TW201123261A - Ultraviolet lamp and ultraviolet irradiating device - Google Patents

Ultraviolet lamp and ultraviolet irradiating device Download PDF

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Publication number
TW201123261A
TW201123261A TW099144047A TW99144047A TW201123261A TW 201123261 A TW201123261 A TW 201123261A TW 099144047 A TW099144047 A TW 099144047A TW 99144047 A TW99144047 A TW 99144047A TW 201123261 A TW201123261 A TW 201123261A
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TW
Taiwan
Prior art keywords
electrode
discharge
ultraviolet
discharge tube
lamp
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TW099144047A
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Chinese (zh)
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TWI366858B (en
Inventor
Kazuya Hatase
Yoshinori Kanamori
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Gs Yuasa Int Ltd
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    • 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
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J5/00Details relating to vessels or to leading-in conductors common to two or more basic types of discharge tubes or lamps
    • H01J5/50Means forming part of the tube or lamps for the purpose of providing electrical connection to it
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/04Electrodes; Screens; Shields
    • H01J61/06Main electrodes
    • H01J61/067Main electrodes for low-pressure discharge lamps
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/52Cooling arrangements; Heating arrangements; Means for circulating gas or vapour within the discharge space
    • H01J61/523Heating or cooling particular parts of the lamp
    • H01J61/526Heating or cooling particular parts of the lamp heating or cooling of electrodes
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/70Lamps with low-pressure unconstricted discharge having a cold pressure < 400 Torr
    • H01J61/72Lamps with low-pressure unconstricted discharge having a cold pressure < 400 Torr having a main light-emitting filling of easily vaporisable metal vapour, e.g. mercury
    • 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

Abstract

An ultraviolet lamp includes a tubular discharge tube, characterized in a curved surface part and a planar part for transmitting ultraviolet on the outer wall of the discharge tube in opposite position. In addition, a surface of the curved surface part inside the discharge tube is a concave. A first electrode is installed on the curved surface part. A second electrode which is line-shaped is installed on the outside of the discharge tube in a manner extending along the lengthwise direction of the discharge tube. The second electrode is located near the central of the planar part. A discharge occurs between the first electrode and the second electrode. There is no other electrode installed on the planner part except the second electrode.

Description

20112326L 六、發明說明: 【發明妍屬之技術領域】 本發明是一種紫外線燈以及紫外線照射裝置。 【先前技術】 作為使用於洗淨液晶面板用玻璃基板等的洗淨裝置等 中的紫外線燈,存在二重管構造的準分子燈(參照曰本專 利公開公報的特開2003 —257375公報及特開平9一97597 號公報)。 進而,作為同樣使用於洗淨裝置等中的紫外線燈,存 在使用圓筒形放電容器的紫外線燈(參照日本專利公開公 報的特開2003 — 197152號公報)。 進而’作為同樣使用於洗淨裝置等中的紫外線燈,存 在使用方箱型放電容器的紫外線燈(參照國際專利申請案 的國際公開第W02004/025175號公報)。 然而,日本專利公開公報的特開2003-257375公報及 特開平9 — 97597號公報中所揭示的二重管構造中,所產生 的紫外線自燈全方向地呈放射狀射出。因此,向與藉由紫 外線洗淨的對象物(產品W)相反的方向放射的紫外線無 法用於洗淨。為了解決該問題,例如圖8所示,於燈100 的後方(產品W侧的相反侧)設置有反射板1〇1。如此’ 藉由將向後方射出的光引導向產品W侧,可提高照射效 率。 而且’為了防止紫外線被燈100周圍的氧氣吸收而導 致照射強度下降’必須採用將燈1〇〇與反射板101之間的 201123261 =密封並封人氮氣而具有密封構造的燈箱心於此情 箱脱的產品〜侧設置用於射出紫外線的 、隹而’如此而使用燈箱1Q3時,存在裝置整體大型化, =構=成本亦變高的問題。而且,嵌入反射板ι〇ι及 W 102中的玻璃材料由於紫外線之影響而隨時間產生劣 化,故而另外必需對該些構件加以維護。結果’產生營運 成本增大的問題。 日本專利公開公報的特開細—197152號中所揭示 之示例中,燈本_相面中,於絲射方向相反側的部 分上安裝有光線反射罩(用於反射光線)。藉由設為如此 之結構,而無需上述燈箱。 然而’紫外線被空氣中的氧吸收。因此,為了將強度 較強的紫外線照射至產品w,必須使燈盡可能靠近產品 W。然而’如此之示例中,由於燈形狀為圓筒形故 線自燈放出直至到達產品w為止的距離根據紫外線向哪 -方向放出、及自燈的哪一位置放出而存在較大差異。因 此,無論使燈如何靠近產品w,必然有一部分紫外線是在 空氣中通過較長距離後到達產品W。結果,該紫外線被氧 氣吸收的比例變尚,故而會產生紫外線的照射效率變 問題。 · 國際專利申請案的國際公開第w〇2〇〇4/〇25175號公 報中所揭示之示例中,放電容器為方箱型。於該放電容^ 中,於下表面上設置有可透過紫外線的網狀電極,於上表 201123261 面上設置有反射紫外線的電極。此例中,由於於上表面上 設置有反射紫外線的電極,故而無需如上所述的燈箱。 另外,為了便於說明,W02004/025175號公報中的如 圖4所示的長方體放電容器的六個面中,將設置有紫外線 反射電極(lb)的面設為上表面,而將設置有可透過紫外 線的網狀電極(lc)的面設為下表面。進而,將剩餘4個 面中面積較大的面設為側面’面積較小的面設為前後面。 進而,自放電容器的中心部,將朝向上表面的方向設為上 方向’將朝向下表面的方向設為下方向,將朝向侧面的方 向設為側方向。 譎W02004/025175號公報之示例中,放電容器為方箱 型,故而產品W侧的面(下表面)成為平面。因此,當使 燈的下表面靠近產品W時,無論於下表面的哪一位置上, 下表面均均一地靠近產品W。因此,與使用如上所述之圓 筒形的燈時相比,可提高紫外線的照射效率。 然而,與圓筒形的燈相比,如此之方箱型的燈存在易 於破碎的問題。準分子燈等紫外線燈的放電容器中,一般 在熄燈時是以低於大氣壓的壓力而封入氣體。而且,亦存 在點瘴時放電容器内的氣壓高於大氣壓的紫外線燈。因 此’熄、燈時的放電容器中,受到來自外部的大氣壓的壓力。 進而’對於燈而言’存在點燈時受到内部氣體的膨脹力之 情形。使用如上所述之方箱型放電容器時,必須將設置有 反射紫外線的電極的上表面、及設置有可透過紫外線的網 狀電極的下表面的面積設為較大。因此,於該些面上大氣 201123261 壓的壓力或内部氣體的膨脹力皆大於其他面。結果,由於 其上表面與下表面受到較大的壓力,故而側面部分上施加 有較大的力。結果,放電容器的側面變得易於破碎。 【發明内容】 本發明疋為了解決上述問題點而研製成的,其目的在 於提供一種具有簡易的結構、可獲得充分的照射效率、且 放電容器不易破碎的紫外線燈以及紫外線照射裝置。 鲁纟發明之第-發明是—種紫外線燈,其具備形成為筒 狀的放電管,其特徵在於,於放電管的外周壁上,在相互 對向的位置上具備曲面部以及用於透過紫外線的平坦部, 且曲面部是藉由使放電管的内部側之面呈凹面而形成的 (參照圖2)。於曲面部上設置有第—電極,於放電管的 外部設置有延伸於放電管長度方向的線狀的第二電極,第 二電極設置於平坦部的中心部附近,且在第一電極與第二 電極之間產生主放電,並且於平坦部上未設置有除^二電 極以外的電極(參照圖3)。另外,於本發明中,為;便 # 於說明,將圖2的上方向設為放電管的上方向(亦即,曲 面部所處的方向為上方向),將圖2的下方向設為放電管 的下方向(亦即,用於透過紫外線的平坦部所處的方向為 下方向)。將圖2的左右方向設為放電管的側方向。進而·, 將圖2中垂直於紙面的方向作為放電管的長度方向。 利用圖14中的放電管的剖面,對於「平坦部的中心部 附近」的含義加以說明。將形成於放電管外壁面上的用^ 透過紫外線的平坦部201之放電管内側的面設為底邊。此 201123261 時’將與底邊平行的直線中,收納於放電管内的部分的長 度最長的直線設為直線WL。將該直線WL與放電管内面 的兩個交點設為W1及W2。進而,將該W1與W2的中心 點設為WC。此時,將直線WL上的點中,與WC的距離 為WC與W1的距離之1/4的兩個點設為W3及W4。此時, 「平坦部的中心部附近」相當於平坦部2〇1的放電管外側 的面中通過W3且垂直於直線WL的直線、與通過”4且 垂直於直線WL的直線之間的部分。亦即,上述的「平垣 部的中心部附近」為圖14的平坦部201的外表面中以粗線 表示之部分。 上述的「第一電極設置於平坦部的中心部附近」是指, 第二電極上垂直於放電管長度方向的剖面的中心點設於 「平坦部的中心部附近」。 根據第-發明’放電管的外周壁上設置有用於透過紫 外線的平坦部。使該平坦部靠近產品w時,由於平坦部較 平坦’故而無論平坦部的哪—位置均均—地靠近產品w。 ^此’使时®筒形放電容糾先制巾所產生的「必然 部分紫外線是在空氣中通過較長距離後到達產品W」 到抑制。結果,與使用圓筒形的燈時相比,可提 同兔外線的照射效率。 例相=而3據第,明’與使用方箱型放電容器的先前 ^目比/獲得放電管不易破碎的效果20112326L VI. Description of the Invention: [Technical Field of Invention] The present invention relates to an ultraviolet lamp and an ultraviolet irradiation device. [Prior Art] As an ultraviolet lamp used in a cleaning device or the like for cleaning a glass substrate for a liquid crystal panel or the like, there is an excimer lamp having a double tube structure (refer to Japanese Patent Laid-Open Publication No. 2003-257375 Kaiping No. 9-97597). Further, as an ultraviolet lamp which is used in a cleaning device or the like, there is an ultraviolet lamp using a cylindrical discharge vessel (refer to Japanese Laid-Open Patent Publication No. 2003-197152). Further, as an ultraviolet lamp which is also used in a cleaning device or the like, an ultraviolet lamp using a square box type discharge vessel is known (refer to International Publication No. WO2004/025175 of the International Patent Application). However, in the double pipe structure disclosed in Japanese Laid-Open Patent Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei 9-97597, the ultraviolet rays generated are emitted radially from the lamp in all directions. Therefore, ultraviolet rays radiated in the opposite direction to the object (product W) washed by the ultraviolet rays cannot be used for washing. In order to solve this problem, for example, as shown in FIG. 8, a reflecting plate 1〇1 is provided at the rear of the lamp 100 (opposite side of the product W side). Thus, the irradiation efficiency can be improved by guiding the light emitted rearward toward the product W side. Moreover, 'in order to prevent the ultraviolet rays from being absorbed by the oxygen around the lamp 100, the irradiation intensity is lowered." It is necessary to use a light box with a sealed structure in which 201123261 between the lamp 1〇〇 and the reflector 101 is sealed and sealed with nitrogen. When the light-emitting box 1Q3 is used in the case where the product is removed from the side of the product, the size of the entire device is increased, and the cost is also high. Moreover, the glass materials embedded in the reflecting plates ι ι and W 102 are deteriorated over time due to the influence of ultraviolet rays, and it is necessary to additionally maintain the members. The result 'creates an increase in operating costs. In the example disclosed in Japanese Laid-Open Patent Publication No. Hei No. 197152, a light reflecting cover (for reflecting light) is attached to a portion on the opposite side of the filament direction in the lamp-phase. By setting it as such, the above light box is not required. However, ultraviolet light is absorbed by oxygen in the air. Therefore, in order to irradiate the stronger ultraviolet rays to the product w, it is necessary to make the lamp as close as possible to the product W. However, in such an example, since the shape of the lamp is a cylindrical shape, the distance from the lamp to the product w is largely different depending on which direction the ultraviolet rays are emitted and from which position of the lamp. Therefore, no matter how close the lamp is to the product w, a part of the ultraviolet rays must arrive at the product W after passing a long distance in the air. As a result, the ratio of the ultraviolet ray absorbed by the oxygen gas is increased, so that the ultraviolet ray irradiation efficiency becomes problematic. In the example disclosed in the International Publication No. WO 〇 2〇〇4/〇25175 of the International Patent Application, the discharge vessel is of a square box type. In the discharge capacitor ^, a mesh electrode that transmits ultraviolet rays is provided on the lower surface, and an electrode that reflects ultraviolet rays is provided on the surface of the above table 201123261. In this example, since the electrode for reflecting ultraviolet rays is provided on the upper surface, the light box as described above is not required. Further, for convenience of explanation, in the six faces of the rectangular parallelepiped discharge vessel shown in FIG. 4 in WO2004/025175, the surface on which the ultraviolet reflective electrode (lb) is provided is referred to as an upper surface, and is provided with a permeable surface. The surface of the ultraviolet mesh electrode (lc) is set as the lower surface. Further, the surface having the larger area among the remaining four surfaces is referred to as the side surface. The surface having a small area is referred to as the front and rear surfaces. Further, in the center portion of the discharge vessel, the direction toward the upper surface is referred to as the upper direction, and the direction toward the lower surface is referred to as the lower direction, and the direction toward the side surface is referred to as the lateral direction. In the example of WO02004/025175, since the discharge vessel is of a square box type, the surface (lower surface) on the side of the product W becomes a flat surface. Therefore, when the lower surface of the lamp is brought close to the product W, the lower surface is uniformly adjacent to the product W regardless of the position of the lower surface. Therefore, the irradiation efficiency of ultraviolet rays can be improved as compared with the case of using a cylindrical lamp as described above. However, such a square box type lamp has a problem that it is easy to be broken as compared with a cylindrical lamp. In a discharge vessel of an ultraviolet lamp such as an excimer lamp, a gas is generally sealed at a pressure lower than atmospheric pressure when the lamp is turned off. Moreover, there is also an ultraviolet lamp in which the pressure inside the discharge vessel is higher than atmospheric pressure. Therefore, in the discharge vessel at the time of extinguishing and extinguishing, the pressure from the outside atmospheric pressure is received. Further, 'for the lamp', there is a case where the expansion force of the internal gas is received when lighting. When the square box type discharge vessel as described above is used, it is necessary to make the area of the upper surface of the electrode on which the ultraviolet ray is reflected and the lower surface of the mesh electrode provided with the ultraviolet ray transparent. Therefore, the atmospheric pressure of the 201123261 pressure or the expansion force of the internal gas on these surfaces is greater than that of the other surfaces. As a result, since the upper surface and the lower surface are subjected to a large pressure, a large force is applied to the side portions. As a result, the sides of the discharge vessel become easily broken. SUMMARY OF THE INVENTION The present invention has been made in order to solve the above problems, and an object thereof is to provide an ultraviolet lamp and an ultraviolet irradiation device which have a simple structure, can obtain sufficient irradiation efficiency, and are not easily broken by a discharge vessel. In the invention of the invention, there is provided an ultraviolet lamp comprising a discharge tube formed in a cylindrical shape, wherein the outer peripheral wall of the discharge tube has a curved surface portion at a position facing each other and is used for transmitting ultraviolet rays. The flat portion is formed by making the surface on the inner side of the discharge tube concave (see FIG. 2). a first electrode is disposed on the curved surface portion, and a second electrode extending in a longitudinal direction of the discharge tube is disposed outside the discharge tube, and the second electrode is disposed near a central portion of the flat portion, and is in the first electrode and the first electrode A main discharge is generated between the two electrodes, and electrodes other than the two electrodes are not provided on the flat portion (refer to FIG. 3). In the present invention, the upper direction of FIG. 2 is the upper direction of the discharge tube (that is, the direction in which the curved surface portion is located), and the lower direction of FIG. 2 is set. The downward direction of the discharge tube (that is, the direction in which the flat portion for transmitting ultraviolet rays is in the downward direction). The left-right direction of FIG. 2 is set as the side direction of a discharge tube. Further, the direction perpendicular to the paper surface in Fig. 2 is taken as the longitudinal direction of the discharge tube. The meaning of the "near the center portion of the flat portion" will be described with reference to the cross section of the discharge tube in Fig. 14 . The surface of the discharge tube formed on the outer wall surface of the discharge tube by the ultraviolet ray-transmissive portion 201 is referred to as a bottom side. In the case of 201123261, the straight line having the longest length of the portion accommodated in the discharge tube is a straight line WL. The two intersections of the straight line WL and the inner surface of the discharge tube are set to W1 and W2. Further, the center points of W1 and W2 are set to WC. At this time, two points of the point on the straight line WL, which is a distance from WC of 1/4 of WC and W1, are set to W3 and W4. In this case, "the vicinity of the center portion of the flat portion" corresponds to a portion between the straight surface of the discharge tube on the outer surface of the flat portion 2〇1 passing through W3 and perpendicular to the straight line WL, and the line passing through "4 and perpendicular to the straight line WL. That is, the above-mentioned "near the center portion of the flat portion" is a portion indicated by a thick line in the outer surface of the flat portion 201 of Fig. 14 . The above-mentioned "the first electrode is provided in the vicinity of the center portion of the flat portion" means that the center point of the cross section perpendicular to the longitudinal direction of the discharge tube on the second electrode is provided in the vicinity of the "central portion of the flat portion". According to the first invention, the outer peripheral wall of the discharge tube is provided with a flat portion for transmitting the ultraviolet rays. When the flat portion is brought close to the product w, since the flat portion is flat, the position of the flat portion is always close to the product w. ^ This is the time when the tube-shaped discharge capacitor is used to correct the amount of "the inevitable part of the ultraviolet light is passed through the air in a long distance and reaches the product W" to suppress. As a result, the irradiation efficiency of the rabbit outer line can be improved as compared with when a cylindrical lamp is used. Example phase = and 3 according to the first, the ratio of the previous box to the use of the box-type discharge vessel / the discharge tube is not easy to break the effect

