TWI833642B - Copper foil for flexible printed circuit boards, copper-clad laminates using the same, flexible printed circuit boards and electronic equipment - Google Patents

Copper foil for flexible printed circuit boards, copper-clad laminates using the same, flexible printed circuit boards and electronic equipment Download PDF

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TWI833642B
TWI833642B TW112116273A TW112116273A TWI833642B TW I833642 B TWI833642 B TW I833642B TW 112116273 A TW112116273 A TW 112116273A TW 112116273 A TW112116273 A TW 112116273A TW I833642 B TWI833642 B TW I833642B
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copper foil
flexible printed
printed circuit
copper
circuit
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TW202403060A (en
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坂東慎介
石野裕士
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日商Jx金屬股份有限公司
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    • CCHEMISTRY; METALLURGY
    • C22METALLURGY; FERROUS OR NON-FERROUS ALLOYS; TREATMENT OF ALLOYS OR NON-FERROUS METALS
    • C22CALLOYS
    • C22C9/00Alloys based on copper
    • 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
    • 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
    • C23FNON-MECHANICAL REMOVAL OF METALLIC MATERIAL FROM SURFACE; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL; MULTI-STEP PROCESSES FOR SURFACE TREATMENT OF METALLIC MATERIAL INVOLVING AT LEAST ONE PROCESS PROVIDED FOR IN CLASS C23 AND AT LEAST ONE PROCESS COVERED BY SUBCLASS C21D OR C22F OR CLASS C25
    • C23F1/00Etching metallic material by chemical means
    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05KPRINTED CIRCUITS; CASINGS OR CONSTRUCTIONAL DETAILS OF ELECTRIC APPARATUS; MANUFACTURE OF ASSEMBLAGES OF ELECTRICAL COMPONENTS
    • H05K1/00Printed circuits
    • H05K1/02Details
    • H05K1/03Use of materials for the substrate

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Organic Chemistry (AREA)
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  • Mechanical Engineering (AREA)
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  • Microelectronics & Electronic Packaging (AREA)
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  • General Chemical & Material Sciences (AREA)
  • Manufacturing Of Printed Circuit Boards (AREA)
  • Parts Printed On Printed Circuit Boards (AREA)
  • ing And Chemical Polishing (AREA)

Abstract

本發明提供一種電路直線性良好,適合於微細電路之撓性印刷基板用銅箔、使用其之覆銅積層體、撓性印刷基板及電子機器。 本發明係一種撓性印刷基板用銅箔,其係含有99.96質量%以上之Cu,其餘部分由不可避免之雜質構成之軋製銅箔,進行300℃×30分鐘之熱處理,對上述軋製銅箔之軋製面之測定視野150 μm×150 μm進行EBSD測定,將方位差5°以上視為晶界時之結晶粒徑之標準偏差為3.0 μm以下。 The present invention provides a copper foil for a flexible printed circuit board that has excellent circuit linearity and is suitable for fine circuits, a copper-clad laminate using the copper foil, a flexible printed circuit board, and an electronic device. The present invention is a copper foil for flexible printed circuit boards. It is a rolled copper foil containing more than 99.96% by mass of Cu and the remaining part is composed of unavoidable impurities. It is heat treated at 300°C x 30 minutes to treat the rolled copper foil. The EBSD measurement was performed with a measuring field of view of 150 μm × 150 μm on the rolling surface of the foil. When the orientation difference of 5° or more is regarded as the grain boundary, the standard deviation of the crystal grain size is 3.0 μm or less.

Description

撓性印刷基板用銅箔、使用其之覆銅積層體、撓性印刷基板及電子機器Copper foil for flexible printed circuit boards, copper-clad laminates using the same, flexible printed circuit boards and electronic equipment

本發明係關於一種適用於撓性印刷基板等配線構件之銅箔、使用其之覆銅積層體、撓性配線板及電子機器。The present invention relates to a copper foil suitable for wiring components such as flexible printed circuit boards, copper-clad laminates using the copper foil, flexible wiring boards, and electronic equipment.

作為電子機器之電路基板,廣泛使用撓性印刷基板(撓性配線板,以下,稱為「FPC」)。FPC係藉由對將銅箔與樹脂積層而成之覆銅積層體(Copper Clad Laminate,以下稱為CCL)進行蝕刻而形成配線,且將其上利用被稱為覆蓋層之樹脂層被覆而成者。貼合於CCL之樹脂可例舉聚醯亞胺系、液晶聚合物、PTFE,但是並不限定於此。As circuit boards of electronic devices, flexible printed circuit boards (flexible wiring boards, hereafter referred to as "FPC") are widely used. FPC is formed by etching a copper clad laminate (hereinafter referred to as CCL) formed by laminating copper foil and resin to form wiring, and covering it with a resin layer called a cover layer. By. Examples of the resin bonded to CCL include polyimide, liquid crystal polymer, and PTFE, but are not limited thereto.

又,如此,覆銅積層體會經過為了形成作為目標之電路而藉由塗佈阻劑及曝光步驟印刷電路,進而去除銅層之不需要部分之蝕刻處理,但是存在以下問題:於進行蝕刻而形成電路時,該電路不會成為如預先形成於表面之遮罩圖案之寬度。 其原因在於,藉由蝕刻而形成之銅電路會自銅層之表面向下,即朝向樹脂層,逐漸擴展地受到蝕刻(產生塌陷)。 因此,正在開發減少該「塌陷」之技術(專利文獻1)。 [先前技術文獻] [專利文獻] In addition, in this way, the copper-clad laminated body undergoes an etching process in which the circuit is printed by applying a resist and exposure steps in order to form a target circuit, and then removes unnecessary parts of the copper layer. However, there is the following problem: it is formed by etching. circuit, the circuit will not be as wide as the mask pattern preformed on the surface. The reason is that the copper circuit formed by etching will be gradually etched (collapsed) from the surface of the copper layer downward, that is, toward the resin layer. Therefore, technology to reduce this "collapse" is being developed (Patent Document 1). [Prior technical literature] [Patent Document]

