TW201111536A - Copper material for use in a sputtering target, and manufacturing method therefor - Google Patents

Copper material for use in a sputtering target, and manufacturing method therefor Download PDF

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TW201111536A
TW201111536A TW099128733A TW99128733A TW201111536A TW 201111536 A TW201111536 A TW 201111536A TW 099128733 A TW099128733 A TW 099128733A TW 99128733 A TW99128733 A TW 99128733A TW 201111536 A TW201111536 A TW 201111536A
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copper
purity
length
copper material
hot extrusion
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TW099128733A
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Chinese (zh)
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TWI504769B (en
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Isao Takahashi
Kiyoshige Hirose
Kazuo Kurahashi
Akifumi Nakajima
wei-ming Zhou
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Furukawa Electric Co Ltd
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    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • CCHEMISTRY; METALLURGY
    • C22METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
    • C22FCHANGING THE PHYSICAL STRUCTURE OF NON-FERROUS METALS AND NON-FERROUS ALLOYS
    • C22F1/00Changing the physical structure of non-ferrous metals or alloys by heat treatment or by hot or cold working
    • C22F1/08Changing the physical structure of non-ferrous metals or alloys by heat treatment or by hot or cold working of copper or alloys based thereon
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • C23C14/3407Cathode assembly for sputtering apparatus, e.g. Target
    • C23C14/3414Metallurgical or chemical aspects of target preparation, e.g. casting, powder metallurgy

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Physics & Mathematics (AREA)
  • Thermal Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Physical Vapour Deposition (AREA)

Abstract

Provided are a copper material for use in a sputtering target, said copper material comprising high-purity copper having a purity of at least 99.99%, and a manufacturing method therefor. X-ray diffraction peak intensities (I{111}, I{200}, I{220}, and I{311}) for surfaces on which sputtering is performed (surface {111}, surface {200}, surface {220}, and surface {311}) satisfy equation (1), and the diameters of crystal grains in the provided copper material are between 100 [mu]m and 200 [mu]m. (1) I{200}/(I{111}+I{200}+I{220}+I{311}) = 0.4

Description

201111536 六、發明說明: 【發明所屬之技術領域】 本發明係、關於-種作為賤㈣而&用之銅材料及 造方法。 ' 【先前技術】 近年來’自移動PC(Personalcomputer,個人電腦)、 行動電話終端等小型電子機器至大型電視為止,於各種尺 寸中使用平板顯示器。於分類為平板顯示器之液晶顯示器 或有機EL ( EleCtroluminescence,電致發光)顯示器中’ 為滿足對高晝質、動態圖像之高速描繪之要求,而開發於 像素點中插人有薄膜電晶體(Thin Film 以下記 為TFT)元件者,目前正成為主流。 圖1中以剖面來圖示液晶顯示器巾之TFT元件之構造 -例。TFT元件、:於玻璃基板2之上有掃描線3及閉極 電極4(掃描線之-部分,作為進行TFT之〇N/〇FF控制而 具有功此)。以利用氮化矽之絕緣膜5進行覆蓋之形態形成 閘極電極,於絕緣膜5夕μ # r*· ,, 豕联 > 之上依序形成非晶矽(以下記為a-Si) 層ό 4雜P (磷)之a_Si層7、源極-沒極電極8及9。以 覆蓋其等之方式形成氮化%之保護膜丨卜於像素區域配置 有摻錫士化銦(以下記為ITO ( Indium Tin 0xide))膜!【。 先則掃描線、閘極電極、及源極-汲極電極係使用m〇、201111536 VI. Description of the Invention: [Technical Field to Be Invented by the Invention] The present invention relates to a copper material and a method for producing the same as 贱(4). [Prior Art] In recent years, flat panel displays have been used in various sizes from small electronic devices such as mobile PCs (personal computers) and mobile phone terminals to large-scale televisions. In the liquid crystal display or organic EL (EleCtroluminescence) display classified as a flat panel display, in order to meet the requirements for high-speed rendering of high-quality and dynamic images, a thin film transistor has been developed for insertion into a pixel ( Thin Film The following is a TFT component and is currently becoming mainstream. Fig. 1 is a cross-sectional view showing a configuration of a TFT element of a liquid crystal display panel. In the TFT element, the scanning line 3 and the closing electrode 4 (the portion of the scanning line are provided on the glass substrate 2 as a function of performing 〇N/〇FF control of the TFT). The gate electrode is formed by covering with the insulating film 5 of tantalum nitride, and amorphous germanium (hereinafter referred to as a-Si) is sequentially formed on the insulating film 5 (μ*r*·, 豕 & >) Layer ό 4 hetero-P (phosphorus) a_Si layer 7, source-polar electrode 8 and 9. A protective film having a % of nitridation is formed by covering it, and an indium-doped indium (hereinafter referred to as an ITO (Indium Tin 0xide)) film is disposed in the pixel region. [. First, the scan line, the gate electrode, and the source-drain electrode are used,

Cr之類的高熔點金屬或鋁及其合金等 '然而,隨著液晶顯 示器之大型化或高後去丄 像素化,由配線長度增加、信號延遲、 電力損失等所引起之圖像顯示不均等問題顯現出來。因此 201111536 電阻率較低之銅配線開始受到關注。 TFT元件之配線使用銅配線膜之問題可舉出:若於玻璃 基板上直接形成Cu膜,則Cu配線膜由於cu/玻璃界面之密 著性較差而自玻璃剝離。 作為用於解決該剝離之問題之發明,提出有專利文獻i 〜3等中所記載之技術。 於專利文獻1中,係藉由在銅配線與玻璃基板之間插 入翻等高熔點金屬,形成與玻璃基板之密著性優異之障壁 層,而抑制剝離。 於專利文獻2及3中,係藉由使用將銅合金化而成之 粗’而使氧化物形成於銅配線與玻璃基板界面,使合金元 素富集於銅配線與玻璃基板界面等,藉由該等方法抑制剝 離。 如專利文獻2及3之發明,亦開發有銅合金化等方法, 但目前在工業上,係如專利文獻丨所記載之發明,將與玻 璃之密著性較好之Mo或Ti等作為圖丨記載之障壁層丨2而 形成於銅配線之下,藉此改善剝離,並利用濺鍍而形成純 銅之配線。 TFT元件之閘極電極之形成步驟中所要求之重要特性 之一,可舉出配線膜之基板面内均勻性。由於膜之均勻性、 即膜厚之不同或凹凸等之存在,而使TFT内之電容變得不 均勻,因此對顯示造成不良影響。另外,於TFT元件製造 步驟中,若存在膜厚之不同、或粗大之團簇(duster)(微 粒、飛濺等),則有於蝕刻製成配線電極時引起斷線及短 4 201111536 路等配線不良之虞。 之^ t &藉&㈣步驟形成成為半導體配線等之純鋼膜 之情形時’可製成均勻 、 9之配線膜且可抑制粗大團簇及抑制 斷線不良的濺鍍靶之發 坦山士* 載之技術。 冑明,一出有專利文獻4〜"中所記 利文獻4令’揭示有如下之难錄無,其藉由將不 _氮石厌及氫之氣體成分的純度99 9999%以上之銅作 為基體並使其於氧濃度〇1 ppm以下炫解、凝固而進行製 造,可獲得不良斷線率較少、超⑶⑽High-melting-point metals such as Cr, aluminum and alloys thereof, etc. However, as the liquid crystal display is enlarged or squashed, the image display is uneven due to an increase in wiring length, signal delay, power loss, and the like. The problem is revealed. Therefore, 201111536 copper wiring with lower resistivity began to receive attention. When a copper wiring film is formed on the wiring of the TFT element, when the Cu film is directly formed on the glass substrate, the Cu wiring film is peeled off from the glass due to poor adhesion between the cu/glass interface. As a invention for solving the problem of the peeling, the techniques described in Patent Documents i to 3 and the like have been proposed. In Patent Document 1, a barrier layer having excellent adhesion to a glass substrate is formed by inserting a high melting point metal between a copper wiring and a glass substrate to suppress peeling. In Patent Documents 2 and 3, an oxide is formed on the interface between the copper wiring and the glass substrate by using a thick alloy formed by copper, and the alloy element is concentrated on the interface between the copper wiring and the glass substrate. These methods inhibit peeling. In the inventions of the patent documents 2 and 3, methods such as copper alloying have also been developed. However, in the industrial invention, as described in the patent document, Mo or Ti having good adhesion to glass is used as a map. The barrier layer 2 described in 丨 is formed under the copper wiring, thereby improving the peeling and forming a wiring of pure copper by sputtering. One of the important characteristics required in the step of forming the gate electrode of the TFT element is the in-plane uniformity of the wiring film. The uniformity of the film, that is, the difference in film thickness or the presence or absence of the unevenness, causes the capacitance in the TFT to become uneven, which adversely affects the display. In addition, in the TFT element manufacturing step, if there is a difference in film thickness or coarse clusters (particles, splashes, etc.), there is a disconnection and short wiring when the wiring electrode is formed by etching. Bad shackles. In the case of forming a pure steel film such as a semiconductor wiring by the steps of < (4), the sputtering target which can be made into a uniform wiring film of 9 and suppresses coarse clusters and suppresses disconnection failure can be used. Shan Shi* contains the technology. Yu Ming, a patent document 4 ~ " in the document of the 4th document, 'disclosed the following is difficult to record, by the non-nitrogen stone and hydrogen gas composition purity of 99 9999% or more copper As a substrate, it can be produced by solidifying and solidifying at an oxygen concentration of 〇1 ppm or less, and it is possible to obtain a poor disconnection rate and super (3) (10).

