Patent Application
20080122336
The present invention relates to an electron-emitting device, electron source using the same, and image display apparatus. The present invention also relates to an information displaying and reproducing apparatus such as a television set for receiving a broad casted signal such as television broadcasting, and for displaying and reproducing image information, character information, audio information, which are included in the broad casted signal.
Electron-emitting devices include such as field emission electron-emitting devices and surface conduction electron-emitting devices. As disclosed in Patent Documents 1 to 3, there are some cases where a surface conduction electron-emitting device is performed a process referred to as “activation”. “Activation” process is a process for forming an electroconductive film (typically a carbon film) in a gap between a pair of electroconductive films and on the electroconductive films adjacent to the gap.
An image display apparatus can be formed by opposing a substrate provided with an electron source having a plurality of such electron-emitting devices arranged thereon to a substrate provided with a phosphor film formed of a phosphor or the like and by maintaining vacuum inside.
[Patent Document 1] JP 2000-251642 A
[Patent Document 2] JP 2000-251643 A
[Patent Document 3] JP 2000-231872 A
[Patent Document 4] U.S. Pat. No. 6,380,665
However, an image display apparatus has been recently required to provide a brighter display image for a long time with stability. Therefore, an electron-emitting device which can realize higher electron emitting efficiency with more stability is desired. Here, the electron emitting efficiency is the ratio of current emitted to the vacuum (hereinafter referred to as emission current Ie) to current flowed between the pair of electroconductive films (hereinafter referred to as device current If) when voltage is applied between the pair of electroconductive films. In other words, an electron-emitting device with the lowest possible device current If and the highest possible emission current Ie is desired. If such high electron emitting efficiency can be achieved with stability for a long time, the above-mentioned image display apparatus can be a high quality image display, apparatus providing a brighter image and consuming less power (e.g., a flat TV set).
Accordingly, an object of the present invention is to provide an electron-emitting device with high electron emitting efficiency which materializes satisfactory electron emitting characteristics for a long time and an electron source and an image display apparatus using the same.
The present invention has been made to solve the above-mentioned problems. According to the present invention, there is provided an electron-emitting device including: a substrate; and first and second electroconductive films disposed on the substrate in opposition to each other to form a gap between ends of the first and second electroconductive films, in which the end of the first electroconductive film have a protrusion protruding toward the second electroconductive film such that a minimum distance d1, which in defined as a distance between an end of the protrusion and the second electroconductive film and which is 10 nm or less, and a minimum distance d2, which is defined as a distance between the second electroconductive film and an edge portion of the first electroconductive film being away from the end of the protrusion by d1, meets a relation: d2/d1≧1.2.
According to the present invention, an electron-emitting device includes: a substrate; and first and second electroconductive films disposed on the substrate in opposition to each other to form a gap between ends of the first and second electroconductive films, in which the first electroconductive film has a first portion at which a minimum distance between the first and second electroconductive films is defined as d1, which is 10 nm or less, and wherein the first electronconductive film has a second portion being away from the first portion by d1, at which a minimum distance between the first and second electroconductive films is defined as d2, and wherein the distance d1 and the distance d2 meet a relation: d2/d1≧1.2.
Further, according to the present invention, the electron-emitting device includes: “the edge portion of meet is in a plane including the protrusion and being parallel to a surface of the substrate”; “the first electroconductive film has a plurality of protrusions arranged so as not to be overlapped with each other in a direction normal to a surface of the substrate”; “the plurality of protrusions are arranged at an interval of 3 d1 or more”; “the plurality of the protrusions are arranged at an interval of 2000 d1 or more”; “the gap extends in a staggering manner”; “the first and second electroconductive films contain carbon”; and “the substrate has a concave on a surface thereof between the first and second electroconductive films”.
According to the present invention, an electron source includes a plurality of the electron-emitting devices according to the present invention and an image display apparatus including the electron source and a phosphor are provided.
According to the present invention, an information displaying and reproducing apparatus includes: a receiver for outputting at least one of an image information, a character information and an audio information contained in a broadcasted signal received; and an image display apparatus connected to the receiver, wherein the image display apparatus is prepared.
According to the present invention, an electron-emitting device with dramatically improved electron emitting efficiency can be provided. As a result, an image display apparatus and an information displaying and reproducing apparatus with excellent display quality for a long time can be provided.
Further, according to the present invention, since, when voltage is applied between the first and second electroconductive films to emit electrons, d2/d1 is 1.2 or more, changing the distribution of electric potential in proximity to the end of the first electroconductive film changes the trajectory of the emitted electrons, and as a result, increases the emission current Ie which reaches an anode (the efficiency becomes higher).
Embodiments of an electron-emitting device according to the present invention will be described in the following. First, an exemplary basic structure of an electron-emitting device according to the present invention is described with reference to
In
When the electron-emitting device as shown in
It is preferable that, in view of the stability of the emission current, the end of the first electroconductive film 21a on the side of the second electroconductive film 21b is provided with a lot of such protrusions (portions A) toward the second electroconductive film 21b as illustrated in
The portions B of the second electroconductive film 21b can be typically referred to as portions of the second electroconductive film 21b and also referred to as portions of the second electroconductive film 21b which are nearest to the portions A. The gap between a portion A and a portion B can be defined as “d1”. In order to set drive voltage necessary for emitting electrons to be 50 V or lower, preferably 20 V or lower, d1 is set to be 10 nm or less, preferably 5 nm or less. In view of the stability when the electron-emitting device is driven and reproducibility in manufacturing, d1 is preferably set to be 1 nm or more, and more preferably set to be 3 nm or more.
The minimum distance between an end of the first electroconductive film 21a on the side of the second electroconductive film 21b (a portion C) and an end of the second electroconductive film 21b on the side of the first electroconductive film 21a (a portion D) in opposition to the end (the portion C), which is away from a protrusion (a portion A) of the first electroconductive film 21a by the distance “d1” is defined as “d2”. More specifically, the minimum distance between the end of the first electroconductive film 21a on the side of the second electroconductive film 21b (the portion C) and the end of the second electroconductive film 21b on the side of the first electroconductive film 21a (the portion D) in opposition to the end (the portion C), which is away from a protrusion of the first electroconductive film 21a along the end of the first electroconductive film 21a forming the periphery (edge) of the gap 8 in a plane substantially in parallel to the surface of the substrate 1 by the same distance as d1 is defined as “d2”.
It is to be noted that d1 is sufficiently small (10 nm or less). Therefore, the above-described “d2” may be defined as the minimum distance between an end of the first electroconductive film 21a on the side of the second electroconductive film 21b (a portion C) which is away by the same distance as “d1” in a direction perpendicular to a line through the portions A and B defining the above-described “d1” and an end of the second electroconductive film 21b on the side of the first electroconductive film 21a (a portion D) in opposition to the end (the portion C). More specifically, the above-described “d2” may be defined as the minimum distance between the end of the first electroconductive film 21a on the side of the second electroconductive film 21b (the portion C) which is away by the same distance as d1 in the direction perpendicular to the line through the portions A and B defining the above-described d1 in the plane substantially in parallel to the surface of the substrate 1 and the end of the second electroconductive film 21b on the side of the first electroconductive film 21a (the portion D) in opposition to the end (the portion C) (see
It is to be noted that “d2” may be 10 nm or less. However, the end of the first electroconductive film 21a (the portion C) which defines “d2” does not correspond to the above-described protrusion (a portion A). More specifically, suppose that the portion C is the above-described protrusion (the portion A), the above-described portion A would exist within “d2” from the portion C, and the distance from the portion A to the second electroconductive film 21b is less than d2. Therefore, according to the present invention, if a portion is defined as the portion A, there would exist no portion where the distance between the first electroconductive film 21a and the second electroconductive film 21b is less than d1 within d1 from the portion A.
Further, as described above, according to the present invention, it is preferable that the electron-emitting device has a lot of such portions A. In such a case, the distance from the portion A to the surface of the substrate 1 (the height of the portion A from the surface of the substrate 1) may be varied. However, in view of the stability of the electron emitting characteristics, it is preferable that the difference in the distance from the plurality of portions A to the surface of the substrate 1 is effectively within d1. Further, the portions A are preferably not arranged perpendicularly to the surface of the substrate 1. In other words, it is preferable that the plurality of portions A are not arranged in the direction of the film thickness of the first electroconductive film 21a.
The thickness of the electroconductive films (21a and 21b) is very small, and practically 1 μm or less and 1 nm or more, preferably 500 nm or less and 1 nm or more, and more preferably 200 nm or less and 1 nm or more. Therefore, arrangement of a lot of such portions A in the perpendicular direction may lead to fluctuations in the electron emitting characteristics over time. This is the reason why it is preferable that the portions A are not arranged perpendicularly.
