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JP4347253B2 - Light emitting device - Google Patents
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JP4347253B2 - Light emitting device - Google Patents

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JP4347253B2
JP4347253B2 JP2005108625A JP2005108625A JP4347253B2 JP 4347253 B2 JP4347253 B2 JP 4347253B2 JP 2005108625 A JP2005108625 A JP 2005108625A JP 2005108625 A JP2005108625 A JP 2005108625A JP 4347253 B2 JP4347253 B2 JP 4347253B2
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久也 高橋
篤史 難波
美由紀 小林
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Subaru Corp
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Fuji Jukogyo KK
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Description

本発明は、電子放出源から電界放出された電子によって蛍光体を励起発光させる発光装置に関する。   The present invention relates to a light-emitting device that excites a phosphor with light emitted from an electron emission source.

近年、白熱電球や蛍光灯といった従来の発光装置に対し、真空中で電子放出源から電界放出させた電子を高速で蛍光体に衝突させることにより、蛍光体を励起発光させる冷陰極電界放出型の発光装置が開発されている。この種の発光装置は、カソード電極に対して正の電位を与えたグリッド電極によって電子を引き出し、更に正の高電圧を与えた蛍光板電極に電子を衝突させて蛍光発光させるものであり、電界放出型照明ランプ(Field Emission Lamp:FEL)や電界放出型表示装置(Field Emission Display:FED)としての用途が見込まれている。   In recent years, compared to conventional light emitting devices such as incandescent bulbs and fluorescent lamps, cold cathode field emission type that excites and emits phosphors by colliding the electrons emitted from the electron emission source in vacuum with the phosphors at high speed. Light emitting devices have been developed. This type of light emitting device is a field emission device in which electrons are drawn out by a grid electrode applied with a positive potential with respect to the cathode electrode, and are further made to emit fluorescent light by colliding electrons with a fluorescent plate electrode applied with a positive high voltage. Applications are expected as a field illumination lamp (FEL) and a field emission display (FED).

例えば、特許文献1には、FELに関連する技術として、カソード電極表面と略平行な略平板に孔を設け、この孔端をカソード電極側に突き出した構造のグリッド電極とする技術が開示されている。この特許文献1の技術によれば、略平板領域における電界よりも孔端における電界を高くすることができ、カソード電極からグリッド電極に飛び込む無効電子を抑制することができる。   For example, Patent Document 1 discloses a technique related to FEL in which a grid electrode having a structure in which holes are formed in a substantially flat plate substantially parallel to the surface of the cathode electrode and the ends of the holes protrude toward the cathode electrode side is disclosed. Yes. According to the technique of this Patent Document 1, the electric field at the hole end can be made higher than the electric field in the substantially flat region, and invalid electrons jumping from the cathode electrode to the grid electrode can be suppressed.

また、特許文献2には、同様にFELに関連して、部分的に開口を備えた半円筒状のグリッド電極が直方体形状カソード電極に対して間隙を持って囲む技術が開示されている。特許文献2の技術では、電子が蛍光板電極に突入したことによって叩き出された正イオンがカソード電極に突入することを抑制し、放電破壊を防止することができる。   Similarly, Patent Document 2 discloses a technique related to FEL in which a semicylindrical grid electrode partially having an opening surrounds a rectangular parallelepiped cathode electrode with a gap. According to the technique of Patent Document 2, it is possible to suppress positive ions struck by the electrons entering the fluorescent plate electrode from entering the cathode electrode, thereby preventing discharge breakdown.

ところで、一般的な方法で成膜された冷陰極の電子放出源は、成膜された部分ごとに一定の電界放出特性を有しておらず、この電界放出特性のバラツキに起因して、蛍光体の発光輝度にムラが発生するという問題がある。この発光ムラについて、図3に示す典型的なFELのカソード極の構造を例に取って説明する。   By the way, an electron emission source of a cold cathode formed by a general method does not have a constant field emission characteristic for each part where the film is formed. There is a problem that unevenness occurs in the light emission luminance of the body. This light emission unevenness will be described by taking the structure of the cathode electrode of a typical FEL shown in FIG. 3 as an example.

