Electrophoretic display having dielectric coating on electrode

Abstract

To provide a favorable electrophoretic display having a dielectric coating on an electrode.SOLUTION: An electrophoretic display (100) comprises an electrophoretic medium (114) having electrically charged particles, which are disposed in a fluid and movable through the fluid on application of an electric field. An electrode (104, 120) is disposed adjacent to the electrophoretic medium and arranged to apply an electric field thereto. A dielectric layer (106, 118) is disposed between the electrophoretic medium (114) and the electrode (104, 120), and has at least one aperture (107, 119) extending therethrough. The provision of the apertures (107, 119) in the dielectric layers enables the dielectric layers (106, 118) to protect the electrodes (104, 120) while reducing electro-optical kickback. When multiple electrodes (104, 120) are present adjacent to the electrophoretic medium (114), more than one or all of the electrodes (104, 120) may be provided with apertured dielectric layers (106, 118).SELECTED DRAWING: Figure 1

Description

[Background technology]

[0001] This application is related to U.S. Patent Nos. 9,726,957 and 10,520,786 and published application No. 2020 / 0117069 A1.

[0002] The entire contents of the aforementioned provisional applications, patents, and published applications, as well as all other US patents and published and co-pending applications mentioned below, are hereby incorporated by reference.

[0003] BACKGROUND OF THEINVENTION

[0004] The present invention relates to electrophoretic displays in which at least one electrode carries a dielectric coating, more particularly, the present invention relates to such electrophoretic displays in which the dielectric coating has at least one aperture therethrough.

[0005] A particle-based electrophoretic display has an electrophoretic medium comprising a plurality of charged particles, which 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 to liquid crystal displays. Typically, an electrophoretic display comprises a layer of electrophoretic material and at least two other layers disposed on either side of the electrophoretic material, one of these two layers being an electrode layer. In most such displays, both layers are electrode layers, and one or both of the electrode layers are patterned to define the pixels of the display. For example, one electrode layer may be patterned into elongated row electrodes and the other into elongated column electrodes extending at right angles to the row electrodes, with the pixels being defined by the intersections of the row and column electrodes. Alternatively, and more commonly, one electrode layer has the form of a single continuous electrode, and the other electrode layer is patterned into a matrix of pixel electrodes, each of which defines one pixel of the display. In another type of electrophoretic display, where the display is intended for use with a separate stylus, printhead, or similar movable electrode, only one of the layers adjacent to the electrophoretic layer comprises an electrode; the layer on the opposite side of the electrophoretic layer is typically a protective layer intended to prevent the movable electrode from damaging the electrophoretic layer.

[0006] In electrophoretic displays having an electrophoretic medium sandwiched between two electrode layers, at least one of the electrode layers must be light-transmitting, and preferably substantially transparent, to allow changes in the optical state of the medium to be visible to an observer viewing the display through the light-transmitting electrode layer. When one electrode layer is a single continuous electrode and the other is patterned to form pixel electrodes, one electrode layer is usually a continuous electrode that forms the viewing surface through which the display is viewed, since a single continuous electrode layer is less likely to produce visual artifacts than a patterned electrode layer. The number of materials possessing the required combination of electrical conductivity and light transparency to form such electrodes is limited, and most commercially available electrophoretic displays use light-transmitting electrode layers formed from sputtered metal oxides such as indium oxide or indium tin oxide, although electrode layers formed from conductive polymers are also used. To ensure adequate transparency, sputtered metal oxide electrode layers are typically less than 1 nm thick.

[0007] It has been known for some time that electrode layers in electrophoretic displays are subject to both mechanical and electrochemical damage. See, for example, U.S. Pat. No. 6,724,519, which describes an electrophoretic display with a protective layer adapted to prevent mechanical or electrochemical damage to the electrodes. The protective layer may include a metal or metal oxide. See also U.S. Pat. No. 8,441,432, which describes a microcell electrophoretic display in which at least one electrode has an electrode protective layer formed from a composition comprising a polar oligomeric or polymeric material containing at least one polar group selected from the group consisting of nitro, hydroxyl, alkoxy, halo, cyano, sulfonate, amino-containing or amino-derived polar groups, carbohydrate groups, phosphorus-containing polar groups, sulfur-containing polar groups, and negative ions, and the display cell or electrode protective layer is about 10 7 ~about 10 12It has a resistivity in the ohm-cm range. U.S. Pat. No. 9,244,325 describes a microcell electrophoretic display having a partition structure dividing the display layer into multiple regions and an electrode protection layer formed integrally with the partition structure, both of which consist of a conductive polymer, primarily a UV-curable polymer with ethylene oxide side chains. U.S. Pat. No. 3,792,308 describes an electrophoretic display in which one or both electrodes are coated with an insulating layer prepared, for example, by coating the electrodes with vinyl acetate resin, polystyrene, or gelatin. Finally, U.S. Pat. No. 6,850,357 describes an electrophoretic display having an electrode protection layer formed from an acrylic photosensitive resin, a non-photosensitive resin, and an inorganic insulating layer.

