CA2529719A1 - Self-stabilized electrophoretically frustrated total internal reflection display - Google Patents
Self-stabilized electrophoretically frustrated total internal reflection display Download PDFInfo
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- CA2529719A1 CA2529719A1 CA002529719A CA2529719A CA2529719A1 CA 2529719 A1 CA2529719 A1 CA 2529719A1 CA 002529719 A CA002529719 A CA 002529719A CA 2529719 A CA2529719 A CA 2529719A CA 2529719 A1 CA2529719 A1 CA 2529719A1
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- image display
- suspension
- front sheet
- voltage
- electrode
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/165—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on translational movement of particles in a fluid under the influence of an applied field
- G02F1/1685—Operation of cells; Circuit arrangements affecting the entire cell
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/165—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on translational movement of particles in a fluid under the influence of an applied field
- G02F1/166—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on translational movement of particles in a fluid under the influence of an applied field characterised by the electro-optical or magneto-optical effect
- G02F1/167—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on translational movement of particles in a fluid under the influence of an applied field characterised by the electro-optical or magneto-optical effect by electrophoresis
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/29—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the position or the direction of light beams, i.e. deflection
- G02F1/31—Digital deflection, i.e. optical switching
- G02F1/315—Digital deflection, i.e. optical switching based on the use of controlled internal reflection
Abstract
An image display (10) has a transparent front sheet (12) with a prismatically microstructured (16) inward surface and a rear sheet (14) substantially parallel to and spaced from the front sheet (12). An electrophoretic suspension fills the space between the sheets (12, 14). The suspension is formed by suspending non-light-scattering light absorptive particles (24) in an electrophoresis medium (22) until the particles (24) form a substantially unitary thermodynamically stable agglomeration (56). Application of a voltage across the suspension establishes an electric field for controllably electrophoretically moving the particle agglomeration (56) as a substantially unitary whole toward the front sheet's inward surface to frustrate total internal reflection at the inward surface of light rays passing through the front sheet (12).
Description
SELF-STABILIZED ELECTROPHORETICALLY FRUSTRATED
TOTAL INTERNAL REFLECTION DISPLAY
Technical Field This invention improves the long-term stability of image displays which electrophoretically frustrate total internal reflection (TIR) .
Back round It is known that images can be displayed by controllably frustrat-ing TIR to switch selected pixels of a mufti-pixel display between a reflective state in which light incident on those pixels undergoes TIR, and a non-reflective state in which TIR is frustrated at those pixels . It is also known that electrophoresis can be used to controllably frustrate TIR
and controllably switch the state of pixels in such displays. Electro-phoresis is a well-known phenomenon whereby an electrostatically-charged species moves through a medium due t~ the influence of an applied electric field. For example, an electromagnetic field can be controllably applied to move particles through an electrophoretic me-dium toward or away from an evanescent wave region to frustrate TIR
at selected pixel portions of the region.
It is also known that repeated switching of a display which utilizes electrophoretically-mobile particles can result in a non-uniform distribu-tion or clustering of the particles, gradually deteriorating the quality of images produced by the display over time. See for example Dalisa, A., "Electrophoretic Display Technology," IEEE Transactions on Electron Devices, Vol. 24, 827-834, 1977; and Miirau et al, "The understanding and elimination of some suspension instabilities in an electrophoretic display," J. Appl. Phys., Vol. 49, No. 9, September 1978, pp.
4820-4829. It has been shown that such undesirable clustering can be reduced by encapsulating groups of suspended particles in separate micro-fluidic regions. See for example Nakamura et al, "Development of Electrophoretic Display Using Microencapsulated Suspension,"
Society for Information Display Symposium Proceedings, 1014-1017, 1998 and Drzaic et al, "A Printed and Rollable Bistable Electronic Display," Society for Information Display Symposium Proceedings, 1131-1134, 199.
Summary of Invention This invention improves the long-term image stability of an electrophoretically-mobile particle display, by providing a thermody-namically stable agglomeration of particles in the electrophoretic sus-pension. The agglomeration can be electrophoretically moved as a substantially unitary whole to switch the display's pixels between reflective and non-reflective states, without encapsulating groups of suspended particles in separate regions.
Brief Description of Drawings Figure 1 is a fragmented, cross-sectional view, on a greatly enlarged scale, of a portion of a prior art electrophoretically frustrated TIR image display, depicting undesirable non-uniform particle distribu-tion.
Figure 2A is a fragmented, cross-sectional view, on a greatly enlarged scale, of a portion of a prior art electrophoretically frustrated TIR image display, before application of an electric field. Figure 2B
depicts the Figure 2A display after selective application of an electric field.
Figure 3A is a fragmented, cross-sectional view, on a greatly enlarged scale, of a portion of one pixel of an electrophoretically frustrated TIR image display in accordance with the invention, before application of an electric field. Figure 3B depicts the Figure 3A display after selective application of an electric field.
Description Throughout the following description, specific details are set forth in order to provide a more thorough understanding of the invention.
TOTAL INTERNAL REFLECTION DISPLAY
Technical Field This invention improves the long-term stability of image displays which electrophoretically frustrate total internal reflection (TIR) .