図3の例では、ガラス基材100上に形成したカソード電極101にカーボンナノチューブ等のエミッタ材料を成膜し、冷陰極の電子放出源102を形成している。また、カソード電極101には、所定の距離をもってグリッド電極103が対向配置されている。カソード電極101とグリッド電極103との距離Aを、例えば100μmとし、電子放出源102からある一定の電子(例えば、100μA/cm2の電流密度)が放出されるための電界強度が1V/μmとすると、カソード電極101を0Vに接地し、グリッド電極103に直流100Vを印加すれば、100μA/cm2の電子が、グリッド電極103、及びカソード電極101に対向配置された蛍光板電極104(図3中においては、上方から見た平面で示す)に向かって放出される。 In the example of FIG. 3, an emitter material such as carbon nanotube is formed on the cathode electrode 101 formed on the glass substrate 100 to form the cold cathode electron emission source 102. A grid electrode 103 is disposed opposite to the cathode electrode 101 with a predetermined distance. The distance A between the cathode electrode 101 and the grid electrode 103 is, for example, 100 μm, and the electric field strength for emitting certain electrons (for example, a current density of 100 μA / cm 2 ) from the electron emission source 102 is 1 V / μm. Then, if the cathode electrode 101 is grounded to 0 V and a direct current of 100 V is applied to the grid electrode 103, 100 μA / cm 2 of electrons are arranged opposite to the grid electrode 103 and the cathode electrode 101 (FIG. 3). In this case, the light is emitted toward a plane seen from above.

従って、蛍光板電極に、例えば5kVの直流電圧を印加すれば、5ekVで加速された電子が蛍光板電極104の蛍光体に衝突して蛍光体が発光するが、このとき、図3に示すように、電子放出源102のAA部の電界放出特性が0.8V/μmでBB部の電界放出特性が1.2V/μmであったとすれば、蛍光板上方から見たときの発光は、AA部が非常に明るく、またBB部は暗くなる。このため、結果として発光ムラが発生することになる。   Therefore, if a DC voltage of, for example, 5 kV is applied to the phosphor plate electrode, electrons accelerated at 5 ekV collide with the phosphor of the phosphor plate electrode 104 and the phosphor emits light. At this time, as shown in FIG. Assuming that the field emission characteristic of the AA part of the electron emission source 102 is 0.8 V / μm and the field emission characteristic of the BB part is 1.2 V / μm, the light emission when viewed from above the fluorescent plate is very high in the AA part. And the BB part becomes dark. As a result, uneven light emission occurs.

このような電子放出源の電界放出特性のバラツキに起因する発光ムラに対処する技術は、特許文献3に開示されている。特許文献3の技術は、FEDに関する技術であり、陰極基板にカーボンナノチューブ製の平面状の冷陰極を形成し、透明な陽極基板に、ストライプ状の透明な陽極ストリップと、これに交差するストライプ状の選択グリッドストリップと、格子状の電子引き出しグリッドとを形成している。   Patent Document 3 discloses a technique for dealing with such light emission unevenness caused by variations in the field emission characteristics of the electron emission source. The technique of Patent Document 3 is a technique related to FED, in which a flat cold cathode made of carbon nanotubes is formed on a cathode substrate, a transparent anode substrate is striped on a transparent anode strip, and a stripe shape intersecting this is formed. The selected grid strip and the grid-like electronic lead-out grid are formed.

特許文献3の技術によれば、冷陰極から放出された電子は、冷陰極と電子引き出しグリッドとの間の電子滞留領域に滞留して電子雲を形成する。そして、何れかの選択グリッドストリップと何れかの陽極ストリップとに電圧が印加されると、電子雲からの電子流が電子引き出しグリッドの開口と選択グリッドストリップの開口とを通過して陽極ストリップ上の蛍光体に衝突する。これにより、冷陰極電界放出に起因する電子の偏在を平均化し、蛍光体の発光ムラをなくすことができる。
特開2004−207066号公報 特開2004−220896号公報 特開2004−335385号公報
According to the technique of Patent Document 3, electrons emitted from the cold cathode are retained in an electron retention region between the cold cathode and the electron extraction grid to form an electron cloud. Then, when a voltage is applied to any selected grid strip and any anode strip, the electron flow from the electron cloud passes through the opening of the electron extraction grid and the opening of the selected grid strip and then on the anode strip. Collides with phosphor. Thereby, the uneven distribution of electrons due to cold cathode field emission can be averaged, and the uneven emission of the phosphor can be eliminated.
JP 2004-207066 A JP 2004-220896 A JP 2004-335385 A

しかしながら、特許文献3に開示されている技術は、陽極(蛍光体電極)をマトリクス状に区分する等して画素毎に蛍光体を発光させる表示装置を前提としている。このため、表示装置よりも遥かに高い輝度が要求され、平面状の蛍光体電極全面を発光させる照明用としての用途を考慮したとき、特許文献3の技術を適用することは困難であるばかりでなく、構造が複雑となってコスト上昇を招いてしまう。   However, the technique disclosed in Patent Document 3 is premised on a display device that emits a phosphor for each pixel by dividing an anode (phosphor electrode) into a matrix. For this reason, brightness much higher than that of the display device is required, and it is difficult to apply the technique of Patent Document 3 when considering an application for illumination that emits light from the entire surface of the planar phosphor electrode. However, the structure becomes complicated and the cost increases.

