Focusing electrode for field emission displays and method

Information

  • Patent Grant
  • 6489726
  • Patent Number
    6,489,726
  • Date Filed
    Monday, August 20, 2001
    23 years ago
  • Date Issued
    Tuesday, December 3, 2002
    22 years ago
Abstract
A display includes a substrate and an emitter formed on the substrate. A first dielectric layer is formed on the substrate to have a thickness slightly less than a height of the emitter above the planar surface and includes an opening formed about the emitter. The display also includes a conductive extraction grid formed on the first dielectric layer. The extraction grid includes an opening surrounding the emitter. The display further includes a second dielectric layer formed on the extraction grid and a focusing electrode formed on the second dielectric layer. The focusing electrode is electrically coupled to the emitter through an impedance element. The focusing electrode includes an opening formed above the apex. The focusing electrode provides enhanced focusing performance together with reduced circuit complexity, resulting in a superior display.
Description




TECHNICAL FIELD




This invention relates in general to visual displays for electronic devices and in particular to improved focusing electrodes and techniques for field emission displays.




BACKGROUND OF THE INVENTION





FIG. 1

is a simplified side cross-sectional view of a portion of a field emission display


10


including a faceplate


20


and a baseplate


21


in accordance with the prior art.

FIG. 1

is not drawn to scale. The faceplate


20


includes a transparent viewing screen


22


, a transparent conductive layer


24


and a cathodoluminescent layer


26


. The transparent viewing screen


22


supports the layers


24


and


26


, acts as a viewing surface and as a wall for a hermetically sealed package formed between the viewing screen


22


and the baseplate


21


. The viewing screen


22


may be formed from glass. The transparent conductive layer


24


may be formed from indium tin oxide. The cathodoluminescent layer


26


may be segmented into localized portions. In a conventional monochrome display


10


, each localized portion of the cathodoluminescent layer


26


forms one pixel of the monochrome display


10


. Also, in a conventional color display


10


, each localized portion of the cathodoluminescent layer


26


forms a green, red or blue sub-pixel of the color display


10


. Materials useful as cathodoluminescent materials in the cathodoluminescent layer


26


include Y


2


O


3


:Eu (red, phosphor P-56), Y


3


(Al, Ga)


5


O


12


:Tb (green, phosphor P-53) and Y


2


(SiO


5


):Ce (blue, phosphor P-47) available from Osram Sylvania of Towanda PA or from Nichia of Japan.




The baseplate


21


includes emitters


30


formed on a planar surface of a substrate


32


that is preferably a semiconductor material such as silicon. The substrate


32


is coated with a dielectric layer


34


. In one embodiment, this is effected by deposition of silicon dioxide via a conventional TEOS process. The dielectric layer


34


is formed to have a thickness that is approximately equal to or just less than a height of the emitters


30


. This thickness is on the order of 0.4 microns, although greater or lesser thicknesses may be employed. A conductive extraction grid


38


is formed on the dielectric layer


34


. The extraction grid


38


may be formed, for example, as a thin layer of polysilicon. An opening


40


is created in the extraction grid


38


having a radius that is also approximately the separation of the extraction grid


38


from the tip of the emitter


30


. The radius of the opening


40


may be about 0.4 microns, although larger or smaller openings


40


may also be employed.




In operation, the extraction grid


38


is biased to a voltage on the order of 100 volts, although higher or lower voltages may be used, while the substrate


32


is maintained at a voltage of about zero volts. Signals coupled to the emitters


30


allow electrons to flow to the emitter


30


. Intense electrical fields between the emitter


30


and the extraction grid


38


cause emission of electrons from the emitter


30


.




A larger positive voltage, ranging up to as much as 5,000 volts or more but usually 2,500 volts or less, is applied to the faceplate


20


via the transparent conductive layer


24


. The electrons emitted from the emitter


30


are accelerated to the faceplate


20


by this voltage and strike the cathodoluminescent layer


26


. This causes light emission in selected areas, i.e., those areas opposite the emitters


30


, and forms luminous images such as text, pictures and the like.