According to the present invention, d1 is 10 nm or less, and at the same time, the above-described ratio of d1 to d2 (d2/d1) is set to be 1.2 or more. Under these conditions, large emission current Ie and high electron emitting efficiency can be obtained.
It is to be noted that
Further, in the configurations illustrated in
Still further, a distance d3 between the portions (protrusions) is preferably set to be 3 d1 or more and 2000 d1 or less. In view of an increase of the emission current Ie and/or suppressing fluctuations in the amount of emitted electrons, it is more preferable that the distance d3 is set to be uniform.
When such an electron-emitting device is used in a high definition display, an area assigned to one electron-emitting device is small. Therefore, there is a tendency that fluctuations in the emission current (Ie) become larger with regard to an electron-emitting device having the smaller number of the portions A (protrusions) compared with an electron-emitting device having the larger number of the portions A. As a result, uniformity of an image displayed on the display is lowered. As a practical range, the distance d3 between the portions A (protrusions) is set to be 2000 d1 or less, and more preferably, to be 500 d1 or less. If the distance d3 is in this range, the fluctuations of the emission current Ie can be suppressed. Although it is preferable that the distance d3 between the portions A (protrusions) is uniform, it may have a distribution to some extent.
Next, a variation of the above-described electron-emitting device according to the present invention will be described with reference to
In such a manner as the above item (1), if the protrusions (portions A) are arranged at uniform intervals, as compared with a case where the gap 8 is linear, more protrusions (portions A) can be provided, and thus, the electron emitting characteristics are thought to be made more stable. Further, in such a manner as the above item (2), voltage can be applied between the electroconductive films 21a and 21b with stability.
In this configuration, the first and second auxiliary electrodes (2 and 3) and the first and second electrodes (4a and 4b) are used. However, according to the present invention, as in the configurations described with reference to
However, in order to connect with stability a power source (voltage supply source) for driving the electron-emitting device according to the present invention to the electroconductive films (21a and 21b) which are very thin, it is preferable to use the auxiliary electrodes (2 and 3) and/or the electrodes (4a and 4b). By connecting terminals of the power source to the electrodes (4a and 4b) or the auxiliary electrodes (2 and 3), voltage can be applied between the electroconductive films (21a and 21b) with stability. Therefore, the auxiliary electrodes (2 and 3) and/or the electrodes (4a and 4b) can be suitably applied also to the configurations of the electron-emitting device described with reference to
According to the present invention, it is preferable that the electron-emitting device including the configurations described with reference to
By providing such a concave 22, ineffective current between the first electroconductive film 21a and the second electroconductive film 21b which is not the emission current Ie is thought to be suppressed. Further, according to the present invention, it is preferable that, as illustrated in
When the above-described electron-emitting device according to the present invention is driven, for example, as illustrated in a schematic structural view of
Here, the field intensity used when the electron-emitting device according to the present invention is driven (when electrons are emitted) (the intensity of electric field applied between the first and second electroconductive films 21a and 21b) is effectively 1×109 V/m or more and less than 2×1010 V/m. If the field intensity is less than this range, the number of electrons which tunnel becomes considerably small, and if the field intensity is more than this range, the first electroconductive film 21a and/or the second electroconductive film 21b may be deformed by the intense electric field, and often electrons are not emitted with stability.
According to the present invention, by setting d2/d1 to be 1.2 or more as described above, the electron-emitting device can decrease the number of electrons absorbed in the second electroconductive film 21b. As a result, the electron emitting efficiency ((current which reaches the anbde)/(current which flows between the first and second electroconductive films 21a and 21b)) can be improved. The reason for this is that strong force away from the surface of the substrate 1 (toward the anode) acts on electrons which have tunneled from the portions A toward the portions B (including electrons scattered in proximity to the portions B) due to the electric field formed by setting d2/d1 to be 1.2 or more.
A variation of the electron-emitting device described with reference to
According to this configuration, the electron-emitting device has, in addition to the features described with reference to
With this configuration, as compared with the electron-emitting device described with reference to
The thickness of the second electroconductive film 21b at the portion B is set to be smaller than that of the second electroconductive film 21b at the portions 35 and 36 (see
Therefore, there is a difference of “h” between the height of the surface of the portions 35 and 36 of the second electroconductive film 21b from the surface of the substrate 1 and the height of the surface of the portion B from the surface of the substrate 1 (“h” may be referred to as the height of the projected portions).
Further, the second electroconductive film 21b has at least two projected portions, and there is a width “w” between the two projected portions. The width w can be, effectively, defined as a gap between portions of the respective “projected portions” which are farthest away from the surface of the substrate (defined as a gap between points (tops or apexes or summits) of the respective “projected portions”). Further, it is preferable that the width w between the above-described “projected portions” is effectively set to be 2 d1 or more and 50 d1 or less. If the width w is in this range, large emission current Ie and high electron emitting efficiency can be obtained. It is to be noted that the height of the point of the portion 35 from the surface of the substrate 1 and the height of the point of the portion 36 from the surface of the substrate 1 may be different from each other.
The height h of the above-described “projected portions” can be, effectively, defined as a value determined by subtracting the distance between the portion B and the surface of the substrate 1 from the distance between the portion of one of the “projected portions” (typically one “projected portion” of the two projected portions (35 and 36) sandwiching the portion B the height of which from the surface of the substrate 1 is smaller than that of the other projected portion) which is farthest away from the surface of the substrate 1 and the surface of the substrate 1. It is preferable that the height h of the “projected portions” is set to be 2 d1 or more and 200 d1 or less.
According to the present invention, as described above, the portions A and B form a part of the periphery of the gap 8 of the electron-emitting device. In order to improve the electron emitting efficiency, it is preferable that the portions 35 and 36 of the second electroconductive film 21b also form the periphery of the gap 8.
Further, according to the present invention, it is preferable that, where the gap between the first and second electroconductive films 21a and 21b is smaller than that of other portions (between the portions A and B in
This can improve the electron emitting efficiency of the electron-emitting device as described with reference to
It is to be noted that
A conductive material such as a metal or a semiconductor including Ni, Au, PdO, Pd, Pt, and C may be used as the material for the electroconductive films (21a and 21b). More preferably, the electroconductive films are films containing carbon in view of a large amount of electron emission and stability over time. Further, practically, it is preferable that the films containing carbon as the main component (more specifically, films containing 70 atoms percent of carbon) are used. When, in this way, the electroconductive films (21a and 21b) are formed by films containing carbon, the electroconductive films (21a and 21b) may be referred to as carbon films.
Next, a method of manufacturing an electron-emitting device according to the present invention will be described.
Although there are many manufacturing methods, the electron-emitting device according to the present invention can be manufactured by, for example, the following processes (1) to (5). Of course, the electron-emitting device according to the present invention is not limited to one manufactured by the below-described manufacturing method.
Exemplary manufacturing methods are described with reference to schematic views of
After the substrate 1 is sufficiently cleaned, a material for forming the auxiliary electrodes 2 and 3 is deposited using vacuum evaporation, sputtering, or the like. Then, the first and second auxiliary electrodes 2 and 3 are formed by using photolithography or the like (
Exemplary materials for the substrate 1 includes quartz glass, soda lime glass, a glass substrate having silicon oxide (typically SiO2) laminated thereon, the silicon oxide being formed by a known film forming method such as sputtering, and a glass substrate with its alkali component decreased. In this way, according to the present invention, a material containing silicon oxide (typically SiO2) is preferable for the material of the substrate.
A length L between the auxiliary electrodes 2 and 3, a length W (see
An electroconductive thin film 4 for connecting the first and second auxiliary electrodes 2 and 3 provided on the substrate 1 is formed (
Exemplary materials for the electroconductive thin film 4 include electroconductive materials such as metals and semiconductors. For example, metals such as Ni, Cr, Au, Mo, W, Pt, Ti, Al, Cu, Pd, Ag and the like and alloys thereof, metal oxides such as PdO, RuO2, transparent conductors such as In2O3—SnO2, and semiconductors such as polysilicon can be used.
It is to be noted that exemplary organic metal solutions include solutions of organic metal compounds the main element of which is Pd, Ni, Au, Pt, or the like of the above-described conductive film material. Although a method of forming the electroconductive thin film 4 by applying an organic metal solution is described here, the method of forming the electroconductive thin film 4 is not limited thereto, and the electroconductive thin film 4 may be formed also by vacuum evaporation, sputtering, CVD, dispersion and application, dipping, spinning, ink jet, or the like.
