and ammonium lauryl sulfate. Useful metal soaps include, but are not limited to, basic or neutral barium petronate, calcium petronate, cobalt, calcium, copper, manganese, magnesium, nickel, zinc, aluminum and iron salts of carboxylic acids such as naphthenic, octanoic, oleic, palmitic, stearic, and myristic acids and the like. Useful block or comb copolymers include, but are not limited to, AB diblock copolymers of (A) polymers of 2-(N,N-dimethylamino) ethyl methacrylate quaternized with methyl p-toluenesulfonate and (B) poly (2-ethylhexyl methacrylate), and comb graft copolymers with oil soluble tails of poly (12-hydroxystearic acid) and having a molecular weight of about 1800, pendant on an oil-soluble anchor group of poly (methyl methacrylate-methacrylic acid). Useful organic amides/amines include, but are not limited to, polyisobutylene succinimides such as OLOA 371 or 1200 (available from Chevron Oronite Company LLC, Houston, Tex.), or SOLSPERSE 17000 or 19000 (available from Lubrizol, Wickliffe, OH: Solsperse is a Registered Trade Mark), and N-vinylpyrrolidone polymers. Useful organic zwitterions include, but are not limited to, lecithin. Useful organic phosphates and phosphonates include, but are not limited to, the sodium salts of phosphated mono- and di-glycerides with saturated and unsaturated acid substituents. Useful tail groups for CCA include polymers of olefins such as poly (isobutylene) of molecular weight in the range of 200-10,000. The head groups may be sulfonic, phosphoric or carboxylic acids or amides, or alternatively amino groups such as primary, secondary, tertiary or quaternary ammonium groups. One class of CCAs that are useful in the disclosed four-particle electrophoretic media are disclosed in U.S. Patent Publication No. 2017/0097556, incorporated by reference herein in its entirety. Such CCAs typically include a quaternary amine head group and an unsaturated polymeric tail, i.e., including at least one C—C double bond. The polymeric tail is typically a fatty acid tail. A variety of CCA molecular weights can be used. In some embodiments, the molecular weight of the CCA is 12,000 grams/mole or greater, e.g., between 14,000 grams/mole and 22,000 grams/mole.
Charge adjuvants used in the media of the present invention may bias the charge on electrophoretic particle surfaces, as described in more detail below. Such charge adjuvants may be Bronsted or Lewis acids or bases. Exemplary charge adjuvants are disclosed in U.S. Pat. Nos. 9,765,015; 10,233,339; and 10,782,586, all of which are incorporated by reference in their entireties. Exemplary adjuvants may include polyhydroxy compounds which contain at least two hydroxyl groups include, but are not limited to, ethylene glycol, 2,4,7,9-tetramethyldecyne-4,7-diol, poly (propylene glycol), pentaethylene glycol, tripropylene glycol, triethylene glycol, glycerol, pentaerythritol, glycerol tris (12-hydroxystearate), propylene glycerol monohydroxystearate, and ethylene glycol monohydroxystearate. Examples of aminoalcohol compounds which contain at least one alcohol function and one amine function in the same molecule include, but are not limited to, triisopropanolamine, triethanolamine, ethanolamine, 3-amino-1-propanol, o-aminophenol, 5-amino-1-pentanol, and tetrakis (2-hydroxyethyl) ethylenediamine. In some embodiments, the charge adjuvant is present in the electrophoretic display medium in an amount of between about 1 to about 500 milligrams per gram (“mg/g”) of the particle mass, and more preferably between about 50 to about 200 mg/g.
Particle dispersion stabilizers may be added to prevent particle flocculation or attachment to the capsule or other walls or surfaces. For the typical high resistivity liquids used as fluids in electrophoretic displays, non-aqueous surfactants may be used. These include, but are not limited to, glycol ethers, acetylenic glycols, alkanolamides, sorbitol derivatives, alkyl amines, quaternary amines, imidazolines, dialkyl oxides, and sulfosuccinates.
As described in U.S. Pat. No. 7,170,670, the bistability of electrophoretic media can be improved by including in the fluid a polymer having a number average molecular weight in excess of about 20,000, this polymer being essentially non-absorbing on the electrophoretic particles; poly (isobutylene) is a preferred polymer for this purpose. Also, as described in, e.g., U.S. Pat. No. 6,693,620, a particle with immobilized charge on its surface sets up an electrical double layer of opposite charge in a surrounding fluid. Ionic head groups of the CCA may be ion-paired with charged groups on the electrophoretic particle surface, forming a layer of immobilized or partially immobilized charged species. Outside this layer is a diffuse layer comprising charged (reverse) micelles comprising CCA molecules in the fluid. In conventional DC electrophoresis an applied electric field exerts a force on the fixed surface charges and an opposite force on the mobile counter-charges, such that slippage occurs within the diffuse layer and the particle moves relative to the fluid. The electric potential at the slip plane is known as the zeta potential.