Integ咖η,大型積體電路)用之配線。藉由減少銅材料中 之雜質量而減少斷線不良等。 於專利文獻5中’揭不有藉由使用於純度99 995%以上 之銅中’使再結晶組織之平均結晶粒徑為8〇微米以下,且 使維氏硬度為100以下之濺鍍靶’而抑制濺鍍粒子之濺出 之擴大及粗大團簇產生。 於專利文獻6中,揭示有於不記氣體成分之純度 99.999%以上之射,提高㈣面中之{1U}面之χ射線繞 射峰強度1{ 11 1},使平均粒徑為250 μηι以下,且使由位置 所致之粒徑偏差為20%以内,藉此使膜厚均勻性良好。 於專利文獻7中,揭示有藉由使於表面朝向{1]〇丨面之 結晶之體積為80%以上,且使該等結晶自表面至中心均勻 地分佈,而使銅原子之濺出垂直於表面,能夠於縱橫比較 大之槽之深處形成薄膜。 於專利文獻8中,揭示有於99.999%以上之純度之銅 201111536 中,將平均結晶粒徑控制為1 〇〜3 〇从爪,使具有(11丨)、 {200}、{220}及{3 11}之各配向之粒子量少於5〇% ,且具有 隨機之配向,藉此可實現均勻性及最小之粒子產生。 於先前之發明中,已能夠藉由控制成分、結晶粒徑、 應變及結晶配向,而控制濺鍍粒子之濺出,控制均勻之膜 生成及抑制粗大團簇。然而,大型電視用液晶顯示器等基 板尺寸之大型化正在發展,於第7代等中已成為l87〇mm>< 2200 mm等超過2 m之基板尺寸。伴隨於此於製成配線 之濺鍍步驟中,亦必須於大型之基板上形成薄膜,即便使 用上述專利文獻中記載之方法,所生成之配線膜之膜厚於 基板之每個部位變得不均勻、粗大團簇之產生變得更多等 問題顯現出來。另外,由於所使用之濺鍍靶自身亦大型化, 因此於濺鍍靶材之每個部位,金屬組織容易變得不均勻, 對膜厚精度及粗大團簇造成之影響變大。 [先前技術文獻] [專利文獻] [專利文獻1]曰本專利特開平7-66423號公報 [專利文獻2]日本專利第4065959號公報 [專利文獻3]日本專利特開2〇〇8_166742號公報 [專利文獻4]曰本專利第37271 15號公報 [專利文獻5]曰本專利第3975414號公報 [專利文獻6]曰本專利第34〇3918號公報 [專利文獻7]日本專利第3997375號公報 [專利文獻8]曰本專利第3971 171號公報 201111536 容 内 明 發 rk [發明所欲解決之問題] 繁於上述先前之問題點,本發明之課題在於提供一種 ==材料’其在利用濺❹驟對…FT液晶面板 二大里基板製成配線時’比先前更均句地產生粒子,且 於使用中亦難以引起該粒子之產生頻率之變化。 [解決問題之技術手段] 本發明者等人藉由對上述課題進行銳意研究而發現, 由將、’Ό aa之配向及結晶粒控制於特定之範圍内,另外, 藉由適當使用可更加均勾地組織控制製造方法之執擠壓 法’可提供-種適於能夠製作均句之配線膜的料乾之銅 材料。 本發明係基於該見解而成者。 亦即’本發明係提供: 〇) —種濺鍍靶用銅材料,其特徵在於:其由純度為 99.99%以上之高純度銅所構《,進行濺鑛之面中之⑴I) 面、陶面、⑽}面、及{311}面各自之乂射線繞射之峰 強度,即1{111}、1{200}、1{220}、及1{311}滿足下述式⑴, 且結晶粒之粒徑為1〇〇〜2〇〇 4 1{200}/(1{1 11} + i{200} + 1{22〇} + 1{311 })> 〇 (2)如(1)項之濺鍍靶用銅材料,其係對純度為99的% 以上之高純度銅之鑄錠進行熱擠壓,將經擠壓之材料於卞° 201111536 熱擠壓後立即冷卻而製造; (3 )如(1 )項之濺鑛靶用柄从丨#" 用銅材料’其係對純度為9 9.9 9 % 以上之高純度銅之鑄鍵進行熱擠壓,將經擠壓之材料於該 熱擠壓後立即冷卻,其後進行冷軋而製造; (4)如(1 )項之濺鍍靶用銅材料,其係於7㈧〜〖ο” 。(:下對純度為99.99%以上之高純度銅之鑄錠進行熱擠壓,Integ coffee η, large integrated circuit) wiring. The wire breakage is reduced by reducing the amount of impurities in the copper material. Patent Document 5 discloses that a sputtering target having a recrystallized structure having an average crystal grain size of 8 μm or less and having a Vickers hardness of 100 or less is used in a copper having a purity of 99 995% or more. It inhibits the expansion of spattered particles and the formation of coarse clusters. Patent Document 6 discloses that the purity of the gas component is not more than 99.999%, and the peak intensity of the x-ray diffraction of the {1U} plane in the (tetra) plane is increased by 1{11 1}, and the average particle diameter is 250 μm. Hereinafter, the particle diameter variation by the position is made 20% or less, whereby the film thickness uniformity is good. Patent Document 7 discloses that the volume of crystals having a surface facing the {1] surface is 80% or more, and the crystals are uniformly distributed from the surface to the center, so that the copper atoms are splashed vertically. On the surface, a film can be formed deep in the vertical and horizontal grooves. In Patent Document 8, it is disclosed that in the copper 201111536 having a purity of 99.999% or more, the average crystal grain size is controlled to be 1 〇 〜 3 〇 from the claws, so that (11 丨), {200}, {220}, and { The amount of particles in each of the alignments is less than 5%, and has a random alignment, thereby achieving uniformity and minimum particle generation. In the prior invention, it has been possible to control the spattering of sputtered particles by controlling the composition, crystal grain size, strain, and crystal orientation, thereby controlling uniform film formation and suppressing coarse clusters. However, the size of a substrate such as a liquid crystal display for a large-sized television has been increasing, and in the seventh generation or the like, it has become a substrate size of more than 2 m such as l87 〇 mm > 2200 mm. In the sputtering step for forming a wiring, it is necessary to form a thin film on a large substrate. Even if the method described in the above patent document is used, the thickness of the formed wiring film becomes not large at each portion of the substrate. Problems such as the generation of uniform and coarse clusters become more apparent. Further, since the sputtering target itself is also increased in size, the metal structure tends to be uneven at each portion of the sputtering target, and the influence on the film thickness precision and the coarse cluster is increased. [PRIOR ART DOCUMENT] [Patent Document 1] Japanese Laid-Open Patent Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. [Patent Document 4] Japanese Patent No. 3,971, 519, and Japanese Patent No. 3,997, 371, and Japanese Patent No. 3,997, 371. [Patent Document 8] Japanese Patent No. 3971 171, 201111536, 容内明发rk [Problems to be Solved by the Invention] The problem of the present invention is to provide a == material which is in the use of splashing When the wiring of the FT liquid crystal panel is made of the two large substrates, the particles are generated more uniformly than before, and it is difficult to cause a change in the frequency of generation of the particles during use. [Means for Solving the Problem] The inventors of the present invention have found that the alignment of the 'Όaa and the crystal grains are controlled within a specific range, and that they can be more uniformly used by appropriate use. The extrusion method for controlling the manufacturing method of the stalking organization can provide a copper material suitable for the production of a wiring film of a uniform sentence. The present invention is based on this insight. That is, the present invention provides: 〇) a copper material for a sputtering target, characterized in that it is composed of high-purity copper having a purity of 99.99% or more, and (1)I in the surface of the splashing surface, Tao The peak intensities of the 乂-ray diffraction of the face, the (10)} face, and the {311} face, that is, 1{111}, 1{200}, 1{220}, and 1{311} satisfy the following formula (1), and crystallize The particle size of the grain is 1〇〇~2〇〇4 1{200}/(1{1 11} + i{200} + 1{22〇} + 1{311 })> 〇(2)如如1 The copper material for sputtering target, which is obtained by hot extrusion of an ingot of high purity copper having a purity of 99% or more, and the extruded material is cooled by hot extrusion at 11°201111536; (3) If the splashing target of item (1) is hot-extruded from the 丨#" copper material's high-purity copper casting with a purity of 99.99% or more, it will be extruded. The material is cooled immediately after the hot extrusion, and then cold rolled to produce; (4) The copper material for the sputtering target of (1) is tied to 7 (eight) to 〖ο". (: the purity of the next pair is 99.99. More than % of high-purity copper ingots are hot extruded,