本発明は上記事情に鑑みてなされたもので、複雑な構造を要することなく、電子放出源の電界放出特性のバラツキに起因する発光ムラを低減することのできる発光装置を提供することを目的としている。   The present invention has been made in view of the above circumstances, and an object thereof is to provide a light emitting device that can reduce unevenness in light emission due to variations in field emission characteristics of an electron emission source without requiring a complicated structure. Yes.

上記目的を達成するため、本発明による発光装置は、少なくとも、電子放出源を有するカソード電極と蛍光体を有する蛍光板電極とが真空中で対向配置された発光装置において、上記電子放出源における電界放出の電流密度が上記蛍光体での発光が飽和状態に達する電流密度以上となる制御電圧を、上記カソード電極に周期的に印加する電圧制御手段を備えたことを特徴とする。 In order to achieve the above object, a light emitting device according to the present invention is a light emitting device in which at least a cathode electrode having an electron emission source and a fluorescent plate electrode having a phosphor are arranged opposite to each other in a vacuum, and the field emission in the electron emission source. And a voltage control means for periodically applying a control voltage at which the current density is equal to or higher than a current density at which light emission from the phosphor reaches a saturated state .

また、カソード電極と蛍光板電極との間にグリッド電極を配置する3極構造の発光装置においては、グリッド電極とカソード電極との間に制御電圧を周期的に印加すると共に、この制御電圧の印加に同期して、蛍光板電極とカソード電極との間に制御電圧よりも高い電圧を印加することが望ましい。   Further, in a light emitting device having a three-pole structure in which a grid electrode is disposed between a cathode electrode and a fluorescent plate electrode, a control voltage is periodically applied between the grid electrode and the cathode electrode, and the control voltage is applied. In synchronization, it is desirable to apply a voltage higher than the control voltage between the fluorescent plate electrode and the cathode electrode.

3極構造の発光装置の電圧制御手段は、カソード電極とグリッド電極と蛍光板電極とを二次側に接続した変圧回路を用いて構成することができ、変圧回路の一次側に周期的な電圧信号を印加することにより、グリッド電極とカソード電極との間の制御電圧と、蛍光板電極とカソード電極との間の電圧とを同期させて周期的に印加することができる。   The voltage control means of the light-emitting device having a three-pole structure can be configured using a transformer circuit in which a cathode electrode, a grid electrode, and a fluorescent plate electrode are connected to the secondary side, and a periodic voltage signal is provided on the primary side of the transformer circuit. Is applied periodically in synchronization with the control voltage between the grid electrode and the cathode electrode and the voltage between the fluorescent plate electrode and the cathode electrode.

カソード電極への制御電圧の印加は、60Hz以上の繰返し周期で行うことが望ましく、また、カソード電極へ制御電圧を印加する周期は、カソード電極へ制御電圧を印加する期間の少なくとも10倍以上とすることが望ましい。   The application of the control voltage to the cathode electrode is preferably performed at a repetition period of 60 Hz or more, and the period of applying the control voltage to the cathode electrode is at least 10 times the period of applying the control voltage to the cathode electrode. It is desirable.

本発明による発光装置は、複雑な構造を要することなく、電子放出源の電界放出特性のバラツキに起因する発光ムラを低減することができる。   The light emitting device according to the present invention can reduce light emission unevenness due to variations in field emission characteristics of the electron emission source without requiring a complicated structure.

以下、図面を参照して本発明の実施の形態を説明する。図1及び図2は本発明の実施の一形態に係り、図1は発光装置の基本構成図、図2は駆動回路の説明図である。   Embodiments of the present invention will be described below with reference to the drawings. 1 and 2 relate to an embodiment of the present invention, FIG. 1 is a basic configuration diagram of a light emitting device, and FIG. 2 is an explanatory diagram of a drive circuit.