Back round It is known that images can be displayed by controllably frustrat-ing TIR to switch selected pixels of a mufti-pixel display between a reflective state in which light incident on those pixels undergoes TIR, and a non-reflective state in which TIR is frustrated at those pixels . It is also known that electrophoresis can be used to controllably frustrate TIR
and controllably switch the state of pixels in such displays. Electro-phoresis is a well-known phenomenon whereby an electrostatically-charged species moves through a medium due t~ the influence of an applied electric field. For example, an electromagnetic field can be controllably applied to move particles through an electrophoretic me-dium toward or away from an evanescent wave region to frustrate TIR
at selected pixel portions of the region.
It is also known that repeated switching of a display which utilizes electrophoretically-mobile particles can result in a non-uniform distribu-tion or clustering of the particles, gradually deteriorating the quality of images produced by the display over time. See for example Dalisa, A., "Electrophoretic Display Technology," IEEE Transactions on Electron Devices, Vol. 24, 827-834, 1977; and Miirau et al, "The understanding and elimination of some suspension instabilities in an electrophoretic display," J. Appl. Phys., Vol. 49, No. 9, September 1978, pp.
4820-4829. It has been shown that such undesirable clustering can be reduced by encapsulating groups of suspended particles in separate micro-fluidic regions. See for example Nakamura et al, "Development of Electrophoretic Display Using Microencapsulated Suspension,"
Society for Information Display Symposium Proceedings, 1014-1017, 1998 and Drzaic et al, "A Printed and Rollable Bistable Electronic Display," Society for Information Display Symposium Proceedings, 1131-1134, 199.
Summary of Invention This invention improves the long-term image stability of an electrophoretically-mobile particle display, by providing a thermody-namically stable agglomeration of particles in the electrophoretic sus-pension. The agglomeration can be electrophoretically moved as a substantially unitary whole to switch the display's pixels between reflective and non-reflective states, without encapsulating groups of suspended particles in separate regions.
Brief Description of Drawings Figure 1 is a fragmented, cross-sectional view, on a greatly enlarged scale, of a portion of a prior art electrophoretically frustrated TIR image display, depicting undesirable non-uniform particle distribu-tion.
Figure 2A is a fragmented, cross-sectional view, on a greatly enlarged scale, of a portion of a prior art electrophoretically frustrated TIR image display, before application of an electric field. Figure 2B
depicts the Figure 2A display after selective application of an electric field.
Figure 3A is a fragmented, cross-sectional view, on a greatly enlarged scale, of a portion of one pixel of an electrophoretically frustrated TIR image display in accordance with the invention, before application of an electric field. Figure 3B depicts the Figure 3A display after selective application of an electric field.
Description Throughout the following description, specific details are set forth in order to provide a more thorough understanding of the invention.
However, the invention may be practiced without these particulars. In other instances, well known elements have not been shown or described in detail to avoid unnecessarily obscuring the invention. Accordingly, the specification and drawings are to be regarded in an illustrative, rather than a restrictive, sense.
Figure 1 depicts a portion of an electrophoretically-frustrated TIR
image display 10 having a transparent front sheet 12 and a rear sheet 14 substantially parallel to and spaced from front sheet 12. Front sheet 12's inward surface is microstructured by forming a large plurality of parallel, reflective micro-prisms 16 thereon. Alternatively, front sheet 12's inward surface can be microstructured by forming a large plurality of approximately hemispherical high refractive index transparent hemi-beads-thereon, as described in United States Patent Publication No.
20030165016 dated 4 September 2003, which is incorporated herein by reference. A thin, continuous, transparent electrode 18 is applied to the inward surfaces of prisms I6. A segmented electrode 20 is applied to the inward surface of rear sheet 14, to apply separate voltages (corre-sponding to individual pixels) between each adjacent pair of prisms 16.
'There need not be a 1:1 correspondence between each pixel and one of prisms 16 or one of the segments of electrode 20; each pixel preferably corresponds to a plurality of prisms 16 and to a (possibly different) plurality of segments of electrode 20. An electrophoresis medium 22, for example, a low refractive index, low viscosity, electrically insulating liquid such as Fluorinert~M perfluorinated hydrocarbon liquid available from 3M, St. Paul, MN substantially fills the space between sheets 12, 14 forming a TIR interface between sheet 12 and medium 22. A finely dispersed suspension of non-light-scattering, light-absorptive particles 24, such as pigment particles, is provided in medium 22.
A voltage source (not shown) is electrically connected between electrodes 18, 20 to controllably apply a voltage across selected pixel regions of medium 22. Application of a voltage across a selected pixel region electrophoretically moves particles 24 suspended within the selected region to form a layer that begins within about 0.25 micron of the evanescent wave zone adjacent the inward surfaces of the selected region's prisms 16 and extends about 5 microns into the region. When electrophoretically moved as aforesaid, particles 24, which have a higher refractive index than the surrounding fluid and are much smaller than a wavelength of light and therefore substantially non-light-scatter-ing, cause the layer to have an effective refractive index that is substan-tially higher than that of the surrounding liquid. This absorptive particle layer has both a real component of the refractive index that frustrates TIR and causes transmission, rather than reflection, of the light ray at the interface; and an imaginary component that causes absorption of the light ray at it passes through the absorptive particle layer. There is essentially no scattering of the light as it interacts with the particles, but rather the light is absorbed. This gives the selected pixel region a dark appearance to an observer who looks at sheet 12's outward surface.