[0008] While it is relatively easy to design protective layers to protect electrodes in electrophoretic displays against mechanical damage, it is more complicated to protect against electrochemical damage. As already mentioned, electrophoretic displays are typically bistable. (The terms "bistable" and "bistable" are used herein in their conventional sense in the art to refer to displays comprising display elements having first and second display states differing in at least one optical property, such that any given element is driven with an address pulse of finite duration to exhibit either the first or second display state, and will remain in that state after the address pulse is terminated for at least several times, e.g., at least four times, the minimum duration of the address pulse required to change the state of the display element.) In U.S. Pat. No. 7,170,670, it is shown 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. It has been shown that displays of this type are properly termed "multistable" rather than bistable, although for convenience the term "bistable" may be used herein to include both bistable and multistable displays. Indeed, such bistability is an important factor in reducing power consumption in portable battery-powered electrophoretic displays, since the display may be driven for perhaps 0.5 seconds to display a first image (e.g., the first page of a book), left undriven for perhaps 30 seconds while the user reads or examines the first image, driven for perhaps 0.5 seconds to display a second image, and so on, so that the display is only driven for a small percentage of the time that the user is using the display.It has long been known that drive schemes used to drive electrophoretic displays should be DC balanced, in the sense that if a particular pixel of the display goes through a series of transitions starting from an initial grey level, reaching other grey levels, but ending up back at the initial grey level, the overall impulse of the series of transitions (the integral of the drive voltage over time) should be substantially zero. If this is not the case, after extended use the display is likely to exhibit permanent electrochemical changes in the electrode layers, and these changes may damage or even destroy the electro-optical performance of the display.

[0009] However, even if the overall driving scheme is DC-balanced, problems can still arise if the waveforms used for the individual transitions are not themselves DC-balanced. Often, electrophoretic displays exhibit a "residual voltage" after driving. This residual voltage, measured as the open circuit voltage across the electrodes of the display, is believed to be due to the accumulation of charge in the various layers of the electrophoretic display and can persist for very long periods after driving of the display has been terminated. The residual voltage can lead to undesirable changes in the optical state of the display during periods when the display is not driven and is intended to remain in the same optical state. Even small residual voltages can cause problems, as most electrophoretic media have little or no threshold voltage, and therefore the presence of even small residual voltages over an extended period between two successive transitions can cause large changes in the optical state of the medium. Such undesirable changes in optical state are particularly difficult to address in full-color displays, since the human eye tends to be more sensitive to slight changes in hue than to minute variations in gray level in monochrome displays; color variations, particularly in flesh tones, are very noticeable, especially when greenish hues occur. Although methods for reducing or eliminating remnant voltages are known (see, for example, U.S. Pat. No. 10,475,396), it is desirable to prevent large remnant voltages from occurring during the operation of electrophoretic displays.

[0010] To prevent the accumulation of residual voltages, electrophoretic displays can be driven using a drive scheme in which each waveform is itself DC balanced, i.e., each waveform and the overall drive scheme is DC balanced. However, having all waveforms DC balanced introduces additional complications, especially for full-color displays. Typically, a DC balanced waveform comprises a DC balance section followed by a drive section, where the DC balance section is arranged to have a net impulse equal in magnitude to that of the drive section but opposite in polarity, so that the net impulse of the overall waveform is essentially zero. For example, referring to U.S. Pat. No. 10,276,109, FIG. 11 shows this type of waveform being used in a four-particle (white, yellow, cyan, and magenta) full-color display. However, not only does the DC balanced section introduce a substantial increase in the duration of the waveform (and therefore the time required for transitions), the DC balanced section also tends to increase the duration of the drive (color rendering) section. Because the DC balance section must have a net impulse of opposite polarity to the drive section, the DC balance section inherently tends to drive the electrophoretic particles in a direction opposite to the direction they would have been driven in during the drive section, and in practice, at the end of the DC balance section, the electrophoretic particles are positioned nearly opposite their desired relative positions. As a result, the drive or color rendering section may need to be long (on the order of a few seconds) to overcome the particle displacements caused by the DC balance section.

[0011] U.S. Patent Publication No. 2022 / 0084473 A1 describes DC unbalanced waveforms for driving four-particle full-color electrophoretic displays, and these waveforms are much shorter than the DC balanced waveforms described in the aforementioned U.S. Patent No. 10,276,109. However, without mitigation of remnant voltage build-up and electrode degradation, such waveforms could not be used in commercial displays with acceptable lifetimes.

[0012] As mentioned above, it is known to protect one or both electrodes of an electrophoretic display by providing a protective (typically dielectric) layer over the electrodes. However, such a dielectric layer introduces a capacitor in series with the electrophoretic medium between the two electrodes of the display. The capacitor becomes charged when the electrophoretic display is driven and the two electrodes are set to the same potential at the end of the waveform (to reduce the electric field across the electrophoretic medium to zero, thus leaving the electrophoretic medium in a desired optical state), and discharging this capacitor can cause sufficient current to flow through the electrophoretic medium, causing a significant and undesirable change in its optical state (a phenomenon known as "electro-optical kickback"). The present invention seeks to reduce or eliminate the problem of kickback while providing the benefits of such a dielectric layer. [Prior art documents] [Patent documents]

[0013] [Patent Document 1] U.S. Patent No. 6,724,519 [Patent Document 2] U.S. Pat. No. 8,441,432 [Patent Document 3] U.S. Patent No. 9,244,325 Summary of the Invention [Means for solving the problem]

[0014] (Summary of the invention)

[0015] The invention therefore provides an electrophoretic display comprising an electrophoretic medium disposed in a fluid and comprising a plurality of charged particles which are movable through the fluid to the electrophoretic medium upon application of an electric field, an electrode disposed adjacent the electrophoretic medium and arranged to apply an electric field thereto, and a dielectric layer disposed between the electrophoretic medium and the electrode, the dielectric layer having at least one opening extending therethrough.