[專利文獻1]日本特開2011-216528號公報[Patent Document 1] Japanese Patent Application Publication No. 2011-216528

[發明所欲解決之課題][Problem to be solved by the invention]

且說,隨著電子機器之小型、薄型、高性能化,而要求FPC之高密度構裝。為了高密度地構裝FPC,需要電路微細化,但於微細電路中為了保持阻抗之整合性,電路寬度於電路整體為固定變得重要。其原因在於,當電路之寬度於電路整體並不固定之情形時,電路會緊挨著(接觸)相鄰之電路,而有變得不良之虞。 而且,如上所述,由於存在電路寬度於樹脂層側(底部側)擴散之傾向,故而底部側更容易與相鄰之電路接觸,於電路整體保持底部側之電路寬度(底部寬度)固定變得更為重要。尤其於如底部寬度為35 μm以下之微細電路之情形時,更容易產生此種不良。 然而,如上述專利文獻1中所記載,雖然揭示有減少電路之頂部寬度與底部寬度之差(塌陷)的技術,但是未發現著眼於底部寬度之技術。 In addition, as electronic devices become smaller, thinner, and more powerful, high-density packaging of FPC is required. In order to build an FPC with high density, circuit miniaturization is required. However, in order to maintain the integrity of impedance in a micro circuit, it is important that the circuit width is fixed throughout the circuit. The reason is that when the width of the circuit is not fixed for the entire circuit, the circuit will be in close proximity (contact) with the adjacent circuit, and there is a risk of becoming defective. Furthermore, as mentioned above, since there is a tendency for the circuit width to spread on the resin layer side (bottom side), the bottom side is more likely to come into contact with adjacent circuits, and keeping the circuit width (bottom width) on the bottom side fixed throughout the circuit becomes more important. Especially in the case of fine circuits with a bottom width of 35 μm or less, such defects are more likely to occur. However, as described in the above-mentioned Patent Document 1, although a technology for reducing the difference (collapse) between the top width and the bottom width of a circuit is disclosed, no technology focusing on the bottom width has been discovered.

本發明係為了解決上述問題而完成者,目的在於提供一種電路直線性良好,適合於微細電路之撓性印刷基板用銅箔、使用其之覆銅積層體、撓性印刷基板及電子機器。 [解決課題之技術手段] The present invention was completed in order to solve the above problems, and aims to provide a copper foil for a flexible printed circuit board that has excellent circuit linearity and is suitable for micro circuits, a copper-clad laminate using the copper foil, a flexible printed circuit board, and an electronic device. [Technical means to solve the problem]

本發明人等進行了各種研究,結果發現為了提高蝕刻銅箔而形成之電路之直線性,重要的是銅箔之金屬組織接近均一,換言之,晶粒之大小一致(結晶粒徑之標準偏差小)。認為其原因在於,若結晶粒徑之標準偏差小,則均一地產生由蝕刻所致之電路形成時之化學反應(蝕刻反應)。The present inventors have conducted various studies and found that in order to improve the linearity of the circuit formed by etching copper foil, it is important that the metal structure of the copper foil is close to uniform, in other words, the size of the crystal grains is consistent (the standard deviation of the crystal grain size is small) ). The reason is considered to be that if the standard deviation of the crystal grain size is small, the chemical reaction (etching reaction) during circuit formation by etching occurs uniformly.

即,本發明之撓性印刷基板用銅箔係含有99.96質量%以上之Cu,其餘部分由不可避免之雜質構成之軋製銅箔,經進行300℃×30分鐘之熱處理時,對上述軋製銅箔之軋製面之測定視野150 μm×150 μm進行EBSD測定,將方位差5°以上視為晶界時之結晶粒徑之標準偏差為3.0 μm以下。That is, the copper foil for flexible printed circuit boards of the present invention is a rolled copper foil that contains 99.96 mass % or more of Cu and the remainder is composed of unavoidable impurities. When heat treatment is performed at 300° C. The measurement field of view of the rolling surface of the copper foil is 150 μm × 150 μm for EBSD measurement. When the orientation difference of 5° or more is regarded as the grain boundary, the standard deviation of the crystal grain size is 3.0 μm or less.

本發明之撓性印刷基板用銅箔,較佳由JIS-H3100(C1100)中規定之精銅或JIS-H3100(C1020)之無氧銅構成。 本發明之撓性印刷基板用銅箔較佳含有10~50質量ppm之P。 The copper foil for flexible printed circuit boards of the present invention is preferably composed of refined copper specified in JIS-H3100 (C1100) or oxygen-free copper specified in JIS-H3100 (C1020). The copper foil for flexible printed circuit boards of the present invention preferably contains 10 to 50 ppm by mass of P.

本發明之覆銅積層體係將上述撓性印刷基板用銅箔與樹脂層積層而成。 本發明之撓性印刷基板係於上述覆銅積層體中之上述銅箔形成電路而成。 本發明之電子機器係使用上述撓性印刷基板而成。 [發明之效果] The copper-clad laminate system of the present invention is formed by laminating the above copper foil and resin layer for the flexible printed circuit board. The flexible printed circuit board of the present invention is formed by forming a circuit on the copper foil in the copper-clad laminate. The electronic device of the present invention is formed using the above-mentioned flexible printed circuit board. [Effects of the invention]

若根據本發明,可獲得一種電路直線性良好,適合於微細電路之撓性印刷基板用銅箔。According to the present invention, it is possible to obtain a copper foil for a flexible printed circuit board that has good circuit linearity and is suitable for micro circuits.

以下,對本發明之銅箔之實施形態進行說明。再者,於本發明中,%只要未特別說明,則表示質量%。Hereinafter, embodiments of the copper foil of the present invention will be described. In addition, in the present invention, % means mass % unless otherwise specified.

