TW201515057A - Excimer lamp and method for producing same - Google Patents

Excimer lamp and method for producing same Download PDF

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Publication number
TW201515057A
TW201515057A TW103130344A TW103130344A TW201515057A TW 201515057 A TW201515057 A TW 201515057A TW 103130344 A TW103130344 A TW 103130344A TW 103130344 A TW103130344 A TW 103130344A TW 201515057 A TW201515057 A TW 201515057A
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tube
discharge
electrode
inner tube
space
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TW103130344A
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Chinese (zh)
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TWI622082B (en
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Hideki Yajima
Go Kobayashi
Izumi Serizawa
Tomohiko Honda
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Orc Mfg Co Ltd
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J9/00Apparatus or processes specially adapted for the manufacture, installation, removal, maintenance of electric discharge tubes, discharge lamps, or parts thereof; Recovery of material from discharge tubes or lamps
    • H01J9/24Manufacture or joining of vessels, leading-in conductors or bases
    • H01J9/245Manufacture or joining of vessels, leading-in conductors or bases specially adapted for gas discharge tubes or lamps
    • H01J9/247Manufacture or joining of vessels, leading-in conductors or bases specially adapted for gas discharge tubes or lamps specially adapted for gas-discharge lamps
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/30Vessels; Containers
    • H01J61/32Special longitudinal shape, e.g. for advertising purposes
    • 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
    • H01J65/046Lamps 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 using capacitive means around the vessel

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Electromagnetism (AREA)
  • Plasma & Fusion (AREA)
  • Manufacturing & Machinery (AREA)
  • Vessels And Coating Films For Discharge Lamps (AREA)

Abstract

Provided is an excimer lamp that prevents damage to an inner tube caused by the difference in thermal expansion coefficient between an inner electrode and the inner tube. The excimer lamp is equipped with: a luminescent tube which has a bottomed cylindrical inner tube, and an outer tube forming a sealed discharge space together with the inner tube, and comprises a dielectric with a discharge gas enclosed in the discharge space; an outer electrode which is disposed on the outer peripheral surface side of the outer tube of the luminescent tube; and an inner electrode which is inserted into the inner tube. With the excimer lamp, stress exerted on the inner tube by the inner electrode when the inner electrode thermally expands due to dielectric barrier discharge between the inner peripheral surface of the inner tube and the outer peripheral surface of the inner electrode is suppressed, and a buffer space having a cross-sectional area which ensures dielectric barrier discharge in the discharge space is formed taking into consideration the size of the discharge space and the size of the discharge voltage.

Description

準分子燈及其製造方法 Excimer lamp and manufacturing method thereof

本發明係有關於一種利用介電質屏障放電或容量結合型高頻放電來放電發光的準分子燈及其製造方法。 The present invention relates to an excimer lamp that uses a dielectric barrier discharge or a capacity-coupled high-frequency discharge to discharge light and a method of manufacturing the same.

準分子燈為,由石英、陶瓷等的讓準分子光穿透的介電質形成具有密閉放電空間的發光管,並將氙(xenon)等的稀有氣體、或將稀有氣體和鹵素氣體混合而成的混合氣體封入該放電空間內作為放電氣體。將數kV之高電壓施加於配置在放電空間內外的內部電極和外部電極之間時,在放電空間中產生介電質屏障放電或容量結合型高頻放電(以下稱之為介電質屏障放電),使得準分子光被放射到發光管外部(例如參照專利文獻1)。 The excimer lamp is a light-emitting tube having a sealed discharge space formed of a dielectric material such as quartz or ceramic that allows excimer light to pass through, and a rare gas such as xenon or a rare gas or a halogen gas is mixed. The resulting mixed gas is sealed in the discharge space as a discharge gas. When a high voltage of several kV is applied between the internal electrode and the external electrode disposed inside and outside the discharge space, a dielectric barrier discharge or a capacity-coupled high-frequency discharge is generated in the discharge space (hereinafter referred to as a dielectric barrier discharge) The excimer light is emitted to the outside of the arc tube (for example, refer to Patent Document 1).

大型準分子燈,在其發光管或電極的形狀或構造上有相當大的自由度。另一方面,本案申請人所開發的小型準分子燈,其發光管之徑為8~20(mm)之譜,由有底筒狀的內管、及與該內管之間形成密閉放電空間的外管而構成發光管,並將放電氣體封入放電空間內。再藉由將高電壓(以下稱之為施加電壓)施加於配置在發光管外管的外周面側的外側電極和插入配置於內管內的內側電極之間,藉此在放電空間中產生介電質屏障放電。此種構造的準分子燈,其發光管由外管和有底筒狀 的內管所構成,因此具有發光管製造容易的優點,且由於內側電極為插入內管內的棒狀(柱狀),因此具有電極製作及電極和燈的固定均容易的優點。 Large excimer lamps have considerable degrees of freedom in the shape or configuration of their tubes or electrodes. On the other hand, the small excimer lamp developed by the applicant of the present invention has a diameter of 8 to 20 (mm), and a sealed discharge space is formed between the inner tube having a bottomed cylindrical shape and the inner tube. The outer tube constitutes an arc tube, and the discharge gas is sealed in the discharge space. Further, a high voltage (hereinafter referred to as an applied voltage) is applied between the outer electrode disposed on the outer peripheral surface side of the outer tube of the arc tube and the inner electrode disposed in the inner tube, thereby generating a dielectric in the discharge space. The electrical barrier discharges. An excimer lamp of such a configuration, the light-emitting tube of which is composed of an outer tube and a bottomed tube Since the inner tube is formed, it has an advantage that the arc tube is easy to manufacture, and since the inner electrode is rod-shaped (columnar) inserted into the inner tube, there is an advantage that the electrode fabrication and the fixing of the electrode and the lamp are easy.

[先行技術文獻] [Advanced technical literature]

專利文獻1:日本特開平6-275242號公報 Patent Document 1: Japanese Patent Laid-Open No. Hei 6-275242

專利文獻2:日本特開2013-69533號公報 Patent Document 2: Japanese Laid-Open Patent Publication No. 2013-69533

但是,在準分子燈中,將施加電壓施加於電極間,在放電空間中產生介電質屏障放電(準分子燈亮燈)時,電極被加熱(或者過熱)。尤其是,在如上述般內側電極為棒狀(例如圓柱狀)的情況下,由於被加熱的內側電極之熱膨脹而對內管施加徑方向的應力,有可能會因為此應力的影響而使內管發生畸變進而造成內管破損的情況。關於本申請人的申請之專利文獻2,係教示確保在該內側電極和內管之間有空間,以使得在內側電極和內管之間產生電暈放電,但完全沒有意識到兩者之接觸所造成的問題點。 However, in an excimer lamp, an applied voltage is applied between the electrodes, and when a dielectric barrier discharge is generated in the discharge space (the excimer lamp is lit), the electrode is heated (or overheated). In particular, when the inner electrode is in the form of a rod (for example, a columnar shape) as described above, a radial stress is applied to the inner tube due to thermal expansion of the heated inner electrode, which may be caused by the influence of the stress. The tube is distorted and the inner tube is damaged. With regard to Patent Document 2 of the applicant's application, it is taught to ensure a space between the inner electrode and the inner tube so that a corona discharge is generated between the inner electrode and the inner tube, but the contact between the two is not recognized at all. The problem caused.

