TWI594290B - Short arc discharge lamp - Google Patents

Short arc discharge lamp Download PDF

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Publication number
TWI594290B
TWI594290B TW103107424A TW103107424A TWI594290B TW I594290 B TWI594290 B TW I594290B TW 103107424 A TW103107424 A TW 103107424A TW 103107424 A TW103107424 A TW 103107424A TW I594290 B TWI594290 B TW I594290B
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cathode
tungsten
aspect ratio
body portion
end portion
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TW103107424A
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Chinese (zh)
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TW201503218A (en
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Hirohisa Iwabayashi
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Ushio Electric Inc
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    • 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
    • H01J61/0675Main electrodes for low-pressure discharge lamps characterised by the material of the electrode
    • H01J61/0677Main electrodes for low-pressure discharge lamps characterised by the material of the electrode characterised by the electron emissive material
    • 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
    • H01J61/073Main electrodes for high-pressure discharge lamps
    • H01J61/0735Main electrodes for high-pressure discharge lamps characterised by the material of the electrode
    • H01J61/0737Main electrodes for high-pressure discharge lamps characterised by the material of the electrode characterised by the electron emissive material
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/02Details
    • H01J61/54Igniting arrangements, e.g. promoting ionisation for starting
    • H01J61/541Igniting arrangements, e.g. promoting ionisation for starting using a bimetal switch
    • H01J61/544Igniting arrangements, e.g. promoting ionisation for starting using a bimetal switch and an auxiliary electrode outside the vessel
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/84Lamps with discharge constricted by high pressure
    • H01J61/86Lamps with discharge constricted by high pressure with discharge additionally constricted by close spacing of electrodes, e.g. for optical projection
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00Gas-discharge or vapour-discharge lamps
    • H01J61/98Lamps with closely spaced electrodes heated to incandescence by light-emitting discharge, e.g. tungsten arc lamp

Description

短弧型放電燈 Short arc discharge lamp

本發明係關於短弧型放電燈者,尤其,關於陰極含有用以有良好之電子放射的射極物質的短弧型放電燈者。 The present invention relates to short arc type discharge lamps, and more particularly to short arc type discharge lamps having a cathode material for good electron emission.

一般來說,在作為放映機用的光源所使用之封入氙的短弧型放電燈、作為半導體曝光、LCD曝光用等的光源所使用之封入水銀的短弧型放電燈中,其陰極為了擔任定常點燈時時常放出電子的作用,應使電子放射容易進行,而於高熔點金屬含有電子放射物質所構成。 In general, a short arc type discharge lamp enclosed in a crucible used as a light source for a projector, and a short arc type discharge lamp in which mercury is enclosed as a light source for semiconductor exposure or LCD exposure, the cathode is used for the purpose of being a constant When lighting, the electrons are often released, so that the electron emission is easy to carry out, and the high melting point metal contains the electron emitting material.

然後,作為該電子放射物質,於要求點光源及高亮度的短弧型放電燈中,作為可提高陰極前端的動作溫度者,一般使用釷。 Then, as the electron emissive material, in a short-arc discharge lamp that requires a point light source and a high-intensity, it is generally used as a temperature at which the operating temperature of the cathode tip can be increased.

然而,因釷是放射性物質,近年來,逐漸被嚴格規制,被要求替代材料的變更。 However, since it is a radioactive substance, it has been gradually regulated in recent years and is required to replace the material.

作為代替該釷的替代物質,提案有使用稀土族元素及其化合物者。稀土族元素是工作函數(一般來說,指電子從物質表面往外面飛出時所需的能量)較低且 具有優良電子放射的物質,被期待作為釷的替代物質。 As an alternative to the ruthenium, it is proposed to use a rare earth element and a compound thereof. The rare earth element is a work function (generally, the energy required for electrons to fly out from the surface of the material) is low and A substance with excellent electron emission is expected to be a substitute for strontium.