図1に示すように、本実施の形態における発光装置1は、例えば、平面状の電界放出型照明ランプとして用いられる発光装置であり、所定間隔で対向配置されたガラス基材2,3の内部を真空状態に維持し、この真空状態下で、カソード電極5、グリッド電極10、蛍光板電極15を順に配置した基本構成を有している。尚、図1においては、カソード電極5とグリッド電極10と蛍光板電極15との3極構造を例示しているが、グリッド電極10を用いない2極構造であっても良い。   As shown in FIG. 1, the light-emitting device 1 in this Embodiment is a light-emitting device used as a planar field emission illumination lamp, for example, and the inside of the glass base materials 2 and 3 opposingly arranged by the predetermined space | interval Is maintained in a vacuum state, and in this vacuum state, the cathode electrode 5, the grid electrode 10, and the fluorescent plate electrode 15 are arranged in this order. In FIG. 1, a three-pole structure including the cathode electrode 5, the grid electrode 10, and the fluorescent plate electrode 15 is illustrated, but a two-pole structure that does not use the grid electrode 10 may be used.

カソード電極5は、ベースとなるガラス基材2上に形成された導電材からなり、例えば、アルミニウムやニッケル等の金属を蒸着やスパッタ法等によって堆積したり、銀ペースト材を塗布して乾燥・焼成する等して形成される。このカソード電極5の表面には、カーボンナノチューブ、カーボンナノウォール、スピント型マイクロコーン、金属酸化物ウィスカー等のエミッタ材料が膜状に塗布されて電子放出源6が形成されている。   The cathode electrode 5 is made of a conductive material formed on the glass substrate 2 serving as a base. For example, a metal such as aluminum or nickel is deposited by vapor deposition or sputtering, or a silver paste material is applied and dried. It is formed by firing. On the surface of the cathode electrode 5, an electron emission source 6 is formed by applying an emitter material such as a carbon nanotube, a carbon nanowall, a spint type micro cone, or a metal oxide whisker in a film shape.

グリッド電極10は、カソード電極5に対向して配置され、カソード電極5との電位差(ゲート電圧)に応じて電子放出源6に電界を印加し、電子を放出させる。このグリッド電極10には、電子放出源6から放出された電子を通過させる微細な開口が多数形成されており、ステンレス材、ニッケル材、アンバー材等の導電性の薄板に、エッチング或はパンチング法等を用いて円形や矩形等の多数の開口が形成される。   The grid electrode 10 is disposed to face the cathode electrode 5 and applies an electric field to the electron emission source 6 according to a potential difference (gate voltage) with the cathode electrode 5 to emit electrons. The grid electrode 10 has a large number of fine openings through which electrons emitted from the electron emission source 6 pass, and is formed by etching or punching a conductive thin plate such as stainless steel, nickel, or amber. Etc., a large number of openings such as a circle and a rectangle are formed.

蛍光板電極15は、投光面となるガラス基材3の裏面側に配置された透明導電膜(例えば、ITO膜)からなり、グリッド電極10(カソード電極5)に対向する面に、電子放出源6から放出された電子によって励起発光される蛍光体16が塗布されている。蛍光体16は、例えば、酸化亜鉛系等の材料を用い、インクジェット法、フォトグラフィ法、沈殿法、電着法等によって蛍光板電極15上に成膜される。   The fluorescent plate electrode 15 is made of a transparent conductive film (for example, ITO film) disposed on the back surface side of the glass substrate 3 serving as a light projecting surface, and has an electron emission source on the surface facing the grid electrode 10 (cathode electrode 5). A phosphor 16 that is excited and emitted by electrons emitted from 6 is applied. The phosphor 16 is formed on the phosphor plate electrode 15 by using an ink jet method, a photolithography method, a precipitation method, an electrodeposition method or the like using, for example, a zinc oxide-based material.

以上の発光装置1においては、ガラス基材2上のカソード電極5及び電子放出源6からなるカソード極7に対して、ガラス基材3上の蛍光板電極15及び蛍光体16からなるアノード極17を所定の正の高電位に維持し、カソード極7とグリッド電極10との間に所定のゲート電圧を印加して電子放出源6から真空中に電子を電界放出させる。この電界放出された電子はアノード極17に向って加速され、グリッド電極10の開口部を通過した電子が蛍光体16に衝突して光を放つ。   In the light emitting device 1 described above, the anode electrode 17 made of the fluorescent plate electrode 15 and the phosphor 16 on the glass substrate 3 is provided with respect to the cathode electrode 7 made of the cathode electrode 5 and the electron emission source 6 on the glass substrate 2. While maintaining a predetermined positive high potential, a predetermined gate voltage is applied between the cathode 7 and the grid electrode 10 to cause electrons to be emitted from the electron emission source 6 into the vacuum. The electrons emitted from the field are accelerated toward the anode electrode 17, and the electrons passing through the openings of the grid electrode 10 collide with the phosphor 16 to emit light.

