TW201013738A - Electrode for cold cathode fluorescent tube and cold cathode fluorescent tube using the same - Google Patents

Electrode for cold cathode fluorescent tube and cold cathode fluorescent tube using the same Download PDF

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TW201013738A
TW201013738A TW98131100A TW98131100A TW201013738A TW 201013738 A TW201013738 A TW 201013738A TW 98131100 A TW98131100 A TW 98131100A TW 98131100 A TW98131100 A TW 98131100A TW 201013738 A TW201013738 A TW 201013738A
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Taiwan
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cold cathode
tube
electrode
cathode fluorescent
fluorescent tube
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TW98131100A
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Chinese (zh)
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TWI451469B (en
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Hiroyuki Sano
Shinji Yamamoto
Hideo Murata
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Stanley Electric Co Ltd
Hitachi Metals Ltd
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Priority claimed from JP2009022840A external-priority patent/JP4934156B2/en
Priority claimed from JP2009192020A external-priority patent/JP4902706B2/en
Application filed by Stanley Electric Co Ltd, Hitachi Metals Ltd filed Critical Stanley Electric Co Ltd
Publication of TW201013738A publication Critical patent/TW201013738A/en
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Publication of TWI451469B publication Critical patent/TWI451469B/en

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Abstract

The present invention provides an electrode for a cold cathode fluorescent tube having excellent anti-sputter capability and workability and capable of reducing tube voltage, and a cold cathode fluorescent tube using the same. The cold cathode fluorescent tube (1) includes an electrode (3) for cold cathode fluorescent tube, which is made from an alloy composed of Mo, Fe of 0.1-30 mass percentage relative to the total amount and unavoidable impurities. Preferably, the above-mentioned alloy contains Mo of 0.1-10 mass percentage relative to the total amount and, more preferably, the alloy contains Mo of 0.1-5.5 mass percentage relative to the total amount and further contains Ru. In another embodiment, the above-mentioned alloy contains Nb of 0.1-10 mass percentage relative to the total amount.

Description

201013738 六、發明說明: 【發明所屬之技術領域】 本發明係關於一種冷陰極螢光管用電極以及使用該電 極的冷陰極螢光管。 【先前技術】 冷陰極螢光管作爲液晶顯示器的背光用光源等,得到 Φ 了廣泛的應用。冷陰極螢光管具有:細口徑的玻璃管和一 對冷陰極螢光管用電極,該玻璃管內部封入有Hg與Ar、 Ne等惰性氣體的同時,在內壁面塗敷有螢光體;前述一 對冷陰極螢光管用電極在管軸方向彼此相對向而被安裝在 該玻璃管內的兩端。藉由對一對冷陰極螢光管用電極間施 加高電壓,在冷陰極螢光管內產生電場,從非加熱狀態的 陰極(冷陰極)放射出電子。接著,因該電子與Hg原子 產生碰撞而使Hg原子被激發,該Hg原子從激發態向基 φ 態遷移時放射出的紫外線照射到螢光體上,由此,從該螢 光體放射出可視光。 在現有技術中,作爲冷陰極螢光管用電極已知有一種 實質上僅由Mo構成的電極(參照日本公開專利特開 2000- 1 3320 1號公報)。前述冷陰極螢光管用電極雖然管 電壓較低、能源效率較好,但存在有如下問題:即,由於 Mo極爲昂貴,製造成本較高,而且,因爲Mo硬度很大 ,將其加工成電極比較困難。 因此,作爲爲了抑制製造成本的同時並得到較良好的 -5- 201013738 加工性而降低Mo含量的電極’已知有如下一種冷陰極螢 光管用電極(參照日本公開專利特開2006_ 1 2505號公報 )。即,該冷陰極螢光管用電極含有相對全量在6〜3 5質 量%範圍內的Mo,且剩餘部分由Ni及不可避免的不純物 的合金構成。 而且,因Ni在塑性加工性上較爲優良,在現有技術 中,作爲前述冷陰極螢光管用電極’實質上是僅由Ni構 成的電極被廣泛使用’並且還被提案有多種由Ni基合金 _ 構成的冷陰極螢光管用電極。例如’本案發明者提案了一 種由含有Mo和Nb的Ni基合金構成的冷陰極螢光管用電 極(參照日本公開專利特開2007_3 1 83 2號公報)。 但同時,實質上是由Ni構成的上述冷陰極登光管用 電極以及由Ni基合金構成的上述冷陰極螢光管用電極’ 構成該電極的Ni容易發生源射’所被濺射的Ni原子與被 封入在玻璃管內的Hg原子起反應’而消耗該Hg原子。 其結果,實質上是由Ni構成的上述冷陰極蜜光管用電極 ❹ 以及由Ni基合金構成的上述冷陰極螢光管用電極具有: 其冷陰極螢光管的使用壽命變短、且對於作爲環境對策的 冷陰極螢光管內的低水銀化對應方面來說是不合適的問題 【發明內容】 本發明的目的在於提供下述一種能夠解決上述問題的 冷陰極螢光管用電極以及使用該電極的冷陰極蛋光管’具 -6- 201013738 有優良的抗濺射性以及加工性,且能夠 ,本發明的目的還在於提供一種冷陰極 使用該電極的冷陰極螢光管,能夠抑制 現作爲環境對策的低水銀化。 本發明者們爲了達成上述目的而進 意到Fe可作爲比Mo成本低、且比Ni 屬元素。然而,由於實質上僅由Fe構 _ 用電極的放電特性不充分,嘗試添加各 份的金屬元素。結果得出,由包含規定 基合金構成的冷陰極螢光管用電極同時 由Mo構成的上述冷陰極螢光管用電極 以及抗濺射性。 於是,本發明者們在由含有Mo的 上述冷陰極螢光管用電極中,藉由使用 異地發現可使抗濺射性提高,且可降低 φ 現使用實質上僅由Fe構成的冷陰極螢 生銹的問題,但藉由形成爲含有規定範 部分實質上爲Fe的合金所構成的冷陰 Mo優先地獲取氧並形成被膜,結果可Ιί 因此,爲了達到上述目的,本發明 電極的特徵在於,由含有相對全量爲〇. 的Mo、Fe以及不可避免的不純物的合 發明的冷陰極螢光管用電極最好是上述 爲0.1〜10質量%範圍內的Mo。 降低管電壓。同時 螢光管用電極以及 與水銀的反應,實 行了種種硏究,注 更具抗濺射性的金 成的冷陰極螢光管 種以Fe爲主要成 範圍內的Mo的Fe 具有可與實質上僅 匹敵的放電特性、 Ni基合金構成的 Fe來取代Ni,驚 管電壓。而且,發 光管用電極時會有 圍內的Mo、剩餘 極螢光管用電極, I抑制.生銹。 的冷陰極螢光管用 1~30質量%範圍內 金構成。另外,本 合金含有相對全量 201013738 此外,爲了實現較低的管電壓’本發明的冷陰極螢光 管用電極最好是上述合金含有相對全量爲1·5~5·5質量% 範圍內的Mo。 在本發明的冷陰極螢光管用電極中’上述合金可以進 一步含有相對全量爲5質量%以下的Ru。根據上述構成, 能夠進一步降低管電壓。而且,根據該構成’上述合金中 的Ru汲取氧而形成由氧化釕構成的被膜,由此能夠進一 步抑制該合金中的Fe的生銹。 φ 並且,本發明的冷陰極螢光管用電極最好由含有相對 全量爲0.1〜3 0質量%範圍內的Mo、〇. 1〜6質量%範圍內的 Nb、Fe以及不可避免的不純物的合金構成。本發明的冷 陰極螢光管用電極因上述合金含有上述範圍內的Nb,能 夠在提高抗濺射性的同時,抑制Fe基合金的生銹,提高 耐腐蝕性。 本發明的冷陰極螢光管用電極能夠應用在冷陰極螢光 管中。 ❹ 【實施方式】 接著,結合附圖對本發明的實施形態進行更爲詳細的 說明。圖1中所示的本實施形態的冷陰極螢光管1用於液 晶顯示器的背光用光源等,例如具有直徑爲3mm、長度 爲3 00mm的玻璃管2、以及安裝在玻璃管2內兩端的一 對冷陰極螢光管用電極3。以下,有時會將冷陰極螢光管 用電極3簡述爲電極3。 -8 - 201013738 玻璃管2在內壁面塗敷有周知的螢光體,並在內部封 入有Hg與Ar、Ne等惰性氣體。 冷陰極螢光管用電極3例如爲一方呈開口的有底筒狀 體,其開口部的外徑爲2.1mm、筒壁厚〇.15mm、長度爲 7.0mm。冷陰極螢光管用電極3雖然也可以設成薄板狀, 但藉由形成爲上述有底筒狀體,而能夠容易地放射出電子 〇 一對冷陰極螢光管用電極3裝設在玻璃管2內,各電 極3的上述開口部在玻璃管2的軸向互相呈相對向。在冷 陰極螢光管用電極3的底部,連接有封接銷4,該封接銷 4由科瓦合金(Kovar)線形成,封接於玻璃管2並向玻 璃管2外側突出。在封接銷4之與冷陰極螢光管用電極3 成反向側的端部,連接有由杜美絲(Dumet wire )形成的 外部導線5。另外,在封接銷4設置有與玻璃管2進行封 接用的玻璃微珠(未被圖示)。 冷陰極螢光管用電極 3由含有 Fe、相對全量爲 0.1〜10質量%範圍內的Mo、以及不可避免的不純物的合 金構成。 本實施形態中的冷陰極螢光管用電極3在構成該電極 3的上述合金中,以Fe爲基元素。由此,能夠抑制從上 述電極3表面以及該電極3濺射的濺射粒子與玻璃管2內 的Hg原子發生的反應,從而抑制Hg的消耗,能夠延長 冷陰極螢光管1的使用壽命。此外,本實施形態中的冷陰 極螢光管用電極3在構成該電極3的上述合金中’藉由將 -9- 201013738201013738 SUMMARY OF THE INVENTION [Technical Field] The present invention relates to an electrode for a cold cathode fluorescent tube and a cold cathode fluorescent tube using the same. [Prior Art] A cold cathode fluorescent tube is widely used as a backlight source for a liquid crystal display. The cold cathode fluorescent tube has a glass tube having a small diameter and a pair of electrodes for a cold cathode fluorescent tube, and the inside of the glass tube is sealed with an inert gas such as Hg and Ar, Ne, and a phosphor is coated on the inner wall surface; A pair of cold cathode fluorescent tube electrodes are attached to both ends of the glass tube in the tube axis direction with respect to each other. By applying a high voltage between the electrodes of a pair of cold cathode fluorescent tubes, an electric field is generated in the cold cathode fluorescent tube, and electrons are emitted from the non-heated cathode (cold cathode). Then, when the electron collides with the Hg atom, the Hg atom is excited, and the ultraviolet light emitted when the Hg atom migrates from the excited state to the base φ state is irradiated onto the phosphor, thereby being emitted from the phosphor. Visible light. In the prior art, an electrode composed of substantially only Mo is known as an electrode for a cold cathode fluorescent tube (refer to Japanese Laid-Open Patent Publication No. 2000-136320). Although the electrode for the cold cathode fluorescent tube has a low tube voltage and good energy efficiency, there is a problem in that Mo is extremely expensive, the manufacturing cost is high, and since Mo is hard, it is processed into an electrode. difficult. Therefore, an electrode for a cold cathode fluorescent tube is known as an electrode for reducing the Mo content in order to suppress the manufacturing cost while obtaining a relatively good -5 - 201013738 processability (refer to Japanese Laid-Open Patent Publication No. 2006_1-2505 ). That is, the electrode for the cold cathode fluorescent tube contains Mo in a range of from 6 to 35 % by mass relative to the total amount, and the remainder is composed of an alloy of Ni and an unavoidable impurity. Further, since Ni is excellent in plastic workability, in the prior art, the electrode for the cold cathode fluorescent tube 'is substantially an electrode composed only of Ni is widely used' and various kinds of Ni-based alloys have been proposed. _ The electrode for the cold cathode fluorescent tube. For example, the inventors of the present invention have proposed an electrode for a cold cathode fluorescent tube comprising a Ni-based alloy containing Mo and Nb (refer to Japanese Laid-Open Patent Publication No. 2007_3 1 83 2). At the same time, the electrode for the cold cathode light-emitting tube made of Ni and the electrode for the cold-cathode fluorescent tube made of a Ni-based alloy are substantially Ni atoms which are formed by the source of the Ni. The Hg atom enclosed in the glass tube reacts to consume the Hg atom. As a result, the electrode for the cold cathode honey tube which is substantially composed of Ni and the electrode for the cold cathode fluorescent tube which is made of a Ni-based alloy have a short life of the cold cathode fluorescent tube and serve as an environment. An object of the present invention is to provide an electrode for a cold cathode fluorescent tube capable of solving the above problems and an electrode using the same. Cold cathode egg tube '--6-201013738 has excellent sputtering resistance and workability, and can also provide a cold cathode fluorescent tube using the electrode for cold cathode, which can suppress the present environment The low mercuryation of the countermeasures. In order to achieve the above object, the inventors of the present invention have conceived that Fe can be used as a lower cost than Mo and is a Ni element. However, since the discharge characteristics of the electrode composed of only Fe are insufficient, it is attempted to add a part of the metal element. As a result, it was found that the electrode for a cold cathode fluorescent tube comprising the electrode of the cold cathode fluorescent tube including the predetermined base alloy and the electrode for cold cathode fluorescent tube and the sputtering resistance. Then, the present inventors have improved the sputtering resistance by using the above-described cold cathode fluorescent tube electrode containing Mo, and it is possible to reduce the φ and use a cold cathode which is substantially composed only of Fe. The problem of rust, but the cold cathode Mo formed by the alloy containing the predetermined portion is substantially Fe, preferentially acquires oxygen and forms a film, and as a result, in order to achieve the above object, the electrode of the present invention is characterized in that The electrode for a cold cathode fluorescent tube of the invention comprising a relatively total amount of Mo, Fe, and an unavoidable impurity is preferably in the range of 0.1 to 10% by mass. Reduce the tube voltage. At the same time, the electrode for the fluorescent tube and the reaction with mercury have been subjected to various investigations, and the cold-cathode fluorescent tube of the metal which is more resistant to sputtering has Fe which is mainly in the range of Fe, and has substantially only The superior discharge characteristics, Fe made of Ni-based alloy replace Ni, and the voltage of the tube. Further, when the electrode for the light-emitting tube is used, there are Mo in the circumference and the electrode for the remaining-pole fluorescent tube, and I suppress and rust. The cold cathode fluorescent tube is composed of gold in the range of 1 to 30% by mass. Further, the present alloy contains a relatively full amount of 201013738. In order to achieve a low tube voltage, the electrode for a cold cathode fluorescent tube of the present invention preferably contains Mo in a range of from about 1.5% to about 5% by mass based on the total amount of the alloy. In the electrode for a cold cathode fluorescent tube of the present invention, the alloy may further contain Ru in an amount of 5% by mass or less based on the total amount. According to the above configuration, the tube voltage can be further reduced. Further, according to the composition of the above-mentioned alloy, Ru is taken up as oxygen, and a film made of ruthenium oxide is formed, whereby rust of Fe in the alloy can be further suppressed. φ Further, the electrode for a cold cathode fluorescent tube of the present invention is preferably an alloy containing Nb, Fe, and unavoidable impurities in a range of from 0.1 to 3% by mass in a range of from 0.1 to 3% by mass in a total amount of from 0.1 to 30% by mass. Composition. In the electrode for a cold cathode fluorescent tube of the present invention, since the alloy contains Nb in the above range, it is possible to suppress the rust of the Fe-based alloy and improve the corrosion resistance while improving the sputtering resistance. The electrode for a cold cathode fluorescent tube of the present invention can be applied to a cold cathode fluorescent tube. [Embodiment] Next, embodiments of the present invention will be described in more detail with reference to the accompanying drawings. The cold cathode fluorescent tube 1 of the present embodiment shown in FIG. 1 is used for a backlight source or the like for a liquid crystal display, for example, a glass tube 2 having a diameter of 3 mm and a length of 300 mm, and two ends mounted on the inside of the glass tube 2. A pair of electrodes 3 for cold cathode fluorescent tubes. Hereinafter, the electrode 3 for the cold cathode fluorescent tube will be briefly described as the electrode 3. -8 - 201013738 The glass tube 2 is coated with a well-known phosphor on the inner wall surface, and is internally filled with an inert gas such as Hg, Ar or Ne. The cold cathode fluorescent tube electrode 3 is, for example, a bottomed cylindrical body having an opening, and has an opening having an outer diameter of 2.1 mm, a tube wall thickness of 1515 mm, and a length of 7.0 mm. The cold cathode fluorescent tube electrode 3 may be formed in a thin plate shape, but by forming the bottomed cylindrical body, the electrons can be easily emitted. A pair of cold cathode fluorescent tube electrodes 3 are attached to the glass tube 2 The openings of the respective electrodes 3 are opposed to each other in the axial direction of the glass tube 2. A sealing pin 4 is formed at the bottom of the electrode 3 for the cold cathode fluorescent tube, and the sealing pin 4 is formed of a Kovar wire, sealed to the glass tube 2, and protrudes to the outside of the glass tube 2. An external lead 5 formed of Dumet wire is connected to the end of the sealing pin 4 on the side opposite to the electrode 3 for the cold cathode fluorescent tube. Further, glass beads (not shown) for sealing the glass tube 2 are provided in the sealing pin 4. The electrode 3 for a cold cathode fluorescent tube is composed of an alloy containing Fe, a relatively total amount of Mo in the range of 0.1 to 10% by mass, and an unavoidable impurity. In the above-described alloy constituting the electrode 3, the electrode 3 for cold cathode fluorescent tubes of the present embodiment contains Fe as a base element. Thereby, it is possible to suppress the reaction between the sputtered particles sputtered from the surface of the electrode 3 and the electrode 3 and the Hg atoms in the glass tube 2, thereby suppressing the consumption of Hg and extending the life of the cold cathode fluorescent tube 1. Further, the electrode 3 for cold cathode fluorescent tubes in the present embodiment is in the above-mentioned alloy constituting the electrode 3' by -9-201013738