As a result, some of the particle types within the electrophoretic medium have different electrophoretic mobilities depending upon the strength of the electric field across the electrophoretic medium. For example, when a first (low strength, i.e., around #10V or less) electric field is applied to the electrophoretic medium, the first type of particles move in one direction relative to the electric field, however, when a second (high strength, i.e., around +20V or more) electric field is applied, having the same polarity as the first electric field, the first type of particles begins to move in the opposite direction relative to the electric field. It is theorized that the behavior results from conduction within the highly non-polar fluid being mediated by charged reverse micelles or counter-charged electrophoretic particles. Accordingly, any electrochemically-generated protons (or other ions) are probably transported through the non-polar fluid in micelle cores or adsorbed on electrophoretic particles. For example, as illustrated in FIG. 5B of U.S. Pat. No. 9,697,778, a positively-charged reverse micelle may approach a negative electrophoretic particle traveling in the opposite direction, wherein the reverse micelle is incorporated into the electric double layer around the negatively charged particle. (The electric double layer includes both the diffuse layer of charge with enhanced counter-ion concentration and the hemi-micellar surface-adsorbed coating on the particle; in the latter case, the reverse micelle charge would become associated with the particle within the slip envelope that, as noted above, defines the zeta potential of the particle.) Through this mechanism, an electrochemical current of positively-charged ions flows through the electrophoretic fluid, and the negatively-charged particles may become biased towards a more positive charge. As a result, the electrophoretic mobility, e.g., of the first negative type of particle is a function of the magnitude of the electrochemical current and the residence time of a positive charge close to the particle surface, which is a function of the strength of the electric field.
Furthermore, as also described in U.S. Pat. No. 9,697,778, positively-charged particles can be prepared that also exhibit different electrophoretic mobilities depending upon the applied electric field. In some embodiments, a secondary (or co-) CCA can be added to the electrophoretic medium to adjust the zeta potentials of the various particles. Careful selection of the co-CCA may allow alteration of the zeta potential of one particle while leaving those of the other particles essentially unchanged, allows close control of both the electrophoretic velocities of the various particles during switching and the inter-particle interactions.
In some embodiments, a portion of the charge control agents intended for the final formulation are added during synthesis of the electrophoretic particles to engineer the desired zeta potential and to influence the reduction in electrophoretic mobility due to a strong electric field. For example, it has been observed that adding quaternary amine charge control agents during polymer grafting will result in some amount of the CCA being complexed to the particles. (This can be confirmed by removing the particles from the electrophoretic fluid and subsequently stripping the surface species from the pigments with THF to remove all adsorbed species. When the THF extract is evaluated with 1H NMR, it is clear that a good amount of the CCA was adsorbed to the pigment particles or complexed with the surface polymer.) Experiments suggest that high CCA loading amongst the surface polymers of the particles facilitates the formation of a charge double layer around the particle in the presence of a strong electric field. For example, magenta particles having greater than 200 mg of a charge control agent (CCA) per gram of finished magenta particle have excellent staying properties in the presence of a high positive electric field. (See, e.g.,
In other embodiments, an electrophoretic medium including four types of particles, in the presence of Solsperse 17000 in Isopar E benefits from the additions of small amounts of acidic entities such as, e.g., aluminum salts of di-t-butyl salicylic acid (Bontron E-88, available from Orient Corporation, Kenilworth, NJ)). Addition of the acidic material moves the zeta potential of many particles (though not all) to more positive values. In one embodiment about 1% of the acidic material and 99% of Solsperse 17000 (based on total weight of the two materials) moves the zeta potential of the third type of particle (Y+) from −5 mV to about +20 mV. Whether or not the zeta potential of a particular particle is changed by a Lewis acidic material like the aluminum salt will depend upon the details of the surface chemistry of the particle.
Table 2 shows exemplary relative zeta potentials of the three types of colored and singular white particles.
The negative (white) particle may have a zeta potential of −30 mV, and the remaining three particles are all positive relative to the white particle. Accordingly, a display comprising positive cyan, magenta, and yellow particles can switch between a black state (with all colored particles in front of the white particle with respect to the viewing surface) and a white state, with the white particle closest to the viewer, and blocking the viewer from perceiving the remaining three particles. In contrast, when the white particle has a zeta potential of 0 V, the negatively-charged yellow particle is the most negative of all the particles, and thus a display comprising this particle would switch between a yellow and a blue state. This would also occur if the white particle were positively charged. The positively-charged yellow particle, however, would be more positive than the white particle unless its zeta potential exceeded +20 m V.
