TWI251108B - Driver mounting method using hysteresis loss, and substrate and anisotropic conductive film - Google Patents

Driver mounting method using hysteresis loss, and substrate and anisotropic conductive film Download PDF

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Publication number
TWI251108B
TWI251108B TW92123060A TW92123060A TWI251108B TW I251108 B TWI251108 B TW I251108B TW 92123060 A TW92123060 A TW 92123060A TW 92123060 A TW92123060 A TW 92123060A TW I251108 B TWI251108 B TW I251108B
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Taiwan
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substrate
driver
conductive film
anisotropic conductive
conductor
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TW92123060A
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Chinese (zh)
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TW200419272A (en
Inventor
Eisaku Kojima
Takeshi Yamada
Masumi Setogawa
Shigetaka Kobayashi
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Chi Mei Optoelectronics Corp
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  • Electric Connection Of Electric Components To Printed Circuits (AREA)
  • Combinations Of Printed Boards (AREA)
  • Liquid Crystal (AREA)

Abstract

The present invention provides a mounting method using an anisotropic conductive film without short circuit between electrodes and also preventing heat convection to each member of a substrate that uses the anisotropic conductive film during connecting components to the substrate. The mounting method using an anisotropic conductive film of the present invention is for mounting a driver on a substrate using an anisotropic conductive film and includes: a step for pinching an anisotropic conductive film between the substrate and the driver; a step for applying a magnetic field to conductive particles in the anisotropic conductive film to generate eddy current and hysteresis loss of the conductive particles; a step for liquefying resin included in the anisotropic conductive film by the heat generated from the eddy current and hysteresis loss of the conductive particles; and a step for curing the liquefied resin and connecting the electrodes of the substrate and the driver to each other by the conductive particles.

Description

1251108 五、發明說明(1) —--- 一、 【發明所屬之技術領域】 本發明係有關於使用各向異性導電膜將驅動器裝在基 板之電極之方法及具有安裝驅動器之構造之基板與 性導電膜。 八 二、 【先前技術】 在裝入液晶模組等之基板安裝驅動器等零件之情況, 使用稱為 ACF (An i s 〇 t r 〇p i c C ond uc t i v e F i 1 m)之各向異性 導電膜安裝之方法。各向異性導電膜如圖88所示,係將微 量之導電粒子1 0 4隨機的分散於厚度2 〇〜3 〇 # m之膠帶狀之 黏接劑1 0 2之高密度電極之連接材料。微量之導電粒子丨〇 4 係V電性之设包覆樹脂製之核心而形成。此外,將膠帶狀 之膠合劑102稱為膠合劑。 " 以下,以液晶模組之組立為例,說明使用各向異性導 電膜1 0 0之零件之安裝。又,在各圖共用之符號使用相同 之符號。 將陣列基板1 1 0和彩色濾光器基板相向,藉著在陣列 基板11 0和彩色濾光器基板之間隙將液晶密封之液晶單 元’再安裝背光或驅動器等,組成液晶模組。 、,在液晶模組之組立,將TCP(Tape Carrier package輸 送膠帶封裝體)和液晶單元之電極連接。TCp丨〇 6係將 Ljl (Large Scale Integration,大型積體電路)晶片放在 薄型之膠卷狀印刷電路之LSi封裝。Tcpi〇6也稱為 TAB-IC(Tape Automated BondingIC,帶狀自動接合式1251108 V. INSTRUCTION OF THE INVENTION (1)---- 1. TECHNICAL FIELD The present invention relates to a method of mounting an actuator on an electrode of a substrate using an anisotropic conductive film, and a substrate having a structure in which a driver is mounted Conductive film. VIII. [Prior Art] When mounting a component such as a driver on a substrate such as a liquid crystal module, an anisotropic conductive film called ACF (An is 〇tr 〇 pic C on uc tive F i 1 m) is used. The method. As shown in Fig. 88, the anisotropic conductive film is obtained by randomly dispersing a small amount of conductive particles 104 in a bonding material of a high-density electrode of a tape-like adhesive of thickness 2 〇 〜 3 〇 # m. A trace amount of conductive particles 丨〇 4 is formed by forming a core made of a resin. Further, the tape-like glue 102 is referred to as a glue. " The following is an example of the assembly of an anisotropic conductive film 100 using the assembly of a liquid crystal module. Further, the same symbols are used for the symbols shared by the respective drawings. The array substrate 110 and the color filter substrate are opposed to each other, and a liquid crystal module is formed by re-installing a backlight or a driver or the like on the liquid crystal cell sealed by the liquid crystal cell in the gap between the array substrate 110 and the color filter substrate. In the assembly of the liquid crystal module, TCP (Tape Carrier package) is connected to the electrodes of the liquid crystal cell. The TCp丨〇 6 system places Ljl (Large Scale Integration) wafers in a LSi package of a thin film-like printed circuit. Tcpi〇6 is also called TAB-IC (Tape Automated BondingIC).

