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JPH0527946B2 - - Google Patents
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JPH0527946B2 - - Google Patents

Info

Publication number
JPH0527946B2
JPH0527946B2 JP59219926A JP21992684A JPH0527946B2 JP H0527946 B2 JPH0527946 B2 JP H0527946B2 JP 59219926 A JP59219926 A JP 59219926A JP 21992684 A JP21992684 A JP 21992684A JP H0527946 B2 JPH0527946 B2 JP H0527946B2
Authority
JP
Japan
Prior art keywords
waveguide
microwave
light source
source device
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
JP59219926A
Other languages
Japanese (ja)
Other versions
JPS6199264A (en
Inventor
Kenji Yoshizawa
Isao Shoda
Hitoshi Kodama
Kazuo Umagome
Kazushi Oonuki
Koji Komura
Hiroshi Ito
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP59219926A priority Critical patent/JPS6199264A/en
Priority to AU39176/85A priority patent/AU574435B2/en
Priority to US06/705,529 priority patent/US4673846A/en
Priority to EP85102201A priority patent/EP0153745B1/en
Priority to DE8585102201T priority patent/DE3582810D1/en
Priority to KR1019850001274A priority patent/KR900000359B1/en
Priority to CA000475611A priority patent/CA1273050A/en
Publication of JPS6199264A publication Critical patent/JPS6199264A/en
Priority to SG810/91A priority patent/SG81091G/en
Priority to HK815/91A priority patent/HK81591A/en
Publication of JPH0527946B2 publication Critical patent/JPH0527946B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J65/00Lamps without any electrode inside the vessel; Lamps with at least one main electrode outside the vessel
    • H01J65/04Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels
    • H01J65/042Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels by an external electromagnetic field
    • H01J65/044Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels by an external electromagnetic field the field being produced by a separate microwave unit
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P7/00Resonators of the waveguide type
    • H01P7/06Cavity resonators

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Circuit Arrangements For Discharge Lamps (AREA)
  • Discharge Lamps And Accessories Thereof (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は発生する光を好ましい状態で使用で
きるように改良されたマイクロ波放電光源装置に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a microwave discharge light source device that has been improved so that the generated light can be used in a preferable manner.

〔従来の技術〕[Conventional technology]

マイクロ波放電を利用した光源装置として、例
えば第5図のような特願昭59−39980号で提案さ
れているものがある。図において、1はマイクロ
波発振器であるマグネトロン、2はマグネトロン
アンテナ、3は端部にこのマイクロ波発振器を装
着した導波管、5はマイクロ波共振空胴で、導波
管3の他端部に接続された空胴壁6と円筒の金属
メツシユよりなる光透過性部材7とから構成され
る。8は空胴壁6に設けられた給電口で、導波管
3よりマイクロ波共振空胴5内にマイクロ波を給
電するものである。9はマイクロ波共振空胴5内
に配設された球形のランプで中に希ガスや水銀等
が封入され、石英ガラスのような透光体でできて
いる。91はランプ9の外壁から伸びたランプ支
持部でやはり石英ガラスのような誘電体であり、
ランプ止めネジ10でランプ9を空胴壁6に固定
している。11はマイクロ波共振空胴5から放射
された光を反射する光反射板、12はマグネトロ
ン1やランプ9を冷却する冷却フアンで、4は冷
却風を導波管内へ導びく通風口、13は全体を覆
う箱体である。
As a light source device using microwave discharge, for example, there is a light source device proposed in Japanese Patent Application No. 59-39980 as shown in FIG. In the figure, 1 is a magnetron which is a microwave oscillator, 2 is a magnetron antenna, 3 is a waveguide with this microwave oscillator attached to its end, 5 is a microwave resonant cavity, and the other end of the waveguide 3 It is composed of a cavity wall 6 connected to a cylindrical metal mesh and a light-transmitting member 7 made of a cylindrical metal mesh. Reference numeral 8 denotes a power feeding port provided in the cavity wall 6, which feeds microwaves from the waveguide 3 into the microwave resonant cavity 5. Reference numeral 9 denotes a spherical lamp disposed within the microwave resonant cavity 5, which is filled with a rare gas, mercury, etc., and is made of a transparent material such as quartz glass. Reference numeral 91 denotes a lamp support extending from the outer wall of the lamp 9, which is also made of a dielectric material such as quartz glass.
The lamp 9 is fixed to the cavity wall 6 with a lamp fixing screw 10. 11 is a light reflection plate that reflects the light emitted from the microwave resonance cavity 5; 12 is a cooling fan that cools the magnetron 1 and the lamp 9; 4 is a ventilation port that guides cooling air into the waveguide; It is a box that covers the whole thing.