Application of an opposite polarity voltage across the selected pixel region electrophoretically moves particles 24 toward that region's electrode 20, such that incident light rays which pass through sheet 12 are reflected by TIR at that region's TIR interface, giving the region a "white" appearance to an observer who looks at sheet 12's outward surface .
Further details of the construction and optical characteristics of electrophoretically-frustrated TIR image displays can be found in United States Patent Nos. 6,064,784; 6,215,920; 6,304,365; 6,384,979;
6,437,921; and 6,452,734 all of which are incorporated herein by reference; and, in the aforementioned United States Patent Publication No. 20030165016.
Electrophoretically-frustrated display 10 can exhibit undesirable clustering of particles 24 over time. More particularly, particles 24 tend to form loose agglomerates 26, surrounded by regions 28 of medium 22 containing relatively few suspended particles 24. Such clustering often results in long-term deterioration of the display's image quality and overall performance.
Figures 2A and 2B depict a prior art technique for reducing undesirable particle clustering in an electrophoretically-frustrated display 30 having a transparent front sheet 32 and a rear sheet 34.
Front sheet 32's inward surface is microstructured by forming a large plurality of parallel, reflective micro-prisms 36 thereon. The apices 3~
of micro-prisms 36 are connected to rear sheet 34's inward surface, forming an encapsulated channel 40 between the opposed facets of each adjacent pair of prisms 36. Each channel 40 is filled with an electro-phoresis medium 42, forming a TIR interface between sheet 32 and medium 42. Within each channel 40, medium 42 contains a finely dispersed suspension of non-light-scattering light-absorptive particles 44, such as pigment particles. Within each channel 40, a thin trans-parent electrode 45 is applied to the inward surfaces of the adjacent prisms 36 which define that channel. A segmented electrode 46 is applied to the inward surface of rear sheet 34, to create separate pixel regions corresponding to each channel 40 (or corresponding to a selected group of adjacent channels 40).
A voltage source (not shown) is electrically connected between each channel's electrode pair 45, 46 to controllably apply a voltage across the corresponding pixel region. Application of a voltage across a selected pixel region electrophoretically moves particles 44 suspended within the selected region to form a layer that begins within about 0.25 micron of the evanescent wave gone adjacent the inward surfaces of the selected region's prisms 16 and extends about 5 microns into the region, as depicted in the case of channel 40C (Figure 2B) . When electrophor-etically moved as aforesaid, particles 44, which have a higher refractive index than the surrounding fluid and are much smaller than a wave-length of light and therefore substantially non-light-scattering, cause the layer to have an effective refractive index that is substantially higher than that of the surrounding liquid. This absorptive particle layer has both a real component of the refractive index that frustrates TIR and causes transmission, rather than reflection, of the light ray at the inter-s face; and an imaginary component that causes absorption of the light ray at it passes through the absorptive particle layer. . There is essentially no scattering of the light as it interacts with the particles, but rather the light is absorbed. This gives the selected pixel region a dark appearance to an observer who looks at sheet 32's outward surface. Application of an opposite polarity voltage across a selected pixel region electro-phoretically moves (i. e, switches) particles 44 toward that region's electrode 46, as depicted in the case of channels 40A and 40B, such that light rays 52, 54 which pass through sheet 32 are reflected by TIR at that region's TIR interface, giving the region a "white" appearance to an observer who looks at sheet 32's outward surface. ' Although encapsulation of groups of particles 44 within separate channels 40 reduces undesirable clustering, it may in some cases be impractical to fabricate, fill or maintain channels 40.
In accordance with the invention, the electrophoresis medium contains a high concentration of light-absorptive pigment particles, forming a sponge-like electrophoretic suspension paste having a volume fraction of particles in the suspension that is sufficiently Iarge that the particles do not move freely within the electrophoresis medium, thus preventing the lateral particle motion which is believed to cause Iong-term particle clustering. More specifically, the volume fraction is sufficiently large that the suspension is in a thermodynamically stable state such that a uniform distribution of particles is maintained. The volume fraction at which this thermodynamic stability occurs depends on the inter-particle force relationship for the specific particles within the particular suspension. The suspension can be formed by adding particles to the electrophoresis medium until the particles form a substantially unitary agglomeration which can be electrophoretically moved and compressed as a substantially unitary whole in response to an applied voltage, to controllably frustrate TIR. Alternatively, a dilute suspension can be initially formed, followed by evaporation of the electrophoresis medium until the desired volume fraction of particles in the suspension is attained. A dispersant such as I~rytox°''N' 157-FSL, Krytox'~ 157-FSM or I~ryto~'~ 157-FSI~ fluorinated oil (respectively having specified molecular weights of approximately 2500, 3500-4000 and 7000-7500, CAS Registry No. 860164-51-4, l~uPont Performance Lubricants, Wilmington, ICE 19880-0023) is preferably added to the suspension to facilitate stable suspension of the particles in the electro-phoresis medium.
