Surface conduction electron-emitting device

Abstract: A surface conduction electron-emitting device is provided which comprises a high-potential electrode (1) provided on a substrate surface, an electron-emitting region (4, 4a, 4b) provided in contact with the periphery of an exposed part of the high-potential electrode, and a low-potential electrode (2a, 2b) further provided in contact with the periphery of the electron-emitting region. The low-potential electrode may project upward in the thickness direction of the substrate to a higher level than the high-potential electrode. A means for applying a voltage may further provided between the high-potential electrode and low-potential electrode. The low-potential electrode may be divided into plural numbers and potential may be applied to each of the low-potential electrodes independently.

Description: BACKGROUND OF THE INVENTION Field of the Invention The present invention relates to an electron-emitting device, and more particularly to a surface conduction electron-emitting device that emits electrons when an electric current is flowed in a highly resistant thin film as defined by the precharacterizing features of claim 1 and known from the SU-A-1 003 195. Related Background Art Hitherto known as a device capable of emitting of electrons With a simple structure is the cold cathode device reported by M.I. Elinson et al (Radio Eng. Electron. Phys., Vol. 10, pp.1290-1296, 1965). This utilizes the phenomenon that electron emission is caused by flowing an electric current to a thin film formed with a small area on a substrate and in parallel to the surface of the film, and is generally called a surface conduction electron-emitting device. This surface conduction electron-emitting device that has been reported includes those employing a SnO₂(Sb) thin film developed by Elinson et al., those employing an Au thin film. (G. Dittmer, "Thin Solid Films", Vol. 9, p.317, 1972), those comprising an ITO thin film, (M. Hartwell and C.G. Fonstad, "IEEE Trans. ED Conf.", p.519, 1975), and those comprising a carbon thin film [Hisaji Araki, "SHINKU" (Vacuum), Vol. 26, No. 1, p.22, 1983]. Typical device constitution of these surface conduction electron-emitting devices is shown in Fig. 17. In Fig. 17, a conventional surface conduction electron-emitting device comprises an insulating substrate 5 having thereon a highly resistant thin film 4 provided between a high-potential electrode 1 and a low-potential electrode 2, where a voltage is applied from an external electric source 3 and thereby electrons are emitted from the highly resistant thin film 4. In these surface conduction electron-emitting devices, it has been hitherto practiced to previously form an electron-emitting region 4 (a high-resistance thin film) by an energizing heat treatment, called "forming", before effecting the electron emission. More specifically, a voltage is applied between the above electrode 1 and electrode 2 to energize the thin film formed with an electron-emitting material to bring the thin film to be locally destroyed, deformed or denatured owing to the Joule heat thereby generated, thus forming the electron-emitting region 4 (a high-resistance thin film) kept in a state of electrically high resistance to obtain an electron-emitting function. However, such a conventional surface conduction electron-emitting device has disadvantages such as the following: (1) The light-emitting region flickers. (2) As shown in Fig. 18, the electron beam tends to deflect by the distance L toward the high-potential electrode 1 side, and in general the beam diverges. (3) Accordingly, as shown in Fig. 19 it is necessary to externally provide a focusing lens system to effect the focusing of the electron beam. This, however, requires preparation of external focusing lenses 17 and 18, requiring an additional step correspondingly. (4) There is required a complicated operation to make axial alignment on the basis of electron optics between the outer focusing lenses 17 and 18 and the surface conduction electron-emitting device. SUMMARY OF THE INVENTION The object of the present invention is to provide a surface conduction electron-emitting device that can solve the problems as mentioned above, caused by the insufficiency in the focusing performance, and can achieve a good beam-focusing performance without requiring any external focusing lenses. This object is attained by the characterizing features of claim 1. Advantageous developments of the invention are given by the subclaims. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1, Fig. 3 to Fig. 88 and 10A to Fig. 14 14 are views illustrating surface conduction electron-emitting devices of the present invention; Fig. 2 is a view explanatory of how electrons emit from the surface conduction electron-emitting device of the present invention; Figs. 9A and 9B are views explanatory of how equipotential lines are formed on the surface conduction electron-emitting devices of the present invention; Fig. 15A to Fig. 16G are flow sheets each showing the manner by which the surface conduction electron-emitting device of the present invention is prepared; Fig. 17 and Fig. 19 are views illustrating a conventional surface conduction electron-emitting device; and Fig. 18 is a view explanatory of how electrons emit from the conventional surface conduction electron-emitting device. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be specifically described below with reference to the accompanying drawings. Fig. 1 is a basic block diagram illustrating an example of the surface conduction electron-emitting device of the present invention. In Fig. 1, the surface conduction electron-emitting device of the present invention comprises a pair of electrodes, of which a high-potential electrode 1 having a round shape and feeding an electric current to an electron-emitting region 4 is concentrically provided on its periphery with the electron-emitting region 4, and a low-potential electrode is similarly concentrically provided around the electron-emitting region 4. In such constitution, the potential is constant everywhere on the respective electrodes. In the conventional surface conduction electron-emitting device illustrated in Fig. 17, the high-potential electrode 1 and the low-potential electrode 2 are separated right and left to form line symmetry, while in the device of the present invention illustrated in Fig. 1, the electrodes form center symmetry and rotation symmetry to bring about remarkably high symmetricalness as a whole. For this reason, the velocity distribution of the electrons to be emitted may be neither irregular nor deflected in contrast with the prior art, but can be uniform distribution having the center symmetricalness and rotation symmetricalness, so that the electron beam emitted from the surface conduction electron-emitting device can be focused at a particular position, i.e., a spot located at the direction perpendicular to the center of said device, and moreover decrease the flickering due to the substantial increase of the area of the light-emitting region. Fig. 2 is a view explanatory of how electrons emit from the surface conduction electron-emitting device of the present invention. In Fig. 2, when a voltage is applied to an accelerating electric source 6, electrons tend to converge to the center as a whole as indicated by arrow A. This is because the potential distribution is generated such that the electrons are inclined to focus to the high-potential side at the center since the high-potential electrode 1 has a high potential and the low-potential electrode has a low potential. For this reason, a good focusing performance can be achieved when electrons are focused to a target electrode 9 with use of the accelerating electric source 6, even without providing any external focusing lenses such as lens electrodes 17 and 18 as illustrated in Fig. 19 of the prior art. Accordingly, such a surface conduction electron-emitting device of the present invention, as having the structure that the electrodes 1 and 2 and focusing lenses 17 and 18 of the prior art have been integrated to the high-potential electrode 1 and low-potential electrode, makes it possible to bring the electrons to focus to a specific part, i.e. a vertically upper part of the center of said device. In addition, in the surface conduction electron-emitting device of the present invention, the electrodes and the electron-emitting region may not necessarily have the round shapes. For example, the same effect as previously stated can be obtained even when as illustrated in Fig. 3, Fig. 4 and Fig. 5, the low-potential electrode is divided into a plural number of electrodes to provide a plural number of electron-emitting regions of curved or linear shapes, so long as the device basically comprises a high-potential electrode provided on a substrate surface, an electron-emitting region provided in contact with the periphery of an exposed part of said high-potential electrode, and a low-potential electrode further provided in contact with the periphery of said electron-emitting region. Here, in the instance where the electron-emitting region is made to have the curved shape, the high-potential electrode may preferably have a round or oval shape (as exemplified by the devices having the electron-emitting region as illustrated in Figs. 1, 3 and 4). Also, in the instance where the electron-emitting region 4 is made to have the linear shape, the high-potential electrode 1 may preferably have a polygonal shape (as exemplified by those illustrated in Fig. 5). In the surface conduction electron-emitting device illustrated in Fig. 4, comprising the high-potential electrode having a round shape and the low-potential electrode made to be composed of four electrodes 2a to 2d, the device is so constituted that the low-potential electrodes 2b and 2d can be selected whether they work as low-potential electrodes (ON) or not (OFF), by means of a switch 10a, and, similarly, ON/OFF of the low-potential electrodes 2a and 2c can be selected by means of a switch 10b. Here, electron-emitting regions 4b and 4d provided between the high-potential electrode 1 and the low-potential electrodes 2b and 2d constitutes one set of electron-emitting regions (referred to as Set I), and, similarly, 4a and 4c constitute one set (referred to as Set II). The ON/OFF of the electron-emitting regions of Set I and that of the electron-emitting regions of Set II can be selected by the switch 10a and switch 10b, respectively. Accordingly, the switch 10b may be kept turn off and only switch 10a may be turned on to drive the surface conduction electron-emitting device of the present invention, so that there is given an electron-emitting device in which the center of the light-emitting region is positioned vertically above the center of the surface conduction electron-emitting device of the present invention and a spare electron-emitting region is provided corresponding to Set II that makes provisions for the case when the electron-emitting regions of Set I turned impossible for use because of end of life of the electron-emitting regions. As illustrated in Fig. 6C, the surface conduction electron-emitting device of the present invention may also be a 'vertical type' surface conduction electron-emitting device comprising; a pair of electrodes 1 and 2b positioned on and beneath a stepped portion of a step-forming layer 15 provided on a substrate 12, said electrodes 1 and 2b oposing each other with said stepped portion between to have electrode spacing; and an electron-emitting region 4b formed at the side end face of the stepped portion positioned between said electrodes 1 and 2b; where electrons are emitted from the electron-emitting region 4b on applying a voltage between the electrodes 1 and 2b. In this embodiment also, the beam of emitted electrons can be brought to focus, so long as the device has the form, as illustrated in Figs. 6A, 6B and 6C, comprising a high-potential electrode 1 provided on a substrate surface, electron-emitting regions 4 and 4a to 4d provided in contact with the periphery of an exposed part of said high-potential electrode, and low-potential electrodes 2 and 2a to 2d further provided in contact with the peripheries of said electron-emitting regions 4 and 4a to 4d. In a surface conduction electron-emitting device of the type that the low-potential electrode described above is divided in plurality so as to provide a plural number of electron-emitting regions in one device, the electron beam can also be brought to deflect to a desired direction by independently applying different potential to each of the low-potential electrodes. As an example thereof, as illustrated in Fig. 7, a low-potential electrode 2 is divided into two parts, 2a and 2b, to which potential Va, Vb is independently applied. Namely, if Va > Vb, the beam deflects toward 2a, and, in the reverse, it deflects toward 2b. In this occasion, the direction and magnitude of the deflection depends on Va minus Vb, and the amount of emitted electrons and the degree of focusing substantially depend on Va plus Vb. Accordingly, the both can be controlled independently. Additionally speaking, the low-potential electrode 2 need not be divided into two parts, and can be divided into desired number of electrodes according to what purpose the device is used for. Next, in the surface conduction electron-emitting device of the present invention, the focusing performance of the electron beam can be more improved by providing a low-potential electrode in such a manner that it projects upward in the thickness direction of the substrate to a higher level than the high-potential electrode. For example, as shown in Figs. 8A and 8B, when the device takes the constitution that a high-potential electrode 1 has a round shape and is surrounded by a low-potential electrode forming a hole in between, the diameter d₁ of the high-potential electrode 1, the diameter d₂ of the hole defined by the low-potential electrode 2 and the height h of the hole (or the distance from the top surface of the high-potential electrode to the top surface of the low-potential electrode) may preferably satisfy the following relationship: d 2 - d 1 ≲ 4 µm d 2 /6 ≲ h ≲ 6 d 2 How the electron beam focusing performance