この場合、電子放出源6の電界放出特性は必ずしも一定ではないことから、通常のゲート電圧で発生する電界強度では、電子放出源6の領域によって電子放出の電流密度が異なり、蛍光体16全体として見ると発光輝度のムラが生じることがある。従って、本発光装置1には、電子放出源6における電界放出の電流密度が設定値以上となる制御電圧Vgをゲート電圧としてカソード電極5に周期的に印加する後述の電圧制御手段が備えられ、この制御電圧Vgにより、蛍光体16全体を高輝度で発光させる電流密度となるような電界強度をカソード極7全体に与える。   In this case, since the field emission characteristics of the electron emission source 6 are not necessarily constant, the current density of the electron emission differs depending on the region of the electron emission source 6 in the electric field intensity generated at a normal gate voltage. When viewed, uneven brightness may occur. Therefore, the light emitting device 1 is provided with voltage control means (described later) for periodically applying the control voltage Vg at which the field emission current density in the electron emission source 6 is equal to or higher than a set value to the cathode electrode 5 as a gate voltage. By this control voltage Vg, an electric field strength that gives a current density that causes the entire phosphor 16 to emit light with high luminance is given to the entire cathode electrode 7.

すなわち、一般に、電界放出の電流密度は、印加する電界強度が比較的小さい場合には、電界強度の増加に応じて電流密度も緩やかに増加するが、或る電界強度を越えると、電流密度が急激に増加する。一方、蛍光体は、電流密度の増加に応じて発光輝度が高くなるが、所定の電流密度以上では発光が飽和状態となり、それ以上電流密度を増加させても、発光輝度は高くならない。従って、カソード極7に与える電界強度を通常よりも大幅に大きくして蛍光体16を飽和状態或は飽和状態に近い高輝度で発光させることにより、電子放出源6の電界放出特性のバラツキによる領域毎の発光輝度の差を小さくすることができ、発光ムラを低減することができる。   That is, in general, the current density of field emission increases gradually as the electric field strength increases when the applied electric field strength is relatively small, but when the electric field strength exceeds a certain electric field strength, the current density increases. Increases rapidly. On the other hand, the phosphor has higher emission luminance as the current density increases. However, the emission luminance is saturated at a predetermined current density or higher, and the emission luminance does not increase even if the current density is increased further. Accordingly, the electric field intensity applied to the cathode electrode 7 is greatly increased than usual so that the phosphor 16 emits light in a saturated state or at a high brightness close to the saturated state, thereby causing a region due to variations in the field emission characteristics of the electron emission source 6. It is possible to reduce a difference in light emission luminance for each light emission and to reduce light emission unevenness.

本実施の形態においては、カソード極7に印加する制御電圧Vgに対応する電流密度の設定値を、蛍光体16での発光が飽和状態に達する電流密度として、電子放出源6における電界放出の電流密度が設定値(蛍光体16での発光が飽和状態に達する電流密度)以上となる電界強度を発生させる制御電圧Vgをカソード極7に印加する。例えば、グリッド電極10とカソード電極15との距離Aを100μmとして、カソード極7において、100μA/cm2の電子放出を得るために必要な電界強度がAA部で0.8V/μm、BB部で1.2V/μmである場合、カソード極7全体に2V/μmの電界を発生させる制御電圧Vgを印加することにより、蛍光体16全体を飽和状態で高輝度発光させる。 In the present embodiment, the current density setting value corresponding to the control voltage Vg applied to the cathode electrode 7 is defined as the current density at which the light emission from the phosphor 16 reaches a saturated state, and the field emission current in the electron emission source 6 is determined. A control voltage Vg for generating an electric field strength at which the density is equal to or higher than a set value (current density at which light emission from the phosphor 16 reaches a saturated state) is applied to the cathode electrode 7. For example, assuming that the distance A between the grid electrode 10 and the cathode electrode 15 is 100 μm, the electric field strength required to obtain the electron emission of 100 μA / cm 2 at the cathode electrode 7 is 0.8 V / μm at the AA portion and at BB portion. When the voltage is 1.2 V / μm, the control voltage Vg for generating an electric field of 2 V / μm is applied to the entire cathode electrode 7, thereby causing the entire phosphor 16 to emit light with high brightness in a saturated state.