The behavior of the electrophoretic media of the invention are consistent with the mobility of the white particle (represented in Table 2 as the zeta potential) being dependent upon the applied electric field. Thus, in the example illustrated in Table 2, when addressed with a low voltage, the white particle might behave as though its zeta potential were −30 mV, but when addressed with a higher voltage it might behave as though its zeta potential were more positive, maybe even as high as +20 mV (matching the zeta potential of the yellow particle). Thus, when addressed with a low voltage, the display would switch between black and white states but when addressed at a higher voltage would switch between blue and yellow states.
The motion of the various particles in the presence of a high (e.g., “±H”, e.g., ±20V, e.g., ±25V) electric field and a low (e.g., “±L”, e.g., ±5V, e.g., ±10V) electric field are shown in
When addressed with a low voltage, as in
In
In
Finally,
To obtain a high-resolution display, individual pixels of a display should be addressable without interference from adjacent pixels. One way to achieve this objective is to provide an array of non-linear elements, such as transistors or diodes, with at least one non-linear element associated with each pixel, to produce an “active matrix” display. An addressing or pixel electrode, which addresses one pixel, is connected to an appropriate voltage source through the associated non-linear element. Typically, when the non-linear element is a transistor, the pixel electrode is connected to the drain of the transistor, and this arrangement will be assumed in the following description, although it is essentially arbitrary and the pixel electrode could be connected to the source of the transistor. Conventionally, in high resolution arrays, the pixels are arranged in a two-dimensional array of rows and columns, such that any specific pixel is uniquely defined by the intersection of one specified row and one specified column. The sources of all the transistors in each column are connected to a single column electrode, while the gates of all the transistors in each row are connected to a single row electrode; again the assignment of sources to rows and gates to columns is conventional but essentially arbitrary, and could be reversed if desired. The row electrodes are connected to a row driver, which essentially ensures that at any given moment only one row is selected, i.e., that there is applied to the selected row electrode a select voltage such as to ensure that all the transistors in the selected row are conductive, while there is applied to all other rows a non-select voltage such as to ensure that all the transistors in these non-selected rows remain non-conductive. The column electrodes are connected to column drivers, which place upon the various column electrodes voltages selected to drive the pixels in the selected row to their desired optical states. (The aforementioned voltages are relative to a common front electrode which is conventionally provided on the opposed side of the electro-optic medium from the non-linear array and extends across the whole display.) After a pre-selected interval known as the “line address time” the selected row is deselected, the next row is selected, and the voltages on the column drivers are changed so that the next line of the display is written. This process is repeated so that the entire display is written in a row-by-row manner.
Conventionally, each pixel electrode has associated therewith a capacitor electrode such that the pixel electrode and the capacitor electrode form a capacitor; see, e.g., International Patent Application WO 01/07961. In some embodiments, N-type semiconductor (e.g., amorphous silicon) may be used to from the transistors and the “select” and “non-select” voltages applied to the gate electrodes can be positive and negative, respectively.
Problems may arise, however, when Vcom is set to a voltage that is not compensated for the kickback voltage. This may occur when it is desired to apply a higher voltage to the display than is available from the backplane alone. It is well known in the art that, e.g., the maximum voltage applied to the display may be doubled if the backplane is supplied with a choice of a nominal +V, 0, or −V, e.g., while Vcom is supplied with −V. The maximum voltage experienced in this case is +2V (i.e., at the backplane relative to the top plane), while the minimum is zero. If negative voltages are needed, the Vcom potential must be raised at least to zero. Waveforms used to address a display with positive and negative voltages using top plane switching must therefore have particular frames allocated to each of more than one Vcom voltage setting.
A set of waveforms for driving a color electrophoretic display having four particles described in U.S. Pat. No. 9,921,451, incorporated by reference herein. In U.S. Pat. No. 9,921,451, seven different voltages are applied to the pixel electrodes: three positive, three negative, and zero. However, in some embodiments, the maximum voltages used in these waveforms are higher than that can be handled by amorphous silicon thin-film transistors. In such instances, suitable high voltages can be obtained by the use of top plane switching. When (as described above) Vcom is deliberately set to VKB, a separate power supply may be used. It is costly and inconvenient, however, to use as many separate power supplies as there are Vcom settings when top plane switching is used. Furthermore, top plane switching is known to increase kickback, thereby degrading the stability of the color states.
