FIELD EMISSION CATHODE AND A DEVICE BASED THEREON

Abstract: A matrix field-emission cathode (5) comprises a monocrystalline silicon substrate (7) on which are arranged epitaxially grown pointed silicon emitters (1) which also act as a ballast resistor connected in series. In an advantageous embodiment of the proposed cathode, for a radius of curvature (r) at the emitter tip not exceeding 10 nm, the ratio of the height (h) of the emitter to the radius (r) is not less than 1000, while the ratio of (h) to the diameter (D) at the emitter base is not less than 1. The angle α at the emitter tip does not exceed 30°. The specific resistance of the emitter material is chosen so as to ensure that the resistance of each emitter will be comparable with the resistance between the cathode and the opposing electrode. The proposed cathode is used in an electronic device for displaying information which also has an anode (3) in the form of a strip (11) of phosphorescent material (10) and a conducting layer (9) whose projection onto the cathode (5) is perpendicular to the conducting paths (6) on the cathode; the anode itself acts as the control electrode.

Description: The present invention relates to electronic devices having a matrix field-emission cathode. Cathodes for field-emission electronics and vacuum microelectronics represent, as a rule, regular tip arrays prepared by means of photolithography, etching, evaporation through a mask, etc. It is known a field-emission cathode formed of silicon tips prepared in the body of a single-crystalline silicon wafer by etching (H.F. Gray et al, US-Pat. 4,307,507, 1981). A shortcoming of such a cathode is that the height of the emitters is inherently not-large, typically several micrometers, that does not allow to have high field enhancement. In addition, the emitter material has relatively large value of work function (4 - 5) eV. Such cathodes can ensure sufficiently high electron currents at either high voltages or at a small disctance between the emitters and an extracting electrode. The latter increases parasitic capacity of the devices limiting possibilities of their applications. In addition, field emission from such cathodes is not uniform. There are known field-emission cathodes formed by arrays of silicon tips prepared by epitaxial deposition of silicon on (100)-oriented silicon substrates (D. Dieumegard et al., FR-A-2629264, 1988; B. B. Siu, US-Pat. 5,094,975, 1992). The tips have a shape of four-fold pyramids formed by (111)-faces. Field emission from such cathodes is not uniform. Also known are field-emission cathodes formed by arrays of Si whiskers, see FR-A-2 658 839. In order to improve the uniformity of the field emission from various emitters in multiple-emitter matrix, it is common to use an additional resistance that is comparable with the differential resisistance of the vacuum gap and that is introduced in series with each of the emitters. Its action is based on the following: if current flowing through a given emitter is larger than that through other ones, a voltage drop on it is larger and, accordingly, the extracting voltage is decreased resulting in a drecrease of the large current flowing. Such an approach is used in patents by meyers (French Pat. 8,411,986, 1985 and US-Pat. 4,908,539, 1990), where the additional ("ballast") resistor is provided by deposition of amorphous silicon film, having a high specific resistivity, onto an insulating substrate, while emitting tips (molybdenum cones) are deposited on the amorphous film. However, the use of the amorphous film limits substantially possibilities for preparation of emitters, particularly of semiconductor ones, because the existing semiconductor technologies need in rather high, temperature at which the amorphous silicon is spontaneously crystallized and losses its high resistivity. It is known a matrix field-emission cathode that consists of single-crystalline silicon substrate and an array of tips that have series ballast resistances prepared integrally by selective impurity diffusion (R. Kane, US-Pat. 5,142,186, 1992). In such a design, the ballast resistance takes a significant area at the substrate where other emitters could be arranged. In addition, the technology for preparation of the resistances needs in several photolithography procedures with fitting operations that complicates the process for fabrication of field emitters and makes it more expensive. It is known an electron device (display) that has a diode design consisting of a flat cathode prepared from diamond or diamond-like carbon and an opposite anode with a phospor (C.Xie, N.Kumar et al., Electron field emission from amorfic diamond thin film, A paper at 6th Intern. Conf. Vacuum Microelectronics, July 1993, Newport, RI, USA). For an effective operation of such a display, rather high voltages (several hundreds volts) are necessary that are hardly compatible with working voltages of other electronic parts of the display. In addition, field-emission properties of the diamond film are difficult to reproduce because they depend strongly on preparation conditions. Finally, in order to obtain sufficient emission currents, anode-to-cathode distances must be small, about 20 µm or less; that makes it difficult to pump gaseous contaminations evolving by the phosphor. It is known a display having a matrix field-emission cathode with tip emitters arranged on an single-crystalline silicon substrate that contains conductive stripes formed by doping, gate electrode, ballast resistors, and an anode with a phosphor (N.N.Chubun et al, Field-emission