[0016] Electrophoretic displays of the present invention may, and typically will, include a second electrode disposed on the opposite side of the electrophoretic medium from the electrode adjacent the dielectric layer. The second dielectric layer is disposed between the electrophoretic medium and the second electrode, and the second dielectric layer may have at least one aperture extending therethrough. The dielectric layer may have a thickness of at least about 10 7 The dielectric layer may have a dielectric strength of about 1000 V / M. Additionally, the dielectric layer may have a thickness in the range of about 10-100 nm, and the at least one opening may be substantially circular and have a diameter in the range of about 1-5 μm. The dielectric layer may be formed from any one or more of silicon dioxide, silicon nitride, metal oxides, or organic materials, such as any one or more of zinc oxide, tantalum oxide, hafnium oxide, perylene, or photoresist.

[0017] Electrophoretic displays of the invention may further comprise an adhesive layer disposed between the dielectric layer and the electrophoretic medium, which adhesive layer may be doped with an ionic material to reduce its electrical resistance.

[0018] Electrophoretic displays of the present invention may be encapsulated or unencapsulated, and when encapsulated, may be of any type known in the art, for example, the charged particles and fluid may be confined within a plurality of capsules or microcells, or may be present as a plurality of separate droplets surrounded by a continuous phase comprising a polymeric material.

[0019] An electrophoretic display of the invention may have a plurality of electrodes disposed adjacent the electrophoretic medium, the display may comprise a voltage control means for varying the potential of the plurality of electrodes independently of one another. The dielectric layer may comprise a plurality of apertures extending to each of the plurality of electrodes, each of the plurality of electrodes having a central region and a peripheral region, and the size and / or number of apertures per unit area may be greater in the central region than in the peripheral regions.

[0020] The invention also provides a process for producing the electrophoretic display of the invention, which includes providing an electrode, coating the electrode with a photoresist, imagewise exposing the photoresist to radiation, washing the exposed photoresist thereby forming at least one opening through the exposed photoresist, and disposing an electrophoretic medium adjacent to the exposed photoresist. In this process, the photoresist can be a cinnamate photoresist. The present specification also provides, for example, the following: (Item 1) 1. An electrophoretic display comprising: an electrophoretic medium comprising a plurality of electrically charged particles disposed in a fluid and movable through the fluid upon application of an electric field to the electrophoretic medium; an electrode disposed adjacent to the electrophoretic medium and configured to apply an electric field to the electrophoretic medium; Equipped with The electrophoretic display is characterized by a dielectric layer disposed between the electrophoretic medium and the electrodes, the dielectric layer having at least one aperture extending therethrough. (Item 2) 2. The electrophoretic display of claim 1, further comprising a second electrode disposed on an opposite side of the electrophoretic medium from the electrode adjacent to the dielectric layer. (Item 3) 3. The electrophoretic display of claim 2, further comprising a second dielectric layer disposed between the electrophoretic medium and the second electrode, the second dielectric layer having at least one opening extending through the second dielectric layer. (Item 4) The dielectric layer has a thickness of at least about 10 7 4. An electrophoretic display according to any of items 1-3, having a dielectric strength of V / M. (Item 5) 5. The electrophoretic display of any of items 1-4, wherein the dielectric layer has a thickness in the range of about 10 to 100 nm, and the at least one opening is substantially circular and has a diameter in the range of about 1 to 5 μm. (Item 6) 6. An electrophoretic display according to any one of claims 1 to 5, wherein the dielectric layer is formed from one or more of silicon dioxide, silicon nitride, a metal oxide, or an organic material. (Item 7) 7. The electrophoretic display of claim 6, wherein the dielectric layer is formed from any one or more of zinc oxide, tantalum oxide, hafnium oxide, perylene, or photoresist. (Item 8) Item 10. The electrophoretic display of item 1, further comprising an adhesive layer disposed between the dielectric layer and the electrophoretic medium. (Item 9) 9. An electrophoretic display as described in item 8, wherein the adhesive layer is doped with an ionic material to reduce its electrical resistance. (Item 10) 10. An electrophoretic display according to any one of claims 1-9, wherein the charged particles and the fluid are confined within a plurality of capsules or microcells. (Item 11) 10. An electrophoretic display according to any one of claims 1-9, wherein the electrically charged particles and the fluid are present as a plurality of separate droplets surrounded by a continuous phase comprising a polymeric material. (Item 12) 12. An electrophoretic display according to any one of items 1-11, comprising a plurality of electrodes disposed adjacent to the electrophoretic medium, the display further comprising voltage control means for varying the potentials of the plurality of electrodes independently of one another, the dielectric layer comprising a plurality of apertures extending to each of the plurality of electrodes, each of the plurality of electrodes having a central region and a peripheral region, the size and / or number of apertures per unit area being greater in the central region than in the peripheral region. (Item 13) 13. An electrophoretic display according to any one of items 1-12 in the form of a front plane laminate or an inverted front plane laminate. (Item 14) 14. A process for producing an electrophoretic display according to any one of items 1 to 13, said process comprising the steps of: Providing an electrode; coating the electrodes with a photoresist; imagewise exposing the photoresist to radiation; washing the exposed photoresist, thereby forming at least one opening through the exposed photoresist; placing the electrophoretic medium adjacent to the exposed photoresist; The process includes: (Item 15) Item 15. The process of item 14, wherein the photoresist is a cinnamic acid photoresist. [Brief description of the drawings]

[0021] BRIEF DESCRIPTION OF THE DRAWINGS

[0022] [Figure 1] FIG. 1 of the accompanying drawings is a schematic cross-section through a microcell electrophoretic display of the present invention.