When “forming” process is carried out in the next process, it is preferable that Rs (sheet resistance) of the electroconductive thin film 4 is in the range of 102Ω/□ to 107Ω/□. It is to be noted that Rs is a value expressed as R=Rs (l/w) where R is resistance in the length direction of a film having the thickness t, the width w, and the length l. When the resistivity is ρ, Rs=ρ/t. Specifically, the film thickness having the above resistance ranges from 5 nm to 50 nm. Further, the width W′ of the electroconductive thin film 4 (see
Next, process called as “forming” is carried out by applying voltage between the auxiliary electrodes 2 and 3. Application of the voltage forms a second gap 7 in a part of the electroconductive thin film 4. As a result, the first and second electrodes 4a and 4b can be disposed in opposition to each other in a lateral direction with respect to the surface of the substrate 1 with the second gap 7 therebetween (
Electric processing after the “forming” process can be carried out by, for example, disposing the substrate 1 in a measurement/evaluation apparatus illustrated in
The “forming” process may be carried out by repeatedly applying a voltage pulse the pulse height value of which is a constant voltage (constant). Alternatively, the “forming” process may be carried out by applying a voltage pulse with the pulse height value gradually increased.
Next,
In the examples described above, when the gap 7 is formed, pulse-like voltage (voltage pulse) is applied between the auxiliary electrodes 2 and 3 to carry out the “forming” process. However, the waveform of the pulse applied between the auxiliary electrodes 2 and 3 is not limited to triangular, and a desired waveform such as a square one may be used. Further, the pulse height value, the pulse width, the pulse interval, and the like are not limited to the above-described values. Appropriate values can be selected according to the resistance of the electroconductive film 4 and the like such that the gap 7 is satisfactorily formed.
Here, a method is illustrated where the first and second electrodes 4a and 4b are formed by carrying out the “forming” process with respect to the electroconductive thin film 4. However, according to the present invention, the first and second electrodes 4a and 4b can be formed using a known patterning technique such as photolithography. Further, when the first and second carbon films 21a and 21b are formed using “activation” process described below, since it is preferable that the gap 7 between the first and second electrodes 4a and 4b is small, the above-described “forming” process is preferably adopted. However, a method where the gap 7 is formed in the electroconductive thin film 4 by irradiating the electroconductive thin film 4 with focused ion beams (FIB) or electron beam lithography may be used to form the first and second electrodes 4a and 4b with a small gap 7 therebetween. Further, if the gap L between the first and second auxiliary electrodes 2 and 3 can be made small (comparable to gap 7) by the various techniques described above, the first and second electrodes 4a and 4b are not necessarily required. However, in order to manufacture the electron-emitting device according to the present invention at a low cost, it is preferable to use the above-described auxiliary electrodes 2 and 3 as electrodes for supplying with stability potential to the carbon films (21a, 21b) formed by the “activation” process described below, and to use the first and second electrodes 4a and 4b as electrodes for depositing with stability at high speed the carbon films (21a, 21b) at the beginning of the “activation” process.
Next, “activation” process is carried out (
An organic material gas may be used as the above-mentioned carbon-containing gas. Organic materials may include: aliphatic hydrocarbons composed of alkanes, alkenes, and alkynes; aromatic hydrocarbons; and organic acids such as alcohols, aldehydes, ketones, amines, phenol, carboxylic acid, and sulfonic acid. Specifically, organic materials including: saturated hydrocarbons represented by Cn H2n+2 such as methane, ethane, and propane; unsaturated hydrocarbons represented by Cn H2n such as ethylene and propylene; benzene; toluene; methanol; ethanol; formaldehyde; acetaldehyde; acetone; methylethylketone; methylamine; ethylamine; phenol; formic acid; acetic acid; and propionic acid can be used.
It is preferable that the above-described carbon-containing gas is introduced into the vacuum chamber after being once depressurized to be on the order of 10−6 Pa. The preferable partial pressure of the carbon-containing gas depends on the form of the electron-emitting device, the shape of the vacuum chamber, the carbon-containing gas to be used, and the like, and is set appropriately.
As the waveform of the voltage applied between the auxiliary electrodes 2 and 3 during the above-described “activation” process, it is preferable to use, for example, a pulse waveform having both polarities (a bipolar voltage pulse) illustrated in
By applying voltage having the waveform illustrated in
On the other hand, by applying voltage having the asymmetrical waveform illustrated in
Either the waveform illustrated in
When the temperature of the substrate rises under the presence of SiO2 (material of the substrate) in the vicinity of carbon, Si is consumed:
SiO2+C→SiO⇑+CO⇑.
It is thought that this chemical reaction consumes Si in the substrate to form the shape where the surface of the substrate is cut (the concave).
The transformed portion of the substrate (concave) 22 increases the distance between the first and second carbon films 21a and 21b along the surface of the substrate. Therefore, electric discharge due to the strong electric field applied between the first and second carbon films 21a and 21b when the device is driven and excess device current If can be suppressed.
Carbon in the first and second carbon films 21a and 21b, which are films containing carbon according to the present invention is now described. Carbon contained in the carbon films (21a and 21b) is preferably graphite-like carbon. Graphite-like carbon according to the present invention includes carbon having the complete crystal structure of graphite (so-called HOPG), carbon having slight irregularities with the grain size of about 20 nm, (PG), carbon having larger irregularities with the grain size of about 2 nm (GC), and amorphous carbon (amorphous carbon and/or a mixture of amorphous carbon and above-described graphite crystallite). In other words, even there are irregularities in layers such as grain boundaries between graphite grains in the graphite-like carbon, it can be suitably used.
Next, processing for shaping the first and second carbon films 21a and 21b into the shape illustrated in
More specifically, by a method using, for example, an atomic force microscope (AFM) illustrated in
The above-described processing using the AFM can be carried out as in the following, for example.
First, a case where the electron-emitting device illustrated in
As described above, when the electron-emitting device illustrated in
Next, a case where the electron-emitting device illustrated in
As described above, when the electron-emitting device illustrated in
The electron-emitting device according to the present invention having the structure illustrated in
Process 1 to Process 3 are similar to the above-described case. The “activation” process in Process 4 may use a similar carbon-containing gas. This process is similar to the above-described Process 4 except that a symmetrical pulse waveform illustrated in
This method is described in the following with reference to
A diameter of an electron beam emitted from an electron emitting means 41 need not be narrowed to the gap 8, and preferably has a range of 1 μm or larger with the gap 8 being the center, taking into consideration the voltage applied between the auxiliary electrodes 2 and 3, the partial pressure of the carbon-containing gas during the “activation” process, and the like. However, if the range of irradiation with the electron beam is too large, the carbon compound may deposit even on a region where it is unnecessary. Therefore, it is preferable to block the electron-beam emitted from the electron emitting means 41 by an electron beam blocking means 42 to suppress the spread of the electron beam. The electron beam irradiation is preferably continuous (DC-like) with the voltage applied between the auxiliary electrodes being pulse-like. The pulse voltage applied between the auxiliary electrodes 2 and 3 preferably has a waveform and voltage values illustrated in
This also allows manufacture of the electron-emitting device having the structure illustrated in
Another exemplary method of manufacturing the electron-emitting device illustrated in
The auxiliary electrodes 2 and 3 are formed on the substrate 1 in a similar way as in the above-described Process 1 (
Next, the first carbon film 21a and the second carbon film 21b are formed in a desired shape between the first and second auxiliary electrodes 2 and 3 through electron beam irradiation (
The carbon films 21a and 21b can be formed with the substrate 1 disposed within the above-described measurement/evaluation apparatus illustrated in
As the carbon-containing gas, a gas similar to the carbon-containing gas described above (Process 4) may be used. When the carbon films 21a and 21b are formed, no voltage is applied to the auxiliary electrodes 2 and 3, and the auxiliary electrodes 2 and 3 are set at the ground voltage. By irradiating the surface of the first and second auxiliary electrodes 2 and 3 and the surface of the substrate between the auxiliary electrodes 2 and 3 with an electron beam narrowed and deflected by the electron beam blocking/deflecting means 42, the carbon films 21a and 21b in the shape illustrated in
The reason that the carbon films 21a and 21b are deposited is thought to be that the carbon-containing gas existing in the atmosphere or a carbon compound attached to the electrodes 2 and 3 and the substrate 1 due to adsorption of the carbon-containing gas on the electrodes 2 and 3 and the substrate 1 are decomposed by irradiating the electron beam, which results in deposition of carbon.
