Reflective edge field-emission pixel and associated display

Information

  • Patent Grant
  • 6693386
  • Patent Number
    6,693,386
  • Date Filed
    Friday, September 13, 2002
    22 years ago
  • Date Issued
    Tuesday, February 17, 2004
    20 years ago
Abstract
A Reflective Field Emission Display (FED) pixel element and system employing same are disclosed. In the FED system disclosed, each pixel element is composed of at least one emitter that is operable to emit electrons and at least one reflector that is operable to attract and reflect the emitted electrons onto a transparent anode layer that oppositely positioned with respect to the emitter and reflector and is operable to attract the reflected electrons. In one aspect of the invention, the emitter layer is shaped to bound the reflector layer forming an electrical boundary that focuses the reflected electron beam onto a phosphor layer interposed between the transparent layer. In another aspect of the invention, a high voltage and a corresponding high voltage phosphor is applied to the transparent anode layer. The use of high voltage and high voltage phosphor is advantageous as it causes the reflected electrons to be drawn deeper into the phosphor layer and, hence, reduces unwanted emissions back into the vacuum of the pixel element. In still another aspect of the invention, a plurality of phosphor layers are applied to the transparent layer to produce a color display as reflected electrons are attracted to the transparent layer.
Description




FIELD OF THE INVENTION




The present invention relates to solid-state displays and more specifically to edge-emitter reflective field emission pixel elements having shaped emitter elements for electron beam focusing for displays.




BACKGROUND OF THE INVENTION




Solid state and non-Cathode Ray Tube (CRT) display technologies are well-known in the art. Light Emitting Diode (LED) displays, for example, include semiconductor diode elements that may be arranged in configurations to display alphanumeric characters. Alphanumeric characters are then displayed by applying a potential or voltage to specific elements within the configuration. Liquid Crystal Displays (LCD) are composed of a liquid crystal material sandwiched between two sheets of a polarizing material. When a voltage is applied to the sandwiched materials, the liquid crystal material aligns in a manner to pass or block light. Plasma displays conventionally use a neon/xenon gas mixture housed between sealed glass plates that have parallel electrodes deposited on the surface.




Passive matrix displays and active matrix displays are flat panel displays that are used extensively in laptop and notebook computers. In a passive matrix display, there is a matrix or grid of solid-state elements in which each element or pixel is selected by applying a potential to a corresponding row and column line that forms the matrix or grid. In an active matrix display, each pixel is further controlled by at least one transistor and a capacitor that is also selected by applying a potential to a corresponding row and column line. Active matrix displays provide better resolution than passive matrix displays, but they are considerably more expensive to produce.




While each of these display technologies has advantages, such as low power and lightweight, they also have characteristics that make them unsuitable for many other types of applications. Passive matrix displays have limited resolution, while active matrix displays are expensive to manufacture.




The edge emitter FED pixel element disclosed in U.S. patent application Ser. No. 10/102,450, entitled “Field-Emission Matrix Display Based on Electron Reflection,” is representative of a pixel element that may be included in a low-cost, lightweight, high-resolution display system. In such a display, a high screen brightness with a minimum power consumption is advantageous. One method for achieving a high screen brightness is to concentrate the reflected electron beam onto an associated phosphor layer with little or no scattering, or cross-talk, of the electron beam from one pixel element into adjacent pixel elements, or as will be appreciated, an adjacent sub-pixel element.




Hence, there is a need for a method of concentrating or focusing the electron beam of edge-emitter FED pixel elements onto associated phosphor layers to substantially reduce electron beam cross-talk between adjacent elements.