第10頁 1251108 五、發明說明(2) 1C)。在TCP1 06包含液晶模組之驅動器。 如圖8b所不’用Tcp 1 〇β和液晶單元之陣列基板11 〇夾 住各向異性導電膜1 〇 〇後,如圖8 C所示,加壓•加熱。各 向異性導電膜1 0 〇之膠合劑〗〇2液化,藉著液化之膠合劑σ 1 〇2冷卻後硬化,可速接陣列基板〇和Tcpi〇6。用導電粒 子104連接TCP1 06之電極和陣列基板丨1〇之電極。因此, TCP1 06之電路和陣列基板11〇在電性上連接,藉以驅動液 晶模組。 因將各向異性導電膜i 〇 0加熱所產生之熱會向陣列基 板110之電極周邊傳導,能將液晶單元之構件加熱•冷4 部。因此’在液晶單元之構件發生膨脹•收縮。因各構件 之熱膨脹率不同,發生膨脹·收縮所引起之應力但若為了 力而降低加熱溫度,則無法確實的連^Tcpi〇6二而 k成接觸不良。。 *日士又道1f106之電極間隔及陣列基板110之電極間隔變 :二電粒子104會令電極間短路之機會升高。因此, no之電極之間。可是,只是加壓·加熱, ^=104之位置。因導電粒子104所引起之電極間短路,令 液日日权組之製造良率降低c 三、【發明内容】 發明欲整^決之譟題 種使用各向異性導電膜之安 本發明之目的在於提供 !2511〇8Page 10 1251108 V. Description of the invention (2) 1C). The driver of the LCD module is included in TCP1 06. After the anisotropic conductive film 1 〇 is sandwiched between Tcp 1 〇β and the array substrate 11 of the liquid crystal cell as shown in Fig. 8b, as shown in Fig. 8C, pressurization and heating are performed. The anisotropic conductive film 10 〇 glue 〇 2 is liquefied, cooled by the liquefied glue σ 1 〇 2 and hardened, and the array substrate 〇 and Tcpi 〇 6 can be connected. The electrodes of the TCP 106 and the electrodes of the array substrate are connected by conductive particles 104. Therefore, the circuit of TCP 106 and the array substrate 11 are electrically connected to drive the liquid crystal module. The heat generated by heating the anisotropic conductive film i 〇 0 is conducted to the periphery of the electrode of the array substrate 110, and the members of the liquid crystal cell can be heated and cooled by four parts. Therefore, the components of the liquid crystal cell expand and contract. Since the thermal expansion coefficient of each member is different, the stress caused by expansion and contraction occurs. However, if the heating temperature is lowered for the purpose of force, it is impossible to reliably connect the contact with the Tcpi〇6. . * The electrode spacing of the 1f106 and the electrode spacing of the array substrate 110 are changed: the second electric particles 104 increase the chance of short circuit between the electrodes. Therefore, no between the electrodes. However, it is only the position of pressurization and heating, ^=104. Due to the short circuit between the electrodes caused by the conductive particles 104, the manufacturing yield of the liquid Japanese yen group is lowered. c. [Inventive content] The object of the invention is to use an anisotropic conductive film for the purpose of the invention. It is provided! 2511〇8