Fe作爲基元素,能夠得到作爲電極的基本電氣特性以及 優良的加工性的同時,能夠實現低成本。 然而,構成冷陰極螢光管用電極3的上述合金如果實 質上僅爲Fe的話,其放電特性則並不充分。因而,本實 施形態中的冷陰極螢光管用電極3在上述合金中添加上述 含量範圍的Mo。 本實施形態中的冷陰極螢光管用電極3藉由使上述合 金含有上述含量範圍的Mo,能夠降低放電時的管電壓, 提高電子放射特性。另外,本實施形態中的冷陰極螢光管 用電極3藉由使上述合金含有上述含量範圍的Mo,能夠 抑制Fe基合金的生銹。此外,本實施形態中的冷陰極螢 光管用電極3藉由使上述合金含有上述含量範圍的Mo, 能夠抑制Fe基合金與Hg的反應。 在構成冷陰極螢光管用電極3的上述合金中,當Mo 的含量爲相對全量爲不滿0.1質量%時,則不能提高電子 放射特性,無法降低管電壓。同時,當Mo的含量爲相對 全量爲未滿0.1質量%時,不能抑制Fe基合金的生銹,且 不能充分抑制Fe基合金與Hg的反應。 而另一方面,在上述合金中,當Mo的含量爲相對全 量爲超過1〇質量%時,在該合金中會形成反映脆性的 FezMo、Fe3Mo3等的金屬間化合物,或者,由於因硬度增 大而降低加工性,不能形成具有想要的形狀的冷陰極螢光 管用電極3。 另外’爲了更可靠地得到上述含有Mo的效果,在上 -10- 201013738 述合金中,Mo的含量最好是相對全量在1.5-5.5質量%範 圍內。 再者,本實施形態中的冷陰極螢光管用電極3可以使 用由如下合金所構成者。即,該合金除了含有Fe、相對 全量在0.1〜10質量%範圍內的Mo、以及不可避免的不純 物之外,還含有相對全量在5質量%以下的Ru。在該情況 下,能夠進一步降低管電壓以及延長冷陰極螢光管1的使 用壽命。 在上述合金中,Ru的含量如果爲相對全量爲超過5 質量%,則無法進一步降低管電壓的同時,成本也增加。 在上述合金中,爲了更可靠地實現因添加Ru而得到的降 低管電壓的效果’可將Ru的含量設定成相對全量在 0.1〜5質量%的範圍內。 此外,本實施形態中的冷陰極螢光管用電極3還可以 使用由如下合金所構成者。即,該合金除了含有Fe、相 對全量在0.1-30質量%範圍內的Mo、以及不可避免的不 純物之外,還含有相對全量在〇」〜6質量%範圍內的Nb。 這時,在上述合金中,當Mo的含量爲相對全量爲不 滿0.1質量%時,則不能提高電子放射特性,無法降低管 電壓。同時,在上述合金中,當Mo的含量爲相對全量不 滿0.1質量%時’不能抑制Fe基合金的生錄,且不能充分 抑制Fe基合金與Hg的反應。 而另一方面,在上述合金中,當Mo的含量爲相對全 量超過30質量%時,無法降低冷陰極螢光管用電極3的 -11 - 201013738 管電壓。並且,在上述合金中,當Mo的含量爲相對全量 超過30質量%時,在該合金中會形成反映脆性的Fe2Mo 、Fe3Mo 3等的金屬間化合物,或者硬度增大。其結果, 加工性降低’不能形成具有想要的形狀的冷陰極螢光管用 電極3。 另外’本實施形態中的冷陰極螢光管用電極3藉由使 上述合金含有上述含量範圍的Nb,能夠降低放電時的管 電壓,提高電子放射特性。另外,電極3藉由使上述合金 含有上述含量範圍的Nb,能夠提高抗濺射性的同時,抑 制F e基合金的生銹,提高耐腐蝕性。 這時’在上述合金中,當Nb的含量爲相對全量不滿 〇· 1質量%時,則無法得到上述效果。 另一方面’在上述合金中,當Nb的含量爲相對全量 超過6質量%時,在該合金中會形成反映脆性的Fe2Nb等 的金屬間化合物’或者因硬度增大而使加工性降低,不能 形成具有想要的形狀的冷陰極螢光管用電極3。 接著’提示實施例以及比較例。 (實施例一) 在本實施例中’首先,在真空熔解爐中將Fe和Mo 構成的鑄錠10kg熔解,調製成熔液,並將該熔液製成規 定形狀的塊。上述塊含有相對全量爲3.4質量%的Mo,剩 餘部分由Fe以及不可避免的不純物的合金構成。上述不 可避免的不純物含有相對上述合金的全量爲〇.1()質量%以 201013738 下的C、0.50質量。/。以下的si、〇.50質量%以下的Mn、 0 _ 0 5質量°/。以下的p、0 · 5 0質量%以下的S。 ' 接著,對上述塊施以溫度1100t:的熱鍛,得到厚度 爲20mm的板材。隨後,藉由對上述厚度爲2〇mm的板材 施以線切割,得到厚度爲lmm的板材。然後,藉由對上 述厚度爲1mm的板材進行硏磨,去除因上述線切割而產 生的氧化皮(〇xide scale)。 ❹ 接著,對已去除上述氧化皮後的厚度爲lmm的板材 ,依序反覆施以常溫下的冷壓延和氫環境下溫度800 °C的 退火,藉此得到厚度爲〇.2mm的薄板材。隨後’對上述 厚度爲0.2mm的薄板材施以1〇分鐘的氫環境下溫度800 °C的退火後,藉由冷卻至常溫’得到用於冷陰極螢光管用 電極3的電極材料。 隨後,測定由本實施例得到的電極材料的維氏硬度( Vickers hardness),其値爲156HV。結果示於表1中。 〇 然後,與本實施例完全相同,測定實質上僅由Ni構 成且剩餘部分是不可避免的不純物的電極材料(參考例一 )的維氏硬度’其値爲75 HV。結果示於表1中。 接著’利用四探針法測定由本實施例得到的電極材料 的電阻率’其値爲19·7μΩ·(;ηι。結果示於表1及圖2中。 隨後,與本實施例完全相同,測定參考例一中的電極 材料的電阻率’其値爲4.6pi^cin。結果示於表1中。 然後’使用本實施例中得到的電極材料,製成出兩枚 縱長20mm、橫寬20mm、厚〇.2mm的試驗片。 -13- 201013738 首先,將第一枚試驗片放置在空氣中2160小時,確 認是否生銹,其結果並沒生銹。 接著,將第二枚試驗片放置在濺射裝置的真空室內, 在5.33<10_叶&的Ar環境下,在供應電力150W的條件下 連續施以濺射8小時。隨後,藉由測定經連續濺射後的上 述試驗片減少的重量,計算出本實施例中得到的電極材料 的濺射率。 然後,關於參考例一的電極材料,與本實施例完全相 同’製成試驗片,藉由測定經連續濺射後的該試驗片減少 的重量,計算出該電極材料的濺射率。將參考例一的電極 材料的濺射率設定爲100%時,本實施例的電極材料的濺 射率相當於59%。結果示於表1中。在表1中,濺射率値 越低,則表示因濺射而產生的消耗越少,抗濺射性越爲優 良。 接著,使用本實施例中得到的電極材料,製成出縱長 15mm、橫寬1.5mm、厚0.2mm的一對薄板狀的冷陰極螢 光管用電極3。 接著,爲了對本實施例中得到的冷陰極螢光管用電極 3的性能進行評價,製成冷陰極管A,該冷陰極管A在內 壁面沒被塗敷螢光體的玻璃管內部,具有一對薄板狀的冷 陰極螢光管用電極3。考慮到隨後檢查有無從冷陰極螢光 管用電極3濺射出原子以及與Hg的反應時的方便性,冷 陰極管A採用了內壁面沒有被塗敷螢光體的玻璃管。 首先,爲了製成冷陰極管A,將由科瓦合金線形成的 -14- 201013738 封接銷4連接到本實施例中得到的一對薄板狀的冷陰極螢 光管用電極3的端部,在該封接銷4之與冷陰極螢光管用 電極3成反向側的端部,連接有由杜美絲形成的外部導線 5。在封接銷4設置有與玻璃管2進行封接用的玻璃微珠 (未被圖示)。 接著,在直徑爲3mm、長爲300mm之在內壁面沒有 被塗敷螢光體的的玻璃管內兩端,裝設有連接了封接銷4 _ 的薄板狀的冷陰極螢光管用電極3。這時,在軸向設置一 對冷陰極螢光管用電極3,以使未被連接有封接銷4之側 的端部相互呈相對向。 隨後,將Hg與Ar以及Ne氣體封入到上述玻璃管內 部後,將封接銷4與該玻璃管封接。這時,使封接銷4向 上述玻璃管的外側突出,從而得到冷陰極管A。 然後,對製成的冷陰極管A的一對上述電極3之間 ,分別施加5 m A、6 m A、7 m A、8 m A的管電流,測定針對 φ 各個管電流而產生的管電壓。將結果示於圖3中。 接著,製成作爲參考例二的一對薄板狀的冷陰極螢光 管用電極,製成具有該一對電極的冷陰極管Β。其中,關 於該電極,除了使用了實質上僅由Mo構成且剩餘部分是 不可避免的不純物的電極材料之外,其他與本實施例完全 相同。對製成的冷陰極管B的一對上述電極之間,分別施 力口 5mA、6mA、7mA、8mA的管電流,測定針對各個管電 流而產生的管電壓。將結果示於圖3中。並且,圖4中示 出了對上述冷陰極管A(具有本實施例的冷陰極螢光管用 -15- 201013738 電極3 )施加了 8mA的管電流時產生的管電壓相對於對上 述冷陰極管B(具有參考例二的冷陰極螢光管用電極)施 加了 8mA的管電流時產生的管電壓的比。 接著,以管電流6mA固定的條件下,使上述冷陰極 管A放電200小時後,將該冷陰極管A開封,取出冷陰 極螢光管用電極3。隨後,爲了檢查有無從冷陰極螢光管 用電極3濺射出原子以及與Hg的反應,藉由電子微探儀 (ΕΡΜΑ : Electron Probe Micro Analyzer)測定該電極 3 的表面組成以及上述玻璃管內壁面的組成。結果示於表2 及表3中,表2表示了冷陰極螢光管用電極3的表面組成 :表3表示上述玻璃管內壁面的組成。 接著,使用本實施例中得到的電極材料,製成兩對冷 陰極螢光管用電極3,該電極3爲一側呈開口的有底筒狀 體,開口部的外徑爲2.1mm、筒壁厚0.15mm、長7.0mm 〇 隨後,爲了對具有本實施例中得到的冷陰極螢光管用 電極3的冷陰極螢光管1進行水銀消耗量評價,製成了冷 陰極螢光管la,該冷陰極螢光管la在內壁面塗敷有螢光 體的玻璃管2的內部具有一對有底筒狀體的冷陰極螢光管 用電極3。 首先,爲了製成冷陰極螢光管la,將由科瓦合金線 形成的封接銷4連接到本實施例中得到的一對有底筒狀體 的冷陰極螢光管用電極3的端部,在該封接銷4之與該電 極3成反向側的端部,連接有由杜美絲形成的外部導線5 -16- 201013738 。在封接銷4上設置有與玻璃管進行封接用的玻璃微珠( 未被圖示)。 接著,在直徑爲3mm、長爲5 69mm之在內壁面塗敷 有螢光體的玻璃管2內兩端,裝設有連接了封接銷4的有 底筒狀體的冷陰極螢光管用電極3。這時,在軸向設置一 對冷陰極螢光管用電極3,以使未被連接封接銷4之側的 端部相互呈相對向。 @ 隨後,將Hg與Ar氣體、Ne氣體封入到玻璃管2內 部。以使Ar氣體以及Ne氣體的合計壓力達到5.3kPa的 形式來實施上述封入。然後,將封接銷4和玻璃管2進行 封接。這時,使封接銷4向上述玻璃管的外側突出,從而 得到冷陰極螢光管la。 接著,以管電流8mA固定的條件下,使被製成的本 實施例的冷陰極螢光管la放電2000小時。隨後,用240 °C的溫度加熱玻璃管2,並使用螢光管中水銀測定裝置, φ 測定從玻璃管2放射出的水銀量作爲有效水銀量,該測定 値爲3.64g。上述有效水銀量相當於上述放電時未被消耗 的金屬水銀量。 其後,用900°C的溫度加熱玻璃管2,測定從玻璃管 2放射出的水銀量作爲消耗水銀量,該測定値爲0.04g。 上述消耗水銀量相當於上述放電時消耗的螢光體和附著在 管壁上的化合物水銀量。上述有效水銀量和上述消耗水銀 量之和相當於製作冷陰極螢光管la時被封入在玻璃管2 內的總水銀量。於是,根據下式(1)計算出上述放電時 -17- 201013738 的水銀消耗率。結果示於表4中。 水銀消耗率(%)= {消耗水銀量(g)/總水銀量(g) } X 1 〇〇(%) · · · ( 1 ) 接著,製作一對有底筒狀體的冷陰極螢光管用電極, 關於該電極,除了使用了參考例一中的電極材料之外,其 他與本實施例完全相同,並製成參考例一的冷陰極螢光管 ,該冷陰極螢光管在內壁面塗敷有螢光體之長5 6 9mm的 玻璃管內部具有上述一對電極。 隨後,以與實施例一完全相同的方式,以管電流8mA 固定的條件下,使被製成的本實施例的冷陰極螢光管放電 2 0 00小時,計算出該放電時的水銀消耗率。結果示於表4 中〇 然後,爲了對具有本實施例中製成的冷陰極螢光管用 電極3的冷陰極螢光管1進行使用壽命的評價,製成冷陰 極螢光管lb,該冷陰極螢光管lb除了玻璃管2的長度爲 3 00mm之外,其他與本實施例的冷陰極螢光管la完全相 同。 接著,在管電流8mA固定的條件下,使被製成的本 實施例的冷陰極螢光管lb放電,測定此時的中心亮度。 隨後,藉由對得出的結果進行萊曼(Lehmann)近似,計 算出冷陰極螢光管lb的中心亮度減半所需的時間。並將 結果示於圖5及表5中。 接著,製作一對有底筒狀體的冷陰極螢光管用電極, -18- 201013738 關於該電極,除了使用了參考例一中的電極材料之外,其 他與本實施例完全相同,並製成參考例一的冷陰極螢光管 ,該冷陰極螢光管在長3 00mm的玻璃管內部具有上述一 對電極。 隨後,與本實施例完全相同,在管電流8mA固定的 條件下,使被製成的本實施例的冷陰極螢光管放電,測定 放電時的中心亮度。隨後,藉由對得出的結果進行萊曼( Lehmann)近似,計算出本實施例的冷陰極螢光管的中心 亮度減半所需的時間。並將結果示於圖5及表5中。 (實施例二) 在本實施例中,製成了本實施例的電極材料。關於該 電極材料,除了使用了含有相對全量爲6.6質量%的Mo、 剩餘部分爲不可避免的不純物的合金之外,其他與實施例 一完全相同。 接著,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的維氏硬度,其値爲200HV。結果示於 表1中。 隨後,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的電阻率,其値爲26.0 μΩ· cm。結果示 於表1及圖2中。 然後,關於由本實施例得到的電極材料,以與實施例 一完全相同的方式,製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 -19- 201013738 將參考例一的電極材料的濺射率設定爲100%時,本實施 例的電極材料的濺射率相當於65%。結果示於表1中。 其後,以與實施例一完全相同的方式,使用從本實施 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極3,並製成冷陰極管C,該冷陰極管C在內壁面沒被塗 敷螢光體的玻璃管內部,具有上述一對電極3。 接著,以與實施例一完全相同的方式,對製成的冷陰 極管C的一對上述電極3之間施加8mA的管電流,測定 產生的管電壓。在圖4中示出上述冷陰極管C的管電壓相 對於上述冷陰極管B的管電壓的比。 (實施例三) 在本實施例中,製成了本實施例的電極材料。關於該 電極材料,除了使用了含有相對全量爲9.9質量%的Mo、 剩餘部分爲Fe以及不可避免的不純物的合金之外,其他 與實施例一完全相同。 接著,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的維氏硬度,其値爲291 HV。結果示於 表1中。 隨後,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的電阻率,其値爲26.2μΩ·(:πι。結果示 於表1及圖2中。 然後,關於由本實施例得到的電極材料,以與實施例 一完全相同的方式,製成試驗片,藉由測定經連續濺射後 -20- 201013738 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本實施 例的電極材料的濺射率相當於71%。結果示於表1中。 其後,以與實施例一完全相同的方式,使用從本實施 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極3,並製成冷陰極管D,該冷陰極管D在內壁面沒被塗 敷螢光體的玻璃管內部,具有上述一對電極3。 接著,以與實施例一完全相同的方式,對製成的冷陰 極管D的一對上述電極3之間施加8mA的管電流,測定 產生的管電壓。在圖4中示出上述冷陰極管D的管電壓 相對於上述冷陰極管B的管電壓的比。 (實施例四) 在本實施例中,製成了本實施例的電極材料。關於該 電極材料,除了使用了含有相對全量爲0.17質量%的Mo 、剩餘部分爲Fe以及不可避免的不純物的合金之外,其 他與實施例一完全相同。 接著,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的維氏硬度,其値爲1 13HV »結果示於 表1中® 隨後,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的電阻率,其値爲11.ΟμΩκιη。結果示 於表1及圖2中。 然後,關於由本實施例得到的電極材料,以與實施例 -21 - 201013738 一完全相同的方式,製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本實施 例的電極材料的濺射率相當於58%。結果示於表1中。 其後,以與實施例一完全相同的方式,使用從本實施 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極3,並製成冷陰極管E,該冷陰極管E在內壁面沒被塗 敷螢光體的玻璃管內部,具有上述一對電極3。 接著,以與實施例一完全相同的方式,對製成的冷陰 極管E的一對上述電極3之間施加8mA的管電流,測定 產生的管電壓。在圖4中示出上述冷陰極管E的管電壓相 對於上述冷陰極管B的管電壓的比。 (實施例五) 在本實施例中,製成了本實施例的電極材料。關於該 電極材料,除了使用了含有相對全量爲1.7質量%的Mo、 剩餘部分爲Fe以及不可避免的不純物的合金之外,其他 與實施例一完全相同。 接著,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的維氏硬度,其値爲149HV。結果示於 表1中。 隨後,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的電阻率,其値爲15.4 μΩκιη。結果示 於表1及圖2中。 -22- 201013738 然後,關於由本實施例得到的電極材料,以與實施例 一完全相同的方式,製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本實施 例的電極材料的濺射率相當於57%。結果示於表1中。 其後,以與實施例一完全相同的方式,使用從本實施 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極3,並製成冷陰極管F,該冷陰極管F在內壁面沒被塗 敷螢光體的玻璃管內部,具有上述一對電極3。 接著,以與實施例一完全相同的方式,對製成的冷陰 極管F的一對上述電極3之間施加8mA的管電流,測定 產生的管電壓。在圖4中示出上述冷陰極管F的管電壓相 對於上述冷陰極管B的管電壓的比。 (實施例六) 在本實施例中,製成了本實施例的電極材料。關於該 電極材料,除了使用了含有相對全量爲5.0質量%的Mo、 剩餘部分爲Fe以及不可避免的不純物的合金之外,其他 與實施例一完全相同。 接著,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的維氏硬度,其値爲175HV。結果示於 表1中。 隨後,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的電阻率,其値爲23.8μΩ·ί:ιη。結果示 -23- 201013738 於表1及圖2中。 然後,關於由本實施例得到的電極材料,以與實施例 —完全相同的方式,製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本實施 例的電極材料的濺射率相當於5 7%。結果示於表1中。 其後,以與實施例一完全相同的方式,使用從本實施 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極3,並製成冷陰極管G,該冷陰極管G在內壁面沒被塗 敷螢光體的玻璃管內部,具有上述一對電極3。 接著,以與實施例一完全相同的方式,對製成的冷陰 極管G的一對上述電極3之間施加8mA的管電流,測定 產生的管電壓。在圖4中示出上述冷陰極管G的管電壓 相對於上述冷陰極管B的管電壓的比。 在本比較例中,製成了本比較例的電極材料。關於該 電極材料,除了使用了實質上僅由Fe構成且剩餘部分爲 不可避免的不純物的金屬之外’其他與實施例一完全相同 〇 接著,以與實施例一完全相同的方式,測定由本比較 例得到的電極材料的維氏硬度’其値爲110HV。結果示於 表1中。 隨後,以與實施例一完全相同的方式,測定由本比較 -24- 201013738 例fg=到的電極材料的電阻率,其値爲1〇.1μίί·ςΐη。結果不 於表1及圖2中。 然後’關於由本比較例得到的電極材料,以與實施例 一完全相同的方式’製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本比較 例的電極材料的濺射率相當於5 8 %。結果示於表1中。 其後,以與實施例一完全相同的方式,使用從本比較 〇 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極,並製成冷陰極管Η,該冷陰極管Η在內壁面沒被塗敷 螢光體的玻璃管內部,具有上述一對電極。 接著,以與實施例一完全相同的方式,對製成的冷陰 極管Η的一對上述電極之間分別施加5mA、6mA、7mA、 8mA的管電流,並分別測定針對各個管電流產生的管電壓 。結果示於圖3中。在圖4中示出上述冷陰極管Η的管 ⑩ 電壓相對於上述冷陰極管Β的管電壓的比。 隨後,以與實施例一完全相同的方式,藉由ΕΡΜΑ測 定上述冷陰極管Η的冷陰極螢光管用電極的表面組成以 及玻璃管內壁面的組成。結果示於表2及表3中。 在本比較例中,製成了本比較例的電極材料。關於該 電極材料,除了使用了含有相對全量爲15.3質量%的Mo 、剩餘部分爲Ni以及不可避免的不純物的合金之外’其 -25- 201013738 他與實施例一完全相同。 接著,以與實施例一完全相同的方式,測定由本比較 例得到的電極材料的維氏硬度,其値爲305HV。結果示於 表1中。 隨後,以與實施例一完全相同的方式,測定由本比較 例得到的電極材料的電阻率,其値爲72·6μΩ·(ίΐη。結果示 於表1中。 然後,關於由本比較例得到的電極材料,以與實施例 一完全相同的方式,製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本比較 例的電極材料的濺射率相當於1 1 1 %。結果示於表1中。 其後,以與實施例一完全相同的方式,使用從本比較 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極,並製成冷陰極管J,該冷陰極管J在內壁面沒被塗敷 螢光體的玻璃管內部,具有上述一對電極。 接著,以與實施例一完全相同的方式,藉由ΕΡΜΑ測 定上述冷陰極管J的冷陰極螢光管用電極的表面組成以及 玻璃管內壁面的組成。結果示於表2及表3中。 (比較例三) 在本比較例中,製成了本比較例的電極材料。關於該 電極材料,除了使用了含有相對全量爲16.0質量%的Mo 、剩餘部分爲Fe以及不可避免的不純物的合金之外,其 -26- 201013738 他與實施例一完全相同。 接著,以與實施例一完全相同的方式,測定由本比較 例得到的電極材料的維氏硬度,其値爲490HV。結果示於· 表1中。 隨後,以與實施例一完全相同的方式,測定由本比較 例得到的電極材料的電阻率,其値爲33·6μΩ·^η。結果示 於表1及圖2中。 0 然後,關於由本比較例得到的電極材料,以與實施例 一完全相同的方式,製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本比較 例的電極材料的濺射率相當於65%。結果示於表1中》 其後,以與實施例一完全相同的方式,使用從本比較 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極,並製成冷陰極管Κ,該冷陰極管Κ在內壁面沒被塗敷 φ 螢光體的玻璃管內部,具有上述一對電極。 接著,以與實施例一完全相同的方式,對製成的冷陰 極管Κ的一對上述電極之間施加8mA的管電流,測定產 生的管電壓。在圖4中示出上述冷陰極管K的管電壓相 對於上述冷陰極管B的管電壓的比。 (比較例四) 在本比較例中,製成了本比較例的電極材料。關於該 電極材料,除了使用了含有相對全量爲23.3質量%的Mo -27- 201013738 、剩餘部分爲Fe以及不可避免的不純物的合金之外,其 他與實施例一完全相同。 接著,以與實施例一完全相同的方式,測定由本比較 例得到的電極材料的維氏硬度,其値爲493 HV。結果示於 表1中。 隨後,以與實施例一完全相同的方式,測定由本比較 例得到的電極材料的電阻率,其値爲36·2μΩ·(:ηι。結果示 於表1及圖2中。 然後,關於由本比較例得到的電極材料,以與實施例 一完全相同的方式,製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本比較 例的電極材料的濺射率相當於83%。結果示於表1中。 其後,以與實施例一完全相同的方式,使用從本比較 例中得到的電極材料製作一對薄板狀的冷陰極螢光管用電 極,並製成冷陰極管L,該冷陰極管L在內壁面沒被塗敷 螢光體的玻璃管內部,具有上述一對電極。 接著’以與實施例一完全相同的方式,對製成的冷陰 極管L的一對上述電極之間施加8mA的管電流,測定產 生的管電壓。在圖4中示出上述冷陰極管L的管電壓相對 於上述冷陰極管B的管電壓的比。 -28- 201013738 (表1)Fe as a base element can attain a low cost as a basic electrical characteristic of an electrode and excellent workability. However, if the alloy constituting the electrode 3 for cold cathode fluorescent tubes is substantially Fe alone, the discharge characteristics are not sufficient. Therefore, in the electrode 3 for cold cathode fluorescent tubes in the present embodiment, Mo in the above content range is added to the above alloy. In the electrode 3 for a cold cathode fluorescent tube of the present embodiment, the alloy containing the above-described content range of Mo can reduce the tube voltage at the time of discharge and improve the electron emission characteristics. Further, in the electrode 3 for cold cathode fluorescent tubes of the present embodiment, by causing the alloy to contain Mo in the above-described range, rust of the Fe-based alloy can be suppressed. Further, the electrode 3 for cold cathode fluorescent tubes of the present embodiment can suppress the reaction between the Fe-based alloy and Hg by causing the alloy to contain Mo in the above-described range. In the alloy of the electrode 3 for the cold cathode fluorescent tube, when the content of Mo is less than 0.1% by mass relative to the total amount, the electron emission characteristics cannot be improved, and the tube voltage cannot be lowered. Meanwhile, when the content of Mo is less than 0.1% by mass relative to the total amount, the rust of the Fe-based alloy cannot be suppressed, and the reaction of the Fe-based alloy with Hg cannot be sufficiently suppressed. On the other hand, in the above alloy, when the content of Mo is more than 1% by mass relative to the total amount, an intermetallic compound such as FezMo or Fe3Mo3 which reflects brittleness is formed in the alloy, or, due to an increase in hardness On the other hand, the workability is lowered, and the electrode 3 for cold cathode fluorescent tubes having a desired shape cannot be formed. Further, in order to obtain the above-described effect of containing Mo more reliably, in the above-mentioned alloy of -10-201013738, the content of Mo is preferably in the range of 1.5 to 5.5% by mass relative to the total amount. Further, the electrode 3 for cold cathode fluorescent tubes in the present embodiment can be composed of the following alloy. That is, the alloy contains, in addition to Fe, a relatively total amount of Mo in the range of 0.1 to 10% by mass, and unavoidable impurities, and also contains Ru in an amount of not more than 5% by mass. In this case, the tube voltage can be further lowered and the life of the cold cathode fluorescent tube 1 can be extended. In the above alloy, if the content of Ru is more than 5% by mass relative to the total amount, the tube voltage cannot be further lowered, and the cost is also increased. In the above alloy, in order to more reliably achieve the effect of reducing the tube voltage obtained by adding Ru, the content of Ru can be set to be in the range of 0.1 to 5% by mass relative to the total amount. Further, the electrode 3 for cold cathode fluorescent tubes in the present embodiment may be made of the following alloy. Namely, the alloy contains Nb in a range of from 〇 to 6% by mass in addition to Fe, a relative amount of Mo in the range of 0.1 to 30% by mass, and unavoidable impurities. In this case, when the content of Mo is less than 0.1% by mass relative to the total amount, the electron emission characteristics cannot be improved, and the tube voltage cannot be lowered. Meanwhile, in the above alloy, when the content of Mo is less than 0.1% by mass relative to the total amount, the growth of the Fe-based alloy cannot be suppressed, and the reaction of the Fe-based alloy with Hg cannot be sufficiently suppressed. On the other hand, in the above alloy, when the content of Mo is more than 30% by mass relative to the total amount, the voltage of the -11 - 201013738 tube of the electrode 3 for the cold cathode fluorescent tube cannot be lowered. In addition, when the content of Mo is more than 30% by mass based on the total amount, an intermetallic compound such as Fe2Mo or Fe3Mo 3 which reflects brittleness is formed in the alloy, or the hardness is increased. As a result, the workability is lowered, and the cold cathode fluorescent tube electrode 3 having a desired shape cannot be formed. Further, the electrode 3 for the cold cathode fluorescent tube of the present embodiment can reduce the tube voltage at the time of discharge and improve the electron emission characteristics by causing the alloy to contain Nb in the above-described content range. Further, by causing the alloy 3 to contain Nb in the above-mentioned content range, the electrode 3 can improve the sputtering resistance and suppress the rust of the Fe-based alloy and improve the corrosion resistance. At this time, in the above alloy, when the content of Nb is less than 全·1% by mass relative to the total amount, the above effects cannot be obtained. On the other hand, when the content of Nb is more than 6% by mass relative to the total amount, an intermetallic compound such as Fe2Nb which reflects brittleness is formed in the alloy, or the workability is lowered due to an increase in hardness, and An electrode 3 for a cold cathode fluorescent tube having a desired shape is formed. Next, the examples and comparative examples are presented. (First Embodiment) In the present embodiment, first, 10 kg of an ingot composed of Fe and Mo was melted in a vacuum melting furnace to prepare a molten metal, and the molten metal was formed into a block of a predetermined shape. The above block contained Mo in an amount of 3.4% by mass relative to the total amount, and the remainder was composed of Fe and an alloy of unavoidable impurities. The above-mentioned unavoidable impurities contain a total amount of 〇.1 ()% by mass to C, 0.50 mass at 201013738, relative to the above alloy. /. The following si, 〇.50 mass% or less of Mn, 0 _ 0 5 mass ° /. The following p, 0, 50% by mass or less of S. Next, the block was subjected to hot forging at a temperature of 1100 t: to obtain a plate having a thickness of 20 mm. Subsequently, a sheet having a thickness of 1 mm was obtained by subjecting the above-mentioned sheet having a thickness of 2 mm to wire cutting. Then, by honing the above-mentioned plate having a thickness of 1 mm, the scale (xx scale) generated by the above-mentioned wire cutting was removed. Next, the sheet having a thickness of 1 mm after the above scale was removed was subjected to cold rolling at room temperature and annealing at a temperature of 800 ° C in a hydrogen atmosphere, thereby obtaining a sheet having a thickness of 0.2 mm. Subsequently, the thin plate having a thickness of 0.2 mm was subjected to annealing at a temperature of 800 °C in a hydrogen atmosphere for 1 minute, and then cooled to a normal temperature to obtain an electrode material for the electrode 3 for cold cathode fluorescent tubes. Subsequently, the Vickers hardness of the electrode material obtained in the present example was measured, and the enthalpy was 156 HV. The results are shown in Table 1. Then, exactly as in the present example, the Vickers hardness of the electrode material (Reference Example 1) which was substantially composed only of Ni and the remainder was unavoidable impurities was measured and the 値 was 75 HV. The results are shown in Table 1. Next, 'the resistivity of the electrode material obtained in the present example was measured by the four-probe method', and the enthalpy was 19·7 μΩ·(; ηι. The results are shown in Table 1 and Fig. 2. Subsequently, the measurement was completely the same as in the present example. The resistivity of the electrode material in Reference Example 1 was 4.6 pi^cin. The results are shown in Table 1. Then, using the electrode material obtained in this example, two longitudinal lengths of 20 mm and widths of 20 mm were produced. -2mm test piece. -13- 201013738 First, the first test piece was placed in the air for 2,160 hours to confirm whether it was rusted, and the result was not rust. Next, the second test piece was placed in the test piece. In the vacuum chamber of the sputtering apparatus, sputtering was continuously performed for 8 hours under the condition of supplying electric power of 150 W in an Ar environment of 5.33 <10_leaf & and then, the above test piece after continuous sputtering was measured by measuring The sputtering rate of the electrode material obtained in the present example was calculated by reducing the weight. Then, the electrode material of Reference Example 1 was exactly the same as that of the present example, and a test piece was prepared by measuring the continuous sputtering. The test piece reduces the weight and calculates The sputtering rate of the electrode material. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering rate of the electrode material of the present example was 59%. The results are shown in Table 1. In the meantime, the lower the sputtering rate 値, the less the consumption due to sputtering is, and the better the sputtering resistance is. Next, using the electrode material obtained in the present example, the length is 15 mm and the width is wide. A pair of thin plate-shaped electrodes for cold cathode fluorescent tubes of 1.5 mm and a thickness of 0.2 mm. Next, in order to evaluate the performance of the electrode 3 for cold cathode fluorescent tubes obtained in the present example, a cold cathode tube A was produced, which was cold. The cathode tube A has a pair of thin-plate cold cathode fluorescent tube electrodes 3 on the inner wall surface of the glass tube to which the phosphor is not coated. Considering whether or not the atom is sputtered from the cold cathode fluorescent tube electrode 3 and For the convenience of the reaction of Hg, the cold cathode tube A uses a glass tube whose inner wall surface is not coated with a phosphor. First, in order to form the cold cathode tube A, the -14-201013738 formed of the Kova wire is sealed. The pin 4 is connected to a pair of thin plates obtained in this embodiment The end portion of the electrode 3 for the cold cathode fluorescent tube is connected to the end portion of the sealing pin 4 opposite to the electrode 3 for the cold cathode fluorescent tube, and the external lead 5 formed of Dumet wire is connected. The pin 4 is provided with glass beads (not shown) for sealing with the glass tube 2. Next, in a glass tube having a diameter of 3 mm and a length of 300 mm on which the inner wall surface is not coated with the phosphor, The electrode 3 for a cold cathode fluorescent tube having a thin plate shape to which the sealing pin 4_ is connected is provided at the end. In this case, a pair of cold cathode fluorescent tube electrodes 3 are provided in the axial direction so that the sealing pin 4 is not connected. The ends on the sides are opposed to each other. Subsequently, after Hg, Ar, and Ne gas are sealed inside the glass tube, the sealing pin 4 is sealed with the glass tube. At this time, the sealing pin 4 is protruded to the outside of the glass tube to obtain a cold cathode tube A. Then, a tube current of 5 m A, 6 m A, 7 m A, and 8 m A was applied between the pair of electrodes 3 of the formed cold cathode tube A, and a tube generated for each tube current of φ was measured. Voltage. The results are shown in Fig. 3. Next, a pair of thin plate-shaped electrodes for cold cathode fluorescent tubes as Reference Example 2 were prepared, and a cold cathode tube having the pair of electrodes was prepared. Here, the electrode is completely the same as the present embodiment except that an electrode material which is substantially composed only of Mo and the remainder is unavoidable impurities is used. A tube current of 5 mA, 6 mA, 7 mA, and 8 mA was applied between the pair of electrodes of the formed cold cathode tube B, and the tube voltage generated for each tube current was measured. The results are shown in Fig. 3. Moreover, FIG. 4 shows a tube voltage generated when a tube current of 8 mA is applied to the above-described cold cathode tube A (having the electrode 3 of the cold cathode fluorescent tube of -15-201013738 of the present embodiment) with respect to the above-mentioned cold cathode tube. B (the electrode for the cold cathode fluorescent tube of Reference Example 2) has a ratio of the tube voltage generated when a tube current of 8 mA is applied. Then, the cold cathode tube A was discharged for 200 hours under the condition that the tube current was fixed at 6 mA, and then the cold cathode tube A was opened, and the cold cathode fluorescent tube electrode 3 was taken out. Subsequently, in order to check whether or not atoms were sputtered from the electrode 3 for cold cathode fluorescent tubes and reacted with Hg, the surface composition of the electrode 3 and the inner wall surface of the glass tube were measured by an electron micro-detector (electron probe Micro Analyzer). composition. The results are shown in Tables 2 and 3, and Table 2 shows the surface composition of the electrode 3 for cold cathode fluorescent tubes. Table 3 shows the composition of the inner wall surface of the glass tube. Next, using the electrode material obtained in the present example, two pairs of cold cathode fluorescent tube electrodes 3 were formed, the electrode 3 being a bottomed cylindrical body having an opening on one side, and the outer diameter of the opening portion was 2.1 mm, and the tube wall After the thickness of the cold cathode fluorescent tube 1 having the electrode 3 for the cold cathode fluorescent tube obtained in the present embodiment was evaluated for mercury consumption, a cold cathode fluorescent tube la was produced. The cold cathode fluorescent tube 1a has a pair of cold cathode fluorescent tube electrodes 3 having a bottomed cylindrical body inside the glass tube 2 to which the phosphor is coated on the inner wall surface. First, in order to form the cold cathode fluorescent tube 1a, the sealing pin 4 formed of the Kova wire is connected to the end of the pair of bottomed cylindrical cold cathode fluorescent tube electrodes 3 obtained in the present embodiment. At the end of the sealing pin 4 opposite to the electrode 3, an external lead 5-16-201013738 formed of Dumet wire is connected. Glass beads (not shown) for sealing the glass tube are provided on the sealing pin 4. Next, a cold cathode fluorescent tube having a bottomed cylindrical body to which a sealing pin 4 is attached is attached to both ends of a glass tube 2 having a diameter of 3 mm and a length of 5 69 mm and having a phosphor coated on the inner wall surface. Electrode 3. At this time, a pair of cold cathode fluorescent tube electrodes 3 are axially disposed so that the ends on the side to which the sealing pin 4 is not connected are opposed to each other. @ Subsequently, Hg, Ar gas, and Ne gas are sealed inside the glass tube 2. The above sealing was carried out in such a manner that the total pressure of the Ar gas and the Ne gas reached 5.3 kPa. Then, the sealing pin 4 and the glass tube 2 are sealed. At this time, the sealing pin 4 is protruded to the outside of the glass tube to obtain a cold cathode fluorescent tube 1a. Next, the prepared cold cathode fluorescent tube 1a of the present embodiment was discharged for 2000 hours under the condition that the tube current was fixed at 8 mA. Subsequently, the glass tube 2 was heated at a temperature of 240 ° C, and the amount of mercury emitted from the glass tube 2 was measured as a effective amount of mercury using a mercury measuring device in a fluorescent tube, and the measured enthalpy was 3.64 g. The amount of effective mercury described above corresponds to the amount of metallic mercury which is not consumed during the above discharge. Thereafter, the glass tube 2 was heated at a temperature of 900 ° C, and the amount of mercury emitted from the glass tube 2 was measured as the amount of mercury consumed, and the measured enthalpy was 0.04 g. The amount of mercury consumed is equivalent to the amount of mercury consumed by the phosphor consumed during the discharge and the compound adhering to the tube wall. The sum of the above-mentioned effective mercury amount and the above-mentioned consumed mercury amount corresponds to the total amount of mercury enclosed in the glass tube 2 when the cold cathode fluorescent tube 1a is produced. Then, the mercury consumption rate at the above discharge -17 - 201013738 was calculated according to the following formula (1). The results are shown in Table 4. Mercury consumption rate (%) = {% of mercury consumed (g) / total amount of mercury (g) } X 1 〇〇 (%) · · · ( 1 ) Next, a pair of bottomed cylindrical cold cathode fluorescent light is produced The electrode for the tube is the same as the embodiment except that the electrode material of the first embodiment is used, and the cold cathode fluorescent tube of the first example is fabricated, and the cold cathode fluorescent tube is coated on the inner wall. The glass tube having a length of 5 6 9 mm coated with a phosphor has the pair of electrodes described above. Subsequently, in the same manner as in the first embodiment, the cold cathode fluorescent tube of the present embodiment was discharged for 2 000 hours under the condition that the tube current was fixed at 8 mA, and the mercury consumption rate at the time of discharge was calculated. . The results are shown in Table 4. Then, in order to evaluate the service life of the cold cathode fluorescent tube 1 having the electrode 3 for the cold cathode fluorescent tube produced in the present embodiment, a cold cathode fluorescent tube lb was produced, which was cold. The cathode fluorescent tube 1b is identical to the cold cathode fluorescent tube 1a of the present embodiment except that the length of the glass tube 2 is 300 mm. Next, the cold cathode fluorescent tube 1b of the present example thus produced was discharged under the condition that the tube current was 8 mA, and the center luminance at this time was measured. Subsequently, by performing a Lehmann approximation on the obtained result, the time required for the center luminance of the cold cathode fluorescent tube lb to be halved is calculated. The results are shown in Fig. 5 and Table 5. Next, an electrode for a cold cathode fluorescent tube having a pair of bottomed cylindrical bodies is produced, and -18-201013738 is identical to the present embodiment except that the electrode material of Reference Example 1 is used. In the cold cathode fluorescent tube of the first example, the cold cathode fluorescent tube has the pair of electrodes inside the glass tube having a length of 300 mm. Subsequently, in the same manner as in the present embodiment, the cold cathode fluorescent tube of the present embodiment thus produced was discharged under the condition that the tube current was fixed at 8 mA, and the center luminance at the time of discharge was measured. Subsequently, the time required for halving the center luminance of the cold cathode fluorescent tube of the present embodiment was calculated by performing a Lehmann approximation on the obtained result. The results are shown in Fig. 5 and Table 5. (Embodiment 2) In this embodiment, the electrode material of this embodiment was fabricated. The electrode material was completely the same as that of the first embodiment except that an alloy containing relatively 6.6% by mass of Mo and the remainder being unavoidable impurities was used. Next, the Vickers hardness of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 200 HV. The results are shown in Table 1. Subsequently, the electrical resistivity of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 26.0 μΩ·cm. The results are shown in Table 1 and Figure 2. Then, with respect to the electrode material obtained in the present example, a test piece was prepared in exactly the same manner as in Example 1, and the sputtering of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. rate. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering rate of the electrode material of the present example was equivalent to 65%. The results are shown in Table 1. Thereafter, in the same manner as in the first embodiment, a pair of thin plate-shaped electrodes 3 for cold cathode fluorescent tubes were produced using the electrode material obtained in the present example, and a cold cathode tube C was formed, which was in the cold cathode tube C. The inner wall surface is not coated with the inside of the glass tube of the phosphor, and has the pair of electrodes 3 described above. Next, in the same manner as in the first embodiment, a tube current of 8 mA was applied between the pair of electrodes 3 of the formed cold cathode tube C, and the generated tube voltage was measured. The ratio of the tube voltage of the above-described cold cathode tube C to the tube voltage of the above-described cold cathode tube B is shown in Fig. 4 . (Embodiment 3) In this embodiment, the electrode material of this embodiment was produced. The electrode material was completely the same as that of the first embodiment except that an alloy containing a relatively total amount of Mo of 9.9% by mass, the remainder being Fe, and unavoidable impurities was used. Next, the Vickers hardness of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 291 HV. The results are shown in Table 1. Subsequently, the specific resistance of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 26.2 μΩ·(:πι. The results are shown in Table 1 and Fig. 2. Then, with respect to the present example The obtained electrode material was subjected to a test piece in exactly the same manner as in Example 1, and the sputtering rate of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering from -20 to 201013738. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering rate of the electrode material of the present embodiment was 71%. The results are shown in Table 1. Thereafter, it was identical to that of Example 1. In the manner of using the electrode material obtained in the present embodiment, a pair of thin plate-shaped electrodes 3 for cold cathode fluorescent tubes are produced, and a cold cathode tube D is formed, which is not coated with a phosphor on the inner wall surface. Inside the glass tube, the pair of electrodes 3 were provided. Next, in the same manner as in the first embodiment, a tube current of 8 mA was applied between the pair of electrodes 3 of the formed cold cathode tube D, and the generated tube voltage was measured. Shown in Figure 4 The ratio of the tube voltage of the cold cathode tube D to the tube voltage of the cold cathode tube B is described. (Embodiment 4) In the present embodiment, the electrode material of the present embodiment was fabricated. Except for the alloy containing a relatively total amount of 0.17 mass% of Mo, the remainder being Fe, and unavoidable impurities, the same as in the first embodiment. Next, in the same manner as in the first embodiment, the obtained by the present example was measured. The Vickers hardness of the electrode material, which is 1 13 HV. The results are shown in Table 1 . Subsequently, the resistivity of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 11. ΟμΩ κιη The results are shown in Table 1 and Fig. 2. Then, with respect to the electrode material obtained in the present example, a test piece was prepared in the same manner as in Example-21 - 201013738 by measuring the continuous sputtering. The weight of the test piece was reduced, and the sputtering rate of the electrode material was calculated. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering of the electrode material of the present example was carried out. The results are shown in Table 1. The results are shown in Table 1. Thereafter, a pair of thin plate-shaped electrodes for cold cathode fluorescent tubes 3 were produced in the same manner as in Example 1 using the electrode material obtained in the present example. The cold cathode tube E is provided, and the cold cathode tube E has the pair of electrodes 3 inside the glass tube to which the phosphor is not coated on the inner wall surface. Next, in the same manner as in the first embodiment, the cold is made. A tube current of 8 mA was applied between the pair of electrodes 3 of the cathode tube E, and the generated tube voltage was measured. Fig. 4 shows the ratio of the tube voltage of the cold cathode tube E to the tube voltage of the cold cathode tube B. (Embodiment 5) In the present embodiment, the electrode material of the present embodiment was produced. Regarding the electrode material, an alloy containing a relatively full amount of 1.7% by mass of Mo, the remainder being Fe, and unavoidable impurities was used. Other than the first embodiment, it is identical. Next, the Vickers hardness of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 149 HV. The results are shown in Table 1. Subsequently, the resistivity of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 15.4 μΩ κιη. The results are shown in Table 1 and Figure 2. -22- 201013738 Then, with respect to the electrode material obtained in the present example, a test piece was prepared in exactly the same manner as in Example 1, and the electrode was calculated by measuring the reduced weight of the test piece after continuous sputtering. The sputtering rate of the material. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering rate of the electrode material of the present example was equivalent to 57%. The results are shown in Table 1. Thereafter, in the same manner as in the first embodiment, a pair of thin plate-shaped electrodes 3 for cold cathode fluorescent tubes were produced using the electrode material obtained in the present example, and a cold cathode tube F was formed, and the cold cathode tube F was The inner wall surface is not coated with the inside of the glass tube of the phosphor, and has the pair of electrodes 3 described above. Next, in the same manner as in the first embodiment, a tube current of 8 mA was applied between the pair of electrodes 3 of the formed cold cathode tube F, and the generated tube voltage was measured. The ratio of the tube voltage of the above-described cold cathode tube F to the tube voltage of the above-described cold cathode tube B is shown in Fig. 4 . (Embodiment 6) In this embodiment, the electrode material of this embodiment was fabricated. The electrode material was completely the same as that of the first embodiment except that an alloy containing a relatively total amount of 5.0% by mass of Mo and the remainder being Fe and unavoidable impurities was used. Next, the Vickers hardness of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 175 HV. The results are shown in Table 1. Subsequently, the resistivity of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 23.8 μΩ·ί: ηη. The results are shown in Table 1 and Figure 2 in -23-201013738. Then, with respect to the electrode material obtained in the present example, a test piece was prepared in exactly the same manner as in the example, and the sputtering of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. rate. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering rate of the electrode material of the present example was equivalent to 5 7%. The results are shown in Table 1. Thereafter, in the same manner as in the first embodiment, a pair of thin plate-shaped electrodes 3 for cold cathode fluorescent tubes were produced using the electrode material obtained in the present example, and a cold cathode tube G was formed, and the cold cathode tube G was The inner wall surface is not coated with the inside of the glass tube of the phosphor, and has the pair of electrodes 3 described above. Next, in the same manner as in the first embodiment, a tube current of 8 mA was applied between the pair of electrodes 3 of the formed cold cathode tube G, and the generated tube voltage was measured. The ratio of the tube voltage of the above-described cold cathode tube G to the tube voltage of the above-described cold cathode tube B is shown in Fig. 4 . In this comparative example, the electrode material of this comparative example was produced. Regarding the electrode material, except that a metal consisting of substantially only Fe and the remainder being unavoidable impurities was used, 'others are identical to the first embodiment. Next, in the same manner as in the first embodiment, the comparison is performed. The Vickers hardness of the electrode material obtained in the example was 110 HV. The results are shown in Table 1. Subsequently, in the same manner as in the first embodiment, the electrical resistivity of the electrode material obtained by the comparison of -24-201013738, fg =, was measured, and the enthalpy was 1 〇.1 μίί·ςΐη. The results are not shown in Table 1 and Figure 2. Then, with respect to the electrode material obtained in the present comparative example, a test piece was prepared in exactly the same manner as in Example 1, and the sputtering of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. rate. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering rate of the electrode material of the comparative example was equivalent to 58%. The results are shown in Table 1. Thereafter, in the same manner as in the first embodiment, a pair of thin plate-shaped electrodes for cold cathode fluorescent tubes were fabricated using the electrode material obtained in the comparative example, and a cold cathode tube was formed, and the cold cathode tube was The inner wall surface is not coated with the inside of the glass tube of the phosphor, and has the pair of electrodes. Then, in the same manner as in the first embodiment, a tube current of 5 mA, 6 mA, 7 mA, and 8 mA was applied between the pair of electrodes of the formed cold cathode tube, and the tubes generated for the respective tube currents were respectively measured. Voltage. The results are shown in Figure 3. The ratio of the voltage of the tube 10 of the above-mentioned cold cathode tube 相对 to the tube voltage of the above-mentioned cold cathode tube 示出 is shown in Fig. 4 . Subsequently, in the same manner as in the first embodiment, the surface composition of the electrode for the cold cathode fluorescent tube of the above cold cathode tube and the composition of the inner wall surface of the glass tube were measured by enthalpy. The results are shown in Table 2 and Table 3. In this comparative example, the electrode material of this comparative example was produced. Regarding the electrode material, except that an alloy containing a relatively total amount of 15.3 mass% of Mo, the remainder being Ni, and unavoidable impurities was used, it was exactly the same as that of the first embodiment. Next, the Vickers hardness of the electrode material obtained in the present comparative example was measured in the same manner as in Example 1, and the enthalpy was 305 HV. The results are shown in Table 1. Subsequently, the resistivity of the electrode material obtained in the present comparative example was measured in the same manner as in Example 1, and the enthalpy was 72·6 μΩ·( ΐ 。. The results are shown in Table 1. Then, regarding the electrode obtained by the present comparative example Materials, a test piece was prepared in exactly the same manner as in Example 1, and the sputtering rate of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. When the electrode of Reference Example 1 was used When the sputtering rate of the material was set to 100%, the sputtering rate of the electrode material of the comparative example was equivalent to 11%. The results are shown in Table 1. Thereafter, in the same manner as in Example 1, the use was carried out. In the electrode material obtained in the comparative example, a pair of thin plate-shaped electrodes for cold cathode fluorescent tubes were produced, and a cold cathode tube J was formed. The cold cathode tube J has the inside of a glass tube on which the phosphor is not coated on the inner wall surface. Next, in the same manner as in the first embodiment, the surface composition of the electrode for the cold cathode fluorescent tube of the cold cathode tube J and the composition of the inner wall surface of the glass tube were measured by ΕΡΜΑ. The results are shown in Table 2 and Table. 3 (Comparative Example 3) In this comparative example, the electrode material of the comparative example was produced, and the electrode material was used except that Mo was contained in a relatively total amount of 16.0% by mass, the remainder was Fe, and unavoidable impurities were used. In addition to the alloy, it is -26-201013738 which is identical to the first embodiment. Next, in the same manner as in the first embodiment, the Vickers hardness of the electrode material obtained in this comparative example was measured, and the enthalpy was 490 HV. In the following Table 1. The resistivity of the electrode material obtained in the present comparative example was measured in the same manner as in Example 1, and the enthalpy was 33·6 μΩ·ηη. The results are shown in Table 1 and Fig. 2 . Then, with respect to the electrode material obtained in this comparative example, a test piece was prepared in exactly the same manner as in Example 1, and the sputtering of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering rate of the electrode material of the comparative example was equivalent to 65%. The results are shown in Table 1 and thereafter, and the examples. One finish In the same manner, a pair of thin plate-shaped electrodes for cold cathode fluorescent tubes were produced using the electrode material obtained in the comparative example, and a cold cathode tube was formed, which was not coated with φ phosphor on the inner wall surface. The inside of the glass tube was provided with the above-mentioned pair of electrodes. Next, in the same manner as in the first embodiment, a tube current of 8 mA was applied between a pair of the electrodes of the formed cold cathode tube, and the generated tube voltage was measured. The ratio of the tube voltage of the cold cathode tube K to the tube voltage of the cold cathode tube B is shown in Fig. 4. (Comparative Example 4) In this comparative example, the electrode material of this comparative example was produced. The electrode material was identical to that of the first embodiment except that an alloy containing a relatively total amount of 23.3% by mass of Mo -27-201013738, the remainder being Fe, and unavoidable impurities was used. Next, the Vickers hardness of the electrode material obtained in this comparative example was measured in the same manner as in Example 1, and the enthalpy was 493 HV. The results are shown in Table 1. Subsequently, the specific resistance of the electrode material obtained in the present comparative example was measured in the same manner as in Example 1, and the enthalpy was 36·2 μΩ·(: ηι. The results are shown in Table 1 and Fig. 2. Then, regarding the comparison For the electrode material obtained in the same manner as in the first embodiment, a test piece was prepared, and the sputtering rate of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. When the sputtering rate of the electrode material of Example 1 was set to 100%, the sputtering rate of the electrode material of the comparative example was 83%. The results are shown in Table 1. Thereafter, in exactly the same manner as in the first embodiment, A pair of thin plate-shaped electrodes for cold cathode fluorescent tubes were produced using the electrode material obtained in the comparative example, and a cold cathode tube L was formed. The cold cathode tube L was inside the glass tube to which the phosphor was not coated on the inner wall surface. There is a pair of electrodes described above. Next, in the same manner as in the first embodiment, a tube current of 8 mA was applied between a pair of the above-mentioned electrodes of the formed cold cathode tube L, and the generated tube voltage was measured. Out of the above cold cathode tube L Tube voltage than the tube voltage to the cold cathode tube relative to the B. -28-201013738 (Table 1)