<組成> 本發明之銅箔含有99.96質量%以上之Cu,其餘部分由不可避免之雜質構成。若含有10~50質量ppm之P作為添加元素,則較佳。此處,若Cu為99.96質量%以上之範圍,則為了改善銅箔之機械特性,亦可使銅箔含有微量之Ag、Sn、Zr等。 若含有P作為添加元素,則存在金屬組織(結晶粒徑)容易變得均一,進而蝕刻後之電路之底部寬度變得固定之傾向。但是,若P之含量超過50質量ppm(0.005質量%),則導電率降低,不適合於撓性印刷基板。 <Composition> The copper foil of the present invention contains more than 99.96% by mass of Cu, and the remainder is composed of unavoidable impurities. It is preferable if it contains 10 to 50 ppm by mass of P as an added element. Here, if Cu is in the range of 99.96 mass % or more, in order to improve the mechanical properties of the copper foil, the copper foil may also contain a trace amount of Ag, Sn, Zr, etc. If P is contained as an additive element, the metal structure (crystal grain size) tends to become uniform, and the bottom width of the circuit after etching tends to become fixed. However, if the P content exceeds 50 mass ppm (0.005 mass %), the electrical conductivity decreases, making it unsuitable for flexible printed circuit boards.

亦可使本發明之銅箔為JIS-H3100(C1100)中規定之精銅或JIS-H3100(C1020)之無氧銅之組成,或者為含有微量之Ag、Sn、Zr等之無氧銅或精銅,進而亦可於該等組成含有10~50質量ppm之P作為添加元素。The copper foil of the present invention may also be composed of refined copper specified in JIS-H3100 (C1100) or oxygen-free copper of JIS-H3100 (C1020), or oxygen-free copper containing trace amounts of Ag, Sn, Zr, etc. Refined copper may further contain 10 to 50 ppm by mass of P as an additive element in the composition.

P濃度之分析,係使用JIS H 1058(銅及銅合金中之磷定量方法)中規定之磷鉬酸(molybdophosphoric acid)萃取磷鉬酸藍吸光測定法(P濃度:適用於0.0005%~0.01%)來實施。The P concentration is analyzed using the molybdophosphoric acid extraction phosphomolybdate blue absorbance measurement method specified in JIS H 1058 (Quantitative method for phosphorus in copper and copper alloys) (P concentration: applicable to 0.0005% to 0.01% ) to implement.

<結晶粒徑之標準偏差> 於經對軋製銅箔進行300℃×30分鐘之熱處理時,對熱處理後之軋製面之測定視野150 μm×150 μm進行EBSD測定,將方位差5°以上視為晶界時之結晶粒徑之標準偏差為3.0 μm以下。 結晶粒徑之標準偏差係藉由EBSD(Electron Back Scatter Diffraction:電子背向散射繞射)測定中之結晶方位解析而算出。 實際之測定係於將試樣表面電解研磨後,利用SEM-EBSD(日本電子股份有限公司JSM-IT500HR、TSL EDAX SCAN GENERATOR-II、TSL OIM DATA COLECTION7)於下述條件下觀察。 再者,EBSD測定只要對自熱處理後之銅箔切出之樣品板(150 mm×150 mm)進行即可。 <Standard deviation of crystal particle size> When the rolled copper foil is heat-treated at 300°C for 30 minutes, EBSD measurement is performed on the rolling surface after heat treatment with a measurement field of view of 150 μm The standard deviation of the diameter is less than 3.0 μm. The standard deviation of the crystal grain size is calculated by crystal orientation analysis in EBSD (Electron Back Scatter Diffraction) measurement. The actual measurement is based on electrolytic polishing of the sample surface and observation using SEM-EBSD (JSM-IT500HR, TSL EDAX SCAN GENERATOR-II, TSL OIM DATA COLECTION7, Japan Electronics Co., Ltd.) under the following conditions. Furthermore, the EBSD measurement only needs to be carried out on a sample plate (150 mm × 150 mm) cut out of the copper foil after autothermal treatment.

・WD:15.0 mm或16.0 mm ・相機仰角:2.7度 ・樣品傾斜角:70.0度 ・相機方位角:0.0度 ・加速電壓:15.0 kV ・探針電流:9.5 nA ・SS-CCD相機:分格8×8 ・增益:300~350(圖案亮度:0.90~0.95) ・曝光時間:4 ms ・背景積分計數:20次 ・觀察倍率:600倍 ・觀察視野:150 μm×150 μm ・步幅:0.5 μm ・掃描模式:六角形柵格 ・相位列表:銅 ・WD: 15.0 mm or 16.0 mm ・Camera elevation angle: 2.7 degrees ・Sample tilt angle: 70.0 degrees ・Camera azimuth angle: 0.0 degrees ・Acceleration voltage: 15.0 kV ・Probe current: 9.5 nA ・SS-CCD camera: 8×8 grid ・Gain: 300~350 (Pattern brightness: 0.90~0.95) ・Exposure time: 4 ms ・Background points count: 20 times ・Observation magnification: 600 times ・Observation field of view: 150 μm×150 μm ・Step size: 0.5 μm ・Scan mode: Hexagonal grid ・Phase list: Copper

又,所獲得之測定資料之解析係使用OIM Analysis Ver8.0 x64 Advanced package於下述條件下實施。 ・將利用晶粒擴張法之Crean Up實施1次(晶粒公差角:5,最小粒度:2點,多列:1,迭代分數:0.25) ・EBSD圖之邊緣之晶粒並非計算對象 ・藉由Number法(將成為計算對象之總面積單純地除以晶粒數之方法),算出結晶粒徑(Diameter)之平均值、標準偏差 再者,Number法係將方位差5°以上視為晶界進行晶粒之判定,利用將成為計算對象之總面積單純地除以晶粒數之方法來算出結晶粒徑,與切斷法不同。 In addition, the analysis of the obtained measurement data was performed under the following conditions using OIM Analysis Ver8.0 x64 Advanced package. ・Implement Crean Up using the grain expansion method once (grain tolerance angle: 5, minimum grain size: 2 points, multi-column: 1, iteration score: 0.25) ・The grains at the edge of the EBSD diagram are not calculated ・Calculate the average and standard deviation of the crystal grain size (Diameter) by the Number method (a method in which the total area to be calculated is simply divided by the number of crystal grains) Furthermore, the Number method regards the azimuth difference of 5° or more as the grain boundary to determine the crystal grains, and calculates the crystal grain size by simply dividing the total area to be calculated by the number of crystal grains, which is different from the cutting method. .