= ΐ使用各向異性導電膜之基板連接零件時,抑 發明^ 構件之傳熱,而且電極間不會產生短路。本 ^ # -一目的在於提供一種基板,具有連接TCP等安f 件之構造。此外,本發明之另外的目的 種各向異性導電膜,用於TCP等之安裝方式。 ” 課題之方4 本發明之驅動器之安裝方法,使用各向異性導電 ,動斋安裝在基板,包含以下之步驟:以該基板和驅動琴 夾,各向異性導電膜;對該各向異性導電膜所含之導電粒 子施加磁場,而使導電粒子產生渦電流及磁滯裉失之^ 驟,利用因该渦電流及磁滯損失而產生之導電粒子之熱, 令該各向異性導電膜所含之樹脂液化之步驟;及令液彳匕之 該樹脂硬化,而以導電粒子連接基板之電極和驅動器 極。 00冤 本發明之驅動器之安裝方法,可包含利用該磁場梯产 將該導電粒子收集於基板之電極和驅動器之電極之間之二 驟。 v 本發明之基板,在驅動器裝載部將導體、在該導體上 所形成之絕緣層以及用以和在該絕緣層上所形成之聽動哭 連接之電極疊層後,藉著使電流流向該導體,可在該電ϋ 上產生磁場。 本發明之基板,在内部形成導體,在驅動器裝载部# 成用以和驅動恭連接之電極,精著使電流流向該導體, 4= 时 When the substrate is connected using an anisotropic conductive film, the heat transfer of the device is prevented, and no short circuit occurs between the electrodes. The purpose of this is to provide a substrate having a structure in which a TCP or the like is connected. Further, another object of the present invention is an anisotropic conductive film for use in a mounting manner of TCP or the like. The method of mounting the driver of the present invention, using anisotropic conduction, and mounting on the substrate, comprises the steps of: anisotropic conductive film with the substrate and the driving mechanism; and the anisotropic conductive film The conductive particles contained in the film apply a magnetic field, and the conductive particles generate eddy currents and hysteresis, and the heat of the conductive particles generated by the eddy current and the hysteresis loss is used to make the anisotropic conductive film a step of liquefying the resin; and curing the resin of the liquid helium, and connecting the electrode of the substrate and the driver electrode with the conductive particles. 00冤 The mounting method of the driver of the present invention may include using the magnetic field to produce the conductive particle Collecting between the electrode of the substrate and the electrode of the driver. v The substrate of the present invention, the conductor, the insulating layer formed on the conductor, and the sound formed on the insulating layer at the driver loading portion After the electrode stack of the crying connection is connected, a magnetic field can be generated on the electrode by causing a current to flow to the conductor. The substrate of the present invention forms a conductor inside and is mounted on the driver. And electrode portions for driving into Christine # of connected, so that the current flows to the fine conductor 4

第12頁 l25ll〇8Page 12 l25ll〇8

在該電極上產生磁場。 本發明之基板’該導體之形狀亦可為蛇行形狀。 本發明之各向異性導電膜,包含導電粒子和膠合劑 邊導電粒子可包含鐵磁性體的構成。 四、【實施方式】 豐Jg之實施你1A magnetic field is generated on the electrode. The substrate of the present invention may also have a serpentine shape. The anisotropic conductive film of the present invention comprises conductive particles and a binder. The conductive particles may comprise a ferromagnetic material. Fourth, [Implementation] Feng Jg implementation of you 1

^使用圖面說明本發明之驅動器的安裝方法及基板之實 加例。在此,在驅動器包含晶片或TCp等之安裝對象零 件。又/在基板包含作為液晶單元之基板之玻璃或 PCBCPrinted Circuit Board ’印刷電路板)等安裝基板。 如圖1所示,用以將驅動器12裝在基板14之壓著頭Μ (bonding head)對驅動器12、ACF(各向異性導電膜)5〇以 及基板1 4施加壓力,而且施加磁場。驅動器丨2之電極丨5例 如係反磁性體之金或銅。基板〗4之電極丨5例如係順磁性體 之鋁。The mounting method of the driver of the present invention and the actual example of the substrate will be described using the drawings. Here, the driver includes a mounting object such as a wafer or a TCp. Further, a mounting substrate such as a glass or a PCBCPrinted Circuit Board printed circuit board as a substrate of the liquid crystal cell is included in the substrate. As shown in Fig. 1, a bonding head for mounting the driver 12 on the substrate 14 applies pressure to the driver 12, the ACF (anisotropic conductive film) 5, and the substrate 14, and a magnetic field is applied. The electrode 丨 of the driver 丨 2 is, for example, gold or copper of a diamagnetic body. The electrode crucible 5 of the substrate 4 is, for example, aluminum of a paramagnetic body.

在圖3a表不埋入壓著頭1〇之導體基板16。導體基板16 係將導體1 7黏在導體丨7用之基板丨8後和交流電源連接而形 成。導體1 7係蛇行形狀,交互重複線狀之部分和折回部2 〇 而形成。以下’在本專利說明書,在圖3b將導體17之線狀 之部分17a和經由折回部2〇a袓鄰之導體17之線狀之部分 1 7 b之中心線稱為間距線2 2。 如以下之說明所示,在圖3b彼此相鄰之間距線22a和 2 2b之間隔和安裝之基板14及驅動器12之電極15間之間隔The conductor substrate 16 of the crimping head 1 is not embedded in Fig. 3a. The conductor substrate 16 is formed by adhering the conductor 17 to the substrate 丨 8 for the conductor 丨 7 and then connecting it to an alternating current power source. The conductor 17 is a serpentine shape, and is formed by alternately repeating a linear portion and a folded portion 2 〇. In the present specification, the center line of the linear portion 17a of the conductor 17 and the linear portion 17b of the conductor 17 adjacent to the folded portion 2〇a is referred to as a pitch line 2 2 in Fig. 3b. As shown in the following description, the interval between the adjacent lines 22a and 22b and the interval between the mounted substrate 14 and the electrode 15 of the driver 12 are adjacent to each other in Fig. 3b.