This is shown- schematically in Figures 3A and 3B, which depict a selected pixel region of the Figure 1 display structure with an electro-phoretic suspension having an electrophoretically compressible, non-light-scattering light absorbing particle agglomeration 56 substituted f~r electrophoresis medium 22 and particles 24. A voltage source 57 is electrically connected between electrodes 18, 20 to controllably apply a voltage across electrophoresis medium 22. The applied voltage affects substantially all particles 24 between electrodes 18, 20 (i.e. particle agglomeration 56). As shown in Figure 3A, the applied voltage electro-phoretically compresses particle agglomeration 56 away from electrode 18 toward electrode 20. This leaves a thin region 58 of low refractive index electrophoretic fluid between the inward surface of sheet 12 and particle agglomeration 56, which is sufficiently thick that it enables substantially all of the evanescent wave to be confined to a particle-free region of fluid and thus causes TIR, such that light ray 60 which passes through sheet 12 is reflected by TIR at the depicted region's TIR
interface, giving the region a "white" appearance to an observer who looks at sheet 12's outward surface.
_g_ More particularly, particles 24 are substantially incompressible, but particle agglomeration S6 has many tiny inter-particle voids contain-ing electrophoresis medium 22. Since particles 24 are electrostatically charged as a result of chemical interactions between the solvent and dis-persant molecules and surface groups on the particles, application of a voltage across particle agglomeration 56 moves particles 24 as a sub-stantially unitary whole toward one or the other of electrodes l~, 20 depending on the polarity of the applied voltage. This compresses par-ticle agglomeration 56, packing particles 24 even more tightly together and forcing electrophoresis medium 22 out of the inter-particle voids.
As shown in Figure 3B, application of an opposite polarity voltage across the depicted pixel region electrophoretically compresses (i.e. switches) particle agglomeration 56 away from electrode 20 toward electrode I g, to within about 0.25 micron of the evanescent wave zone adjacent the inward surfaces of the depicted region's prisms 16. When electrophoretically compressed toward electrode 1 ~ as aforesaid, particle agglomeration 56 scatters or absorbs incident light ray 62 by causing a refractive index mismatch which frustrates TIR, giving the depicted pixel region a dark appearance to an observer who looks at sheet I2's outward surface.
It is counterintuitive that the large volume fraction of particles 24 in the suspension allows sufficient motion of particles 24 within the evanescent wave region to controllably modulate TIR. Although the large volume fraction of particles 24 in the suspension gives the suspen-sion high bulk viscosity, the low refractive index electrophoresis medium 22 filling the inter-particle voids has very low viscosity, and thus it is comparatively easy to compress particle agglomeration 56 to force a region of particle-free low refractive index electrophoresis medium 22 into contact with the inward surface of sheet 12. More specifically, since the viscosity of electrophoresis medium 22 is low and since the particle-free region need only be thick enough to confine substantially all of the evanescent wave, good optical control can be maintained.
Electrode 20 can be segmented to provide a plurality of electrode segments, as shown in Figure 1. A suitable controller (not shown) can then be used to apply a first voltage between the first electrode and a first one of the electrode segments, apply a second voltage between the first electrode and a second one of the electrode segments, etc. in order to establish distinct electric fields between selected electrodes. Each electrode segment (or group of adjacent electrode segments) corresponds to an individually controllable pixel.
As will be apparent to those skilled in the art in light of the foregoing disclosure, many alterations and modifications are possible in the practice of this invention without departing from the spirit or scope thereof. For example, as previously explained, the volume fraction of particles 24 in the suspension should be sufficiently large that the sus-pension is in a thermodynamically-stable state such that a uniform dis-tribution of particles is maintained. The volume fraction at which this thermodynamic stability occurs depends on the inter-particle force relationship for the specific particles within the particular suspension.
For many suspensions this thermodynamic stability occurs within the range of about 25 % to 75 % , with efficacy improving as the volume fraction of particles 24 is increased within the foregoing range. Electro-phoresis medium 22 and the dispersant constitute the remaining volume fraction of particle agglomeration 56 which is not occupied by particles 24. Higher volume fractions of particles 24 in the suspension (within the aforementioned range) reduce the likelihood of particles 24 cluster-ing together after repeated switching. But, if the volume fraction of particles 24 in the suspension is greater than about 75 % , insufficient electrophoresis medium 22 remains in the inter-particle voids, making it difficult to attain the highly reflective state by compressing particle agglomeration 56 and forcing a sufficient quantity of electrophoresis - to -medium 22 out of the inter-particle voids to form low refractive index electrophoretic fluid region 58. The desired compressibility of particle agglomeration 56 is also impaired if insufficient dispersant is provided in the suspension, resulting in non-stable suspension of particles 24 S which can cause particles 24 to adhere to one another. The scope of the invention is to be construed in accordance with the substance defined by the following claims.
Figure 1 depicts a portion of an electrophoretically-frustrated TIR
image display 10 having a transparent front sheet 12 and a rear sheet 14 substantially parallel to and spaced from front sheet 12. Front sheet 12's inward surface is microstructured by forming a large plurality of parallel, reflective micro-prisms 16 thereon. Alternatively, front sheet 12's inward surface can be microstructured by forming a large plurality of approximately hemispherical high refractive index transparent hemi-beads-thereon, as described in United States Patent Publication No.