この装置の動作は次のようである。マグネトロ
ン1で発振されたマイクロ波はマグネトロンアン
テナ2から導波管3へ伝搬モードとして励振され
る。このマイクロ波は給電口8を通じて空胴壁6
と光透過性部材7とで囲まれたマイクロ波共振空
胴5へ給電される。このマイクロ波によつてラン
プ9中の希ガスが放電し、このエネルギーでラン
プ壁が加熱され、封入された水銀等が蒸発、ガス
化して放電は水銀等の金属ガスの放電が主とな
り、ガスの種類に応じたスペクトルで発光する。
The operation of this device is as follows. The microwave oscillated by the magnetron 1 is excited as a propagation mode from the magnetron antenna 2 to the waveguide 3. This microwave is transmitted to the cavity wall 6 through the power supply port 8.
Power is supplied to the microwave resonant cavity 5 surrounded by the light transmitting member 7 and the light transmitting member 7. The rare gas in the lamp 9 is discharged by this microwave, and the lamp wall is heated by this energy, and the enclosed mercury etc. evaporate and gasify, and the discharge is mainly a discharge of metal gas such as mercury. It emits light in a spectrum depending on its type.

光透過性部材7はマイクロ波に対しては金属と
同様、反射するように作用し、光はメツシユ開口
部から透過するようになつている。すなわち、マ
イクロ波には不透明体として、光には透明体とし
て働く。したがつて、ランプ9からの光はマイク
ロ波共振空胴5から外へ放射され、光反射板11
で反射される。光反射板11は光の用途により
種々の形状に設計される。
The light-transmitting member 7 acts to reflect microwaves like metal, and the light is transmitted through the mesh openings. In other words, it acts as an opaque body for microwaves and as a transparent body for light. Therefore, the light from the lamp 9 is radiated out from the microwave resonant cavity 5 and the light reflecting plate 11
reflected. The light reflecting plate 11 is designed in various shapes depending on the use of light.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

上記のような従来のマイクロ波放電光源装置で
は、導波管3が光の放射方向の後方に伸びており
後方に多くの空間を占有する。したがつて、光源
と被照射面の距離が近づき、被照射面の端部では
光線が広がつたものとなり、平行光が要求される
ものでは満足な性能が得られない問題点があつ
た。
In the conventional microwave discharge light source device as described above, the waveguide 3 extends rearward in the light emission direction and occupies a large amount of space at the rear. Therefore, the distance between the light source and the surface to be irradiated becomes closer, and the light rays become spread out at the ends of the surface to be irradiated, causing the problem that satisfactory performance cannot be obtained in devices that require parallel light.

この発明はかかる問題点を解決するためになさ
れたもので、光源と被照射面の距離が近づかない
ように装置の奥行きを浅くできるマイクロ波放電
光源装置を提供することを目的とする。
The present invention was made to solve this problem, and an object of the present invention is to provide a microwave discharge light source device in which the depth of the device can be made shallow so that the distance between the light source and the surface to be irradiated does not become close.

〔問題点を解決するための手段〕[Means for solving problems]

この発明によるマイクロ波放電光源装置は、給
電口を光の放射方向と反対側に設け、かつマイク
ロ波発振器が装着された側の導波管軸の向きと、
給電口の面が直交せず、マイクロ波発振器とマイ
クロ波共振空胴を導波管に対し同じ側に設けたも
のである。
The microwave discharge light source device according to the present invention has a power supply port provided on the opposite side to the light emission direction, and the direction of the waveguide axis on the side where the microwave oscillator is attached.
The planes of the feed ports are not perpendicular to each other, and the microwave oscillator and microwave resonant cavity are provided on the same side of the waveguide.

〔作用〕[Effect]

この発明におけるマイクロ波放電光源装置は、
導波管がランプを有するマイクロ波共振空胴の後
方に伸びない構成となり、装置の奥行きを浅くす
る。
The microwave discharge light source device in this invention includes:
The configuration is such that the waveguide does not extend behind the microwave resonant cavity having the lamp, reducing the depth of the device.