Mo mm%) Fe (質量%) Ni (MM%) 維氏硬度 (HV) 電阻率 (μΩ-cm、 濺射率 (%) 參考例一 - - 100* 75 4.6 100 實施例一 3.4 剩餘部分* 一 156 19.7 59 實施例二 6.6 剩餘部分* 一 200 26.0 65 實施例三 9.9 剩餘部分* 一 291 26.2 71 實施例四 0.17 剩餘部分* 一 113 11.0 58 實施例五 1.7 剩餘部分* 一 149 15.4 57 實施例六 5.0 剩餘部分* 175 卜 23.8 57 比較例一 — 100* — 110 10.1 58 比較例二 15.3 一 餘部分* 305 72.6 111 比較例三 16.0 剩餘部分* 一 490 33.6 65 比較例四 23.3 剩餘部分* 一 493 36.2 83 *:包含不可避免的不純物 從表1可以明顯看出,實施例一〜實施例六的電極材 料與比較例二的電極材料相比,維氏硬度較小,加工性優 良。上述實施例一〜實施例六的電極材料由含量爲相對全 量爲0.17〜9.9質量%範圍內的Mo、以及剩餘部分實質上 爲Fe的合金構成。而上述比較例二的電極材料由含量爲 ® 相對全量爲15.3質量%範圍內的Mo、以及剩餘部分實質 上爲Ni的合金構成。一般對於金屬材料來說,維氏硬度 較低的材料冷塑加工性較爲優良,維氏硬度要是在3 00HV 以下,則容易進行冷加工。所以,從表1的結果可以明顯 看出,實施例一 ~實施例六的電極材料可容易加工成實施 例1的冷陰極螢光管用電極3。 同時,從表1可以明顯看出,比較例二的電極材料的 濺射率比參考例一的電極材料要大。上述比較例二的電極 材料由含量爲相對全量爲15.3質量%範圍內的Mo、剩餘 -29- 201013738 部分實質上爲Ni的合金構成。上述參考例一的電極材料 實質上僅由Ni構成。而另一方面,明顯可以看出實施例 一〜實施例六的電極材料的濺射率比參考例一的電極材料 要小。上述實施例一〜實施例六的電極材料由含量爲相對 全量爲0.17〜9.9質量%範圍內的Mo、剩餘部分實質上爲 Fe的合金構成。所以,可以明顯得出實施例一〜實施例六 的電極材料因濺射率小而具備優良的抗濺射性。 另外,從圖2可以明顯看出Mo含量越大、電阻率越 大,因而明顯可以得出實施例一〜實施例六的電極材料的 放電特性較爲優良。特別是因爲當Mo的含量爲相對於全 量超過1 〇質量%時,電阻率急劇上升,因此可以明顯看 出在含有Mo且由Fe基合金構成的電極材料中,較爲理 想的是將Mo的含量設定爲相對於全量在10質量%以下。 此外,從圖3可以明顯看出,實施例一的冷陰極螢光 管用電極3與實質上僅由Fe構成的比較例一的冷陰極螢 光管用電極相比,儘管Mo的含量少,但管電壓小。上述 實施例一的冷陰極螢光管用電極3由含量爲相對全量爲 3.4質量%的Mo、剩餘部分實質上爲Fe的合金構成。同 時,明顯可以看出,使用實施例一的冷陰極螢光管用電極 3時的管電壓,與使用參考例二的實質上僅由Mo構成的 冷陰極螢光管用電極時的管電壓較爲接近。所以,明顯可 知實施例一的冷陰極螢光管用電極3的管電壓較低,能源 效率較爲良好。Mo mm%) Fe (% by mass) Ni (MM%) Vickers hardness (HV) Resistivity (μΩ-cm, sputtering rate (%) Reference Example 1 - - 100* 75 4.6 100 Example I 3.4 Remaining part* 156 19.7 59 Example 2 6.6 Remaining part * A 200 26.0 65 Example 3 9.9 Remaining part * A 291 26.2 71 Example 4 0.17 Remaining part * A 113 11.0 58 Example V 1.7 Remaining part * A 149 15.4 57 Example Six 5.0 Remaining part * 175 Bu 23.8 57 Comparative Example 1 - 100* - 110 10.1 58 Comparative Example 2 15.3 Remaining part * 305 72.6 111 Comparative Example 3 16.0 Remaining part * One 490 33.6 65 Comparative Example 4 23.3 Remaining part * One 493 36.2 83 *: Containing unavoidable impurities As apparent from Table 1, the electrode materials of Examples 1 to 6 have smaller Vickers hardness and excellent workability than the electrode materials of Comparative Example 2. The electrode material of the first to sixth embodiments is composed of an alloy containing Mo in a range of from 0.17 to 9.9% by mass relative to the total amount, and an alloy partially remaining Fe. The electrode material of the above Comparative Example 2 is made of a relative amount of ® The amount of Mo in the range of 15.3 mass% and the alloy in which the remainder is substantially Ni. Generally, for metal materials, the material having a lower Vickers hardness is more excellent in cold plastic workability, and the Vickers hardness is at 300 HV. In the following, it is easy to carry out cold working. Therefore, it is apparent from the results of Table 1 that the electrode materials of the first to sixth embodiments can be easily processed into the electrode 3 for the cold cathode fluorescent tube of the first embodiment. It can be clearly seen that the sputtering rate of the electrode material of Comparative Example 2 is larger than that of the electrode material of Reference Example 1. The electrode material of the above Comparative Example 2 is composed of Mo in a range of 15.3 mass% relative to the total amount, and remaining -29- 201013738 Partially composed of an alloy of Ni. The electrode material of the above Reference Example 1 consists essentially of only Ni. On the other hand, it is apparent that the sputtering rate of the electrode materials of Examples 1 to 6 is higher than that of the reference example. The electrode material of one of the above embodiments is small. The electrode material of the first embodiment to the sixth embodiment is composed of Mo in a range of from 0.17 to 9.9% by mass relative to the total amount, and the remainder is substantially Fe. Therefore, it is apparent that the electrode materials of the first to sixth embodiments have excellent sputtering resistance due to a small sputtering rate. Further, it is apparent from Fig. 2 that the larger the Mo content and the higher the specific resistance Therefore, it is apparent that the electrode materials of the first to sixth embodiments have excellent discharge characteristics. In particular, when the content of Mo is more than 1% by mass relative to the total amount, the electrical resistivity sharply rises, so it is apparent that in the electrode material containing Mo and composed of a Fe-based alloy, it is preferable to use Mo. The content is set to be 10% by mass or less based on the total amount. Further, as is apparent from Fig. 3, the electrode 3 for the cold cathode fluorescent tube of the first embodiment is smaller than the electrode for the cold cathode fluorescent tube of the first comparative example consisting of only Fe, although the content of Mo is small. The voltage is small. The electrode 3 for cold cathode fluorescent tubes of the first embodiment described above is composed of an alloy having a content of relatively 3.4 mass% of Mo and a remainder of substantially Fe. Meanwhile, it is apparent that the tube voltage when the electrode 3 for the cold cathode fluorescent tube of the first embodiment is used is closer to the tube voltage when the electrode for the cold cathode fluorescent tube consisting of substantially only Mo is used in Reference Example 2. . Therefore, it is apparent that the electrode 3 for the cold cathode fluorescent tube of the first embodiment has a low tube voltage and is excellent in energy efficiency.