The acceleration voltage of the electron beam is preferably set to be about 1 kV to 20 kV. The electron beam irradiation is preferably continuous (DC-like). The current of the electron beam is preferably in the range of 0.1 uA to 100 uA.
In this way, the electron-emitting device according to the present invention can be manufactured.
It is to be noted that the method of manufacturing the electron-emitting device according to the present invention described with reference to
Excess carbon and organic substances attached to or deposited on the surface of the substrate 1 and other locations of the electron-emitting device according to the present invention manufactured as described above due to the above-described “activation” process and the like are preferably removed before the device is practically driven (when applied to an image display apparatus, before a phosphor is irradiated with an electron beam) by, preferably, carrying out “stabilization” process, which is heating process in a vacuum.
More specifically, in a vacuum container, excess carbon and organic substances are discharged. It is desirable that the organic substances in the vacuum container are discharged as much as possible, and it is preferable that the organic substances are eliminated such that the partial pressure thereof is 1×10−8 Pa or lower. Further, the total pressure in the vacuum container of gases including gases other than the organic substances is preferably 3×10−6 Pa or lower, and particularly preferably 1×10−7 Pa or lower. Further, when discharge is carried out from within the vacuum container, it is preferable that the whole vacuum container is heated.
When the electron-emitting device is driven after the “stabilization” process, it is preferable that the atmosphere when the “stabilization” process is completed is maintained, but the present invention is not limited thereto. So far as the organic substances are sufficiently removed, even if the pressure itself becomes higher, sufficiently stable characteristics can be maintained.
Next, basic properties of the electron-emitting device according to the present invention are described with reference to
Since the emission current Ie is considerably smaller than the device current If, the respective measures of current are selected accordingly in
First, the emission current Ie of the electron-emitting device according to the present invention suddenly begins to increase when the applied device voltage reaches a certain level (Vth in
Second, since the emission current Ie depends on the device voltage Vf, the emission current Ie can be controlled by the device voltage Vf.
Third, the emitted electric charge captured by the anode electrode 44 depends on the time period during which the device voltage Vf is applied. In other words, the amount of electric charge captured by the anode electrode 44 can be controlled by the time period during which the device voltage Vf is applied.
By utilizing the above properties of the electron-emitting device, the electron emitting characteristics can be easily controlled according to an input signal.
Although a case where the electron-emitting device is disposed on a plate-like substrate 1 is described here, the electron-emitting device according to the present invention may be disposed on an upper surface or a side surface of an insulating member in a predetermined shape (i.e., in a cubic shape or polyhedron) prepared on the substrate. In particular, by disposing a side surface of the insulating member so as to form an angle with respect to the plane of the anode electrode 44 and disposing the electron-emitting device according to the present invention on the side surface (by setting the opposed direction between the electroconductive films 21a and 21b to a direction heading to the anode), the electron emitting efficiency can be improved. For example, when the electron-emitting device having the structure illustrated in
Next, a method of observing the neighborhood of the gap 8 of the electron-emitting device according to the present invention illustrated in
A plan SEM, a section SEM, a section TEM, 3D-TEM (tomography), or the like can be used for the observation. When a microstructure such as that of the electron-emitting device according to the present invention is observed, it is preferable to use 3D-TEM (tomography).
In order to obtain a 3D-TEM image, first, the substrate 1 is cut (etched) from a side opposite to the surface where the electron-emitting device is disposed (from a rear side) (
Next, an exemplary application of the electron-emitting device according to the present invention is described in the following.
A plurality of the electron-emitting devices according to the present invention can be arranged on a substrate to form, for example, an electron source or an image display apparatus such as a flat panel television set.
Exemplary arrangements of the electron-emitting devices on the substrate includes an arrangement where m X-directional wirings and n Y-directional wirings are prepared and the first electroconductive film 21a (typically the first auxiliary electrode 2) of the electron-emitting device according to the present invention is electrically connected to one of the m X-directional wirings, while the second electroconductive film 21b (typically the second auxiliary electrode 3) is electrically connected to one of the n Y-directional wirings (referred to as a “matrix arrangement”) (m and n are positive integers).
Next, this matrix arrangement is described in detail.
According to the above-described three basic properties of the electron-emitting device according to the present invention, when the voltage is the threshold voltage or higher, the electron-emitting device can be controlled by the pulse height value and the width of the pulse-like voltage applied between the first and second electroconductive films 21a and 21b. On the other hand, when the voltage is lower than the threshold voltage, substantially no electrons are emitted. According to this property, even when a lot of electron-emitting devices are arranged, by appropriately applying the above-described pulse-like voltage to the respective electron-emitting devices, the amount of electrons emitted from a selected electron-emitting device can be controlled based on an input signal.
Next, a structure of an electron source substrate of matrix arrangement formed based on the above is described with reference to
M X-directional wirings 72 Dx1, Dx2, . . . , Dxm are formed on an insulating substrate 71 using vacuum evaporation, printing, sputtering, or the like. The X-directional wirings 72 are made of a conductive material such as a metal. N Y-directional wirings 73 Dy1, Dy2, . . . , Dyn may be formed by a similar method and may be made of a similar material to those of the X-directional wirings 72. An insulating layer (not shown) is disposed between the m X-directional wirings 72 and n Y-directional wirings 73. The insulating layer may be formed using vacuum evaporation, printing, sputtering, or the like.
A scan signal applying means (not shown) for applying a scan signal is electrically connected to the X-directional wirings 72. A modulation signal applying means (not shown) for applying a modulation signal for modulating an electron emitted from a selected electron-emitting device in synchronization with a scan signal is electrically connected to the Y-directional wirings 73. Drive voltage Vf applied to the electron-emitting devices is supplied as difference voltage between the applied scan signal and the modulation signal.
Next, an exemplary electron source and an exemplary image display apparatus using the electron source substrate of matrix arrangement are described with reference to
In
The container (display panel) 88 can be formed by the face plate 86, the support frame 82, and the rear plate 81. However, the main object of providing the rear plate 81 is to reinforce the substrate 71. Therefore, when the substrate 71 itself is strong enough, the rear plate 81 is not necessary. In that case, the support frame 82 may be directly seal-bonded to the substrate 71 such that the face plate 86, the support frame 82, and the substrate 71 form the container (display panel) 88.
Further, by providing a support member called a spacer (not shown) between the face plate 86 and the substrate 71, the container 88 can be sufficiently strong against atmospheric pressure.
An electroconductive film 85 referred to as a “metal back” is provided on the inner surface side (on the side of the electron-emitting device 74) of the phosphor film 84. The electroconductive film 85 is provided in order to specularly reflect light toward the side of the electron-emitting device 74 out of light emitted from the phosphor 92 to the side of the face plate 86 to improve the brightness, in order to utilize the electroconductive film 85 as an electrode for applying voltage for accelerating the electron beam, in order to suppress damage of the phosphor due to collision of negative ions generated in the envelope 88, and the like.
The electroconductive film 85 is preferably an aluminum film. The electroconductive film 85 may be formed by, after the phosphor film 84 is formed, smoothing the surface of the phosphor film 84 (normally referred to as “filming”), and after that, depositing Al using vacuum evacuation or the like.
The face plate 86 may be provided with a transparent electrode (not shown) made of ITO or the like between the phosphor film 84 and the transparent substrate 83 in order to enhance the conductivity of the phosphor film 84.
By applying voltage to the respective electron-emitting devices 74 in the envelope 88 via terminals Dox1 to Doxm and Doy1 to Doyn connected to the X-directional wirings and Y-directional wirings which are described with reference to
The details of the above-described structure such as the materials of the members are not limited to the above, and are appropriately changed according to the object.
The container (display panel) 88 according to the present invention described with reference to
More specifically, the information displaying and reproducing apparatus includes a receiver for receiving a broadcast signal for television broadcast or the like, a tuner for selecting a received signal, and an image display apparatus for outputting at least one of image information, character information, and audio information contained in the selected signal to the display panel 88 to display and/or reproduce the information on a screen. It can be said that the “screen” here corresponds to the phosphor film 84 of the display panel 88 illustrated in
Outputting image information or character information to the display panel 88 to display and/or reproduce the information on the screen can be carried out in the following way. For example, first, image signals corresponding to the respective pixels of the display panel 88 are generated from the received image information or character information. Then, the generated image signals are inputted to a drive circuit of the display panel 88. Next, based on the image signals inputted to the drive circuit, voltage applied from the drive circuit to the respective electron-emitting devices in the display panel 88 is controlled to display the image.