管中’與祕透過紫外線的平㈣對向的相壁,U 201123261 侧的面呈凹面的曲面部。因此,該放電管中即使受到大氣 壓=力或内部氣體的膨脹力,該力皆並非集中於一部位 而疋/刀散的。因此,如WO2004/025175號公報的圖4所示 的長方體放電容器時產生的力集中於側面而導致側面易於 破碎之問題,在本發明中得到抑制。 再者根據第一發明,使用有延伸於放電管長度方向的 線狀電極作為用於主放電的第二電極。結果,可將由第二 春電極所遮擋的紫外線的量抑制為較少。進而,由於平坦部 上未设置除第二電極以外的電極,故可獲得由電極所遮擋 的紫外線量較少的燈。進而,根據上述發明,除沿著形成 為放電管的内部側的面呈凹面的曲面部2〇5而設有第一電 極以外,第二電極設置於平坦部201的中心部附近。藉由 如此之兩個電極的組合,於第一電極的較寬範圍内,與第 二電極的距離均大致均一。結果,於放電管内的較寬範圍 内產生放電,故而可獲得紫外線強度變強的效果。 當然,第一發明的「平坦部」中的「平坦」並非表示 # 完全的平面。顯然,即使平坦部稍有傾斜,但若與對向的 凹面部相比足夠平坦,亦可獲得本發明的效果。 另外’第一發明中的曲面部未必僅由曲面所構成。例 如,如圖9所示,與用於透過紫外線的平坦部2〇1相對向 的曲面部亦可包括:兩個圓弧狀部203 ;以及夹於上述兩 個圓弧狀部之間,且寬度窄於用於透過紫外線的平坦部 201的平坦部202。顯然,如此之情形時亦可獲得第一發明 的效果。如此之情形時,曲面部所包含的平坦部2〇2的寬 201123261 度,較好的是小於等於用於透過紫外線的平坦部2〇1寬度 的2/3,進而好的是小於等於1/2 ,更好的是小於等於1/3二 平坦部202的寬度等於或大於用於透過紫外線的平坦部 2〇1的寬度時,不包含於本發明之第一發明中。如此之情 形時,與使用方箱型放電容H時同樣,由於對向的兩個平 ,部上承受大氣壓的壓力,因此平坦部2q2兩侧的圓弧狀 壯亦承受較強的力。結果,該圓孤狀部易於破碎。因此, 無法獲得本發明之第一發明中放電管不易破碎的效果。 進而,第一發明中的曲面部,如圖1〇所示亦可包括 寬度充分小於用於透過紫外線的平坦部2G1的多個平坦部 2〇4。顯然,如此之情形時,亦可獲得第一發明的效果。 其中,較理想的是,第一發明中的曲面部由不包含平 部的一個凹曲面構成。藉此,可進—步增強放電 度0 進而,進崎的是,第—發明中的曲面部由不包含平 且剖面為’狀的—個凹曲面構成。藉此,可特別 增強放電料綠。 明之第二發明是’如第_發明中的紫外線燈,其 部上設置有紫外線反射構件,紫外線反射構件 部且較自放電管的其中一個側部至另-個 整個範圍更寬,於垂直於放電管長度方向的紫 中,=赫二Γ上在紫外線反射構件中的紫外線反射面 ;八 個側部更下側的部分的點上,垂直於紫外 201123261 線反射㈣娜面且偷放電管 個侧部朝向另一個側部的方向更朝下。較自其中 相的放電管的剖面,對於第二發明中的側部 明。將形成於放電管外壁面上而用於 坦部201之放電管内側的面設為底邊。將 的曲面部205之靖的内側的面 二距,底邊最遠的點設為頂點Τ1通過該頂點τ而與底 ,^的直輕為基準線。㈣鱗線與底相交點設為 底點Β。將通過頂點Τ與底點Β的中心點而與基準線正交 的直線設為中心線。此時,將曲面部2G5之放電管的外側 的面與該中心線的兩個交點設為側部S卜S2。以上說明是 利用如圖11所示之剖面進行的朗,但實際上於放電管 中,存在垂直於圖U的紙面的方向之長度,故該些侧部是 延伸於放電管的長度方向的線。另外,該側部的定義於第 二發明以外的發明中亦與此相同。 第二發明中的「紫外線反射構件形成為沿著曲面部且 籲較自放電管的其中-個側部至另一個側部為止的整個範圍 更寬」是指,紫外線反射構件206至少存在於沿著曲面部 205自其中一個側部S1至另一個側部S2為止的整個範圍 内,進而,於兩個側部的至少一個上,紫外線反射構件2〇6 超過該側部並進而延伸至下方向。 圖12疋放電管為圓筒形的比較例之情形下的放電管 的剖面圖。如圖12所示,關於圓筒形放電管207,為了抑 制來自放電管的側方向的紫外線之放出,而與本發明之第 11 201123261 二發明同樣地,使紫外線反射構件206延伸至較侧部SI 更下側。於此情形時,自較側部S1更下側的紫外線反射 構件的點A、垂直於紫外線反射構件的反射面的切平面且 朝向放電管内部的方向(圖12中,自點A朝向放電管内 部的箭頭方向),變得較自侧部S1朝向侧部S2的方向更 為上方向。亦即,於由較該侧部S1更下側的紫外線反射 構件206所反射的紫外線,向上方向前進的傾向強於向下 方向前進的傾向。因此,在紫外線的一部分中,直至自放 電管朝向產品W放出為止,在放電管内反射的次數變多。 如此,當反射次數變多時,紫外線減弱。結果,產生照射 至產品W的紫外線量變少的問題。 該情況於設有方箱型放電容器之情形時亦相同。於方 箱型放電容器中,為了抑制紫外線向侧方向洩漏 ,而於兩 個侧面上設置紫外線反射構件。於此情形,在相向的兩個 側面之間,一部分紫外線由於反射而多次往復。紫外線在 朝向產品W放出之前會減弱。因此,使用方箱型放電容器 時亦存在放出的紫外線強度變弱的問題點。 於本發明之第二發明中,如圖11所示,在較其中一個 侧部S1更下_部分的點A上,垂直於紫外線反射面的 切平面且朝向放電管内部的方向(圖11 +,是自點A朝 向放電管内部的箭頭額),較自其中—侧部31朝向 另一個側部S2的方向更朝下。亦即,於較該側部S1更下 ^的i外線反射構件2G6上所反射的紫外線,向下方向前 的傾向強於向上方向前進的傾向。因此,紫外線直至自 12 201123261 為止’在放電管内反射的次數變 二右=,次數變少’則可抑制紫外線的減弱。 、‘果’可抑制照射至產品w的紫外線 的「紫外線反射構件形成為沿著曲面部且 側部至另一_部為止的整個範圍 =二,並非疋心紫外線反射構件2〇6必須沿著曲面部2〇5 其中一個側部S1直至另-個側部S2為止的整 個王部I巳圍内。例如,於自其中一個側 的整個範圍中的一部分上存在用以測定紫外線 ^的透Μ,該透光窗的部分上可不設置紫外線反射構 。賴’於如此之情料,若料線反射構件· 作為整體之自其中—個侧部si至另—個側部幻為 止的整個範圍的大致整體上,則亦可獲得第二發明的效果。 於第一發明中,在紫外線反射構件中的紫外線反射面 中’較其中一個側部更下側的部分的所有點上,垂直於紫 外線反射面的切平面且朝向放電管内部的方向,無須均較 自其中-個侧部朝向另一個側部的方向更朝下。顯然,即 使存在一部分不滿足如此之條件的點,但若於較其中一個 側部更下_部分的大部錄上滿足如此之條件/,、 獲得第二發明的效果。 於圖11中’紫外線反射構件206形成於放電管的外表 面彳-本發明之第二發明並不限定於如此之情形,紫外線 反射構件206亦可形成於放電管的内面。 、 13 201123261 本發明之第三發明是,如第一發明中的紫外線燈,於 曲面部上設置有紫外線反射構件,紫外線反射構件形成為 沿著曲面部且較自放電管的其中一個侧部至另一個側部為 止的整個範圍更寬,並且紫外線反射構件是用以產生主放 電的第一電極,該主放電用以產生紫外線。 例如,將鋁等固著於曲面部205的外壁面上而形成第 一電極時,亦可將該第一電極作為紫外線反射構件2〇6而 使用。若第一電極具有作為紫外線反射構件的功能,則除 第·電極以外無須另設紫外線反射構件2〇6。結果,可削 減製造製程及材料費,故而可使燈廉價。 於使用方箱型放電容器的比較例的燈中,為了抑制紫 外線自放電容器的側方向放出,自放電容器的上表面跨越 兩側的側面而設置有具有作為料線反㈣件的功能的第 -電極。如此之情形時’難以將與第一電極形成放電的第 二電極設置為具有實用的形狀、且其與第—電極的距離在 第-電極的任何部分上均均—。結果,第_電極與第二電 極間的距離根據第-電極的部分而不同。因此,第一電極 與第二電極之間’放電集巾於電極間距雜短處。結果, 產生放電強度變弱的問題。 對此,本發明之第三發明中,於曲面部上設置有用以 產生主放ί的第—電極’該主放電用以產生紫外線。因此, 與使用方彳目型放的比較例讀形不同,即使於側方 向上設置有具有作為紫外線反射構件的功能的第一 電極之In the tube, the surface wall opposite to the flat (four) that transmits ultraviolet rays, and the surface on the side of U 201123261 is a concave curved surface portion. Therefore, even if the discharge tube is subjected to atmospheric pressure = force or expansion force of the internal gas, the force is not concentrated on one portion and the knives are scattered. Therefore, the force generated when the rectangular parallelepiped discharge vessel shown in Fig. 4 of WO2004/025175 is concentrated on the side surface causes the side surface to be easily broken, and is suppressed in the present invention. Further, according to the first invention, a linear electrode extending in the longitudinal direction of the discharge tube is used as the second electrode for main discharge. As a result, the amount of ultraviolet rays blocked by the second spring electrode can be suppressed to be small. Further, since the electrode other than the second electrode is not provided on the flat portion, a lamp having a small amount of ultraviolet rays blocked by the electrode can be obtained. Further, according to the invention described above, the second electrode is provided in the vicinity of the central portion of the flat portion 201 except that the first electrode is provided along the curved surface portion 2〇5 which is formed as a concave surface on the inner surface of the discharge tube. With such a combination of the two electrodes, the distance from the second electrode is substantially uniform over a wide range of the first electrode. As a result, a discharge is generated in a wide range in the discharge tube, so that an effect of increasing the ultraviolet ray intensity can be obtained. Of course, "flat" in the "flat portion" of the first invention does not mean a #complete plane. Obviously, even if the flat portion is slightly inclined, the effect of the present invention can be obtained if it is sufficiently flat compared with the opposite concave surface. Further, the curved surface portion in the first invention is not necessarily constituted by only a curved surface. For example, as shown in FIG. 9, the curved surface portion facing the flat portion 2〇1 for transmitting ultraviolet rays may further include: two arc-shaped portions 203; and sandwiched between the two arc-shaped portions, and The width is narrower than the flat portion 202 of the flat portion 201 for transmitting ultraviolet rays. Obviously, the effect of the first invention can also be obtained in such a case. In such a case, the width of the flat portion 2〇2 included in the curved surface portion is 201123261 degrees, preferably 2/3 or less of the width of the flat portion 2〇1 for transmitting ultraviolet rays, and more preferably 1/3 or less. 2. It is more preferable that the width of the flat portion 202 equal to or smaller than 1/3 is equal to or larger than the width of the flat portion 2〇1 for transmitting ultraviolet rays, and is not included in the first invention of the present invention. In such a case, as in the case of using the square box type discharge capacitor H, since the opposing flat portions are subjected to the atmospheric pressure, the arcs on both sides of the flat portion 2q2 are also subjected to a strong force. As a result, the round orphan is easily broken. Therefore, the effect that the discharge tube is not easily broken in the first invention of the present invention cannot be obtained. Further, the curved surface portion in the first invention may include a plurality of flat portions 2〇4 having a width sufficiently smaller than that of the flat portion 2G1 for transmitting ultraviolet rays, as shown in Fig. 1A. Obviously, in such a case, the effect of the first invention can also be obtained. Among them, it is preferable that the curved surface portion in the first invention is constituted by a concave curved surface which does not include a flat portion. Thereby, the degree of discharge 0 can be further enhanced. Further, in the first invention, the curved surface portion is composed of a concave curved surface which does not include a flat cross section. Thereby, the discharge green can be particularly enhanced. The second invention of the invention is the ultraviolet lamp according to the invention, wherein the ultraviolet reflecting member is provided on the portion, and the ultraviolet reflecting member portion is wider than one of the side portions of the discharge tube to the other one, perpendicular to In the purple of the length of the discharge tube, the ultraviolet reflecting surface of the ultraviolet reflecting member on the upper side of the erbium; the point of the lower side of the eight side parts, which is perpendicular to the ultraviolet 201123261 line (four) and the sneak tube The side faces further downward toward the other side. The cross section of the discharge tube from the phase is the side portion of the second invention. The surface formed on the outer wall surface of the discharge tube and used for the inner side of the discharge tube of the stem portion 201 is referred to as a bottom side. The surface on the inner side of the curved surface portion 205 is two points apart, and the point farthest from the bottom side is the vertex Τ1, and the straight line of the bottom and the bottom is the reference line. (4) The intersection point between the scale and the bottom is set to the bottom point. A line orthogonal to the reference line passing through the center point of the vertex 底 and the bottom point 设为 is set as the center line. At this time, the two intersections of the outer surface of the discharge tube of the curved surface portion 2G5 and the center line are referred to as side portions S2. The above description is performed by using the cross section shown in FIG. 11, but actually, in the discharge tube, there is a length perpendicular to the direction of the paper surface of FIG. U, so the side portions are lines extending in the longitudinal direction of the discharge tube. . Further, the definition of the side portion is the same as in the invention other than the second invention. In the second invention, the "ultraviolet-reflecting member is formed to be wider along the curved surface portion and the entire range from the side to the other side of the discharge tube" means that the ultraviolet-ray reflecting member 206 exists at least along the edge. The entire surface of the curved portion 205 from one of the side portions S1 to the other side portion S2, and further, at least one of the two side portions, the ultraviolet reflecting member 2〇6 extends beyond the side portion and further extends to the lower direction . Fig. 12 is a cross-sectional view showing the discharge tube in the case of a comparative example in which the discharge tube is cylindrical. As shown in FIG. 12, in the cylindrical discharge tube 207, in order to suppress the release of ultraviolet rays from the side of the discharge tube, the ultraviolet reflection member 206 is extended to the side portion as in the 11th 201123261 invention of the present invention. SI is lower. In this case, the point A of the ultraviolet ray reflection member from the lower side S1 is perpendicular to the tangential plane of the reflection surface of the ultraviolet ray reflection member and toward the inside of the discharge tube (in FIG. 12, from the point A toward the discharge tube) The direction of the arrow in the interior becomes higher than the direction from the side portion S1 toward the side portion S2. In other words, the ultraviolet ray reflected by the ultraviolet ray reflecting member 206 on the lower side of the side portion S1 tends to advance in the upward direction rather than the downward direction. Therefore, in a part of the ultraviolet ray, the number of times of reflection in the discharge tube increases until the self-discharge tube is discharged toward the product W. Thus, when the number of reflections increases, the ultraviolet rays are weakened. As a result, there is a problem that the amount of ultraviolet rays irradiated to the product W becomes small. This case is also the same in the case of a square box type discharge vessel. In the box type discharge vessel, in order to suppress leakage of ultraviolet rays to the side, ultraviolet reflecting members are provided on both sides. In this case, a part of the ultraviolet rays reciprocate a plurality of times due to reflection between the opposite side faces. Ultraviolet light is attenuated before it is released toward the product W. Therefore, when a square box type discharge vessel is used, there is also a problem that the emitted ultraviolet light intensity is weak. In the second invention of the present invention, as shown in Fig. 11, at a point A which is lower than the portion of the one side portion S1, perpendicular to the tangential plane of the ultraviolet ray reflecting surface and toward the inside of the discharge tube (Fig. 11 + It is the arrow amount from the point A toward the inside of the discharge tube, and is more downward than the direction from the side 31 toward the other side S2. In other words, the ultraviolet rays reflected on the i-outer line reflection member 2G6 which is lower than the side portion S1 tend to be stronger in the upward direction than in the upward direction. Therefore, the ultraviolet rays are reduced until the number of times of reflection in the discharge tube becomes smaller from the time of 12 201123261, and the number of times is decreased. The 'fruit' can suppress the ultraviolet ray that is irradiated to the product w. The ultraviolet ray reflection member is formed along the curved surface portion and the entire range from the side portion to the other portion = two, and the ultraviolet ray reflection member 2 〇 6 must not be along The curved portion 2〇5 has one of the side portions S1 up to the other side portion S2. For example, there is a portion for measuring the ultraviolet rays on a part of the entire range from one side. The portion of the light transmission window may not be provided with an ultraviolet reflection structure. In this case, if the material line reflection member is as a whole, the entire range from the side si to the other side is illusory. In a substantially general aspect, the effect of the second invention can also be obtained. In the first invention, at all points of the portion of the ultraviolet reflecting surface in the ultraviolet reflecting member that is lower than one of the side portions, perpendicular to the ultraviolet reflection The tangential plane of the face and the direction toward the inside of the discharge tube do not need to be more downward than the direction from one side to the other side. Obviously, even if there is a point that does not satisfy such a condition, The condition of the second invention is satisfied in the larger part of the lower portion than the one of the side portions. The effect of the second invention is obtained. In Fig. 11, the 'ultraviolet reflecting member 206 is formed on the outer surface of the discharge tube 彳 - the present invention The second invention is not limited to such a case, and the ultraviolet ray reflecting member 206 may be formed on the inner surface of the discharge tube. 13 201123261 The third invention of the present invention is characterized in that the ultraviolet ray lamp according to the first invention is provided on the curved surface portion. The ultraviolet reflecting member, the ultraviolet reflecting member is formed to be wider along the curved portion and wider than the entire range from one side to the other side of the discharge tube, and the ultraviolet reflecting member is the first electrode for generating the main discharge, The main discharge is used to generate ultraviolet rays. For example, when aluminum or the like is fixed to the outer wall surface of the curved surface portion 205 to form the first electrode, the first electrode may be used as the ultraviolet reflection member 2〇6. When the electrode has a function as an ultraviolet reflecting member, the ultraviolet reflecting member 2〇6 is not required to be provided in addition to the first electrode. As a result, the manufacturing process and material cost can be reduced. Therefore, in the lamp of the comparative example using the square box type discharge vessel, in order to suppress the ultraviolet light from being discharged from the side of the discharge capacitor, the upper surface of the self-discharging capacitor is provided to have a side opposite to the side surfaces of the discharge tube. (d) the function of the first electrode of the member. In such a case, it is difficult to set the second electrode that forms a discharge with the first electrode to have a practical shape, and the distance from the first electrode is on any portion of the first electrode. As a result, the distance between the _ electrode and the second electrode differs depending on the portion of the first electrode. Therefore, the 'discharge hood between the first electrode and the second electrode is short at the electrode pitch. As a result, the discharge intensity is generated. In this regard, in the third invention of the present invention, a first electrode for generating a main discharge is provided on the curved surface portion, and the main discharge is used to generate ultraviolet rays. Therefore, it is placed on the curved surface of the user. The comparative example has a different read pattern, and is provided with a first electrode having a function as an ultraviolet reflecting member even in the side direction.

