JPS62276749A - Luminous radiation electron tube - Google Patents
Luminous radiation electron tubeInfo
- Publication number
- JPS62276749A JPS62276749A JP12061086A JP12061086A JPS62276749A JP S62276749 A JPS62276749 A JP S62276749A JP 12061086 A JP12061086 A JP 12061086A JP 12061086 A JP12061086 A JP 12061086A JP S62276749 A JPS62276749 A JP S62276749A
- Authority
- JP
- Japan
- Prior art keywords
- cathode
- anode
- magnetic force
- lines
- tube
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000005855 radiation Effects 0.000 title claims abstract description 5
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 abstract description 5
- 229910052753 mercury Inorganic materials 0.000 abstract description 4
- DGAQECJNVWCQMB-PUAWFVPOSA-M Ilexoside XXIX Chemical compound C[C@@H]1CC[C@@]2(CC[C@@]3(C(=CC[C@H]4[C@]3(CC[C@@H]5[C@@]4(CC[C@@H](C5(C)C)OS(=O)(=O)[O-])C)C)[C@@H]2[C@]1(C)O)C)C(=O)O[C@H]6[C@@H]([C@H]([C@@H]([C@H](O6)CO)O)O)O.[Na+] DGAQECJNVWCQMB-PUAWFVPOSA-M 0.000 abstract description 2
- 229910052792 caesium Inorganic materials 0.000 abstract description 2
- TVFDJXOCXUVLDH-UHFFFAOYSA-N caesium atom Chemical compound [Cs] TVFDJXOCXUVLDH-UHFFFAOYSA-N 0.000 abstract description 2
- 229910052708 sodium Inorganic materials 0.000 abstract description 2
- 239000011734 sodium Substances 0.000 abstract description 2
- 230000002093 peripheral effect Effects 0.000 abstract 2
- 230000035699 permeability Effects 0.000 abstract 1
- 230000008092 positive effect Effects 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 3
- 230000005284 excitation Effects 0.000 description 3
- 230000004323 axial length Effects 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000010438 granite Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000005191 phase separation Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Landscapes
- Vessels And Coating Films For Discharge Lamps (AREA)
- Discharge Lamps And Accessories Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
3、発明の詳細な説明
[技術分野1
本発明は管体内部に封入した光放射気体を電子の衝突に
より励起させ、光を管体外へ放射する光放射電子管に関
するものである。Detailed Description of the Invention 3. Detailed Description of the Invention [Technical Field 1 The present invention relates to a light-emitting electron tube that excites a light-emitting gas sealed inside a tube by collision of electrons and emits light to the outside of the tube. It is.
[背景技術1
従来技術としで、たとえば、特開昭57−130364
号公報に開示されたようなランプがある。[Background technology 1 Prior art, for example, Japanese Patent Application Laid-Open No. 57-130364
There is a lamp as disclosed in the publication.
かかるランプは第5図に示すように管体1内を完全な真
空とするのではな(、例えば水銀蒸気が数mToor程
度存在する低真空とし、熱電子放出型カソード2より放
出された電子を?!!界により加速すると共にアノード
3を電子通過性の形状にすることにより、電子の大半を
背後空間4°で紫外線放射気体である水銀蒸気に衝突さ
せて水銀を励起して紫外線放射を起こし、この紫外線を
管体1の内面に塗布せる蛍光体(ga外era起型)に
当で、所望の可視光変換を行わせるものである。尚同図
中5は直流電源である。As shown in FIG. 5, such a lamp does not create a complete vacuum in the tube body 1 (for example, it creates a low vacuum in which mercury vapor exists at a depth of several mToor), and the electrons emitted from the thermionic-emitting cathode 2 are By accelerating the electrons by the field and making the anode 3 pass through the electrons, most of the electrons collide with mercury vapor, which is an ultraviolet emitting gas, at 4° in the back space, exciting the mercury and emitting ultraviolet radiation. The ultraviolet rays are applied to a phosphor (Ga-era type) applied to the inner surface of the tube body 1, and the desired visible light conversion is carried out.The reference numeral 5 in the figure is a DC power source.