The I/F unit C30 may be configured to be connected to an image recording device or an image output device such as a printer, a digital video camera, a digital camera, a hard disk drive (HDD), or a digital video disk (DVD). This can configure an information displaying and reproducing apparatus (or a television set) with which an image recorded in the image recording device can be displayed on the display panel 88, and an image displayed on the display panel 88 can be processed as needed and can be outputted to the image output device.
The structure of the information displaying and reproducing apparatus is only an example and various variations are possible based on the technical idea of the present invention. Further, the information displaying and reproducing apparatus according to the present invention can form various kinds of information displaying and reproducing apparatus by connecting it to a videoconference system, a computer system, or the like.
The present invention is now described in further detail with reference to examples.
The basic structure of an electron-emitting device according to this example is similar to that illustrated in
First, photoresist shaped correspondingly to the pattern of the auxiliary electrodes 2 and 3 was formed on the cleaned quartz substrate 1. Then, Ti at the thickness of 5 nm and Pt at the thickness of 45 nm were deposited in this order by electron beam vapor deposition. The photoresist pattern was dissolved away by organic solvent, the Pt/Ti deposition film was lifted off, and the first and second auxiliary electrodes 2 and 3 in opposition to each other with a length L of 20 μm therebetween were formed. The width W of the auxiliary electrodes 2 and 3 (see
After an organic palladium compound solution was spin coated by a spinner so as to connect the first and second auxiliary electrodes 2 and 3, bake processing were carried out. In this way, an electroconductive thin film the main component of which was Pd was formed.
Next, the electroconductive thin film was patterned to form the electroconductive thin film 4 (
The device electrodes 2 and 3 and the electroconductive thin film 4 were formed through the above-described processes.
Next, the substrate 1 was disposed in the measurement/evaluation apparatus illustrated in
In
Next, in order to carry out the “activation” process, acrylonitrile was introduced into the vacuum chamber through a slow leak valve and 1.3×10−4 Pa was maintained. Then, the pulse voltage having the waveform illustrated in
After 100 minutes lapsed from the beginning of the “activation” process, it was confirmed that the graph entered deep enough the region which was on the right side of the dotted line in
In this process, electron-emitting devices A which underwent “activation” process with the highest voltage value being ±14 V, electron-emitting devices B which underwent “activation” process with the highest voltage value being ±16 V, and electron-emitting devices C which underwent “activation” process with the highest voltage value being ±18 V were manufactured. Eight electron-emitting devices A (A1 to A8) in total were manufactured by the same manufacturing method as described above. Six electron-emitting devices B (B1 to B6) in total were manufactured by the same manufacturing method as described above. Four electron-emitting devices C (C1 to C4) in total were manufactured by the same manufacturing method as described above.
SEM plan images and SEM section images of electron-emitting devices (A′, B′, and C′) manufactured by the same manufacturing method as Process-a to Process-e in the above were observed. It was found that, regardless of the voltage applied in the “activation” process, the thickness of the end of the first carbon film 21a (the portion forming the periphery of the gap 8) and the thickness of the end of the second carbon films 21b (the portion forming the periphery of the gap 8) are almost the same, and the gap 8 was serpentine. Further, in all the electron-emitting devices, there were a lot of portions (portions A and B) where the gap between the first and second electroconductive films 21a and 21b is smaller than that in other portions.
3D-TEM image in the neighborhood of the gap 8 of the electron-emitting devices (A′, B′, and C′) manufactured by the same manufacturing method as that of the respective electron-emitting devices A, B, and C was observed. The distance d1 between a portion A of the first carbon film 21a and a portion B of the second carbon film 21b was 2.3 nm on average with regard to the electron-emitting devices A′, 2.8 nm on average with regard to the electron-emitting devices B′, and 3.3 nm on average with regard to the electron-emitting devices C′.
The minimum distance d2 between a portion of the first electroconductive film 21a which is away from a portion A along the periphery of the gap 8 by the same distance as d1 and a portion of the second electroconductive film 21b in opposition to that portion which was measured using 3D-TEM images was 2.5 nm on average with regard to the electron-emitting devices A′ (d2/d1 was 1.1 or less with regard to all the electron-emitting devices A′), 3.0 nm on average with regard to the electron-emitting devices B′ (d2/d1 was 1.1 or less with regard to all the electron-emitting devices B′), and 3.5 nm on average with regard to the electron-emitting devices C′ (d2/d1 was 1.1 or less with regard to all the electron-emitting devices C′).
Then, the electron-emitting devices according to this example (A, B, and C) after Process-e were taken out from the measurement/evaluation apparatus illustrated in
In this example, first by cutting the end of the first carbon film 21a using an AFM, the distance d1 between a portion A and a portion B was set to be 2.5 nm with regard to all the electron-emitting devices A (A1 to A8), 3.0 nm with regard to all the electron-emitting devices B (B1 to B6), and 3.5 nm with regard to all the electron-emitting devices C (C1 to C4).
Further, each of the end of the first carbon film 21a was processed using an AFM such that d2 of the electron-emitting device A1 was 2.8 nm, d2 of the electron-emitting device A2 was 3.0 nm, d2 of the electron-emitting device A3 was 3.3 nm, d2 of the electron-emitting device A4 was 3.6 nm, d2 of the electron-emitting device A5 was 4.0 nm, d2 of the electron-emitting device A6 was 4.2 nm, d2 of the electron-emitting device A7 was 5.0 nm, and d2 of the electron-emitting device A8 was 10 nm. It is to be noted that d2/d1 was 1.1 with regard to the electron-emitting device A1 and was 1.2 or more with regard to the electron-emitting devices A2 to A8.
Further, each of the end of the first carbon film 21a was processed using an AFM such that d2 of the electron-emitting device B1 was 3.3 nm, d2 of the electron-emitting device B2 was 3.6 nm, d2 of the electron-emitting device B3 was 4.0 nm, d2 of the electron-emitting device B4 was 4.2 nm, d2 of the electron-emitting device B5 was 5.0 nm, d2 of the electron-emitting device B6 was 10 nm. It is to be noted that d2/d1 was 1.1 with regard to the electron-emitting device B1 and was 1.2 or more with regard to the electron-emitting devices B2 to B6.
Further, each of the end of the first carbon film 21a was processed using an AFM such that d2 of the electron-emitting device C1 was 4.0 nm, d2 of the electron-emitting device C2 was 4.2 nm, d2 of the electron-emitting device C3 was 5.0 nm, d2 of the electron-emitting device C4 was 10 nm. It is to be noted that d2/d1 was 1.1 with regard to the electron-emitting device C1 and was 1.2 or more with regard to the electron-emitting devices C2 to C4.
Further, in the same method as the above Process-a to Process-e, three kinds of electron-emitting devices were manufactured as Comparative Example 1. Each of the electron-emitting devices of Comparative Example 1 had different voltages to be applied in the activation process. In the activation process, the highest voltage value was ±14 V′ with regard to the first device, ±16 V with regard to the second device, and ±18 V with regard to the third device. The above Process-f was not carried out with regard to the electron-emitting devices of Comparative Example 1.
Next, the electron-emitting devices manufactured according to this example after Process-f and the electron-emitting devices of Comparative Example 1 were disposed in the measurement/evaluation apparatus illustrated in
More specifically, with the vacuum chamber and the electron-emitting devices maintained at about 250° C. by heating them by a heater, the vacuum chamber was evacuated. After 20 hours elapsed, the heating by the heater was stopped to allow them to reach room temperature. The pressure in the vacuum chamber reached about 1×10−8 Pa. Next, electron emitting characteristics were measured.
In measuring the electron emitting characteristics, the distance H between the anode electrode 44 and the electron-emitting device was 2 mm, and a high voltage power source 43 gave a potential of 1 kV to the anode electrode 44. With this state maintained, the power source 41 was used to apply drive voltage between the auxiliary electrodes 2 and 3 of the respective electron-emitting devices so that the potential of the first auxiliary electrode 2 was lower than that of the second auxiliary electrode 3. Square pulse voltage having the pulse height value of 12 V was applied to the electron-emitting devices A1 to A8 and the first device of Comparative Example 1, square pulse voltage having the pulse height value of 14 V was applied to the electron-emitting devices B1 to B6 and the second device of Comparative Example 1, and square pulse voltage having the pulse height value of 16 V was applied to the electron-emitting devices C1 to C4 and the third device of Comparative Example 1.
In the measurement, the device current If and the emission current Ie of the electron-emitting devices of this example and that of Comparative Example 1 were measured by ammeters 40 and 42, respectively, and electron emitting efficiency (Ie/If) was calculated.
Table 1 shows the calculated electron emitting efficiency and Table 2 shows the emission current Ie. The device current If was about 1.0 mA with regard to all the electron-emitting devices.