20030165016 dated 4 September 2003, which is incorporated herein by reference. A thin, continuous, transparent electrode 18 is applied to the inward surfaces of prisms I6. A segmented electrode 20 is applied to the inward surface of rear sheet 14, to apply separate voltages (corre-sponding to individual pixels) between each adjacent pair of prisms 16.
'There need not be a 1:1 correspondence between each pixel and one of prisms 16 or one of the segments of electrode 20; each pixel preferably corresponds to a plurality of prisms 16 and to a (possibly different) plurality of segments of electrode 20. An electrophoresis medium 22, for example, a low refractive index, low viscosity, electrically insulating liquid such as Fluorinert~M perfluorinated hydrocarbon liquid available from 3M, St. Paul, MN substantially fills the space between sheets 12, 14 forming a TIR interface between sheet 12 and medium 22. A finely dispersed suspension of non-light-scattering, light-absorptive particles 24, such as pigment particles, is provided in medium 22.
A voltage source (not shown) is electrically connected between electrodes 18, 20 to controllably apply a voltage across selected pixel regions of medium 22. Application of a voltage across a selected pixel region electrophoretically moves particles 24 suspended within the selected region to form a layer that begins within about 0.25 micron of the evanescent wave zone adjacent the inward surfaces of the selected region's prisms 16 and extends about 5 microns into the region. When electrophoretically moved as aforesaid, particles 24, which have a higher refractive index than the surrounding fluid and are much smaller than a wavelength of light and therefore substantially non-light-scatter-ing, cause the layer to have an effective refractive index that is substan-tially higher than that of the surrounding liquid. This absorptive particle layer has both a real component of the refractive index that frustrates TIR and causes transmission, rather than reflection, of the light ray at the interface; and an imaginary component that causes absorption of the light ray at it passes through the absorptive particle layer. There is essentially no scattering of the light as it interacts with the particles, but rather the light is absorbed. This gives the selected pixel region a dark appearance to an observer who looks at sheet 12's outward surface.
Application of an opposite polarity voltage across the selected pixel region electrophoretically moves particles 24 toward that region's electrode 20, such that incident light rays which pass through sheet 12 are reflected by TIR at that region's TIR interface, giving the region a "white" appearance to an observer who looks at sheet 12's outward surface .
Further details of the construction and optical characteristics of electrophoretically-frustrated TIR image displays can be found in United States Patent Nos. 6,064,784; 6,215,920; 6,304,365; 6,384,979;
6,437,921; and 6,452,734 all of which are incorporated herein by reference; and, in the aforementioned United States Patent Publication No. 20030165016.
Electrophoretically-frustrated display 10 can exhibit undesirable clustering of particles 24 over time. More particularly, particles 24 tend to form loose agglomerates 26, surrounded by regions 28 of medium 22 containing relatively few suspended particles 24. Such clustering often results in long-term deterioration of the display's image quality and overall performance.
Figures 2A and 2B depict a prior art technique for reducing undesirable particle clustering in an electrophoretically-frustrated display 30 having a transparent front sheet 32 and a rear sheet 34.
Front sheet 32's inward surface is microstructured by forming a large plurality of parallel, reflective micro-prisms 36 thereon. The apices 3~
of micro-prisms 36 are connected to rear sheet 34's inward surface, forming an encapsulated channel 40 between the opposed facets of each adjacent pair of prisms 36. Each channel 40 is filled with an electro-phoresis medium 42, forming a TIR interface between sheet 32 and medium 42. Within each channel 40, medium 42 contains a finely dispersed suspension of non-light-scattering light-absorptive particles 44, such as pigment particles. Within each channel 40, a thin trans-parent electrode 45 is applied to the inward surfaces of the adjacent prisms 36 which define that channel. A segmented electrode 46 is applied to the inward surface of rear sheet 34, to create separate pixel regions corresponding to each channel 40 (or corresponding to a selected group of adjacent channels 40).
A voltage source (not shown) is electrically connected between each channel's electrode pair 45, 46 to controllably apply a voltage across the corresponding pixel region. Application of a voltage across a selected pixel region electrophoretically moves particles 44 suspended within the selected region to form a layer that begins within about 0.25 micron of the evanescent wave gone adjacent the inward surfaces of the selected region's prisms 16 and extends about 5 microns into the region, as depicted in the case of channel 40C (Figure 2B) . When electrophor-etically moved as aforesaid, particles 44, which have a higher refractive index than the surrounding fluid and are much smaller than a wave-length of light and therefore substantially non-light-scattering, cause the layer to have an effective refractive index that is substantially higher than that of the surrounding liquid. This absorptive particle layer has both a real component of the refractive index that frustrates TIR and causes transmission, rather than reflection, of the light ray at the inter-s face; and an imaginary component that causes absorption of the light ray at it passes through the absorptive particle layer. . There is essentially no scattering of the light as it interacts with the particles, but rather the light is absorbed. This gives the selected pixel region a dark appearance to an observer who looks at sheet 32's outward surface. Application of an opposite polarity voltage across a selected pixel region electro-phoretically moves (i. e, switches) particles 44 toward that region's electrode 46, as depicted in the case of channels 40A and 40B, such that light rays 52, 54 which pass through sheet 32 are reflected by TIR at that region's TIR interface, giving the region a "white" appearance to an observer who looks at sheet 32's outward surface. ' Although encapsulation of groups of particles 44 within separate channels 40 reduces undesirable clustering, it may in some cases be impractical to fabricate, fill or maintain channels 40.