A display device may be constructed using an electrophoretic fluid of the invention in several ways that are known in the prior art. The electrophoretic fluid may be encapsulated in microcapsules or incorporated into microcell structures that are thereafter sealed with a polymeric layer. The microcapsule or microcell layers may be coated or embossed onto a plastic substrate or film bearing a transparent coating of an electrically conductive material. This assembly may be laminated to a backplane bearing pixel electrodes using an electrically conductive adhesive. Alternatively, the electrophoretic fluid may be dispensed directly on a thin open-cell grid that has been arranged on a backplane including an active matrix of pixel electrodes. The filled grid can then be top-sealed with an integrated protective sheet/light-transmissive electrode.
Most commercial electrophoretic displays use amorphous silicon based thin-film transistors (TFTs) in the construction of active matrix backplanes (202/024) because of the wider availability of fabrication facilities and the costs of the various starting materials. Unfortunately, amorphous silicon thin-film transistors become unstable when supplied gate voltages that would allow switching of voltages higher than about +/−15V. Nonetheless, as described below, the performance of ACeP is improved when the magnitudes of the high positive and negative voltages are allowed to exceed +/−15V. Accordingly, as described in previous disclosures, improved performance is achieved by additionally changing the bias of the top light-transmissive electrode with respect to the bias on the backplane pixel electrodes, also known as top-plane switching. Thus, if a voltage of +30V (relative to the backplane) is needed, the top plane may be switched to −15V while the appropriate backplane pixel is switched to +15V. Methods for driving a four-particle electrophoretic system with top-plane switching are described in greater detail in, e.g., U.S. Pat. No. 9,921,451.
These waveforms require that each pixel of the display can be driven at five different addressing voltages, designated +Vhigh, +Vlow, 0, −Vlow and −Vhigh, illustrated as 30V, 15V, 0, −15V and −30V. In practice, it may be preferred to use a larger number of addressing voltages. If only three voltages are available (i.e., +Vhigh, 0, and −Vhigh), it may be possible to achieve the same result as addressing at a lower voltage (say, Vhigh/n where n is a positive integer>1) by addressing with pulses of voltage Vhigh, but with a duty cycle of 1/n.
Although
Of course, achieving the desired color with the driving pulses of
In addition, the foregoing discussion of the waveforms, and specifically the discussion of DC balance, ignores the question of kickback voltage. In practice, as previously, every backplane voltage is offset from the voltage supplied by the power supply by an amounts equal to the kickback voltage VKB. Thus, if the power supply used provides the three voltages +V, 0, and −V, the backplane would actually receive voltages V+VKB, VKB, and −V+VKB (note that VKB, in the case of amorphous silicon TFTs, is usually a negative number). The same power supply would, however, supply+V, 0, and −V to the front electrode without any kickback voltage offset. Therefore, e.g., when the front electrode is supplied with −V the display would experience a maximum voltage of 2V+VKB and a minimum of VKB. Instead of using a separate power supply to supply VKB to the front electrode, which can be costly and inconvenient, a waveform may be divided into sections where the front electrode is supplied with a positive voltage, a negative voltage, and VKB.
A five-particle electrophoretic medium according to one aspect of the invention can provide a plurality of colored optical states at each pixel, including an improved black optical state. The five-particle electrophoretic medium is similar to the four-particle electrophoretic media disclosed above with the further addition of black particles.
The five-particle electrophoretic medium includes a first white particle of a first polarity and four other particles (including the black particle) having the opposite polarity with different magnitudes of charge. Preferably, the medium includes a negatively-charged white particle and positively-charged yellow, magenta, cyan, and black particles comprising subtractive primary colors. Additionally, as described above, some particles may be engineered as previously discussed so that their electrophoretic mobility is non-linear with respect to the strength of the applied electric field. Thus, one or more particles can experience a decrease in electrophoretic mobility with the application of a high electric field (e.g., 20V or greater) of the correct polarity. Such a five-particle system is shown schematically in
As shown in
The white, yellow, cyan, and magenta particles in the five-particle system in accordance with various embodiments are the same as or similar to the respective particles in the four particle media described above with respect to charge polarity, zeta potential, surface treatment, and behavior in the presence of different electric fields.
For instance, the white particles (W−*) in the five-particle electrophoretic medium are negatively charged and may be surface treated so that the electrophoretic mobility of the particles is dependent upon the strength of the driving electric field. In such instances, the electrophoretic mobility of the white particles actually decreases in the presence of a stronger electric field, which is somewhat counter-intuitive.