is improved by virtue of the electrodes 1 and 2 will be described here with reference to Figs. 9A and 9B. In Figs. 9A and 9B, the numeral 1 denotes a high-potential electrode; 2, a low-potential electrode; and 4, an electron-emitting region. Though not illustrated here, assume that a plane target electrode to which a positive voltage of several to several ten kV has been applied is disposed above the surface conduction electron-emitting device. Fig. 9A shows equipotential lines in the vicinity of a surface conduction electron emitting device comprising electrodes 1 and 2 both made equal in thickness, and the direction of a representative force exerted to the electron beam, which is indicated by arrows F. Similarly, Fig. 9B shows a state in the vicinity of a surface conduction electron-emitting device comprising the low-potential electrode 2 projected upward in the thickness direction of the substrate to a higher level than the high-potential electrode 1. As will be seen by comparing these Fig. 9A and Fig. 9B, in the surface conduction electron-emitting device of the present invention, the slant of equipotential lines is greater in the case where the low-potential electrode 2 has a larger thickness than the high-potential electrode 1, as compared with that in Fig. 9A. Accordingly, the electron beam undergoes a greater focusing force toward the center at the emission initial stage in which it has a small magnitude of the velocity component toward the target electrode and is subject to influence by the electric field. In Figs. 8A and 8B, the electrodes and electron-emitting regions have round shapes, but the same effect as previously stated can be obtained even when as illustrated in Fig. 10, Fig. 11 and Fig. 12, the low-potential electrode is divided into a plural number of electrodes to provide a plural number of electron-emitting regions of curved or linear shapes, so long as the device comprises a high-potential electrode provided on a substrate surface, an electron-emitting region provided in contact with the periphery of an exposed part of said high-potential electrode, and a low-potential electrode further provided in contact with the periphery of said electron-emitting region in such a manner that it projects upward in the thickness direction of the substrate to a higher level than the high-potential electrode. In the surface conduction electron-emitting device of the present invention, unevenness as illustrated in Figs. 13A to 13C may further be made on at least one of the boundary between the low-potential electrode and the electron-emitting region and the boundary between the high-potential electrode and the electron-emitting region. Forming the boundary in such a shape makes stronger the local electric field desirably. Also, as illustrated in Fig. 13D, the low-potential electrode 2 can be made to have any desired outer side shape according to any conditions of arrangement or wiring. As illustrated in Fig. 14, the surface conduction electron-emitting device according to the present invention may also constitute a plural number of devices arranged on the same substrate and driven independently, so that there can be obtained a plural number of independent electron beams. An example of methods for preparing the surface conduction electron-emitting device of the present invention will be described below with reference to Figs. 15 and Figs. 16. In Figs. 15A to 15E, the surface of a substrate 16 is first oxidized to form an insulating film, thus preparing an insulating substrate 5 (Fig. 15A). Next, part of the insulating substrate 5 is etched to make a hole, and thereafter a metal film 20 is formed on the whole surface by vapor deposition (Fig. 15B). This metal film 20 is further etched as illustrated in Fig. 15C to prepare a high-potential electrode 1 and low-potential electrodes 2a and 2c. Next, a thin film 21 is formed by vapor deposition, and then a forming treatment is carried out (Fig. 15D). In this instance, unless the high-potential electrode 1 and the low-potential electrodes 2a and 2c are masked, the thin film adheres also on top surfaces of these, but this does not affect the characteristics of the device in practical use. If necessary, however, it is of course possible to cover with a mask the top surfaces of the high-potential electrode 1 and low-potential electrodes 2a and 2c to prevent the thin film from adhering thereon. Then, application of a voltage between the low-potential electrodes 2a and 2c and the substrate 16 from an external electric source 3 brings about emission of electrons from electron-emitting regions 4a and 4c (Fig. 15B). To describe another method for preparing the surface conduction electron-emitting device of the present invention, with reference to Figs. 16A to 