於日本特開2006-286236號公報(專利文獻1),揭示有於身為陰極材料的鎢,作為射極物質,附加地含有氧化鑭(La2O3)的短弧型放電燈。 Japanese Laid-Open Patent Publication No. 2006-286236 (Patent Document 1) discloses a short arc type discharge lamp which contains tungsten as a cathode material and additionally contains lanthanum oxide (La 2 O 3 ) as an emitter material.

然而,如氧化鑭(La2O3)的稀土族氧化物,係蒸氣壓高於氧化釷(ThO2),故比較容易蒸發。因此,作為於陰極含有的射極物質,使用稀土族氧化物來代替氧化釷時,會發生該稀土族氧化物過度蒸發,導致早期枯竭之事態。有因該射極物質的枯竭,喪失陰極之電子放射功能,產生閃爍而燈管壽命變短的問題。 However, a rare earth oxide such as lanthanum oxide (La 2 O 3 ) has a vapor pressure higher than that of cerium oxide (ThO 2 ), so that it is relatively easy to evaporate. Therefore, when a rare earth oxide is used instead of cerium oxide as an emitter material contained in the cathode, excessive evaporation of the rare earth oxide occurs, leading to an early exhaustion. There is a problem that the electron emission function of the cathode is lost due to the depletion of the emitter material, and flicker is generated and the life of the lamp is shortened.

尤其,需要高溫動作的陰極,亦即,在電流密度較高之90A/mm2以上之陰極的狀況中比較明顯。因為超過該電流密度時,陰極前端的溫度會接近熔點,身為電極材料的鎢的蒸發會變得明顯。 In particular, a cathode that requires a high temperature operation, that is, a cathode having a current density of 90 A/mm 2 or more is more conspicuous. Since the temperature at the front end of the cathode is close to the melting point when the current density is exceeded, the evaporation of tungsten as an electrode material becomes conspicuous.

[先前技術文獻] [Previous Technical Literature] [專利文獻] [Patent Literature]

[專利文獻1]日本特開2006-286236號公報 [Patent Document 1] Japanese Patent Laid-Open Publication No. 2006-286236

本發明係有鑑於前述先前技術的問題點,提供於發光管的內部,對向配置陰極與陽極的短弧型放電燈中,即使於陰極作為射極,添加稀土族氧化物,也可防止該射極的早期的枯竭,長時間維持電子放出功能,可謀求 燈管之閃爍壽命的長期化的構造者。 The present invention is directed to the short-arc discharge lamp in which the cathode and the anode are disposed opposite to each other in the interior of the arc tube, and even if the rare earth oxide is added to the cathode as the emitter, the present invention can be prevented. The early exhaustion of the emitter and the electronic release function for a long time can be sought A long-term constructor of the flashing life of the lamp.

為了解決前述課題,在本發明中,特徵為:前述陰極由本體部與被接合於其前端側之前端部所成;前述本體部由作為射極而添加稀土族氧化物的鎢所成;前述前端部由純鎢所成,並且前述本體部之鎢粒子的長寬比,比前述前端部之鎢粒子的長寬比還大。 In order to solve the above problems, the present invention is characterized in that the cathode is formed by a main body portion and a front end portion joined to the front end side thereof, and the main body portion is made of tungsten to which a rare earth oxide is added as an emitter; The front end portion is made of pure tungsten, and the aspect ratio of the tungsten particles in the main body portion is larger than the aspect ratio of the tungsten particles in the front end portion.

又,特徵為:前述本體部之鎢粒子的長寬比為3~30;前述前端部之鎢粒子的長寬比未滿3。 Further, it is characterized in that the aspect ratio of the tungsten particles in the main body portion is 3 to 30; and the aspect ratio of the tungsten particles in the front end portion is less than 3.

又,特徵為:前述稀土族氧化物,係包含氧化鑭、氧化鈰及氧化釓之任一。 Further, the rare earth oxide is characterized in that it contains any of cerium oxide, cerium oxide and cerium oxide.