ところでかかる従来例においては電子を背後空間4゛に
入射させるために、管体1内部の空間電荷の影響を除去
させる必要があった9そのためアノードには封入物質の
電離電圧以上の電位をかけ、管体1内をプラズマ状態に
しなければならず、その結果背後空間4゛内の電子エネ
ルギは第6図の口面線で示すようにかなり高く、励起発
尤に最適な値(pIS6図のイ曲#i)からは大きくず
れており、非常に発光効率が悪いという問題があった。By the way, in such a conventional example, in order to allow electrons to enter the back space 4', it was necessary to remove the influence of the space charge inside the tube body 19. Therefore, a potential higher than the ionization voltage of the enclosed substance was applied to the anode. The inside of the tube 1 must be brought into a plasma state, and as a result, the electron energy in the back space 4 is quite high as shown by the mouth line in Fig. 6, and is at an optimal value for excitation and emission (the image in Fig. pIS6). There was a large deviation from song #i), and there was a problem in that the luminous efficiency was extremely low.
[発明の目的]
本発明は上記の欠点に鑑みてなされたもので、その目的
とするところは管体内での電子のエネル゛ ギを低下さ
せ、より発光効率のよい光放射電子管を提供するにある
。[Object of the Invention] The present invention has been made in view of the above-mentioned drawbacks, and its purpose is to reduce the energy of electrons within the tube and provide a light-emitting electron tube with higher luminous efficiency. be.
[発明の開示1
本発明は内部に低圧の光放射気体が封入され、光放射に
対して透光性を有し両端が連通した環状の管体と、該管
体内部に配置された熱電子放出型カソードと、該カソー
ドからの相離が電子の平均自由行程以下で管体内部に配
置された7)−ドと上りなる光放射電子管において、管
体内を周方向の形状に沿うように磁力線が発生するよう
に配設した磁石と、上記ア/−ドと上記カソードとを結
ぶ線が上記磁力線と直交するように7メードとカソード
とを配設したことを特徴とするものである。[Disclosure of the Invention 1] The present invention comprises an annular tube in which a low-pressure light emitting gas is sealed, transparent to the light emission, and communicating at both ends, and a thermionic tube disposed inside the tube. In an emitting cathode and a light-emitting electron tube arranged inside a tube whose phase separation from the cathode is less than the mean free path of electrons, magnetic lines of force are formed along the circumferential shape of the tube. The present invention is characterized in that a magnet is disposed so as to generate a magnetic force, and a seven-meter and a cathode are disposed so that a line connecting the a/- and the cathode is orthogonal to the line of magnetic force.
以下本発明を実施例により説明する。The present invention will be explained below with reference to Examples.
えI汁と
第1図(a)(b)は実施例の概略Nt成を示しており
、透光性を有する、環状の管体1内には水銀、セシウム
、ナトリウム等の光放射気体が低圧で封入さ八、又中心
透孔7内には永久磁石からなる磁石6を発生する磁力線
が管体1の周方向の形状に沿うように配設しである。そ
して管体1内部には熱電子放出型カソード2を設けると
ともに、正特性放電が得られるように該カソード2がら
の距離が電子の平均自由行程に等しいか或いはそれ以下
で且つカソード2とを結、「線が磁石6が発生する磁力
線と直交するように77−ド3を配設しである。Figures 1(a) and 1(b) schematically show the Nt composition of the embodiment, in which a light emitting gas such as mercury, cesium, sodium, etc. is inside the annular tube body 1 having translucent properties. It is sealed at low pressure, and lines of magnetic force that generate a magnet 6 made of a permanent magnet are arranged in the center through hole 7 so as to follow the shape of the tube body 1 in the circumferential direction. A thermionic emission type cathode 2 is provided inside the tube 1, and the distance between the cathode 2 is equal to or less than the mean free path of electrons, and the cathode 2 is connected to the cathode 2 so that a positive characteristic discharge can be obtained. , 77-domain 3 is arranged so that its lines are perpendicular to the lines of magnetic force generated by magnet 6.