SUMMARY OF THE INVENTION




An edge-emitter Field Emission Display (FED) pixel element and associated matrix display is disclosed. The FED pixel element has a reflector layer and an anode layer having a phosphor layer thereon, and a shaped emitter layer, which bounds a reflector layer and focuses a reflected electron beam to avoid scattering of the electron beam as it travels to the anode. Also disclosed is the use of high-voltage and high-voltage phosphor on the anode layer that advantageously improves the pixel element's operational life. Also disclosed, is a method of determining the voltage on the anode layer to enhance the focusing of the electron beam based on the distance between the anode and the reflecting surface. In another aspect of the invention, a plurality of phosphor layers are applied to the transparent layer, which produce different levels of color as reflected electrons are attracted to the transparent layer and bombard corresponding phosphor layers.











BRIEF DESCRIPTION OF THE DRAWINGS




In the drawings:





FIGS. 1



a


-


1




e


illustrate cross-sectional views of different embodiments of Field-Emission Display (FED) pixel element in accordance with the principles of the invention;





FIGS. 2



a


-


2




b


illustrate a top view of the shaped-emitter pixel element in accordance with the principles of the invention;





FIG. 3

illustrates a top view of the second embodiment of a shaped-emitter pixel element in accordance with the principles of the invention;





FIGS. 4



a


and


4




b


illustrate top views of shaped-emitter pixel elements for color pixel elements in accordance with the principles of the invention;





FIG. 5

illustrates a cross sectional view of a color pixel element in accordance with the principles of the present invention; and





FIG. 6

illustrates a graph of line current versus reflector layer voltage for a pixel element fabricated in accordance with the principles of the invention.











It is to be understood that these drawings are solely for purposes of illustrating the concepts of the invention and are not intended as a definition of the limits of the invention. It will be appreciated that the same reference numerals, possibly supplemented with reference characters where appropriate, have been used throughout to identify corresponding parts.




DETAILED DESCRIPTION OF THE INVENTION





FIG. 1



a


illustrates a cross-sectional view of an edge-emitter Field Emission Display (FED) pixel element


100


in accordance with the principles of the invention. In this exemplary embodiment, pixel element


100


is fabricated by depositing at least one reflective layer


110


on a dielectric or non-conductive substrate


120


, e.g. glass, silicon dioxide (SiO2). Reflective layer


110


is representative of an electrode that may also be used to control a voltage or potential applied to pixel elements


100


that are arranged in a row or column, which are oriented orthogonal to the plane of

FIG. 1



a


, as will more fully be explained. Reflective electrode


110


may be any material possessing a high electrical conductivity and reflectivity selected from a group of metals, such as, gold, silver, aluminum, vanadium, niobium, chromium, molybdenum, etc. In a preferred embodiment, reflective layer


110


is formed from niobium.




Insulator layer


130


, preferably silicon dioxide, SiO


2


, is next deposited on reflective layer


110


. Insulator layer


130


electrically isolates reflective layer


110


and is preferably in the range of about 0.5 microns thick. Emitter layer


140


is next deposited on insulating layer


130


. Emitter layer


140


is of a material that is operative to emit electrons when a sufficient potential difference exists between reflective layer


110


and emitter layer


140


. Emitter layer


140


is preferably selected from materials that emit electrons from an edge


142


when a potential difference exists between reflector layer


110


and emitter layer


140


. In the illustrated, and preferred, embodiment, emitter layer


140


is comprised preferably of a bottom conductive layer


150


and an edge emitter layer


170


having emitter edge


142


. Emitter edge layer or cathode layer


170


is composed of a material having a low-work function for emitting electrons. Emitter edge layer


170


may be a resistive material. In a preferred embodiment emitter edge layer


170


is an alpha-carbon (α-C) material formed as an edge in the range of 50-80 nanometers-thick. Alpha-carbon film is well known to have a low work function for electron emission into a vacuum. Conductive layer


150


is representative of an electrically conductive material that provides an electrical contact to the edge emitter layer


170


and may be used as a column or row connector in a FED display, as will be further explained.