並且,從圖4可以明顯看出,當將管電流設爲8mA -30- 201013738 時,實施例一〜實施例六的冷陰極螢光管用電極3與比較 例一的實質上僅由Fe構成的冷陰極螢光管用電極相比, 管電壓較小。上述實施例一〜實施例六的冷陰極營光管用 電極3由含量爲相對全量爲0.17〜9.9質量%範圍內的Mo 、剩餘部分實質上爲Fe的合金構成。另外,明顯可知: Mo的含量爲相對全量爲1.5〜5.5質量%範圍內、剩餘部分 實質上爲Fe的實施例一、五、六的冷陰極螢光管用電極 3因管電壓特別低,能源效率較爲良好。 (表2 ) 電極表1 5的組成(質量%) Mo Fe Ni Hg 0 實施例一 3.6 96.4 — — — 比較例一 — 97.5 — 2.5 — 比較例二 10.52 — 68.69 — 20.79 未檢測出 φ (表 3) \ 玻璃管內壁面的組成(質量%) Mo Fe Ni Hg 0 Na A1 Si K 實施例一 — 3.3 — — 56.8 0.7 1.8 31.9 5.5 比較例一 — 3.9 — — 57.1 0.6 1.7 31.2 5.5 比較例二 1.5 一 43.33 1.2 46.16 — 0.38 6.47 0.96 -:未檢測出 另外,從表2可以明確知道,在冷陰極管A(具有實 施例一的薄板狀的冷陰極螢光管用電極3)中,該電極3 的表面上並不存在Hg原子。並且,從表3可以明顯看出 -31 - 201013738 ,在上述冷陰極管A中,玻璃管的內壁面上有相對全量 爲3.3質量%的Fe原子,但並不存在Hg原子。這個可以 認爲是由於冷陰極螢光管用電極3的表面上有Mo存在。 所以,在上述冷陰極管A中,雖然構成上述電極3的Fe 原子些微被濺射,但是該電極3的表面和玻璃管的內壁面 兩處並沒有形成合金(汞合金(amalgam ))。由此,可 以明確知道,冷陰極管A不會有因汞合金的形成而消耗 玻璃管內的Hg,能夠延長該冷陰極管A的使用壽命。 另一方面,從表2可以明顯看出,在冷陰極管Η (具 有比較例一的薄板狀的冷陰極螢光管用電極)中,該電極 的表面上存在相對全量爲2.5質量%的Hg原子。所以, 明顯可知,在冷陰極管Η中,雖然只是微量,但是Fe和 Hg在上述電極表面上進行了反應。因此明確可知,冷陰 極管Η由於汞合金的形成,消耗了玻璃管內的Hg,該冷 陰極管Η的使用壽命變短。 此外,從表3可知,在冷陰極管J (具有比較例二的 薄板狀的冷陰極螢光管用電極)中,在玻璃管內壁面上存 在有相對全量爲1.5質量%的Mo原子、44.3 3質量%的Ni 原子以及1.2質量%的Hg原子。所以,明顯可知,在冷 陰極管J中,構成上述電極的Mo原子以及Ni原子被大 量濺射並附著在玻璃管的內壁面上,形成了易與Hg起反 應的Ni和Hg構成的汞合金。因此明確可知,冷陰極管J 由於汞合金的形成,消耗了玻璃管內的Hg’該冷陰極管J 的使用壽命變短。 -32- 201013738 所以,可以明確知道:在內壁面塗敷螢光體的玻璃管 2的內部具有上述各實施例一 ~實施例六的冷陰極螢光管 用電極3的冷陰極螢光管1,因不會由於汞合金的形成而 消耗玻璃管內的Hg’能夠延長該螢光管1的壽命。Further, as is apparent from Fig. 4, when the tube current is set to 8 mA -30 to 201013738, the electrode 3 for cold cathode fluorescent tubes of the first to sixth embodiments and the electrode 3 of the first embodiment are substantially composed only of Fe. The tube voltage of the cold cathode fluorescent tube is smaller than that of the electrode. The cold cathode camping tube electrode 3 of the above-described first to sixth embodiments is composed of an alloy having a content of Mo in a range of from 0.17 to 9.9 mass% relative to the total amount and a Fe content substantially in the remainder. Further, it is apparent that the electrode 3 for cold cathode fluorescent tubes of Examples 1, 5, and 6 in which the content of Mo is in the range of 1.5 to 5.5% by mass relative to the total amount and the remainder is substantially Fe is particularly low in tube voltage, and energy efficiency. More good. (Table 2) Composition of electrode table 15 (% by mass) Mo Fe Ni Hg 0 Example 1 3.6 96.4 — — — Comparative Example 1 — 97.5 — 2.5 — Comparative Example 2 10.52 — 68.69 — 20.79 φ was not detected (Table 3 \ Composition of the inner wall of the glass tube (% by mass) Mo Fe Ni Hg 0 Na A1 Si K Example 1 - 3.3 - 56.8 0.7 1.8 31.9 5.5 Comparative Example 1 - 3.9 - 57.1 0.6 1.7 31.2 5.5 Comparative Example II 1.5 43.33 1.2 46.16 — 0.38 6.47 0.96 -: Not detected. Further, it can be clearly seen from Table 2 that the surface of the electrode 3 is in the cold cathode tube A (electrode 3 having the thin plate-shaped cold cathode fluorescent tube of the first embodiment). There is no Hg atom on it. Further, as apparent from Table 3, in the above-mentioned cold cathode tube A, the inner wall surface of the glass tube has a relatively total amount of 3.3% by mass of Fe atoms, but there is no Hg atom. This is considered to be due to the presence of Mo on the surface of the electrode 3 for the cold cathode fluorescent tube. Therefore, in the above-described cold cathode tube A, although the Fe atoms constituting the electrode 3 are slightly sputtered, an alloy (amalgam) is not formed on the surface of the electrode 3 and the inner wall surface of the glass tube. From this, it is clear that the cold cathode tube A does not consume Hg in the glass tube due to the formation of the amalgam, and the service life of the cold cathode tube A can be prolonged. On the other hand, as is apparent from Table 2, in the cold cathode tube Η (the electrode for the cold cathode fluorescent tube having a thin plate shape of Comparative Example 1), a relatively total amount of Hg atoms of 2.5% by mass is present on the surface of the electrode. . Therefore, it is apparent that in the cold cathode tube crucible, although only a trace amount is present, Fe and Hg react on the surface of the above electrode. Therefore, it is clear that the cold cathode tube consumes Hg in the glass tube due to the formation of the amalgam, and the service life of the cold cathode tube is shortened. Further, as is clear from Table 3, in the cold cathode tube J (the electrode for the thin-plate cold cathode fluorescent tube of Comparative Example 2), a relatively total amount of 1.5% by mass of Mo atoms and 44.3 3 were present on the inner wall surface of the glass tube. Mass% of Ni atoms and 1.2% by mass of Hg atoms. Therefore, it is apparent that in the cold cathode tube J, Mo atoms and Ni atoms constituting the above electrode are sputtered in a large amount and adhere to the inner wall surface of the glass tube, forming an amalgam composed of Ni and Hg which are easily reacted with Hg. . Therefore, it is clear that the cold cathode tube J consumes Hg' in the glass tube due to the formation of the amalgam, and the service life of the cold cathode tube J becomes short. -32-201013738 Therefore, it is clear that the inside of the glass tube 2 coated with the phosphor on the inner wall surface has the cold cathode fluorescent tube 1 of the electrode 3 for the cold cathode fluorescent tube of each of the first to sixth embodiments, Since the Hg' in the glass tube is not consumed due to the formation of the amalgam, the life of the fluorescent tube 1 can be prolonged.