次に本発明光放射電子管の動作を第2図の原理図゛に基
づいて説明する。Next, the operation of the light emitting electron tube of the present invention will be explained based on the principle diagram shown in FIG.
まずカソード2と7ノ一ド3間に直流taSの電圧を印
加すると、カソード2を飛び出した電子は磁石6の磁力
線(ffi2図において破線で示す)に巻き付きながら
発光空間4に入射し、そこで封入しである光放射気体、
例えばHg原子と衝突し、軌道を変える。つまり他の磁
力線へ移る。そして電子は電界により加速されHg原子
とまた衝突する。この動きを何度も繰り返することによ
り発光空間4は全面均一発光する。ここでHg原子に衝
突する時の電子のエネルギについて説明すると。First, when a DC taS voltage is applied between the cathode 2 and the seventh node 3, the electrons ejected from the cathode 2 enter the light emitting space 4 while being wrapped around the magnetic field lines of the magnet 6 (indicated by broken lines in the FFI2 figure), where they are enclosed. A light emitting gas, which is
For example, it collides with an Hg atom and changes its orbit. In other words, it moves to other lines of magnetic force. The electrons are then accelerated by the electric field and collide with the Hg atoms again. By repeating this movement many times, the light emitting space 4 emits light uniformly over the entire surface. Let us now explain the energy of electrons when they collide with Hg atoms.
まず第3図にアノード3とカソード2間の電位分布を示
す。この図よりカソード2を飛び出した電子が初めて衝
突するまでに得られrこエネルギはりtE、J9で示さ
れる。First, FIG. 3 shows the potential distribution between the anode 3 and cathode 2. From this figure, the energy obtained by the electrons ejected from the cathode 2 until they collide for the first time is expressed as tE, J9.
ここで電子が第3図に示すようなカソード2→0.1→
Q、2→Q−−(1,+→アノード3という順路を通っ
たと仮定すれば、この過程における得られたエネルギは
So、 E da、 +fa、 E da +ra E
do、 十fa、 E da、 = eVaとなる。Here, electrons are transferred to the cathode 2→0.1→ as shown in Figure 3.
Assuming that the path is Q, 2 → Q--(1, + → anode 3), the energy obtained in this process is So, E da, +fa, E da +ra E
do, 10 fa, E da, = eVa.
これより電子が衝突するまでに得ろエネルぞは7)−ド
3に与える電位よりもがなり低くなる。尚Vaは7ノ一
ド電位、Eは電界の強さである9つまり発光すべき空間
での電子のエネルギはアノード3に与える電位よりもか
なり低くなって例えば紫外線を励起するに適し、より発
光効率が上昇する。From this, the energy obtained before the electrons collide becomes much lower than the potential given to the 7)-domain 3. In addition, Va is the node potential, and E is the strength of the electric field.9 In other words, the energy of electrons in the space where light should be emitted is much lower than the potential given to the anode 3, making it suitable for excitation of ultraviolet light, for example, and emitting more light. Efficiency increases.
及l鯵玄
本実施例(1±)−:f’、 ′=F施イη1]1が6
井汀6とLでikグ諧石を用いたが、第5図に示すよう
に本実施例では磁石6として電磁石を用いたものである
。and Genmoto Example (1±) −: f', ′=F η1] 1 is 6
Ik granite was used for the magnets 6 and L, but as shown in FIG. 5, in this embodiment, an electromagnet was used as the magnet 6.
尚各実施例では管体1として軸方向の長さが短い環状の
管体を使用しているが、軸方向の長さが比較的艮い環状
つまり円筒状のものでもよいのは勿論である。In each of the embodiments, an annular tube with a short axial length is used as the tube 1, but it is of course possible to use an annular or cylindrical tube with a relatively short axial length. .
