JPH0636354B2 - Light emitting electron tube - Google Patents

Light emitting electron tube

Info

Publication number
JPH0636354B2
JPH0636354B2 JP12061086A JP12061086A JPH0636354B2 JP H0636354 B2 JPH0636354 B2 JP H0636354B2 JP 12061086 A JP12061086 A JP 12061086A JP 12061086 A JP12061086 A JP 12061086A JP H0636354 B2 JPH0636354 B2 JP H0636354B2
Authority
JP
Japan
Prior art keywords
cathode
tube
anode
light emitting
light
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.)
Expired - Lifetime
Application number
JP12061086A
Other languages
Japanese (ja)
Other versions
JPS62276749A (en
Inventor
唯夫 植月
眞 東方
宏司 平松
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP12061086A priority Critical patent/JPH0636354B2/en
Publication of JPS62276749A publication Critical patent/JPS62276749A/en
Publication of JPH0636354B2 publication Critical patent/JPH0636354B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【発明の詳細な説明】 [技術分野] 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。
Description: TECHNICAL FIELD The present invention relates to a light emitting electron tube which emits light to the outside of a tube by exciting a light emitting gas sealed inside the tube by collision of electrons.

[背景技術] 従来技術として、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 ART As a conventional technique, for example, Japanese Patent Laid-Open No. 57-130364
There is a lamp as disclosed in Japanese Patent 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
空とするのではなく、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
れた電子を電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(紫外線励起型)に当て、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。
In such a lamp, the inside of the tube body 1 is not made into a complete vacuum as shown in FIG. By accelerating with and making the anode 3 into an electron-passing shape, most of the electrons collide with mercury vapor, which is an ultraviolet ray radiating gas, in the back space 4 ', excite mercury to cause ultraviolet ray emission, and this ultraviolet ray is emitted. It is applied to a phosphor (ultraviolet-excited type) applied to the inner surface of the tubular body 1 to perform desired visible light conversion. In the figure, 5 is a DC power supply.

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。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図のロ曲線で示すようにかなり高く、励起発
光に最適な値(第6図のイ曲線)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, it is necessary to remove the influence of the space charge inside the tubular body 1 in order to make the electrons enter the back space 4 '. Therefore, it is necessary to apply a potential higher than the ionization voltage of the enclosed substance to the anode so that the inside of the tube body 1 is in a plasma state, and as a result, the electron energy in the back space 4'is considerably large as shown by the curve B in FIG. It is high and deviates greatly from the optimum value for excited light emission (curve A in FIG. 6), and there is a problem that the light emission efficiency is very poor.

[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 an object of the present invention is to reduce the energy of electrons in a tubular body,
Another object is to provide a light emitting electron tube with higher luminous efficiency.

[発明の開示] 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
体で囲繞される中央透孔内に、該中央透孔の直径方向に
N、Sの磁極を位置させた磁石を配置し、該磁石から発
生する磁力線にアノードとカソードとを結ぶ線が直交す
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
するものである。
DISCLOSURE OF THE INVENTION According to the present invention, a low-pressure light emitting gas is sealed inside, an annular tube body that is transparent to light radiation and has both ends communicating with each other, and a thermoelectron disposed inside the tube body. In a light emitting electron tube comprising an emission type cathode and an anode arranged inside the tube at a distance from the cathode which is equal to or less than the mean free path of electrons, the central through hole is surrounded by the tube. A magnet having N and S magnetic poles arranged in the diametrical direction is arranged, and the anode and the cathode are arranged so that the line connecting the anode and the cathode is orthogonal to the magnetic force line generated from the magnet. It is a thing.

以下本発明を実施例により説明する。The present invention will be described below with reference to examples.

実施例1 第1図(a)(b)は実施例の概略構成を示しており、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れ、また管体1で囲
繞される中心透孔7内には永久磁石からなる磁石6を、
中心透光7の直径方向に両端のN,Sの磁極を位置させ
て、発生する磁力線が管体1の周方向の形状に沿うよう
に配設してある。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か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とを結ぶ線が磁石
6が発生する磁力線と直交するようにアノード3を配設
してある。
Example 1 FIGS. 1 (a) and (b) show a schematic configuration of an example, in which a light-emitting gas such as mercury, cesium, sodium or the like is emitted at a low pressure in an annular tube body 1 having a light-transmitting property. The magnet 6 made of a permanent magnet is enclosed in the central through hole 7 surrounded by the tube body 1.
The N and S magnetic poles at both ends are positioned in the diameter direction of the central light transmission 7, and the generated magnetic force lines are arranged along the circumferential shape of the tubular body 1. Further, a thermionic emission type cathode 2 is provided inside the tube body 1, and the distance from the cathode 2 is equal to or less than the mean free path of electrons so as to obtain a positive characteristic discharge, and the cathode 2 is connected. The anode 3 is arranged so that the lines are orthogonal to the lines of magnetic force generated by the 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 described based on the principle diagram of FIG.