本發明係基於上述的準分子燈(尤其是小型的準分子燈)的問題意識,其目的在於提供小型準分子燈及其製造方法,其不會因為內側電極和內管的熱膨脹係數的差而造成內管破損,且能夠有效率地放射紫外線。 The present invention is based on the above-described problem of the excimer lamp (especially a small excimer lamp), and aims to provide a small excimer lamp and a method of manufacturing the same, which is not caused by the difference in thermal expansion coefficients of the inner electrode and the inner tube. The inner tube is broken and the ultraviolet rays can be efficiently emitted.

本發明的準分子燈之特徵在於包括:發光管,其具備有底筒狀的內管、及在與該內管之間形成密閉的放電空間 之外管,其由將放電氣體封入上述放電空間內的介電質構成;外側電極,其配置於該發光管的外管的外周面側;以及內側電極,其插入配置於該內管內;藉由將放電電壓施加於該外側電極和內側電極之間,以使得在該放電空間中產生介電質屏障放電或容量結合型高頻放電的準分子燈,其中,在該內管的內周面和內側電極的外周面之間,當該介電質屏障放電或容量結合型高頻放電造成該內側電極熱膨脹時,抑制該內側電極對內管施以應力,並參酌該放電空間的大小及該放電電壓的大小,形成確保在該放電空間中的介電質屏障放電或容量結合型高頻放電的剖面積之緩衝空間。 The excimer lamp of the present invention is characterized by comprising: an arc tube having a bottomed cylindrical inner tube and a sealed discharge space formed between the inner tube and the inner tube The outer tube is composed of a dielectric material that encloses the discharge gas in the discharge space; the outer electrode is disposed on the outer peripheral surface side of the outer tube of the arc tube; and the inner electrode is inserted into the inner tube; Applying a discharge voltage between the outer electrode and the inner electrode to cause a dielectric barrier discharge or a capacity-coupled high-frequency discharge excimer lamp in the discharge space, wherein the inner circumference of the inner tube Between the outer peripheral surface of the surface and the inner electrode, when the dielectric barrier discharge or the capacity-coupled high-frequency discharge causes the inner electrode to thermally expand, the inner electrode is restrained from stressing the inner tube, and the size of the discharge space is considered and The magnitude of the discharge voltage forms a buffer space that ensures a cross-sectional area of dielectric barrier discharge or capacity-coupled high-frequency discharge in the discharge space.

在本發明的準分子燈之較佳實施形態中,由固持部封住該內管之底部的相反側的端部和插入於該內管的該內側電極之間的縫隙,並在該內管的底部內面和該內側電極的先端部之間,形成與該緩衝空間連通的軸端空間。 In a preferred embodiment of the excimer lamp of the present invention, the end portion on the opposite side of the bottom portion of the inner tube and the gap interposed between the inner electrode of the inner tube are sealed by the holding portion, and the inner tube is A shaft end space communicating with the buffer space is formed between the bottom inner surface and the front end portion of the inner electrode.

該緩衝空間之與發光管軸線垂直方向的剖面積為下記公式的範圍:0.05×G≦H≦0.1932×V×J;上述H表示緩衝空間的剖面積(mm2),G表示內側電極的剖面積(mm2),V表示施加電壓(kV),J表示放電空間的剖面積(mm2)。 The cross-sectional area of the buffer space perpendicular to the axis of the arc tube is the range of the following formula: 0.05 × G ≦ H ≦ 0.1932 × V × J; the above H represents the sectional area (mm 2 ) of the buffer space, and G represents the section of the inner electrode Area (mm 2 ), V represents an applied voltage (kV), and J represents a sectional area (mm 2 ) of the discharge space.

可以使該內管的底部和外管互相接觸。 The bottom and outer tubes of the inner tube can be brought into contact with each other.

具體言之,本發明的準分子燈,適用於該外管的外徑為8~20mm,且該外側電極和內側電極間的施加電壓為2~8kV的準分子燈。 Specifically, the excimer lamp of the present invention is suitable for an excimer lamp having an outer diameter of 8 to 20 mm and an applied voltage between the outer electrode and the inner electrode of 2 to 8 kV.

本發明之準分子燈的製造方法的態樣之特徵在於包括:準備至少有一端部是開放的介電質構成的筒狀的外管素 材的步驟;準備介電質構成的有底筒狀的內管素材的步驟;以該內管素材之底部為前方,將該內管素材從該外管素材的該一端開放部插入的步驟;在該外管素材和內管素材之間形成放電空間,將放電氣體封入該放電空間內,並將該放電空間密閉的步驟;以及將具有與該內管素材的內周面之間形成緩衝空間之外徑的內側電極插入配置於該內管素材內,並將外側電極配置於該外管素材的外周面的步驟。 The aspect of the method for producing an excimer lamp of the present invention is characterized by comprising: preparing a tubular outer tube composed of a dielectric having at least one end open a step of preparing a bottomed cylindrical inner tube material composed of a dielectric material; and a step of inserting the inner tube material from the one end opening portion of the outer tube material with the bottom of the inner tube material as a front side; Forming a discharge space between the outer tube material and the inner tube material, sealing a discharge gas into the discharge space, and sealing the discharge space; and forming a buffer space between the inner peripheral surface and the inner tube material The inner electrode of the outer diameter is inserted into the inner tube material, and the outer electrode is placed on the outer peripheral surface of the outer tube material.

製造方法的較佳態樣中,更包括:將該內管素材的底部相反側的端部和內側電極之間的縫隙封住的步驟。 In a preferred aspect of the manufacturing method, the method further includes the step of sealing the gap between the end portion on the opposite side of the bottom of the inner tube material and the inner electrode.

依據本發明,在小型準分子燈中,不會因為內側電極的熱膨脹而使發光管破損,而且能夠保證在放電空間中之介電質屏障放電的產生,並能夠有效率地放射紫外線。 According to the present invention, in the small excimer lamp, the arc tube is not damaged by the thermal expansion of the inner electrode, and the generation of the dielectric barrier discharge in the discharge space can be ensured, and the ultraviolet ray can be efficiently emitted.