16G, a wiring electrode 14 is first patterned in the shape of a stripe on a substrate 12 made of glass, quartz or the like (Fig. 16A). Next, an insulating layer 13 is formed on the substrate 12 and wiring electrode 14 (Fig. 16B), and this insulating layer 13 is worked to make a hole by etching as illustrated in Fig. 16C. Subsequently, a metal film is formed by vapor deposition, followed by etching to prepare a high-potential electrode 1 (Fig. 16 D). A thin film 4 is further formed by vapor deposition and a forming treatment is carried out (Fig. 16E). Then a metal film 2 that formed the high-potential electrode 1 is formed by vapor deposition (Fig. 16F), followed by working to make a hole by etching to prepare low-potential electrode 2a and 2c (Fig. 16G). In the above methods, electron-emitting regions 4a and 4c (Figs. 15 and 16) are formed by vapor deposition, but, without limitation thereto, also available is a method in which a dispersion obtained by dispersing fine particles of an electron-emitting material in a dispersion medium is applied by, for example, dipping or spin coating, followed by baking. In this instance, the dispersion medium may be any of those capable of dispersing the fine particles without any change of their properties, and there may be used, for example, alcohols, methyl ethyl ketone, cyclohexane, and a mixture of any of these. The fine particles may preferably have a particle diameter of several ten angstroms to several um. Materials will be described below. Materials for constituting the surface conduction electron-emitting device of the present invention may be any of those used in conventional surface conduction electron-emitting devices. For example, the substrate 16 (Fig. 15) may be made of any materials so long as they are electroconductive, including n-type Si, P-Si, or metals such as Al and Cu. The high-potential electrode 1 and low-potential electrodes 2a and 2c (Figs. 15 and 16), and also the wiring electrode 14 (Fig. 16) may also be made of any materials so long as they are good conductors, and there can be used, for example, metals such as Cu, Pb, Ni, Al, Au, Pt and Ag, and oxides such as SnO₂ andITO. The insulating substrate 5 (Fig. 15) may also be made of any materials so long as the insulating film formed thereon comprises an insulator, but what can be simple in view of preparation methods may preferably include SiO₂ and Al₂O₃ obtainable by oxidation of the substrate. Insulators such as SiO₂, MgO and glass are also used in the substrate 12 and insulating layer 13 (Fig. 16). Further used in the electron-emitting regions 4a, 4c (Figs. 15 and 16) are, for example, metal oxides such as In₂O₃, SnO₂ and PbO, metals such as Ag, Pt, Al, Cu and Au, carbon, and other various semiconductors. As for the size of each component, the high-potential electrode 1 may be made to have a size of from 1 nm to several mm, the electron-emitting regions 4a and 4c may each have a width of the size corresponding to that of a conventional surface conduction electron-emitting device (for example, 1 µm to several ten mm), and the low-potential electrodes 2a and 2c may have any size. The electron-emitting regions 4a and 4c may also each have a thickness corresponding to that of a conventional surface conduction electron-emitting device (for example, several ten Å to several µm). The high-potential electrode 1 and the low-potential electrodes 2a and 2c may have any thickness. Since, however, an excessively large thickness may cause hindrance of electron emission, the high-potential electrode 1 may desirably have a little larger thickness than the film thickness of the electron-emitting regions. The insulating substrate may have any thickness. When the low-potential electrodes 2a and 2c are formed to have a larger thickness than the high-potential electrode 1, in order to they improve the electron beam focusing, should be formed so as to satisfy the relationship of the formulas (a) and (b) previously described. In case where a number of the surface conduction electron-emitting devices are provided in arrangement, the wiring electrode 14 may be formed on the substrate 12 by patterning to have a desired shape such as a stripe on a desired position and then the high-potential electrode 1 may be provided on this wiring electrode 14 as shown in Figs. 16, thus preferably making easy the manufacture. In the instance where the surface conduction electron-emitting device of the present invention has a vertical type structure previously described, an insulating material is used in general as the step-forming layer 15 as illustrated in Fig. 6C and Fig. 12C. For example, the material may be SiO₂, MgO, TiO₂, Ta₂O₅ and Al₂O₃, a laminate of any of these, or a mixture of any of these. The spacing between the