認為若結晶粒徑之標準偏差為3.0 μm以下,則銅箔之金屬組織接近均一(晶粒之大小一致),且均一地產生由蝕刻所致之電路形成時之化學反應(蝕刻反應)。It is believed that if the standard deviation of the crystal grain size is 3.0 μm or less, the metal structure of the copper foil is nearly uniform (the size of the crystal grains is consistent), and the chemical reaction (etching reaction) during circuit formation caused by etching occurs uniformly.

<電路直線性> 於對銅箔進行表面處理後,切出樣品板(150 mm×150 mm),施加熱處理而製成覆銅積層板後,於以下之蝕刻條件下,自覆銅積層板之銅箔側形成直線電路(參照圖2),於將電路之底部寬度w測定多次時,由底部寬度w(μm)之標準偏差σ(μm)與底部寬度w之平均值Aw(μm)表示之σ/Aw若未達0.03,則較佳。其原因在於,若σ/Aw未達0.03,則經驗上可得知存在電路直線性優異之傾向。 蝕刻條件: 蝕刻液之組成:CuCl 2-2H 2O=3 mol/L(比重1.24),HCl=4 mol/L,液溫=50℃,蝕刻液之噴壓=0.22 MPa,對經遮蔽電路部分之軋製銅箔進行蝕刻處理而形成電路。 σ/Aw係將蝕刻形成之電路之實際之底部寬度w測定多次(較佳為10處以上,更佳為50處,進而較佳為電路之長邊方向每30 μm為100處)而求出σ及Aw,算出σ/Aw。 <Circuit linearity> After surface treatment of the copper foil, cut out a sample plate (150 mm × 150 mm), apply heat treatment to make a copper-clad laminated board, and then use the following etching conditions to cut out the copper-clad laminated board. A linear circuit is formed on the copper foil side (see Figure 2). When the bottom width w of the circuit is measured multiple times, it is expressed by the standard deviation σ (μm) of the bottom width w (μm) and the average value Aw (μm) of the bottom width w. If σ/Aw does not reach 0.03, it is better. The reason is that if σ/Aw is less than 0.03, it is empirically known that the linearity of the circuit tends to be excellent. Etching conditions: Etching liquid composition: CuCl 2 -2H 2 O = 3 mol/L (specific gravity 1.24), HCl = 4 mol/L, liquid temperature = 50°C, etching liquid spray pressure = 0.22 MPa, for shielded circuits Parts of the rolled copper foil are etched to form circuits. σ/Aw is obtained by measuring the actual bottom width w of the circuit formed by etching multiple times (preferably 10 or more places, more preferably 50 places, further preferably 100 places every 30 μm in the long side direction of the circuit) Find σ and Aw, and calculate σ/Aw.

具體而言,如圖1所示,將銅箔蝕刻形成而成之電路21、22自表面朝向下方(樹脂層4側(底部側))擴展,將該底部側之電路寬度(底部寬度)w測定多次。此處,符號wt為表面(頂部)側之電路寬度(頂部寬度)。 再者,如圖2所示,可自各電路21、22分別於特定之測定點,如電路寬度w1、w2、w100、w101、w102、w200・・・般測定50處。亦可於1個電路上測定。 Specifically, as shown in FIG. 1 , circuits 21 and 22 formed by etching copper foil expand from the surface toward the bottom (resin layer 4 side (bottom side)), and the circuit width (bottom width) w on the bottom side is Measured multiple times. Here, the symbol wt is the circuit width (top width) on the surface (top) side. Furthermore, as shown in Figure 2, each circuit 21, 22 can be measured at specific measurement points, such as circuit widths w1, w2, w100, w101, w102, w200, etc., at 50 locations. It can also be measured on a single circuit.

若σ/Aw未達0.03,則底部寬度w之不均較小,表示電路直線性優異。尤佳於底部寬度w為10~35 μm之範圍中電路直線性亦優異。If σ/Aw is less than 0.03, the unevenness of the bottom width w is small, indicating excellent linearity of the circuit. In particular, the linearity of the circuit is excellent even in the range of bottom width w of 10 to 35 μm.

銅箔之電路部分之遮罩,例如可利用使用光阻劑(乾膜阻劑等)藉由光罩僅對作為電路保留之部分保留阻劑之公知方法來形成。作為乾膜阻劑,例如可使用日立化成製造之製品名RY-5107(厚度7 μm)。The mask of the circuit portion of the copper foil can be formed by a known method of using a photoresist (dry film resist, etc.) and leaving the resist only on the portion reserved for the circuit through a photomask. As a dry film resist, for example, product name RY-5107 (thickness: 7 μm) manufactured by Hitachi Chemical Co., Ltd. can be used.

此處,圖3係表示評估電路直線性時之用以蝕刻形成直線電路之曝光遮罩。曝光遮罩之阻劑/空間之圖案有10種,且為圖3中越靠左側(編號10側)空間越寬,越靠右側越窄之設計。而且,於對所有圖案依次進行曝光、顯影、蝕刻、乾膜剝離之後,使用SEM將接近目標之L/S(L/S=10/40~30/20)之電路自所有圖案之中選擇1個,用於評估。Here, FIG. 3 shows the exposure mask used for etching to form a linear circuit when evaluating the linearity of the circuit. There are 10 types of resist/space patterns in the exposure mask. In Figure 3, the space is wider toward the left (numbered side 10) and narrower toward the right. Furthermore, after sequentially exposing, developing, etching, and dry film peeling all the patterns, use SEM to select 1 circuit that is close to the target L/S (L/S=10/40~30/20) from all the patterns. for evaluation.