10‧‧‧小型準分子燈 10‧‧‧Small excimer lamp

20‧‧‧發光管 20‧‧‧Light tube

30‧‧‧外側電極 30‧‧‧Outer electrode

31‧‧‧內側電極 31‧‧‧Inside electrode

32‧‧‧內側電極外周面 32‧‧‧The inner surface of the inner electrode

40‧‧‧外管 40‧‧‧External management

40X‧‧‧外管素材 40X‧‧‧External material

42‧‧‧外管底部 42‧‧‧Bottom of the outer tube

43‧‧‧排氣管 43‧‧‧Exhaust pipe

44‧‧‧外管端部 44‧‧‧End of the outer tube

50‧‧‧內管 50‧‧‧Inside

50X‧‧‧內管素材 50X‧‧‧Inner material

51‧‧‧內管內周面 51‧‧‧ inner tube inner circumference

52‧‧‧內管底部 52‧‧‧ bottom of the inner tube

53‧‧‧內管內周面和內側電極外周面的接觸部分 53‧‧‧Contact portion of the inner circumferential surface of the inner tube and the outer peripheral surface of the inner electrode

60‧‧‧放電空間 60‧‧‧discharge space

70‧‧‧緩衝空間 70‧‧‧ buffer space

71‧‧‧軸端空間(緩衝空間) 71‧‧‧Axis end space (buffer space)

80‧‧‧固持部 80‧‧‧ Holding Department

81‧‧‧交流電源部 81‧‧‧AC power supply department

第1圖顯示本發明準分子燈的第1實施形態,為通過準分子燈之軸線的剖面圖。 Fig. 1 is a cross-sectional view showing the first embodiment of the excimer lamp of the present invention, which is an axis passing through an excimer lamp.

第2圖為沿著第1圖的II-II線的剖面圖。 Fig. 2 is a cross-sectional view taken along line II-II of Fig. 1.

第3圖為第1圖的III部放大剖面圖。 Fig. 3 is an enlarged sectional view showing a portion III of Fig. 1.

第4圖顯示本發明之準分子燈的第2實施形態,為對應於第1圖的剖面圖。 Fig. 4 is a cross-sectional view corresponding to Fig. 1 showing a second embodiment of the excimer lamp of the present invention.

第5圖為沿著第4圖的V-V線的剖面圖。 Fig. 5 is a cross-sectional view taken along line V-V of Fig. 4.

第6圖(A)至(D)為顯示本發明的準分子燈之製造方法的一實施形態的剖面圖。 Fig. 6 (A) to (D) are cross-sectional views showing an embodiment of a method for producing an excimer lamp of the present invention.

第7圖為顯示本發明之準分子燈的緩衝空間之剖面積、放電空間的剖面積、施加電壓及紫外線放射量之關係的實驗結果的圖。 Fig. 7 is a graph showing experimental results showing the relationship between the sectional area of the buffer space of the excimer lamp of the present invention, the sectional area of the discharge space, the applied voltage, and the amount of ultraviolet radiation.

以下,參照圖式說明本發明的實施形態。專利文獻2中記載的準分子燈為臭氧生成用的燈,其係為將大氣導入內側電極的周圍,並在該內側電極和發光管之間產生電暈放電,但本實施形態為抑制紫外線放射用的燈之破損的裝置,其不產生臭氧,而僅有効活用介電質屏障放電之紫外線。 Hereinafter, embodiments of the present invention will be described with reference to the drawings. The excimer lamp described in Patent Document 2 is a lamp for generating ozone, which introduces the atmosphere around the inner electrode and generates a corona discharge between the inner electrode and the arc tube. However, in this embodiment, ultraviolet radiation is suppressed. The damaged device of the lamp does not generate ozone, but only effectively uses ultraviolet rays discharged by the dielectric barrier.

第1圖至第3圖顯示本發明之小型準分子燈10的第1實施形態。 Fig. 1 to Fig. 3 show a first embodiment of the small excimer lamp 10 of the present invention.

小型準分子燈10為一放電燈,其包括:石英玻璃、陶瓷等的透光性之介電質構成的發光管20、外側電極30、及柱狀的內側電極31,其係設置於進行紫外線照射等的裝置。本實施形態的發光管20(外管40)之直徑為8~20(mm)。 The small excimer lamp 10 is a discharge lamp including an arc tube 20 made of a translucent dielectric such as quartz glass or ceramics, an outer electrode 30, and a columnar inner electrode 31 which is provided for ultraviolet rays. A device such as irradiation. The diameter of the arc tube 20 (outer tube 40) of the present embodiment is 8 to 20 (mm).

發光管20,在外管40、以及配置於外管40內的內管50之間有密閉空間(以下稱之為放電空間)60。在此實施形態中,外管40及內管50均為有底筒狀管形狀(剖面略U字形狀),其一端(第1圖的右端)具有封閉的底部42及底部52,該底部42和底部52彼此接觸。外管40的另一端部41和內管50的外周部連結為一體(被熔融接著為一體),在外管40和外管50之間構成剖面為甜甜圈狀(doughnut-shaped)的放電空間60。Xe等的稀有氣體、或稀有氣體和鹵素氣體的混合氣體被封入此放電空間60中以作為放電氣體。另外,內管50的底部52和外管40的底部42 也可以彼此不接觸。 In the arc tube 20, a sealed space (hereinafter referred to as a discharge space) 60 is provided between the outer tube 40 and the inner tube 50 disposed in the outer tube 40. In this embodiment, the outer tube 40 and the inner tube 50 are both in the shape of a bottomed cylindrical tube (slightly U-shaped in cross section), and one end (the right end of the first drawing) has a closed bottom portion 42 and a bottom portion 52. The bottom 52 is in contact with each other. The other end portion 41 of the outer tube 40 and the outer peripheral portion of the inner tube 50 are integrally coupled (melted and integrated), and a doughnut-shaped discharge space is formed between the outer tube 40 and the outer tube 50. 60. A rare gas such as Xe or a mixed gas of a rare gas and a halogen gas is sealed in the discharge space 60 as a discharge gas. In addition, the bottom 52 of the inner tube 50 and the bottom 42 of the outer tube 40 They can also be out of contact with each other.

在圖示例中,外管40及內管50係如第2圖所示般為剖面同心圓形狀,但也可以為楕圓形狀等非圓形剖面,只要是能夠在兩者之間形成密閉的放電空間60的形狀即可。 In the illustrated example, the outer tube 40 and the inner tube 50 have a concentric shape as shown in Fig. 2, but may have a non-circular cross section such as a circular shape, as long as it can form a seal between the two. The shape of the discharge space 60 is sufficient.

外側電極30係沿著外管40的外周面配置,其為例如帶狀、膜狀、或線狀等,以使得將從放電空間放出的準分子光向外部透出或反射。此外側電極30可以和外管40的外周面密接,也可以隔著既定的距離。另外,外側電極30設置於外管40的外周面之至少一部份即可。 The outer electrode 30 is disposed along the outer peripheral surface of the outer tube 40, and is, for example, a strip shape, a film shape, or a line shape, so that excimer light emitted from the discharge space is transmitted or reflected to the outside. Further, the side electrode 30 may be in close contact with the outer peripheral surface of the outer tube 40 or may be separated by a predetermined distance. Further, the outer electrode 30 may be provided on at least a portion of the outer peripheral surface of the outer tube 40.

內側電極31為例如直徑在0.7~4.0(mm)的範圍之圓柱狀。 The inner electrode 31 is, for example, a columnar shape having a diameter in the range of 0.7 to 4.0 (mm).