array cathodes for a flat-panel display, Techn. Dig. IVMC-91, Nagahama, Japan, 1991.). In the device, the tip emitters (Mo cones) were formed on an n-type single-crystalline silicon substrate with the stripes formed by doping with acceptor impurity, This means that, there, an isolation by p-n junction was realized. Gating columns (as Mo-film stripes) were placed on the cathode, too, normal to the conductive stripes (lines) being isolated by a dielectric film. In order to increase uniformity of field-emission current from the emitters, discrete ballast resistors were introduced in series with each of the lines that decreased scattering of brightness along the columns within 15%. However, in such a way, it is impossible to control brightness along the lines. In addition, such a design is rather cumbersome and not suitable for high-resolution displays. The aim of the invention is to design a field-emission cathode that has lower working voltages, is operative under relatively poor vacuum conditions, and ensures a high emission uniformity over a large area. Another aim of such a design is to ensure a high uniformity on all over the display, and low parasitic capacity of display, based on the cathode. The aim is reached by an electronic device having a matrix field cathode as defined in claim 1. In the cathode, ratios of the heights of the emitters h to their radii of curvature at the tip ends r are not less than 1000, the radii being less than 10 nm, while ratio of h to the diameter of the emitters at the base D is not less than 10. Angles α at the ends are preferentially less than 30°. The specific resistivity of emitter material is chosen so that the resistance of each emitter would be comparable with resistance of the vacuum gap between the emitter and gate electrode. Ends of the tip Si emitters can have coatings of materials decreasing electron work function, for example, of diamond while curvature radii of the coating are from 10 nm to 1µm. A preferential diameter D is 1 to 10 µm, while the specific resistivity of the material is not less than 1 Ohm-cm. The large height and the small curvature radius of the field emitters give large field enhancement; at the same time, the diamond coatings having low work functions, together with geometrical characteristics of the emitters, ensure low working voltages and decrease demands to vacuum conditions. Another aim is reached by an electronic device providing a display containing a matrix field-emission cathode which is provided with silicon tip emitters on conductive doped stripes in a single-crystalline silicon substrate with an anode provided with phoshorescence material and conductive, transparent layers, wherein the anode is provided with stripes the projection of which on the cathode perpendicular to the conductive stripes, and whereby the anode implements the function of a gate electrode. Brief description of the drawings The invention is illustrated by the following figures. Fig. 1 - Silicon tip emitter prepared of a whisker. Fig. 2 - Current-voltage characteristics of emitters with diamond particles and without them. Fig. 3 - Current-voltage characteristics of diamond-coated emitters having different heights. Fig. 4 - Matrix field-emission cathodes prepared by charpening of whisker arrays (versions). Fig. 5 - Matrix field-emissions cathode consisted of regular array of emitters with diamond particles on tips: a - a scheme; b - a micrograph. Fig. 6 - Schemes of silicon tip arrays (a), with single particles (b) with tips coated by almost continuous layer of diamond particles (c) and with tips coated by diamond-like material (d). Fig. 7 - A scheme of display. Best version of the invention In Fig. 1, a tip emitter (1), prepared of silicon whisker is shown. Field-emission current I (A) of such an emitter depends on work function  (eV) of the material at the top (2) of the emitter (1), radius of curvature of the tip r (nm), its height h (µm), distance d (mm) between the anode (3), and the emitter (1), and on voltage V (Volts) at the anode-cathode gap according to the equation: I = (K 1 /) (fhV/rd) 2 exp[-K 2 rd 3/2 /fhV] where K 1 = 1.4 10 -6 , K 2 = 6.83x10 7 (0.95-1.48x10 -7 E/ 2 ), where f is the coefficient of ideality of the emitter that depends on the. ratio of the emitter height to the emitter diameter D at its basis and on the angle α of tip cone; E is electrical field strength. It is seen from the formula {1} } that the ratio h/r is one of the most important parameters that influence the emission current. At the emitter height more than 10 µm and the radius less than 10 nm, the value h/r is more than 1000 for an ideal emitter. Another important factor in the formula {1} is f , a "coefficient of ideality of emitter". For an ideal emitter f =1, real emitters have f from 0.1 to 0.8 depending on their shape. Calculations by T.Utsumi (T. Utsumi, Vacuum microelectronics: what's new and exciting, IEEE Trans Electron Devices 38, 2276, 1991) show that in order to reach maximal values of f , it is necessary to use emitters with ratio of the emitter height to the basis diameter as large as possible (for example, 10 to 100) and with low angles α (for example, 15 to 20°) Another important parameter for the emission is the value of the effective work function . By decreasing  it is possible, firstly, to decrease the operation voltage and, secondly, to decrease influence of differences in curvature radii and heights of emitters on uniformity of emission from arrays. In order to lower the work function of the emitters, it is possible to deposit onto the emitters a