1. Field of the Invention
This invention relates generally to field emission devices, and in particular to cathode structures for field emission devices having protected gate electrodes.
2. Background of the Invention
Flat panel displays (FPDs) using carbon nanotube (CNT) technology are replacing and superseding existing display technologies, including those that use cathode ray tubes (CRTs), thin film transistor liquid crystals (TFT-LCDs), plasma display panels (PDPs), and organic light emitting diodes (OLEDs). The emerging CNT-based flat panel display technology uses a process for generating pictures similar to the method used in CRTs. But instead of a CRT's single hot filament electron gun, CNT-based displays use a planar array of carbon nanotube emitters as a source of electrons.
In one example, a CNT-based field emission display comprises a cathode structure (also called an emitter structure) disposed on a back plate and an anode structure on an opposing faceplate. The cathode structure includes a matrix of row electrodes and column electrodes (either of which may be emitter or gate electrodes). Electron emitters, such as CNTs, are disposed within cavities or holes in the cathode structure that correspond to particular pairs of row and column electrodes. When an appropriate voltage is applied between a particular row and column electrode, electrons are emitted from the emitters corresponding to that pair of row and column electrodes. These emitted electrons are accelerated towards the anode structure on the faceplate by an electric field, normally created by a combination of the anode and the row and column electrodes. The anode structure includes color elements (e.g., phosphors), each of which absorbs the energy from the emitted electrons and emits light of a particular color. This light, when combined with the light from other color elements, creates an image on the display.
The display can be matrix-addressed by applying voltages to each of its row and column electrons to control precisely the electron emission of the emitters for any particular row and column. The intersection of a row line and a column line in the matrix defines a picture element, or sub-pixel, the smallest addressable element in an electronic display. In a typical color display system, each pixel includes three picture elements corresponding to the pixel's component colors (e.g., red, green, and blue). Controlling the emission of electrons of each picture element controls the light intensity of each picture element and, in turn, the color of each pixel and the overall picture on the display. By matrix-addressing each picture element or pixel of the display, any desired refresh rate can be accomplished.
In the field emission display described above, each picture element has its own source of electrons—the set of emitters that corresponds to a particular row and column electrode pair. This provides a highly redundant electron source for the display. Compared to competing technologies, CNT-based field emission displays provide pristine picture quality, robust video response, wide viewing angles, and low power consumption. This alleviates the size, weight, and power limitations of a conventional CRT, while providing higher picture quality, lower manufacturing cost, and more efficient power consumption than LCDs.
A problem arises in the design of such displays, however, due to their use of electric fields between the emitters and the other electrodes to cause emission of the electrons for driving the display. In many existing embodiments of field emission devices sealed in vacuum envelopes, a gate electrode in the cathode structure is exposed to the conductive portions of a highly charged faceplate structure. In operation of such a device, a voltage potential serving as a control signal is applied to the exposed gate electrode. The gate electrode is typically the uppermost electrode in the cathode structure, which is used for controlling the emission of electrons (and thus the image of a display when the electron-emitting device is used in a field emission display system). A high voltage potential is then applied to the black matrix of a faceplate (or anode) structure, causing emitted electrons to be accelerated from the cathode structure towards the faceplate.
Due to the exposure of the gate electrode to the high voltage anode structure of the faceplate within the vacuum-sealed portions of a field emission device, arcing may occur between the gate electrode and the anode structure. This arcing is an electrical breakdown in the vacuum envelope with a high voltage anode, caused by the significant difference in electrical potential between the gate and anode electrodes. In vacuum electronics, electrical arcing can be a critical problem for the proper operation of field emission electron-emitting devices. As described, the arcing problem is related to the varying potentials of the cathode, faceplate, and spacer materials and structures, and specifically to the two electrodes that are commonly found therebetween—the gate electrode of the cathode and the anode electrode of the faceplate.
Previous solutions to the arcing problem have employed an insulating passivation layer above the gate electrode to prevent arcing. But these solutions have left portions of the gate layer exposed and have therefore not fully prevented arcing between the gate electrode and anode.