銅箔之厚度以JISC6515中規定之標稱厚度計,較佳為17 μm以下。厚度越薄,則施加至銅箔之應力越小,故而越有助於提高彎折性,並且亦越有助於可攜式機器之小型化、薄型化、輕量化。The thickness of the copper foil is based on the nominal thickness specified in JISC6515, and is preferably 17 μm or less. The thinner the thickness, the smaller the stress applied to the copper foil, which helps to improve the bendability, and also contributes to the miniaturization, thinning, and weight reduction of portable devices.

<製造> 本發明之銅箔,例如可以如下方式製造。首先,可藉由根據需要向銅鑄錠添加P進行熔解、鑄造之後,重複進行熱軋、冷軋及退火而製造箔。 此處,可於冷軋之中途,實施規定之冷卻速度之中間退火,將中間退火時產生之氧化銹皮去除且進行中間冷軋之後,進行最終退火、最終冷軋而獲得目標之最終厚度之箔。 中間退火之最高溫度可設為350~500℃。中間退火之冷卻速度,較佳自中間退火中之最高溫度TM(℃)以50~150℃/h冷卻至(TM-200)℃之溫度。 <Manufacturing> The copper foil of the present invention can be produced in the following manner, for example. First, foil can be produced by adding P to a copper ingot as necessary, melting it, casting it, and then repeating hot rolling, cold rolling, and annealing. Here, intermediate annealing at a predetermined cooling rate can be performed during cold rolling, and the oxide scale generated during the intermediate annealing can be removed and intermediate cold rolling can be performed, followed by final annealing and final cold rolling to obtain the target final thickness. foil. The maximum temperature of intermediate annealing can be set to 350~500℃. The cooling rate of intermediate annealing is preferably from the highest temperature TM (°C) in intermediate annealing to a temperature of 50 to 150°C/h to a temperature of (TM-200)°C.

如上述,若將中間退火之冷卻速度設定為50~150℃/h,則冷卻速度較一般的條件變慢。而且,中間退火之冷卻速度越慢,則材料內之溫度梯度越小(最先冷卻之部位與最後冷卻之部位之溫度差變小),藉此,金屬組織容易變得均一(晶粒之大小一致),經對最終厚度之箔進行熱處理時之結晶粒徑之標準偏差變小。其結果,認為均一地產生由蝕刻所致之電路形成時之化學反應(蝕刻反應),故而電路直線性提高。As mentioned above, if the cooling rate of intermediate annealing is set to 50 to 150°C/h, the cooling rate will be slower than under normal conditions. Moreover, the slower the cooling rate of intermediate annealing, the smaller the temperature gradient within the material (the temperature difference between the first and last cooled parts becomes smaller), thereby making it easier for the metal structure to become uniform (the size of the grains consistent), the standard deviation of the crystal grain size becomes smaller after heat treatment of the final thickness foil. As a result, it is considered that the chemical reaction (etching reaction) during circuit formation by etching occurs uniformly, thereby improving circuit linearity.

圖4、圖5係表示金屬組織越均一(晶粒之大小一致),則電路直線性越提高之機制。 如圖4所示,蝕刻係蝕刻液自無阻劑之部分(相當於直線電路之間之空間)滲入銅箔內部而擴展,而蝕刻係自空間朝向銅箔之左右擴展。此時,如圖1所示,蝕刻(電路)自表面朝向下方(樹脂層側(底部側))擴展。 Figures 4 and 5 show the mechanism that the more uniform the metal structure is (the size of the grains is consistent), the more the circuit linearity is improved. As shown in Figure 4, the etching liquid penetrates into the copper foil from the resistor-free part (equivalent to the space between linear circuits) and spreads, and the etching spreads from the space toward the left and right sides of the copper foil. At this time, as shown in Figure 1, etching (circuit) spreads from the surface toward the bottom (resin layer side (bottom side)).

此處,如圖5(a)所示,於金屬組織不均一(晶粒之大小不一致)之情形時,圖1所示之電路21、22之底部寬度w之不均變大(於圖5(a)中,電路21、22之邊緣並非直線狀,而是以起伏之方式彎曲)。 認為其原因係如圖5(b)所示,例如於視野150 μm×150 μm內,若電路21側之銅箔之晶粒大,電路22側之銅箔之晶粒小,則金屬組織並不均一(晶粒之大小不一致),晶粒大之電路21側之蝕刻速度變大,於與晶粒小之部位之間,蝕刻量改變,甚至底部寬度w之不均變大。 Here, as shown in Figure 5 (a), when the metal structure is not uniform (the size of the grains is inconsistent), the unevenness of the bottom width w of the circuits 21 and 22 shown in Figure 1 becomes larger (in Figure 5 In (a), the edges of circuits 21 and 22 are not straight, but curved in an undulating manner). The reason is believed to be as shown in Figure 5(b). For example, within a field of view of 150 μm × 150 μm, if the crystal grains of the copper foil on the circuit 21 side are large and the crystal grains of the copper foil on the circuit 22 side are small, the metal structure will not be the same. Non-uniformity (the size of the grains is inconsistent), the etching speed on the circuit 21 side with large grains becomes larger, the etching amount changes between the parts with smaller grains, and even the unevenness of the bottom width w becomes larger.

再者,於圖5(b)中,由於晶粒與晶界中蝕刻速度不同,故而若晶粒之大小不一致,則蝕刻速度會局部地大幅度變動。再者,於本試驗之蝕刻液中,晶界之蝕刻速度較晶粒慢,但亦存在相反之情形。Furthermore, in Figure 5(b), since the etching speeds in the grains and grain boundaries are different, if the sizes of the grains are not consistent, the etching speed will locally vary significantly. Furthermore, in the etching solution used in this experiment, the etching speed of grain boundaries is slower than that of crystal grains, but the opposite situation also exists.