將經擠壓之材料於該熱擠壓後立即以5『c/秒以上之冷卻速 度冷卻而製造; T ⑴-種減鍍靶用銅材料之製造方法,其係製造如⑴ 項之㈣把用銅材料之方法,其特徵在於包含如下步驟: 於〜刪t下對純度為99.99%以上之高純度銅進行埶 擠壓’將經擠壓之材料於熱擠壓後立即以賦/秒以上之冷 卻速度冷卻。 [發明之效果] 藉由本發明,可提供—種適於能夠製作均勻之配線膜 的錢錢挺之銅材斜。士 & ηα 何抖本發明之濺鍍靶用銅材料,在利用濺 鑛步驟對用於TFT液曰 液曰s面板專之大型基板製成配線時,比 先前更均勻地產峰备工 α 生拉子’且於使用中亦難以引起該粒子之 產生頻率之變化。 、、適田地隨附之圖式,並根據下述之記載而闡明本 發明之上述及其他特徵及優點。 【實施方式】 本發明之滅鑛乾用銅材料,係於由純度為99.99%以上 之高純度銅(以下,簡稱為「純銅」)所構成之銅材料中, 8 201111536 將材料表面之微組織之結晶配向及結晶粒徑設為特定之範 圍者。 純銅若藉由退火而進行再結晶,則容易生成丨丨丨”面、 {200}面、{220}面、及{311}面。通常該等係隨機配向,但 本發明者等人發現,該等之中{200}面之濺鍍特性尤為優 異,將{111}面、{200}面、{220}面、及{311}面各自之X 射線繞射之峰強度設為I{111}、1{2〇〇}、】{22〇丨、及"3丨1} 時,虽1{200}之比例為40%以上,亦即滿足下述式(^ )之 情形時,會形成濺鍍特性、例如成臈時之膜厚之均勻性與 膜質之均質性優異者。The extruded material is produced by cooling at a cooling rate of 5 『c/sec or more immediately after the hot extrusion; T (1) - a method for producing a copper material for a target for deplating, which is manufactured as in (1) (4) The method of using a copper material is characterized in that the method comprises the following steps: 埶 埶 高 高 删 删 删 删 删 高 9 9 9 高 高 9 高 高 9 高 高 高 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度 纯度The cooling rate is cooled. [Effect of the Invention] According to the present invention, it is possible to provide a copper material which is suitable for being able to produce a uniform wiring film.士和amp; ηα 何抖 The copper material for the sputtering target of the present invention is more uniform than the previous one when the wiring is applied to the large substrate for the TFT liquid 曰 面板 panel. It is also difficult to cause a change in the frequency of generation of the particles during use. The above and other features and advantages of the present invention are set forth in the description of the appended claims. [Embodiment] The copper material for ore-killing of the present invention is a copper material composed of high-purity copper having a purity of 99.99% or more (hereinafter, simply referred to as "pure copper"), 8 201111536. The crystal orientation and crystal grain size are set to a specific range. When pure copper is recrystallized by annealing, it is easy to form a 丨丨丨" face, a {200} face, a {220} face, and a {311} face. Usually these are randomly aligned, but the inventors have found that The sputtering characteristics of the {200} plane are particularly excellent, and the peak intensities of the X-ray diffraction of the {111} plane, the {200} plane, the {220} plane, and the {311} plane are set to I{111. }, 1{2〇〇}, {22〇丨, and "3丨1}, although the ratio of 1{200} is 40% or more, that is, when the following formula (^) is satisfied, The sputtering characteristics, for example, the uniformity of the film thickness at the time of formation and the homogeneity of the film quality are excellent.

0 · 5以上 以上’更佳為0.7〜0.9。 1已向度)小於〇.4之情形時, ’因此宜為〇·4以上,較佳為0 · 5 or more or more 'more preferably 0.7 to 0.9. When the degree of 1 degree is less than 〇.4, it is preferably 〇·4 or more, preferably

a曰配向同樣對濺鍍特性造成影響。本 料之結晶粒之粒徑為1〇〇〜2〇〇只爪,較 更佳為120〜18〇 。 匕Χ射線繞射之峰強度係使X 之表面入射而測定之各繞射面The a曰 alignment also affects the sputtering characteristics. The crystal grain size of the material is 1 〇〇 2 2 〇〇 claws, more preferably 120 〜 18 〇. The peak intensity of the ray diffraction is the diffraction surface of the surface where X is incident.