The result shows that, when d2/d1 is 1.2 or more, the electron-emitting devices of this example has larger emission current Ie and higher electron emitting efficiency than those of the electron-emitting devices of Comparative Example 1. Further, after the evaluation of the characteristics, the same pulse voltage as that applied in the evaluation of the characteristics was applied to the electron-emitting devices of this example and the devices were driven for a long time. The characteristics shown in Tables 1 and 2 were maintained for a long time without much fluctuation over time.
After the evaluation of the characteristics described above, the neighborhood of the gap 8 of the electron-emitting devices (A, B, and C) manufactured in this example was observed using the above-described 3D-TEM. The distance d1 between a portion A of the first carbon film 21a and a portion B of the second carbon film 21b was confirmed to be 2.5 nm with regard to the electron-emitting devices A, 3.0 nm with regard to the electron-emitting devices B, and 3.5 nm with regard to the electron-emitting devices C. Similarly, the distance d2 was confirmed to be 2.8 nm with regard to the electron-emitting device A1, 3.0 nm with regard to the electron-emitting device A2, 3.3 nm with regard to the electron-emitting device A3, 3.5 nm with regard to the electron-emitting device A4, 4.0 nm with regard to the electron-emitting device A5, 4.2 nm with regard to the electron-emitting device A6, 5.0 nm with regard to the electron-emitting device A7, 10 nm with regard to the electron-emitting device A8, 3.3 nm with regard to the electron-emitting device B1, 3.5 nm with regard to the electron-emitting device B2, 4.0 nm with regard to the electron-emitting device B3, 4.2 nm with regard to the electron-emitting device B4, 5.0 nm with regard to the electron-emitting device B5, nm with regard to the electron-emitting device B6, 4.0 nm with regard to the electron-emitting device C1, 4.2 nm with regard to the electron-emitting device C2, 5.0 nm with regard to the electron-emitting device C3, and 10 nm with regard to the electron-emitting device C4.
With regard to all the electron-emitting devices, it was confirmed that the transformed portion of the substrate (concave) 22 was formed in the surface of the substrate 1 between the first and second carbon films 21a and 21b.
The distance d3 between the respective protrusions was measured using SEM plan views, and the distribution was studied.
With regard to all the electron-emitting devices, the distribution of the distance d3 was from 3 d1 to 500 d1 with the peak being 30 to 40 d1. Although the distribution of the distance d3 was as described above with regard to the electron-emitting devices A to C of this example, the present invention is not limited thereto, and the distance d3 may have a broader distribution. However, in order to obtain the emission current Ie in a practical range, it is preferable that the distribution is within 2000 d1.
Further, in order to obtain larger emission current Ie, it is most preferable that d3 is from 3 d1 to 40 d1 and all d3 are the same (the distribution is concentrated).
This example is a further preferable example of the present invention.
In this example, electron-emitting devices were manufactured in the same way as that in Example 1 except that Process-e and Process-f of Example 1 were modified as described in the following. Thus, here, Process-e and Process-f will be described.
Following Process-e, in order to carry out the activation process, acrylonitrile was introduced into the vacuum chamber through a slow leak valve. Then, the pulse voltage having the waveform illustrated in
After 120 minutes lapsed from the beginning of the activation process, it was made sure that the graph entered deep enough the region which was on the right side of the dotted line in
In this process, electron-emitting devices D which underwent “activation” process with the highest voltage value being ±14 V, electron-emitting devices E which underwent “activation” process with the highest voltage value being ±16 V, and electron-emitting devices C which underwent “activation” process with the highest voltage value being ±18 V were manufactured. Eight electron-emitting devices D (D1 to D8) in total were manufactured by the same manufacturing method as described above. Six electron-emitting devices E (E1 to E6) in total were manufactured by the same manufacturing method as described above. Four electron-emitting devices F (F1 to F4) in total were manufactured by the same manufacturing method as described above.
SEM plan views and SEM sectional views of electron-emitting devices manufactured by the same manufacturing method as Process-a to Process-e in the above were observed. It was found that, regardless of the voltage applied in the “activation” process, the thickness of the end of the first carbon film 21a and the thickness of the end of the second carbon films 21b (the portion forming the periphery of the gap 8) are asymmetric, and the gap 8 was serpentine. Further, in all the electron-emitting devices, there were a plurality of portions (portions A and B) where the gap between the first and second electroconductive films 21a and 21b is smaller than that in other portions.
3D-TEM image observation in the neighborhood of the gap 8 of the electron-emitting devices (D′, E′, and F′) manufactured by the same manufacturing method as that of the respective electron-emitting devices D, E, and F was made. The distance d1 between a portion A of the first carbon film 21a and a portion B of the second carbon film 21b was 2.3 nm on average with regard to the electron-emitting devices D′, 2.8 nm on average with regard to the electron-emitting devices E′, and 3.3 nm on average with regard to the electron-emitting devices F′.
The minimum distance d2 between a portion of the first electroconductive film 21a which is away from a portion A along the periphery of the gap 8 by the same distance as d1 and a portion of the second electroconductive film 21b in opposition to that portion which was measured using 3D-TEM images was 2.5 nm on average with regard to the electron-emitting devices D′ (d2/d1 was 1.1 or less with regard to all the electron-emitting devices D′), 3.0 nm on average with regard to the electron-emitting devices E′ (d2/d1 was 1.1 or less with regard to all the electron-emitting devices E′), and 3.5 nm on average with regard to the electron-emitting devices F′ (d2/d1 was 1.1 or less with regard to all the electron-emitting devices F′).
The neighborhood of the gap 8 of the electron-emitting devices D′ was observed using SEM section views. The thickness of the end of the first carbon film 21a was 20 nm and the thickness of the end of the second carbon film 21b was 75 nm. The thickness of the second carbon film 21b which exists on a line extending in a direction in which a portion A of the first carbon film 21a is in opposition to a portion B of the second carbon film 21b (in a direction of emission of electrons) was 100 nm.
Then, the electron-emitting devices according to this example (D, E, and F) after Process-e were taken out from the measurement/evaluation apparatus illustrated in
By cutting the end of the first carbon film 21a, the distance d1 between a portion A of the first carbon film 21a and a portion B of the second carbon film 21b was set to be 2.5 nm with regard to all the electron-emitting devices D (D1 to D8), 3.0 nm with regard to all the electron-emitting devices E (E1 to E4), and 3.5 nm with regard to all the electron-emitting devices F (F1 to F4).
Further, each of the end of the first carbon film 21a was processed using an AFM such that d2 of the electron-emitting device D1 was 2.8 nm, d2 of the electron-emitting device D2 was 3.0 nm, d2 of the electron-emitting device D3 was 3.3 nm, d2 of the electron-emitting device D4 was 3.6 nm, d2 of the electron-emitting device D5 was 4.0 nm, d2 of the electron-emitting device D6 was 4.2 nm, d2 of the electron-emitting device D7 was 5.0 nm, and d2 of the electron-emitting device D8 was 10 nm. It is to be noted that d2/d1 was 1.1 with regard to the electron-emitting device D1 and was 1.2 or more with regard to the electron-emitting devices D2 to D8. Further, each of the end of the first carbon film 21a was processed using an AFM such that d2 of the electron-emitting device E1 was 3.3 nm, d2 of the electron-emitting device E2 was 3.6 nm, d2 of the electron-emitting device E3 was 4.0 nm, d2 of the electron-emitting device E4 was 4.2 nm, d2 of the electron-emitting device E5 was 5.0 nm, d2 of the electron-emitting device E6 was 10 nm. It is to be noted that d2/d1 was 1.1 with regard to the electron-emitting device E1 and was 1.2 or more with regard to the electron-emitting devices E2 to E6.
Further, each of the end of the first carbon film 21a was processed using an AFM such that d2 of the electron-emitting device F1 was 4.0 nm, d2 of the electron-emitting device F2 was 4.2 nm, d2 of the electron-emitting device F3 was 5.0 nm, d2 of the electron-emitting device F4 was 10 nm. It is to be noted that d2/d1 was 1.1 with regard to the electron-emitting device F1 and was 1.2 or more with regard to the electron-emitting devices F2 to F4.
With regard to each electron-emitting device, cutting was carried out so that the thickness of the portions B of the second electroconductive film 21b is equal to that of the portions A of the first electroconductive film 21a, and the thickness difference h between the portions B and the portions 35 and 36 of the second electroconductive film 21b (the height h of the “projected portions” (see
The thickness of the second carbon film 21b which exists on a line extending in a direction in which a portion A of the first carbon film 21a is in opposition to a portion B of the second carbon film 21b (in a direction of emission of electrons) was 100 nm.