另一方面,如第3圖所示,內側電極31於內管50內以同軸狀的方式配置在內管50的底部52之內側。在圖示實施形態中,在內管50中形成直徑向先端方向逐漸縮小的錐面50T,圓柱狀之內側電極31的先端外周緣31R抵接於此錐面50T,藉此使得內側電極31同軸狀地配置於內管50內。內管50之底部52相反側的端部和內側電極31,藉由插入兩者之間的環狀空間之固持部80而被固持為一體,在內側電極31的外周面32和內管50的內周面51之間形成和內管50同心狀的緩衝空間70。另外,在內側電極31的先端部和內管50的底部52之間,形成和此緩衝空間70連通的軸端空間71。固持部80可以由接著劑或收縮管構成。另外,也可以不藉由內側電極31的先端外周緣31R和錐面50T的抵接關係,而藉由固持部80使內側電極31和內管50配置為同軸。 On the other hand, as shown in FIG. 3, the inner electrode 31 is disposed inside the inner tube 50 coaxially inside the bottom portion 52 of the inner tube 50. In the illustrated embodiment, a tapered surface 50T whose diameter gradually decreases toward the distal end is formed in the inner tube 50, and the distal end outer circumference 31R of the cylindrical inner electrode 31 abuts against the tapered surface 50T, whereby the inner electrode 31 is coaxial It is disposed in the inner tube 50 in a shape. The end portion on the opposite side of the bottom portion 52 of the inner tube 50 and the inner electrode 31 are integrally held by the retaining portion 80 of the annular space interposed therebetween, on the outer peripheral surface 32 of the inner electrode 31 and the inner tube 50. A buffer space 70 concentric with the inner tube 50 is formed between the inner peripheral faces 51. Further, between the tip end portion of the inner electrode 31 and the bottom portion 52 of the inner tube 50, a shaft end space 71 communicating with the buffer space 70 is formed. The holding portion 80 may be composed of an adhesive or a shrink tube. In addition, the inner electrode 31 and the inner tube 50 may be disposed coaxially by the holding portion 80 without the contact relationship between the distal end outer edge 31R of the inner electrode 31 and the tapered surface 50T.

外側電極30和內側電極31與交流電源部81連接。 透過交流電源部81將數kV的高頻高電壓作為施加電壓以施加於外側電極30和內側電極31之間時,在作為介電質的外管40和內管50之間產生介電質屏障放電。由於稀有氣體或稀有氣體和鹵素的混合氣體已封入放電空間60中作為放電氣體,因此藉由介電質屏障放電而在放電空間60內產生紫外光,亦即對應於稀有氣體及鹵素之波長的光。其結果為,從發光管放射出紫外光。另外,本實施形態並不需要有臭氧的產生、以及伴隨而來的臭氧的放出。因此,可以藉由例如固持部80將緩衝空間70密閉以防止在緩衝空間70中產生的臭氧放出。另外,也可以將例如惰性氣體等封入以使得密閉的緩衝空間70內沒有氧氣,來防止臭氧的發生。 The outer electrode 30 and the inner electrode 31 are connected to the alternating current power supply unit 81. When a high-frequency high voltage of several kV is applied as an applied voltage through the AC power supply unit 81 to be applied between the outer electrode 30 and the inner electrode 31, a dielectric barrier is generated between the outer tube 40 as the dielectric and the inner tube 50. Discharge. Since a rare gas or a mixed gas of a rare gas and a halogen is sealed in the discharge space 60 as a discharge gas, ultraviolet light is generated in the discharge space 60 by dielectric barrier discharge, that is, corresponding to the wavelengths of the rare gas and the halogen. Light. As a result, ultraviolet light is emitted from the arc tube. Further, in the present embodiment, the generation of ozone and the accompanying release of ozone are not required. Therefore, the buffer space 70 can be sealed by, for example, the holding portion 80 to prevent the ozone generated in the buffer space 70 from being released. Further, for example, an inert gas or the like may be enclosed so that oxygen is not contained in the sealed buffer space 70 to prevent the occurrence of ozone.

緩衝空間70的尺寸(剖面積)係依後述方式決定。 The size (sectional area) of the buffer space 70 is determined in the manner described below.

首先,當此緩衝空間70的尺寸為0(亦即內側電極31和內管50的內周面51密接)時,則內管50(亦即發光管20)有破損之虞。準分子燈亮燈時,內側電極31的溫度有時會上升到數百度,當內側電極31的外徑和內管50的內徑幾乎相同,且內側電極31的外周面32和內管50的內周面51密接時,由於內側電極31的熱膨脹而對內管50施以徑方向的應力。此應力集中於例如內管50的底部52,其結果可能為造成準分子燈破損的要因之一。例如,當內側電極31由柱狀的金屬構成,而發光管20由石英玻璃構成時,兩者的線膨脹係數係以內側電極31較大。 First, when the size of the buffer space 70 is 0 (that is, the inner electrode 31 and the inner peripheral surface 51 of the inner tube 50 are in close contact with each other), the inner tube 50 (i.e., the arc tube 20) is damaged. When the excimer lamp is turned on, the temperature of the inner electrode 31 sometimes rises to several hundred degrees, and the outer diameter of the inner electrode 31 and the inner diameter of the inner tube 50 are almost the same, and the outer peripheral surface 32 of the inner electrode 31 and the inner tube 50 are When the inner peripheral surface 51 is in close contact, the inner tube 50 is subjected to a radial stress due to thermal expansion of the inner electrode 31. This stress concentrates, for example, on the bottom 52 of the inner tube 50, which may be one of the causes of damage to the excimer lamp. For example, when the inner electrode 31 is made of a columnar metal and the arc tube 20 is made of quartz glass, the linear expansion coefficient of both is larger by the inner electrode 31.

在本實施形態中,係將緩衝空間70的最小剖面積(緩衝空間剖面積下限值Hmin)設定為,使得在內管50上不會產生像上述那樣的由內側電極31的熱膨脹而造成的應力集中。本 案發明者依經驗得知,在施加電壓為2~8(kV)的範圍內,可以由燈徑方向剖面中緩衝空間70的剖面積H、及內側電極31的剖面積G的關係,決定不會產生內管50破損的緩衝空間的剖面積之下限。具體言之,可以得知:當施加電壓為2~8(kV)時,可以用以下的公式(1)求出緩衝空間剖面積下限值(Hmin)。 In the present embodiment, the minimum cross-sectional area (buffer space sectional area lower limit value Hmin) of the buffer space 70 is set such that the thermal expansion of the inner electrode 31 as described above does not occur in the inner tube 50. Stress concentration. this The inventors have learned from experience that the relationship between the sectional area H of the buffer space 70 and the sectional area G of the inner electrode 31 in the cross section of the lamp diameter direction can be determined in the range of the applied voltage of 2 to 8 (kV). The lower limit of the sectional area of the buffer space in which the inner tube 50 is broken is generated. Specifically, it can be known that when the applied voltage is 2 to 8 (kV), the buffer space sectional area lower limit value (Hmin) can be obtained by the following formula (1).