蛍光体16を高輝度発光させる制御電圧Vgは、蛍光体16の焼損や無駄な電力消費を防止するため短時間だけ印加し、この短時間の高輝度発光を周期的に繰返すことにより、人間の視覚の残像現象を利用した連続発光として認識させる。制御電圧Vgをゲート電圧として印加する高輝度発光の期間以外は、本実施の形態においては、ゲート電圧を零としてカソード電流を流さない休止期間とする。   The control voltage Vg for causing the phosphor 16 to emit light with high brightness is applied only for a short time in order to prevent burning of the phosphor 16 and wasteful power consumption. Recognize as continuous light emission using visual afterimage phenomenon. Except for the period of high-luminance light emission in which the control voltage Vg is applied as the gate voltage, in this embodiment, the gate voltage is set to zero and the rest period in which no cathode current flows is set.

制御電圧Vgをカソード電極5に印加する電圧制御手段としての機能は、具体的には、図2に示すトランスからなる変圧回路20によって実現することができる。変圧回路20は、一次側に図示しないパルス発生源が接続され、二次側の高圧用の第1タップTP1に蛍光板電極15(アノード極17)、二次側の低圧用の第2タップTP2にカソード電極5(カソード極7)、二次側の高圧と低圧との間の第3タップTP3にグリッド電極10がそれぞれ接続されている。第1タップTP1と第2タップTP2とは、蛍光板電極15からカソード電極5に印加する正の高電圧(アノード電圧)Vaを発生する二次巻線に設けられ、第3タップTP3と第2タップTP2とは、グリッド電極10からカソード電極5に印加する制御電圧Vgを発生する二次巻線に設けられている。   Specifically, the function as voltage control means for applying the control voltage Vg to the cathode electrode 5 can be realized by the transformer circuit 20 including a transformer shown in FIG. The transformer circuit 20 has a pulse generation source (not shown) connected to the primary side, the fluorescent plate electrode 15 (anode electrode 17) on the secondary high voltage first tap TP1, and the secondary low voltage second tap TP2. The grid electrode 10 is connected to the cathode electrode 5 (cathode electrode 7) and the third tap TP3 between the high and low pressures on the secondary side. The first tap TP1 and the second tap TP2 are provided in the secondary winding that generates a positive high voltage (anode voltage) Va applied from the fluorescent plate electrode 15 to the cathode electrode 5, and the third tap TP3 and the second tap TP2 are provided. TP2 is provided in a secondary winding that generates a control voltage Vg applied from the grid electrode 10 to the cathode electrode 5.

パルス発生源からは、ON(ハイレベル)期間がT2で、ON(ハイレベル),OFF(ローレベル)の周期がT1のパルス信号が出力され、このパルス信号を変圧回路20の一次側に印加することにより、T2期間で二次側の第3タップTP3と第2タップTP2との間に発生する制御電圧Vgがグリッド電極10からカソード電極5に周期的に印加され、蛍光体16が飽和状態で周期的に高輝度発光する。前述したように、蛍光体16が飽和状態に達した電流を流し続けると、蛍光体16の焼損や電力の無駄な消費につながる。従って、制御電圧Vgを印加するT2期間に対し、(T1−T2)期間はゲート電圧が零とされてカソード電流を流さない十分な休止期間として設けられる。この十分な休止期間を確保するためには、例えば、繰返し周期T1を、蛍光体16を飽和状態で高輝度発光させるT2期間の少なくとも10倍以上とすることが望ましい。   The pulse generation source outputs a pulse signal having an ON (high level) period of T2 and an ON (high level) and OFF (low level) period of T1, and this pulse signal is applied to the primary side of the transformer circuit 20. As a result, the control voltage Vg generated between the third tap TP3 and the second tap TP2 on the secondary side in the period T2 is periodically applied from the grid electrode 10 to the cathode electrode 5, and the phosphor 16 is saturated. Periodically emits high-intensity light. As described above, if the current that the phosphor 16 reaches the saturation state is continuously supplied, the phosphor 16 is burned out and the power is wasted. Therefore, the (T1-T2) period is provided as a sufficient pause period in which the gate voltage is zero and no cathode current flows, in contrast to the T2 period in which the control voltage Vg is applied. In order to ensure this sufficient rest period, for example, it is desirable to set the repetition period T1 to at least 10 times the T2 period during which the phosphor 16 emits light with high brightness in a saturated state.