In accordance with the invention, the electrophoresis medium contains a high concentration of light-absorptive pigment particles, forming a sponge-like electrophoretic suspension paste having a volume fraction of particles in the suspension that is sufficiently Iarge that the particles do not move freely within the electrophoresis medium, thus preventing the lateral particle motion which is believed to cause Iong-term particle clustering. More specifically, the volume fraction is sufficiently large that the suspension is in a thermodynamically stable state such that a uniform distribution of particles is maintained. The volume fraction at which this thermodynamic stability occurs depends on the inter-particle force relationship for the specific particles within the particular suspension. The suspension can be formed by adding particles to the electrophoresis medium until the particles form a substantially unitary agglomeration which can be electrophoretically moved and compressed as a substantially unitary whole in response to an applied voltage, to controllably frustrate TIR. Alternatively, a dilute suspension can be initially formed, followed by evaporation of the electrophoresis medium until the desired volume fraction of particles in the suspension is attained. A dispersant such as I~rytox°''N' 157-FSL, Krytox'~ 157-FSM or I~ryto~'~ 157-FSI~ fluorinated oil (respectively having specified molecular weights of approximately 2500, 3500-4000 and 7000-7500, CAS Registry No. 860164-51-4, l~uPont Performance Lubricants, Wilmington, ICE 19880-0023) is preferably added to the suspension to facilitate stable suspension of the particles in the electro-phoresis medium.
This is shown- schematically in Figures 3A and 3B, which depict a selected pixel region of the Figure 1 display structure with an electro-phoretic suspension having an electrophoretically compressible, non-light-scattering light absorbing particle agglomeration 56 substituted f~r electrophoresis medium 22 and particles 24. A voltage source 57 is electrically connected between electrodes 18, 20 to controllably apply a voltage across electrophoresis medium 22. The applied voltage affects substantially all particles 24 between electrodes 18, 20 (i.e. particle agglomeration 56). As shown in Figure 3A, the applied voltage electro-phoretically compresses particle agglomeration 56 away from electrode 18 toward electrode 20. This leaves a thin region 58 of low refractive index electrophoretic fluid between the inward surface of sheet 12 and particle agglomeration 56, which is sufficiently thick that it enables substantially all of the evanescent wave to be confined to a particle-free region of fluid and thus causes TIR, such that light ray 60 which passes through sheet 12 is reflected by TIR at the depicted region's TIR
interface, giving the region a "white" appearance to an observer who looks at sheet 12's outward surface.
_g_ More particularly, particles 24 are substantially incompressible, but particle agglomeration S6 has many tiny inter-particle voids contain-ing electrophoresis medium 22. Since particles 24 are electrostatically charged as a result of chemical interactions between the solvent and dis-persant molecules and surface groups on the particles, application of a voltage across particle agglomeration 56 moves particles 24 as a sub-stantially unitary whole toward one or the other of electrodes l~, 20 depending on the polarity of the applied voltage. This compresses par-ticle agglomeration 56, packing particles 24 even more tightly together and forcing electrophoresis medium 22 out of the inter-particle voids.
As shown in Figure 3B, application of an opposite polarity voltage across the depicted pixel region electrophoretically compresses (i.e. switches) particle agglomeration 56 away from electrode 20 toward electrode I g, to within about 0.25 micron of the evanescent wave zone adjacent the inward surfaces of the depicted region's prisms 16. When electrophoretically compressed toward electrode 1 ~ as aforesaid, particle agglomeration 56 scatters or absorbs incident light ray 62 by causing a refractive index mismatch which frustrates TIR, giving the depicted pixel region a dark appearance to an observer who looks at sheet I2's outward surface.
It is counterintuitive that the large volume fraction of particles 24 in the suspension allows sufficient motion of particles 24 within the evanescent wave region to controllably modulate TIR. Although the large volume fraction of particles 24 in the suspension gives the suspen-sion high bulk viscosity, the low refractive index electrophoresis medium 22 filling the inter-particle voids has very low viscosity, and thus it is comparatively easy to compress particle agglomeration 56 to force a region of particle-free low refractive index electrophoresis medium 22 into contact with the inward surface of sheet 12. More specifically, since the viscosity of electrophoresis medium 22 is low and since the particle-free region need only be thick enough to confine substantially all of the evanescent wave, good optical control can be maintained.
Electrode 20 can be segmented to provide a plurality of electrode segments, as shown in Figure 1. A suitable controller (not shown) can then be used to apply a first voltage between the first electrode and a first one of the electrode segments, apply a second voltage between the first electrode and a second one of the electrode segments, etc. in order to establish distinct electric fields between selected electrodes. Each electrode segment (or group of adjacent electrode segments) corresponds to an individually controllable pixel.
As will be apparent to those skilled in the art in light of the foregoing disclosure, many alterations and modifications are possible in the practice of this invention without departing from the spirit or scope thereof. For example, as previously explained, the volume fraction of particles 24 in the suspension should be sufficiently large that the sus-pension is in a thermodynamically-stable state such that a uniform dis-tribution of particles is maintained. The volume fraction at which this thermodynamic stability occurs depends on the inter-particle force relationship for the specific particles within the particular suspension.