20112326L 情形時,亦可易於設計第一電極與第二電極的距離大致均 一的燈(例如,參照圖2)。 於圖2中,第-電極形成於放電管的外表面,但本發 明之第三發明並秘定於如此之情形,第—電極亦形成 於放電管的内面。 本發明之第四發明是,如第一發明中的紫外線燈,其 中,放電管的材質為石英玻璃。 1 ’、In the case of 20112326L, it is also easy to design a lamp in which the distance between the first electrode and the second electrode is substantially uniform (for example, refer to Fig. 2). In Fig. 2, the first electrode is formed on the outer surface of the discharge tube, but the third invention of the present invention is secreted in such a case that the first electrode is also formed on the inner surface of the discharge tube. According to a fourth aspect of the invention, in the ultraviolet lamp of the first aspect, the material of the discharge tube is quartz glass. 1 ',

於使用方箱型放電容器的比較例的燈中,照射於放電 容器的内面中的下表面與側面之間的角上的紫外線照射量 與其周圍部分相比較少。已知石英玻璃照射 引起分子構造中產生變化,且考慮到其變化的程度虚^ 線照射量成正比。因此’於放電管的材料中使用石英玻 時,於角及其周财’分子構造變化的程度會產生不=璃 結果’存在於放電容H中產生㈣㈣得易於破碎題。 本發明之第四發明中,於放電管的外周壁上 於透過紫外_平坦部對向的位置上,具備放電管内部 的面呈凹面的曲面部。藉由將放電管設為如此之形狀 使照射於放電管_面巾的平坦部兩端的角的部分 外線量與其周圍部分相比不會有較大差異。結果 不 易因紫外線照射而導致石英玻璃變形,故而放電管不易於 破碎。 本發明之第五發明是,如第三發明的紫外線燈,其中, 第-電極用於接地連接,且第一電極設置於曲面部的 面’並且放電管的㈣設置有賴連接高電壓的第二電極。 15 201123261 於先前的使用方箱型放電容器的燈中,為了製造的簡 便、及抑制由於使用燈而造成的電極的劣化等,而將誘發 放電的兩個電極均設置於放電容器的外侧。使燈點亮時, 在其中接地連接的一個電極(接地電極)與施加有高電壓 交流的電極(高電壓電極)之間產生放電。此時,若用於 透過紫外線的下表面上使用高電壓電極,由於高電壓電極 與產品w靠近’則會根據產品w的種類而引起高電壓電 極與產品W之間產生放電的問題。因此,必須於用於透過 紫外線的下表面使用接地電極,而於上表面使用高電壓電 極。於使用如此之方箱型放電容器的比較例的燈中,為了 抑制紫外線自放電容器的側方向放出,而自放電容器的上 表面跨越兩側的側面而設置有具有作為紫外線反射構件的 功能的高電壓電極。如此之情形時,高電壓電極中放電容 器側面上的部分靠近產品W。結果,根據產品w的種類, 而會存在尚電壓電極與產品w之間易於產生放電的問題。 本發明之第五發明中,第一電極設置於放電管的曲面 部的外表面。因此,可易於製造第一電極,且可抑制由於 燈的使用而造成的第一電極的劣化。進而,第五發明中, 第一電極用於接地連接。因此,儘管第一電極設置於放電 管的曲面部的外表面,亦不會自第一電極向產品w產生放 電。進而,第五發明中’用於連接高電壓的第二電極設置 於放電管的内部,故自第二電極向產品w的放電亦得 制。 201123261 另外,使用先前的圓筒形放電管之情形時,設為將第 電極δ又置於放電管的曲面部的外表面而用於 壓。如此之情形時,由於放電管為圓筒形,故第一電極並 未靠近至產品w的附近。因此,關於圓筒形的放電管即 使於將第一電極設置於放電管曲面部的外表面而用於連接 高電壓時,第一電極與產品w之間的放電亦幾乎沒有問 題。因此,本發明之第五發明可解決於放電管中存在用於 透過紫外線的平坦部之情形時所特有的問題。 籲 本發明之第六發明是,如第一發明的紫外線燈,其構 成為於曲面部上設置有第一電極,第一電極形成為沿著曲 面部且較自放電管的其中一個側部至另一個側部為止的整 個範圍更寬,放電管的内部設置有延伸於放電管長度方向 的線狀的第二電極,第二電極設置於平坦部的中心部附近 且在第一電極與第二電極之間產生主放電。 利用圖13中的放電管的剖面,對於第六發明中的「平 坦部的中心部附近」的含義加以說明。將形成於放電管外 • 壁面上的用於透過紫外線的平坦部201之放電管内側的面 設為底邊。此時,將與底邊平行的直線之收納於放電管内 的部分的長度最長的直線設為直線WL。將該直線WL與 放電管内面的兩個交點設為W1及W2。進而,將該W1 與W2的中心點設為WC。此時,將直線WL上的點中、 與WC的距離為WC與W1的距離之1/4的兩個點設為 W3及W4。此時,「平坦部的中心部附近」限定於通過 W3且垂直於直線WL的直線、與通過W4且垂直於直線 17 201123261 WL的直線之間。進而,將形成於放電管外壁面上的曲面 部2〇5 +、放電管内侧的面中距離底邊最遠的點設為頂點 T。將通過該頂點τ、且與底邊正交的直線設為基準線。將 該基準線與底邊的交點設為底點B。將與底邊平行的直線 中、通過頂點τ與底點B的中心點的直線設為直線Hc。 此時,「平坦部的中心部附近」限定於直線Hc與底邊之 間。亦即,第六發明中的「平坦部的中心部附近」為圖13 的放電管内所揭示的方形的内部。 第✓、發明中的「第二電極設置於平坦部的中心部附近」 是指,第二電極的垂直於放電管長度方向的剖面的中心點 設置於「平坦部的中心部附近」。 根據第六發明,使用有線狀的電極作為第二電極。因 此,無須使用如先前的方箱型紫外線燈的放電容器的紫外 線透過面上所使用的網狀電極作為第二電極。結果,可將 由第二電極所遮擋的紫外線的量抑制為較少。進而,根據 第六發明’除沿著形成為放電管内部側的面呈凹面的曲面 部205而設置有第一電極以外,且第二電極設置於平坦部 201的中心部附近。藉由如此之兩個電極的組合,於第一 電極的較寬範圍内,與第二電極的距離均大致均一。結果, 於放電管内的較寬範圍内產生放電,故而可獲得紫外線強 度變強的效果。 本發明之第七發明是,如第六發明的紫外線燈,其中, 第一電極的剖面為大致圓弧狀,且在與第一電極的上述剖 18 201123261 =的各關轉距_位置上,設置有延伸於放電 度方向的線狀的第二電極。 長 第七發明中的「等距離」並非僅指距離完 形。雖然距離稍不同作實際μ笛L ^ 放電之情形,亦二第:電極的大致整體均產生 :據第七發明,實際上可使自第一電極的大致整體產 域電管⑽更寬麵时產纽電。結果, 可獲件紫外線強度變得更強的效果。 本=之第八發明是,如第—發明的紫外線燈其構 $為你於曲面部上設置有第1極,於放電管的内部設置 於放電管長度方向的線狀的第二電極’且在第一電 Μ 一電極之間產生主放電,並且,於平坦部上設置有 極,且在第二電極與辅助電極之間產生辅助放電(參 照圖4 )。 此處,輔助電極起到如下作用,即,使第—電極與第 一電極之間易產生放電(域電),並且使主放電穩定化。 即’首先在第二電極與辅助電極之間引起放電(辅助 放電)。藉由該放電所產生的帶電粒子或亞穩態(metastabie _)的原子或離子、甚至光子,使產生、轉主放電時 所必需的施加電壓降低、结果,可使開始點燈時的電壓降 低,且可使點燈時的放電電漿穩定化。 而且,對於該種燈,為高輸出化而期望提高封入氣體 的。但;^,如此而設計時,財會使放電變得不穩定 (乂同封入氣體的壓力與在施加電壓恆定時增大電極間距 201123261 離具有大致相同的效果)。但是,第八發明中,可同樣且 有效地將藉由輔助放電而產生的帶電粒子或亞穩離原子 或離子、甚至光子供給至主放電空間内,故而^存在於 主放電空間内的放電氣體的電離係數(i〇nizati〇n coefficient)增加。隨之,由於主放電空間呈易於引起放電 的狀態,故可不使施加電壓增加而確保放電的穩定性。 第八發明中,在設置於放電管内部的第二電極、與設 置於平坦部上的辅助電極之間進行辅助放電,並且,在設 置於放電管内部的第二電極、與設置於曲面部上的第一冑 Φ 極之間進行主放電。藉由設為如此之構成,可高效藉由輔 助放電而誘導主放電’且可於放電管内確保較寬的主放電 區域。 本發明之第九發明是,如第一發明的紫外線燈,其構 成為,於曲面部上設置有第一電極,於放電管的内部設置 有延伸於放電管長度方向的線狀的第二電極,第二電極設 置於平坦部的中心部附近,且在第一電極與第二電極之間 產生主放電,並且於平坦部上不設置除第二電極以外的電 着 極。 第九發明中的「第二電極設置於坦部的中心部附近」 的含義與第六發明中的情形相同。 第九發明中的「平坦部上不設置除第二電極以外的電 極」並非指第二電極必須設置於平坦部上。第二電極可設 置於平坦部上,亦可離開平坦部而崎於放電管的内部。 20 201123261 根據第九發明,使用有延伸於放電管長度方向的線狀 電極作為用於主放電的第二電極。結果,可將由第二電極 所遮擋的紫外線的量抑制為較少。進而,由於平坦部上未 設有除第二;電極以外的電極,故可獲得由電極所遮擋的紫 外線量較少的燈。進而,根據第九發明,除沿著形成為放 電管的内部側的面呈凹面的曲面部205而設置有第一電極 以外,第二電極設置於平坦部201的中心部附近。藉由如 此之兩個電極的組合,於第一電極的較寬範圍内,與第二 電極的距離大致均一。結果,於放電管内的較寬範圍内產 生放電,故而可獲得紫外線強度變強的效果。 本發明之第十一發明是,如第一發明的紫外線燈,其 中,於曲面部的外表面設置有第一電極,且於曲面部的外 表面中、平坦部與曲面部的邊界附近未設置有第一電極(例 如,參照圖3)。 根據第十一發明,於平坦部與曲面部的邊界附近未設 置有第一電極,故第一電極與產品w的距離變遠。因此, • 即使將第一電極作為用於連接高電壓的電極而使用時,亦 可獲得難以在第一電極與產品…之間產生放電的效果。 本發明之第十二發明是,如第八發明的紫外線燈其 中,輔助電極設置於放電管之整個長度方向上。 紫外線照射裝置中所使用之放電管,通常使用長度方 向上較長的放電管。該較長的放電管中,僅於偏離紫外線 照射部位的長度方向的-端上設置有輔助電極。如此之情 形時,藉由於點亮燈時在放電管之端所產生的輔助放電,In the lamp of the comparative example using the square box type discharge vessel, the amount of ultraviolet rays irradiated on the corner between the lower surface and the side surface of the inner surface of the discharge container was smaller than that of the surrounding portion. Quartz glass irradiation is known to cause changes in the molecular structure, and the amount of exposure is proportional to the degree of change. Therefore, when quartz glass is used in the material of the discharge tube, the degree of change in the molecular structure at the angle and its periphery will result in a non-glass result, which occurs in the discharge capacitance H, and (4) (4) is easily broken. According to a fourth aspect of the invention, the outer peripheral wall of the discharge tube is provided with a curved surface portion having a concave surface inside the discharge tube at a position facing the ultraviolet-transparent portion. By setting the discharge tube to such a shape, the amount of the outer line which is irradiated to the corners of both ends of the flat portion of the discharge tube_skin is not greatly different from that of the surrounding portion. As a result, the quartz glass is not easily deformed by the ultraviolet ray irradiation, so that the discharge tube is not easily broken. A fifth invention of the present invention is the ultraviolet lamp of the third aspect, wherein the first electrode is used for the ground connection, and the first electrode is disposed on the surface of the curved portion and the (four) of the discharge tube is disposed adjacent to the second portion of the high voltage electrode. 15 201123261 In the lamp of the prior art box type discharge vessel, both electrodes for inducing discharge were provided outside the discharge vessel for ease of manufacture and suppression of deterioration of the electrode due to the use of the lamp. When the lamp is turned on, a discharge is generated between one electrode (ground electrode) connected to the ground and an electrode (high voltage electrode) to which a high voltage is applied. At this time, if a high voltage electrode is used on the lower surface for transmitting ultraviolet rays, since the high voltage electrode is close to the product w, there is a problem that discharge occurs between the high voltage electrode and the product W depending on the type of the product w. Therefore, it is necessary to use a ground electrode for the lower surface for transmitting ultraviolet rays and a high voltage electrode for the upper surface. In the lamp of the comparative example using such a square box type discharge vessel, in order to suppress the discharge of the ultraviolet light from the side direction of the discharge capacitor, the upper surface of the discharge capacitor is provided with a function as an ultraviolet reflection member across the side surfaces of both sides. High voltage electrode. In this case, the portion of the high voltage electrode on the side of the discharge capacitor is close to the product W. As a result, depending on the kind of the product w, there is a problem that the discharge between the voltage electrode and the product w is liable to occur. In the fifth invention of the present invention, the first electrode is provided on the outer surface of the curved portion of the discharge tube. Therefore, the first electrode can be easily manufactured, and deterioration of the first electrode due to use of the lamp can be suppressed. Further, in the fifth invention, the first electrode is used for the ground connection. Therefore, although the first electrode is disposed on the outer surface of the curved portion of the discharge tube, no discharge is generated from the first electrode toward the product w. Further, in the fifth invention, the second electrode for connecting the high voltage is provided inside the discharge tube, so that the discharge from the second electrode to the product w is also obtained. In the case of using the conventional cylindrical discharge tube, it is assumed that the first electrode δ is placed on the outer surface of the curved surface portion of the discharge tube for pressure. In this case, since the discharge tube is cylindrical, the first electrode is not close to the vicinity of the product w. Therefore, with regard to the cylindrical discharge tube, even when the first electrode is provided on the outer surface of the curved surface portion of the discharge tube for connecting a high voltage, there is almost no problem in discharge between the first electrode and the product w. Therefore, the fifth invention of the present invention can solve the problems unique to the case where a flat portion for transmitting ultraviolet rays exists in the discharge tube. According to a sixth aspect of the invention, the ultraviolet lamp of the first aspect of the invention is characterized in that the first electrode is provided on the curved surface portion, and the first electrode is formed along the curved surface portion and from one side of the discharge tube to The entire range from the other side is wider, the inside of the discharge tube is provided with a linear second electrode extending in the longitudinal direction of the discharge tube, and the second electrode is disposed near the center portion of the flat portion and at the first electrode and the second A main discharge is generated between the electrodes. The meaning of the "near the center portion of the flat portion" in the sixth invention will be described with reference to the cross section of the discharge tube in Fig. 13 . The surface on the inner side of the discharge tube of the flat portion 201 for transmitting ultraviolet rays formed on the outer wall surface of the discharge tube is referred to as a bottom side. At this time, a straight line having the longest length of the portion of the straight line parallel to the bottom side and housed in the discharge tube is defined as a straight line WL. The two intersections of the straight line WL and the inner surface of the discharge tube are set to W1 and W2. Further, the center point of W1 and W2 is WC. At this time, two points of the point on the straight line WL and the distance from the WC are 1/4 of the distance between WC and W1, and W3 and W4 are set. At this time, "the vicinity of the center portion of the flat portion" is limited to a straight line passing through W3 and perpendicular to the straight line WL, and a straight line passing through W4 and perpendicular to the straight line 17 201123261 WL. Further, the curved portion 2〇5 + formed on the outer wall surface of the discharge tube and the point on the inner side of the discharge tube which is the farthest from the base are set as the apex T. A straight line passing through the vertex τ and orthogonal to the bottom side is used as a reference line. Set the intersection of the baseline and the bottom edge as the bottom point B. A straight line passing through the center point of the vertex τ and the bottom point B in a straight line parallel to the bottom side is defined as a straight line Hc. At this time, "the vicinity of the center portion of the flat portion" is limited between the straight line Hc and the bottom side. In other words, the "near the center portion of the flat portion" in the sixth invention is the inside of the square disclosed in the discharge tube of Fig. 13. In the invention, "the second electrode is provided in the vicinity of the center portion of the flat portion" means that the center point of the cross section perpendicular to the longitudinal direction of the discharge tube of the second electrode is provided in the vicinity of the "center portion of the flat portion". According to the sixth invention, a wire-shaped electrode is used as the second electrode. Therefore, it is not necessary to use the mesh electrode used on the ultraviolet ray transmitting surface of the discharge vessel of the conventional square box type ultraviolet lamp as the second electrode. As a result, the amount of ultraviolet rays blocked by the second electrode can be suppressed to be small. Further, according to the sixth invention, the first electrode is provided except for the curved surface portion 205 which is concave on the surface on the inner side of the discharge tube, and the second electrode is provided in the vicinity of the central portion of the flat portion 201. With such a combination of the two electrodes, the distance from the second electrode is substantially uniform over a wide range of the first electrode. As a result, a discharge is generated in a wide range in the discharge tube, so that the ultraviolet intensity is enhanced. According to a seventh aspect of the present invention, in the ultraviolet lamp of the sixth aspect, the first electrode has a substantially arc-shaped cross section, and is located at each of the off-horizontal positions of the first electrode and the section 18 201123261 = A linear second electrode extending in the direction of the discharge is provided. The "equal distance" in the seventh invention is not only the distance completion. Although the distance is slightly different as the actual μ flute L ^ discharge, the second: the substantially whole of the electrode is generated: according to the seventh invention, the substantially whole field of the electric tube (10) from the first electrode can be made wider. Production of new electricity. As a result, the effect that the ultraviolet ray intensity becomes stronger is obtained. According to an eighth aspect of the present invention, in the ultraviolet lamp of the first aspect of the invention, the first electrode is provided on the curved surface portion, and the second electrode is disposed in the longitudinal direction of the discharge tube in the longitudinal direction of the discharge tube. A main discharge is generated between the first electrode and the electrode, and a pole is provided on the flat portion, and an auxiliary discharge is generated between the second electrode and the auxiliary electrode (refer to Fig. 4). Here, the auxiliary electrode functions to cause discharge (domain electric power) between the first electrode and the first electrode, and to stabilize the main discharge. That is, first, a discharge (auxiliary discharge) is caused between the second electrode and the auxiliary electrode. By the charged particles or metastable atoms or ions or even photons generated by the discharge, the applied voltage necessary for generating and rotating the main discharge is lowered, and as a result, the voltage at the start of lighting can be lowered. And the discharge plasma at the time of lighting can be stabilized. Further, in order to increase the output of such a lamp, it is desirable to increase the amount of the enclosed gas. However, when designed in this way, the discharge becomes unstable (the pressure of the enclosed gas is approximately the same as the increase of the electrode spacing when the applied voltage is constant). However, in the eighth invention, the charged particles or metastable atoms or ions or even photons generated by the auxiliary discharge can be supplied to the main discharge space in the same manner and effectively, so that the discharge gas existing in the main discharge space The ionization coefficient (i〇nizati〇n coefficient) increases. As a result, since the main discharge space is in a state of being easily discharged, the stability of the discharge can be ensured without increasing the applied voltage. According to an eighth aspect of the invention, the auxiliary electrode is provided between the second electrode provided inside the discharge tube and the auxiliary electrode provided on the flat portion, and is provided on the second electrode provided inside the discharge tube and on the curved surface portion. The main discharge is performed between the first Φ poles. With such a configuration, the main discharge can be efficiently induced by the auxiliary discharge and a wide main discharge region can be secured in the discharge tube. According to a ninth aspect of the present invention, in the ultraviolet lamp of the first aspect of the present invention, the first electrode is provided on the curved surface portion, and the second electrode extending in the longitudinal direction of the discharge tube is provided inside the discharge tube. The second electrode is disposed in the vicinity of the central portion of the flat portion, and a main discharge is generated between the first electrode and the second electrode, and an electrode other than the second electrode is not disposed on the flat portion. The meaning of "the second electrode is provided in the vicinity of the center portion of the stem portion" in the ninth invention is the same as that in the sixth invention. The "electrode other than the second electrode is not provided on the flat portion" in the ninth invention does not mean that the second electrode must be provided on the flat portion. The second electrode may be disposed on the flat portion or may be apart from the flat portion and may be inside the discharge tube. According to the ninth invention, a linear electrode extending in the longitudinal direction of the discharge tube is used as the second electrode for main discharge. As a result, the amount of ultraviolet rays blocked by the second electrode can be suppressed to be small. Further, since the electrode other than the second electrode is not provided on the flat portion, a lamp having a small amount of ultraviolet rays blocked by the electrode can be obtained. Further, according to the ninth aspect of the invention, the second electrode is provided in the vicinity of the center portion of the flat portion 201 except that the first electrode is provided along the curved surface portion 205 which is formed as a concave surface on the inner side of the discharge tube. With a combination of the two electrodes as such, the distance from the second electrode is substantially uniform over a wide range of the first electrode. As a result, a discharge is generated in a wide range in the discharge tube, so that an effect of increasing the ultraviolet ray intensity can be obtained. According to an eleventh aspect of the present invention, in the ultraviolet lamp of the first aspect of the present invention, the first electrode is provided on the outer surface of the curved surface portion, and the outer surface of the curved surface portion is not disposed near the boundary between the flat portion and the curved portion There is a first electrode (for example, see Fig. 3). According to the eleventh aspect of the invention, since the first electrode is not provided in the vicinity of the boundary between the flat portion and the curved surface portion, the distance between the first electrode and the product w becomes longer. Therefore, even when the first electrode is used as an electrode for connecting a high voltage, it is possible to obtain an effect that it is difficult to generate a discharge between the first electrode and the product. According to a twelfth aspect of the invention, in the ultraviolet lamp of the eighth aspect of the invention, the auxiliary electrode is disposed in the entire length direction of the discharge tube. As the discharge tube used in the ultraviolet irradiation device, a discharge tube having a long length in the longitudinal direction is usually used. In the longer discharge tube, the auxiliary electrode is provided only at the end which is deviated from the longitudinal direction of the ultraviolet ray irradiation portion. In such a situation, by the auxiliary discharge generated at the end of the discharge tube when the lamp is lit,