〔実施例〕〔Example〕

以下、この発明の一実施例を図について説明す
る。第1図はこの発明の一実施例によるマイクロ
波放電光源装置を示す要部断面図であり、給電口
8の面と、マグネトロン1が装着された側の導波
管軸の向きは直交しないように、導波管3にコー
ナ部を設けている。31はこのような導波管のコ
ーナ部を示す。ここで、導波管3は方形導波管
で、第1図は、電界Eに垂直な断面図であり、コ
ーナ部はEコーナである。一方、第2図は第1図
に示される導波管、共振空胴中の電界E、磁界H
の分布を示す断面図である。図において、実線E
は電気力線すなわち電界を示し、小円Hは磁力線
すなわち磁界を示す。又、ここで、マイクロ波共
振空胴5は円筒形である。導波管3中のモードは
方形TE10モードであり、マイクロ波共振空胴5
中のモードは円筒のTE111モード、すなわち、ど
の方向にも電磁界の山が1つあるモードで励振さ
れている。導波管3中のTE10モードはコーナ部
31で図のように、電界、磁界の向きが共に変え
られる。この場合は、コーナ部31の角度θを
45°にして、電界、磁界の向きを直角に変えてい
る。したがつて、給電口8の導波管側の電磁界モ
ードは、第2図で示すの導波管長さがたとえ1/
4管内波長以下の短いものでも、TE10に非常に近
いモードになる。よつて、第5図の提案例を示す
円筒のマイクロ波共振空胴と同じものが、この発
明の構成のマイクロ波共振空胴として使用でき
る。すなわち、方形導波管のTE10モードから、
円筒共振空胴のTE111モードが第2図のように良
好に励振できるのである。ただし、が小さい場
合は、導波管側のモードがTE10と全く同一では
ないために、給電口の形状は第5図のものと少し
変える必要が生ずる場合もあるが、空胴は同一の
ものが使える。
An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 is a sectional view of a main part of a microwave discharge light source device according to an embodiment of the present invention, and the direction of the plane of the power supply port 8 and the axis of the waveguide on the side where the magnetron 1 is attached are not perpendicular to each other. In addition, a corner portion is provided in the waveguide 3. 31 indicates a corner portion of such a waveguide. Here, the waveguide 3 is a rectangular waveguide, and FIG. 1 is a cross-sectional view perpendicular to the electric field E, and the corner portion is the E corner. On the other hand, Figure 2 shows the waveguide shown in Figure 1, the electric field E in the resonant cavity, and the magnetic field H.
FIG. In the figure, the solid line E
indicates electric lines of force, that is, an electric field, and small circle H indicates lines of magnetic force, that is, a magnetic field. Also, here, the microwave resonant cavity 5 has a cylindrical shape. The mode in the waveguide 3 is a square TE 10 mode, and the microwave resonant cavity 5
The mode inside is excited as a cylindrical TE 111 mode, that is, a mode with one peak of electromagnetic field in every direction. In the TE 10 mode in the waveguide 3, the directions of both the electric and magnetic fields are changed at the corner 31 as shown in the figure. In this case, the angle θ of the corner portion 31 is
The angle is set at 45°, and the directions of the electric and magnetic fields are changed to right angles. Therefore, the electromagnetic field mode on the waveguide side of the power feed port 8 is generated even if the waveguide length shown in Fig. 2 is 1/
Even short wavelengths of less than 4 tube wavelengths result in a mode very close to TE 10 . Therefore, the same cylindrical microwave resonant cavity as the proposed example shown in FIG. 5 can be used as the microwave resonant cavity in the configuration of the present invention. That is, from the TE 10 mode of the rectangular waveguide,
The TE 111 mode of the cylindrical resonant cavity can be excited well as shown in Figure 2. However, if is small, the mode on the waveguide side is not exactly the same as TE 10 , so the shape of the feed port may need to be slightly different from that in Figure 5, but the cavity is the same. Things can be used.