material decreasing the work function, for example, diamond, or diamond-like material. It is known (F.J. Himpsel et al.,.Quantum photoyield of diamond (111) - a stable negative-affinity emitter, Phys. Rev. B20, 624, 1979) that the face (111) of diamond has negative electron affinity that allows to obtain values of effective work function less than 2 eV (E.I. Givargizov et al., Microstructure and field emission of diamond particles on silicon tips, Appl. Surf. Sci. 87/88, 24, 1995). In Fig. 2 three current-voltage (I-V) plots of emitters of Fig. 1 are given: with diamond particle on the tip for work function of 1 eV (1), 2.5 eV (2), and without diamond coating for =4.5 eV (3). In all the cases, the height of emitters is 100 µm, and the curvature radius of the tip is 10 nm. Fig. 2 illustrates a possibility to obtain large currents at rather low operation voltage from emitters with diamond particles, that exceed strongly field-emission currents that could be obtained without such particles. In Fig. 3, are given I-V plots of field emitters with diamond particle, having effective size of 10 nm for different emitter heights: 10 µm (1), 50 µm (2), and 100 µm (3), at =2.5 eV. These characteristics indicate to significant increase of the emission current at the same voltage with increase of the emitter height. In Fig. 4, examples of tip arrays prepared from grown whiskers are shown. Field-emission cathodes with such arrays can have areas of several square centimeters with tip density of 10 4 to 10 6 cm -2 . Multiple-tip field-emission cathodes allow to obtain, at relatively low voltages and at independent action of different emitters, a large current that equals to the current of single emitter multiplied by number of emitters. In Fig. 5 are given a scheme and a micrograph of tip emitters with diamond particles (4) on their ends (2). In Fig. 6, are given schemes of various diamond coatings: with single particles (Fig. 6b), with ends coated by almost continuous layer of fine diamond particles (Fig. 6c), and with a film of diamond-like material (Fig. 6d). At deposition of diamond or diamond-like material onto tips, their radii of curvature are certainly increased, for example, up to 1 µm. This increase of the radius can be partly or completely compensated by decrease of the work function, as it was proved by direct experiments. In order to improve uniformity of the field emission of a multiple-tip cathode on a large area it is desirable each emitter to have electrical resistance comparable with that of vacuum gap (typically, this is a value about 10 6 - 10 7 Ohm). Such a large resistance of an emitter can be reached at a suitable choice of its geometrical characteristics ( a small cross-section D, a significant height h , a small angle at the end α that involves elongation of the conical part) and at suitable doping level ( specific resistivity ρ). The resistance can be calculated according to the expression R=4hρ/πD 2 (supposing a cylindrical shape of the emitter). An example of the calculation of the emitter resistance: at the cross-section area 1 µm 2 , height 50 µm and specific resistivity 10 Ohm-cm, resistance of the emitter is about 5x10 6 Ohm. The conical shape of the emitter contributes an additional resistance. Further increase of the resistance is possible by increase of the specific resistivity. It is known, that at crystallization of silicon from the vapor phase it is possible to obtain a material with a specific resistivity up to 100 Ohm-cm. An additional factor in controlling of resistance of the emitter is its doping with such an impurity as gold that is commonly(as here) used as an agent for growing of whiskers by the vapor-liquid-solid mechanism ( others are related transient elements such as copper, silver, nickel, palladium etc.). It is known that gold is a compensating impurity that ensures a high specific resistivity of silicon. Finally, in Fig. 7 is shown a display that includes the matrix field emission cathode (5) according to Figs. 4 and 5, where silicon tip emitters (1) are implemented on linear(striped) n + -areas (6) prepared by doping in silicon p-type substrate (7). To each of the linear n + -type areas (6), as well as to the p-type substrate (7) an electrical contact (8) is made. At a distance 0.1-1 mm of the cathode (5) is placed an anode (3) where optically-transparent conductive layer (9) and phosphor (10) are made as linear (striped) areas (11) whose projections on the silicon substrate (7), a cathode basis, are perpendicular to the linear n + -areas (6). To each of linear area (11) of the anode (3), that includes the conductive layer (9) and phosphor (10), an electrical contact (12) is made. At applying of voltage from an external source (13) between two chosen linear areas (11) of anode (3) and (6) of cathode (5), a small area of the anode is shining. In order to avoid electrical connection between different areas of the cathode, a small (several Volts) voltage V rev in reverse direction between the linear n + -type area (6) and p-type substrate (7) is established. In this design, the anode implements functions of a gate electrode. The device can serve as a field-emission flat panel display without a close-spaced gate electrode. The diamond coating (4) of emitter tip (2) allows to increase the electron emission ( at a given field strength at the tip) and to improve its stability and robustness against destroying and deterioration of its properties. Industrial applications. The invention can be used in TV, computers and other information devices in various areas of applications.