S 21 201123261 =產=電粒子等。由於該些帶電粒子等,而使得輔助電 附’生主放電,進而該主放電科離獅電極較遠之 位置上產生主放電,藉此,整體放電管產生放電。然而, 於如此之情料’於離難電極較遠處,並沒有使點燈時 使放電穩定化_職€的效果。目此 均或火花狀放電。結果,產生均齊度(捕二 dlummance)降低或處理的不穩定性的問題。對此,本發 明之第十二發财,辅助電極設置於放電管之整個長度方S 21 201123261 = production = electric particles, etc. Due to the charged particles or the like, the auxiliary electrode is discharged, and the main discharge is generated at a position far from the lion electrode, whereby the entire discharge tube generates a discharge. However, in such a situation, it is far from the electrode that is divorced, and there is no effect of stabilizing the discharge when lighting. This is the case or spark discharge. As a result, there arises a problem that the uniformity (dlummance) is lowered or the instability of the treatment is caused. In this regard, the twelfth fortune of the present invention, the auxiliary electrode is disposed over the entire length of the discharge tube

向上。因此,因輔助放電而產生的帶電粒子等均一分^於 放電管内的整體上。結果’可獲得主放電穩定的效果。 另外,第十二發明中的整個長度方向是指,放電管内 使放電產生的部分的大致全長。例如,於放電管的端部上 未設輩有第一及第二電極,因此當設有不產生放電的;分 時,即使於該部分上未設置有輔助電極,亦相當於第;二 發明。關於該情形,若考慮到輔助電極的設置目的,装二 為當然。 Μ 【實施方式】up. Therefore, the charged particles and the like which are generated by the auxiliary discharge are uniformly divided into the entire inside of the discharge tube. As a result, the effect of stabilizing the main discharge can be obtained. Further, the entire longitudinal direction in the twelfth invention means substantially the entire length of a portion where discharge occurs in the discharge tube. For example, the first and second electrodes are not provided on the end of the discharge tube, so that when no discharge is generated, the time division, even if the auxiliary electrode is not provided on the portion, is equivalent to the second invention; . In this case, it is a matter of course to take into consideration the purpose of setting the auxiliary electrode. Μ [Embodiment]

&lt;第1實施形態&gt; 以下,參照圖1及圖2,詳細說明將本發明具體化 第1實施形態。 八 、 圖1表示本實施形態的準分子燈丨的侧剖面圖,圖2 表示垂直於放電管長度方向的面的剖面圖。該準分子燈工 中具備放電管2。放電管2成為具備如下部位的二重^構 22 201123261 造,即:外管部3,由石英破螭 由石英玻璃所形成且插入外管部^ ’ a内管部4,同樣 外管部3呈如下形狀,即 圓弧的-部分進行打磨而使其=長的圓筒中對外周壁 拱形的曲面部5 ;以及連接該曲 。即,具備:剖面為 平板狀的平坦部6。曲面部ΐ與平弧的兩端緣的 5A呈弧形。另一方面,内管部J C所接合的角部分 筒狀,且配置於平坦部6的内小於外管部3的圓 上。外管部3與内管部二==向=&lt;First Embodiment&gt; Hereinafter, the present invention will be described in detail with reference to Figs. 1 and 2 . 8. Fig. 1 is a side sectional view showing the excimer lamp holder of the embodiment, and Fig. 2 is a cross-sectional view showing a surface perpendicular to the longitudinal direction of the discharge tube. The excimer lamp is provided with a discharge tube 2. The discharge tube 2 is a double structure 22 201123261, that is, the outer tube portion 3 is formed of quartz glass and is inserted into the outer tube portion 4 a inner tube portion 4, and the outer tube portion 3 is similarly formed. The curved surface portion 5 having a shape in which a portion of the circular arc is polished so that the outer circumference wall is arched in the long cylinder; and the curved portion is connected. In other words, the flat portion 6 having a flat plate shape is provided. The curved portion is curved in the 5A of both ends of the flat arc. On the other hand, the corner portion to which the inner tube portion J C is joined is cylindrical, and is disposed inside the flat portion 6 to be smaller than the circle of the outer tube portion 3. Outer tube part 3 and inner tube part two == direction =