一例として、特願昭59−39980号で提案された
と同じ、導波管3の断面形状が95mm×54mmの方形
のもので、マイクロ波共振空胴5は直径80mm、高
さ90mmの円筒空胴で、ランプ9は直径30mmの球形
に、Ar60torr、Hg100mg封入したものを用い、
導波管のコーナ部として、第2図のθが45°,
が8mmのものを用いた結果、周波数2450MHz、電
力800Wのマイクロ波で励振して定常に達するま
で約5秒、導波管とマイクロ波共振空胴の整合状
態は定常時で、マイクロ波の電力反射係数が0.1
以下となつた。このようにコーナ部を用いて、コ
ーナ部から給電口までが短いものでも、さらには
上記が0のものでも、良好な特性が得られる。
すなわち、給電口の位置で基本モードのTE10
外のモードが混入していると考えられる、が1/
2管内波長以下の場合でも、良好な特性が得られ
ることがわかつた。
As an example, the waveguide 3 has a rectangular cross-sectional shape of 95 mm x 54 mm, which is the same as that proposed in Japanese Patent Application No. 59-39980, and the microwave resonant cavity 5 is a cylindrical cavity with a diameter of 80 mm and a height of 90 mm. Lamp 9 is a sphere with a diameter of 30 mm, filled with 60 torr of Ar and 100 mg of Hg.
As the corner of the waveguide, θ in Fig. 2 is 45°,
As a result of using a microwave with a frequency of 8 mm and a power of 800 W, it took about 5 seconds to reach a steady state after exciting with a microwave with a frequency of 2450 MHz and a power of 800 W. The matching state between the waveguide and the microwave resonant cavity was steady, and the microwave power Reflection coefficient is 0.1
It was as follows. By using the corner portions in this manner, good characteristics can be obtained even if the distance from the corner portions to the power feeding port is short, or even if the above distance is zero.
In other words, it is thought that a mode other than the basic mode TE 10 is mixed in at the power supply port position.
It was found that good characteristics can be obtained even when the wavelength is less than 2 tube wavelengths.

以上の構成のマイクロ波放電光源装置をフイル
ムの転写装置の光源として用いた場合、動作は次
のようになる。第3図がフイルム転写装置の概略
構成図であり、枠14の中にマイクロ波放電光源
装置17あるいは18を設置する。点線で示すマ
イクロ波放電光源装置17は先に提案された第5
図のそれを上下逆にしたものであり、実線で示す
マイクロ波放電光源装置18はこの発明による第
1図のそれである。枠14の上面には被転写フイ
ルム15と転写フイルム16を重ねて置き、光源
装置からの光により転写フイルム16が感光され
被転写フイルム15が転写フイルム16に転写さ
れる。被転写フイルム15は編集のために数枚重
ねたものを用いることもある。このような場合、
被転写フイルムに厚みがあるため、光線がフイル
ム面に対して垂直でなければ転写フイルム16へ
転写される像がボケたものになつてしまう。した
がつて、光線はできるだけフイルム面に対して垂
直、すなわち平行光に近いものが要求される。先
に提案されたマイクロ波放電光源装置17を用い
た場合は、光源の位置が高いため、光線は点線の
矢印線で示されるように広がり、平行光からはか
なりずれた光線となる。一方、この発明によるマ
イクロ波放電光源装置18を用いた場合は、光源
の位置を低くできるため、被照射面に照射される
光線は実線の矢印線で示されるように、より平行
光に近い光線となる。したがつて転写される像の
ボケも少なく質のよい転写が可能となる。
When the microwave discharge light source device having the above configuration is used as a light source of a film transfer device, the operation is as follows. FIG. 3 is a schematic diagram of the film transfer device, in which a microwave discharge light source device 17 or 18 is installed in a frame 14. The microwave discharge light source device 17 shown by the dotted line is the fifth one proposed earlier.
The microwave discharge light source device 18 shown by the solid line is the one shown in FIG. 1 according to the present invention, which is turned upside down. A transfer film 15 and a transfer film 16 are placed on top of each other on the upper surface of the frame 14, and the transfer film 16 is exposed to light from a light source device, so that the transfer film 15 is transferred onto the transfer film 16. The transferred film 15 may be a stack of several sheets for editing. In such a case,
Since the transferred film is thick, unless the light beam is perpendicular to the film surface, the image transferred to the transfer film 16 will be blurred. Therefore, the light beam is required to be as perpendicular to the film surface as possible, that is, to be close to parallel light. When the previously proposed microwave discharge light source device 17 is used, since the light source is located high, the light beam spreads as shown by the dotted arrow line, resulting in a light beam that is considerably deviated from parallel light. On the other hand, when the microwave discharge light source device 18 according to the present invention is used, the position of the light source can be lowered, so that the light rays irradiated onto the irradiated surface become more parallel light, as shown by the solid arrow line. becomes. Therefore, the transferred image is less blurred and high-quality transfer is possible.