Pixel well


145


is next created by etching, for example using photo-resistant patterning, through emitter layer


140


and insulator film layer


130


to expose reflector layer


110


. Emitter layer


140


is etched or shaped such that it borders on all sides, i.e., circumjacent, exposed reflector layer


110


. Photo-resistant patterning is well known in the art and need not be discussed in detail herein. Pixel


100


preferably is in the order of 300×300 microns.




As will be appreciated, the exposed width of reflector layer


110


may be determined by appropriately timing the etching of insulating layer


130


. Hence, in one aspect, emitter layer


140


, and more specifically, edge


142


and reflective layer


110


may be aligned and non-overlapping, i.e., self-aligned. In another aspect, emitter layer


140


, and more specifically, edge


142


may overlap reflective layer


110


, as shown.




A transparent electrode, preferably an Indium Titanium Oxide (ITO)


180


is deposited on transparent plate


190


, e.g., glass. ITO layer


180


is an optically transparent conductive material that may be used to provide a known potential in selective areas of ITO


180


.




Phosphor layer


195


is then deposited on ITO


180


. Phosphor layer


195


produces a predetermined or desired level of photonic activity or illumination when activated or bombarded by impinging electrons. In a preferred aspect, phosphor layer is deposited such that it is opposite a corresponding pixel well


145


.




Although not shown, it would be appreciated that a dielectric material, such as SiO


2


, may be selectively placed as spacers to electrically separate transparent substrate


190


and emitter layer


140


.




The confined pixel volume contained between pixel well


145


and transparent surface


190


is further evacuated to a pressure in the range of, 10


−5


to 10


−7


, and preferably, 10


−6


torr. Methods for evacuating the gases within a sealed pixel element are well known in the art and need not be discussed in detail.




In the operation of pixel element


100


, the application of a positive voltage or potential to reflective layer


110


relative to emitter layer


140


creates an electrical field that draws electrons from edge


142


of emitter layer


140


to reflective layer


110


. Electrons reflected from reflective layer


110


are then attracted to a positive voltage applied to ITO layer


180


, which in turn bombard phosphor layer


195


. It will be appreciated that emitter layer


140


and reflective layer


110


may be held at a known potential difference with is not sufficient to cause the emission of electrons from emitter layer


140


. An additional voltage, in the form of a pulse, may then be applied to reflective layer


110


to create a potential difference sufficient for emitter layer


140


to emit electrons.




As will be appreciated, the gap between the edge


142


and reflector layer


110


can be made extremely small, preferably less than or equal to one (1) micron. In this case, the voltage or potential difference between edge


142


and reflector layer


110


can be reduced to a level between 20 and 200 volts. In a preferred embodiment, the potential between emitter layer


140


and reflector layer


110


is in the order of 25-50 volts. The potential of the combined phosphor


195


/ITO layer


180


may be kept at a significantly higher voltage to attract reflected electrons to a corresponding phosphor layer to illuminate substantially the entire phosphor layer corresponding the pixel element without reflected electrons being spread into an adjacent pixel element phosphor layer.





FIG. 1



b


illustrates a second embodiment


200


of the invention in which emitter layer


140


is represented as layer


210


. In this embodiment, layer


210


is made of a conductive material suitable for emitting electrons from edge


215


when a potential difference exists between reflector layer


110


and emitter layer


210


. In this embodiment, layer


210


may be an electrically conductive material such as gold, silver, aluminum, molybdenum, etc. Preferably, layer


210


is fabricated from molybdenum.





FIG. 1



c


illustrates a third embodiment


300


of the present invention in which emitter layer


140


includes layer


210


and insulating layer


310


, such as SiO


2


, deposited on layer


210


.





FIG. 1



d


illustrates a fourth embodiment


400


of the present invention in which emitter layer


140


is composed of a resistive material


410


, such as alpha-silicon (α-Si), imposed between conductive layer


150


and edge emitter layer


170


, of

FIG. 1



a.