尚、休止期間である(T1−T2)期間には、ゲート電圧を完全に零にすることなく、弱い発光が可能となる電圧としても良い。当然ながら、この状態では、蛍光体16のAA部に対向する位置では若干発光してもBB部に対向する位置は殆ど発光しなくなり、発光輝度のムラが発生するが、人間の視覚にはT2期間における高輝度発光が残像として残り、周期T1の周波数が略60Hz以上であれば、連続発光として認識される。   Note that in the (T1-T2) period, which is a pause period, the gate voltage may be set to a voltage at which weak light emission is possible without being completely zero. Of course, in this state, even if light is emitted slightly at the position facing the AA portion of the phosphor 16, light is hardly emitted at the position facing the BB portion and unevenness in light emission luminance occurs. If high-intensity light emission in the period remains as an afterimage and the frequency of the period T1 is approximately 60 Hz or more, it is recognized as continuous light emission.

例えば、変圧回路20の一次側に入力するパルス信号を、周期T1=10ms(周波数100Hz)、制御電圧Vgを印加する期間T2=1msの信号として、1msの期間に、AA部から300μA/cm2の電子放出が得られ、また、BB部から200μA/cm2の電子放出が得られものとし、更に、蛍光体16の発光が200μA/cm2の電流密度で飽和状態に達するものとすると、制御電圧Vgを印加する1msでAA部もBB部もほぼ同じ発光輝度が得られ、休止期間(T1−T2)の9msでの残像により、連続した輝度ムラのない均一な発光として認識される。 For example, a pulse signal input to the primary side of the transformer circuit 20 is a signal having a period T1 = 10 ms (frequency 100 Hz) and a period T2 = 1 ms in which the control voltage Vg is applied, and is 300 μA / cm 2 from the AA unit in a 1 ms period. electron emission is obtained, also with those of the electron emission obtained 200 .mu.A / cm 2 from the BB unit, further, assuming that light emitted from the phosphor 16 reaches saturation at a current density of 200 .mu.A / cm 2, the control The AA portion and the BB portion have substantially the same emission luminance in 1 ms when the voltage Vg is applied, and it is recognized as uniform light emission without continuous luminance unevenness due to the afterimage in 9 ms of the rest period (T1-T2).

また、本実施の形態では、制御電圧Vgの印加に同期して、蛍光板電極15からカソード電極5へ高圧のアノード電圧Vaを印加する。すなわち、パルス信号のT2期間で、グリッド電極10からカソード電極5に蛍光体16の飽和状態での高輝度発光を可能とする制御電圧Vgが印加されると共に、この制御電圧Vgが印加されるT2期間のみ、蛍光板電極15からカソード電極5に高電圧のアノード電圧Vaが印加される。   In the present embodiment, a high voltage anode voltage Va is applied from the fluorescent plate electrode 15 to the cathode electrode 5 in synchronization with the application of the control voltage Vg. That is, during the T2 period of the pulse signal, the control voltage Vg that enables high-luminance light emission in the saturation state of the phosphor 16 is applied from the grid electrode 10 to the cathode electrode 5, and T2 is applied to this control voltage Vg. Only during the period, a high anode voltage Va is applied from the fluorescent plate electrode 15 to the cathode electrode 5.

これにより、蛍光体16を飽和状態で高輝度発光させるT2期間以外では、蛍光板電極15及びグリッド電極10からの電圧を零として、不要な電力消費を防止することができる。また、変圧回路20にパルス信号を入力するのみで、発光に必要な期間のみアノード電圧及びゲート電圧を同時に印加することができ、従来のように、アノード電圧やゲート電圧を印加するために整流回路等を用いて直流高電圧を生成する必要がなく、簡素な構成としてコスト低減を図ることができる。   This makes it possible to prevent unnecessary power consumption by setting the voltages from the fluorescent plate electrode 15 and the grid electrode 10 to zero except during the T2 period in which the phosphor 16 emits light with high brightness in a saturated state. In addition, the anode voltage and the gate voltage can be simultaneously applied only during a period necessary for light emission only by inputting a pulse signal to the transformer circuit 20, and a rectifier circuit for applying the anode voltage and the gate voltage as in the prior art. Etc., and it is not necessary to generate a high DC voltage, and the cost can be reduced with a simple configuration.

実際の装置設計では、目的とする発光輝度と発光の均一性を得るように、蛍光板電極15に塗布する蛍光体16の種類や厚み、蛍光板電極15及びグリッド電極10に印加する電圧、パルス信号の周期T1、制御電圧Vgを印加する期間T2の時間等を最適に調節する。   In the actual device design, the type and thickness of the phosphor 16 applied to the phosphor plate electrode 15, the voltage applied to the phosphor plate electrode 15 and the grid electrode 10, and the pulse signal so as to obtain the desired emission luminance and emission uniformity. The period T1 and the time period T2 during which the control voltage Vg is applied are optimally adjusted.