201111536 於結晶粒徑較小之情形時,結晶粒界相對地變多,但 結晶粒界之原子排列混亂,濺鍍時之元素之易飛濺度與粒 内不同,因此所形成之膜容易變得不均勻。另外,於結晶 粒控較大之情形時,為使靶物質飛起而必需較高之能量, 使數個靶原子同時濺出等粗大團簇之形成增加,所形成之 膜容易變得不均勻。 另外,於本發明中,結晶粒之粒徑表示基於JIS η 〇5〇 i (切割法)所測定之平均粒徑(粒度)。 再者,推測{200}面之濺鍍特性優異之主要原因在於: 於考慮FCC ( Face-Centered Cubic,面心立方)金屬中之各 面之原子密度之情形時,{11U面最多,其次{2〇〇}面較多, 但{111}面最密,因此為使丨個原子飛起所需之能量較大, 平衡最佳者為{200}面。 本發明之濺鍍靶用銅材料之製造方法並無特別限定, 作為提高{200}面之配向之製造程序,較佳為使用熱擠壓。 熱擠壓時預先將材料之加熱溫度設為7〇〇<»c以上為宜。於低 於700 C之情形時,無法於擠壓中充分地產生動態再結晶, 難以獲得(1 )式之關係《再者,加熱溫度之上限並無特別 限定,但由於純銅之熔點約為1〇8〇t ,故若過高則小坯會 部分性地熔解而無法進行擠壓。熱擠壓之溫度更佳為 〜900°C。熱擠壓可使用通常之擠壓機,且可以任意之壓力 進行。 經熱擠壓之材料之溫度非常高,通常於短時間内結晶 粒粗大化、成長,成$ 200 ,以上。為防止該情況並使結 10 201111536 晶之粒徑為1 〇〇〜200 μηι,較佳為於擠壓後立即(通常為自 模具擠出後5秒以内)藉由水冷等將材料以5〇〇c /秒以上之 冷卻速度冷卻。冷卻速度更佳為1 〇〇艺/秒以上。該冷卻速 度之上限值並無特別限制,實際上通常為3〇〇/秒左右以 下。另外,較佳為進行冷卻直至材料成為2〇〇t以下為止。 結晶之配向、即上述式(1 )所示之結晶配向度由於熱 加工時之加工之方向(金屬流根據鍛造、軋製、擠壓而不 同,因此方向分別發生改變)、加工率(量)、溫度等發 生各種變化。藉由熱擠壓進行加工,"將上述結晶配向 度控制為滿足本發明所規定之上述式(丨) 外,於自上述動態再結晶至粒成長之階段,斤結:::大: 確定。除此以外,為固定熱擠壓組織,較佳為於上述擠壓 後立即進行冷卻。#由達成該等兩點,可獲得本發明之銅 材料。 另外,就熱鍛造而t,對應近年來之無之大型化要求 之尺寸以消除鍛造後之冷卻:之不均勾,無法獲得均句 之結晶粒組織。 轡-:外’為獲得上述結晶配向或結晶粒a,純銅之純度 :I作為製造純銅之鑄料的原料之電解銅中含有 以程度之雜胃,純銅之鑄鍵中亦出現該等雜質。若雜質 二!材料之耐熱性提高’難以產生再結晶,變得難以 獲?寸、、,。晶配向。於太恭 , 、本發明中’純銅之純度必須為99.99%以 佳為9 9.9 9 5 %以上。再者,於 再者於上述熱擠壓及緊跟其後 之7部之純銅之純度實質上並無變化。 11 201111536 作為熱擠壓之優異之方面,可舉出:可於擠壓材料之 則端後端及寬度方向上以較小之偏差進行利用上述結晶 配向或冷卻速度之結晶粒徑控制。 先^鋼靶材係藉由熱軋而製造,但由於熱軋係經幾道 次〜十幾道次而使經加熱之錠坯逐漸變薄,故於軋製中產 生溫度下降,該溫度下降容易於材料之前後端產生差異。 另外,寬度方向之兩側之溫度由於散熱而容易下降。進而 最後實施之水冷,一般係自軋製材料之單側逐漸進入水冷 帶,因此於此處亦容易產生前後端之差異。 方面由於熱擠壓係將經擠壓之材料立即冷卻而 形成㈣材料,因此不會於長度方向及寬度方向上產生冷 卻過程之/皿度差。所產生之溫度差為擠壓開始與擠壓結束 之小堪之溫度下降,但由於與熱軋相比加工時間較短’:因 此下降量較少,亦會產生加工發熱之蓄積,故溫度差幾乎 :會:為問題。如此1用熱擠壓所製造之材料於長度方 向、寬度方向上特性偏純小,0此將其 板而進行”造之類的大型顯示器㈣材料時、、,有容= 勻地形成濺鍍膜之效果。 = ,於該熱擠 可藉由與先 另外,更佳為將熱擠壓所獲得之擠壓材料 壓後立即將材料冷卻之步驟之後,進行冷軋。 前相同之條件而進行冷軋。 12 201111536 5 1〜1 00 Hv (維氏硬度)之範固。若應變過多,則靶原子 較多地聚集並濺出而增加粗大團簇之形成,所形成之膜容 易變得不均勻’期望使硬度為1〇〇 Hv以下。再者已知,一 般而言,關於無氧銅(C1020),完全地進行再結晶或退火, 並進行拉伸強度達到最低之熱處理之情形(〇材)時之硬度 為51〜59 Hv (「伸銅品數據手冊(第2版)」日本伸銅協 會編2009年3月31日第2版發行61頁),硬度之較佳 範圍之下限值係基於該值者。 再者’硬度之調節係藉由軋製等冷加工而進行,將冷 加工之加工率抑制為30%以下左右,藉此可使硬度之較佳 範圍之上限值為1 〇〇 Hv以下,從而簡便地獲得硬度為5 i 〜100 Hv之銅材料。 如上所述,冷加工係為調節硬度而實施。加工率為〇%、 即完全退火之狀態(〇材)下之硬度為51〜59Hv,若提高 加工率,則硬度緩慢提高,加工率為3〇%時硬度達到1〇〇201111536 When the crystal grain size is small, the grain boundary is relatively large, but the atomic arrangement of the grain grain boundary is disordered, and the splashing degree of the element during sputtering is different from that in the grain, so the formed film is likely to become Not uniform. Further, in the case where the crystal grain size is large, a high energy is required for the target material to fly, and formation of coarse clusters such as simultaneous splashing of several target atoms is increased, and the formed film is liable to become uneven. . Further, in the present invention, the particle diameter of the crystal grains means an average particle diameter (particle size) measured based on JIS η 〇 5 〇 i (cutting method). Furthermore, it is presumed that the main reason for the excellent sputtering characteristics of the {200} surface is: When considering the atomic density of each surface in the FCC (Face-Centered Cubic) metal, the {11U surface is the most, and secondly { 2〇〇} has more faces, but the {111} face is the densest, so the energy required to make one atom fly is larger, and the best balance is {200} face. The method for producing the copper material for a sputtering target of the present invention is not particularly limited, and it is preferable to use hot extrusion as a manufacturing procedure for improving the orientation of the {200} plane. In the hot extrusion, it is preferred to set the heating temperature of the material to 7 〇〇 <»c or higher. When the temperature is lower than 700 C, dynamic recrystallization cannot be sufficiently produced in the extrusion, and it is difficult to obtain the relationship of the formula (1). Further, the upper limit of the heating temperature is not particularly limited, but since the melting point of pure copper is about 1 〇8〇t, so if it is too high, the small billet will partially melt and cannot be extruded. The hot extrusion temperature is preferably -900 ° C. The hot extrusion can be carried out using a conventional extruder and can be carried out at any pressure. The temperature of the material which is hot extruded is very high, and the crystal grains are usually coarsened and grown in a short time, and become $200 or more. In order to prevent this and make the particle size of the 201111536 crystal 1 〇〇~200 μηι, it is preferable to use 5 〇 by water cooling or the like immediately after extrusion (usually within 5 seconds after extrusion from the mold). Cool down at a cooling rate of 〇c / sec. The cooling rate is preferably 1 〇〇 / sec or more. The upper limit of the cooling rate is not particularly limited, but is usually about 3 Å/sec or less. Moreover, it is preferable to cool until the material becomes 2 〇〇t or less. The orientation of the crystal, that is, the crystal orientation indicated by the above formula (1) is the direction of processing during hot working (the metal flow varies depending on forging, rolling, and extrusion, and the direction is changed separately), and the processing ratio (amount) Various changes occur in temperature and the like. By processing by hot extrusion, "the above crystal aligning degree is controlled to satisfy the above formula (丨) prescribed by the present invention, and from the above dynamic recrystallization to the stage of grain growth, the knot:::large: determined . In addition to this, in order to fix the hot extruded structure, it is preferred to perform cooling immediately after the above extrusion. # The copper material of the present invention can be obtained by achieving these two points. In addition, in the case of hot forging, t corresponds to the size of the large-scale requirement in recent years to eliminate the cooling after forging: the uneven grain is not obtained, and the crystal grain structure of the uniform sentence cannot be obtained.辔-: outside' is to obtain the above crystal alignment or crystal grain a, and the purity of pure copper: I is contained in the electrolytic copper of the raw material for producing pure copper, and the impurities are also present in the cast bond of pure copper. If the impurities are two! The heat resistance of the material is increased. It is difficult to recrystallize and become difficult to obtain. Inch,,,. Crystal alignment. Yu Taigong, in the present invention, the purity of pure copper must be 99.99% or more preferably 99.99% or more. Further, the purity of the pure copper in the above-mentioned hot extrusion and the subsequent 7 portions is substantially unchanged. 11 201111536 As an excellent aspect of hot extrusion, it is possible to control the crystal grain size by the above-described crystal orientation or cooling rate with a small variation in the end and the width direction of the extruded material. The first steel target is manufactured by hot rolling, but since the hot rolling is gradually thinned by several passes to several dozen passes, a temperature drop occurs during rolling, and the temperature is lowered. It is easy to make a difference in the front end of the material. In addition, the temperature on both sides in the width direction is liable to lower due to heat dissipation. Further, the final water cooling is generally carried out from the one side of the rolled material into the water cooling zone, so that the difference between the front and rear ends is also likely to occur here. In the aspect of the hot extrusion, the extruded material is immediately cooled to form a (four) material, so that the difference in the length direction and the width direction of the cooling process does not occur. The temperature difference produced is a small temperature drop at the beginning of the extrusion and the end of the extrusion, but the processing time is shorter than that of the hot rolling': therefore, the amount of decrease is small, and the accumulation of processing heat is also generated, so the temperature difference Almost: Yes: For the problem. In this way, the material produced by hot extrusion has a small purity in the longitudinal direction and the width direction, and when the material is made into a large-sized display (four) material, it has a capacity to form a sputter film uniformly. The effect of the hot extrusion can be carried out by the step of cooling the material immediately after pressing the extruded material obtained by hot extrusion, and then cold rolling. Rolling 12 201111536 5 1~1 00 Hv (Vickers hardness). If the strain is too much, the target atoms will accumulate and spatter and increase the formation of coarse clusters, and the formed film tends to become uneven. 'It is desirable to have a hardness of 1 〇〇 Hv or less. It is also known that, in general, for oxygen-free copper (C1020), recrystallization or annealing is completely performed, and heat treatment at the lowest tensile strength is achieved (coffin) The hardness is 51~59 Hv ("Extension Copper Data Sheet (2nd Edition)", Japan Copper Association, March 31, 2009, 2nd edition, page 61), the lower limit of the hardness range Based on this value. In addition, the adjustment of the hardness is performed by cold working such as rolling, and the processing rate of cold working is suppressed to about 30% or less, whereby the upper limit of the preferable range of hardness can be made 1 〇〇Hv or less, which is simple. A copper material having a hardness of 5 i to 100 Hv is obtained. As described above, cold working is performed to adjust the hardness. The processing rate is 〇%, that is, the hardness under the state of complete annealing (coffin) is 51 to 59 Hv. If the processing rate is increased, the hardness is slowly increased, and the hardness is 1 时 when the processing rate is 3〇%.