FIG. 1



e


illustrates a fifth embodiment


500


of the present invention, in which insulating layer


510


is deposited on edge emitter layer


170


shown in

FIG. 1



d


. Although not shown it will be appreciated that edge emitter layer


170


may be replaced by materials similar to those selected for edge emitter layer


210


.





FIG. 2



a


illustrates a top view of a shaped-emitter, non-self-aligned, pixel element


600


in accordance with the principles of the invention. In this aspect, the edges


142


of emitter layer


140


extend over reflective layer


110


, as represented by dashed lines


605


. Emitter layer


140


is further shaped such that edges


142


form a perimeter, vertically offset from, around the reflective surface of reflector layer


110


. In this aspect, the reflective surface is substantially contained within the perimeter boundary determined by the edges


142


. A potential or voltage applied to emitter layer


140


, thus, creates an electrical barrier that restrains, or confines, the direction of electrons reflected from reflector layer


110


to remain within the bounds of edges


142


. Restraint or containment of the reflected electron beam substantially within the bounds of edges


142


is advantageous as it limits the spread of the electron beam and reduces cross-talk between pixel element or sub-pixel elements in color displays, as will be shown.




Further illustrated is that emitter layer


140


may be in electrical communication with similar pixel elements (not shown) by at least one column row line


610


and reflective layer


110


may be in electrical communication with similar pixel elements (not shown) by row lines


620


. As is known in the art, pixel element


100


may be identified or addressed in a display unit composed of a matrix of similar pixel elements by its row identifier and its column identifier. Pixel element


600


may also be identified by a plurality of emitter layer


140


connected in rows and reflector layers


110


connected in columns, as is well-known.





FIG. 2



b


illustrates a cross-sectional view through section A—A of the pixel element


600


shown in

FIG. 2



a


, showing paths of electrons reflected from reflector layer


110


. In this case, electrons


635


emitted from emitter layer


140


are attracted to, and reflected from, reflector layer


110


. The path of electrons reflected from reflector layer


110


at an initial angle substantially different than 90 degrees, as illustrated by angle


640


, may be directed or deflected by the potential difference between the reflected electron and the potential or voltage applied to emitter layer


140


to a substantially perpendicular direction of travel to ITO layer


180


. Hence, electrons


635


may be substantially maintained within the bounds of emitter layer


140


and as fewer electrons


635


penetrate the electrical barrier created by shaped-emitter layer


140


less interference with adjacent phosphor layers occurs and more electrons strike the desired phosphor layer


195


.




Also illustrated are spacers


630


, which provide electrical separation of the electrically conductive ITO layer


180


and emitter layer


140


. Spacers


630


are conventionally fabricated from a dielectric material, such as SiO


2


, and further provide mechanical support to transparent layer


190


when the volume between transparent layer


190


and pixel well


145


is evacuated to create a vacuum therein.




Although not shown, it would be appreciated that a cross-section view through section B—B of

FIG. 2



a


would provide a similar deflection of reflected electrons. Hence, reflected electrons are restrained in both a lateral and orthogonal direction.





FIG. 3

illustrates a top view of a second aspect of the shaped emitter layer


140


in accordance with the principles of the invention. In this aspect, emitter layer


140


is further shaped to contain a plurality of digits or projections that extend over reflective surface of reflector layer


110


. This addition of digits or projections to shaped-emitter layer


140


is advantageous as it increases the length of edge


142


, which increases the number of emitted electrons. Also, the increased edge length creates additional electrical barriers that further restrain electrons from exiting the pixel region.





FIG. 4



a


illustrates a top view of another embodiment


700


of a color FED pixel element in accordance with the principles of the present invention. In this embodiment, pixel


700


is partitioned into three sub-pixel elements, represented as


710




a


,


710




b


,


710




c


, which may be associated with red, green and blue phosphor layers, i.e., RGB.