實施例一 參考例一 有效水銀量(g) 3.64 2.11 消耗水銀量(g) 0.04 0.27 總冰銀量(g) 3.68 2.3B 水銀消耗率(%) 1.09 11.34 從表4明確可知,實施例一的冷陰極螢光管用電極3 與參考例一的實質上僅由Ni構成的冷陰極螢光管用電極 相比,水銀消耗率格外低。上述實施例一的冷陰極螢光管 用電極3由含量爲相對全量爲3.4質量%的Mo、剩餘部分 實質上爲Fe的合金構成。所以可知,實施例一的冷陰極 〇 螢光管1的玻璃管2內的Hg的消耗非常少’能夠延長該 螢光管1的使用壽命。 (實施例七) 在本實施例中,製成了本實施例的電極材料。關於該 電極材料,除了使用了含有相對全量爲3.4質量%的Mo、 相對全量爲0.6質量%的Ru、以及剩餘部分爲Fe以及不 可避免的不純物的合金之外,其他與實施例一完全相同。 接著,以與實施例一完全相同的方式’測定由本實施 -33- 201013738 例得到的電極材料的維氏硬度,其値爲153HV。 隨後,以與實施例一完全相同的方式,測定由本實施 例得到的電極材料的電阻率,其値爲22.1 μΩ·cm。 然後,關於由本實施例得到的電極材料,以與實施例 一完全相同的方式,製成試驗片,藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。當 將參考例一的電極材料的濺射率設定爲100%時,本實施 例的電極材料的濺射率相當於7 1 %。 其後,以與實施例一完全相同的方式,使用從本實施 例中得到的電極材料製作一對有底筒狀體的冷陰極螢光管 用電極3,並製成冷陰極螢光管1,該冷陰極螢光管1在 內壁面塗敷有螢光體的長3 0 0mm的玻璃管2內部,具有 上述電極3。 隨後,除了使用了由本實施例得到的冷陰極螢光管1 以外,其餘與本實施例完全相同,測定在管電流8mA固 定的條件下放電時的中心亮度,藉由對得出的結果進行萊 曼(Lehmann )近似,計算出冷陰極螢光管1的中心亮度 減半所需的時間。並將結果示於圖5及表5中。 (表5 ) 預測使用壽命減半的時間 (時間) 實施例一 333000 實施例七 480000 參考例一 213000 201013738 根據圖5以及表5可以推測出,實施例一的冷陰極螢 光管1與參考例一的冷陰極螢光管相比,中心亮度減半所 需的時間較長,而實施例七的冷陰極螢光管1與實施例一 的冷陰極螢光管1相比,中心亮度減半所需的時間更長。 所以,明顯可知,特別是實施例七的冷陰極螢光管1能夠 延長使用壽命。 上述實施例一的冷陰極螢光管1具有含量爲相對全量 爲3.4質量%的Mo、剩餘部分實質上爲Fe的冷陰極螢光 管用電極3。上述實施例七的冷陰極螢光管1具有含量爲 相對全量爲3.4質量%的Mo、相對全量爲〇.6質量%的Ru 、剩餘部分實質上爲1^的冷陰極螢光管用電極3°上述 參考例一的冷陰極螢光管具有實質上僅由Ni構成的冷陰 極螢光管用電極。 (實施例八) 在本實施例中’首先’藉由在真空熔解爐中將Fe、 Mo以及Nb熔解,調製成熔液並進行鑄造,製成約重 10kg的鑄錠。上述鑄錠含有相對全量爲3·4質量%的Mo 與1.6質量。/。的Nb、剩餘部分由Fe及不可避免的不純物 的合金構成。上述不可避免的不純物含有相對上述合金的 全量爲〇.1〇質量。以下的c、0·50質量%以下的Si、〇_80 質量%以下的Mu、〇.〇5質量%以下的P、以及0·50質量% 以下的S ° 接著,除了使用了由本實施例得到的鑄錠以外,其他 -35- 201013738 以與實施例一完全相同的方式製作本實施例的電極材料。 隨後,以與實施例一完全相同的方式,使用本實施例 中得到的電極材料製成試驗片,並藉由測定經連續濺射後 的該試驗片減少的重量,計算出該電極材料的濺射率。 然後,對於實質上僅由Ni構成、剩餘部分爲不可避 免的不純物的電極材料(參考例三),與本實施例完全相 同,製成試驗片,藉由測定經連續濺射後的該試驗片減少 的重量,計算出該電極材料的濺射率。將參考例三的電極 材料的濺射率設定爲100%時,本實施例的電極材料的濺 射率相當於69.1%。結果示於表6中。 接著,爲了對本實施例中得到的電極材料的加工性進 行評價,進行了張力試驗。首先,對由本實施例得到的上 述鑄錠,施以溫度11 00 °C的熱锻,並反覆進行常溫下的 冷壓延、以及氫環境下溫度 800 °C的退火。在氫環境下 800 °C的退火進行10分鐘後,藉由冷卻至常溫,製成圓棒 試驗片。上述圓棒試驗片具有作爲平行部的小徑部、和在 該試驗片兩端的大徑部,平行部長24mm、直徑爲8mm。 隨後,對該圓棒試驗片進行張力速度爲2 4mm/秒的張 力試驗,測定張力強度爲502N/mm2。並且,測定張力試 驗後的圓棒試驗片的平行部的長度以及直徑,計算出張力 試驗的延伸率及頸縮率,延伸率爲34.9%、頸縮率爲 59.6%。結果示於表7中。 然後,針對參考例三的電極材料,以與本實施例完全 相同的方式’製作圓棒試驗片,並進行張力試驗,測定張 -36- 201013738 力強度的同時,計算出延伸率以及頸縮率,分別 強度爲36lN/mm2、延伸率爲18.8%、頸縮率爲 果示於表7中。 接著,以與實施例一完全的方式,使用由本 到的電極材料製成兩對本實施例的薄板狀的冷陰 用電極3。 隨後,爲了對由本實施例得到的冷陰極螢光 A 3的性能進行評價,以與本實施例一完全相同的 成冷陰極管Μ,該冷陰極管Μ在內壁面沒被塗 的直徑爲3mm、長爲3 00mm的玻璃管內部,具 板狀的該電極3。 然後,以管電流6mA固定的條件下,使上 管Μ放電300小時後,開封該冷陰極管M,並 極螢光管用電極3。接著,爲了檢査有無從冷陰 用電極3濺射出的原子以及與Hg的反應,藉由 φ 定冷陰極螢光管用電極3的表面組成以及上述玻 面的組成。結果,將在冷陰極螢光管用電極3的 玻璃管的內壁上有無水銀原子示於表8中。 接著,除了使用了參考例三的電極材料之外 本實施例完全相同的方式,製作一對薄板狀的冷 管用電極,製成具有該電極的冷陰極管N (參考 針對得到的冷陰極管N,以與本實施例一完全相 ,藉由ΕΡΜΑ測定冷陰極螢光管用電極的表面組 璃管內壁面的組成。結果示於表8中。 得出張力 6.4%。結 實施例得 極螢光管 管用電極 方式,製 敷螢光體 有一對薄 述冷陰極 取出冷陰 極螢光管 ΕΡΜΑ 測 璃管內壁 表面以及 ,其餘與 陰極螢光 例三)。 同的方式 成以及玻 -37- 201013738 爲了對由本實施例得到的冷陰極螢光管用電極3的性 能進行評價,以與實施例一完全相同的方式,製成冷陰極 螢光管lc,該冷陰極螢光管lc在內壁面被塗敷了螢光體 的直徑爲3mm、長爲300mm的玻璃管2內部,具有一對 薄板狀的上述電極3。 接著,對製成的本實施例的冷陰極螢光管1的一對上 述電極3之間分別施加5mA、6mA、7mA、8mA的管電流 ,並分別測定針對各個管電流產生的管電壓。結果示於圖 6中。 然後,除了使用了參考例一的電極材料以外,其他以 與本實施例完全相同的方式,製成一對冷陰極螢光管用電 極,並製成具有該電極的冷陰極螢光管(參考例三)。對 製成的冷陰極螢光管的一對上述電極之間分別施加5mA、 6mA、7mA、8mA的管電流,並分別測定針對各個管電流 產生的管電壓。結果示於圖6中。 (比較例五) 在本比較例中,製成了本比較例的電極材料。關於該 電極材料,除了使用實質上僅由Mo構成、剩餘部分爲不 可避免的不純物的金屬之外,其他與實施例八完全相同。 接著,與實施例八完全相同,使用由本比較例得到的 電極材料製成試驗片,藉由測定經連續濺射後的該試驗片 減少的重量’計算出該電極材料的濺射率。將參考例三的 電極材料的濺射率設定爲100%時,本比較例的電極材料 -38- 201013738 的濺射率相當於83.4%。結果示於表6中。 隨後,以與實施例八完全相同的方式,對由本比較例 得到的電極材料製作圓棒試驗片,並進行張力試驗,測定 張力強度的同時,計算出延伸率以及頸縮率,分別得出張 力強度爲33 5N/mm2、延伸率爲2.4%、頸縮率爲1.6%。 結果示於表7中。 然後’以與實施例八完全相同的方式,使用由本比較 ❹ 例得到的電極材料,製成一對薄板狀的冷陰極螢光管用電 極,並製成冷陰極管P,該冷陰極管P在內壁面沒被塗敷 螢光體的玻璃管內部,具有上述一對電極。 接著,針對上述冷陰極管P,以與實施例八完全相同 的方式’藉由ΕΡΜΑ測定冷陰極螢光管用電極的表面組成 以及玻璃管內壁面的組成。結果示於表8中。 隨後,以與實施例八完全相同的方式,使用由本比較 例得到的電極材料,製成一對薄板狀的冷陰極螢光管用電 φ 極’並製成冷陰極螢光管,該冷陰極螢光管在內壁面塗敷 有螢光體的玻璃管內部,具有上述一對電極。對製成的冷 陰極螢光管的一對上述電極之間分別施加5mA、6mA、 7mA、8mA的管電流,並分別測定針對各個管電流產生的 管電壓。結果示於圖6中。 (比較例六) 在本比較例中,製成了本比較例的電極材料。關於該 電極材料,除了使用實質上僅由Fe構成、剩餘部分爲不 -39- 201013738 , 可避免的不純物的金屬之外,其他與實施例八完全相同。 然後,以與實施例八完全相同的方式,使用由本比較 例得到的電極材料,製成一對薄板狀的冷陰極螢光管用電 極,並製成冷陰極管Q,該冷陰極管Q在內壁面沒被塗敷 螢光體的玻璃管內部,具有上述一對電極。 接著,針對上述冷陰極管Q,以與實施例八完全相同 的方式,藉由ΕΡΜΑ測定冷陰極螢光管用電極的表面組成 以及玻璃管內壁面的組成。結果示於表8中。 隨後,以與實施例八完全相同的方式,使用由本比較 例得到的電極材料,製成一對薄板狀的冷陰極螢光管用電 極,並製成冷陰極螢光管,該冷陰極螢光管在內壁面塗敷 有螢光體的玻璃管內部,具有上述一對電極。對製成的冷 陰極螢光管的一對上述電極之間分別施加5mA、6mA、 7mA、8mA的管電流,並分別測定針對各個管電流產生的 管電壓。結果示於圖6中。Example 1 Reference Example 1 Effective Mercury Amount (g) 3.64 2.11 Mercury Consumption (g) 0.04 0.27 Total Ice Silver (g) 3.68 2.3B Mercury Consumption Rate (%) 1.09 11.34 As is clear from Table 4, Example 1 The electrode for cold cathode fluorescent tube 3 is particularly low in mercury consumption compared with the electrode for cold cathode fluorescent tube which is substantially composed of Ni only in Reference Example 1. The electrode 3 for a cold cathode fluorescent tube of the first embodiment described above is composed of an alloy having a content of 3.4% by mass relative to the total amount of Mo and a remainder of substantially Fe. Therefore, it is understood that the consumption of Hg in the glass tube 2 of the cold cathode 萤 fluorescent tube 1 of the first embodiment is extremely small, and the life of the fluorescent tube 1 can be prolonged. (Embodiment 7) In this embodiment, the electrode material of this embodiment was produced. The electrode material was completely the same as that of the first embodiment except that an alloy containing a relatively total amount of 3.4% by mass of Mo, a relative amount of 0.6% by mass of Ru, and the remainder being Fe and an unavoidable impurity was used. Next, the Vickers hardness of the electrode material obtained in the example of the present invention - 33 - 201013738 was measured in exactly the same manner as in Example 1, and the enthalpy was 153 HV. Subsequently, the electrical resistivity of the electrode material obtained in the present example was measured in the same manner as in Example 1, and the enthalpy was 22.1 μΩ·cm. Then, with respect to the electrode material obtained in the present example, a test piece was prepared in exactly the same manner as in Example 1, and the sputtering of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. rate. When the sputtering rate of the electrode material of Reference Example 1 was set to 100%, the sputtering rate of the electrode material of the present example was equivalent to 71%. Thereafter, in the same manner as in the first embodiment, a pair of bottomed cylindrical cold cathode fluorescent tube electrodes 3 are produced using the electrode material obtained in the present embodiment, and a cold cathode fluorescent tube 1 is formed. The cold cathode fluorescent tube 1 is provided inside the glass tube 2 having a length of 300 mm of a phosphor coated on the inner wall surface, and has the electrode 3. Subsequently, except that the cold cathode fluorescent tube 1 obtained in the present embodiment was used, the same as in the present example, the center luminance at the time of discharge under a condition of a tube current of 8 mA was measured, and the result was obtained by The Lehmann approximation calculates the time required to halve the center luminance of the cold cathode fluorescent tube 1. The results are shown in Fig. 5 and Table 5. (Table 5) Time (time) for halving the service life. Example 1 333000 Example 7 480000 Reference Example 1 213000 201013738 According to FIG. 5 and Table 5, the cold cathode fluorescent tube 1 of the first embodiment and the reference example can be inferred. Compared with the cold cathode fluorescent tube of the first embodiment, the time required for halving the center luminance is longer, and the cold cathode fluorescent tube 1 of the seventh embodiment is halved compared with the cold cathode fluorescent tube 1 of the first embodiment. It takes longer. Therefore, it is apparent that the cold cathode fluorescent tube 1 of the seventh embodiment in particular can extend the service life. The cold cathode fluorescent tube 1 of the first embodiment described above has the electrode 3 for a cold cathode fluorescent tube having a content of 3.4% by mass relative to the total amount of Mo and a remaining portion substantially Fe. The cold cathode fluorescent tube 1 of the above-described seventh embodiment has an electrode having a content of about 3.4% by mass relative to the total amount of Mo, a relative amount of 6% by mass of Ru, and a remaining portion of substantially 1^ of the cold cathode fluorescent tube electrode. The cold cathode fluorescent tube of the above-mentioned Reference Example 1 has an electrode for a cold cathode fluorescent tube which is substantially composed only of Ni. (Embodiment 8) In the present embodiment, in the first place, Fe, Mo, and Nb were melted in a vacuum melting furnace to prepare a molten metal and cast, thereby producing an ingot having a weight of about 10 kg. The ingot described above contains Mo and 1.6 masses in a relative total amount of 3.4% by mass. /. The Nb and the remainder are composed of Fe and an alloy of unavoidable impurities. The above unavoidable impurities contain a total mass of 〇.1 相对 relative to the above alloy. The following c, 0.50% by mass or less of Si, 〇_80% by mass or less of Mu, 〇.〇5 mass% or less of P, and 0.50% by mass or less of S °, respectively, except that the present embodiment is used. Other than the obtained ingot, the other -35-201013738 was fabricated in the same manner as in the first embodiment. Subsequently, in the same manner as in the first embodiment, the test piece was prepared using the electrode material obtained in the present example, and the sputtering of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. Rate of incidence. Then, an electrode material (Reference Example 3) consisting essentially of only Ni and the remainder being unavoidable impurities was prepared in the same manner as in the present example, and a test piece was prepared by measuring the test piece after continuous sputtering. The reduced weight was calculated and the sputtering rate of the electrode material was calculated. When the sputtering rate of the electrode material of Reference Example 3 was set to 100%, the sputtering rate of the electrode material of the present embodiment was equivalent to 69.1%. The results are shown in Table 6. Next, in order to evaluate the workability of the electrode material obtained in the present example, a tensile test was conducted. First, the ingot obtained in the present example was subjected to hot forging at a temperature of 1100 °C, and was repeatedly subjected to cold rolling at normal temperature and annealing at 800 °C in a hydrogen atmosphere. After annealing at 800 ° C for 10 minutes in a hydrogen atmosphere, the test piece was rounded by cooling to room temperature. The round bar test piece had a small diameter portion as a parallel portion and a large diameter portion at both ends of the test piece, and had a parallel length of 24 mm and a diameter of 8 mm. Subsequently, the round bar test piece was subjected to a tensile test at a tension speed of 24 mm/sec, and the tensile strength was measured to be 502 N/mm2. Further, the length and the diameter of the parallel portion of the round bar test piece after the tensile test were measured, and the elongation and the necking ratio of the tensile test were calculated, and the elongation was 34.9% and the necking rate was 59.6%. The results are shown in Table 7. Then, with respect to the electrode material of Reference Example 3, a round bar test piece was produced in exactly the same manner as in the present example, and a tensile test was performed to measure the tensile strength and the necking rate while measuring the tensile strength of Zhang-36-201013738. The intensities were 36 lN/mm2, the elongation was 18.8%, and the necking rate was shown in Table 7. Next, in the same manner as in the first embodiment, two pairs of the thin plate-like cold cathode electrodes 3 of the present embodiment were produced using the electrode material of the present invention. Subsequently, in order to evaluate the performance of the cold cathode fluorescent A 3 obtained in the present embodiment, a cold cathode tube which is identical to the first embodiment has a diameter of 3 mm which is not coated on the inner wall surface. The inside of the glass tube having a length of 300 mm has a plate-shaped electrode 3. Then, the upper tube was discharged for 300 hours under the condition that the tube current was fixed at 6 mA, and then the cold cathode tube M and the electrode 3 for the fluorescent tube were opened. Next, in order to check the presence or absence of atoms sputtered from the cold cathode electrode 3 and the reaction with Hg, the surface composition of the electrode 3 for cold cathode fluorescent tubes and the composition of the above-mentioned glass surface are determined by φ. As a result, anhydrous silver atoms on the inner wall of the glass tube of the electrode 3 for cold cathode fluorescent tubes are shown in Table 8. Next, in the same manner as in the present embodiment except that the electrode material of Reference Example 3 was used, a pair of thin plate-shaped electrodes for cold tubes were fabricated to prepare a cold cathode tube N having the electrodes (refer to the obtained cold cathode tube N). The composition of the inner wall surface of the surface glass tube of the electrode for cold cathode fluorescent tubes was measured by ΕΡΜΑ in the same manner as in the first example. The results are shown in Table 8. The tension was found to be 6.4%. The tube is made of an electrode, and the phosphor is coated with a pair of thin cold cathodes to take out the cold cathode fluorescent tube ΕΡΜΑ the inner surface of the glass tube and the rest with the cathode fluorescent example 3). In the same manner as in the glass-37-201013738, in order to evaluate the performance of the electrode 3 for the cold cathode fluorescent tube obtained in the present embodiment, a cold cathode fluorescent tube lc is formed in the same manner as in the first embodiment, and the cold is formed. The cathode fluorescent tube lc is coated on the inner wall surface with a phosphor having a diameter of 3 mm and a length of 300 mm, and has a pair of thin electrodes. Next, tube currents of 5 mA, 6 mA, 7 mA, and 8 mA were applied to the pair of the electrodes 3 of the cold cathode fluorescent tube 1 of the present embodiment, and the tube voltages generated for the respective tube currents were measured. The results are shown in Figure 6. Then, in addition to the electrode material of Reference Example 1, an electrode for a cold cathode fluorescent tube was fabricated in the same manner as in the present embodiment, and a cold cathode fluorescent tube having the electrode was prepared (Reference Example 3) ). A tube current of 5 mA, 6 mA, 7 mA, and 8 mA was applied to each of the pair of electrodes of the prepared cold cathode fluorescent tube, and the tube voltage generated for each tube current was measured. The results are shown in Figure 6. (Comparative Example 5) In this comparative example, the electrode material of this comparative example was produced. The electrode material is completely the same as that of the eighth embodiment except that a metal which is substantially composed only of Mo and the remainder is an unavoidable impurity is used. Next, in the same manner as in the eighth embodiment, a test piece was prepared using the electrode material obtained in the comparative example, and the sputtering rate of the electrode material was calculated by measuring the reduced weight of the test piece after continuous sputtering. When the sputtering rate of the electrode material of Reference Example 3 was set to 100%, the sputtering rate of the electrode material -38 - 201013738 of the comparative example was equivalent to 83.4%. The results are shown in Table 6. Subsequently, in the same manner as in the eighth embodiment, a round bar test piece was prepared on the electrode material obtained in the comparative example, and a tensile test was performed to measure the tensile strength, and the elongation and the necking rate were calculated, respectively, and the tension was obtained. The strength was 33 5 N/mm 2 , the elongation was 2.4%, and the necking rate was 1.6%. The results are shown in Table 7. Then, in the same manner as in the eighth embodiment, an electrode material obtained by the comparative example was used to form a pair of thin plate-shaped electrodes for cold cathode fluorescent tubes, and a cold cathode tube P was formed. The inside of the glass tube to which the wall surface is not coated with the phosphor has the pair of electrodes. Next, with respect to the above-described cold cathode tube P, the surface composition of the electrode for cold cathode fluorescent tubes and the composition of the inner wall surface of the glass tube were measured by ΕΡΜΑ in the same manner as in the eighth embodiment. The results are shown in Table 8. Subsequently, in the same manner as in the eighth embodiment, using the electrode material obtained in the present comparative example, a pair of thin plate-shaped cold cathode fluorescent tubes were fabricated and used to form a cold cathode fluorescent tube, which was made into a cold cathode fluorescent tube. The light pipe has a pair of electrodes inside the glass tube to which the phosphor is coated on the inner wall surface. A tube current of 5 mA, 6 mA, 7 mA, and 8 mA was applied between the pair of electrodes of the formed cold cathode fluorescent tube, and the tube voltage generated for each tube current was measured. The results are shown in Figure 6. (Comparative Example 6) In this comparative example, the electrode material of this comparative example was produced. The electrode material is completely the same as that of the eighth embodiment except that a metal which is substantially composed only of Fe and the remainder is not -39-201013738 and which can be avoided as an impurity is used. Then, in the same manner as in the eighth embodiment, an electrode material obtained by the present comparative example was used to form a pair of thin plate-shaped electrodes for cold cathode fluorescent tubes, and a cold cathode tube Q was formed, which was formed on the inner wall surface. The inside of the glass tube to which the phosphor is not applied has the pair of electrodes described above. Next, with respect to the above-described cold cathode tube Q, the surface composition of the electrode for cold cathode fluorescent tubes and the composition of the inner wall surface of the glass tube were measured by ΕΡΜΑ in the same manner as in the eighth embodiment. The results are shown in Table 8. Subsequently, in the same manner as in the eighth embodiment, using the electrode material obtained in the present comparative example, a pair of thin plate-shaped electrodes for cold cathode fluorescent tubes were fabricated, and a cold cathode fluorescent tube was fabricated, and the cold cathode fluorescent tube was The inside of the glass tube to which the inner wall surface is coated with the phosphor has the pair of electrodes. A tube current of 5 mA, 6 mA, 7 mA, and 8 mA was applied between the pair of electrodes of the formed cold cathode fluorescent tube, and the tube voltage generated for each tube current was measured. The results are shown in Figure 6.