依據本發明,於作為射極物質,添加稀土族氧化物之本體部的前端,接合由純鎢所成之前端部,前述本體部之鎢粒子的長寬比,比前述前端部之鎢粒子的長寬比還大,藉此,因為本體部的鎢粒子於電極軸方向比較長,所以,射極接觸鎢粒子的面積變大。 According to the invention, the front end of the main body portion to which the rare earth oxide is added as the emitter material is joined to the front end portion formed of pure tungsten, and the aspect ratio of the tungsten particles in the main body portion is larger than that of the tungsten particles at the front end portion Since the aspect ratio is also large, since the tungsten particles in the main body portion are relatively long in the direction of the electrode axis, the area in which the emitter contacts the tungsten particles becomes large.

燈管點燈中,於鎢固熔稀土族氧化物中的氧的話,相關之稀土族氧化物之稀土族金屬的氧化價數變小,容易熔融。結果,稀土族氧化物容易擴散粒界。具體來說,氧化鑭之狀況中,會喪失氧,從La2O3變成LaOxIn the lamp lighting, in the tungsten solid-melting rare earth oxide, the rare earth metal of the related rare earth oxide has a small oxidation number and is easily melted. As a result, the rare earth oxides easily diffuse the grain boundaries. Specifically, in the case of cerium oxide, oxygen is lost and La 2 O 3 is changed to LaO x .

然後,於本體部中,因為鎢的粒界往電極軸 方向延伸,擴散路徑是沿著軸的直線狀,故容易擴散。 Then, in the body portion, because the grain boundary of tungsten is toward the electrode axis The direction is extended, and the diffusion path is linear along the axis, so it is easy to spread.

如此,擴散於本體部的射極,係到達前端部時,因其前端部的溫度較高,擴散速度變快,但是,於該前端部中,鎢粒子的長寬比相較於本體部,比較小,擴散不會極度進行,會幾乎合適於本體部之射極的供給狀態,而往前端移動。 As described above, when the emitter that has diffused in the main body portion reaches the tip end portion, the temperature of the tip end portion is high, and the diffusion speed is increased. However, in the tip end portion, the aspect ratio of the tungsten particles is larger than that of the body portion. It is relatively small, and the diffusion does not proceed extremely, and it is almost suitable for the supply state of the emitter of the body portion, and moves toward the front end.

結果,於本體部中,射極會迅速擴散,於前端部中,射極的擴散速度變慢,抑制射極早期枯竭之狀況,所以,可抑制早期損耗,取得獲得較長之使用壽命的陰極。 As a result, in the main body portion, the emitter rapidly diffuses, and in the tip end portion, the diffusion speed of the emitter is slowed, and the state in which the emitter is depleted early is suppressed. Therefore, the early loss can be suppressed, and the cathode having a long service life can be obtained. .

又,本體部之鎢粒子的長寬比為3~30,前端部之鎢粒子的長寬比未滿3,因此,容易從溫度較低的下部發生身為射極的La的擴散,在溫度較高的前端部分中,擴散速度被制約,可抑制不必要的蒸發。又,因射極存在於鎢的粒界,藉由所謂固著效果,抑制粒成長,進行穩定之射極的供給。 Further, the aspect ratio of the tungsten particles in the main portion is 3 to 30, and the aspect ratio of the tungsten particles at the tip end portion is less than 3, so that it is easy to diffuse La which is an emitter from a lower portion of the temperature, at a temperature. In the higher front end portion, the diffusion speed is restricted, and unnecessary evaporation can be suppressed. Further, since the emitter is present at the grain boundary of tungsten, the so-called anchoring effect suppresses grain growth and supplies a stable emitter.

進而,因為作為射極的稀土族氧化物具備氧化鑭、氧化鈰及氧化釓之任一,在燈管動作中,於本體部中產生稀土族氧化物的熔融,圓滑地進行朝向前端側的擴散,可獲得具有良好電子放射特性的陰極。 Further, since the rare earth group oxide as the emitter includes any of cerium oxide, cerium oxide, and cerium oxide, the rare earth oxide is melted in the main portion during the operation of the lamp, and the diffusion toward the tip end is smoothly performed. A cathode having good electron emission characteristics can be obtained.