Electrons emitted from each emitter


30


in a conventional field emission display


10


tend to spread out as the electrons travel from the emitter


30


to the cathodoluminescent layer


26


on the faceplate


20


. If the electron emission spreads out too far, it will impact on more than one localized portion of the cathodoluminescent layer


26


of the field emission display


10


. This phenomenon is known as “bleedover.” The likelihood that bleedover may occur is exacerbated by any misalignment between the localized portions of the cathodoluminescent layer


26


and their associated sets of emitters


30


.




When the electron emission from an emitter


30


associated with a first localized portion of the cathodoluminescent layer


26


also impacts on a second localized portion of the cathodoluminescent layer


26


, both the first and second localized portions of the cathodoluminescent layer


26


emit light. As a result, the first pixel or sub-pixel uniquely associated with the first localized portion of the cathodoluminescent layer


26


correctly turns on, and a second pixel or sub-pixel uniquely associated with the second localized portion of the cathodoluminescent layer


26


incorrectly turns on. In a color field emission display


10


, this can cause purple light to be emitted from a blue sub-pixel and a red sub-pixel together when only red light from the red sub-pixel was desired. As a result, a degraded image is formed on the faceplate


20


of the field emission display


10


.




In a monochrome field emission display


10


, color distortion does not occur, but the resolution of the image formed on the faceplate


20


is reduced by bleedover. In conventional field emission displays


10


, bleedover is alleviated in several ways. A relatively high anode voltage V


a


may be applied to the transparent conductive layer


24


of the conventional field emission display


10


, so that the electrons emitted from the emitters


30


are strongly accelerated to the faceplate


20


. As a result, the electron emissions spread out less as they travel from the emitters


30


to the faceplate


20


. A relatively small gap between the faceplate


20


and the baseplate


21


may be used, again reducing opportunity for spreading of the emitted electrons. However, it has been found that these are impractical solutions because too high a voltage applied between the transparent conductive layer


24


and the baseplate


21


, or too small a gap between the faceplate


20


and the baseplate


21


may cause arcing.




Another way in which bleedover is reduced in conventional field emission displays


10


is by spacing the localized portions of the cathodoluminescent layer


26


relatively far apart. This is possible because of the relatively low display resolution provided by conventional field emission displays


10


. As a result, the electron emissions impact on the correct localized portion of the cathodoluminescent layer


26


.




Another approach to controlling the spatial spread of electrons emitted from a group of the emitters


30


is to surround the area emitting the electrons with a focusing electrode (not illustrated in FIG.


1


). This allows increased control over the spatial distribution of the emitted electrons via control of the voltage applied to the focusing electrode, which in turn provides increased resolution for the resulting image. One such approach, where each focusing element serves many emitters, is described in U.S. Pat No. 5,528,103, entitled “Field Emitter With Focusing Ridges Situated To Sides Of Gate”, issued to Spindt et al.




There are several disadvantages to these prior art approaches. In most prior art approaches, the focusing electrode is biased by a voltage source that is independent of other bias voltage sources associated with the emitter


30


. As a result, the use of a focusing electrode generally requires another bias voltage source to bias the focusing electrode. This, in turn, leads to problems due to variations in turn on voltage from one emitter


30


to another when a single bias voltage is applied for several focusing electrodes. When a group of emitters


30


are all affected by a single focusing electrode, some of the emitters


30


may exhibit a turn on voltage that differs from that exhibited by other emitters


30


. The effect that the focusing electrode has on the electrons emitted from each of these emitters


30


will differ. Additionally, some of the current through the emitter


30


will be collected by the focusing electrode. This complicates the relationship between the emitter current and light emission because some of the current through the emitter


30


is diverted from the faceplate


20


by the focusing electrode. Further, the effects of the focusing electrode are different for emitters that are closer to the focusing electrode than for emitters


30


that are farther away from the focusing electrode. The lack of control over the amount of light emitted in response to a known emitter current results in poorer imaging characteristics for the display


10


.




The problem of bleedover is exacerbated by the trend to higher resolution field emission displays


10


. High resolution field emission displays use fewer emitters


30


per pixel or sub-pixel. This arises for several reasons, one of which is that a smaller pixel or sub-pixel subtends a smaller area in which the emitters


30


can be provided. As display engineers attempt to increase the display resolution of conventional field emission displays


10


, the localized portions of the cathodoluminescent layer


26


are necessarily crowded closer together. As a result, each emitter


30


in a high resolution field emission display makes a greater contribution to the pixel or sub-pixel associated with it. This increases the need to be able to control electron emissions and the spread of electron emissions from each emitter


30


.