Hv。若加工率過高,則硬度會超過100 Hv,而產生上述問 題。 將於熱擠壓後立即進行冷卻,並視需要進行冷軋所製 造之材料、較佳為平板狀之材料,藉由車床加工等任意之 機械加工等加工至靶形狀為止,而用於濺鍍。 [實施例] 以下’基於實施例更詳細地說明本發明,但本發明並 不限定於該等實施例。 (實施例1 ) 13 201111536 製作具有表1所示純度之材料Ν〇·ι〜§的直徑300 mm X長度800 mm之铸錠,作為熱擠壓用小坯。將上述小坯加 熱至約1 000 C後進行擠壓,繼而立即將擠壓材料以冷卻速 度約100C/秒進行20秒鐘水冷而獲得厚度22 mmx寬度2〇〇 mm之素板。繼而對上述素板進行冷軋,製造出厚度2〇爪爪 X寬度200 mmx長度約12 m之平板(擠壓)之濺鍍靶用銅 材料Νο.Ι-Κι再者,n〇.h〜15為本發明例,n〇卜6 〜1-8為銅之純度低於本發明例之比較例。 另外’作為先前例,係於製造程序中使用熱乳而製作 平板线餘用銅材料㈤如⑷。亦即,製作材料 版卜^之純度之厚度…啊寬度㈣崎長度函 mm之鎮錠,作a赦击 。、- 、、…、軋用紋坯。將上述錠坯加熱至約1 000 4進订‘、、、軋而製作出厚度23瓜戰寬度㈣咖之素板。 $軋時之材料冷卻係藉由於最終道次後使材料通過水冷區 域而進行。繼而對所 斤獲仵之素板之表面進行平面切削後, 利用冷軋製成厚度2〇 m 分,藉此製造出厚度2G度Gmm,進而切除邊緣部 平板(軋製)之賤L mmx寬度2GGmmx長度約丨21"之 錢乾用銅材料No. 1-9〜1-1 1。Hv. If the processing rate is too high, the hardness will exceed 100 Hv, which causes the above problem. It is cooled immediately after hot extrusion, and if necessary, the material produced by cold rolling, preferably a flat material, is processed to a target shape by any mechanical processing such as lathe processing, and is used for sputtering. . [Examples] Hereinafter, the present invention will be described in more detail based on examples, but the present invention is not limited to the examples. (Example 1) 13 201111536 An ingot having a diameter of 300 mm X and a length of 800 mm having a material of the purity shown in Table 1 was prepared as a small billet for hot extrusion. The pellet was heated to about 1 000 C and then extruded, and then the extruded material was immediately cooled at a cooling rate of about 100 C/sec for 20 seconds to obtain a plain plate having a thickness of 22 mm x 2 mm. Then, the above-mentioned plain plate is cold-rolled to produce a copper plate material for a sputtering target having a thickness of 2 〇 claw X width 200 mm×length of about 12 m (Ν), 再ο.Ι-Κι再者, n〇.h~ 15 is an example of the present invention, and n 〇 6 〜 1-8 is a comparative example in which the purity of copper is lower than that of the present invention. Further, as a prior art, a copper wire material for a flat wire is produced by using hot milk in a manufacturing process (5) as in (4). That is, the thickness of the purity of the material of the material is made... ah width (four) the length of the strip of the length of the town of mm, for a sniper. , -,, ..., rolling grain. The above ingot is heated to about 1 000 4 to make a ‘,, and rolled to produce a thickness of 23 melons and a width (4). The material cooling during the rolling is carried out by passing the material through the water-cooled zone after the final pass. Then, after planar cutting of the surface of the obtained plate, the thickness is 2 〇m by cold rolling, thereby producing a thickness of 2 G degrees Gmm, and then cutting the width of the edge plate (rolling) 贱 L mm x width 2GGmmx length about 丨21" The money is dried with copper material No. 1-9~1-1 1.