(1)Hmin=0.05×G (1)Hmin=0.05×G

其中,Hmin表示緩衝空間剖面積下限值(mm2),G表示內側電極的剖面積(mm2)。 Here, Hmin represents the lower limit value (mm 2 ) of the sectional area of the buffer space, and G represents the sectional area (mm 2 ) of the inner electrode.

另一方面,緩衝空間70的最大剖面積(緩衝空間剖面積上限值Hmax)為,按照內側電極31的剖面積、放電空間60的剖面積、及施加於外側電極30和內側電極31之間的施加電壓,確保在放電空間60中的介電質屏障放電之發生的剖面積。換言之,此最大剖面積是抑制緩衝空間70之存在所造成的在放電空間60中的介電質屏障放電之減少(所伴隨的紫外線放射量的減少)的剖面積。準分子燈,依據其發光原理,若內側電極31的外周面32未接觸內管50的內周面51,則其徑方向静電容量變小、電場也變弱。當電場變弱時介電質屏障放電就會減少,且紫外線的放射量也減少。另外,當施以施加電壓時,有時在內側電極31和內管50之間會產生明顯的不平等電場,在緩衝空間70中產生流光電暈放電。當流光電暈放電發生時,會妨礙放電空間60中的介電質屏障放電,使得紫外線的放射量減少。 On the other hand, the maximum cross-sectional area (buffer space sectional area upper limit value Hmax) of the buffer space 70 is between the outer electrode 30 and the inner electrode 31 in accordance with the sectional area of the inner electrode 31, the sectional area of the discharge space 60, and The applied voltage ensures the cross-sectional area of the dielectric barrier discharge in the discharge space 60. In other words, this maximum sectional area is a sectional area of the dielectric barrier discharge in the discharge space 60 (the accompanying decrease in the amount of ultraviolet radiation) caused by the presence of the suppression buffer space 70. In the excimer lamp, if the outer peripheral surface 32 of the inner electrode 31 does not contact the inner peripheral surface 51 of the inner tube 50, the electrostatic capacitance in the radial direction becomes small and the electric field also becomes weak. When the electric field becomes weak, the dielectric barrier discharge is reduced, and the amount of ultraviolet radiation is also reduced. Further, when an applied voltage is applied, a significant unequal electric field is sometimes generated between the inner electrode 31 and the inner tube 50, and a flow photo-wave discharge is generated in the buffer space 70. When the flow photo-foam discharge occurs, the dielectric barrier discharge in the discharge space 60 is hindered, so that the amount of ultraviolet radiation is reduced.

本案發明者由經驗得知:紫外線之放射量的減少量係隨著發生介電質屏障放電的放電空間的大小、妨礙介電質屏障放電要因之緩衝空間的大小、及施加電壓的大小而改變; 以及,當施加電壓V為2~8(kV)時,刻意不讓放電空間60中的介電質屏障放電減少的緩衝空間70之剖面積的最大值(緩衝空間剖面積上限值Hmax)係依以下的公式(2)求出。 The inventors of the present invention have learned from experience that the amount of reduction in the amount of ultraviolet radiation varies depending on the size of the discharge space in which the dielectric barrier discharge occurs, the size of the buffer space that hinders the discharge of the dielectric barrier, and the magnitude of the applied voltage. ; And, when the applied voltage V is 2 to 8 (kV), the maximum value of the sectional area of the buffer space 70 (the buffer space sectional upper limit Hmax) which deliberately prevents the dielectric barrier discharge in the discharge space 60 from being reduced is It is obtained by the following formula (2).

(2)Hmax=0.1932×V×J (2) Hmax = 0.1932 × V × J

其中,Hmax表示緩衝空間剖面積上限值(mm2),J表示放電空間的剖面積(mm2),V表示施加電壓(kV)。 Here, Hmax represents the upper limit value (mm 2 ) of the sectional area of the buffer space, J represents the sectional area (mm 2 ) of the discharge space, and V represents the applied voltage (kV).

此外,在第1圖至第3圖的實施形態中,在內側電極31的先端部和內管50的底部52之間形成端部空間71。若像這樣形成端部空間71,則能夠抑制內管底部52所承受的內側電極31之熱膨脹造成的軸方向的應力。另外,藉由將容易集中燈徑方向之應力的內管底部52設置端部空間71,而能夠使其對於燈徑方向的應力有耐受性,再加上緩衝空間70,就能夠更進一步防止內管的破損。而且,也可以為省略端部空間71(使內側電極31和內管底部52密接)的態様、或者相反地,使內側電極31的先端部和內管50的底部52完全分離的態様。 Further, in the embodiment of Figs. 1 to 3, an end space 71 is formed between the tip end portion of the inner electrode 31 and the bottom portion 52 of the inner tube 50. When the end space 71 is formed in this manner, it is possible to suppress the axial stress caused by the thermal expansion of the inner electrode 31 received by the inner tube bottom portion 52. Further, by providing the end space 71 with the inner tube bottom portion 52 which tends to concentrate the stress in the direction of the lamp diameter, it is possible to withstand the stress in the lamp diameter direction, and furthermore, the buffer space 70 can be further prevented. Damage to the inner tube. Further, in a state in which the end space 71 is omitted (the inner electrode 31 and the inner tube bottom 52 are in close contact with each other), or vice versa, the front end portion of the inner electrode 31 and the bottom portion 52 of the inner tube 50 may be completely separated.

第4圖及第5圖顯示本發明的小型準分子燈10的第2實施形態。 Fig. 4 and Fig. 5 show a second embodiment of the compact excimer lamp 10 of the present invention.

在此實施形態中,內管50的軸線和柱狀之內側電極31的軸線不一致,內側電極31配置為偏向內管50之內徑內的一方。亦即,內側電極31的外周面32和內管50的內周面51的一部53接觸,內管50的內周面51和內側電極31的外周面32之間之緩衝空間70並非與內管50(內側電極31)同軸。另外,內側電極31的先端部和內管50的底部52未接觸。 In this embodiment, the axis of the inner tube 50 does not coincide with the axis of the columnar inner electrode 31, and the inner electrode 31 is disposed to be biased toward the inner diameter of the inner tube 50. That is, the outer peripheral surface 32 of the inner electrode 31 is in contact with a portion 53 of the inner peripheral surface 51 of the inner tube 50, and the buffer space 70 between the inner peripheral surface 51 of the inner tube 50 and the outer peripheral surface 32 of the inner electrode 31 is not in contact with The tube 50 (inner electrode 31) is coaxial. Further, the tip end portion of the inner electrode 31 and the bottom portion 52 of the inner tube 50 are not in contact.