(表6 ) \ Mo (質量%) Nb (質量%) Fe (質量%) Ni (質量%) 濺射率 (%) 參考例三 - - - 100* 100 實施例八 3.4 1.6 剩餘部分* - 69.1 比較例五 100* - - - 83.4 *:包含不可避免的不純物 從表6明顯可知,實施例八的電極材料與比較例五的 實質上由Mo構成的電極材料相比’濺射率較小’具有優 -40- 201013738 良的抗濺射性。上述實施八的電極材料由含量爲相對全量 爲3.4質量%的Mo、1.6質量%的Nb、剩餘部分實質上 爲Fe的合金構成。 (表7 )(Table 6) \ Mo (% by mass) Nb (% by mass) Fe (% by mass) Ni (% by mass) Sputtering rate (%) Reference Example 3 - - - 100* 100 Example 8 3.4 1.6 Remaining portion * - 69.1 Comparative Example 5: 100* - - - 83.4 *: Containing unavoidable impurities It is apparent from Table 6 that the electrode material of Example 8 has a smaller sputtering rate than the electrode material of Comparative Example 5 which is substantially composed of Mo. Excellent anti-sputtering properties from -40 to 201013738. The electrode material of the above-described eighth embodiment is composed of an alloy having a content of 3.4% by mass relative to the total amount of Mo, 1.6% by mass of Nb, and the balance being substantially Fe. (Table 7)