關於如此所得之N 對基於圖2之模式办挪〜1-12之平板之銅材料21,針 方向前端部(長圓之說明圖中所示的擠壓時之長度 (長度别端)之寬度 側部(端1 ( 23 )、山 〇之中央0P ( 22 )及兩 部(長度中央)之寬唐(24))、擠壓時之長度方向中央 (26)、端2 (27)方向之中央部(25)及兩側部(端1 、及擠壓時之長度方向後端部(長度 14 201111536 後端)之寬度方向之中央部(28 )及兩側部(端1 ( 29 )、 端2 ( 30 ))之合計9個部位,藉由下述方法調查結晶方位 分佈、結晶粒徑及硬度。另外,自基於圖3之模式立體圖 之說明圖中所示的擠壓時之長度方向前端部(長度前端) 31、擠壓時之長度方向中央部(.長度中央)32、及擠壓時 之長度方向後端部(長度後端)3 3之3個部位切下直徑6 英吋之圓形板,藉由下述方法調查濺鍍特性。 [1 ]結晶方位分佈 關於銅材料板中之結晶方位,係於上述各部位,使X 射線自做為乾來使用之表面入射,測定來自各繞射面之強 度。比較其中主要之i i}、{2〇〇)、{22〇}及{31 i}面各自之 繞射強度’算出上述式(丨)之強度比(結晶配向度)。再 者,將X射線照射之條件設為:χ射線之種類為CuK α i, 管電壓為40 kv ’管電流為20 mA。 [2 ]結晶粒徑 關於銅材料板中之結晶粒徑,係於上述各部位中,於 做為靶來使用之表面進行微組織觀察,並基於JIS Η 〇5〇1 (切割法)進行測定。 [3] 硬度 銅材料板中之硬度係於做為靶來使用之表面,依據JIS Z 2244並利用微維氏硬度試驗機而進行測定。 [4] 濺鍍特性 於圖3所示之位置31、32、33,自所獲得之銅材料板 切下直徑卢6英对(15 24 cm)、厚度8 _,並進行研磨而 15 201111536 製成濺鍍靶。為消除靶面之粗糙度之影響,粗糙度係將所 有最大粗糙度Ra研磨為0.5〜o s μπι並使其一致。使用如 上所述而製成之濺鍍靶,利用DC ( Direct Current,直流) 磁控濺鍍裝置,對膜厚〇·7 mm之日本電氣硝子公司製造之 OA-1 〇玻璃基板實施濺鑛而製成〇 3 膜厚之銅配線。濺 鍍條件為將Ar氣壓力設為〇 4 pa,將放電功率設為12 W/cm2。其後於真空中進行3〇(rc、3〇min之熱處理。對熱 處理後之銅配線之膜厚進行1〇點測定,將最大膜厚及最小 膜厚之範圍達到±7%者設4「良」’將存在其以上之偏差者 設為「不良」。 將結果示於表2、3。本發明例之滿足任一 特性。比較例之N 〇. i - 6〜i _ 8中,結晶配向度、結晶粒㈣ 材枓之整個區域或-部分中偏離本發明之規 為「不良」。先前例之-―係利二 :’結晶配向度於所有示例之整個區域中成為本發明 規=以外。另外,雖結晶粒徑於本發明之規定範圍 另外=寬度方向上,兩端之結晶粒徑小於中央部, 傾向等:方向上不均勻’即後端出現結晶粒徑較大之 與本發明例相比,硬度亦於材料寬度方 rt變得不均勻。據此先前例之濺鎪特性幾乎^為「不又 16 201111536 [表i] 表1Regarding the N obtained in this way, the copper material 21 of the flat plate of the type 1 to 12 is moved according to the mode of Fig. 2, and the front end portion of the needle direction (the length of the extrusion (the end of the length) shown in the illustration of the long circle is shown. The center (end 1 ( 23 ), the center of the mountain ridge 0P ( 22 ) and the two parts (the center of the length) of the wide Tang (24)), the center of the length direction (26), the end 2 (27) direction Center portion (28) and both side portions (end 1 (29), end portions in the width direction of the end portion (25) and the side portions (end 1 and the rear end portion in the longitudinal direction of the extrusion (length 14 201111536 rear end)) In the total of 9 parts of 2 (30)), the crystal orientation distribution, crystal grain size, and hardness were investigated by the following method, and the longitudinal direction of the extrusion direction as shown in the explanatory view of the mode perspective view based on Fig. 3 Part (length front end) 31, the center portion (.length center) 32 in the longitudinal direction at the time of pressing, and the rear end portion (length rear end) 3 3 at the time of extrusion are cut into a diameter of 6 inches. For the circular plate, the sputtering characteristics were investigated by the following method. [1] Crystal orientation distribution regarding the crystal orientation in the copper material plate, Each part is made to have X-rays incident on the surface used as dry, and the intensity from each diffraction surface is measured. Compare the main ii}, {2〇〇), {22〇} and {31 i} faces. The diffraction intensity 'calculates the intensity ratio (crystal orientation) of the above formula (丨). Further, the conditions of the X-ray irradiation are: the type of the x-ray is CuK α i , and the tube voltage is 40 kv 'the tube current is 20 mA. [2] Crystal grain size Regarding the crystal grain size in the copper material sheet, it is used in the above-mentioned various parts, and the microstructure is observed on the surface used as a target, and based on JIS Η 〇5〇1 (cutting method) [3] The hardness in the hardness copper material sheet is measured on the surface used as a target, and is measured in accordance with JIS Z 2244 using a micro Vickers hardness tester. [4] The sputtering characteristics are shown in Fig. 3. The positions 31, 32, and 33 are cut from the obtained copper material plate by 6 inches (15 24 cm) and thickness 8 _, and are ground and 15 201111536 is used as a sputtering target. The effect of roughness, roughness is to grind all the maximum roughness Ra to 0.5~os μπι and make them consistent. Sputtering of the OA-1 bismuth glass substrate manufactured by Nippon Electric Glass Co., Ltd. with a thickness of 7·7 mm by a DC (Direct Current) magnetron sputtering device using the sputtering target prepared as described above A copper wiring having a thickness of 〇3 was formed. The sputtering conditions were such that the Ar gas pressure was set to 〇4 pa, and the discharge power was set to 12 W/cm2. Thereafter, heat treatment was performed in a vacuum of 3 Torr (rc, 3 〇 min). The film thickness of the copper wiring after the heat treatment is measured at a point of 1 point, and the range of the maximum film thickness and the minimum film thickness is ±7%, and 4 "good" is set. The results are shown in Tables 2 and 3. The inventive example satisfies any of the characteristics. In the case of N 6. i - 6 to i _ 8 of the comparative example, the crystal orientation, the entire region or the portion of the crystal grain (tetra) enthalpy deviated from the "defect" of the present invention. The previous example - "Benefit 2:" crystal orientation is outside the scope of the present invention in all of the examples. Further, although the crystal grain size is in the predetermined range of the present invention in the width direction, the crystal grain size at both ends is smaller than the center portion, and the tendency is such that the direction is not uniform, that is, the crystal grain size at the rear end is large. In comparison, the hardness also becomes uneven at the material width rt. According to the previous example, the splash characteristics are almost "not again 16 201111536 [Table i] Table 1

No. 材料 No. 銅之純度 (mass% ) 製造工藝 本發明例 1-1 1 99.994 熱擠壓 1-2 2 99.996 1-3 3 99.992 1-4 4 99.998 1-5 5 99.997 比較例 1-6 6 99.958 熱擠壓 1-7 7 99.929 1-8 8 99.976 1-9 1 99.994 先前例 1-10 3 99.992 熱軋 1-11 5 99.997 [表2] 表2No. Material No. Copper purity (mass%) Manufacturing process Inventive Example 1-1 1 99.994 Hot extrusion 1-2 2 99.996 1-3 3 99.992 1-4 4 99.998 1-5 5 99.997 Comparative Example 1-6 6 99.958 Hot extrusion 1-7 7 99.929 1-8 8 99.976 1-9 1 99.994 Previous example 1-10 3 99.992 Hot rolling 1-11 5 99.997 [Table 2] Table 2