使該第2實施形態的小型準分子燈10亮燈時,與內 側電極31接觸的內表面53受到內側電極31之熱膨脹的應力之影響,但內側電極31由於熱膨脹而向具有緩衝空間70的方向移動。具有緩衝性(彈性)的固持部80使該內側電極31的移動成為可能。因此,即使內側電極31和內表面53接觸,只要有既定剖面積的緩衝空間就沒問題。另外,在第4圖及第5圖的實施形態中,內側電極31的軸線和內管50的軸線平行,不過也可以不平行,只要在兩者之間形成緩衝空間70即可。 When the small excimer lamp 10 of the second embodiment is turned on, The inner surface 53 where the side electrode 31 is in contact is affected by the thermal expansion stress of the inner electrode 31, but the inner electrode 31 moves in the direction of the buffer space 70 due to thermal expansion. The cushioning (elasticity) holding portion 80 makes it possible to move the inner electrode 31. Therefore, even if the inner electrode 31 and the inner surface 53 are in contact, there is no problem as long as there is a buffer space having a predetermined sectional area. Further, in the embodiments of FIGS. 4 and 5, the axis of the inner electrode 31 and the axis of the inner tube 50 are parallel, but they may not be parallel, and a buffer space 70 may be formed therebetween.

如上述,即使內側電極31的軸線和內管50的軸線不一致,也不會對放電發光造成實質的不良影響。亦即,當內側電極31的軸線和內管50的軸線不一致時,內側電極31和外側電極30的距離在燈周方向上是不均一的,徑方向静電容量也沿著周方向有不均一的情況。在静電容量相對較大的部分,通常電場也相對較強,因而產生介電質屏障放電。因此,静電容量相對較小的另一電極部分所蓄積的電荷,朝向產生該介電質屏障放電的電極間部分移動。其結果為,在放電空間60內的特定空間領域中產生介電質屏障放電。紫外線放射係以該放電發生位置為中心發光,藉由施加電壓之施加而在整個電極間蓄積的電荷直接有效利用於介電質屏障放電,因此能夠得到具有光強度的紫外光。此種準分子燈,在供給電力小的情況下,藉由界定其放射方向而能夠以足夠強度發光。 As described above, even if the axis of the inner electrode 31 does not coincide with the axis of the inner tube 50, there is no substantial adverse effect on the discharge luminescence. That is, when the axis of the inner electrode 31 and the axis of the inner tube 50 do not coincide, the distance between the inner electrode 31 and the outer electrode 30 is not uniform in the lamp circumferential direction, and the radial capacitance is also uneven along the circumferential direction. Case. In a portion where the electrostatic capacity is relatively large, the electric field is usually relatively strong, thereby generating a dielectric barrier discharge. Therefore, the electric charge accumulated in the other electrode portion having a relatively small electrostatic capacitance moves toward the inter-electrode portion where the dielectric barrier discharge is generated. As a result, a dielectric barrier discharge is generated in a specific spatial domain within the discharge space 60. The ultraviolet radiation emits light around the discharge generation position, and the electric charge accumulated between the entire electrodes by the application of the applied voltage is directly and effectively utilized for the dielectric barrier discharge, so that ultraviolet light having a light intensity can be obtained. Such an excimer lamp can emit light with sufficient intensity by defining its radiation direction when the supplied electric power is small.

第6圖顯示本發明的準分子燈之製造方法的一實施形態。 Fig. 6 is a view showing an embodiment of a method for producing an excimer lamp of the present invention.

如第6圖(A)所示,由介電質構成的內管素材50X,係為先端底部52封閉的有底筒狀材,同樣由介電質構成的外管 素材40X則為一端開放部44為開放、另一端部具有小徑的排氣部43的筒狀材。上述的內管素材50X,係以其先端底部52為前方,從一端開放部44插入外管素材40X內,並使其底部52位於排氣部43的附近。 As shown in Fig. 6(A), the inner tube material 50X made of a dielectric material is a bottomed cylindrical material closed by the tip end bottom 52, and an outer tube which is also composed of a dielectric material. The material 40X is a cylindrical material in which the one end opening portion 44 is open and the other end portion has a small diameter exhaust portion 43. The inner tube material 50X is inserted into the outer tube material 40X from the one end opening portion 44 with the tip end bottom portion 52 as the front side, and the bottom portion 52 is located in the vicinity of the exhaust portion 43.

在此狀態下,將外管素材40X的一端開放部44加熱熔融,以使其和內管素材50X的外周熔接,構成和外管40的一端連接部41(同圖(B))。然後,從排氣部43將作為放電空間60的空間之空氣(氣體)排氣,並將放電氣體封入該放電空間60內之後(將放電空間60內的空氣置換為放電氣體後),使該排氣部43軟化熔融(熔接)以形成底部52。該底部52與內管素材50X(內管50)的底部42接觸(同圖(C))。 In this state, the one end opening portion 44 of the outer tube material 40X is heated and melted so as to be welded to the outer circumference of the inner tube material 50X, and is configured to be connected to the one end connecting portion 41 of the outer tube 40 (Fig. (B)). Then, the air (gas) which is the space of the discharge space 60 is exhausted from the exhaust portion 43, and the discharge gas is sealed in the discharge space 60 (after replacing the air in the discharge space 60 with the discharge gas), The exhaust portion 43 is softened and melted (fused) to form the bottom portion 52. The bottom portion 52 is in contact with the bottom portion 42 of the inner tube material 50X (the inner tube 50) (Fig. (C)).

繼之,將棒狀內側電極31插入內管素材50X內,並使其先端部與底部42接觸,用密封材(固持材)80固持底部42之相反側的端部之內管素材50X和內側電極31之間的環狀縫隙。另外,也可以將緩衝空間70密封(同圖(D))。內側電極31的外徑為,在其與內管素材50X的內周面51之間形成上述大小(剖面積)的緩衝空間70之外徑。另外,在外管40的外側配置外側電極30(同圖(D))。 Then, the rod-shaped inner electrode 31 is inserted into the inner tube material 50X, and the tip end portion thereof is brought into contact with the bottom portion 42, and the inner tube material 50X and the inner side of the end portion on the opposite side of the bottom portion 42 are held by the sealing member (holding material) 80. An annular gap between the electrodes 31. Alternatively, the buffer space 70 may be sealed (the same figure (D)). The outer diameter of the inner electrode 31 is an outer diameter of the buffer space 70 having the above-described size (sectional area) formed between the inner tube surface 51 and the inner circumferential surface 51 of the inner tube material 50X. Further, the outer electrode 30 is disposed outside the outer tube 40 (the same figure (D)).

外管素材40X的排氣部43也可以形成為孔,而不形成為同軸筒狀。 The exhaust portion 43 of the outer tube material 40X may be formed as a hole instead of being formed in a coaxial cylindrical shape.

在本準分子燈10中能夠藉由選擇封入放電空間60的氣體,而改變發光波長。例如可以封入氬和氟的混合氣體,以使其放射波長193nm的光。另外,為了外管素材40X及內管素材50X之玻璃的脆化保護、以及防止玻璃和封入氣體的反 應,可以在外管及內管形成氧化鋁膜、二氧化鈦膜、氧化鎂膜等的保護膜。封入氣體中含有鹵素時,可以形成氟化鎂膜。 In the present excimer lamp 10, the emission wavelength can be changed by selecting the gas enclosed in the discharge space 60. For example, a mixed gas of argon and fluorine may be enclosed to emit light having a wavelength of 193 nm. In addition, the embrittlement protection of the glass of the outer tube material 40X and the inner tube material 50X, and the prevention of the glass and the enclosed gas are reversed. A protective film such as an aluminum oxide film, a titanium oxide film, or a magnesium oxide film can be formed on the outer tube and the inner tube. When the enclosed gas contains a halogen, a magnesium fluoride film can be formed.