[0023] [Diagram 2] FIG. 2 is a circuit diagram of a model of a prior art electrophoretic display lacking a dielectric layer.

[0024] [Diagram 3] FIG. 3 is a schematic diagram similar to that of FIG. 2, but of a model of an electrophoretic display of the present invention having a dielectric layer with a plurality of apertures.

[0025] [Figure 4] FIG. 4 is a schematic cross-section through a portion of an electrophoretic display of the invention showing a single aperture through the dielectric layer and illustrating the method used to calculate the resistance of the dielectric layer with the aperture.

[0026] [Diagram 5] FIG. 5 is a top plan view of the backplane of an electrophoretic display of the present invention, showing the distribution of apertures across each electrode.

[0027] [Figure 6] FIG. 6 is a graph showing the optical kickback of a full-color electrophoretic display of the present invention as a function of dielectric layer thickness.

[0028] [Figure 7] FIG. 7 is a graph similar to FIG. 6, but showing the optical kickback of a similar full-color electrophoretic display lacking a dielectric layer, but with an external parallel resistor and capacitor in series with the display to mimic the effect of a dielectric layer with an aperture. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0029] (Detailed Description)

[0030] As already mentioned, the present invention provides an electrophoretic display comprising an electrophoretic medium, an electrode disposed adjacent the electrophoretic medium, and a dielectric layer disposed between the electrophoretic medium and the electrode, the dielectric layer having at least one aperture extending therethrough.

[0031] The electrophoretic medium and electrodes used in the present invention can be of any of the types known in the art. Numerous patents and applications assigned to or in the name of Massachusetts Institute of Technology (MIT), E Ink Corporation, E Ink California, LLC. and affiliates describe the various techniques used for encapsulation and microcell electrophoresis and other electro-optical media. Encapsulated electrophoretic media comprises a number of 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 in a polymer adhesive to form a coherent layer positioned between two electrodes. In microcell electrophoretic displays, the charged particles and fluid are not encapsulated in microcapsules, but instead are held in a number of cavities, which are formed in a carrier medium (typically a polymer film). Techniques described in these patents and applications include: (a) electrophoretic particles, fluids, and fluid additives (see, e.g., U.S. Pat. Nos. 7,002,728 and 7,679,814); (b) capsules, binders, and encapsulation processes (see, e.g., U.S. Pat. Nos. 6,922,276 and 7,411,719); (c) microcell structures, wall materials, and methods of forming the microcells (see, e.g., U.S. Pat. Nos. 7,072,095 and 9,279,906); (d) methods of filling and sealing microcells (see, e.g., U.S. Pat. Nos. 7,144,942 and 7,715,088); (e) films and assemblies containing electro-optical materials (see, e.g., U.S. Pat. Nos. 6,982,178 and 7,839,564); (f) backplanes, adhesive layers, and other auxiliary layers, and methods used in displays (e.g., U.S. Pat. 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WO 00 / 38000, see European Patent Nos. 1,099,207 B1 and 1,145,072 B1); (g) Color formation and color control (e.g., U.S. Patent Nos. 6,017,584, 6,545,797, 6,664,944, 6,788,452, 6,864,875, 6,914,714, 6,972,893, 7,038,656, 7,038,670, 7,046,228, 7,052,571, 7,075,502, 7,167,155, 7,385,751, 7,492,505, 7,667,684, 7,684,108, 7,791,789, 7,800,813, No. 7,821,702, No. 7,839,564, No. 7,910,175, No. 7,952,790, No. 7,956,841, No. 7, No. 982,941, No. 8,040,594, No. 8,054,526, No. 8,098,418, No. 8,159,636, No. 8,213 ,076, No. 8,363,299, No. 8,422,116, No. 8,441,714, No. 8,441,716, No. 8,466,8 No. 52, No. 8,503,063, No. 8,576,470, No. 8,576,475, No. 8,593,721, No. 8,605,354 , No. 8,649,084, No. 8,670,174, No. 8,704,756, No. 8,717,664, No. 8,786,935, No. No. 8,797,634, No. 8,810,899, No. 8,830,559, No. 8,873,129, No. 8,902,153, No. 8,9 No. 02,491, No. 8,917,439, No. 8,964,282, No. 9,013,783, No. 9,116,412, No. 9,146 ,439, No. 9,164,207, No. 9,170,467, No. 9,170,468, No. 9,182,646, No. 9,195,11 No. 1, No. 9,199,441, No. 9,268,191, No. 9,285,649, No. 9,293,511, No. 9,341,916 , No. 9,360,733, No. 9,361,836, No. 9,383,623, No. 9,423,666, No. 9,436,056, No. 9 ,459,510, No. 9,513,527, No. 9,541,814, No. 9,552,780, No. 9,640,119, No. 9,6 No. 46,547, No. 9,671,668, No. 9,697,778, No. 9,726,959, No. 9,740,076, No. 9,759,No. 981, No. 9,761,181, No. 9,778,538, No. 9,779,670, No. 9,779,671, No. 9,812,073, No. 9,829,764 , No. 9,921,451, No. 9,922,603, No. 9,989,829, No. 10,032,419, No. 10,036,929, No. 10,036,931, No. No. 10,332,435, No. 10,339,876, No. 10,353,266, No. 10,366,647, No. 10,372,010, No. 10,380,931 , No. 10,380,955, No. 10,431,168, No. 10,444,592, No. 10,467,984, No. 10,475,399, No. 10,509,293 Nos. 2008 / 0043318, 2008 / 0048970, 2009 / 0225398, 2010 / 0156780, 2011 / 0043543, 2012 / 0326957, 2013 / 0242378, 2013 / 0278995, 2014 / 027911, and 2015 / 027911. 4 / 0055840, No. 2014 / 0078576, No. 2015 / 0103394, No. 2015 / 0118390, No. 2015 / 0124345, No. 2015 / 0268531, No. 2015 / 0301246, No. 2016 / 0026062, No. 2016 / 0048054, and No. 2016 / 0116818); (h) methods of driving displays (see, e.g., U.S. Pat. Nos. 7,012,600 and 7,453,445); (i) display applications (see, e.g., U.S. Pat. Nos. 7,312,784 and 8,009,348); (j) Non-display applications of encapsulation and microcell technology (see, e.g., U.S. Pat. No. 7,615,325 and U.S. Patent Application Publication Nos. 2015 / 0005720 and 2016 / 0012710).