No. 材料 No. 結晶配向度 結晶粒徑(μηι) 長度前端 長度中央 長度後端 長度前端 艮度中央 - Pc度後端 端1 中央 端2 端1 中央 端2 端1 中央 端2 端1 中央 端2 端1 中央 端2 端1 中央 端2 本 發 明 例 1-1 1 0.7 0.6 0.6 0.5 0.6 0.6 0.6 0.5 0.5 160 160 160 160 160 150 160 150 150 1-2 2 0.6 0.6 0.7 0.6 0.7 0.6 0.6 0,6 0.6 160 170 170 170 170 160 160 170 170 1-3 3 0.7 0.8 0.7 0.8 0,7 0.7 0.7 0.8 0.7 140 140 130 130 130 140 140 140 130 1-4 4 0.6 0.6 0.6 0.7 0.6 0.6 0.6 0.7 0.6 180 170 170 180 180 180 180 180 190 1-5 5 0.8 0.8 0.7 0.7 0.8 0.8 0.8 0.8 0.8 150 150 160 150 150 160 140 150 160 比 較 例 1-6 6 0.3 0.4 0.3 0.5 0.3 0.3 0.4 0.3 0.3 90 100 90 100 90 100 90 100 90 1-7 7 0.2 0.3 0.3 0.3 0.4 0.3 0.3 0.4 0.3 80 70 90 70 80 80 80 80 70 1-8 δ 0.3 0.4 0.4 0.3 0,4 0.5 0.4 0.5 0.3 100 110 110 100 110 100 90 110 90 先 前 例 1-9 1 0.3 0.3 0.2 0,2 0.3 0.2 0.3 0.1 0.2 120 150 110 130 170 130 150 180 140 1-10 3 0.3 0.2 0.3 0.2 0.2 0.1 0.1 0.2 0.3 110 120 110 140 160 130 140 170 140 1-11 5 0.4 0.3 0.1 0.2 0.2 0.1 0.2 0.2 0.1 120 140 120 150 160 150 150 170 160 17 201111536 [表3] 表3 材料 維氏硬度 濺餹特性 ]> Jo. No· 长 度.前知 長度中央 長度後端 長度 長度 中央 長度 後端 端1 中央 端2 端1 中央 端2 端1 中央 端? 前端 本 1-1 1 88 86 84 85 85 87 84 83 86 η 良 良 發 1-2 2 85 81 83 82 85 83 84 83 80 良 良 良 明 l-i 3 84 88 89 85 86 89 82 87 91 η 良 良 例 1-4 4 78 77 82 81 79 79 78 74 80 良 良 良 l-b 5 78 73 70 74 72 76 74 78 78 良 良 良 比 1-6 6 100 89 97 92 81 88 84 75 86 不良 不良 不良 較 1-7 7 122 110 123 104 92 101 86 79 84 不良 不良 不良 例 1-8 8 90 83 88 78 70 82 76 65 78 良 良 不良 先 1-9 1 110 99 107 102 91 98 94 85 96 不良 不良 不良 前 1-10 3 132 120 133 114 102 111 96 89 94 良 不良 不良 例 1-11 5 100 93 98 88 80 92 86 75 88 良 不良 不良 (實施例2) 製作由實施例1中之純銅No. 1所構成之小坯,以表4 所示之熱擠壓條件A〜I進行擠壓。條件A〜F為本發明例, 條件G〜I為比較例。再者,加熱溫度之調整係藉由加熱爐 之爐溫設定而進行。另外,冷卻速度係藉由水冷帶之噴淋 量之變更而進行。對所獲得之熱擠壓材料與實施例丨同樣 進行冷軋,而製造出厚度20 mmx寬度200 mmx長度約m 之平板之濺鍍靶用銅材料。另外,與實施例丨同樣對結晶 方位分佈、結晶粒徑、硬度及濺鍍特性進行調查。 將結果示於表5、6。本發明例中製造之銅材料滿足任 —特性。比較例G中製造之銅材料,其結晶配向度於本發 明之規定範圍内,但結晶粒徑低於100 μηι,濺鍍特性部分 性地不良。比較例Η中製造之銅材料,其結晶配向度於本 18 201111536 發明之規定範圍 β ’但結晶粒徑超過200 μηι,濺鍵特性部 分性地不良。比知 伙例I中,加熱溫度較高而於加熱爐内產生 局部熔解,並生1 “'、去進行擠壓。 [表4]No. Material No. Crystalline Alignment Crystal grain size (μηι) Length Front end Length Center length Rear end length Front end center - Pc degree Rear end 1 Center end 2 End 1 Center end 2 End 1 Center end 2 End 1 Center end 2 end 1 central end 2 end 1 central end 2 Inventive Example 1-1 1 0.7 0.6 0.6 0.5 0.6 0.6 0.6 0.5 0.5 160 160 160 160 160 150 160 150 150 1-2 2 0.6 0.6 0.7 0.6 0.7 0.6 0.6 0,6 0.6 160 170 170 170 170 160 160 170 170 1-3 3 0.7 0.8 0.7 0.8 0,7 0.7 0.7 0.8 0.7 140 140 130 130 130 140 140 140 130 1-4 4 0.6 0.6 0.6 0.7 0.6 0.6 0.6 0.7 0.6 180 180 170 170 180 180 180 180 180 190 1-5 5 0.8 0.8 0.7 0.7 0.8 0.8 0.8 0.8 0.8 150 150 160 150 150 160 140 150 160 Comparative Example 1-6 6 0.3 0.4 0.3 0.5 0.3 0.3 0.4 0.3 0.3 90 100 90 100 90 100 90 100 90 1-7 7 0.2 0.3 0.3 0.3 0.4 0.3 0.3 0.4 0.3 80 70 90 70 80 80 80 80 70 1-8 δ 0.3 0.4 0.4 0.3 0,4 0.5 0.4 0.5 0.3 100 110 110 100 110 100 90 110 90 1-9 1 0.3 0.3 0.2 0,2 0.3 0.2 0.3 0.1 0.2 120 150 110 130 170 130 150 180 140 1-10 3 0.3 0.2 0.3 0.2 0. 2 0.1 0.1 0.2 0.3 110 120 110 140 160 130 140 170 140 1-11 5 0.4 0.3 0.1 0.2 0.2 0.1 0.2 0.2 0.1 120 140 120 150 160 150 150 170 160 17 201111536 [Table 3] Table 3 Material Vickers hardness splash Features]> Jo. No. Length. Former length length Central length Rear length Length Central length Rear end 1 Center end 2 End 1 Center end 2 End 1 Center end? Front end 1-1 1 88 86 84 85 85 87 84 83 86 η Liang Liangfa 1-2 2 85 81 83 82 85 83 84 83 80 Liangliang Liangming li 3 84 88 89 85 86 89 82 87 91 η Good example 1-4 4 78 77 82 81 79 79 78 74 80 Liangliangliang lb 5 78 73 70 74 72 76 74 78 78 Liangliangliang ratio 1-6 6 100 89 97 92 81 88 84 75 86 Bad defects are better than 1- 7 7 122 110 123 104 92 101 86 79 84 Adverse defects 1-8 8 90 83 88 78 70 82 76 65 78 Good and bad first 1-9 1 110 99 107 102 91 98 94 85 96 Adverse bad 1 -10 3 132 120 133 114 102 111 96 89 94 Good and bad defects 1-11 5 100 93 98 88 80 92 86 75 88 Good defects (Example 2) Preparation of pure copper No. 1 in Example 1 The green compacts were extruded under the hot extrusion conditions A to I shown in Table 4. Conditions A to F are examples of the invention, and conditions G to I are comparative examples. Further, the adjustment of the heating temperature is performed by setting the furnace temperature of the heating furnace. Further, the cooling rate is performed by changing the amount of spray of the water-cooling belt. The obtained hot extruded material was cold rolled in the same manner as in Example ,, and a copper material for a sputtering target having a thickness of 20 mm x width of 200 mm x and a length of about m was produced. Further, the crystal orientation distribution, crystal grain size, hardness, and sputtering characteristics were investigated in the same manner as in Example 。. The results are shown in Tables 5 and 6. The copper material produced in the examples of the present invention satisfies any of the characteristics. The copper material produced in Comparative Example G had a crystal orientation within the range specified in the present invention, but the crystal grain size was less than 100 μm, and the sputtering property was partially inferior. The copper material produced in the comparative example had a crystal orientation of the predetermined range β ‘ of the invention of 18 201111536, but the crystal grain size exceeded 200 μm, and the sputtering bond characteristics were partially poor. In the case of the example I, the heating temperature is higher and local melting occurs in the heating furnace, and a "" is taken, and the extrusion is performed. [Table 4]