【實施例】 [Examples]

下文中使用實施例說明滿足上述(1)式的放電準分子燈10。 The discharge excimer lamp 10 satisfying the above formula (1) will be described below using an embodiment.

進行實驗,將準分子燈10之軸直交剖面中的緩衝空間70的剖面積相對於內側電極31的剖面積變動,再藉由亮燈以測定內管50有無破損。說明實驗的具體例。 In the experiment, the cross-sectional area of the buffer space 70 in the axial cross section of the excimer lamp 10 was changed with respect to the sectional area of the inner electrode 31, and the inner tube 50 was measured for damage by lighting. A specific example of the experiment will be described.

使內側電極31的剖面積為3.14(mm2)(半徑1mm、一定),並以具有緩衝空間70的剖面積在0.04~0.21(mm2)變動的發光管20的準分子燈為樣本群1~6,施加電壓為2~8(kV)以使其亮燈,並觀察內管50有無破損。後述表1為其結果。 The cross-sectional area of the inner electrode 31 is 3.14 (mm 2 ) (radius 1 mm, constant), and the excimer lamp of the arc tube 20 having the cross-sectional area of the buffer space 70 varying from 0.04 to 0.21 (mm 2 ) is taken as the sample group 1 ~6, apply a voltage of 2~8 (kV) to make it light, and observe whether the inner tube 50 is damaged. Table 1 below is the result.

依據表1,緩衝空間70的剖面積(mm2)為內側電極31的剖面積(mm2)之約4%的樣本1,發現內管50有破損,相對於此,同剖面積比超過5%的樣本2至6的內管50則沒有破損。亦 即,可以得知:內管50不發生破損的緩衝空間70之剖面積(mm2)和內側電極31的剖面積(mm2)之相關性,係為緩衝空間70的剖面積(mm2)為內側電極31的剖面積(mm2)之5%以上。另外,內側電極70的剖面積為0.38~12.5(mm2)之間的情況下,緩衝空間70的剖面積(mm2)和內側電極31的剖面積(mm2)的相關性亦導出相同的結果。 Table 1 based on the cross-sectional area (mm 2) of the buffer space 70 is a cross-sectional area of the inner electrode 31 (mm 2) of samples 1 to about 4%, we found damaged tube 50, whereas the same cross-sectional area ratio exceeds 5 The inner tube 50 of % of samples 2 to 6 was not damaged. That is, it can be known that the correlation between the sectional area (mm 2 ) of the buffer space 70 in which the inner tube 50 is not damaged and the sectional area (mm 2 ) of the inner electrode 31 is the sectional area of the buffer space 70 (mm 2 ). The cross-sectional area (mm 2 ) of the inner electrode 31 is 5% or more. Further, when the cross-sectional area of the inner electrode 70 is between 0.38 and 12.5 (mm 2 ), the correlation between the cross-sectional area (mm 2 ) of the buffer space 70 and the cross-sectional area (mm 2 ) of the inner electrode 31 is also derived. result.

繼之,使用實施例說明滿足上述(2)式的放電準分子燈。 Next, a discharge excimer lamp satisfying the above formula (2) will be described using an embodiment.

當放電空間60變大時,確保在放電空間60中紫外線之放射的緩衝空間70的剖面積H的大小也相對地變大。另外,因為施加電壓變高時紫外線放射量也變大,所以能推知緩衝空間70的剖面積H也相對地變大。在此,執行分別改變施加電壓V(kV)、緩衝空間70的剖面積H(mm2)、及放電空間60的剖面積J(mm2)的情況下之紫外線放射量的減少量測定實驗。 When the discharge space 60 becomes large, the size of the cross-sectional area H of the buffer space 70 that ensures the emission of ultraviolet rays in the discharge space 60 is also relatively large. In addition, since the amount of ultraviolet radiation is also increased when the applied voltage is increased, it can be inferred that the cross-sectional area H of the buffer space 70 is relatively large. Here, an experiment for measuring the amount of decrease in the amount of ultraviolet radiation in the case where the applied voltage V (kV), the sectional area H (mm 2 ) of the buffer space 70, and the sectional area J (mm 2 ) of the discharge space 60 are respectively changed is performed.

製作準分子燈以作為實驗樣本(實驗準分子燈),其係使內側電極31的剖面積G為一定、並分別改變緩衝空間70的剖面積H(mm2)、施加電壓V(kV)、及放電空間60的剖面積J(mm2),再測定各準分子燈的紫外線放射量。另外,製作比較準分子燈以作為上述各實驗準分子燈的紫外線放射量之比較対象,其係使施加電壓V及放電空間60的剖面積J和各實驗準分子燈相同,僅使緩衝空間70的剖面積H為緩衝空間剖面積下限值,並測定紫外線放射量,分別將各實驗準分子燈的紫外線放射量和比較用準分子燈的紫外線放射量進行比較。內側電極31的剖面積G為12.57(mm2)時的實驗結果作為具體例顯示於第7 圖中。 An excimer lamp was prepared as an experimental sample (experimental excimer lamp), which made the cross-sectional area G of the inner electrode 31 constant, and changed the sectional area H (mm 2 ) of the buffer space 70, the applied voltage V (kV), And the sectional area J (mm 2 ) of the discharge space 60, and the amount of ultraviolet radiation of each excimer lamp was measured. Further, a comparison of the excimer lamp was made as a comparison of the ultraviolet radiation amount of each of the above experimental excimer lamps, and the sectional area J of the applied voltage V and the discharge space 60 was the same as that of each of the experimental excimer lamps, and only the buffer space 70 was made. The sectional area H is the lower limit of the sectional area of the buffer space, and the amount of ultraviolet radiation is measured, and the ultraviolet radiation amount of each experimental excimer lamp and the ultraviolet radiation amount of the comparative excimer lamp are respectively compared. The experimental results when the cross-sectional area G of the inner electrode 31 is 12.57 (mm2) are shown in Fig. 7 as a specific example.

由第7圖可知,可依式(2)求出能夠抑制紫外線放射量之減少的緩衝空間60的剖面積H之最大值(緩衝空間剖面積上限值;Hmax)。而且,當內側電極31的剖面積G為0.3~13(mm2)、施加電壓V為2~8(kV)、放電空間60的剖面積J為8.5~300.5(mm2)的範圍中時,緩衝空間剖面積上限值Hmax和內側電極31的剖面積G、施加電壓V、及放電空間60的剖面積J的相關性也是導出幾乎相同的結果。 As can be seen from Fig. 7, the maximum value (the buffer space sectional area upper limit value; Hmax) of the sectional area H of the buffer space 60 capable of suppressing the decrease in the amount of ultraviolet radiation can be obtained by the equation (2). Further, when the cross-sectional area G of the inner electrode 31 is 0.3 to 13 (mm 2 ), the applied voltage V is 2 to 8 (kV), and the sectional area J of the discharge space 60 is in the range of 8.5 to 300.5 (mm 2 ), The correlation between the buffer space sectional upper limit value Hmax, the sectional area G of the inner electrode 31, the applied voltage V, and the sectional area J of the discharge space 60 is also derived almost identically.