部3、4所包圍的放電空間7内填充有 於以兩S 電用氣體,例如可使軌氣、氬 :。作為放 所使用的氣體。 ^ H等該種燈中通常 第-中設置有—對電極&quot;。該些-對電極中, 第電極8含有固著於外管部3的曲面部 二二 反射紫Μ卜料第電的材f,較好的是使用可 質。作為如此之材質,例如可使用】 3的立中ί —電極8軸為沿著曲面部5且較自外管部 L二:侧部至另一個側部為止的整個範圍更寬。進 ρ電ίΐ於放電管2長度方向的紫外線燈的剖面上,於 第電極8的紫外線反射面中較其中一個側部 ==垂直於紫外線反射面的切平面且朝向輸= 4的方向’較自其中一個側部朝向另—個側部的方向更朝 23 201123261 且’該第一電極8的端緣部8A與平坦部6的侧端 彎曲面1矣自平坦部6的平坦的面,向具有曲率的 f曲:移:的邊界位置)之間設有不存在第-電極8的間 立、、而S之’第-電極8於曲.面部5上設置於較與平坦 =接合位置更退後的值置上。另一方面,與該第一電 4* j對的第二電極9包含錄線,插入内管部4的内部且 Η 越其全長。此處,第二電極9設置於與第一電極8 上的各點均為等距離的位置上。 琴此it —電極8、9上連接有導線1G、11的—端部,且 lG、U的另—端部連接於交流電源裝置12。 效果r★’說明如上述方式而構成的本實施形態的作用及 昭射1以平坦部6側作為出射面而設置於紫外線 3裝置(未圖示)中。即’準分子燈i於例如照射室中, 於傳送騎縣產品W的倾帶 坦部^則朝向下方(產品而安裝。 方將千 當對產品W進行紫外線照射處 照射室内。自上方藉由準分子燈 線m產品〜上。此時,放電管内所產生的紫外 冰嫂圖Γ,以虛線箭頭表示)中向平坦部6方向前進的紫 、,直接通過平坦部6而朝向產品w射出。另一方” 向曲面部5方向前進的紫外線被第一電極8反射後,自平 坦。(5 6側朝向產品w射出。 24 201123261 照射完成後,產品w藉由傳輪帶自照射室傳送出並運 送至下一製程。 如上所述,根據本實施形態,於放電管2的外管部$ 上設置有平坦部6及曲面部5,且第一電極8設置於曲面 部5上。若藉由具備如此之結構的準分子燈丨進行照射, 則由於出射面側為平坦的面,故而整個出射面整體與產品 W的距離均等。因此,即使在大氣下亦可將紫外線被氧氣 吸收的損耗抑制為最小限度,進而,可均等地對產品w的 •整個面進行照射。 而且’使第一電極8由如鋁之紫外線的反射率較高的 材料而形成時’第一電極8起到將向曲面部5側放射的紫 外線反射而向平坦部6側(出射面側)聚集的反射板的作 用。如此’無需另外設置反射板而可使紫外線聚集於出射 面側,故而能夠以簡易的結構而提高照射效率。 進而’第一電極8與平坦部6的侧端緣6A之間空開 間隔而設置。此處,若第一電極8的端緣部8A到達照射 φ 面(平坦部6),則例如產品W為導電性,且產品W與 第一電極8之間存在電位差時,可能導致在該產品w與第 一電極8的端緣部8A之間引起放電。但是,本實施形態 中設為’第一電極8的端緣部8A位於較照射面更退後的 位置上’故而可避免其與產品W之間引起放電。 另外’放電管2為具備外管部3以及内管部4的二重 管構造’且第二電極9形成於内管部4的内部。根據如此 之構成’平坦部6 (出射面)上不存在電極,故而即使電 25 201123261 極產生氧化、劣化,亦不會因由如此之劣化所產生的微粒 而污染產品w。 另外,本實施形態中,第二電極9是由金屬線所形成 的線狀電極。根據如此之構成,在線狀電極的周圍電場強 度變高。電場強度較高之處,電子的速度分佈向高能量側 偏移而放電用氣體的電離概率(i〇nizati〇n pr〇babiHty)變 高,故而電離係數變大。即,使用如此之不平等電場的放 電方式中,線狀電極附近呈特別易於放電的狀態。因此, 即使在放電管2長度方向上的電極間距離存在少許不均, 亦難以產生放電不均。而且,一對電極之兩者為以某程度 ^面積而展開的形態,與易受電極間距離的不均(例如, 介電體的厚度*均或平板的彎曲或凹凸等)影響的先前的 燈相比較,放電的均一性較好。 進而,可盡可能減少由於第二電極9所引起的出射光 的遮蔽,故而光的導出效率較好。 進而,第1實施形態成為如下構造,即,相當於「發 ,之揭不」中所揭示的本發明之第一發明、第二發明第 j明日、第四發明、第六發明、第七發明、第九發明及第 於「發,。因此,作為藉由該些發明所獲得的效果而揭示 ;發明之揭不」中的效果,於第1實施形態中可獲得。 &lt;第2實施形態&gt; π@以下參照圖3說明本發明的第2實施形態。本實施 的準刀子燈2〇與第!實施形態主要的不同之處在於, 26 201123261 ,電管21為單管構造、以及第二電極㈣置於平3 上0 子施職神分子―的剖面圖。該準分 ί二電管2卜該放電管21由石英_所構 -呷八打磨而“单Γ ’於細長的圓筒中將外周壁圓弧的 心打磨而使其平板化。即,放電管2 =χ及連接該曲面部22中圓弧的兩端緣的二 放電管21的曲面部22上,盘坌!也 f V 一第1實施形態相同地設 置有第電極24。另一方面,第二電極25設置㈣ 第&quot;電極25以放㈣21長度方向的大 产==二為細線狀’且配置於該平坦部23的寬 度方向(侧方向)中央位置上。該些電極24、^ ^線的一端部’且該些導線的另—端部連接於交流電源裝 平2g時,與第1實施形態同樣,使 二?側朝向產e〇w側而設置於紫外線 圖不)上’而進行照射。此時,由於出射面侧 故而整個出射面整體與產品|的_ 社一’ 大氣下亦可將紫外線被氧吸收:損耗離二最结:限=The discharge space 7 surrounded by the sections 3 and 4 is filled with a gas for two S, and for example, a rail gas or an argon gas can be used. Used as a gas for discharge. ^ H and other such lamps are usually provided with a - counter electrode &quot;. Among the counter-electrodes, the first electrode 8 is provided with a curved surface portion fixed to the outer tube portion 3, and the second material is reflected from the vitreous material, and it is preferable to use a mass. As such a material, for example, the center of the electrode 8 can be used to be wider along the entire surface of the curved portion 5 and from the outer tube portion L: the side portion to the other side portion. In the cross section of the ultraviolet lamp in the longitudinal direction of the discharge tube 2, the side of the ultraviolet reflecting surface of the first electrode 8 is more than one side == perpendicular to the tangent plane of the ultraviolet reflecting surface and oriented toward the direction of the input = 4 The direction from one of the side portions toward the other side portion is further toward 23 201123261 and the end edge portion 8A of the first electrode 8 and the side end curved surface 1 of the flat portion 6 are flat from the flat surface of the flat portion 6 The f-curve having a curvature: the boundary position of the shift: is provided with the vacancy in which the first electrode 8 is absent, and the 'first electrode 8' of the S is provided on the face 5. The face 5 is disposed more than the flat=joining position. The value of the back is set. On the other hand, the second electrode 9 of the pair of the first electric wires 4* includes a recording line which is inserted into the inside of the inner tube portion 4 and has a full length thereof. Here, the second electrode 9 is disposed at a position equidistant from each point on the first electrode 8. This is the end of the electrodes 1 and 9 to which the wires 1 and 11 are connected, and the other ends of the lG and U are connected to the AC power supply unit 12. The effect r★' indicates that the action of the present embodiment and the first shot 1 configured as described above are provided in the ultraviolet ray device (not shown) with the flat portion 6 side as the exit surface. In other words, the excimer lamp i is, for example, in the irradiation chamber, and the tilting belt portion of the product of the riding county is placed downward (the product is installed. The square is irradiated with ultraviolet rays to the product W. The excimer lamp line m is on the product w. At this time, the ultraviolet ray pattern generated in the discharge tube, which is indicated by a broken line arrow, is purple which is advanced in the direction of the flat portion 6, and is directly emitted toward the product w through the flat portion 6. The other side "the ultraviolet light that has proceeded in the direction of the curved surface portion 5 is reflected by the first electrode 8, and is self-flattening. (5 6 side is emitted toward the product w. 24 201123261 After the irradiation is completed, the product w is transported from the irradiation chamber by the transfer belt and As described above, according to the present embodiment, the flat portion 6 and the curved surface portion 5 are provided on the outer tube portion $ of the discharge tube 2, and the first electrode 8 is provided on the curved surface portion 5. When the excimer lamp having such a configuration is irradiated, since the exit surface side is a flat surface, the entire exit surface is equidistant from the product W. Therefore, the loss of ultraviolet rays absorbed by oxygen can be suppressed even in the atmosphere. To the minimum, the entire surface of the product w can be uniformly irradiated. Further, when the first electrode 8 is formed of a material having a high reflectance of ultraviolet rays such as aluminum, the first electrode 8 serves as a direction. The ultraviolet ray emitted from the side of the curved surface portion 5 is reflected by the reflecting plate that is concentrated on the side of the flat portion 6 (the emitting surface side). Thus, it is possible to condense the ultraviolet ray on the emitting surface side without separately providing a reflecting plate. Further, the irradiation efficiency is improved by the simple structure. Further, the first electrode 8 is provided at an interval from the side edge 6A of the flat portion 6. Here, when the edge portion 8A of the first electrode 8 reaches the irradiation φ plane (flat In the portion 6), for example, when the product W is electrically conductive and there is a potential difference between the product W and the first electrode 8, the discharge may be caused between the product w and the edge portion 8A of the first electrode 8. However, this is caused. In the embodiment, it is assumed that the end edge portion 8A of the first electrode 8 is located at a position further away from the irradiation surface. Therefore, it is possible to prevent the discharge from occurring between the product and the product W. Further, the discharge tube 2 is provided with the outer tube portion 3 and The double pipe structure of the inner tube portion 4 and the second electrode 9 are formed inside the inner tube portion 4. According to the configuration, the electrode is not present on the flat portion 6 (exit surface), so that even if the electricity 25 201123261 is extremely oxidized, Deterioration does not contaminate the product w by the particles generated by such deterioration. In the present embodiment, the second electrode 9 is a linear electrode formed of a metal wire. According to such a configuration, around the linear electrode The electric field strength becomes high. Electric field strength At a higher point, the velocity distribution of the electrons shifts toward the high energy side and the ionization probability of the discharge gas (i〇nizati〇n pr〇babiHty) becomes higher, so the ionization coefficient becomes larger. That is, the use of such an unequal electric field is used. In the discharge method, the vicinity of the linear electrode is in a state of being particularly easy to discharge. Therefore, even if there is a slight unevenness in the distance between the electrodes in the longitudinal direction of the discharge tube 2, it is difficult to cause discharge unevenness. The uniformity of the discharge is compared with the previous lamp which is affected by a certain degree of area and the influence of the unevenness of the distance between the electrodes (for example, the thickness of the dielectric * or the curvature or unevenness of the flat plate). Further, the shielding of the emitted light due to the second electrode 9 can be reduced as much as possible, so that the light extraction efficiency is good. Further, the first embodiment has the following structure, that is, the first invention, the second invention, the seventh invention, the fourth invention, the sixth invention, and the seventh invention of the present invention disclosed in "Send, Uncover" The ninth invention and the effect of the invention are disclosed in the first embodiment as disclosed in the first embodiment. &lt;Second Embodiment&gt; π@ Hereinafter, a second embodiment of the present invention will be described with reference to Fig. 3 . The knives of this implementation are 2 〇 and the first! The main difference of the embodiment is that, in 26 201123261, the electric tube 21 is a single-tube structure, and a cross-sectional view of the second electrode (four) placed on the flat 3 on the service god. The discharge tube 21 is polished by a quartz _ 呷 呷 而 而 而 而 而 而 “ “ “ “ “ “ 于 于 于 于 于 于 于 于 于 于 于 于 于 于 于 细长 细长 细长 细长 细长 细长 细长 细长 细长 细长 细长 细长 细长 细长 细长 细长2 = χ and the curved surface portion 22 of the two discharge tubes 21 that connect the both end edges of the arc of the curved surface portion 22, and the first electrode 24 is provided in the same manner as in the first embodiment. The second electrode 25 is provided with (four) the second electrode 25 in the longitudinal direction of the discharge (four) 21, and the second electrode is disposed in the center of the width direction (lateral direction) of the flat portion 23. The electrodes 24, ^ When the other end of the wire is connected to the AC power supply 2g, as in the first embodiment, the second side is placed on the ultraviolet ray side. At this time, due to the exit surface side, the entire exit surface and the product | _ 社 一 ' atmosphere can also absorb ultraviolet light by oxygen: loss from the two most knot: limit =

仃照射,進而,可均等地對整個產品|進行 X 本實施形態令,第二電極25設置於平坦部t 管外侧之面上^此時,藉由使第二電極25形 可將電極25的粗歧為必要的最低限度且可盡可能減少 27 201123261 對出射光的遮擋。而且,藉由將第二電極25配置於平垣部 23的寬度方向(侧方向)的中心位置,可避免在照射面的 寬度方向上產生照射強度的不均。 進而,第2實施形態成為如下構造,即,相當於「發 明之揭示」中所揭示之本發明的第一發明、第二發明、第 三發明、第四發明、第七發明、第十發明及第十一發明。 因此,作為藉由該些發明所獲得的效果而揭示於「發明之 揭示」中的效果,於第2實施形態中亦可獲得。仃 irradiation, and further, the entire product can be uniformly performed. In this embodiment, the second electrode 25 is disposed on the outer surface of the flat portion t tube. At this time, the second electrode 25 can be formed to shape the electrode 25 Roughness is the minimum necessary and can be minimized. 27 201123261 The occlusion of the outgoing light. Further, by arranging the second electrode 25 at the center position in the width direction (lateral direction) of the flat portion 23, unevenness in the irradiation intensity in the width direction of the irradiation surface can be avoided. Furthermore, the second embodiment corresponds to the first invention, the second invention, the third invention, the fourth invention, the seventh invention, and the tenth invention of the present invention disclosed in the "Disclosure of the Invention". The eleventh invention. Therefore, the effects disclosed in the "disclosure of the invention" as an effect obtained by the inventions are also obtained in the second embodiment.

&lt;第3實施形態&gt; 以下,參照圖4〜圖6,對本發明的第3實施形態進行 說明。本實施形態中的準分子燈3〇與第丨實施形態的主要 不同之處在於,於平坦部35的外壁上設置有輔助電極39。 圖4表示本實施形態中的準分子燈30的剖面圖。該準 =子燈30具備放電管31&lt;)放電管31與第i實施形態同樣, ,為具備如下部位的二重管構造,包括外管部32,其由石 英玻璃形成;以及内管部33,其同樣由石英玻摘形成 插入外管部32的内部。 驭&lt;Third Embodiment&gt; Hereinafter, a third embodiment of the present invention will be described with reference to Figs. 4 to 6 . The excimer lamp 3A of the present embodiment is mainly different from the second embodiment in that an auxiliary electrode 39 is provided on the outer wall of the flat portion 35. Fig. 4 is a cross-sectional view showing the excimer lamp 30 of the present embodiment. The sub-lamp 30 includes a discharge tube 31 &lt;) The discharge tube 31 is a double tube structure including the outer tube portion 32 formed of quartz glass and the inner tube portion 33 as in the i-th embodiment. It is also formed by quartz glass to form the inside of the outer tube portion 32.驭

yr言邵32與第1實施形態同樣設為如下形狀,即 細長的圓筒中將外周_弧的—部分打磨而使其平板4 即’具備拱形的曲面部34、以及連接該曲面部%的^ 兩端緣的平板狀的平坦部35,且曲面部34與平坦部3 ^的角部分34A成弧形。另-方面,内管部33亦與 實施形態同樣’為赵小於外管部32的圓筒狀,且配: 平坦部35的内壁面上寬度方向(放電管31的側方向: 28 201123261 管部32與内管部33是以兩端相互接合, 用L 33所包圍的放電空間36内填充有放電 極37':ί電J 31中與第1實施形態相同地設置有-對電 L J ^•電極37包含固著於外管部32的曲面部料 ._ 的鋁膜。另一方面,第二電極38與第i實施形 j樣由鎳線形成,且插人内f部33的码 =該地37、38上輸導_1== 線的另端部連接於交流電源裝置。 而35中外管部的外側之面上,錢跨越整個面 而叹置有輔助電極39。該輔助電極39辅助一 於本實施㈣中,由於平坦部35側為出 射面故而輔助電極39形成為網狀,以使其盡可能不雜 自放電管31的内侧所放射出的光。另外,較好的是輔^ =39設置於放電管31之整個長度方向上。其原因在於, 藉此,可在放電管31之整個長度方向上使放 &quot;f用如此之準分子燈3〇時,與第丄實施形態同樣,使 平坦部35側朝向產品w侧綠置於紫外線照射裝置 圖示)上,並進行照射。 藉由高頻電源而向第一電極37及輔助電極39 二電極38之間施加高頻電壓時’首先,於第二電極%的 附近’在第二電極與輔助電極3 9之間引起放電。繼而,誃 放電沿著平坦部35的板面向側方向展開(輔助放電;參^ 29 201123261 圖5)。其後,亦在第一電極37與第二電極38之間引起 主放電,放電在整個放電空間36内展開(參照圖6)。 另外,使用實際的準分子燈30時,由於通常施加高頻 交流電壓,故而難以目測確認階段性引起輔助放電與主放 電的情形。但是,藉由使用示波器觀察有關輔助放電與主 放電的放電電流’則可確認如上所說明的輔助放電及主放 電的階段性的產生。 牝處,相對於第二電極38而將辅助電極39配置於較In the same manner as the first embodiment, the yr rhyme 32 has a shape in which the outer circumference of the arc is partially polished, and the flat plate 4, that is, the curved surface portion 34 having the arch shape, and the % of the curved surface portion are connected. ^ The flat flat portion 35 at both end edges, and the curved surface portion 34 and the corner portion 34A of the flat portion 3^ are curved. On the other hand, the inner tube portion 33 is also cylindrical in shape smaller than the outer tube portion 32 in the same manner as the embodiment, and is provided with the width direction of the inner wall surface of the flat portion 35 (the side direction of the discharge tube 31: 28 201123261 tube portion) 32 and the inner tube portion 33 are joined to each other at both ends, and the discharge space 36 surrounded by L 33 is filled with a discharge electrode 37': in the same manner as in the first embodiment, a pair of electric LJ is provided. The electrode 37 includes an aluminum film fixed to the curved surface portion of the outer tube portion 32. On the other hand, the second electrode 38 is formed of a nickel wire and the i-th embodiment, and the code of the in-part f portion 33 is The other end of the line 137=38 on the ground 37, 38 is connected to the AC power supply unit. On the outer side of the outer tube portion of the 35, the auxiliary electrode 39 is slanted across the entire surface. In the fourth embodiment, the auxiliary electrode 39 is formed in a mesh shape so that the light emitted from the inner side of the discharge tube 31 is not trapped as much as possible. The auxiliary ^=39 is disposed in the entire length direction of the discharge tube 31. The reason is that, thereby, the entire length of the discharge tube 31 can be The discharge &quot; f 3〇 when using an excimer lamp so, similarly to the first embodiment Shang form the flat portion 35 side toward the side of the green product is placed w ultraviolet irradiation device shown), and irradiated. When a high-frequency voltage is applied between the first electrode 37 and the second electrode 38 of the auxiliary electrode 39 by the high-frequency power source, 'first, near the second electrode %', a discharge is caused between the second electrode and the auxiliary electrode 39. Then, the 放电 discharge is spread along the plate-facing side of the flat portion 35 (auxiliary discharge; see Fig. 5 201123261 Fig. 5). Thereafter, a main discharge is also caused between the first electrode 37 and the second electrode 38, and the discharge is developed in the entire discharge space 36 (see Fig. 6). Further, when the actual excimer lamp 30 is used, since a high-frequency AC voltage is usually applied, it is difficult to visually confirm that the auxiliary discharge and the main discharge are caused stepwise. However, by observing the discharge current of the auxiliary discharge and the main discharge by using an oscilloscope, the staged generation of the auxiliary discharge and the main discharge as described above can be confirmed. At the crucible, the auxiliary electrode 39 is disposed relative to the second electrode 38

第一電極37距離更近的位置上,故而,首先在第二電極 38與輔助電極%之間引起輔助放電。藉由該放電所產生 的帶電粒子或亞穩態的原子或離子、甚至光子,使在第一 =極37與第二電極38之間用於產生主放電的電壓降低。 釔果^可使準分子燈30開始點燈時的電壓降低,且可使放 電穩定化。 的壓於該種燈’期望獲得高輸出而提高封入氣體 穩定疋,如此進行設計時,通常會使得放電變得不The first electrode 37 is at a closer distance, so that an auxiliary discharge is first caused between the second electrode 38 and the auxiliary electrode %. The voltage used to generate the main discharge between the first = electrode 37 and the second electrode 38 is lowered by the charged particles or metastable atoms or ions or even photons generated by the discharge. The result is that the voltage at which the excimer lamp 30 starts to light is lowered, and the discharge can be stabilized. The pressure on the lamp is expected to obtain a high output to increase the stability of the enclosed gas. When designing, the discharge is usually not made.