[0032] Many of the aforementioned patents and applications recognize that the walls surrounding the separate microcapsules in an encapsulated electrophoretic medium may be replaced with a continuous phase, thus producing so-called polymer-dispersed electrophoretic displays in which the electrophoretic medium comprises a plurality of separate droplets of electrophoretic fluid and a continuous phase of polymer material, and that the separate droplets of electrophoretic fluid in such polymer-dispersed electrophoretic displays may be considered capsules or microcapsules even though a separate capsule membrane is not associated with each individual droplet (see, e.g., U.S. Pat. No. 6,866,760).

[0033] In many cases, the electrophoretic medium is opaque (e.g., because in many electrophoretic media the particles substantially block the transmission of visible light through the display) and operates in a reflective mode, but 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-transmitting (see, 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 are similar to electrophoretic displays, but rely on variations in electric field strength and 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 a shutter mode. Electro-optic media operating in shutter mode may be used in multi-layer structures for full color displays, in which at least one layer adjacent to the viewing surface of the display operates in shutter mode to reveal or conceal a second layer that is further from the viewing surface.

[0034] An electrophoretic display typically comprises a layer of electrophoretic material and at least two other layers disposed on either side of the electrophoretic material, one of these two layers being an electrode layer. In most such displays, both layers are electrode layers, and one or both of the electrode layers are patterned to define the pixels of the display. For example, one electrode layer may be patterned into elongated row electrodes and the other into elongated column electrodes extending at right angles to the row electrodes, the pixels being defined by the intersections of the row and column electrodes. Alternatively, and more commonly, one electrode layer has the form of a single continuous electrode, and the other electrode layer is patterned into a matrix of pixel electrodes, each of which defines one pixel of the display. In another type of electrophoretic display, where the display is intended for use with a separate stylus, printhead, or similar movable electrode, only one of the layers adjacent to the electrophoretic layer comprises an electrode; the layer on the opposite side of the electrophoretic layer is typically a protective layer intended to prevent the movable electrode from damaging the electrophoretic layer.

[0035] The aforementioned U.S. Patent No. 6,982,178 describes a method for assembling solid electro-optic displays (including encapsulated electrophoretic displays) that is highly suitable for mass production. Essentially, this patent describes a so-called "front plane laminate" ("FPL") that comprises, in order, a light-transmitting conductive layer, a layer of solid electro-optic medium in electrical contact with the conductive layer, an adhesive layer, and a release sheet. Typically, the light-transmitting conductive layer is supported on a light-transmitting substrate, which is preferably flexible in the sense that the substrate can be manually wrapped around a 10 inch (254 mm) diameter drum (for example) without permanent deformation. In this application and herein, the term "light-transmissive" is used to mean that the layer so designated transmits sufficient light to enable an observer looking through the layer to observe a change in the display state of the electro-optic medium, which would normally be visible through the conductive layer and adjacent substrate (if present); if the electro-optic medium displays a change in reflectance at non-visible wavelengths, the term "light-transmissive" should of course be interpreted to refer to the transmission of the relevant non-visible wavelengths. The substrate is typically a polymeric film and will usually have a thickness within the range of about 1 to about 25 mils (25 to 634 μm), preferably about 2 to about 10 mils (51 to 254 μm). The conductive layer may conveniently be a thin metal or metal oxide layer, for example, aluminum or ITO, or may be a conductive polymer. Poly(ethylene terephthalate) (PET) films coated with aluminum or ITO are commercially available, for example as "aluminized Mylar" from EI du Pont de Nemours & Company (Wilmington Del.) ("Mylar" is a registered trademark), and such commercial materials can be used with good results in front plane laminates.

[0036] Assembly of an electro-optic display using such a front plane laminate may be accomplished by removing the release sheet from the front plane laminate and contacting the adhesive layer with the backplane under conditions effective to adhere the adhesive layer to the backplane, thereby securing the adhesive layer, layer of electro-optic medium, and conductive layer to the backplane. This process is well suited to mass production, as the front plane laminate can be mass produced, typically using roll-to-roll coating techniques, and then cut into pieces of any size required for use with a particular backplane.

[0037] No. 7,839,564 describes a so-called "inverted front plane laminate," which is a variation of the front plane laminate described in the aforementioned U.S. Pat. No. 6,982,178. This inverted front plane laminate comprises, in order, at least one of a light-transmissive protective layer and a light-transmissive conductive layer, an adhesive layer, a layer of a solid electro-optic medium, and a release sheet. This inverted front plane laminate is used to form electro-optic displays having a layer of laminating adhesive between the electro-optic layer and the front electrode or front substrate, and a second, typically thin, layer of adhesive may or may not be present between the electro-optic layer and the backplane. Such electro-optic displays can combine good resolution with good low temperature performance.