第4図はこの発明の他の実施例によるマイクロ
波放電光源装置を示す要部断面図である。図にお
いて、マイクロ波共振空胴5は光反射板を兼ねる
回転対称形の空胴壁61と光透過性部材7とから
構成され、球形のランプ9は2本の支持棒91に
より両側から支えられている。この装置の場合、
マイクロ波共振空胴5内に励振される電磁界モー
ドは第1図のものとは異なるが、やはり導波管の
TE10モードにより励振されるモードを用い、導
波管にコーナ部31があつても励振可能である。
よつて、コーナ部を用いることで、光源の光の照
射方向に対する奥行きを浅くでき、第1図のもの
と同様の効果がある。
FIG. 4 is a sectional view of a main part of a microwave discharge light source device according to another embodiment of the present invention. In the figure, the microwave resonant cavity 5 is composed of a rotationally symmetrical cavity wall 61 that also serves as a light reflection plate and a light transmitting member 7, and a spherical lamp 9 is supported from both sides by two support rods 91. ing. For this device,
The electromagnetic field mode excited in the microwave resonant cavity 5 is different from that in Fig. 1, but it is still caused by the waveguide.
Using a mode excited by the TE 10 mode, it is possible to excite even if the waveguide has a corner portion 31.
Therefore, by using the corner portion, the depth of the light source with respect to the light irradiation direction can be made shallow, and the same effect as that shown in FIG. 1 can be obtained.

なお、上記二実施例ではコーナ部としてEコー
ナを用いたものを示したが、Hコーナを用いても
よく、上記実施例と同様の効果を奏する。
In the above two embodiments, an E corner is used as the corner portion, but an H corner may be used, and the same effect as in the above embodiment can be obtained.

また上記各実施例ではマイクロ波発振器が装着
された側の導波管軸の向きと給電口の面とが平行
となるものを示したが、両者が平行ではなく斜め
となるような構成のものでもよく、奥行きを浅く
させる効果がある。またこの場合、モードも所定
のものを得ることが可能である。
Furthermore, in each of the above embodiments, the direction of the waveguide axis on the side where the microwave oscillator is installed is parallel to the surface of the feed port, but there is a configuration in which the two are not parallel but diagonal. However, it often has the effect of making the depth shallower. In this case, it is also possible to obtain a predetermined mode.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明したように、給電口を光の
放射方向と反対側に設け、かつマイクロ波発振器
が装着された側の導波管軸の向きと、給電口の面
が直交せず、マイクロ波発振器とマイクロ波共振
空胴を導波管に対し同じ側に設けたので、装置の
奥行きが浅くでき、限られた空間で光源と被照射
面との距離を離すことができ、被照射面でより平
行光線に近いものが得られる効果がある。さら
に、装置自体も、筺体への取り付けが容易で、か
つスペース効率が良いコンパクトなものとなる効
果がある。また、ランプの冷却も均一にでき、こ
れにより多くのマイクロ波電力が投入できて、よ
り強い光が得られる効果がある。
As explained above, this invention provides a power feed port on the side opposite to the light emission direction, and the direction of the waveguide axis on the side where the microwave oscillator is attached is not perpendicular to the surface of the power feed port. Since the wave oscillator and the microwave resonant cavity are installed on the same side of the waveguide, the depth of the device can be made shallow, and the distance between the light source and the irradiated surface can be increased in a limited space. This has the effect of obtaining parallel light rays. Furthermore, the device itself has the effect of being compact, easy to attach to the housing, and space-efficient. In addition, the lamp can be cooled uniformly, which allows more microwave power to be input, which has the effect of producing stronger light.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の一実施例によるマイクロ波
放電光源装置を示す要部断面図、第2図はこの発
明の一実施例に係る導波管からマイクロ波共振空
胴へのマイクロ波の励振を示す部分断面図、第3
図はこの発明の一実施例によるマイクロ波放電光
源装置を使用したフイルム転写装置を示す概略構
成図、第4図はこの発明の他の実施例によるマイ
クロ波放電光源装置を示す要部断面図、第5図は
先に提案されたマイクロ波放電光源装置を示す要
部断面図である。 1……マグネトロン、3……導波管、5……マ
イクロ波共振空胴、7……光透過性部材、8……
給電口、9……ランプ、31……コーナ部。な
お、図中、同一符号は同一又は相当部分を示す。
FIG. 1 is a sectional view of a main part showing a microwave discharge light source device according to an embodiment of the present invention, and FIG. 2 is a diagram showing microwave excitation from a waveguide to a microwave resonant cavity according to an embodiment of the present invention. Partial sectional view showing 3rd
The figure is a schematic configuration diagram showing a film transfer device using a microwave discharge light source device according to an embodiment of the present invention, and FIG. 4 is a sectional view of essential parts showing a microwave discharge light source device according to another embodiment of the present invention. FIG. 5 is a sectional view of a main part of the previously proposed microwave discharge light source device. 1... Magnetron, 3... Waveguide, 5... Microwave resonant cavity, 7... Light transmitting member, 8...
Power supply port, 9... lamp, 31... corner section. In addition, in the figures, the same reference numerals indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】 1 端部にマイクロ波発振器が装着された導波
管、この導波管の他端部から給電口を通してマイ
クロ波が給電され、少なくとも壁面の一部に光透
過性部材を有するマイクロ波共振空胴、及びこの
マイクロ波共振空胴内に配設されたランプを備え
たものにおいて、上記給電口は光を放射する側と
反対側に設けられ、かつ上記マイクロ波発振器が
装着された側の導波管軸の向きと、上記給電口の
面が直交せず、上記マイクロ波発振器と上記マイ
クロ波共振空胴が上記導波管に対し同じ側に設け
られたことを特徴とするマイクロ波放電光源装
置。 2 導波管にコーナ部を設けたことを特徴とする
特許請求の範囲第1項記載のマイクロ波放電光源
装置。 3 導波管のコーナ部はEコーナであることを特
徴とする特許請求の範囲第2項記載のマイクロ波
放電光源装置。 4 導波管のコーナ部はHコーナであることを特
徴とする特許請求の範囲第2項記載のマイクロ波
放電光源装置。 5 コーナ部から給電口までの導波管長さは1/2
管内波長以下であることを特徴とする特許請求の
範囲第3項記載のマイクロ波放電光源装置。
[Claims] 1. A waveguide having a microwave oscillator attached to its end, microwaves being supplied from the other end of the waveguide through a power supply port, and having a light-transmitting member on at least a part of the wall surface. and a lamp disposed within the microwave resonant cavity, the power supply port is provided on the side opposite to the light emitting side, and the microwave oscillator is attached. The direction of the waveguide axis on the side where the waveguide is connected is not perpendicular to the plane of the feed port, and the microwave oscillator and the microwave resonance cavity are provided on the same side with respect to the waveguide. Microwave discharge light source device. 2. The microwave discharge light source device according to claim 1, wherein the waveguide is provided with a corner portion. 3. The microwave discharge light source device according to claim 2, wherein the corner portion of the waveguide is an E corner. 4. The microwave discharge light source device according to claim 2, wherein the corner portion of the waveguide is an H corner. 5 The waveguide length from the corner to the feed port is 1/2
4. The microwave discharge light source device according to claim 3, wherein the wavelength is equal to or less than the tube wavelength.
JP59219926A 1984-03-02 1984-10-19 Microwave electric-discharge light source Granted JPS6199264A (en)