In a FED display system, each sub-pixel element is independently controlled by column lines


610




a


,


610




b


,


610




c


and row line


620


. Each sub-pixel emitter edge, represented as


142




a


,


142




b


,


142




c


, respectively, operates as previously described to prevent electrons emitted from a corresponding reflector layer


110




a


,


110




b


,


110




c


, to impinge upon the phosphor layers corresponding to an adjacent sub-pixel element phosphor layer. To maintain a desired 330×330 micron pixel size, each sub-pixel element


710




a


,


710




b


,


710




c


, is in the order of 330×110 microns.





FIG. 4



b


illustrates a cross-sectional view of embodiment shown in

FIG. 4



a


, which depicts the containment of electron beams,


635




a


,


635




b


,


635




c


, reflected from corresponding reflector layers


110




a


,


110




b


,


110




c


, as they are attracted to phosphor layers


755




a


,


755




b


,


755




c


. In a preferred embodiment phosphor layers


755




a


,


755




b


,


755




c


emit a light in a band corresponding to one of the primary colors, i.e., red, green, blue. As would be appreciated the selection of colors and the order of the color phosphor layers may be exchanged without altering the scope of the invention.





FIG. 5

illustrates a top-view of a preferred embodiment of a color FED pixel element using a shaped-emitter layer similar to that shown in FIG.


3


. As previously discussed, the increase of the length of the emitter layer


140


edge


142


is advantageous as it increases the number of electrons emitted.




Returning to

FIG. 2



b


, it will be understood, that the confinement of the electron path by shaped-emitter layer


140


is not exact and electrons


635


may continue toward ITO layer


180


on a path that may not be substantially perpendicular to reflector layer


110


. Hence, electron beam paths may cross before reaching the corresponding phosphor layer. One factor where electron beams may cross is the voltage or potential applied to ITO layer


180


as this voltage determines the level of attraction of electrons to ITO layer


180


. Thus, the electrons beam may be focused to a point between ITO layer


180


and reflector layer


110


. Hence, to have a maximum number of electrons strike a corresponding phosphor layer, ITO layer


180


may be positioned approximately at the electron focal point. Table 1 tabulates voltage or values on ITO layer


180


with regard to a distance between ITO layer


180


and reflector layer


110


that achieve reasonable focus with sufficient illumination of the corresponding phosphor layer.












TABLE 1











Applied ITO Voltage v. Distance














Preferred Voltage Range




Maximum Voltage






Distance




(volts)




(volts)









 200 microns




600-800




1000






 600 microns




2000-3000




4000






1100 microns




6000-7000




9000














Accordingly, for a desired distance between ITO layer


190


and reflector layer


110


, the voltage on ITO layer


190


may be selected to achieve a desired level of focus or image sharpness. As the distance between emitter layer


140


and reflector layer


110


is typically in the order of 1-2 microns, there is a negligible difference in the distance between emitter layer


140


and ITO layer


190


.




The relatively high voltage on ITO layer


180


requires high-voltage phosphor, similar to that used on Cathode Ray Tubes (CRT), rather than the low-voltage phosphor used in current solid-state display technology. The high voltage and high-voltage phosphor is advantageous as it enables the electrons to penetrate deeper into the phosphor layer and reduces the emission of impurities into the evacuated FED pixel element, which occurs when electrons bombard the phosphor. High-voltage phosphor having low sulfur content is preferred.




As would be understood by those skilled in the art, a sold-state flat panel display using reflected electron FED pixel elements disclosed herein may be formed by arranging a plurality of reflective edge pixel elements


100


, wherein emitter layers


140


are electrically connected in rows and reflector layer


110


are electrically connected in columns. The pixel elements may be formed on a single dielectric surface having spacers positioned thereon to establish a desired distance between pixel elements and transparent layer


190


. The spacers further provide mechanical support when the space between the pixel elements and the transparent surface


190


is evacuated and a vacuum is contained therein.