Further, in the same method as the above Processes-a to Processes-e, three kinds of electron-emitting devices were manufactured as Comparative Example 2. Each of the electron-emitting devices of Comparative Example 2 had different voltages to be applied in the activation process. In the activation process, the highest voltage value was ±14 V with regard to the first device, ±16 V with regard to the second device, and ±18 V with regard to the third device. The above Process-f was not carried out with regard to the electron-emitting devices of Comparative Example 2.
Next, the electron-emitting devices after Process-f and the electron-emitting devices of Comparative Example 2 were disposed in the measurement/evaluation apparatus illustrated in
More specifically, with the vacuum chamber and the electron-emitting devices maintained at about 250° C. by heating them by a heater, the vacuum chamber was evacuated. After 20 hours elapsed, the heating by the heater was stopped to allow them to reach room temperature. The pressure in the vacuum chamber reached about 1×10−8 Pa. Next, electron emitting characteristics were measured.
In measuring the electron emitting characteristics, the distance H between the anode electrode 44 and the electron-emitting device was 2 mm, and a high voltage power source 43 gave a potential of 1 kV to the anode electrode 44. With this state maintained, the power source 41 was used to apply drive voltage between the auxiliary electrodes 2 and 3 of the respective electron-emitting devices such that the potential of the first auxiliary electrode 2 was lower than that of the second auxiliary electrode 3. Square pulse voltage having the pulse height value of 12 V was applied to the electron-emitting devices D1 to D8 and the first device of Comparative Example 2, square pulse voltage having the pulse height value of 14 V was applied to the electron-emitting devices E1 to E6 and the second device of Comparative Example 2, and square pulse voltage having the pulse height value of 16 V was applied to the electron-emitting devices F1 to F4 and the third device of Comparative Example 2.
In the measurement, the device current If and the emission current Ie of the electron-emitting devices of this example and of Comparative Example 2 were measured by ammeters 40 and 42, respectively, and electron emitting efficiency (Ie/If) was calculated.
Table 3 shows the calculated electron emitting efficiency and Table 4 shows the emission current Ie. The device current If was about 1.0 mA with regard to all the electron-emitting devices.
The result shows that, when d2/d1 is 1.2 or more, the electron-emitting devices of this example has larger emission current Ie and higher electron emitting efficiency η than those of the electron-emitting devices of Comparative Example 2. Further, after the evaluation of the characteristics, the same pulse voltage as that applied in the evaluation of the characteristics was applied to the electron-emitting devices of this example and the devices were driven for a long time. The characteristics shown in Tables 3 and 4 were maintained for a long time without much fluctuation over time.
After the evaluation of the characteristics described above, the neighborhood of the gap 8 of the electron-emitting devices (D, E, and F) manufactured in this example was observed using the above-described 3D-TEM. The distance d1 between a portion A of the first carbon film 21a and a portion B of the second carbon film 21b was confirmed to be 2.5 nm with regard to the electron-emitting devices D (D1 to D8), 3.0 nm with regard to the electron-emitting devices E (E1 to E6), and 3.5 nm with regard to the electron-emitting devices F (F1 to F4). Similarly, the distance d2 was confirmed to be 2.8 nm with regard to the electron-emitting device D1, 3.0 nm with regard to the electron-emitting device D2, 3.3 nm with regard to the electron-emitting device D3, 3.6 nm with regard to the electron-emitting device D4, 4.0 nm with regard to the electron-emitting device D5, 4.2 nm with regard to the electron-emitting device D6, 5.0 nm with regard to the electron-emitting device D7, 10 nm with regard to the electron-emitting device D8, 3.3 nm with regard to the electron-emitting device E1, 3.6 nm with regard to the electron-emitting device E2, 4.0 nm with regard to the electron-emitting device E3, 4.2 nm with regard to the electron-emitting device E4, 5.0 nm with regard to the electron-emitting device E5, 10 nm with regard to the electron-emitting device E6, 4.0 nm with regard to the electron-emitting device F1, 4.2 nm with regard to the electron-emitting device F2, 5.0 nm with regard to the electron-emitting device F3, and 10 nm with regard to the electron-emitting device F4.
With regard to all the electron-emitting devices, it was confirmed that the transformed portion of the substrate (concaved portion) 22 was formed in the surface of the substrate 1 between the first and second carbon films 21a and 21b.
Further, the width w between portions 35 and 36 (the width w between “projected portions”) was confirmed to be 5 nm with regard to the electron-emitting devices D, 6 nm with regard to the electron-emitting devices E, and 7 nm with regard to the electron-emitting devices F. These values (of the width w) were d1 of the respective electron-emitting devices multiplied by two.
The distance d3 between the respective protrusions (portions A) was measured using SEM plan views, and the distribution was studied. The distribution was similar to that illustrated in
Further, in order to obtain larger emission current Ie, it is most preferable that d3 is from 3 d1 to 45 d1 and all d3 are the same (the distribution is concentrated).
In addition, with regard to electron-emitting devices manufactured by a similar manufacturing method to that of the electron-emitting device E3, seven kinds of electron-emitting devices (E3-1 to E3-7) having different values of the width w were manufactured, and the characteristics of the respective devices were evaluated. The width w was 3 nm with regard to the electron-emitting device E3-1, 5 nm with regard to the electron-emitting device E3-2, 6 nm with regard to the electron-emitting device E3-3, 15 nm with regard to the electron-emitting device E3-4, 50 nm with regard to the electron-emitting device E3-5, 150 nm with regard to the electron-emitting device E3-6, and 300 nm with regard to the electron-emitting device E3-7. When voltage of 14 V was applied to these electron-emitting devices to drive the devices, the electron emitting efficiency η and the emission current Ie of E3-2 were almost the same as those of E3-1. The emission current Ie of E3-3 was almost the same as that of E3-2, but the electron emitting efficiency η of E3-3 was improved to be about 1.1 times as much as that of E3-2. The emission current Ie and the electron emitting efficiency η of E3-4 were improved to be about 1.2 times as much as that of E3-3. The electron emitting efficiency η of E3-5 was improved to be about 1.1 times as much as that of E3-4. The electron emitting efficiency η and the emission current Ie of E3-6 were almost the same as those of E3-5. The electron emitting efficiency η and the emission current Ie of E3-7 decreased compared with that of E3-6. Such tendency was similarly observed in other electron-emitting devices (D, E, and F) of this example. The above result indicated that setting w to be twice as large as d1 or more had an effect of improving the emission current Ie and the electron emitting efficiency η. It was also made clear that, when w exceeds 50 d1, that effect began to decrease.
Also, with regard to the thickness difference h (the height h of the “projected portions”), characteristics of five kinds of electron-emitting devices (E3-8 to E3-12) having different values of the thickness difference h and manufactured by a similar manufacturing method to that of the electron-emitting device E3 were evaluated. The thickness difference h was 3 nm with regard to the electron-emitting device E3-8, 4 nm with regard to the electron-emitting device E3-9, 6 nm with regard to the electron-emitting device E3-10, 10 nm with regard to the electron-emitting device E3-11, and 70 nm with regard to the electron-emitting device E3-12.
When voltage of 14 V was applied to these electron-emitting devices to drive the devices, the electron emitting efficiency q and the emission current Ie of E3-9 were almost the same as those of E3-8. The emission current Ie of E3-10 was improved to be about 1.2 times as much as that of E3-9 while the electron emitting efficiency η of E3-10 was almost the same as that of E3-9. The electron emitting efficiency η of E3-11 was improved to be about 1.2 times as much as that of E3-10. The electron emitting efficiency η of E3-12 was improved to be about 1.1 times as much as that of E3-11, but the emission current Ie of E3-12 was almost the same as that of E3-11.
The above result indicated that setting h to be twice as large as d1 or more had an effect of improving the emission current Ie and the electron emitting efficiency η. Such tendency was similarly observed in other electron-emitting devices (D, E, and F) of this example. Further, since it is made clear by calculation by the present inventors that the emission current Ie becomes larger and the electron emitting efficiency η becomes higher even when the thickness difference h is 70 nm or more, the upper limit of the thickness difference h is not limited. However, in view of the manufacturing cost and problems relating to the quality (electric discharge and the like), it is effectively preferable that the thickness difference h is set to be less than 200 d1.