Priority Applications (9)

Application Number Priority Date Filing Date Title
JP59219926A JPS6199264A (en) 1984-10-19 1984-10-19 Microwave electric-discharge light source
AU39176/85A AU574435B2 (en) 1984-03-02 1985-02-26 Microwave discharge light source apparatus
US06/705,529 US4673846A (en) 1984-03-02 1985-02-26 Microwave discharge light source apparatus
KR1019850001274A KR900000359B1 (en) 1984-03-02 1985-02-28 Microwave discharge light source apparatus
DE8585102201T DE3582810D1 (en) 1984-03-02 1985-02-28 MICROWAVE DISCHARGE LIGHT SOURCE.
EP85102201A EP0153745B1 (en) 1984-03-02 1985-02-28 Microwave discharge light source apparatus
CA000475611A CA1273050A (en) 1984-03-02 1985-03-01 Microwave discharge light source apparatus
SG810/91A SG81091G (en) 1984-03-02 1991-10-05 Microwave discharge light source apparatus
HK815/91A HK81591A (en) 1984-03-02 1991-10-17 Microwave discharge light source apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59219926A JPS6199264A (en) 1984-10-19 1984-10-19 Microwave electric-discharge light source

Publications (2)

Publication Number Publication Date
JPS6199264A JPS6199264A (en) 1986-05-17
JPH0527946B2 true JPH0527946B2 (en) 1993-04-22

Family

ID=16743181

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59219926A Granted JPS6199264A (en) 1984-03-02 1984-10-19 Microwave electric-discharge light source

Country Status (1)

Country Link
JP (1) JPS6199264A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
ES2195651T3 (en) * 1998-11-28 2003-12-01 Quay Technologies Ltd MICROWAVE ULTRAVIOLET LIGHT SOURCE.

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58100353A (en) * 1981-12-09 1983-06-15 Mitsubishi Electric Corp Micro-wave electric-discharge light source device

Also Published As

Publication number Publication date
JPS6199264A (en) 1986-05-17

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