[0038] The electrodes in both the front plane laminate and the inverted front plane laminate may comprise a dielectric layer with an aperture in accordance with the present invention.

[0039] FIG. 1 of the accompanying drawings is a schematic cross-section through a microcell display of the present invention, generally designated as 100. A first substrate 102, which may be formed from glass or a polymer, has formed thereon a first electrode layer 104, which is divided into a plurality of pixel electrodes 104A, each of which defines one pixel of the display. The substrate 102 and the first electrode layer 104 together form the backplane of the display 100. The pixel electrodes 104A may form part of an active matrix backplane comprising row and column electrodes and transistors associated with each individual pixel electrode 104A, although these conventional components are omitted from FIG. 1 for ease of illustration. Alternatively, the display 100 may be a direct drive type display in which each individual pixel electrode 104A is provided with a separate voltage supply line (not shown).

[0040] A dielectric layer 106 having an opening 107 extending therethrough is in contact with the first electrode layer 104. The number of openings 107 shown in FIG. 1 is fewer than would typically be used in practice for ease of illustration. Furthermore, although FIG. 1 shows a dielectric layer associated with both electrode layers, the invention extends to displays where only one electrode layer has a dielectric layer associated with it. A conductive adhesive layer 108 overlies the dielectric layer 106, which is in turn overlaid by a seal layer 110.

[0041] The display 100 further comprises an electrophoretic medium 114, which is confined within microcells defined by the polymer layer 116, the dividing walls 112, and the aforementioned sealing layer 110. The sealing layer 116 is in contact with a second dielectric layer 118, which has openings 119, which is adhered to a transparent electrode layer 120 formed on a second substrate 122. Again, the number of openings 119 shown in FIG. 1 is fewer than would typically be used in practice, for ease of illustration. The polymer layer 116 may comprise a primer layer to aid adhesion on the electrode layer 120 and other components of the microcell layer.

[0042] The microcell display shown in FIG. 1 can be produced with minor modifications of the prior art processes for producing and filling microcell displays described in the patents and applications mentioned above. As described, the microcell display can be produced by first forming the electrode 120 on the second substrate 122; in practice, films comprising a transparent electrode layer on a polymer-based film are readily commercially available, and such films can be readily used to form the electrode 120 and the substrate 122. With the electrode layer 120 facing up, a layer of embossable prepolymer is then coated over the second electrode 120, embossed, and cured to form the polymer layer 116 and the dividing walls 112. The resulting open microcells are then filled with an electrophoretic medium 114, and a prepolymer film is coated over the microcells and cured to form the sealing layer 110. Separately, the backplane comprising layers 102 and 104 is formed and coated with adhesive layer 208; in practice, it is usually accomplished off-line, and adhesive layer 208 is covered with a release film (not shown). The microcell film and backplane film are then laminated together (after removal of the release film from the backplane film, if necessary), typically in a roll-to-roll lamination process, to form the final display as shown in FIG.

[0043] This prior art process can be easily modified to incorporate one or both of the apertured dielectric layers 106 and 118 shown in Figure 1 by (a) coating the dielectric layer 106 over the first electrode layer 104 before the adhesive layer 108 is applied, and / or (b) coating the dielectric layer 118 over the second electrode layer before the prepolymer is applied to form the microcells. In principle, a dielectric layer with apertures can be incorporated between any two adjacent layers of the display 100 shown in Figure 1, but in practice it is preferred that the dielectric layer is in contact with the first or second electrode layer 104 or 120 as shown in Figure 1.

[0044] The dielectric layers 104 and 120 may be formed from organic or inorganic materials, such as organic materials such as silicon dioxide, silicon nitride, metal oxides such as zinc oxide, tantalum oxide, hafnium oxide, etc., and perylene or other polymeric compounds. A combination of two or more materials may be used, and the dielectric layers may comprise two or more sub-layers, with the various sub-layers being formed from different materials. As discussed in more detail below, the dielectric layers may also be formed from photoresist. The material used should be impermeable to ions and electrons (as it is exposed to the high electric fields used to drive electrophoretic displays, typically about 10 6 High dielectric strength, preferably at least about 10 V / m 7 V / m. The optimum thickness for the dielectric layer depends on its dielectric constant, as discussed in more detail below.

[0045] As noted above, the incorporation of a dielectric layer into an electrophoretic display such as that shown in FIG. 1 introduces a capacitor in series with the electrophoretic fluid between the two electrodes; if the two electrodes are held at the same potential after a transition, discharging this capacitor can lead to sufficient current flowing through the electrophoretic medium to cause an undesirable shift in the optical state, the so-called electro-optic kickback. Using a dielectric layer with apertures according to the present invention effectively introduces a resistor (formed by the apertures) in parallel with a capacitor (formed by the non-apertured portion of the dielectric layer), this RC arrangement being in series with the electrophoretic fluid. The size and number of apertures in the dielectric layer controls the flow of current through the electrophoretic medium and therefore the relaxation rate of the charge stored in the capacitance of the dielectric layer. The ability to control this electrical relaxation time improves the performance of electrophoretic displays by limiting electro-optic kickback and the build-up of residual voltages and controlling the local electric field associated with the display. If the area of ​​the opening is small relative to the total area of ​​the dielectric layer, the RC time to discharge the dielectric layer can be much shorter than the RC time to discharge the interfacial bilayer formed in ion-doped conductive polymer adhesives (typically used in electrophoretic displays).