electrodes 1 and 2 depends on the thickness of the step-forming layer 15 and the thickness of the electrodes 1 and 2, but may preferably be several ten angstroms to several um. Other component members may employ the same materials and constitution as those previously described. As described above, the surface conduction electron-emitting device of the present invention comprises a high-potential electrode provided on a substrate surface, an electron-emitting region provided in contact with the periphery of an exposed part of said high-potential electrode, and a low-potential electrode further provided in contact with the periphery of said electron-emitting region. It is possible to focus the electron beam to a particular position, i.e., a spot located at the direction perendicular to the center of said device, and moreover decrease the flickering at the light-emitting region. Also, if the low-potential electrode of said device is divided into a plural number of electrodes to provide a plural number of electron-emitting regions, it is possible for the surface conduction electron-emitting device of the present invention to be provided with a spare electron-emitting region. In addition, the surface conduction electron-emitting device of the present invention, when taking the constitution comprising an inside high-potential electrode and an outside low-potential electrode projecting upward in the thickness direction of a substrate, can further enhance the beam-focusing performance, make smaller the size of the electron beam on a target electrode, and make it unnecessary to provide any external focusing lenses. Example 1 A surface conduction electron-emitting device was prepared in a manner shown in Figs. 15A to 15E. The surface of an n-type Si substrate was oxidized to form an insulating film comprising SiO₂, and part thereof was etched to make a hole, followed by vapor deposition of an Al metal film on the whole surface. The resulting deposited film was further etched to prepare high-potential and low-potential electrodes. A thin Au film was further formed thereon by vapor deposition, and a forming treatment was carried out, thus obtaining the surface conduction electron-emitting devices illustrated each in Fig. 1 and Fig. 5. Employment of this surface conduction electron-emitting device brought about a decrease in the flickering as in the prior art. Here, assuming the electron electric current ejected from the surface conduction electron-emitting device as I e , the swing of the electron electric current as ΔI e , and ΔI e /I e as an index of the flickering at the light-emitting region, the surface conduction electron-emitting device of the present invention showed about 1/2 flicker as compared with 16 % flicker in the conventional device (Fig. 17), and the center of the light-emitting spot was positioned at the direction perpendicular to the center of the surface conduction electron-emitting device. Example 2 Example 1 was repeated to prepare the surface conduction electron-emitting device illustrated in Fig. 3. The flickering at the light-emitting region thereof was 1/1.4 of that in the prior art. The center of the light-emitting spot was also positioned at the direction perpendicular to the center of the device. Example 3 Example 1 was repeated to prepare the surface conduction electron-emitting device illustrated in Fig. 4. The flickering at the light-emitting region thereof was 1/1.4 of that in the prior art. The center of the light-emitting spot was also positioned at the direction perpendicular to the center of the device. Example 4 A surface conduction electron-emitting device was prepared in a manner shown in Figs. 16A to 16G. In Figs. 8A and 8B, the numeral 12 denotes a glass substrate, and 14 denotes a wiring electrode which is provided in a stripe pattern on the substrate 12. The material for the wiring electrode 14 was comprised of a laminate of Cr of 50 angstroms thick and Ta of 1,000 angstroms thick. The numeral 13 denotes an insulating layer, which was formed by coating a liquid SiO₂ coating preparation (OCD, available from Tokyo Ohka Kogyo) to a thickness of 1 micron. Photolithoetching was conducted to make a hole in the insulating layer 13, followed by deposition of Cu to a thickness of 1.2 µm thereon, and the copper other than that necessary for the high-potential electrode 1 was removed by photolithoetching. Subsequently, as an electron-emitting material, a solution of an organic palladium compound (Catapaste CCP, available from Okuno Seiyaku Kogyo) was applied thereon by spinner coating. Thereafter, the coating was baked for 1 hour at 400°C to prepare a thin film 4 having a film thickness of 1,500 angstroms and containing Pd fine particles. Next, as a low-potential electrode 2, Al was