An approach to focusing electrons emitted from the emitter


30


without requiring a separate bias voltage source to bias the focusing electrode is described in U.S. Pat. No. 5,191,217 , entitled “Method and Apparatus for Field Emission Device Electrostatic Electron Beam Focussing,” issued to Kane et al. This approach makes no provision for modifying the focus parameters in response to the amount of current through the emitter


30


.




There is, therefore, a need to provide more reliable control of the spatial distribution of the electrons delivered to the faceplate without causing other problems in field emission displays.




SUMMARY OF THE INVENTION




In accordance with one aspect of the invention, a field emission display includes a substrate, a plurality of emitters formed on the substrate, and a dielectric layer formed on the substrate having an opening formed about each of the emitters. The field emission display also includes a conductive extraction grid formed substantially in a plane of tips of the plurality of emitters. The extraction grid includes openings each formed about a tip of one of the emitters. In accordance with an aspect of the invention, a focusing electrode that physically confines emitted electrons provides enhanced focusing performance together with reduced circuit complexity compared to prior approaches. This, in turn, results in superior display performance, especially for high resolution field emission displays.




In another aspect of the invention, a focus electrode is formed on the substrate having an opening positioned above the emitter. An impedance element is electrically coupled between the focus electrode and the emitter. The impedance element allows a portion of those electrons that were emitted from the emitter and that were intercepted by the focus electrode to return to the emitter. The current flow through the impedance element produces a voltage that biases the focus electrode.











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

is a simplified side cross-sectional view of a portion of a field emission display according to the prior art.





FIG. 2

is a simplified side cross-sectional view of a portion of a field emission display including a focusing electrode according to an embodiment of the invention.





FIGS. 3A

,


3


B and


3


C are a simplified plan views of a portion of a field emission display including a focusing electrode according to embodiments of the invention.





FIG. 4

is a simplified schematic view of a field emission display and one emitter and focusing electrode biasing arrangement according to an embodiment of the invention.





FIG. 5

is a simplified schematic view of a field emission display and another emitter and focusing electrode biasing arrangement according to another embodiment of the invention.





FIG. 6

is a flow chart of a process for manufacturing a focusing electrode according to an embodiment of the present invention.





FIG. 7

is a simplified block diagram of a computer including a field emission display using the focusing electrode according to embodiments of the present invention.











DETAILED DESCRIPTION OF THE INVENTION





FIG. 2

is a simplified side cross-sectional view of a portion of a field emission display


11


including a focusing electrode


62


in accordance with one embodiment of the invention.

FIG. 2

is not drawn to scale. Many of the components used in the field emission display


11


shown in

FIG. 2

are identical to components used in the field emission display


10


of FIG.


1


. Therefore, in the interest of brevity, these components have been provided with the same reference numerals, and an explanation of them will not be repeated.




The pattern made by the emitted electrons when they strike the faceplate


20


is optimized by incorporating focusing electrodes


62


into the circuitry associated with the emitter


30


. This is particularly desirable for high resolution field emission displays


11


. The focusing electrodes


62


may be supported above the extraction grid


38


by a dielectric layer


64


as illustrated or may be placed in the plane of the extraction grid


38


(not illustrated).




Significantly, forming the opening in the focusing electrode


62


smaller than the diameter of the beam of electrons that would be emitted from the emitter


30


if the focusing electrode were not present causes the opening in the focusing electrode


62


to act as a pinhole. In other words, placing the focusing electrode


62


such that it physically confines the electrons emitted from the emitter


30


returns a portion of the emitted electrons to the emitter


30


. Under these circumstances, the shape of the electron distribution when the emitted electrons reach the faceplate


20


is determined more by the opening in the focusing electrode


62


than by the geometry of the tip of the emitter


30


. This allows a more uniform image to be displayed despite variations in the tips of the emitters


30


. This effect results from either making the diameter of the opening in the focusing electrode


62


small placing the focusing electrode


62


at a relatively large distance (e.g., up to five to ten microns) above the extraction grid


38


and the emitters


30


.