<覆銅積層體及撓性印刷基板> 又,對本發明之銅箔,例如(1)澆鑄樹脂前驅物(例如被稱為清漆之聚醯亞胺前驅物)且施加熱而使之聚合及(2)使用與基膜為相同種類之熱塑性接著劑將基膜層壓於本發明之銅箔,藉此可獲得由銅箔與樹脂基材之2層構成之覆銅積層體(CCL)。又,藉由將塗佈有接著劑之基膜層壓於本發明之銅箔,可獲得由銅箔、樹脂基材及其間之接著層此3層構成的覆銅積層體(CCL)。於製造該等CCL時銅箔受熱處理而再結晶化。 對該等使用光蝕刻技術形成電路,視需要對電路實施鍍覆,將覆蓋層膜層壓,藉此可獲得撓性印刷基板(撓性配線板)。 <Copper-clad laminates and flexible printed circuit boards> In addition, for the copper foil of the present invention, for example, (1) cast a resin precursor (for example, a polyimide precursor called varnish) and apply heat to polymerize it; and (2) use the same type of thermoplastic as the base film. By laminating the base film on the copper foil of the present invention using an adhesive, a copper-clad laminate (CCL) composed of two layers of copper foil and a resin base material can be obtained. Furthermore, by laminating a base film coated with an adhesive on the copper foil of the present invention, a copper-clad laminate (CCL) composed of three layers: copper foil, a resin base material, and an adhesive layer between them can be obtained. During the manufacture of these CCLs, the copper foil is heat treated and recrystallized. A flexible printed circuit board (flexible wiring board) can be obtained by forming a circuit using photolithography technology, plating the circuit if necessary, and laminating a cover film.

因此,本發明之覆銅積層體係將銅箔與樹脂層積層而成。又,本發明之撓性印刷基板係將電路形成於覆銅積層體之銅箔而成。 作為樹脂層,可舉PET(聚對苯二甲酸乙二酯)、PI(聚醯亞胺)、LCP(液晶聚合物)、PEN(聚2,6萘二甲酸乙二酯),但是並不限定於此。又,亦可使用該等樹脂膜作為樹脂層。 作為樹脂層與銅箔之積層方法,亦可將成為樹脂層之材料塗佈於銅箔表面進行加熱成膜。又,亦可使用樹脂膜作為樹脂層,於樹脂膜與銅箔之間使用以下之接著劑,亦可不使用接著劑而將樹脂膜熱壓接於銅箔。但是,自不對樹脂膜施加多餘之熱的方面上,較佳使用接著劑。 Therefore, the copper-clad laminate system of the present invention is formed by laminating a copper foil and a resin layer. Furthermore, the flexible printed circuit board of the present invention is formed by forming a circuit on the copper foil of the copper-clad laminate. Examples of the resin layer include PET (polyethylene terephthalate), PI (polyimide), LCP (liquid crystal polymer), and PEN (polyethylene 2,6-naphthalate). Limited to this. Moreover, these resin films can also be used as a resin layer. As a method of laminating the resin layer and the copper foil, the material that becomes the resin layer can also be coated on the surface of the copper foil and heated to form a film. In addition, a resin film may be used as the resin layer, and the following adhesive may be used between the resin film and the copper foil. Alternatively, the resin film may be thermocompression-bonded to the copper foil without using an adhesive. However, in terms of not applying unnecessary heat to the resin film, it is preferable to use an adhesive.

於使用膜作為樹脂層之情形時,可將該膜隔著接著劑層而積層於銅箔。於該情形時,較佳使用與膜為相同成分之接著劑。例如,於使用聚醯亞胺膜作為樹脂層之情形時,接著劑層亦較佳使用聚醯亞胺系接著劑。再者,此處所稱之聚醯亞胺接著劑,係指含有醯亞胺鍵之接著劑,亦包含聚醚醯亞胺等。When using a film as a resin layer, the film can be laminated on a copper foil via an adhesive layer. In this case, it is better to use an adhesive with the same components as the film. For example, when a polyimide film is used as the resin layer, it is also preferable to use a polyimide-based adhesive for the adhesive layer. Furthermore, the polyimide adhesive here refers to an adhesive containing an imine bond, and also includes polyether imine and the like.

再者,本發明並不限定為上述實施形態。又,只要發揮本發明之作用效果,則上述實施形態中之銅合金亦可含有其他成分。 例如,亦可對銅箔表面實施粗化處理、防銹處理、耐熱處理或該等處理組合而成之表面處理。 [實施例] In addition, the present invention is not limited to the above-mentioned embodiment. In addition, as long as the effects of the present invention are exerted, the copper alloy in the above embodiment may contain other components. For example, the surface of the copper foil can also be subjected to surface treatment including roughening treatment, anti-rust treatment, heat-resistant treatment or a combination of these treatments. [Example]

其次,舉實施例對本發明更詳細地進行說明,但是本發明並不限定於該等實施例。 使用電解銅於非氧化性環境下製作鑄錠。鑄錠所含之銅之比例為99.96質量%以上。將該鑄錠於900℃以上均質化退火後,進行熱軋與冷軋。於冷軋中實施最高溫度400℃之中間退火,使中間退火之冷卻速度為表1之值,進行冷卻至較最高溫度低200℃之溫度。實施例之冷卻速度係根據將與該實施例不同之材料退火時之材料溫度實測資料來推算。將中間退火時產生之氧化銹皮去除且進行中間冷軋後,進行最終退火、最終冷軋而獲得目標之最終厚度12 μm之箔。再者,關於比較例,則藉由傳熱模擬而求出至較最高溫度低200℃之溫度為止之中間退火之冷卻速度,記載於表1中。 Next, although an Example is given and this invention is demonstrated in more detail, this invention is not limited to these Examples. Ingots are made using electrolytic copper in a non-oxidizing environment. The proportion of copper contained in the ingot is 99.96% by mass or more. After the ingot is homogenized and annealed at 900°C or above, hot rolling and cold rolling are performed. During cold rolling, intermediate annealing at a maximum temperature of 400°C is performed, the cooling rate of the intermediate annealing is set to the value in Table 1, and cooling is performed to a temperature 200°C lower than the maximum temperature. The cooling rate of the Example is calculated based on the actual measured material temperature data when annealing a material different from that of the Example. After removing the oxide scale generated during intermediate annealing and performing intermediate cold rolling, final annealing and final cold rolling are performed to obtain a foil with a target final thickness of 12 μm. Furthermore, regarding the comparative example, the cooling rate of the intermediate annealing to a temperature 200° C. lower than the maximum temperature was obtained by heat transfer simulation, and is listed in Table 1.