電'極|^==氣體壓力與在施加電壓蚊的情況下增大 可-檨H 有大致相_效果)。但是,本實施形態中, 態的原子辅助放電所產生的帶電粒子或亞穩 使主放雷L 、甚至光子供給至主放電空間内,故而可 之,由於ΓΓ内所存在的放電氣體的電離係數增加。隨 施加電壓間呈綠引起放電陳g,故無須增加 电壓而可確保放電的穩定性。 30 201123261 2著放電所放射的紫外線(圖中,以虛線箭頭表示) 中’向平坦部35方向前進的紫外線直接通過平坦部% 辅助電極39的網眼而朝向產品W射出。另-方面,向曲 面部34方向前進的紫外線被第一電極37反射後,曰 部35側朝向產品w射出。 — 如此,根據本實施形態,可降低燈開始點燈時的 且可確保放電穩定性。 鲁 另外,更好的是,第二電極38位於第一電極37與輔 助電極39之間,且接近辅助電極39,最好的是,如本實 施形態般,收納第二電極38的内管部33大致密著於平坦 部35的内壁面。 其中,第二電極38亦可不必如上述般而配置。若將第 一電極38配置於如下位置上,即施加有電壓時,在第二電 極38與辅助電極39之間引起輔助放電,而後於第一電極 37與第二電極38之間引起主放電,則可達成本發明的目 的。換而&amp;之,在第二電極38—輔助電極39之間,較在 • 第一電極37~第二電極38之間更先引起放電之方法較有 效’可使第二電極38配置於如下位置上,即,將第一電極 37與第二電極38的最短距離設為La,將電極39與第二 電極38的最短距離設為Lb時,滿足 La&gt;Lb 的關係。 而且’於本實施形態中,亦與第1實施形態同樣將平 坦部35設為用於光透過,且出射面側為平坦的面。因此, 31 201123261 整個出射面與產品w的距離均等,故而,即使在大氣下亦 可將紫外線被氧其魏的損耗抑料最小限度。進而,可 均等地對產品W的整個面進行照射^而且,由於第一電極 37由可反射紫外線的材料而形成,故而第―電極37起到 將向曲面部34側放射的紫外線反射而聚集向平坦部%側 (出射面侧)的反射板的作用。繼而,設置於平坦部35 上的辅助電極39設為網狀’以使其不遮擋射出的光。根據 如此之構成’與第1實施形態同樣,可無須另外設置反射 板而使紫外線聚集於出射面侧,故而可以簡易的結構提高 照射效率》 進而’第3貫施形態成為如下構造,即,相當於「發 明之揭示」中所揭示之本發明的第—發明、第二發明、^ 三發明、第四發明、第五發明、第六發明、第七發明、第 八發明、第十-發明及第十二發明。因此作為藉由該些 發明所獲得的效果而揭示於「發明之揭示」中的效果,於 第3實施形態中可獲得。 ' 實施例 [確認紫外線的照射效率的實施例] 1.燈的製作 C實施例1&gt; 製作具有與第1實施形態同樣構造的準分子燈。使鋁 蒸鍍於與第1實施形態的外管部3形狀相同的筒狀電子管 上,以使其大致覆蓋曲面部的外侧。另外,筒狀電子管為 σ成石英(信越石英股份有限公司製SUp_F31〇)製,^ 201123261 半=Γ6子 職,曲面部外周面的曲率 曲㈣與平㈣接合的肖部分_弧的外 周面之曲率核為5 mm。於該電 約為4麵、壁厚約為。.8mm的合成石卜; 的内部插入有直徑約為! mm的鎳線。於電子管内^^ =放 =直至,為止,綱極作為: C # t Μ二U *壓電極,並施加3 G kHz的高頻電壓 管的整Sir使其放電。放料-地產生於電子 &lt;比較例1&gt; 另一方面,為了進行比較,製作先前的具有二重管構 造的燈。將18驗於外徑為32 mm的電子管的外周面之 後二藉由侧而形成網狀電極(開口率為議)。於該電 子官的内σρ配置有與上述實施例構造相同的合成石英管, 且使錄線插入其内部。於電子管内封入氣氣作為放電氣體 直至”Γ為止’將|g紐電轉為接地電極,將錄線 籲作為面壓電極’並施加30 kHz的高頻電壓(峰值電壓為8 kV)而使其放電。 2.點燈測試 不使用照射用具而在大氣中點亮實施例及比較例的 燈’在燈正下方3mm的位置上使用uv感測器以3m/min 的速度於水平方向上進行掃描。對累計光量進行比較的結 果為’實施例的燈約為比較例的燈的3倍,可確認能夠將 紫外線高效地照射於被照射物上。 33 201123261 [確認輔助電極之效果的實施例] &lt;實施例2&gt; 製作具有與第3實施形態構造相同的準分子燈。使長 度為1000 mm、厚度為0.2 mm的鎳膜(外側電極)固著 於與第3實施形態的外管部32形狀相同的筒狀電子管上, 且使其大致覆蓋曲面部的外表面。另外,筒狀電子管為合 成石英(信越石英股份有限公司製SUPRASIL_F31〇)製, 壁厚為2 mm、電子管長為1100 mm、曲面部外周面的曲 率半徑為16mm,曲面部與平坦部接合的角部分的圓弧之 外周面的曲率半徑為5 mm。於該電子管的内部,配置有 夕+卜徑約為5 mm、内徑約為2 mm的合成石英管,且於該石 英管的内部插入有直徑約為18mm的鎳線(内側電極卜 而且’於筒狀電子管中固著有寬度為22咖、長度 致厚上為G.2 mm的sus製網狀板(辅助電極).,: 使其大致覆i平坦㈣外表面。自中心軸至 坦部的固著面)為止__為^^ 於電子管内封入亂氣作為放電氣體直至 士,將錄膜及網狀板作為接地電極,將古為 並施加7〇此的大致為矩形的高輕電極’ 若逐漸提高施加電堡,則在峰值達 ^放電。 坦部的内壁面而產生辅助放電,发 = 2kV時沿著平 側電極(錄線)—外侧電極(錦膜 j5.5kV時於内 可知,主放電並不妨礙辅助放電 曰 主放電。並且 最低限度的施加電㈣5.5 kv。另Θ始點燈時所需之 乃—方面,為了進行比較, 34 201123261 製作除未设網狀板(辅助電極)以外皆與實施例2中相同 的燈而進行測試時,若不施加峰值為約1〇 kV的電壓則 不f生主放電。如此,設有辅助電極的燈中,能夠以約為 未没置輔助電極的燈的二分之一的施加電壓而產生主放 電。 七進而,於實施例2的燈中,將開始點燈後的峰值電壓 固定為5.5 kV而調查放電穩定性時,不會產生火花狀放電 鲁 或放電不均,自開始點燈後可實現穩定的放電。對此,在 未没置辅助電極的燈中進行同樣的實驗時,產生火花,且 產生放電不均。 &lt;其他實施形態&gt; 本發明的技術性範圍並非由上述實施形態所限定,例 如,如下所揭示的内容亦包含於本發明的技術範圍内。 (1) 上述各實施形態中,第一電極8與平坦部6的端 緣之間空開間隙而設置,但例如產品為非金屬等,在產品 與電,之間不存在放電的可能時,亦可藉由其中一個電極 Φ 而覆蓋曲面部的整個面。 (2) 第2實施形態中,第二電極25形成為細線狀, 但例如第二電極可跨越整個平坦部而形成為網狀,亦可形 成為將多個細線狀金屬箔並排的條紋狀。 /3)第1實施形態中’放電管2是設為具備外管部3 及内管部4的二重管構造,且第二電極9設置於内管部4 的内侧,但本發明並非限定於如此之情形。例如,如圖7 所示的準分子燈40般,亦可為如下構造,即,放電管41 35 201123261 設為與第2實施形制樣具有單管結構, ==收納於内管部中,而是直接以== 式配,放電管41的内側”戈者亦可為如下構造: 棒狀的第二電極上包覆有絕緣膜之後配置於放電 ⑷於第3實施形態中亦可為如下構造,即 非收納於内管部中,而直接無遮蔽地配置 於放電管的_。於此情形,最好的是,第二電極於 管中大致密著於平坦部的關面,但第二電極可配置於如 下巧的情形與第3實施形態的情形同樣,即於電極間施 加電壓時’在第二電極與輔助電極之間引起辅助放電,其 後在第二電極與第一電極之間引起主放電。 (5 )上述各實施形態巾,任—平坦部與曲面部的連接 部分均為具有曲率而f曲的面,但亦可成為局部性經由平 坦的面而連接的形狀。 (6)第3實施形態中,平坦部35被設為可使光透過 的出射面’但例如若使第-電極37形成為網狀、細線狀等 可使光透過的形狀’亦可自曲面部側射出光。 另外,上述實施例是就準分子燈之情形加以說明,但 本發明並不限找準分子燈讀形,村為核燈等準分 子燈以外的紫外線燈。 本申請案是基於2005年7月29曰所申請的曰本專利 申請案(特願2005-221143)及2006年2月8曰所申請 的曰本專利申請案(特願2006 —031051),該些内容以^ 36 201123261 考的形式而倂入本申請案中。 【圖式簡單說明】 圖1是第1實施形態的準分子燈的側剖面圖。 圖2是第1實施形態的準分子燈的剖面圖。 圖3是第2實施形態的準分子燈的剖面圖。 圖4是第3實施形態的準分子燈的刳面圖。 圖5是表示第3實施形態的準分子燈中在平坦部的内 侧面上引起輔助放電的情形之剖面圖。 圖6是表示第3實施形態的準分子燈中,除辅助放電 以外在第一電極與第二電極之間引起主放電的情形之剖面 圖。 圖7是其他實施形態的準分子燈的剖面圖。 圖8是收納有先前的準分子燈的燈箱的剖面圖。 圖9是本發明的紫外線燈的放電管之一例的剖面圖。 圖10是本發明的紫外線燈的放電管之一例的剖面圖。 圖11是表示本發明的紫外線燈的放電管之侧部的圖。 圖12是具備圓筒形放電管的比較例中的紫外線燈的 剖面圖。 圖13是表示本發明之第六發明中「平坦部的中心部附 近」的圖。 圖14是表示本發明之第十發明中「平坦部的中心部附 近」的圖。 【主要元件符號說明】 1、20、30、40 :準分子燈 37 201123261 2、 21、3卜41 :放電管 3、 32 :外管部 4、 33 :内管部 5、 22、34、205 :曲面部 5A、34A :角部分 6、 23、35、202、204 :平坦部 6A :側端緣 7、 36 :放電空間 8、 24、37 :第一電極 8A :端緣部 9、 25、38、42 :第二電極 10、 11 :導線 12 :交流電源裝置 39 :輔助電極 100 :燈 101 :反射板 102 :用於射出紫外線的窗部 103 :燈箱 201 ··用於透過紫外線的平坦部 203 :圓弧狀部 206 :紫外線反射構件 207 :圓筒形放電管 A、W3、W4 :點 B :底點 38 201123261 HC、WL :直線 La、Lb :距離 S卜S2 :側部 T :頂點 W :產品 Wl、W2 :交點 WC :中心點Electric 'pole|^== gas pressure and increase in the case of applying voltage mosquitoes - 檨H has a roughly _ effect). However, in the present embodiment, the charged particles or metastable generated by the atomic auxiliary discharge in the state cause the main discharge L and even the photons to be supplied into the main discharge space, so that the ionization coefficient of the discharge gas existing in the crucible may be used. increase. When the voltage is applied between the applied voltages, the discharge is green, so that it is not necessary to increase the voltage to ensure the stability of the discharge. 30 201123261 2 The ultraviolet rays that are emitted by the discharge (indicated by the dotted arrows in the figure) are irradiated toward the product W directly through the mesh of the flat portion % auxiliary electrode 39. On the other hand, the ultraviolet rays which are advanced in the direction of the curved surface 34 are reflected by the first electrode 37, and the side of the crotch portion 35 is emitted toward the product w. As described above, according to the present embodiment, it is possible to reduce the discharge stability at the time of starting the lighting of the lamp. Further, it is more preferable that the second electrode 38 is located between the first electrode 37 and the auxiliary electrode 39 and is close to the auxiliary electrode 39. Preferably, the inner tube portion of the second electrode 38 is housed as in the present embodiment. 33 is substantially adhered to the inner wall surface of the flat portion 35. However, the second electrode 38 does not have to be disposed as described above. When the first electrode 38 is disposed at a position where a voltage is applied, an auxiliary discharge is caused between the second electrode 38 and the auxiliary electrode 39, and then a main discharge is caused between the first electrode 37 and the second electrode 38. Then it can achieve the purpose of the invention. In other words, the method of causing the discharge between the second electrode 38 and the auxiliary electrode 39 to be caused between the first electrode 37 and the second electrode 38 is more effective, and the second electrode 38 can be disposed as follows. In the position, that is, the shortest distance between the first electrode 37 and the second electrode 38 is La, and when the shortest distance between the electrode 39 and the second electrode 38 is Lb, the relationship of La &gt; Lb is satisfied. In the present embodiment, as in the first embodiment, the flat portion 35 is a surface for light transmission and a surface on the exit surface is flat. Therefore, 31 201123261 The distance between the entire exit surface and the product w is equal, so that even in the atmosphere, the ultraviolet light can be minimized by the loss of oxygen. Further, the entire surface of the product W can be uniformly irradiated. Further, since the first electrode 37 is formed of a material that can reflect ultraviolet rays, the first electrode 37 reflects and diffuses the ultraviolet rays emitted toward the curved surface portion 34 side. The role of the reflector on the flat portion % side (the exit surface side). Then, the auxiliary electrode 39 provided on the flat portion 35 is formed in a mesh shape so as not to block the emitted light. According to the configuration of the first embodiment, the ultraviolet ray is concentrated on the emission surface side without separately providing a reflector, so that the irradiation efficiency can be improved with a simple configuration. Further, the third embodiment has the following structure, that is, The invention of the invention, the second invention, the third invention, the fourth invention, the fifth invention, the sixth invention, the seventh invention, the eighth invention, the tenth invention, and the invention disclosed in the "Disclosure of the Invention" Twelfth invention. Therefore, the effects disclosed in the "disclosure of the invention" as an effect obtained by the inventions are obtained in the third embodiment. EXAMPLES Example of Confirming Irradiation Efficiency of Ultraviolet Light 1. Production of Lamp C Example 1&gt; An excimer lamp having the same structure as that of the first embodiment was produced. Aluminum is vapor-deposited on the tubular tube having the same shape as that of the outer tube portion 3 of the first embodiment so as to substantially cover the outer side of the curved portion. In addition, the cylindrical tube is made of σ-formed quartz (SUp_F31〇 manufactured by Shin-Etsu Co., Ltd.), ^ 201123261 half = Γ 6 sub-job, the curvature of the outer peripheral surface of the curved surface (4) and the flat portion of the flat (four) _ the outer peripheral surface of the arc The curvature nucleus is 5 mm. The electric current is about 4 faces and the wall thickness is about. .8mm synthetic stone; the internal insertion has a diameter of about! Mm nickel wire. In the electron tube ^^ = put = until, the outline is as follows: C # t Μ 二 U * pressure electrode, and the entire Sir of the high frequency voltage tube of 3 G kHz is applied to discharge it. The discharge-ground was generated in the electron &lt;Comparative Example 1&gt; On the other hand, for comparison, a conventional lamp having a double tube structure was produced. A web electrode (opening ratio) was formed by the side of the outer peripheral surface of the outer tube having an outer diameter of 32 mm. The inner σρ of the electronic organ is provided with the same synthetic quartz tube as that of the above embodiment, and the recording line is inserted into the inside thereof. The gas is sealed in the electron tube as a discharge gas until the "g" is turned into a ground electrode, and the recording line is called a surface pressure electrode', and a high-frequency voltage of 30 kHz (peak voltage of 8 kV) is applied thereto. 