vapor deposited to a thickness of 10 µm, and, as shown in Fig. 8A and Fig. 8B, the peripheral area of the high-potential electrode 1 was removed by conventional photolithoetching. At the same time, the low-potential electrode 2 was etched to give the shape of a stripe serving also as a wiring electrode. The diameter d₁ of the high-potential electrode 1, the diameter d₂ of the hole of the low-potential electrode 2, and the height h thereof were made to have the following relationship: d 1 ∼ 10 µm d 2 ∼ 14 µm h ∼ 10 µm Application of a voltage of 10 to 20 V applied between the electrode 1 and the electrode 2 brought about emission of electrons from the electron-emitting region 4a. At an upper part of the surface conduction electron-emitting device as in the above, placed was a target electrode coated with a phosphor and applied with an accelerated voltage, and the spreading of the electron beam was measured. As a result, it was confirmed that the spreading was about 3/5 with a remarkable enhancement of the focusing performance, as compared with a surface conduction electron emitting device comprising electrodes 1 and 2 both made equal in thickness. Example 5 The present Example will be described making reference to Fig. 10. In the present Example, the device was made to have the same structure as in Example 4 except that the high-potential electrode 1 was held between two thick low-potential electrodes 2a and 2b from the both sides. A remarkable enhancement of the focusing performance was confirmed also in the present Example. Example 6 The present Example will be described making reference to Fig. 11. In the present Example, the device was made to have the same structure as in Example 4 except that the high-potential electrode 1 was surrounded by four thick low-potential electrodes 2a to 2d. A remarkable enhancement of the focusing performance was confirmed also in the present Example.

Claims: A surface conduction electron-emitting device comprising a high-potential electrode (1) provided on a substrate surface (5) , an electron-emitting region (4) formed by a resistant film and provided in contact with the periphery of an exposed part of said high-potential electrode (1), and a low-potential electrode (2) further provided in contact with the periphery of said electron-emitting region (4), characterized in that said high-potential electrode (1) is surrounded at least to a major portion by said electron-emitting region (4) which, in turn is surrounded at least to a major portion by said low-potential electrode (2), and in that said high-potential electrode (1), said electron-emitting region (4) and said low-potential electrode (2) are positioned such that they are symmetrical upon two major axes contained in the plane of the substrate surface (5). The device according to claim 1, wherein said overall structure is rotationally symmetric. The device according to claim 1 or 2, wherein said low-potential electrode (2) is divided into a plural number of electrodes (2a, 2b, ...). The device according to claim 1, 2 or 3, wherein unevenness is made on the side coming into contact with the electron-emitting region (4) of at least one electrode of the high-potential electrode (1) and the low-potential electrode (2). The device according to any one of claims 1 to 4, comprising a means for applying a voltage between the high-potential electrode and the low-potential electrode. The device according to claim 5, wherein said electron-emitting region (4) emits electrons on flowing an electric current. The device according to claim 5 or 6, wherein said means for applying a voltage is a means for applying an equal magnitude of potential to each of a plurality of low-potential electrodes (2a, 2b, ...). A device according to claim 5 or 6, wherein said means for applying a voltage is a means for applying different potentials independently to each of a plurality of said low-potential electrodes (2a, 2b, ...). The device according to claim 8, wherein said means for applying different potentials is a means capable of independently adjusting the magnitude of the potential to be applied to each of said low-potential electrode (2a, 2b, ...). A device according to any one of claims 1 to 9, wherein said low-potential electrode (2) projects upward in the thickness direction of the substrate (5) to a higher level than the high-potential electrode (1).

Inventors: BANNO YOSHIKAZU, KANEKO TETSUYA, NOMURA ICHIRO, OKUNUKI MASAHIKO, ONO HARUHITO, SHIMIZU AKIRA, SUZUKI HIDETOSHI, TAKEDA TOSHIHIKO, BANNO, YOSHIKAZU, KANEKO, TETSUYA, NOMURA, ICHIRO, OKUNUKI, MASAHIKO, ONO, HARUHITO, SHIMIZU, AKIRA, SUZUKI, HIDETOSHI, TAKEDA, TOSHIHIKO
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1988
Main classification: H01J1
IPC codes: H01J3, H01J1