In this example, the electron-emitting device illustrated in
Next, the substrate 1 having the auxiliary electrodes 2 and 3 formed thereon was disposed in the measurement/evaluation apparatus illustrated in
Here, the thickness of the end of the first carbon film 21a and the thickness of the end of the second carbon films 21b (the portion forming the periphery of the gap 8) were set to form a symmetrical structure (see
By using such a method, electron-emitting devices (G1 to G5) having different values of d2 were manufactured. The distance d2 was 3.7 nm with regard to the electron-emitting device G1, 4.0 nm with regard to the electron-emitting device G2, 4.2 nm with regard to the electron-emitting device G3, 5.0 nm with regard to the electron-emitting device G4, and 10 nm with regard to the electron-emitting device G5. The distance d3 of the electron-emitting devices was set to be 30 d1. It is to be noted that d2/d1 was 1.1 with regard to the electron-emitting devices G1 and G2 and was 1.2 or more with regard to the electron-emitting devices G3 to G5.
Then, with the vacuum chamber being evacuated, the electron-emitting devices of this' example after Process-b were heated and voltage was applied to them. After 20 hours elapsed, the heating by the heater was stopped to allow them to reach room temperature. The pressure in the vacuum chamber reached about 1×10−8 Pa. Next, electron emitting characteristics were measured.
In measuring the electron emitting characteristics, the distance H between the anode electrode 44 and the electron-emitting device was 2 mm, and the high voltage power source 43 gave a potential of 1 kV to the anode electrode 44. With this state maintained, the power source 41 was used to apply square pulse voltage having the pulse height value of 16 V between the auxiliary electrodes 2 and 3 so that the potential of the first auxiliary electrode 2 was lower than that of the second auxiliary electrode 3.
In the measurement, the device current If and the emission current Ie of the electron-emitting devices of this example were measured by the ammeters 40 and 42, respectively, and electron emitting efficiency was calculated.
Table 5 shows the calculated electron emitting efficiency and the emission current Ie. The device current If was about 2.5 mA with regard to all the electron-emitting devices.
The result showed that, when d2/d1 was 1.2 or more, the electron-emitting devices of this example had larger emission current Ie and higher electron emitting efficiency q. Further, after the evaluation of the characteristics, the same pulse voltage as that applied in the evaluation of the characteristics was applied to the electron-emitting devices of this example and the devices were driven for a long time. The characteristics shown in Table 5 were maintained for a long time without much fluctuation over time compared with the electron-emitting devices manufactured in Example 1.
After the evaluation of the characteristics, the neighborhood of the gap 8 of the electron-emitting devices manufactured in this example was observed using 3D-TEM images, and the structure was approximately as schematically illustrated in
The distance d2 was 3.7 nm with regard to the electron-emitting devices G1, 4.0 nm with regard to the electron-emitting device G2, 4.2 nm with regard to the electron-emitting device G3, 5.0 nm with regard to the electron-emitting device G4, and 10 nm with regard to the electron-emitting device G5.
The distribution of the distance d3 was studied using SEM plan views.
In this example, electron-emitting devices with the first and second carbon films 21a and 21b illustrated in
Four modifications were made to Process-b of the electron-emitting devices of Example 3: (1) with regard to the electron-emitting devices (G1 to G5), electron beam irradiation was used so that the thickness of the portions B of the second carbon film 21b was equal to that of the portions A of the first carbon film 21a (see
In measuring the electron emitting characteristics manufactured in this example, the distance H between the anode electrode 44 and the electron-emitting device was 2 mm, and the high voltage power source 43 gave a potential of 1 kV to the anode electrode 44. With this state maintained, the power source 41 was used to apply square pulse voltage having the pulse height value of 16 V between the auxiliary electrodes 2 and 3 so that the potential of the first auxiliary electrode 2 was lower than that of the second auxiliary electrode 3.
In the measurement, the device current If and the emission current Ie of the electron-emitting devices of this example were measured by the ammeters 40 and 42, respectively, and electron emitting efficiency was calculated.
Table 6 shows the calculated electron emitting efficiency and the emission current Ie. The device current If was about 2.5 mA with regard to all the electron-emitting devices.
The result showed that, when d2/d1 was 1.2 or more, the electron-emitting devices (G1 to G5′) of this example had larger emission current Ie and higher electron emitting efficiency η. Further, after the evaluation of the characteristics, the same pulse voltage as that applied in the evaluation of the characteristics was applied to the electron-emitting devices of this example and the devices were driven for a long time. The characteristics shown in Table 6 were maintained for a long time without much fluctuation over time compared with the electron-emitting devices manufactured in Example 2.
After the evaluation of the characteristics, the electron-emitting devices manufactured in this example were observed using 3D-TEM. The value of d1 was 3.5 nm. The value of d2 was 3.7 nm with regard to the electron-emitting device G1′, 4.0 nm with regard to the electron-emitting device G2′, 4.2 nm with regard to the electron-emitting device G3′, 5.0 nm with regard to the electron-emitting device G4′, and 10 nm with regard to the electron-emitting device G5′.
The thickness of the portions B of the second carbon film 21b was equal to that of the portions A of the first carbon film 21a, and the thickness difference h between the portions B and the portions 35 and 36 of the second electroconductive film 21b (the height h of the “projected portions”) was 50 nm. Further, the width w between portions 35 and 36 (the width w between “projected portions”) was 7 nm.
The distance d3 between the respective protrusions was measured using SEM plan views, and the distribution was studied. Similarly to the distribution illustrated in
In this example, a lot of electron-emitting devices manufactured by a similar manufacturing method to that of the electron-emitting device C3 manufactured in Example 1 of the present invention were arranged in a matrix on a substrate to form an electron source, and the electron source was used to manufacture the image display apparatus illustrated in
An SiO2 film was formed on the glass substrate 71. Further, a lot of first and second auxiliary electrodes 2 and 3 were formed on the substrate 71 (
Then, as illustrated in
Then, as illustrated in
As illustrated in
By ink jetting, the electroconductive thin film 4 was formed between the auxiliary electrodes 2 and 3 on the substrate 71 having the matrix wirings formed thereon (
In this example, an organic palladium complex solution was used as the ink used for the ink jetting. The organic palladium complex solution was applied between the auxiliary electrodes 2 and 3. After that, the substrate 71 was heated and baked in the air to form the electroconductive thin film 4 made of palladium oxide (PdO).
Then, the substrate 71 having thereon a plurality of units formed by the auxiliary electrodes 2 and 3 and the electroconductive thin film 4 for connecting the auxiliary electrodes 2 and 3 was disposed in the vacuum chamber 23. After the vacuum chamber was evacuated, the “forming” process and the “activation” process were carried out. The waveform of voltage applied to the respective unit during the “forming” process and the “activation” process and the like were as described in the method of manufacturing the electron-emitting device C3 of Example 1.
The “forming” process was carried out by applying pulses one by one to the plurality of X-directional wirings 72 selected one by one in sequence. More specifically, a process where “after one pulse is applied to one X-directional wiring selected from the plurality of X-directional wirings 72, another X-directional wiring is selected and one pulse is applied thereto” was repeated.
In this way, the substrate 71 having a plurality of electron-emitting devices formed thereon could be manufactured.
Then, the two kinds of substrates 1 having a lot of electron-emitting devices formed thereon after the “activation” process were taken out from the vacuum chamber to the atmosphere, and, as described in the method of manufacturing the electron-emitting device C3 of Example 1, the carbon was shaped using an AFM.
With regard to all the electron-emitting devices, d1 was set to be 3.5 nm and d2 was set to be 5.0 nm (d2/d1=1.4).
In this way, the substrate 71 having the electron source of this example (the plurality of electron-emitting devices) formed thereon was manufactured.
Next, as illustrated in
Although
In this example, in order to realize color display, the phosphor film 84 which was an image forming member was a phosphor in the shape of stripes (see
The metal back 85 formed of aluminum was provided on the inner surface side (on the side of the electron-emitting devices) of the phosphor film 84. The metal back 85 was formed by vacuum evaporation of Al on the inner surface side of the phosphor film 84.
A desired electron-emitting device was selected via the X-directional wirings and Y-directional wirings of the image display apparatus manufactured as described above, and pulse voltage of +18 V was applied so that the potential on the side of the second auxiliary electrode of the selected electron-emitting device was higher than that on the side of the first auxiliary electrode. At the same time, voltage of 10 kV was applied to the metal back 73 via a high voltage terminal Hv. A bright and satisfactory image could be displayed for a long time.
The embodiments and examples according to the present invention described above are as exemplary only, and various variations as to the material and the size are not precluded by the present invention.
This application claims priority from Japanese Patent Application No. 2004-379955 filed Dec. 28, 2004, which is hereby incorporated by reference herein.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2004-379955 | Dec 2004 | JP | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/JP05/24013 | 12/21/2005 | WO | 00 | 5/29/2007 |