For many suspensions this thermodynamic stability occurs within the range of about 25 % to 75 % , with efficacy improving as the volume fraction of particles 24 is increased within the foregoing range. Electro-phoresis medium 22 and the dispersant constitute the remaining volume fraction of particle agglomeration 56 which is not occupied by particles 24. Higher volume fractions of particles 24 in the suspension (within the aforementioned range) reduce the likelihood of particles 24 cluster-ing together after repeated switching. But, if the volume fraction of particles 24 in the suspension is greater than about 75 % , insufficient electrophoresis medium 22 remains in the inter-particle voids, making it difficult to attain the highly reflective state by compressing particle agglomeration 56 and forcing a sufficient quantity of electrophoresis - to -medium 22 out of the inter-particle voids to form low refractive index electrophoretic fluid region 58. The desired compressibility of particle agglomeration 56 is also impaired if insufficient dispersant is provided in the suspension, resulting in non-stable suspension of particles 24 S which can cause particles 24 to adhere to one another. The scope of the invention is to be construed in accordance with the substance defined by the following claims.
Claims (24)
1. ~An image display (10), comprising a transparent front sheet (12), a rear sheet (14) substantially parallel to and spaced from the front sheet (12), an electrophoretic suspension substantially filling the space between the sheets (12, 14), the suspension further comprising an electrophoresis medium (22) with non-light-scattering light absorptive particles (24) suspended in the medium (22), the display (10) characterized by:
(a) ~the particles (24) occupying a sufficiently large volume fraction of the suspension to form a thermodynamically stable agglomeration (56); and, (b) ~means for applying a voltage across the suspension for controllably electrophoretically moving the agglomeration (56) as a substantially unitary whole toward an inward surface of the front sheet (12) to frustrate total internal reflection at the inward surface of light rays passing through the front sheet (12).
(a) ~the particles (24) occupying a sufficiently large volume fraction of the suspension to form a thermodynamically stable agglomeration (56); and, (b) ~means for applying a voltage across the suspension for controllably electrophoretically moving the agglomeration (56) as a substantially unitary whole toward an inward surface of the front sheet (12) to frustrate total internal reflection at the inward surface of light rays passing through the front sheet (12).
2. An image display (10) as defined in claim 1, wherein the particles (24) occupy more than about a 25 % volume fraction of the suspension.
3. An image display (10) as defined in claim 1, wherein the particles (24) occupy between about a 25% and a 75% volume fraction of the suspension.
4. An image display (10) as defined in claim 1, the suspension further comprising a dispersant.
5. ~An image display (10) as defined in claim 4, the dispersant further comprising a fluorinated oil.
6. ~An image display (10) as defined in claim 4, further characterized by the agglomeration (56) being compressible as a substantially unitary whole toward:
(a) ~the front sheet (12) in response to a first applied voltage;
and, (b) ~the rear sheet (14) in response to a second applied voltage.
(a) ~the front sheet (12) in response to a first applied voltage;
and, (b) ~the rear sheet (14) in response to a second applied voltage.
7. ~An image display (10) as defined in claim 6, wherein the front sheet (12) inward surface is microstructured.
8.~An image display (10) as defined in claim 6, wherein the front sheet (12) inward surface is prismatically microstructured (16).
9. ~An image display (10) as defined in claim 6, wherein the front sheet (12) inward surface further comprises a plurality of approximately hemispherical transparent hemi-beads.
10. ~An image display (10) as defined in claim 6, wherein the electro phoresis medium (22) is a perfluorinated hydrocarbon liquid
11. ~An image display (10) as defined in claim 6, wherein the means for applying a voltage is further characterized by a transparent first electrode (18) on the front sheet (12) inward surface and a second electrode (20) on an inward surface of the rear sheet (14).
12. ~An image display (10) as defined in claim 11, the second electrode (20) further characterized by a plurality of electrode segments, wherein application of the voltage between the first electrode (18) and a selected one of the electrode segments establishes an electric field distinct from any electric field established by application of the voltage between the first electrode (18) and any of the electrode segments other than the selected segment.
13. An image display method, characterized by:
(a) positioning a transparent front sheet (12) substantially parallel to and spaced from a rear sheet (14);
(b) suspending non-light-scattering light absorptive particles (24) in an electrophoresis medium (22) to create an electrophoretic suspension in which the particles occupy a sufficiently large volume fraction of the suspension to form a thermodynamically stable agglomeration (56);
(c) substantially filling the space between the sheets (12, 14) with the electrophoretic suspension; and, (d) applying a voltage across the suspension to controllably electrophoretically move the agglomeration (56) as a substantially unitary whole toward an inward surface of the front sheet (12) to frustrate total internal reflection at the inward surface of light rays passing through the front sheet (12).
(a) positioning a transparent front sheet (12) substantially parallel to and spaced from a rear sheet (14);
(b) suspending non-light-scattering light absorptive particles (24) in an electrophoresis medium (22) to create an electrophoretic suspension in which the particles occupy a sufficiently large volume fraction of the suspension to form a thermodynamically stable agglomeration (56);
(c) substantially filling the space between the sheets (12, 14) with the electrophoretic suspension; and, (d) applying a voltage across the suspension to controllably electrophoretically move the agglomeration (56) as a substantially unitary whole toward an inward surface of the front sheet (12) to frustrate total internal reflection at the inward surface of light rays passing through the front sheet (12).