對所獲得之箔,於大氣環境中,施加300℃×30分鐘之熱處理,獲得銅箔樣品。具體而言,為了防止氧化而將銅箔樣品夾於寬度30 mm×長度130 mm×厚度0.15 mm之2片C7025板之間,利用A4尺寸之已退火之C1100進行包裝後,打開已為300℃之高溫熱風乾燥機之門而投入,於30分鐘後打開門進行回收,取出銅箔樣品。熱處理後之銅箔模仿於CCL之積層時受熱處理之狀態。於將熱處理後之銅箔之軋製面電解研磨後,對測定視野150 μm×150 μm進行EBSD測定,求出將方位差5°以上視為晶界時之結晶粒徑之標準偏差。EBSD測定之條件如上述記載。The obtained foil was subjected to heat treatment at 300° C. for 30 minutes in an atmospheric environment to obtain a copper foil sample. Specifically, in order to prevent oxidation, the copper foil sample was sandwiched between two C7025 plates with a width of 30 mm × a length of 130 mm × a thickness of 0.15 mm. After packaging with A4-sized annealed C1100, it was opened to 300°C. Open the door of the high-temperature hot air dryer and put it in. After 30 minutes, open the door for recycling and take out the copper foil sample. The heat-treated copper foil simulates the state of heat treatment during lamination of CCL. After the rolled surface of the heat-treated copper foil was electrolytically polished, EBSD measurement was performed on a measurement field of view of 150 μm × 150 μm, and the standard deviation of the crystal grain size when an orientation difference of 5° or more was regarded as a grain boundary was determined. The conditions for EBSD measurement are as described above.

又,於對進行最終冷軋所得之箔進行表面處理後,積層25 μm之UpilexVT(宇部興產股份有限公司製造),利用加熱壓製機進行300℃×30 min之熱處理而形成為覆銅積層板後,使用乾膜阻劑(日立化成製造之製品名RY-5107,厚度7 μm),將銅箔之電路部分藉由光蝕刻進行遮蔽,進行L+S為50 μm間距之乾膜圖案化。阻劑之顯影、蝕刻及阻劑之剝離,則使用SunTechno System股份有限公司之「顯影・蝕刻・剝離生產線」(裝置名:DERM)。蝕刻條件如上述「<電路直線性>」中所記載。In addition, after surface treatment of the foil obtained by final cold rolling, 25 μm UpilexVT (manufactured by Ube Kosan Co., Ltd.) was laminated, and heat treatment was performed at 300°C × 30 minutes using a heating press to form a copper-clad laminated board. Then, using a dry film resist (product name RY-5107 manufactured by Hitachi Chemical, thickness 7 μm), the circuit part of the copper foil was masked by photoetching, and dry film patterning was performed with an L+S pitch of 50 μm. For resist development, etching and resist stripping, SunTechno System Co., Ltd.'s "Development, Etching, and Stripping Production Line" (device name: DERM) is used. The etching conditions are as described in the above "<Circuit Linearity>".

<電路直線性之評估> 藉由上述蝕刻條件,實際測定以接近目標之L/S(L/S=10/40~30/20)之方式針對各實施例及各比較例分別改變蝕刻時間而進行條件設定者,結果底部寬度w之平均值Aw成為如表1所示之值。平均值Aw表示L/S之L。又,「50 μm-平均值Aw」表示L/S之S。針對各實施例及各比較例,分別將各電路之底部寬度w如圖2所示測定50處,求出平均值Aw。 再者,各實施例係分別對相同之銅箔,於36~54秒之範圍內分別改變蝕刻時間。同樣地,各比較例係分別對相同之銅箔,於36~54秒之範圍分別改變蝕刻時間。 <Evaluation of circuit linearity> Based on the above etching conditions, it was actually measured to set the conditions by changing the etching time for each example and each comparative example in such a way that it is close to the target L/S (L/S = 10/40 ~ 30/20). The results are at the bottom. The average value Aw of the width w becomes the value shown in Table 1. The average value Aw represents L of L/S. In addition, "50 μm - average value Aw" represents S of L/S. For each Example and each Comparative Example, the bottom width w of each circuit was measured at 50 locations as shown in Figure 2, and the average value Aw was calculated. Furthermore, in each embodiment, the etching time was changed in the range of 36 to 54 seconds for the same copper foil. Similarly, in each comparative example, the etching time was changed in the range of 36 to 54 seconds for the same copper foil.

將所獲得之結果示於表1中。此處,實施例1~7之P濃度為10~50質量ppm之範圍,比較例1~7之P濃度未達10 ppm。P濃度之分析藉由上述方法而進行。The results obtained are shown in Table 1. Here, the P concentration in Examples 1 to 7 is in the range of 10 to 50 ppm by mass, and the P concentration in Comparative Examples 1 to 7 is less than 10 ppm. Analysis of P concentration was performed by the above method.