また、本発明の発光方式では、パルス信号の周波数を、例えば60Hzから200Hz程度に可変することにより、発光輝度を自由に調節することができる。更に、カソード極に流れる平均電流または実効電流を検出し、常時一定のカソード電流が流れ続けるように、パルス信号の周期を自動調節すれば、カソードの経年的な変化に伴う発光輝度の低下を自動的に補正することも可能である。   In the light emission method of the present invention, the emission luminance can be freely adjusted by changing the frequency of the pulse signal from, for example, about 60 Hz to 200 Hz. Furthermore, if the average or effective current flowing through the cathode electrode is detected and the period of the pulse signal is automatically adjusted so that a constant cathode current continues to flow at all times, the decrease in emission luminance associated with changes over time in the cathode is automatically performed. It is also possible to correct automatically.

発光装置の基本構成図Basic configuration diagram of light emitting device 変圧回路の構成図Configuration diagram of transformer circuit 従来の発光装置における発光ムラを示す説明図Explanatory drawing which shows the light emission nonuniformity in the conventional light-emitting device.

符号の説明Explanation of symbols

1 発光装置
5 カソード電極
6 電子放出源
10 グリッド電極
15 蛍光板電極
16 蛍光体
20 変圧回路(電圧制御手段)
Vg 制御電圧
DESCRIPTION OF SYMBOLS 1 Light-emitting device 5 Cathode electrode 6 Electron emission source 10 Grid electrode 15 Phosphor plate electrode 16 Phosphor 20 Transformer circuit (voltage control means)
Vg control voltage

Claims (5)

少なくとも、電子放出源を有するカソード電極と蛍光体を有する蛍光板電極とが真空中で対向配置された発光装置において、
上記電子放出源における電界放出の電流密度が上記蛍光体での発光が飽和状態に達する電流密度以上となる制御電圧を、上記カソード電極に周期的に印加する電圧制御手段を備えたことを特徴とする発光装置。
At least in a light emitting device in which a cathode electrode having an electron emission source and a fluorescent plate electrode having a phosphor are arranged opposite to each other in a vacuum,
A voltage control means is provided for periodically applying a control voltage at which the current density of field emission in the electron emission source is equal to or higher than a current density at which light emission from the phosphor reaches a saturated state to the cathode electrode. Light-emitting device.
上記発光装置は、
上記カソード電極と上記蛍光板電極との間にグリッド電極を配置し、
上記電圧制御手段は、
上記グリッド電極と上記カソード電極との間に上記制御電圧を周期的に印加すると共に、上記蛍光板電極と上記カソード電極との間に上記制御電圧よりも高い電圧を同期して印加することを特徴とする請求項記載の発光装置。
The light emitting device
A grid electrode is disposed between the cathode electrode and the fluorescent plate electrode,
The voltage control means is
The control voltage is periodically applied between the grid electrode and the cathode electrode, and a voltage higher than the control voltage is synchronously applied between the fluorescent plate electrode and the cathode electrode. The light-emitting device according to claim 1 .
上記電圧制御手段を、上記カソード電極と上記グリッド電極と上記蛍光板電極とを二次側に接続した変圧回路を用いて構成し、
上記変圧回路の一次側に周期的な電圧信号を印加することにより、上記グリッド電極と上記カソード電極との間に上記制御電圧を印加すると共に、上記蛍光板電極と上記カソード電極との間に上記制御電圧よりも高い電圧を同期して印加することを特徴とする請求項記載の発光装置。
The voltage control means is configured using a transformer circuit in which the cathode electrode, the grid electrode, and the fluorescent plate electrode are connected to the secondary side,
By applying a periodic voltage signal to the primary side of the transformer circuit, the control voltage is applied between the grid electrode and the cathode electrode, and the control is performed between the fluorescent plate electrode and the cathode electrode. 3. The light emitting device according to claim 2 , wherein a voltage higher than the voltage is applied synchronously.
上記カソード電極へ60Hz以上の繰返し周期で上記制御電圧を印加することを特徴とする請求項1〜3の何れか一に記載の発光装置。 The light-emitting device according to claim 1 , wherein the control voltage is applied to the cathode electrode at a repetition period of 60 Hz or more. 上記カソード電極へ上記制御電圧を印加する周期を、上記カソード電極へ上記制御電圧を印加する期間の少なくとも10倍以上とすることを特徴とする請求項1〜4の何れか一に記載の発光装置。 5. The light-emitting device according to claim 1 , wherein a period in which the control voltage is applied to the cathode electrode is at least 10 times longer than a period in which the control voltage is applied to the cathode electrode. .
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