1‧‧‧短弧型放電燈 1‧‧‧Short arc discharge lamp

2‧‧‧發光管 2‧‧‧Light tube

3‧‧‧陰極 3‧‧‧ cathode

4‧‧‧陽極 4‧‧‧Anode

5‧‧‧射極 5‧‧‧射极

31‧‧‧本體部 31‧‧‧ Body Department

32‧‧‧前端部 32‧‧‧ front end

[圖1]具有本發明相關陰極構造之短弧型放電燈的整體圖。 Fig. 1 is an overall view of a short arc type discharge lamp having a cathode structure according to the present invention.

[圖2]表示本發明之一實施例的陰極構造圖。 Fig. 2 is a view showing a cathode structure of an embodiment of the present invention.

[圖3]圖2之A部的放大剖面圖。 Fig. 3 is an enlarged cross-sectional view showing a portion A of Fig. 2;

[圖4]圖2之射極擴散作用圖。 [Fig. 4] The emitter diffusion diagram of Fig. 2.

[圖5]說明長寬比的測定方法之一例的圖。 Fig. 5 is a view showing an example of a method of measuring an aspect ratio.

[圖6]表示本發明之效果的圖表。 Fig. 6 is a graph showing the effects of the present invention.

圖1係揭示具有本發明之陰極構造的短弧型放電燈的整體構造,短弧型放電燈1係於發光管2的內部,對向配置陰極3與陽極4。 Fig. 1 is a view showing the overall structure of a short arc type discharge lamp having a cathode structure of the present invention. The short arc type discharge lamp 1 is disposed inside the arc tube 2, and the cathode 3 and the anode 4 are disposed opposite to each other.

如圖2所示,陰極3係由本體部31與被接合於其前端之前端部32所成。前述本體部31係由鎢所成,作為射極物質,添加氧化鑭(La2O3)等的稀土族氧化物。 As shown in Fig. 2, the cathode 3 is formed by the body portion 31 and the end portion 32 before being joined to the front end thereof. The main body portion 31 is made of tungsten, and a rare earth oxide such as lanthanum oxide (La 2 O 3 ) is added as an emitter material.

前述前端部32係藉由固相接合等的手段,被接合於前述本體部31的前端,亦即,與陽極4對向之面。然後,該前端部32係由不包含射極物質的純鎢所成,理想來說,由4N以上的純鎢所成。 The distal end portion 32 is joined to the distal end of the main body portion 31 by means of solid phase bonding or the like, that is, the surface facing the anode 4. Then, the front end portion 32 is made of pure tungsten which does not contain an emitter material, and is preferably made of pure tungsten of 4N or more.

但是,如圖3所示,前述本體部31之鎢粒子的長寬比,比前端部32之鎢粒子的長寬比還大。該長寬比係表示晶粒粒子之長度與寬度的關係的指標,在長寬比較大時,表示軸方向之長度的比例較大。 However, as shown in FIG. 3, the aspect ratio of the tungsten particles of the main body portion 31 is larger than the aspect ratio of the tungsten particles of the distal end portion 32. This aspect ratio is an index indicating the relationship between the length and the width of the crystal grain, and when the length and the width are relatively large, the ratio indicating the length in the axial direction is large.

藉由具有此種陰極構造,可獲得以下的作用、效果。 By having such a cathode structure, the following actions and effects can be obtained.

如圖4所示,因燈管點燈中,陰極變熱,作為包含於 本體部31之射極物質5的稀土族氧化物中的氧會固溶於鎢,稀土族氧化物還原而產生氧化價數更小的氧化物。如此,因為熔點降低,在鎢粒子內產生熔融,主要透過粒子間的粒界,在陰極本體部31內擴散。射極係遵從溫度梯度,越向陰極前端側則擴散速度越快,在前端部32中,鎢粒子的長寬比比本體部31小,移動路徑未沿著軸方向形成,故難以朝向陰極前端移動。 As shown in Fig. 4, the cathode is heated due to the lamp lighting, as included in Oxygen in the rare earth oxide of the emitter 5 of the main body portion 31 is solid-solubilized in tungsten, and the rare earth oxide is reduced to produce an oxide having a smaller oxidation number. As described above, since the melting point is lowered, melting occurs in the tungsten particles, and the grain boundary between the particles is mainly transmitted through the cathode body portion 31. The emitter follows the temperature gradient, and the diffusion speed increases toward the front end side of the cathode. In the distal end portion 32, the aspect ratio of the tungsten particles is smaller than that of the main body portion 31, and the moving path is not formed along the axial direction, so that it is difficult to move toward the front end of the cathode. .