まずカソード2とアノード3間に直流電源5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(第2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、そこで封入してある光放射気体、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。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
に得られたエネルギは∫lEdlで示される。
First, when the voltage of the DC power supply 5 is applied between the cathode 2 and the anode 3, the electrons that have flown out of the cathode 2 enter the light emitting space 4 while being wrapped around the magnetic field lines (shown by the broken line in FIG. 2) of the magnet 6 and are sealed therein. It collides with a light emitting gas, such as Hg atoms, and changes its orbit. In other words, move to another magnetic field line. Then, the electrons are accelerated by the electric field and collide with Hg atoms again. By repeating this movement many times, the light emitting space 4 emits light uniformly over the entire surface. Here, the energy of electrons when they collide with Hg atoms will be described. First, FIG. 3 shows the potential distribution between the anode 3 and the cathode 2. From this figure, the energy obtained until the first collision of the electron jumping out of the cathode 2 is represented by ∫lEdl.

ここで電子が第3図に示すようなカソード2→l1→l2
l3→l4→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∫lEdl+∫l
Edl+∫lEdl+∫lEdl=eVaとなる。これよ
り電子が衝突するまでに得る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る。尚Vaはアノード電位、
Eは電界の強さである。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。
Here, the electron is the cathode 2 → l 1 → l 2 → as shown in Fig. 3.
Assuming that the route is l 3 → l 4 → anode 3,
The energy obtained in this process is ∫lEdl + ∫l
Edl + ∫lEdl + ∫lEdl = eVa. From this, the energy obtained until the electrons collide is considerably lower than the potential applied to the anode 3. Va is the anode potential,
E is the strength of the electric field. That is, the energy of the electrons in the space to emit light is considerably lower than the potential applied to the anode 3, which is suitable for exciting, for example, ultraviolet rays, and the light emission efficiency is further increased.

実施例2 本実施例は上記実施例1が磁石6として永久磁石を用い
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。
Example 2 In this example, a permanent magnet was used as the magnet 6 in Example 1 above, but as shown in FIG. 5, an electromagnet was used as the magnet 6 in this example.

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長い環状
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 tubular body having a short axial length is used as the tubular body 1, but it goes without saying that an annular tubular body having a relatively long axial length may be used.

[発明の効果] 本発明は上述のように構成した光放射電子管において、
管体で囲繞される中央透孔内に、該中央透孔の直径方向
にN、Sの磁極を位置させた磁石を配置し、該磁石から
発生する磁力線にアノードとカソードとを結ぶ線が直交
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一つ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 configured as described above,
A magnet having N and S magnetic poles positioned in the diameter direction of the central through hole is arranged in the central through hole surrounded by the tubular body, and a line connecting the anode and the cathode is orthogonal to a magnetic force line generated from the magnet. Since the anode and the cathode are arranged so that the energy of the electron in the space to emit light is much lower than the potential applied to the anode, it is suitable for excitation. There is an effect that the rate of excitation by the γ is increased, the luminous efficiency is increased, and moreover, the annular luminescent space can be made to uniformly emit light by the above-described swirling motion of the electrons.

【図面の簡単な説明】[Brief description of drawings]

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、第2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の概略斜視図、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。
1 (a) and 1 (b) are a top view and a side sectional view showing a schematic configuration of a first embodiment of the present invention, FIG. 2 and FIG. 3 are explanatory diagrams of the same operating principle, and FIG. 5 is a schematic perspective view of Embodiment 2 of FIG.
FIG. 6 is a schematic configuration diagram of a conventional example, and FIG. 6 is an energy distribution explanatory diagram of the same as above. Reference numeral 1 is a tubular body, 2 is a cathode, 3 is a cathode, and 6 is a magnet.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】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た環状の管体と、該管体内部に
配置された熱放出型カソードと、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、管体で囲繞され
る中央透孔内に、該中央透孔の直径方向にN、Sの磁極
を位置させた磁石を配置し、該磁石から発生する磁力線
にアノードとカソードとを結ぶ線が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. A low-pressure light-emitting gas is sealed inside, an annular tube having a light-transmitting property with respect to light radiation, a heat-releasing cathode disposed inside the tube, and a cathode from the cathode. In a light emitting electron tube consisting of an anode disposed inside the tube at a distance equal to or less than the mean free path of electrons, in a central through hole surrounded by the tube, N, S in the diameter direction of the central through hole A light emitting electron tube characterized in that a magnet having magnetic poles is arranged, and an anode and a cathode are arranged such that a line connecting the anode and the cathode is orthogonal to a line of magnetic force generated from the magnet.
JP12061086A 1986-05-26 1986-05-26 Light emitting electron tube Expired - Lifetime JPH0636354B2 (en)

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 JPS62276749A (en) 1987-12-01
JPH0636354B2 true 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)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
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
JPS62276749A (en) 1987-12-01

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