As shown in the simplified plan view of

FIG. 3A

, a field emission display


11


includes a focusing electrode


62


surrounding a three emitters


30


, grouped in a linear array. Three emitters


30


are shown in

FIG. 3A

for clarity of explanation and ease of illustration, however, it will be appreciated that more or fewer emitters


30


could be associated with a given focus electrode


62


, with one to ten emitters


30


being desirable, although more may be employed. The emitters


30


may be arranged in a single line, as shown in

FIG. 3A

, or may be configured in a double line as shown in

FIG. 3B

or may be staggered in a double line of emitters


30


as shown in

FIG. 3C

, or may be in some other configuration. In the embodiments shown in

FIGS. 3A through 3C

, the focusing electrode


62


is preferably spaced laterally (i.e., left to right in

FIGS. 3A through 3C

) from the emitters


30


by a micron or more. Edge or end effects are reduced if the ends (i.e., top and bottom) of the focusing electrode


62


are several microns away from those emitters


30


that are located at the ends of the groups of emitters


30


.




An advantage provided by a linear array of emitters


30


within an oblong focusing electrode


62


is that the focusing electrode


62


provides a more uniform effect on each of the emitters


30


compared to a focusing electrode surrounding a large group of emitters


30


because the emitters


30


in the group are at different distances from the focus electrode. A field emission display using a focusing electrode to surround a group of emitters is described, for example, in U.S. Pat. No. 5,528,103. The uniformity of the linear arrangements shown in

FIGS. 3A through 3C

renders the focusing electrodes


62


more effective.




A linear arrangement is preferred for several reasons. First, emitters in other arrangements may function differently depending upon their location. Furthermore, a focusing electrode optimized for one electrode may not be optimized for other emitters in the group. In contrast, the emitters


30


shown in

FIGS. 3A-3C

are all the same distance from a focusing electrode


62


and the focus influence thus should be similar for each of the emitters


30


.





FIG. 4

is a simplified schematic view of one embodiment of a field emission display


11


′ in accordance with the invention having the emitter


30


electrically coupled via an optional impedance


66


to the focusing electrode


62


. The focusing electrode


62


is formed above the extraction grid


38


as described above with reference to

FIG. 2. A

bias voltage is applied to the extraction grid


38


via a power supply


68


, and a bias voltage is supplied to the faceplate


20


via a power supply


70


. In this embodiment, the electrons supplied to the emitter


30


are modulated a current source


72


, such as a Field Effect Transistor (FET), or other similar devices.




By electrically coupling a focusing electrode


62


to the emitter


30


, several different objectives can be met while also simplifying the biasing arrangements for the emitter


30


and ancillary circuitry. One of these objectives is that the current coupled through the emitter


30


by the current source


72


is proportional to the current through the faceplate


20


because any electrons collected by the focusing electrode


62


are automatically resupplied to the emitter


30


through the optional impedance


66


. Many of the prior art arrangements for biasing focusing electrodes permit an undefined amount of the current carried by the emitters to be diverted via the focusing electrodes. This means that the luminosity of the pixel associated with the emitters


30


is not necessarily related to the current that was directed through the emitters


30


. Another of these objectives is that there is no need to adjust the bias voltage on the focusing electrode


62


to compensate for variations in the voltage on the emitter


30


. Further, there is no need for a separate bias voltage source for the focusing electrode


62


.





FIG. 5

is a simplified schematic view of another embodiment of a field emission display


11


″ in accordance with the invention. In the display


11


″electrons are supplied to the emitter


30


via a current-limiting element, such as a resistor


73


, that is electrically coupled between the emitter


30


and ground. In this approach, the current through the emitter


30


is ultimately set by a bias voltage applied to the extraction grid


38


. The arrangement of

FIG. 5

is used to permit each emitter


30


to be self-biasing and ensures that if one or more of the emitters


30


become short-circuited, e.g., to the extraction grid


38


, the entire pixel is not short-circuited, because the resistor


73


limits the current through any one emitter


30


.