如此,配合燈管點燈時之陰極前端的溫度梯度,鎢粒子的組織形態(金屬相),在本體部31中,具備雖然射極5的移動速度較慢,但延伸於易於往前端部32側移動之軸方向的組織構造,在該前端部32中,雖然射極的移動速度較快,但是,前端具有難以馬上移動的組織構造,所以,關於存在於本體部31的射極,可往陰極的前端部側迅速擴散(移動),可消除供給中斷的問題,關於往前端部32移動的射極,可抑制軸方向的移動速度過度變快,且可抑制早期枯竭。 In this manner, in accordance with the temperature gradient of the tip end of the cathode when the lamp is turned on, the structure (metal phase) of the tungsten particles is provided in the main body portion 31 so that the moving speed of the emitter 5 is slow, but it is easy to extend to the front end portion. In the distal end portion 32, although the moving speed of the emitter is fast, the tip end has a structure in which it is difficult to move immediately. Therefore, the emitter existing in the main body portion 31 can be used. The tip end portion of the cathode is rapidly diffused (moved), and the problem of interruption in supply can be eliminated. The emitter moving toward the distal end portion 32 can suppress the excessively rapid moving speed in the axial direction and can suppress early depletion.

接下來,一邊參照圖5,一邊說明鎢(W)粒子之長寬比的測定方法之一例。 Next, an example of a method of measuring the aspect ratio of tungsten (W) particles will be described with reference to FIG. 5.

在此,說明鎢切斷法所致之測定方法。 Here, the measurement method by the tungsten cutting method will be described.

軸方向切斷陰極並對剖面進行研磨後蝕刻,藉由金屬顯微鏡,放大200倍程度來進行觀察時,在剖面中可看到被切斷之晶粒的形狀。依據JISH0501所記載的切斷法,於剖面的照片,畫上縱與橫直線,計算藉由各直線所完全切取的晶粒粒數,將其切段長度的平均值作為晶粒的長度 及寬度。 The cathode was cut in the axial direction, and the cross section was polished and etched, and when observed by a metal microscope at a magnification of 200 times, the shape of the cut crystal grains was observed in the cross section. According to the cutting method described in JISH0501, the longitudinal and horizontal straight lines are drawn on the photograph of the cross section, and the number of grain grains completely cut by each straight line is calculated, and the average value of the cut length is taken as the length of the crystal grain. And width.

參照圖5(A)(B)進行具體說明。於圖5(A)中,藉由直線A-A’所切斷之晶粒為5個,「平均之晶粒的長度」為(A1-A6的長度)/5。 The details will be described with reference to Fig. 5 (A) and (B). In Fig. 5(A), the number of crystal grains cut by the straight line A-A' is five, and the "average crystal grain length" is (the length of A1-A6)/5.

同樣地考察直線B-B’時,被切斷之晶粒為5個,「平均之晶粒的寬度」為(B1-B6的長度)/5。 Similarly, when the straight line B-B' is examined, five crystal grains are cut, and "the average crystal grain width" is (the length of B1-B6)/5.

於圖5(B)中,藉由直線A-A’所切斷之晶粒為1個,「平均之晶粒的長度」為(A1-A2的長度)/1。同樣地考察直線B-B’時,被切斷之晶粒為7個,「平均之晶粒的寬度」為(B1-B8的長度)/7。 In Fig. 5(B), one crystal grain is cut by the straight line A-A', and "the average length of the crystal grain" is (the length of A1-A2) / 1. Similarly, when the straight line B-B' is examined, the number of crystal grains to be cut is seven, and the "average grain width" is (length of B1 - B8) / 7.