Pixel elements may then be selected to produce an image viewable through transparent layer


190


by the application of voltages to selected rows and columns. Control of selected rows and columns may be performed by any means, for example, a processor, through appropriate row controller circuitry and column controller circuitry. As will be appreciated, a processor may be any means, such as a general purpose or special purpose computing system, or may be a hardware configuration, such as a dedicated logic circuit, integrated circuit, Programmable Array Logic, Application Specific Integrated circuit or any device that provides known voltage outputs on corresponding row and column lines in response to known inputs.





FIG. 6

illustrates a graph


810


of measured line currents for two selected lines of a display constructed having 160 rows and 170 columns (160×170) of reflective pixel elements in accordance with the principles of the invention having 3 kv applied to ITO layer


180


. In this illustrated example of measured currents, as the reflector layer


110


voltage, represented as · V


R


, above a known threshold voltage increases, the current drawn by emitter layers of the pixel elements in the selected row,


820




a


,


820




b


, referred to as I


e


, is shown to increase non-linearly, but substantially consistently. Similarly, the reflected current,


830




a


,


830




b


, referred to as I


a


is only a portion of the emitter current.




In this specific embodiment, the threshold voltage is 90 volts. However, it would be appreciated that the threshold voltage for electron flow depends on the material selected for emitter layer


140


. Hence, although the characteristics of the present invention is presented with regard to an alpha-carbon material, it would be known by those skilled in the art to substitute a metal, for example, as emitter layer


140


and adjust the threshold voltage accordingly.




Efficiency of the display may be determined as the power provided to the anode or ITO layer


180


and the power necessary to drive the display: Accordingly efficiency may be determined as:






η
=



I
a



V
a





I
a



V
a


+


I
e



V
r














Although I


e


is larger than I


a


, the efficiency remains significantly high as the value of V


r


is significantly lower than V


a


.




The brightness of the FED display may be determined as






B
=


η






I
a



V
a



π





A












where A is the area of the spot size on phosphor layer


195


.




While there has been shown, described, and pointed out, fundamental novel features of the present invention as applied to preferred embodiments thereof, it will be understood that various omissions and substitutions and changes in the apparatus described, in the form and details of the devices disclosed, and in their operation, may be made by those skilled in the art without departing from the spirit of the present invention. For example, it is expressly intended that all combinations of those elements which perform substantially the same function in substantially the same way to achieve the same results are within the scope of the invention. Substitutions of elements from one described embodiment to another are also fully intended and contemplated.