To address this arcing problem, a cathode structure for an electron-emitting device includes a passivation layer, or other dielectric or insulating material, situated over or otherwise protecting the gate layer. To minimize exposure of the gate electrode to the anode while allowing exposure of the gate electrode for providing an electric field for drawing electrons from the emitter, the passivation layer covers and overhangs the gate layer on a top side thereof. This leaves an underside or other portion of the gate electrode exposed to the emitter structure while still protected from the anode structure. The passivation layer covers the gate electrode at least in part to inhibit arcing between the gate electrode and the anode structure.
The cathode structure can be used to supply electrons for lighting a picture element in a display system, such as a CNT flat panel display. In one embodiment, a display system comprises a matrix of pixels, each pixel having one or more picture elements. For each picture element of each pixel, the display system comprises a color element that emits light when excited by electrons and an electron emitting device as described herein and configured to emit electrons towards the color element, thereby causing the color element to emit light.
In another embodiment, a method for making a cathode structure having an overhanging passivation layer comprises forming an emitter electrode on a substrate, forming an insulating layer over the emitter electrode, forming a gate electrode over the insulating layer, forming a passivation layer over the gate electrode, and forming at least one emitter hole through the insulating layer and the passivation layer (and possibly through the gate electrode). The passivation layer is formed so that it overhangs the gate electrode over the emitter hole or otherwise protects the gate electrode from arcing with an anode placed opposite the cathode structure. In one embodiment, where the emitter hole is formed by etching, the passivation layer and the insulating layer are selected so that the passivation layer has a higher etch selectivity relative to the insulating layer.
In an embodiment in which the field emission device is to be used in a display system, the cathode structure lies opposite a corresponding anode structure, as shown. The anode structure comprises an anode 165 and a color element 160, such as a phosphor, both of which are disposed on a faceplate 170. Preferably, the faceplate 170 is made of a transparent material, such as glass, so that light emitted from the color element 160 can shine through the faceplate 170. This enables the field emission device to generate a colored pixel of an image when the color element 160 is excited by electrons emitted from the emitters 155.
A bottom or underside of the gate electrode 130 is exposed (e.g., without electrical insulation) at least in localized areas near the emission elements 155 of the cathode structure. In this way, a voltage applied between the gate electrode 135 and the emitter electrode 110 creates an electrical field therebetween. If sufficient to overcome the work function of the emitters 155, this enables the gate electrode 130 to create an electrical field to cause electron emission from the electron-emission elements. For proper exposure, the gate electrode 135 may overhang the emitter hole, a cavity formed through the insulating layer 125 in which the emitters 155 are situated, although other means of exposure may be provided.
Although exposed to the emitters hole, the gate electrode 130 is preferably protected from exposure to the anode 165 to prevent arcing therebetween. Accordingly, passivation layer 135 is situated over and overhangs the gate electrode 130. The passivation layer 135 may comprise one or more of a number of dielectric or insulating materials. By covering a top surface of the gate electrode 130 with the passivation layer 135 or other insulation means, the electric field that could cause arcing between the gate electrode 130 and the anode 165 is significantly reduced. Beneficially, reducing this electric field for a given set of conditions allows the anode voltage to be increased. A higher anode voltage allows for increased acceleration of emitted electrons from the cathode, resulting in higher brightness and generally improved performance of the display.
In
After the gate electrode 130 is patterned, a passivation layer 135 is deposited thereover. In one embodiment, the passivation layer 135 comprises silicon nitride (SiN). The passivation layer 135 may alternatively comprises one or a combination of a number of other insulator materials. In one embodiment, the passivation layer 135 has a thickness is in the range of about 100 nm to about 1000 nm.
As shown in
In one embodiment, so that the gate layer 130 is covered on a top side by the passivation layer 135 but exposed on a bottom side by the insulating layer 125, the passivation layer 135 is selected to have a higher etch selectivity relative to the etch selectivity of the insulating layer 125 (in the BHF wet etching process or whichever etch is performed). In this way, the etching process removes the insulating layer 125 faster than the passivation layer 135, so that the process can be stopped when the desired structure is obtained. In one embodiment, the ratio of the etch selectivity of the passivation layer 135 to the insulating layer 125 is in the range of about 2 to about 20.