10‧‧‧小型準分子燈 10‧‧‧Small excimer lamp

20‧‧‧發光管 20‧‧‧Light tube

30‧‧‧外側電極 30‧‧‧Outer electrode

31‧‧‧內側電極 31‧‧‧Inside electrode

32‧‧‧內側電極外周面 32‧‧‧The inner surface of the inner electrode

40‧‧‧外管 40‧‧‧External management

42‧‧‧外管底部 42‧‧‧Bottom of the outer tube

43‧‧‧排氣管 43‧‧‧Exhaust pipe

44‧‧‧外管端部 44‧‧‧End of the outer tube

50‧‧‧內管 50‧‧‧Inside

51‧‧‧內管內周面 51‧‧‧ inner tube inner circumference

52‧‧‧內管底部 52‧‧‧ bottom of the inner tube

60‧‧‧放電空間 60‧‧‧discharge space

70‧‧‧緩衝空間 70‧‧‧ buffer space

71‧‧‧軸端空間(緩衝空間) 71‧‧‧Axis end space (buffer space)

80‧‧‧固持部 80‧‧‧ Holding Department

81‧‧‧交流電源部 81‧‧‧AC power supply department

Claims (7)

一種準分子燈,其包括:一發光管,其具備有底筒狀的內管、及在與該內管之間形成密閉的放電空間之外管,其由將放電氣體封入上述放電空間內的介電質構成;一外側電極,其配置於該發光管的外管的外周面側;以及一內側電極,其插入配置於該內管內;將放電電壓施加於該外側電極和內側電極之間,藉此以使得在該放電空間中產生介電質屏障放電或容量結合型高頻放電的準分子燈,其中,在該內管的內周面和內側電極的外周面之間,當該介電質屏障放電或容量結合型高頻放電造成該內側電極熱膨脹時,抑制該內側電極對內管施以應力,並參酌該放電空間的大小及該放電電壓的大小,形成確保在該放電空間中的介電質屏障放電或容量結合型高頻放電的剖面積之緩衝空間。 An excimer lamp comprising: an arc tube having a bottomed cylindrical inner tube; and a tube forming a sealed discharge space between the inner tube and the inner tube, the discharge gas being enclosed in the discharge space a dielectric material; an outer electrode disposed on an outer peripheral surface side of the outer tube of the arc tube; and an inner electrode interposed in the inner tube; and applying a discharge voltage between the outer electrode and the inner electrode Thereby, an excimer lamp for causing a dielectric barrier discharge or a capacity-coupled high-frequency discharge in the discharge space, wherein between the inner peripheral surface of the inner tube and the outer peripheral surface of the inner electrode, When the electric barrier discharge or the capacity-coupled high-frequency discharge causes the inner electrode to thermally expand, the inner electrode is restrained from applying stress to the inner tube, and the size of the discharge space and the magnitude of the discharge voltage are determined to be ensured in the discharge space. The buffer space of the cross-sectional area of the dielectric barrier discharge or the capacity combined high-frequency discharge. 如申請專利範圍第1項所述之準分子燈,其中,由固持部封住該內管之底部的相反側的端部和插入於該內管的該內側電極之間的縫隙,在該內管的底部內面和該內側電極的先端部之間,形成與該緩衝空間連通的軸端空間。 The excimer lamp of claim 1, wherein the end portion of the opposite side of the bottom portion of the inner tube and the gap between the inner electrode of the inner tube are sealed by the holding portion, A shaft end space communicating with the buffer space is formed between the inner surface of the bottom of the tube and the tip end portion of the inner electrode. 如申請專利範圍第1或2項所述之準分子燈,其中:該緩衝空間之與發光管軸線垂直方向的剖面積為下記公式的範圍: 0.05×G≦H≦0.1932×V×J;上述H表示緩衝空間的剖面積(mm2),G表示內側電極的剖面積(mm2),V表示施加電壓(kV),J表示放電空間的剖面積(mm2)。 The excimer lamp according to claim 1 or 2, wherein: the cross-sectional area of the buffer space perpendicular to the axis of the arc tube is a range of the following formula: 0.05 × G ≦ H ≦ 0.1932 × V × J; H represents a sectional area (mm 2 ) of the buffer space, G represents a sectional area (mm 2 ) of the inner electrode, V represents an applied voltage (kV), and J represents a sectional area (mm 2 ) of the discharge space. 如申請專利範圍第1~3項中任一項所述之準分子燈,其中該內管的底部和外管互相接觸。 The excimer lamp of any one of claims 1 to 3, wherein the bottom of the inner tube and the outer tube are in contact with each other. 如申請專利範圍第1~4項中任一項所述之準分子燈,其中該外管的外徑為8~20mm,該外側電極和內側電極間的施加電壓為2~8kV。 The excimer lamp according to any one of claims 1 to 4, wherein the outer tube has an outer diameter of 8 to 20 mm, and an applied voltage between the outer electrode and the inner electrode is 2 to 8 kV. 一種準分子燈的製造方法,其包括:準備至少有一端部是開放的介電質構成的筒狀的外管素材的步驟;準備介電質構成的有底筒狀的內管素材的步驟;以該內管素材之底部為前方,將該內管素材從該外管素材的該一端開放部插入的步驟;在該外管素材和內管素材之間形成放電空間,將放電氣體封入該放電空間內,並將該放電空間密閉的步驟;以及將具有與該內管素材的內周面之間形成緩衝空間之外徑的內側電極插入配置於該內管素材內,並將外側電極配置於該外管素材的外周面的步驟。 A method for producing an excimer lamp, comprising: preparing a tubular outer tube material having at least one end open dielectric material; and preparing a bottomed cylindrical inner tube material having a dielectric material; a step of inserting the inner tube material from the one end opening portion of the outer tube material with the bottom of the inner tube material as a front portion; forming a discharge space between the outer tube material and the inner tube material to seal the discharge gas into the discharge a step of sealing the discharge space in the space; and inserting an inner electrode having an outer diameter forming a buffer space with an inner circumferential surface of the inner tube material in the inner tube material, and disposing the outer electrode in the space The step of the outer peripheral surface of the outer tube material. 如申請專利範圍第6項所述之準分子燈的製造方法,更包括:將該內管素材的底部相反側的端部和內側電極之間的縫隙封住的步驟。 The method for producing an excimer lamp according to claim 6, further comprising the step of sealing a gap between the end portion on the opposite side of the inner tube material and the inner electrode.
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