分別於縱與橫,以等間隔拉出20條程度的直線,分別求出「平均之晶粒的長度或寬度」。關於縱方向,將20個程度所求出之「平均之晶粒的長度」的平均值,設為該區域之「晶粒的長度」。同樣地,關於橫方向,將20個程度所求出之「平均之晶粒的寬度的平均值」,設為該區域之「晶粒的寬度」。使用該「晶粒的長度與寬度」,求出鎢(W)粒子的長寬比。 In the vertical and horizontal directions, 20 straight lines are drawn at equal intervals, and the "average crystal grain length or width" is obtained. Regarding the longitudinal direction, the average value of the "average crystal grain length" obtained by 20 degrees is defined as the "die length" of the region. Similarly, in the horizontal direction, the "average value of the average grain width" obtained by 20 degrees is defined as the "width of the crystal grain" in the region. Using the "length and width of the crystal grains", the aspect ratio of the tungsten (W) particles was determined.

再者,在此,作為陰極3之鎢粒子的長寬比的理想的範圍,係於本體部31中為3~30,於前端部32中為未滿3。 Here, the ideal range of the aspect ratio of the tungsten particles as the cathode 3 is 3 to 30 in the main body portion 31 and less than 3 in the front end portion 32.

又,鎢粒子的長寬比,係藉由對鎢的鑄錠進行加熱,並對其往徑方向進行型鍛(swage)加工,鎢粒子成為往軸方向延伸的形狀,並藉由控制該程度來獲得最佳的長寬比。 Further, the aspect ratio of the tungsten particles is obtained by heating the ingot of tungsten and swaging it in the radial direction, and the tungsten particles are shaped to extend in the direction of the axis, and by controlling the degree To get the best aspect ratio.

<壽命試驗> <Life test>

依據以下的規格,將陰極前端部32的構造設為純鎢,製作於本體部31含有由稀土族氧化物所成之射極的多種陰極。 According to the following specifications, the structure of the cathode tip end portion 32 is made of pure tungsten, and the main body portion 31 is made of a plurality of kinds of cathodes including an emitter formed of a rare earth oxide.

陰極的前端部32係以混合長寬比未滿3之鎢粒子的純鎢所構成,其全長(厚度)設為2mm。 The tip end portion 32 of the cathode is made of pure tungsten in which tungsten particles having an aspect ratio of less than 3 are mixed, and the total length (thickness) thereof is set to 2 mm.

陰極的本體部31係鎢粒子的長寬比分別為1、2、3、5、10、20、25、30,於該鎢含有La2O3(2.5wt%)與ZrO2(0.07wt%)所構成。 The body portion 31 of the cathode has an aspect ratio of tungsten particles of 1, 2, 3, 5, 10, 20, 25, 30, respectively, and the tungsten contains La 2 O 3 (2.5 wt%) and ZrO 2 (0.07 wt%). ) constitutes.

接合各長寬比的本體部31與前端部32,來製作各種陰極,製作額定消費電力為2kW的超高壓水銀燈。 The main body portion 31 and the front end portion 32 of each aspect ratio are joined to produce various cathodes, and an ultrahigh pressure mercury lamp having a rated power consumption of 2 kW is produced.

針對不同陰極的規格所製作之超高壓水銀燈,進行壽命試驗,確認照度維持率‧閃爍的發生‧陰極損耗。再者,關於照度維持率,使燈管連續點燈,測定放射照度,設為維持率。 The ultra-high pressure mercury lamp produced for the specifications of different cathodes was subjected to a life test to confirm the illuminance maintenance rate ‧ the occurrence of flicker and the cathode loss. In addition, regarding the illuminance maintenance rate, the lamp was continuously turned on, and the illuminance was measured, and the maintenance rate was set.

於圖6揭示其結果。 The results are revealed in Figure 6.

圖6所示之「長寬比(1~30)」係揭示是陰極本體部31的長寬比。 The "aspect ratio (1 to 30)" shown in Fig. 6 reveals the aspect ratio of the cathode body portion 31.