[0046] Those skilled in the art of electrophoretic display technology recognize that the electrical behavior of an electrophoretic display can be modeled as a series of Voigt elements (i.e., a parallel arrangement of storage and loss components) corresponding to the various layers and interfaces between the electrodes. Although these models are oversimplifications of the electrical behavior of actual electrophoretic displays, they provide a useful basis for understanding the effect of introducing additional layers into the display, such as the apertured dielectric layer used in the present invention. Figure 2 is a schematic diagram of such a model of a prior art encapsulated electrophoretic display, lacking any dielectric layer adjacent to the electrodes, while Figure 3 is a schematic diagram of an encapsulated electrophoretic display of the present invention, having an apertured dielectric layer adjacent one of the electrodes.

[0047] As shown in FIG. 2, a prior art encapsulated electrophoretic display (whether the encapsulation is in microcells as shown in FIG. 1, in separate capsules, or as a polymer dispersed electrophoretic medium is irrelevant for this purpose) is modeled as a stack of Voigt elements, with element C1 / R1 for the electrophoretic medium itself, element C2 / R2 representing the interface between the electrophoretic medium itself and the external phase, element C3 / R3 representing the external phase, and element C4 / R4 representing the interface between the external phase and the electrodes. (The term "external phase" is used in its conventional sense with respect to electrophoretic displays to refer to all layers that make up the display other than the electrophoretic medium itself. Thus, in the display shown in FIG. 1, the term "external phase" includes not only the polymer layer 116 that surrounds the electrophoretic medium, the dividing wall 112, and the sealing layer 110, but also the adhesive layer 108.)

[0048] A typical electrophoretic medium ("internal phase") comprising a solvent with a low dielectric constant (about 2) has a dielectric constant of 0.02 to 5 nF / cm when in a layer having a thickness in the range of 10 to 25 μm. 2 with bulk capacitance C1 in the range of approximately 1 to 10 MΩ.cm 2 The capacitance C2 at the interface between the electrophoretic fluid and the external phase is more difficult to estimate, but can be approximated by combining two capacitors in series, each with a dielectric thickness approximated by the Debye length of each medium (i.e., the internal and external phases). This is about 10-100 nF / cm 2 gives an estimate for C2 of 100 kΩ. The interfacial resistance R2, which corresponds to the passage of ions across the boundary, is more difficult to estimate. If this resistance is too high, the display will exhibit electrical (and possibly optical) kickback. The value of R2 that gives the best agreement with current measurements when driving a typical display is approximately the same as the resistance of the external phase, i.e., 1-10 MΩ.cm 2 The bulk capacitance C3 of the external phase, assuming it comprises a polymeric material with a dielectric constant of about 10 containing mobile ions, is in the range of about 0.1 to 10 nF / cm 2The resistance of the external phase, R3, is estimated to be 1 to 10 MΩ.cm. 2 Finally, the interfacial capacitance C4 at the electrode boundary is estimated from the Debye length in the doped polymer external phase. Its conductivity is approximately the same as that of the internal phase, but the mobility of the charge carriers is much lower, since the viscosity of the polymer is several orders of magnitude higher than that of the electrophoretic solvent. As a consequence, the concentration of ions must be much higher in the external phase than in the internal phase, and, consequently, the Debye length must be much shorter. The interfacial capacitance is in the range of 2-20 nF / cm 2 , i.e., much larger than any other capacitance in the system. It is possible that the electrochemical reaction at this interface could produce a "resistance" path R4 in FIG. 2, which would not be a simple resistor. This path is undesirable as it could lead to eventual degradation of the electrodes, as explained above. Methods of mitigating electrochemical currents in electrophoretic displays are discussed in detail, for example, in International Patent Application WO 2014 / 110394 A1.

[0049] The time required to produce an image is related to the RC time constant for charging the capacitor C2, which is typically less than 1 second. However, the RC time constant for charging the capacitance C4 at the electrode interface is much longer, typically about 100 seconds, so C4 will only be partially charged in the time that C2 is fully charged. The voltage across C4 is an approximation of the "residual voltage" stored in the display. In a DC balanced waveform, this residual voltage will be discharged most of the time, but in a non-DC balanced waveform, it will persist. Because the RC time for charging and discharging C4 is so long, it is not practical to fully discharge this capacitance by placing both electrodes at the same potential. To make matters worse, if there is a possibility of discharging C4 by the electrochemical reaction shown as R4 in FIG. 2, there may also be a slow electrochemical degradation of the electrodes in the undriven display caused by the residual voltage after updating.

[0050] The circuit diagram in Fig. 3 for an electrophoretic display of the invention having a dielectric layer with an aperture adjacent to one electrode has the same Voigt elements C1 / R1, C2 / R2, and C3 / R3 as those shown in Fig. 2. However, if the percentage of the area of ​​the dielectric layer occupied by the aperture is a, then the external phase / electrode interface must be modeled in parallel as a combination of (a) Voigt element C4.a / R5, representing the aperture itself (there is a potential for electrochemical current flow within the aperture, represented by R5), and (b) capacitor C4.(1-a) (representing the portion of the interface without an aperture) in series with capacitor C5.(1-a) (representing the capacitance of the dielectric layer itself); obviously, there is no potential for electrochemical current flow in this region, and therefore no resistive element is required.