In either of the embodiments


11


′ and


11


″ of

FIGS. 4 and 5

, the relationship between the current through the faceplate


20


and the emitter


30


current is simplified compared to the situation where an independent bias voltage source is used to set the voltage on a focusing electrode. In both embodiments


11


′ and


11


″, the focusing electrode


62


is electrically coupled to the emitter


30


via the optional impedance


66


. This arrangement ensures that the current through the controlled current source


72


is either directed to the extraction grid


38


or is directed through the opening


40


and is collected by the faceplate


20


. As a result, the focusing electrode


62


does not provide additional path whereby current flowing through the emitter


30


may be diverted. For the case where the optional impedance


66


is simply an interconnection, the effect of the focusing electrode


62


is readily modeled because the potential on the focusing electrode


62


is exactly the same as the potential on the emitter


30


.




When the optional impedance


66


comprises a current-limiting element, such as, for example, a high value resistor, the focusing electrode


62


becomes self-biasing because the electrons collected by the focusing electrode


62


bias the focusing electrode


62


negative with respect to the emitter


30


. As the voltage on the focusing electrode becomes more negative, it attracts fewer electrons, thus limiting the voltage on the focusing electrode


62


from becoming even more negative. The use of the impedance


66


does not impair the benefits of not requiring a separate focus power supply and of ensuring that the emitter current corresponds to the luminance. Additionally, a short circuit between the focusing electrode


62


and, for example, the extraction grid


38


(or other structures), need not completely prevent the emitter


30


from functioning, because the impedance


66


isolates the emitter


30


from the focusing electrode


62


to some degree.




It will be appreciated that current-limiting elements other than an impedance


66


may be employed, such as constant current elements (e.g., reverse-biased diodes or FETs having the source connected to the gate) or constant voltage elements (e.g., Zener diodes) and the like, to either provide a bias voltage on the focusing electrode


62


that is related to the emitter


30


current or that has a known relationship to the voltage present on the emitter


30


.




In the embodiments of

FIGS. 3 through 5

, the focusing achieved by the focusing electrode


62


is determined by the geometry and placement of the focusing electrode


62


with respect to the other structures, and especially the emitter


30


, forming the field emission display


11


,


11


′ or


11


″ . Both the lateral separation of the focusing electrode


62


from the tips of the emitters


30


, typically on the order of one or two micrometers, and the vertical separation of the focusing electrode


62


from the extraction grid


38


, may be varied. The vertical separation may range from zero microns when the focusing electrode


62


is placed in the plane of the extraction grid


38


(not illustrated), to one to five microns or even as much as ten microns or more.





FIG. 6

is a flow chart of a process


80


for manufacturing the focusing electrode


62


according to an embodiment of the present invention. The substrate


32


having a plurality of the emitters


30


has been previously formed, and the surface of the substrate


32


and the emitters


30


have been previously coated with the dielectric layer


34


. The extraction grid


38


has also already been formed.




The second dielectric layer


64


is formed on the extraction grid


38


in step


82


. A conductive layer is formed on the second dielectric layer


64


in step


84


. The conductive layer is patterned to form the focusing electrode


62


in step


86


. The second dielectric layer is then patterned in step


88


so as to form an opening surrounding each emitter


30


or group of emitters.




In one embodiment, the conductive layer is formed as a polysilicon layer, and the second dielectric layer


64


is a layer of silicon dioxide deposited on the extraction grid


38


. This arrangement allows the second dielectric layer


64


to be patterned via the buffered oxide etch using the focusing electrode


62


as a self-aligned mask. The focusing electrode


62


is electrically coupled to the emitter


30


via the optional impedance


66


in step


90


. The process


80


then ends and processing of the field emission display


11


,


11


′ or


11


″ is subsequently completed via conventional fabrication steps.





FIG. 7

is a simplified block diagram of a portion of a computer


100


including the field emission display


11


,


11


′ or


11


″ having the focusing electrode


62


as described with reference to

FIGS. 2 through 6

and associated text. The computer


100


includes a central processing unit


102


coupled via a bus


104


to a memory


106


, function circuitry


108


, a user input interface


110


and the field emission display


11


,


11


′ or


11


″ including the focusing electrode


62


according to the embodiments of the present invention. The memory


106


may or may not include a memory management module (not illustrated) and does include ROM for storing instructions providing an operating system and a read-write memory for temporary storage of data. The processor


102


operates on data from the memory


106


in response to input data from the user input interface


110


and displays results on the field emission display


11


,


11


′ or


11


″. The processor


102


also stores data in the read-write portion of the memory


106


. Examples of systems where the computer


100


finds application include personal/portable computers, camcorders, televisions, automobile electronic systems, microwave ovens and other home and industrial appliances.