Mo (質量%) Nb 償量%) Fe (質量%) Ni (質量%) 張力強度 (N/mm2) 延伸率 (%) 頸縮率 (%) 參考例三 - - - 100* 361 18.8 6.4 實施例八 3.4 1.6 剩餘部分* - 502 34.9 59.6 比較例五 100* - - - 335 2.4 1.6 :包含不可避免的不純物 另外,從表7可以明顯看出,實施例八的電極材料與 比較例五相比,張力強度較大,具有優良的強度。此外, 從表7可以明顯得出,實施例八的電極材料與比較例五相 比,延伸率以及頸縮率特別大,具有優良的加工性。 \ Mo 償量%) Nb (質量%) Fe (質量%) Ni (質量%) 電極表面 Hg 玻璃管內壁 Hg 參考例三 - - - 100* 有(87質量%) 有(21質量%) 實施例八 3.4 1.6 剩餘部分* - - - 比較例五 100* - - - - 比較例六 - - 100* - 有(2.5質量%) - 包含不可避免的不純物 從表8可以明顯看出,在冷陰極管M(具有實施例八 -41 - 201013738Mo (% by mass) Nb Reward %) Fe (% by mass) Ni (% by mass) Tensile strength (N/mm2) Elongation (%) Necking rate (%) Reference Example 3 - - - 100* 361 18.8 6.4 Implementation Example 8 3.4 1.6 Remaining portion * - 502 34.9 59.6 Comparative Example 5 100* - - - 335 2.4 1.6: Containing unavoidable impurities In addition, it is apparent from Table 7 that the electrode material of Example 8 is compared with Comparative Example 5. The tensile strength is large and has excellent strength. Further, as apparent from Table 7, the electrode material of Example 8 was particularly large in elongation and necking ratio as compared with Comparative Example 5, and had excellent workability. \ Mo Replenishment %) Nb (% by mass) Fe (% by mass) Ni (% by mass) Electrode surface Hg Glass tube inner wall Hg Reference Example 3 - - - 100* Yes (87% by mass) Yes (21% by mass) Example 8 3.4 1.6 Remaining part * - - - Comparative Example 5 100* - - - - Comparative Example 6 - - 100* - Yes (2.5 mass%) - Contains unavoidable impurities from Table 8 It is apparent that in the cold cathode Tube M (with embodiment eight-41 - 201013738