2. Discharge. 2. Lighting test in the atmosphere without using an illuminating device. The lamp of the embodiment and the comparative example was scanned in the horizontal direction at a speed of 3 m/min using a uv sensor at a position 3 mm directly below the lamp. As a result of the comparison of the cumulative amount of light, the lamp of the example was approximately three times as large as the lamp of the comparative example, and it was confirmed that the ultraviolet ray can be efficiently irradiated onto the object to be irradiated. 33 201123261 [Example of confirming the effect of the auxiliary electrode] &lt;Example 2&gt; An excimer lamp having the same structure as that of the third embodiment was produced. A nickel film (outer electrode) having a length of 1000 mm and a thickness of 0.2 mm was fixed to the outer tube portion 32 of the third embodiment. The tubular tube of the same shape covers the outer surface of the curved surface portion. The tubular tube is made of synthetic quartz (SUPRASIL_F31〇 manufactured by Shin-Etsu Co., Ltd.) with a wall thickness of 2 mm and a length of the tube. 1100 mm, the radius of curvature of the outer peripheral surface of the curved surface portion is 16 mm, and the radius of curvature of the outer peripheral surface of the arc portion of the curved portion where the curved surface portion and the flat portion are joined is 5 mm. The inner portion of the electron tube is arranged with an outer diameter of about 5 Mm, synthetic quartz tube with an inner diameter of about 2 mm, and a nickel wire with a diameter of about 18 mm inserted inside the quartz tube (the inner electrode and the width of the tubular tube are fixed at 22 coffee, length a sus mesh plate (auxiliary electrode) of G.2 mm thick.,: It is made to cover the flat surface of the flat (four) outer surface. From the central axis to the fixed surface of the tang, __ is ^^ in the electron tube Sealed into a chaotic gas as a discharge gas until the stone, the recording film and the mesh plate are used as the grounding electrode, and the roughly rectangular high-light electrode is applied to the old one. If the electric bunker is gradually increased, the peak is discharged. Auxiliary discharge is generated on the inner wall surface of the stalk, and the flat side electrode (recording line)-outer side electrode when the hair is at 2kV (the film is j5.5kV), the main discharge does not hinder the auxiliary discharge 曰 main discharge. Minimum applied electricity (four) 5.5 kv. In the case of comparison, 34 201123261 was produced by testing the same lamp as in Example 2 except that no mesh plate (auxiliary electrode) was used, and if no voltage of about 1 〇 kV was applied, In the lamp provided with the auxiliary electrode, the main discharge can be generated with a voltage applied to about one-half of the lamp in which the auxiliary electrode is not provided. Further, in the lamp of the second embodiment, When the peak voltage after the start of lighting is fixed to 5.5 kV and the discharge stability is investigated, spark-like discharge or uneven discharge is not generated, and stable discharge can be achieved after starting lighting. On the other hand, when the same experiment was carried out in a lamp in which the auxiliary electrode was not provided, a spark was generated and uneven discharge occurred. &lt;Other Embodiments&gt; The technical scope of the present invention is not limited to the above-described embodiments, and for example, the following disclosure is also included in the technical scope of the present invention. (1) In the above embodiments, the first electrode 8 and the edge of the flat portion 6 are provided with a gap therebetween. However, for example, the product is non-metal or the like, and there is no possibility of discharge between the product and the electric power. The entire surface of the curved portion can also be covered by one of the electrodes Φ. (2) In the second embodiment, the second electrode 25 is formed in a thin line shape. For example, the second electrode may be formed in a mesh shape across the entire flat portion, or may be formed in a stripe shape in which a plurality of thin metal foils are arranged side by side. /3) In the first embodiment, the discharge tube 2 is a double tube structure including the outer tube portion 3 and the inner tube portion 4, and the second electrode 9 is provided inside the inner tube portion 4, but the present invention is not limited thereto. In such a situation. For example, as in the excimer lamp 40 shown in FIG. 7, the discharge tube 41 35 201123261 is configured to have a single tube structure with the second embodiment, and == is housed in the inner tube portion, and In the third embodiment, the rod-shaped second electrode is coated with an insulating film and then placed in the discharge (4). In the third embodiment, the following structure may be used. That is, it is not stored in the inner tube portion, but is disposed directly in the discharge tube without shielding. In this case, it is preferable that the second electrode is substantially close to the flat surface of the flat portion in the tube, but the second The electrode can be disposed as follows in the case of the third embodiment, that is, when a voltage is applied between the electrodes, 'an auxiliary discharge is caused between the second electrode and the auxiliary electrode, and thereafter between the second electrode and the first electrode. (5) In the above-described embodiments, the connection portion between the flat portion and the curved surface portion is a surface having curvature and f-curve, but may be locally connected via a flat surface. In the third embodiment, the flat portion 35 is set to allow light However, in the case where the first electrode 37 is formed into a mesh shape or a thin line shape, for example, a shape in which light can be transmitted can be emitted from the curved surface side, the above embodiment can be used in the case of an excimer lamp. However, the present invention is not limited to finding an excimer lamp reading type, and the village is an ultraviolet lamp other than an excimer lamp such as a nuclear lamp. The present application is based on a patent application filed on July 29, 2005 (the special wish) 2005-221143) and the patent application filed on February 8th, 2006 (Special Wish 2006-031051), these contents are incorporated into this application in the form of ^ 36 201123261. [Simplified illustration Fig. 1 is a side cross-sectional view of the excimer lamp of the first embodiment. Fig. 2 is a cross-sectional view of the excimer lamp of the first embodiment. Fig. 3 is a cross-sectional view of the excimer lamp of the second embodiment. Fig. 5 is a cross-sectional view showing a state in which an auxiliary discharge is caused on the inner surface of the flat portion in the excimer lamp of the third embodiment. Fig. 6 is a cross-sectional view showing the third embodiment. In the excimer lamp, in addition to the auxiliary discharge at the first electrode Fig. 7 is a cross-sectional view of an excimer lamp according to another embodiment. Fig. 8 is a cross-sectional view of a light box in which a prior excimer lamp is housed. Fig. 9 is a view of the present invention. Fig. 10 is a cross-sectional view showing an example of a discharge tube of the ultraviolet lamp of the present invention. Fig. 11 is a view showing a side portion of a discharge tube of the ultraviolet lamp of the present invention. A cross-sectional view of the ultraviolet lamp in the comparative example of the cylindrical discharge tube. Fig. 13 is a view showing "the vicinity of the center portion of the flat portion" in the sixth invention of the present invention. Fig. 14 is a view showing "the vicinity of the center portion of the flat portion" in the tenth invention of the present invention. [Description of main component symbols] 1, 20, 30, 40: excimer lamp 37 201123261 2, 21, 3b 41: discharge tube 3, 32: outer tube portion 4, 33: inner tube portion 5, 22, 34, 205 : curved surface portions 5A, 34A: corner portions 6, 23, 35, 202, 204: flat portion 6A: side end edges 7, 36: discharge spaces 8, 24, 37: first electrode 8A: end edge portions 9, 25, 38, 42: second electrode 10, 11: lead 12: AC power supply device 39: auxiliary electrode 100: lamp 101: reflector 102: window portion 103 for emitting ultraviolet rays: light box 201 · flat portion for transmitting ultraviolet rays 203: arc-shaped portion 206: ultraviolet reflecting member 207: cylindrical discharge tube A, W3, W4: point B: bottom point 38 201123261 HC, WL: straight line La, Lb: distance S Bu S2: side portion T: vertex W : Product Wl, W2: intersection WC: center point