Claims
  • 1. A reflective emission pixel element comprising:a substrate layer; at least one reflector layer; at least one emitter layer, electrically isolated and positioned above a corresponding one of said at least one reflector layer, said at least one emitter layer to circumjacent said at least one reflector layer; means for applying a first potential to said at least one reflector layer, wherein a potential difference between said at least one emitter layer and said corresponding one of said at least one reflector layer is operable to draw electrons from said at least one emitter layer to said corresponding one of said reflector layer; a transparent layer oppositely positioned a predetermined distance from said at least one emitter layer, said transparent layer having a conductive layer deposited thereon; means for applying a second potential to said conductive layer to attract electrons reflected from said at least one reflective layer; at least one phosphor layer on said conductive layer oppositely opposed to said corresponding one of said at least one reflector layer.
  • 2. The pixel element as recited in claim 1, further comprising:a vacuum created between said substrate layer and said transparent layer.
  • 3. The pixel element as recited in claim 1, wherein said at least one emitter layer is selected from a group comprising: chromium, niobium, vanadium, aluminum, molybdenum, gold, silver, copper.
  • 4. The pixel element as recited in claim 1, wherein said at least one reflector layer is selected from a group comprising: aluminum, chromium, niobium, vanadium, gold, silver, copper.
  • 5. The pixel element as recited in claim 1, wherein said at least one emitter layer further comprising:a conductive layer; and an emitter edge layer in electrical contact with said conductive layer.
  • 6. The pixel element as recited in claim 5, wherein said emitter edge layer is an alpha-carbon material.
  • 7. The pixel element as recited in claim 5, further comprising:a resistive material imposed between said conductive layer and said edge emitter layer.
  • 8. The pixel element as recited in claim 7, wherein said resistive material is an alpha-silicon material.
  • 9. The pixel element as recited in claim 5, further comprising:means for selectively applying a third potential to said conductive layer, wherein said third potential is more negative than said first potential.
  • 10. The pixel element as recited in claim 5, further comprising:a dielectric material deposited on said emitter edge layer.
  • 11. The pixel element as recited in claim 1, wherein said at least one phosphor layer is a high-voltage phosphor.
  • 12. The pixel element as recited in claim 11, wherein said at least one phosphor layer is selected from a group comprising: red, green, blue.
  • 13. The pixel element as recited in claim 1, wherein said at least one emitter layer is distributed within said pixel element.
  • 14. The pixel element as recited in claim 1, wherein said at least one emitter layer extends over said at least one reflector layer.
  • 15. The pixel element as recited in claim 1, wherein said at least one emitter layer is partitioned into a plurality of digits extending over the corresponding one of said reflector layer.
  • 16. The pixel element as recited in claim 1, wherein said second potential is selectively applied to selected areas of said transparent electrode layer.
  • 17. The pixel element as recited in claim 1, wherein said first potential includes a known constant potential and a potential applied as a pulse.
  • 18. The pixel element as recited in claim 1, further comprising:means for selectively applying a third potential to said at least one emitter layer, wherein said third potential is more negative than said first potential.
  • 19. The pixel element as recited in claim 18 wherein a difference between said first potential and said third potential exceeds a known threshold value.
  • 20. The pixel element as recited in claim 1, further comprising:a connectivity layer associated with each of said at least one reflective layer, said connectivity layer positioned between said at least one reflective layer and said substrate layer.
  • 21. The pixel element as recited in claim 20, wherein said second potential is determined to achieve a desired level of image sharpness.
  • 22. The pixel element as recited in claim 1, wherein said second potential is determined based on said predetermined distance.
  • 23. A reflective edge Field Emission Display (FED) comprising:a substrate layer having fabricated thereon a plurality of reflective pixel elements arranged in a matrix of rows and columns thereon, each of said pixel elements identified by a row and a column designation comprising: at least one reflector layer deposited on said substrate; and an emitter layer electrically isolated from and having an edge operable to emit electrons therefrom shaped to bound a corresponding one of said at least one reflector layer; a transparent layer electrically isolated from said substrate layer, having deposited thereon: at least one conductive layer; and a phosphor layer associated with each of said at least one conductive layer, wherein said phosphor layer is oppositely opposed to a corresponding one of said at least one reflector layer; at least one non-conductive spacer selectively positioned between said substrate layer and said transparent layer to maintain a substantially desired distance between said substrate layer and said transparent layer; and a seal between said substrate layer and said transparent layer operative to sustain a vacuum therebetween.