The magenta particles (M++*) are positively charged, and may also be surface treated (or purposely untreated) so that either the electrophoretic mobility of the magenta particles is dependent upon the strength of the driving electric field, or the rate of unpacking of a collection of the magenta particles, after having been driven to one side of the cavity containing the particles upon reversal of the electric field direction, is slower than the rate of unpacking of collections of the yellow and cyan particles.
The yellow particles (Y+) are positive, but has a charge magnitude that is smaller than the magenta particle. Additionally, the yellow particles may be surface treated, but not in a way that causes the electrophoretic mobility of the yellow particles to depend upon the strength of the driving electric field. That is, the yellow particles may have a surface treatment, however such a surface treatment does not result in the aforementioned reduction in electrophoretic mobility with an increased electric field.
The cyan particles (C+++) have a higher magnitude positive charge than the magenta particles and the same type of surface treatment as the yellow particles.
The black particles (K++++) have the highest magnitude positive charge. The black particles have a relatively low concentration in the electrophoretic medium. For example, the black particles can comprise 0.5-2% by weight of the entire internal phase, including the solvent, dispersed polymer, CCA, and other pigment particles. Also, the ratio of black to magenta particles by number of particles (black: magenta) is typically between 1:10 and 1:5, e.g., 1:7.
While the particles disclosed herein are nominally white, magenta, yellow, black, and cyan in color to produce colors as shown in
The electrophoretic medium of the five-particle system may be in any of the forms discussed above. Thus, the electrophoretic medium may be unencapsulated, encapsulated in discrete capsules surrounded by capsule walls, encapsulated in sealed microcells, or in the form of a polymer-dispersed medium.
Table 3 below shows exemplary zeta potentials for the particles of a five-particle electrophoretic medium in one or more embodiments.
Starting from a first state, in which all of the positive particles are present at the viewing surface (nominally black), the electrophoretic medium can be driven to a plurality of different optical states, including the four optical states shown in
When addressed with a low voltage, as in
In
In
Finally,
Thus, as summarized in
The presence of the black particles in the black optical state provides an improved, more saturated black optical state at the viewing surface. It may also shift the chroma of the process black so that a viewer perceives a “more pure” black. This is especially important when using “dark mode” to read white text on a black background.
The presence of the black particles in the red, magenta, and yellow optical states has the effect of reducing the lightness of the color being rendered. This effect, however, is limited due to the low concentration of black particles relative to the other colored particles in the electrophoretic medium. Further, reduction in the lightness of the colors being rendered can be mitigated by changing the intensity or spectrum of the lighting used for the front light of the display device to illuminate the viewing surface.
Having thus described several aspects and embodiments of the technology of this application, it is to be appreciated that various alterations, modifications, and improvements will readily occur to those of ordinary skill in the art. Such alterations, modifications, and improvements are intended to be within the spirit and scope of the technology described in the application. For example, those of ordinary skill in the art will readily envision a variety of other means and/or structures for performing the function and/or obtaining the results and/or one or more of the advantages described herein, and each of such variations and/or modifications is deemed to be within the scope of the embodiments described herein. Those skilled in the art will recognize, or be able to ascertain using no more than routine experimentation, many equivalents to the specific embodiments described herein. It is, therefore, to be understood that the foregoing embodiments are presented by way of example only and that, within the scope of the appended claims and equivalents thereto, inventive embodiments may be practiced otherwise than as specifically described. In addition, any combination of two or more features, systems, articles, materials, kits, and/or methods described herein, if such features, systems, articles, materials, kits, and/or methods are not mutually inconsistent, is included within the scope of the present disclosure.
This application is a continuation-in-part of U.S. patent application Ser. No. 18/140,161 filed Apr. 27, 2023, which is a continuation of U.S. patent application Ser. No. 17/474,582 filed Sep. 14, 2021, which claims priority to U.S. Provisional Patent Application No. 63/078,829 filed Sep. 15, 2020 and U.S. Provisional Patent Application No. 63/191,075 filed May 20, 2021. This application also claims priority to U.S. Provisional Patent Application No. 63/613,889 filed Dec. 22, 2023. Each of the applications identified above are incorporated by reference in their entireties. All patents and publications disclosed herein are also incorporated by reference in their entireties.
| Number | Date | Country | |
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| 63191075 | May 2021 | US | |
| 63078829 | Sep 2020 | US | |
| 63613889 | Dec 2023 | US |
| Number | Date | Country | |
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| Parent | 17474582 | Sep 2021 | US |
| Child | 18140161 | US |
| Number | Date | Country | |
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| Parent | 18140161 | Apr 2023 | US |
| Child | 18744857 | US |