Claims (1)

201123261 七、申請專利範圍: 1·一種紫外線燈,包括形成為筒狀的放電管,其特徵 在於, 於上述放電管的外周壁上,在相互對向的位置上包括 曲面部以及用於透過紫外線的平坦部, 上述曲面部是藉由使上述放電管的内部侧之面呈凹面 的方式而形成的, 於上述曲面部上設置有第一電極, 於上述放電管的外部,設置有延伸於上述放電管長度 方向的線狀第二電極, 上述第二電極設置於上述平坦部的中心部附近, 在上述第-電極與上述第二電極之間產生主放電,並 且 部上,未設置除上述第二電極以外的電極。 2.如申請專利範圍第1項所述之料線燈,其中, 於上述曲面部上設置有紫外線反射構件,、 放電牛形成為沿上述曲面部且較自上述 ίί:其中-個側部至另-個側部為止的整個範圍更 於垂直於上述放電營4i 上,上述紫外線反射構件的“線=述紫外線燈的剖面 中-個侧部更下側的部分的點、、面中’在較上述其 面的切平面且朝向上述放雷技’垂直於上述紫外線反射 一個側部朝向上述另-個側;下較自上述其中 201123261 3. 如申請專利範圍第1項所述之紫外線燈,其中, 上述曲面部上設置有紫外線反射構件, 上述紫外線反射構件形成為沿著上述曲面部且較自上 述放電管的其中一個側部至另一個側部為止的整個範圍更 寬,並且 上述紫外線反射構件是用以產生主放電的第一電極, 該主放電用以產生紫外線。 4. 如申請專利範圍第丨項所述之紫外線燈,其中,上 述放電管的材質為石英玻璃。 5.如申請專利範圍第1項所述之料線燈,其中, 於上述曲面部的外表面設置有第^201123261 VII. Patent application scope: 1. An ultraviolet lamp comprising a discharge tube formed in a cylindrical shape, characterized in that the outer peripheral wall of the discharge tube includes a curved surface portion at a position opposite to each other and is used for transmitting ultraviolet rays. The flat portion is formed by forming a surface of the inner surface of the discharge tube to be concave, wherein the curved surface portion is provided with a first electrode, and the outer surface of the discharge tube is provided with an extension a linear second electrode in the longitudinal direction of the discharge tube, wherein the second electrode is provided in the vicinity of the center portion of the flat portion, and a main discharge is generated between the first electrode and the second electrode, and the portion is not provided An electrode other than the two electrodes. 2. The wire lamp according to claim 1, wherein the curved surface portion is provided with an ultraviolet reflecting member, and the discharge cattle are formed along the curved surface portion and from the side of the above-mentioned ίί: The entire range from the other side is more perpendicular to the discharge camp 4i, and the line of the ultraviolet reflecting member is a point of the portion of the cross section of the ultraviolet lamp that is lower than the side portion, and the surface is in the The ultraviolet light lamp of the first aspect of the invention is directed to the above-mentioned other side from the tangential plane of the above-mentioned light-receiving technique and perpendicular to the ultraviolet ray. The curved surface portion is provided with an ultraviolet reflecting member, and the ultraviolet reflecting member is formed to be wider along the curved surface portion and from the one side portion to the other side portion of the discharge tube, and the ultraviolet reflection is The member is a first electrode for generating a main discharge, and the main discharge is used to generate ultraviolet rays. 4. The ultraviolet lamp according to the above-mentioned claim, wherein The material of the discharge tube is a quartz glass. The wire lamp according to claim 1, wherein the outer surface of the curved surface portion is provided with a ^ ttl1!專利範圍第1項所述之紫外線燈,其中, 述紫外線燈為準分子燈。The ultraviolet lamp of the first aspect of the invention, wherein the ultraviolet lamp is an excimer lamp. ’其使用如申請 項中任-項所述之紫外線燈。 41'Using the ultraviolet lamp as described in any of the items in the application. 41
TW099144047A 2005-07-29 2006-07-28 Ultraviolet lamp and ultraviolet irradiating device TWI366858B (en)

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