[表5] 表5 結晶配向度 結晶拉搜(um) —长 度前i 長度中央 長度後端 县疳前诚 再府Φ 4?· 端1 中央 端2 端1 中央 端7 端1 中央 端? 昨1 中央 端2 端1 巾Λ 端? 瑞1 吗7 本發明例 A 0.6 0.5 0.6 0.6 0.6 0.7 0.5 0.6 0.6 17.0 no no 17,0 no P0 no no no B 0.6 υ.ί> 0.5 0.5 0.5 0.5 0.6 0.S 0 S 100 no no 110 110 100 110 100 HO (J 0.7 0.6 0.6 0.7 0.6 0.8 0.6 0.7 0.7 150 160 ISO 150 ISO 160 160 140 ISO D 0.7 υ.6 0.6 0.6 0.5 0.6 0.6 0.5 0,6 140 ISO iso ISO 140 140 1/10 140 140 E 0.5 0.6 0.5 0.5 0.5 0.6 0.6 0.6 0.6 180 190 180 170 m 180 170 190 180 F 0.6 U.7 0.6 0.6 0.5 0.5 0.5 06 06 170 170 170 180 180 17Π ικη 1 7Π ion 比較例 G 0.4 0.5 0.5 0.5 0.4 0.5 0.4 0.4 04 ς〇 Q〇 100 q〇 90 80 80 Η 0.6 0.6 0.5 0.6 0.5 0.7 0.6 0.6 0.5 240 240 710 ??0 740 ?40 ?40 7^0 I 無法擠壓 法擠 $ 19 201111536 [表6] 表6 維氏硬度 濺鍍特性 長度前端 長度中央 長度後端 長度 長度 長度 端1 中央 端2 端1 中央 端2 端1 中央 端2 前端 中央 後端 A 83 86 85 85 84 89 91 89 85 良 η 良 本發明 B 101 103 97 103 98 97 104 100 101 良 η 良 C 79 81 85 85 90 82 83 86 89 良 η 良 例 D 80 78 81 82 85 79 83 86 84 良 良 良 t 81 79 76 88 85 80 89 85 87 良 良 良 l· 80 76 85 84 91 76 83 89 90 良 良 ή 比較例 G 121 124 119 Ϊ27 123 116 125 ΈΓ 124 了 一不良 良 H T 78 75 80 79 81 79 81 80 76 良 不良 不良 對本發明及其實施態樣一併進行了說明,但只要本發 月者未特別指$,則於說明之任__細節中均不對本發明加 以限定,應在不違反隨附之申請專利範圍所示之發明之精 神及範圍的情況下,進行廣泛之解釋。 本案係基於2009年8月28日於日本提出申請之曰 :利特願2__198982而主張優先權,本案以參照之 其内容作為本說明書之記載之—部分而併人本文中。 【圖式簡單說明】 例之概 圖1係表示液晶顯示器中之TFT元件的構造— 略剖面圖。 _ 2係貫施例中之結晶方位分佈 之測定試驗的取樣之說明圖。 圖3係實施例中之濺錢特性試樣之取樣之說明圖 【主要元件符號說明】 20 201111536 1 TFT元件 2 玻璃基板 3 掃描線 4 閘極電極 5 氮化矽之絕緣膜 6 非晶矽層 7 摻磷非晶矽層 8、9 源極-沒極電極 10 氮化矽之保護膜 11 摻錫氧化銦膜 12 障壁層 21 平板之銅材料 22 擠壓時之長度方 度方向之中央部 23、24 擠壓時之長度方 度方向之兩側部 25 擠壓時之長度方 度方向之中央部 26 ' 27 擠壓時之長度方 度方向之兩側部 28 擠壓時之長度方 度方向之中央部 29、30 擠壓時之長度方 度方向之兩側部 向前端部(長度前端)之寬 向前端部(長度前端)之寬 向中央部(長度中央)之寬 向中央部(長度中央)之寬 向後端部(長度後端)之寬 向後端部(長度後端)之寬 21 201111536 31 擠壓時之長度 32 擠壓時之長度 33 擠壓時之長度 方向前端部(長度前端) 方向中央部(長度中央) 方向後端部(長度後端) 22[Table 5] Table 5 Crystalline Alignment Crystallization pull (um) - length before i length center length back end County Yuqian Cheng Zaifu Φ 4? · End 1 Central end 2 End 1 Central End 7 End 1 Central end? Yesterday 1 Central end 2 end 1 towel 端 end?瑞1吗 7 Inventive Example A 0.6 0.5 0.6 0.6 0.6 0.7 0.5 0.6 0.6 17.0 no no 17,0 no P0 no no no B 0.6 υ.ί> 0.5 0.5 0.5 0.5 0.6 0.S 0 S 100 no no 110 110 100 110 100 HO (J 0.7 0.6 0.6 0.7 0.6 0.8 0.6 0.7 0.7 150 160 ISO 150 ISO 160 160 140 ISO D 0.7 υ.6 0.6 0.6 0.5 0.6 0.6 0.5 0,6 140 ISO iso ISO 140 140 1/10 140 140 E 0.5 0.6 0.5 0.5 0.5 0.6 0.6 0.6 0.6 180 190 180 170 m 180 170 190 180 F 0.6 U.7 0.6 0.6 0.5 0.5 0.5 06 06 170 170 170 180 180 17Π ικη 1 7Π ion Comparative Example G 0.4 0.5 0.5 0.5 0.4 0.5 0.4 0.4 04 ς〇Q〇100 q〇90 80 80 Η 0.6 0.6 0.5 0.6 0.5 0.7 0.6 0.6 0.5 240 240 710 ?? 0 740 ?40 ?40 7^0 I Can not squeeze the squeeze $ 19 201111536 [Table 6] Table 6 Vickers hardness sputtering characteristics length front end length central length rear end length length length end 1 central end 2 end 1 central end 2 end 1 central end 2 front end central rear end A 83 86 85 85 84 89 91 89 85 good η good invention B 101 103 97 103 98 97 104 100 101 good η good C 79 81 85 85 90 82 83 86 89 good η good example D 80 7 8 81 82 85 79 83 86 84 良良良 t 81 79 76 88 85 80 89 85 87 良良良 l· 80 76 85 84 91 76 83 89 90 良良ή Comparative example G 121 124 119 Ϊ27 123 116 125 ΈΓ 124 A bad HT 78 75 80 79 81 79 81 80 76 Good and bad, the invention and its implementation are described together, but as long as the current month does not specifically refer to $, in the description of the __ details The invention is not limited thereto, and a broad interpretation should be made without departing from the spirit and scope of the invention as set forth in the appended claims. This case is based on the application filed in Japan on August 28, 2009. Litto 2__198982 claims priority, and the contents of this case are referred to in the present specification as part of this specification. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a cross-sectional view showing the structure of a TFT element in a liquid crystal display. _ 2 is an explanatory diagram of the sampling of the measurement test of the crystal orientation distribution in the embodiment. Fig. 3 is an explanatory diagram of sampling of a splash characteristic sample in the embodiment [Description of main component symbols] 20 201111536 1 TFT element 2 Glass substrate 3 Scanning line 4 Gate electrode 5 Insulating film of tantalum nitride 6 Amorphous layer 7 Phosphorus-doped amorphous germanium layer 8, 9 source-nothing electrode 10 protective film of tantalum nitride 11 tin-doped indium oxide film 12 barrier layer 21 copper material of flat plate 22 central portion of length direction direction when extruded 23 24 when the two sides of the length direction of the extrusion are pressed, the central portion of the length direction of the extrusion is 26 ' 27 when the two sides of the length direction of the extrusion are pressed. The width of the front end portion (length end) of the front end portion (length end) of the center portion 29, 30 is wide toward the center portion (length center) toward the center portion (length) Width of the center to the rear end (length rear end) to the rear end (length rear end) 21 201111536 31 Length of extrusion 32 Length of extrusion 33 Length direction of the front end of the extrusion (length front end In the direction Central part (length center) Direction rear end (length rear end) 22

Claims (1)

201111536 七、申請專利範圍: 1· 一種濺鍍靶用銅材料,其特徵在 直 田吨度% 99.99%以上之高純度銅所構成,進行濺鍍之面中之丨1 1 ·、· 面、面、{22〇}面、及{311}面各自之乂射線繞射= 強度,即【⑴小叩⑼卜叫卟及屮⑴滿足下述式㈠), 且結晶粒之粒徑為100〜200 μηι ; ’ 1{200}/(1{111} + 1{20〇} + 1{22〇} + 1{311})^〇4 〇)〇 2·如申請專利範圍項之軸乾用銅材料,其係對純 度為99.99%以上之高純度銅之铸錠進行熱擠壓,將經擠壓 之材料於該熱擠壓後立即冷卻而製造。 3.如申請專利範圍第i項之濺鍍靶用銅材料,其係對純 度為99.99%以上之高純度銅之鑄錠進行熱擠壓將經擠壓 之材料於該熱擠壓後立即冷卻,其後進行冷軋而製造。 4·如申請專利範圍第丨項之職鑛乾用銅材料,其係於 :〇〇〜U)5(TC下對純度為99 99%以上之高純度銅之鑄錠進 行熱擠壓,將經擠壓之材料於該熱擠壓後立即以秒以 上之冷卻速度冷卻而製造。 μ 5.-種濺鍍乾用銅材料之製造方法,其係製造中請專利 々圍第1項之濺鍍靶用銅材料之方法’其特徵在於包含如 下步驟:於700〜]05代下對純度為99 99%以上之高純度 銅進行熱擠壓’將經擠壓之材料於熱擠壓後立即以50。。/秒 以上之冷卻速度冷卻。 23201111536 VII. Patent application scope: 1. A copper material for sputtering target, characterized by high-purity copper with a linear tonnage of 99.99% or more, in the surface of the sputtering surface 1 1 ··· face, surface , {22〇} face, and {311} face each ray diffraction = intensity, that is, [(1) small 叩 (9) 卟 卟 and 屮 (1) satisfy the following formula (1)), and the crystal grain size is 100~200 Ηηι ; ' 1{200}/(1{111} + 1{20〇} + 1{22〇} + 1{311})^〇4 〇)〇2·The copper material for shaft dry as claimed in the patent scope It is produced by hot-extruding an ingot of high-purity copper having a purity of 99.99% or more, and cooling the extruded material immediately after the hot extrusion. 3. The copper material for sputtering target according to the scope of patent application item i, which is subjected to hot extrusion of an ingot of high purity copper having a purity of 99.99% or more, and the extruded material is cooled immediately after the hot extrusion. Then, it is produced by cold rolling. 4. If the copper material for dry ore in the application for the scope of patent application is: 〇〇~U)5 (hot extrusion of high-purity copper ingot with a purity of 99 99% or more under TC, The extruded material is produced by cooling at a cooling rate of at least two seconds after the hot extrusion. μ 5.- A method for manufacturing a dry-plated copper material, which is required to be sprayed in the first item of the patent. A method for plating a copper material for a target is characterized in that it comprises the steps of: hot-squeezing high-purity copper having a purity of 99 99% or more under 700~]05 generations, immediately after hot extrusion of the extruded material Cool at a cooling rate of 50% or more. 23
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