Field emission displays


11


,


11


′ or


11


″ for such applications provide significant advantages over other types of displays, including reduced power consumption, improved range of viewing angles, better performance over a wider range of ambient lighting conditions and temperatures and higher speed with which the display can respond. Field emission displays find application in most devices where, for example, liquid crystal displays find application.




Although the present invention has been described with reference to a preferred embodiment, the invention is not limited to this preferred embodiment. Rather, the invention is limited only by the appended claims, which include within their scope all equivalent devices or methods which operate according to the principles of the invention as described.



Claims
  • 1. A method of operating a field emission display comprising:emitting a stream of electrons from a first emitter; focusing the stream of electrons emitted from the first emitter with a first focus electrode that is electrically coupled to the first emitter and that physically confines the stream of electrons; and setting the voltage on the first focus electrode to be a function of a first bias current through the first emitter.
  • 2. The method of claim 1, further comprising setting a voltage on the first focus electrode to be equal to a voltage on the first emitter.
  • 3. The method of claim 2, further comprising steps of:emitting a stream of electrons from a second emitter; and focusing the electrons emitted from the second emitter with a second focus electrode that is electrically coupled to the second emitter and that physically confines the stream of electrons from the second emitter.
  • 4. The method of claim 3, further comprising setting the voltage on the second focus electrode to be equal to a voltage on the second emitter.
  • 5. A method of operating a field emission display comprising:emitting a stream of electrons from a first emitter; focusing the stream of electrons emitted from the first emitter with a first focus electrode that is electrically coupled to the first emitter and that physically confines the stream of electrons; and setting a voltage on the first focus electrode to be equal to a voltage on the first emitter.
  • 6. The method of claim 5, further comprising steps of:emitting a stream of electrons from a second emitter; and focusing the electrons emitted from the second emitter with a second focus electrode that is electrically coupled to the second emitter and that physically confines the stream of electrons from the second emitter.
  • 7. The method of claim 6, further comprising setting the voltage on the second focus electrode to be equal to a voltage on the second emitter.
  • 8. A method of operating a field emission display comprising:emitting a stream of electrons from a first emitter; focusing the stream of electrons emitted from the first emitter with a first focus electrode that is electrically coupled to the first emitter and that physically confines the stream of electrons; setting a voltage on the first focus electrode to be equal to a voltage on the first emitter; emitting a stream of electrons from a second emitter; and focusing the electrons emitted from the second emitter with a second focus electrode that is electrically coupled to the second emitter and that physically confines the stream of electrons from the second emitter.
  • 9. The method of claim 8, further comprising setting the voltage on the second focus electrode to be equal to a voltage on the second emitter.
  • 10. A method of operating a field emission display comprising:emitting a stream of electrons from a first emitter; focusing the stream of electrons emitted from the first emitter with a first focus electrode that is electrically coupled to the first emitter and that physically confines the stream of electrons; setting a voltage on the first focus electrode to be equal to a voltage on the first emitter; emitting a stream of electrons from a second emitter; focusing the electrons emitted from the second emitter with a second focus electrode that is electrically coupled to the second emitter and that physically confines the stream of electrons from the second emitter; and setting the voltage on the second focus electrode to be equal to a voltage on the second emitter.
CROSS-REFERENCE TO RELATED APPLICATION

This application is a continuation of U.S. patent application Ser No. 09/085,333 filed May 26, 1998 and now U.S. Pat. No. 6,326,725.

GOVERNMENT RIGHTS

This invention was made with government support under Contract No. DABT63-93-C-0025 awarded by Advanced Research Projects Agency (ARPA). The government has certain rights in this invention.

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Entry
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Continuations (1)
Number Date Country
Parent 09/085333 May 1998 US
Child 09/933641 US