Claims: Electronic device having a matrix field-emission cathode (5), an opposite electrode (3) opposite to said cathode (5) a vacuum gap between said cathode (5) and the said electrode (3) and ballast resistors connected in series with the vacuum gap, said cathode containing a single-crystalline silicon substrate (7) and an array of silicon tip emitters (1), wherein the silicon tip emitters (1) are made of silicon whiskers epitaxially grown on the single-crystalline silicon substrate (7) and having a resistance of about 10 6 -10 7 Ohms which enables the emitters to implement the function of the ballast resistors. Device according to claim 1, wherein the ratio of the height h of the emitter (1) to the curvature radius r at the apex (2) of the emitter (1) is not less than 1000, and wherein radius r does not exceed 10 nm. Device according to claim 2, wherein the ratio of the height h of the emitter to the diameter D at its basis is not less than 10 and wherein the diameter D of the silicon tip emitter (1) is of 1 to 10 µm each. Device according to claims 2 and 3, wherein the angle α at the emitter apex is not larger than 30°. Device according to claim 4, wherein the specific resistivity of the emitter material is chosen so that the resistance of each of the silicon tip emitters is comparable with the resistance of the vacuum gap between the cathode (5) and the opposite electrode (3). Device according to claim 1, wherein the apex (2) of the silicon tip emitters (1) has a coating that reduces the electron work function. Device according to claim 6, wherein the coating is of diamond or diamond-like material. Device according to claim 7 having a radius of the diamond coating at the apex of 10 nm to 1 µm. Device according to claims 1 to 8, wherein the specific resistivity of the emitter material is larger than 1 Ohm-cm. Device according to anyone of claims 1 - 9, providing a display, having a cathode (5), which is provided with silicon tip emitters (1) on conductive stripes (6) in a single-crystalline silicon substrate (7), an anode (3) provided with phoshorescent material (10) and conductive, transparent layers (9), wherein the anode (3) is provided with stripes (11) the projection of which on the cathode (5) is perpendicular to the conductive stripes (6), and whereby the anode implements the function of a gate electrode.

Inventors: GIVARGIZOV EVGENY INVIEVICH, OBOLENSKAYA LIDIA NIKOLAEVNA, STEPANOVA ALLA NIKOLAEVNA, ZHIRNOV VIKTOR VLADIMIROVICH, GIVARGIZOV, EVGENY INVIEVICH, OBOLENSKAYA, LIDIA NIKOLAEVNA, STEPANOVA, ALLA NIKOLAEVNA, ZHIRNOV, VIKTOR VLADIMIROVICH
Applicants: GIVARGIZOV EVGENY INVIEVICH, OBOLENSKAYA LIDIA NIKOLAEVNA, STEPANOVA ALLA NIKOLAEVNA, ZHIRNOV VIKTOR VLADIMIROVICH, GIVARGIZOV, EVGENY INVIEVICH, OBOLENSKAYA, LIDIA NIKOLAEVNA, STEPANOVA, ALLA NIKOLAEVNA, ZHIRNOV, VIKTOR VLADIMIROVICH
Application year: 1995
Main classification: H01J1
IPC codes: H01J1, H01J31, H01J19