  • 24. The FED as recited in claim 23, wherein said pixel element emitter layers are electrically connected in said rows and said reflector layers are electrically connected in said columns.
  • 25. The FED as recited in claim 23, wherein said pixel element emitter layers are electrically connected in said columns and said reflector layers are electrically connected said rows.
  • 26. The FED as recited in claim 23, further comprising:means for applying a first potential to each of said at least one reflector layer; means for applying a second potential, determined in relation to said distance, to each of said at least one conductive layer; means for applying a third potential to each of said emitter layers, wherein a potential difference between said first potential and said third potential is operable to attract electrons emitted by an associated emitter layer.
  • 27. The FED as recited in claim 26, wherein said potential difference is a range of 10-200 volts.
  • 28. The FED as recited in claim 26, wherein said first potential is in a range of 0-100 volts greater than a threshold potential.
  • 29. The FED as recited in claim 28, wherein said threshold potential is determined based on said emitter layer material.
  • 30. The FED as recited in claim 26, wherein said first potential comprises a constant potential and a potential applied as pulse.
  • 31. The FED as recited in claim 26, wherein said second potential is in a range of 1000-9000 volts.
  • 32. The FED as recited in claim 23, wherein said conductive layer is partitioned into a plurality of electrically isolated stripes.
  • 33. The FED as recited in claim 23, wherein said phosphor layer is a high-voltage phosphor.
  • 34. The FED as recited in claim 23, wherein said phosphor layer has a minimum amount of sulfur content.
  • 35. The FED as recited in claim 23, wherein said at least one reflector layer is selected from a group comprising gold, silver, aluminum, copper, chromium, niobium, vanadium, molybdenum.
  • 36. The FED as recited in claim 23, wherein said at least one reflector layer is niobium.
  • 37. The FED as recited in claim 23, wherein said emitter layer is selected from a group comprising gold, silver, aluminum, copper, chromium, niobium, vanadium, molybdenum.
  • 38. The FED as recited in claim 23, wherein said emitter layer is molybdenum.
  • 39. The FED as recited in claim 23, wherein said pixel element further comprises:a second conductive layer imposed between said emitter layer and said substrate, said second conductive layer being in electrical contact with said emitter layer and electrically isolated from said at least one reflector layer.
  • 40. The FED as recited in claim 39, wherein said emitter layer is a resistive material.
  • 41. The FED as recited in claim 40, wherein said emitter layer is an alpha-carbon.
  • 42. The FED as recited in claim 23, wherein said pixel element further comprises:a resistive material imposed between said second conductive layer and said emitter layer.
  • 43. The FED as recited in claim 42, wherein said resistive material is an alpha-silicon.
  • 44. The FED as recited in claim 23, wherein said pixel element further comprises:an insulating layer deposited on said emitter layer.
  • 45. The FED as recited in claim 23, wherein said emitter layer shape is selected from a group comprising: square, rectangle, circle, triangle.
  • 46. The FED as recited in claim 23, wherein a light color emitted by said phosphor layer is selected from a group comprising: red, blue, green.
  • 47. The FED as recited in claim 23, wherein said emitter layer edge is aligned to an edge of a corresponding one of said at least one reflector layer.
  • 48. The FED as recited in claim 23, wherein said emitter layer edge extends over a corresponding one of said at least one reflector layer.
  • 49. The FED as recited in claim 23, wherein said emitter layer is partitioned into a plurality of digits.
  • 50. The FED as recited in claim 23, wherein said emitter layer digits extend over a corresponding one of said at least one reflector layer.
  • 51. The FED as recited in claim 23, wherein said vacuum is in the range of 10−5 to 10−7 torr.
PRIORITY FILING DATE

This application claims the benefit of the earlier filing date, under 35 U.S.C. §119, of U.S. Provisional Patent Applications; Serial No. 60/403,938, entitled “Configuration of Edge Emitter Display,” filed on Aug. 16, 2002; and Serial No. 60/399,825, entitled “Reflective Edge Emitter FED with Shaped Emitter Layer,” filed on Jul. 31, 2002, the entirety of which are incorporated by reference herein. This application is a continuation-in-part of commonly assigned, co-pending, patent application: Ser. No. 10/102,450, entitled “Field-Emission Matrix Display Based on Electron Reflection,” filed on Mar. 20, 2002, the entirety of which is incorporated by reference herein.

US Referenced Citations (4)
Number Name Date Kind
5620832 Sung et al. Apr 1997 A
6032126 Kaehler Feb 2000 A
6329750 Hofmann et al. Dec 2001 B1
6614149 Kastalsky et al. Sep 2003 B2
Provisional Applications (2)
Number Date Country
60/403938 Aug 2002 US
60/399825 Jul 2002 US
Continuation in Parts (1)
Number Date Country
Parent 10/102450 Mar 2002 US
Child 10/243894 US