的薄板狀的冷陰極螢光管用電極3)中’在該電極3的表 面以及玻璃管的內壁面上不存在Hg原子。所以’在上述 冷陰極管Μ中,雖然構成冷陰極螢光管用電極3的Fe原 子些微被濺射,但在該電極3的表面以及玻璃管的內壁面 兩處明顯沒有形成Fe和Hg構成的合金(汞合金)。由 此可以明確得知,上述冷陰極管Μ不會因形成汞合金而 消耗玻璃管內的Hg,從而,能夠延長該冷陰極管Μ的使 用壽命。In the thin plate-shaped cold cathode fluorescent tube electrode 3), there is no Hg atom on the surface of the electrode 3 and the inner wall surface of the glass tube. Therefore, in the cold cathode tube, the Fe atoms constituting the electrode 3 for the cold cathode fluorescent tube are slightly sputtered, but the surface of the electrode 3 and the inner wall surface of the glass tube are not formed of Fe and Hg. Alloy (amalgam). From this, it is clear that the cold cathode tube crucible does not consume Hg in the glass tube due to the formation of the amalgam, and thus the service life of the cold cathode tube crucible can be prolonged.

而另一方面,明顯可知,在冷陰極管Ν (具有參考例 三的薄板狀的冷陰極螢光管用電極)中,該電極表面上存 在有相對全量爲87質量%的Hg原子,玻璃管的內壁面上 存在有相對全量爲2 1質量%的Hg原子。所以,明顯可知 ,在上述冷陰極管N中,構成上述冷陰極螢光管用電極 的Ni原子被濺射,在該電極表面上,形成了 Ni與Hg構 成的汞合金。由此可以明確得知,上述冷陰極管N因形 成汞合金而消耗了玻璃管內的Hg,會縮短該冷陰極管N 的使用壽命。 而且,明顯可知,在冷陰極管Q (具有比較例六的薄 板狀的冷陰極螢光管用電極)中,雖然在玻璃管的內壁面 上不存在Hg原子,但在該電極表面上存在相對全量爲 2.5質量%的Hg原子。所以,明顯可知,在上述冷陰極管 Q中,構成上述冷陰極螢光管用電極的Fe原子被濺射, 在該電極表面上,形成了些微Fe和Hg構成的汞合金。 由此可以明確得知,上述冷陰極管Q因形成汞合金而消 -42- 201013738On the other hand, it is apparent that in the cold cathode tube Ν (the electrode for the thin-plate cold cathode fluorescent tube having the reference example 3), a relatively total amount of Hg atoms of 87% by mass is present on the surface of the electrode, and the glass tube is A relatively total amount of Hg atoms of 21% by mass is present on the inner wall surface. Therefore, it is apparent that in the cold cathode tube N, Ni atoms constituting the electrode for the cold cathode fluorescent tube are sputtered, and an amalgam composed of Ni and Hg is formed on the surface of the electrode. From this, it is clear that the cold cathode tube N consumes Hg in the glass tube due to the formation of the amalgam, which shortens the service life of the cold cathode tube N. Further, it is apparent that in the cold cathode tube Q (the electrode for the thin-plate cold cathode fluorescent tube of Comparative Example 6), although there is no Hg atom on the inner wall surface of the glass tube, there is a relative total amount on the surface of the electrode. It is 2.5% by mass of Hg atoms. Therefore, it is apparent that in the cold cathode tube Q, Fe atoms constituting the electrode for the cold cathode fluorescent tube are sputtered, and amalgam composed of micro Fe and Hg is formed on the surface of the electrode. It can be clearly seen that the above cold cathode tube Q is eliminated by the formation of amalgam -42 - 201013738

耗了玻璃管內的Hg,與冷陰極管Μ相比,該冷陰極管Q 的使用壽命變短。 另外’從圖6明顯可知,實施例八的冷陰極螢光管用 電極3與實質上由Ni構成的參考例三的冷陰極螢光管用 電極相比’ Mo的含量雖然相對全量只有較少的3.4質量% ’但是管電壓較小。並且還明顯可知,使用實施例八的冷 陰極螢光管用電極3時的管電壓,與使用比較例五的實質 上由Mo構成的冷陰極螢光管用電極時的管電壓較爲接近 。所以,明顯可知實施例八的冷陰極螢光管用電極3的管 電壓較低,能源效率較爲良好。 【圖式簡單說明】 圖1是表示本實施形態的冷陰極螢光管及冷陰極螢光 管用電極的說明圖。 圖2是表示具有實施例一〜實施例六的冷陰極螢光管 φ 用電極的冷陰極管的電阻率的圖表。 圖3是表示具有實施例一的冷陰極螢光管用電極的冷 陰極管的電流電壓特性的圖表。 圖4是表示具有實施例一〜實施例六的冷陰極螢光管 用電極的冷陰極管的管電壓比的圖表。 圖5是表示實施例一、實施例七的冷陰極螢光管的使 用壽命的圖表。 圖6是表示具有實施例八的冷陰極螢光管用電極的冷 陰極螢光管的管電壓比的圖表。 -43- 201013738 【主要元件符號說明】 1 :冷陰極螢光管 2 :玻璃管 3:冷陰極螢光管用電極 4 :封接銷 5 :外部導線The Hg in the glass tube is consumed, and the service life of the cold cathode tube Q is shortened compared to the cold cathode tube. In addition, it is apparent from Fig. 6 that the electrode 3 for the cold cathode fluorescent tube of the eighth embodiment has a lower content of Mo than the electrode for the cold cathode fluorescent tube of the third example which is substantially composed of Ni. Mass % 'but the tube voltage is small. Further, it is also apparent that the tube voltage when the electrode 3 for a cold cathode fluorescent tube of the eighth embodiment is used is close to the tube voltage when the electrode for a cold cathode fluorescent tube which is substantially composed of Mo of Comparative Example 5 is used. Therefore, it is apparent that the electrode 3 for the cold cathode fluorescent tube of the eighth embodiment has a low tube voltage and is excellent in energy efficiency. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is an explanatory view showing an electrode for a cold cathode fluorescent tube and a cold cathode fluorescent tube according to the embodiment. Fig. 2 is a graph showing the electrical resistivity of the cold cathode tubes having the electrodes for the cold cathode fluorescent tubes φ of the first to sixth embodiments. Fig. 3 is a graph showing current-voltage characteristics of a cold cathode tube having an electrode for a cold cathode fluorescent tube of the first embodiment. Fig. 4 is a graph showing the tube voltage ratio of the cold cathode tubes having the electrodes for the cold cathode fluorescent tubes of the first to sixth embodiments. Fig. 5 is a graph showing the service life of the cold cathode fluorescent tubes of the first embodiment and the seventh embodiment. Fig. 6 is a graph showing the tube voltage ratio of the cold cathode fluorescent tube having the electrode for cold cathode fluorescent tubes of the eighth embodiment. -43- 201013738 [Description of main component symbols] 1 : Cold cathode fluorescent tube 2 : Glass tube 3 : Electrode for cold cathode fluorescent tube 4 : Sealing pin 5 : External wire

-44--44-

Claims (1)

201013738 七、申請專利範圍: 1-一種冷陰極螢光管用電極,其特徵在於:由含有相 對全量爲0.1 ~3 0質量%範圍內的Mo、Fe以及不可避免的 不純物的合金構成。 2.如申請專利範圔第1項之冷陰極螢光管用電極,其 中,上述合金含有相對全量爲0.1-10質量%範圍內的Mo 〇 A 3.如申請專利範圍第1項之冷陰極螢光管用電極,其 中,上述合金含有相對全量爲1.5〜5.5質量%範圍內的Mo 〇 4·如申請專利範圍第1項之冷陰極螢光管用電極,其 中’上述合金含有相對全量爲5質量%以下的Ru。 5·如申請專利範圍第1項之冷陰極螢光管用電極’其 中,上述合金含有相對全量爲〇·1〜6質量%範圍內的Nb。 6. —種冷陰極螢光管,其特徵在於具有:由含有相對 . 全量爲0.1〜3 0質量%範圍內的Mo、Fe以及不可避免的不 純物的合金構成的冷陰極螢光管用電極。 7. 如申請專利範圍第6項之冷陰極螢光管’其中’上 述合金含有相對全量爲〇.1~1〇質量%範圍內的M〇° 8. 如申請專利範圍第6項之冷陰極蛋光管’其中’上 述合金含有相對全量爲1.5-5.5質量%範圍內的Mo° 9. 如申請專利範圍第6項之冷陰極螢光管’其中’上 述合金含有相對全量爲5質量%以下的Ru ° 1〇·如申請專利範圍第6項之冷陰極螢光管,其中, -45 - 201013738 上述合金含有相對全量爲ο·1-6質量%範圍內的Nb。201013738 VII. Patent application scope: 1. An electrode for a cold cathode fluorescent tube, which is characterized in that it is composed of an alloy containing Mo, Fe, and unavoidable impurities in a relative total amount of 0.1 to 30% by mass. 2. The electrode for a cold cathode fluorescent tube according to the first aspect of the invention, wherein the alloy contains Mo 〇A in a range of from 0.1 to 10% by mass relative to the total amount. 3. The cold cathode fluorescing of the first item of claim 1 The electrode for a light pipe, wherein the alloy contains Mo 〇4 in a range of 1.5 to 5.5% by mass relative to the total amount, and the electrode for a cold cathode fluorescent tube according to the first aspect of the patent application, wherein the above alloy contains a relative total amount of 5% by mass. The following Ru. 5. The electrode for cold cathode fluorescent tube according to the first aspect of the invention, wherein the alloy contains Nb in a range of from 1 to 6 mass% relative to the total amount. A cold cathode fluorescent tube comprising: an electrode for a cold cathode fluorescent tube comprising an alloy containing Mo, Fe, and unavoidable impurities in a range of 0.1 to 30% by mass in total. 7. The cold cathode fluorescent tube of claim 6 of the patent application, wherein the above alloy contains M 〇 in a range of 〇.1~1〇% by mass. 8. Cold cathode as in claim 6 The egg light pipe 'where the above alloy contains a relative amount of Mo in the range of 1.5 to 5.5% by mass. 9. The cold cathode fluorescent tube of the sixth aspect of the patent application' wherein the above alloy contains a relative total amount of 5% by mass or less Ru ° 1 〇 · The cold cathode fluorescent tube of claim 6 of the patent scope, wherein -45 - 201013738 The above alloy contains Nb in a range of relatively full amount of ο·1-6 mass%. -46 --46 -
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