[表1]    實施例1 實施例2 實施例3 實施例4 實施例5 實施例6 實施例7 比較例1 比較例2 比較例3 比較例4 比較例5 比較例6 比較例7 中間退火之 冷卻速度 (℃/h) 91 91 91 91 91 91 91 49400 (13.72 ℃/s) 49400 49400 49400 49400 49400 49400 平均 結晶粒徑 (µm) 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 結晶粒徑之 標準偏差 (µm) 1.7 1.7 1.7 1.7 1.7 1.7 1.7 3.6 3.6 3.6 3.6 3.6 3.6 3.6 底部寬度w之平均值Aw (µm) 12.0 13.6 18.6 22.6 23.2 26.0 27.5 11.6 16.1 16.5 19.2 20.1 25.7 27.1 底部寬度w之標準偏差σ (µm) 0.321 0.299 0.410 0.546 0.526 0.489 0.676 0.518 0.607 0.569 0.588 0.648 0.871 1.060 σ/Aw 0.027 0.022 0.022 0.024 0.023 0.019 0.025 0.045 0.038 0.034 0.031 0.032 0.034 0.039 [Table 1] Example 1 Example 2 Example 3 Example 4 Example 5 Example 6 Example 7 Comparative example 1 Comparative example 2 Comparative example 3 Comparative example 4 Comparative example 5 Comparative example 6 Comparative example 7 Cooling rate of intermediate annealing (℃/h) 91 91 91 91 91 91 91 49400 (13.72℃/s) 49400 49400 49400 49400 49400 49400 Average crystal particle size (µm) 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 2.9 Standard deviation of crystal particle size (µm) 1.7 1.7 1.7 1.7 1.7 1.7 1.7 3.6 3.6 3.6 3.6 3.6 3.6 3.6 Average value Aw of bottom width w (µm) 12.0 13.6 18.6 22.6 23.2 26.0 27.5 11.6 16.1 16.5 19.2 20.1 25.7 27.1 Standard deviation σ of bottom width w (µm) 0.321 0.299 0.410 0.546 0.526 0.489 0.676 0.518 0.607 0.569 0.588 0.648 0.871 1.060 σ/Aw 0.027 0.022 0.022 0.024 0.023 0.019 0.025 0.045 0.038 0.034 0.031 0.032 0.034 0.039

使用結晶粒徑之標準偏差為3.0 μm以下之實施例之銅箔製成撓性印刷基板後,結果可知σ/Aw未達0.03,幾乎未發現與相鄰之電路之接觸,電路直線性優異。 另一方面,使用結晶粒徑之標準偏差超過3.0 μm之比較例之銅箔製成撓性印刷基板後,結果可知σ/Aw為0.03以上,與相鄰之電路之接觸到處可見,電路直線性差。 When a flexible printed circuit board was made from the copper foil of the example with a standard deviation of crystal grain size of 3.0 μm or less, the results showed that σ/Aw did not reach 0.03, and there was almost no contact with adjacent circuits, and the circuit linearity was excellent. On the other hand, when the copper foil of the comparative example with a standard deviation of the crystal grain size exceeding 3.0 μm was used to make a flexible printed circuit board, it was found that σ/Aw was 0.03 or more. Contact with adjacent circuits was everywhere, and the linearity of the circuit was poor. .

4:樹脂層 21,22:電路 w:電路之底部寬度 w1,w2,w100,w101,w102,w200:電路寬度 wt:電路寬度(頂部寬度) 4: Resin layer 21,22:Circuit w: Width of the bottom of the circuit w1,w2,w100,w101,w102,w200: circuit width wt: circuit width (top width)

[圖1]係表示經蝕刻而形成之電路之底部寬度w之圖。 [圖2]係表示將電路之底部寬度w測定多次之方法之俯視圖。 [圖3]係表示評估電路直線性時之用以蝕刻形成直線電路之曝光遮罩之圖。 [圖4]係表示於直線電路中蝕刻進展之狀態之示意圖。 [圖5]係表示當金屬組織不均一(晶粒之大小不一致)之情形時,電路直線性降低之機制之示意圖。 [Fig. 1] is a diagram showing the bottom width w of a circuit formed by etching. [Fig. 2] is a top view showing a method of measuring the bottom width w of a circuit multiple times. [Figure 3] is a diagram showing the exposure mask used to form a linear circuit by etching when evaluating the linearity of the circuit. [Fig. 4] is a schematic diagram showing the progress of etching in a linear circuit. [Figure 5] is a schematic diagram showing the mechanism by which circuit linearity is reduced when the metal structure is not uniform (the size of the grains is inconsistent).

4:樹脂層 21,22:電路 w:電路之底部寬度 wt:電路寬度(頂部寬度) 4: Resin layer 21,22:Circuit w: Width of the bottom of the circuit wt: circuit width (top width)

Claims (6)

一種撓性印刷基板用銅箔,其係含有99.96質量%以上之Cu,其餘部分由不可避免之雜質構成之軋製銅箔, 經進行300℃×30分鐘之熱處理時,對該軋製銅箔之軋製面之測定視野150 μm×150 μm進行EBSD測定,將方位差5°以上視為晶界時之結晶粒徑之標準偏差為3.0 μm以下。 A copper foil for flexible printed circuit boards, which is a rolled copper foil containing more than 99.96% by mass of Cu, and the remainder is composed of unavoidable impurities. After heat treatment at 300°C for 30 minutes, EBSD measurement was performed on the rolling surface of the rolled copper foil with a measuring field of view of 150 μm x 150 μm. An orientation difference of 5° or more was regarded as the standard for the crystal grain size at the grain boundary. The deviation is 3.0 μm or less. 如請求項1之撓性印刷基板用銅箔,其由JIS-H3100(C1100)中規定之精銅或JIS-H3100(C1020)之無氧銅構成。For example, the copper foil for flexible printed circuit boards in claim 1 is composed of refined copper specified in JIS-H3100 (C1100) or oxygen-free copper specified in JIS-H3100 (C1020). 如請求項1或2之撓性印刷基板用銅箔,其含有10~50質量ppm之P。For example, the copper foil for flexible printed circuit boards of claim 1 or 2 contains 10 to 50 ppm by mass of P. 一種覆銅積層體,其係將如請求項1或2之撓性印刷基板用軋製銅箔與樹脂層積層而成。A copper-clad laminated body formed by laminating the flexible printed circuit board according to claim 1 or 2 with a rolled copper foil and a resin layer. 一種撓性印刷基板,其係於如請求項4之覆銅積層體中之該軋製銅箔形成電路而成。A flexible printed circuit board in which a circuit is formed on the rolled copper foil in the copper-clad laminate according to claim 4. 一種電子機器,其使用有如請求項5之撓性印刷基板。An electronic device using the flexible printed circuit board of claim 5.
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CN110072333A (en) * 2018-01-22 2019-07-30 捷客斯金属株式会社 Flexible printed board copper foil, copper clad layers stack, flexible printed board and electronic equipment using it
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