[0051] To determine R5, it is necessary to consider the resistance of a perforated sheet of dielectric material with a single aperture in contact with the conductive layer, as shown in Figure 4. This resistance R can be estimated by calculating the flux of the current in the conductive layer through the aperture (i.e., by solving Laplace's equation for the geometry illustrated in Figure 4). For the case where the radius of the aperture is much smaller than the distance between the electrodes, it is l=2πr a σ(V TP -V P ) where l is the effective compliance and r a is the radius of the aperture, and V TP and V P are the top plane (front) and pixel electrode potentials, respectively.

[0052] The resistance is therefore inversely proportional to the radius of the aperture and to the conductivity of the overlying layer. For a plurality of n similar apertures, the resistance of the combination of the dielectric layer with the apertures and the overlying conductive material is the harmonic sum of the resistances associated with each individual aperture. Varying the radius and density of the apertures can therefore be used to adjust the RC time constant for the electrical relaxation of the capacitor formed by the dielectric layer. This capacitance depends on the dielectric constant of the dielectric layer and is inversely proportional to its thickness.

[0053] It is not required that the aperture density be constant over the entire area of ​​the dielectric layer, nor that all apertures have the same dimensions. Thus, by suitable selection of the aperture pattern in a particular area, it is possible to control the local electrical relaxation time of the dielectric layer. In areas with a lower aperture density, this relaxation time will be longer. FIG. 5 is a top plan view of a pixel arrangement, in which a dielectric layer with overlapping apertures has a varying aperture density. The dielectric layer associated with each pixel has a central region and a peripheral region, and the number of apertures per unit area is greater in the central region than in the peripheral region. The longer relaxation time provided by the lower aperture density in the peripheral region may allow for better control of fringe fields and therefore reduced edge artifacts in the display.

[0054] As previously mentioned, the present invention can reduce optical kickback in electrophoretic displays by allowing relaxation of the charge stored on the capacitor provided by the dielectric layer. Figure 6 shows the (dE) of a full-color electrophoretic display having an apertureless dielectric layer of various thicknesses. * FIG. 7 shows the optical kickback of the same electrophoretic display with the same electrophoretic medium but lacking a dielectric layer, with an external parallel capacitor / resistor in series with the display to mimic the effect of a dielectric layer with an aperture, the capacitor having a capacitance of 300 nF / cm 2The resistance is selected to correspond to a dielectric layer of less than about 360 kΩ and less than about 7 MΩ.cm 2 When the external capacitor (blue line) corresponds to 0 V, the optical kickback (gray line) can be mitigated to be intermediate in value with neither the external capacitor (blue line) nor the external resistor (orange line).

[0055] As shown in FIG. 1, the conductive material present on the opposite side of the dielectric layer from the electrode may be an adhesive layer, which may be doped with an ionic material to improve its conductivity. It may be desirable to provide two or more layers of conductive material adjacent the dielectric layer with the opening, each of the layers of conductive material having a different conductivity. The conductivity of the layer in contact with the dielectric layer (which thus fills the opening in the dielectric layer) may be adjusted so that the combination of this layer with the dielectric layer achieves the desired electrical properties, while other layers spaced from the dielectric layer may be optimized for other properties, such as adhesion or compliance.

[0056] As will be apparent from the discussion of Figure 4 above, in displays of the present invention, it may be necessary for electrochemical current to flow through openings in the dielectric to protect the underlying electrode material from oxidative or reductive damage. For example, in the area of ​​the openings, the electrode material (typically metal) may be made thicker than would conventionally be the case. Alternatively, a conductive layer in contact with the dielectric layer may include an electron donor or electron acceptor, as is known in the art.

[0057] The dielectric layer with apertures may be formed by any convenient process, depending on the dielectric material used. For example, if the dielectric layer is inorganic, the apertures may be formed by laser ablation. However, given the large number and small size of the apertures required in practice (e.g., FIG. 5 shows a dielectric layer with 44 apertures per pixel, or over 20 million apertures on an 800×600 display, the apertures are typically 1-5 μm in diameter), forming the apertures by photolithography is often the most convenient method. The electrodes to support the dielectric layer with apertures are coated with a photoresist, which is then imagewise exposed to radiation and washed to form the apertures. Any intervening layers, such as electrophoretic medium and adhesive, are then placed adjacent to the exposed photoresist. Such photoresist-based processes for the formation of the dielectric layer with apertures are well adapted for mass production of electrophoretic displays. Photoresists with suitable dielectric properties for use in the dielectric layer with apertures are commercially available, e.g., cinnamate class photoresists. U.S. Patent No. 7,981,989 describes a polymer adduct of poly(hydroxyethyl methacrylate) and cinnamoyl chloride, which in a capacitor configuration exhibits a capacitance of 2×10 -9 A / cm 2 and 1 × 10 under a field of 4 MV / cm -8 A / cm 2 and a leakage current density of 6.0 nF / cm in a 460 nm thick layer. 2and a breakdown voltage of over 200 volts. Similar photopatternable organic dielectric materials are described in U.S. Patent Nos. 8,338,555, 8,937,301, 9,082,981, 9,341,948, 9,704,997, 9,923,158, 10,147,895, and 10,551,745. The variety of available photopatternable polymeric dielectric materials allows for precise tuning of the dielectric properties to optimize the performance of the dielectric layer. These dielectric materials are solution processable, and commercialization of these types of materials has already been demonstrated for the production of organic thin film transistor devices using solvents and processes compatible with existing TFT manufacturing lines.

[0058] From the above, it will be seen that the present invention can provide electrophoretic displays with controlled current and reduced electro-optic kickback, thereby enabling such displays to be driven with DC unbalanced waveforms without damage to the display.

Claims

[Claim 1] The invention described in this specification.

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