前端部32的長寬比為未滿3,關於具有超過其之長寬比的燈管(長寬比5~30),即使超過1500小時,處理量也不會大幅掉落,可舒服地使用之基準的照度維持率為85%,可確認維持其照度維持率85%以上。 The aspect ratio of the front end portion 32 is less than three, and the lamp tube (length to width ratio 5 to 30) having an aspect ratio exceeding the length is not drastically dropped even if it exceeds 1500 hours, and can be used comfortably. The illuminance maintenance rate of the standard was 85%, and it was confirmed that the illuminance maintenance rate was maintained at 85% or more.

如以上說明般,依據本發明,陰極由本體部 與接合於其之前端部所成,前述本體部由包含由稀土族氧化物所成之射極的鎢所成,前述前端部由純鎢所成,並且將本體部之鎢粒子的長寬比,設為大於前端部之長寬比,藉此,可提供包含於本體部的射極不會早期枯竭,且可獲得具備較長之使用壽命的陰極的短弧型放電燈。 As described above, according to the present invention, the cathode is provided by the body portion And the front portion joined to the front portion thereof, the body portion is made of tungsten containing an emitter made of a rare earth oxide, the front end portion is made of pure tungsten, and the aspect ratio of the tungsten particles in the body portion is It is set to be larger than the aspect ratio of the front end portion, whereby a short arc type discharge lamp in which the emitter included in the main body portion is not depleted early and a cathode having a long service life can be obtained.

3‧‧‧陰極 3‧‧‧ cathode

5‧‧‧射極 5‧‧‧射极

31‧‧‧本體部 31‧‧‧ Body Department

32‧‧‧前端部 32‧‧‧ front end

Claims (3)

一種短弧型放電燈,係於發光管的內部對向配置陽極與陰極,前述陰極含有由稀土族氧化物所成之射極的短弧型放電燈,其特徵為:前述陰極,係由本體部,與被接合於該本體部的前端側之前端部所成;前述本體部,係由含有由稀土族氧化物所成之射極的鎢所成,並且前述前端部,係由純鎢所成;前述本體部之鎢粒子的長寬比,比前述前端部之鎢粒子的長寬比還大;前述鎢粒子的長邊方向沿著前述陰極的軸方向配置。 A short arc type discharge lamp is a short arc type discharge lamp in which an anode and a cathode are arranged opposite to each other in an inner portion of an arc tube, and the cathode includes an emitter formed by a rare earth oxide, and the cathode is a body The portion is formed by a front end portion joined to the front end side of the main body portion, and the main body portion is made of tungsten containing an emitter made of a rare earth oxide, and the front end portion is made of pure tungsten. The aspect ratio of the tungsten particles in the main body portion is larger than the aspect ratio of the tungsten particles at the tip end portion; and the longitudinal direction of the tungsten particles is arranged along the axial direction of the cathode. 如申請專利範圍第1項所記載之短弧型放電燈,其中,前述本體部之鎢粒子的長寬比為3~30;前述前端部之鎢粒子的長寬比未滿3。 The short arc type discharge lamp according to the first aspect of the invention, wherein the aspect ratio of the tungsten particles in the main body portion is 3 to 30; and the aspect ratio of the tungsten particles in the front end portion is less than 3. 如申請專利範圍第1項或第2項所記載之短弧型放電燈,其中,前述稀土族氧化物,係包含氧化鑭、氧化鈰及氧化釓之任一。 The short arc type discharge lamp according to the first or second aspect of the invention, wherein the rare earth oxide includes any of cerium oxide, cerium oxide and cerium oxide.
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TW200742494A (en) * 2005-12-27 2007-11-01 Harison Toshiba Lighting Corp Short arc type discharge lamp operating apparatus, ultraviolet irradiation apparatus and method of ultraviolet irradiating

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* Cited by examiner, † Cited by third party
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JP2009259790A (en) * 2008-03-26 2009-11-05 Harison Toshiba Lighting Corp High-pressure discharge lamp
JP5584093B2 (en) * 2010-11-05 2014-09-03 株式会社ユメックス Cathode for short arc discharge lamp and method for producing the same

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TW200742494A (en) * 2005-12-27 2007-11-01 Harison Toshiba Lighting Corp Short arc type discharge lamp operating apparatus, ultraviolet irradiation apparatus and method of ultraviolet irradiating

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