As shown in
With the catalyst layer 150 formed, the electron-emitting elements 155 are grown, as shown in
In an alternative embodiment, the gate electrode 130 is initially deposited over the insulating layer 125 as a continuous strip, without any holes patterned over the emitter electrode 110. Accordingly, the process of forming the holes 145 through the passivation layer 135 and insulating layer 125 (e.g., using the photoresist pattern 140) further includes forming the corresponding holes through the gate electrode 130. Forming the holes through each of these layers using the same photoresist pattern 140 may help to align the holes through each layer and thus produce a more uniform cavity 145.
Although various embodiments for forming the cathode structure for a field emission device have been described and illustrated, it can be appreciated that any number of variations can be made to these while achieving the benefit of protecting the gate electrode to avoid electrical arcing and shorting. Various embodiments of electron-emitting devices that can be used in conjunction with or modified by the improved cathode structure described herein as well as various processes for producing a cathode structure suitable for a field emission device (such as a display system) are described in the following, each of which is incorporated by reference in its entirety: U.S. application Ser. No. 10/080,057, filed Feb. 20, 2002; U.S. application Ser. No. 10/080,012, filed Feb. 20, 2002; U.S. application Ser. No. 10/302,126, filed Nov. 22, 2002; U.S. application Ser. No. 10/226,405, filed Aug. 22, 200; U.S. application Ser. No. 10/226,873, filed Aug. 22, 2002; U.S. application Ser. No. 10/327,529, filed Dec. 20, 2002; U.S. application Ser. No. 10/600,226, filed Jun. 19, 2003; U.S. application Ser. No. 10/807,485, filed Mar. 27, 2004; and U.S. application Ser. No. 10/952,352, filed Sep. 27, 2004.
Embodiments of the field emission devices can be used in display systems, such as matrix-addressable CNT-based field emission display. For example, the device illustrated in
The emitters associated with a picture element can be made to emit electrons (toward an anode on a faceplate structure, not shown) through appropriate driving of the row driver 440 and column driver 450, which are coupled to the row electrodes 410 and column electrodes 420, respectively. When an appropriate voltage is applied between a particular row and column electrode 410 and 420, electrons are emitted from the emitters corresponding to that pair of row and column electrode 410 and 420. In this way, the display is matrix-addressable to control precisely the electron emission of the emitters for each row and column. The emitted electrons are accelerated towards an anode structure on the faceplate by an electric field. The anode structure includes a plurality of color elements (e.g., phosphors), which absorb the energy from the emitted electrons and emit light of a particular color. In a typical color display system, each pixel includes three picture elements corresponding to the pixel's component colors (e.g., red, green, and blue). Controlling the emission of electrons of each picture element thus controls the light intensity of each picture element and, in turn, the color of each pixel and the overall picture on the display.
As used herein, the terms situated over, formed over, and overlying, as well as other terms applied to layers, are not meant to limit the structure such that the layers must necessarily be directly over one another or that the layers must be in physical contact, unless expressly disclosed as such. Where one layer is over another layer, in any sense, there may exist other layers between those layers. Moreover, two layers need not be coextensive, or even overlap, for one layer to be over the other. These terms thus refer to the layers' respective ordering in various embodiments of the devices described herein, and should be understood in the broad context of the disclosure.
The foregoing description of the embodiments of the invention has been presented for the purpose of illustration; it is not intended to be exhaustive or to limit the invention to the precise forms disclosed. Persons skilled in the relevant art can appreciate that many modifications and variations are possible in light of the above teachings. For example, the insulator layer may be a single material, more than two layers of distinct materials, or a material with continuously varying properties. Moreover, additional layers may be used, layers may be eliminated, and the layers may be ordered differently. It is therefore intended that the scope of the invention be limited not by this detailed description, but rather by the claims appended hereto.
This application claims the benefit of U.S. Provisional Application No. 60/563,075, filed Apr. 15, 2004, which is incorporated by reference in its entirety.
Number | Date | Country | |
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60563075 | Apr 2004 | US |