14. An image display method as defined in claim 13, further characterized by the particles (24) occupying more than about a 25% volume fraction of the suspension.
15. An image display method as defined in claim I3, further characterized by the particles (24) occupying between about a 25 % and a 75 % volume fraction of the suspension.
-14-~
-14-~
16. An image display method as defined in claim 13, further characterized by adding a dispersant to the suspension.
17. An image display method as defined in claim 16, wherein the dispersant is a fluorinated oil.
18. An image display method as defined in claim 16, wherein applying the voltage further comprises:
(a) applying a first voltage to compress the agglomeration (56) as a substantially unitary whole toward the front sheet (12);
and, (b) applying a second voltage to compress the agglomeration (56) as a substantially unitary whole toward the rear sheet (14).
(a) applying a first voltage to compress the agglomeration (56) as a substantially unitary whole toward the front sheet (12);
and, (b) applying a second voltage to compress the agglomeration (56) as a substantially unitary whole toward the rear sheet (14).
19. An image display method as defined in claim 18, further characterized by microstructuring the inward surface of the front sheet (12).
20. An image display method as defined in claim 18, further characterized by prismatically microstructuring (16) the inward surface of the front sheet (12).
21. An image display method as defined in claim 18, further characterized by forming a plurality of approximately hemispherical transparent hemi-beads on the inward surface of the front sheet (12).
22. An image display method as defined in claim 18, wherein the electrophoresis medium (22) is a perfluorinated hydrocarbon liquid.
23. An image display method as defined in claim 18, further characterized by:
(a) applying a transparent first electrode (18) to the inward surface of the front sheet (12);
(b) applying a second electrode (20) to the inward surface of the rear sheet (14);
wherein applying the voltage is further characterized by applying the voltage between the first and second electrodes (18, 20).
(a) applying a transparent first electrode (18) to the inward surface of the front sheet (12);
(b) applying a second electrode (20) to the inward surface of the rear sheet (14);
wherein applying the voltage is further characterized by applying the voltage between the first and second electrodes (18, 20).
24. An image display method as defined in claim 23, further characterized by dividing the second electrode (20) into a plurality of electrode segments, wherein applying the voltage further comprises applying the voltage between the first electrode (18) and a selected one of the electrode segments to establish an electric field distinct from any electric field established by applying the voltage between the first electrode (18) and any of the electrode segments other than the selected segment.
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US10/625,805 | 2003-07-24 | ||
| US10/625,805 US6865011B2 (en) | 2002-07-30 | 2003-07-24 | Self-stabilized electrophoretically frustrated total internal reflection display |
| PCT/CA2003/001927 WO2005010604A1 (en) | 2003-07-24 | 2003-12-10 | Self-stabilized electrophoretically frustrated total internal reflection display |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2529719A1 true CA2529719A1 (en) | 2005-02-03 |
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ID=34103232
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002529719A Abandoned CA2529719A1 (en) | 2003-07-24 | 2003-12-10 | Self-stabilized electrophoretically frustrated total internal reflection display |
Country Status (8)
| Country | Link |
|---|---|
| US (1) | US6865011B2 (en) |
| EP (1) | EP1660936A1 (en) |
| JP (1) | JP2007505330A (en) |
| KR (1) | KR100722648B1 (en) |
| CN (1) | CN100363832C (en) |
| AU (1) | AU2003294518A1 (en) |
| CA (1) | CA2529719A1 (en) |
| WO (1) | WO2005010604A1 (en) |
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-
2003
- 2003-07-24 US US10/625,805 patent/US6865011B2/en not_active Expired - Lifetime
- 2003-12-10 CN CNB2003801103876A patent/CN100363832C/en not_active Expired - Fee Related
- 2003-12-10 JP JP2005504510A patent/JP2007505330A/en active Pending
- 2003-12-10 CA CA002529719A patent/CA2529719A1/en not_active Abandoned
- 2003-12-10 EP EP03785411A patent/EP1660936A1/en not_active Withdrawn
- 2003-12-10 WO PCT/CA2003/001927 patent/WO2005010604A1/en active Application Filing
- 2003-12-10 KR KR1020067001106A patent/KR100722648B1/en not_active IP Right Cessation
- 2003-12-10 AU AU2003294518A patent/AU2003294518A1/en not_active Abandoned
Also Published As
| Publication number | Publication date |
|---|---|
| JP2007505330A (en) | 2007-03-08 |
| US20040136047A1 (en) | 2004-07-15 |
| WO2005010604A1 (en) | 2005-02-03 |
| CN100363832C (en) | 2008-01-23 |
| EP1660936A1 (en) | 2006-05-31 |
| US6865011B2 (en) | 2005-03-08 |
| AU2003294518A1 (en) | 2005-02-14 |
| KR20060041243A (en) | 2006-05-11 |
| CN1820223A (en) | 2006-08-16 |
| KR100722648B1 (en) | 2007-05-28 |
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| Date | Code | Title | Description |
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| EEER | Examination request | ||
| FZDE | Discontinued |