[発明の効果]
本発明は上述のようにMIJ&した光放射電子管におい
て、管体内を周方向の形状に沿うように磁力線を発生す
るように配設した磁石と、上記アノードと上記カソード
とを結ぶ線が上記磁力線と直交するようにアノードとカ
ソードとを配設したので、発光すべき空間での電子のエ
ネルギはアノードに与える電位よりもかなり低くなって
励起に適し、また磁力線により電子が旋回運動を行うた
め−っの電子が励起する割合が増加して発光効率が上昇
、し、しかも環状の発光空間を上記の電子の旋回運動に
より均一に発光させることができるという効果を奏する
。[Effects of the Invention] The present invention provides a light-emitting electron tube that has undergone MIJ as described above, and connects a magnet disposed so as to generate lines of magnetic force along the circumferential shape of the tube, and the anode and cathode. Since the anode and cathode are arranged so that the lines are perpendicular to the magnetic field lines, the energy of the electrons in the space where light is to be emitted is much lower than the potential applied to the anode, which is suitable for excitation, and the magnetic field lines cause the electrons to rotate. In order to do this, the rate at which the electrons are excited increases and the luminous efficiency increases, and furthermore, the annular luminescent space can be uniformly emitted by the swirling movement of the electrons.
第1図(a)及び(b)は本発明の実施例1の概略構成
を示す上面図及び側断面図、152図、第3図は同上の
動作原理説明図、第4図は本発明の実施例2の概略耕視
図、第5図は従来例の概略構成図、第6図は同上のエネ
ルギ分布説明図であり、1は管体、2はカソード、3は
カソード、6は磁石である。
代理人 弁理士 石 1)艮 七
第1図
第2図
第3図FIGS. 1(a) and (b) are a top view and a side sectional view showing a schematic configuration of Embodiment 1 of the present invention, FIGS. Embodiment 2 is a schematic perspective view, FIG. 5 is a schematic configuration diagram of a conventional example, and FIG. 6 is an energy distribution explanatory diagram of the same as above, where 1 is a tube body, 2 is a cathode, 3 is a cathode, and 6 is a magnet. be. Agent Patent Attorney Ishi 1) Ai 7 Figure 1 Figure 2 Figure 3
Claims (1)
して透光性を有し両端が連通した環状の管体と、該管体
内部に配置された熱電子放出型カソードと、該カソード
からの距離が電子の平均自由行程以下で管体内部に配置
されたアノードとよりなる光放射電子管において、管体
内を周方向の形状に沿うように磁力線が発生するように
配設した磁石と、上記アノードと上記カソードとを結ぶ
線が上記磁力線と直交するようにアノードとカソードと
を配設したことを特徴とする光放射電子管。(1) An annular tube in which a low-pressure light emitting gas is sealed, transparent to light radiation, and communicating at both ends, and a thermionic emission cathode disposed inside the tube; In a light-emitting electron tube consisting of an anode arranged inside a tube at a distance from the cathode that is less than the mean free path of electrons, a magnet is arranged so that lines of magnetic force are generated along the circumferential shape of the tube. and a light-emitting electron tube, characterized in that the anode and the cathode are arranged so that a line connecting the anode and the cathode is orthogonal to the line of magnetic force.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12061086A JPH0636354B2 (en) | 1986-05-26 | 1986-05-26 | Light emitting electron tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12061086A JPH0636354B2 (en) | 1986-05-26 | 1986-05-26 | Light emitting electron tube |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS62276749A true JPS62276749A (en) | 1987-12-01 |
JPH0636354B2 JPH0636354B2 (en) | 1994-05-11 |
Family
ID=14790504
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12061086A Expired - Lifetime JPH0636354B2 (en) | 1986-05-26 | 1986-05-26 | Light emitting electron tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0636354B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH03236153A (en) * | 1990-02-13 | 1991-10-22 | Matsushita Electric Works Ltd | Light emitting electron tube |
-
1986
- 1986-05-26 JP JP12061086A patent/JPH0636354B2/en not_active Expired - Lifetime
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH03236153A (en) * | 1990-02-13 | 1991-10-22 | Matsushita Electric Works Ltd | Light emitting electron tube |
Also Published As
Publication number | Publication date |
---|---|
JPH0636354B2 (en) | 1994-05-11 |
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