第13頁 1251108 五、發明說明(5) —^ 相等。換言之,和應安裝之基板1 4及驅動器1 2之電極丨5間 之間距對應的決定間距線22之間隔,將導體17形成蛇行形 狀。導體基板1 6用於使施加磁場之電流流向各向異性導^ 膜50。 ’ 在圖2表示各向異性導電膜5 〇之構造。各向異性導電 膜5 0由用樹脂等形成之膠合劑5 2和混入膠合劑5 2之導電粒 子54構成。膠合劑52係周知之黏接材料,藉著加熱至高溫 時液化,然後利用冷卻硬化。 本發明之導電粒子5 4和以往之導電粒子不同,包含鐵 磁性體。.例如如圖2所示,由球形之核心56、包覆核心56 之鐵磁性層5 8以及包覆鐵磁性層5 8之殼6 〇構成。核心5 β如 以往般係樹脂性核心,對於壓力具有柔軟性。鐵磁性層58 如以下之說明所示,用鐵磁性且對於磁場之磁滯損失大之 材料形成。例如鐵磁性層58用!^、c〇、Fe等形成。殼6〇係 對鐵磁性層5 8例如鍛金的。 ’' 、導電粒子54所含之鐵磁性層53受到交流磁場作用時產 生渦電流,持久的發熱。又,鐵磁性層58受到交流磁場作 用時因磁滯損失而週期性的發熱。 在圖4表示鐵磁性體在磁場中之磁滯。藉著自外部供 給鐵磁性層58交流磁場,以CDEFGC包圍之面積之功作為z磁 滞損失所引起之發熱,用於安裝。 使用圖5說明將驅動器丨2裝在基板14之方法。將各向 異性導電膜50黏在基板14或驅動器12。將基板14之電極15 和驅動器12之電極15之位置對準後,使得在其中間夾住各Page 13 1251108 V. Description of invention (5) —^ Equal. In other words, the conductor 17 is formed into a serpentine shape at a distance from the corresponding pitch line 22 between the substrate 14 to be mounted and the electrode 5 of the driver 12. The conductor substrate 16 is for flowing a current applying a magnetic field to the anisotropic film 50. The structure of the anisotropic conductive film 5 表示 is shown in Fig. 2 . The anisotropic conductive film 50 is composed of a binder 5 2 formed of a resin or the like and conductive particles 54 mixed with a binder 5 2 . The adhesive 52 is a well-known adhesive material which is liquefied by heating to a high temperature and then hardened by cooling. The conductive particles 504 of the present invention, unlike conventional conductive particles, comprise a ferromagnetic body. For example, as shown in FIG. 2, the spherical core 56, the ferromagnetic layer 58 covering the core 56, and the shell 6 包覆 covering the ferromagnetic layer 58 are formed. The core 5 β is a resinous core as in the past and is soft to pressure. The ferromagnetic layer 58 is formed of a material having ferromagnetism and a large hysteresis loss to a magnetic field as shown in the following description. For example, the ferromagnetic layer 58 is formed using ^^, c〇, Fe, or the like. The shell 6 is a pair of ferromagnetic layers 58 such as wrought gold. The ferromagnetic layer 53 contained in the conductive particles 54 generates an eddy current when subjected to an alternating magnetic field, and generates a long-lasting heat. Further, when the ferromagnetic layer 58 is subjected to an alternating magnetic field, it periodically generates heat due to hysteresis loss. The hysteresis of the ferromagnetic body in the magnetic field is shown in FIG. The external magnetic field of the ferromagnetic layer 58 is supplied from the outside, and the work of the area surrounded by the CDEFGC is used as heat generated by the z hysteresis loss for mounting. A method of mounting the driver 丨 2 on the substrate 14 will be described using FIG. The anisotropic conductive film 50 is adhered to the substrate 14 or the driver 12. Aligning the electrodes 15 of the substrate 14 with the electrodes 15 of the driver 12, so that each of them is sandwiched therebetween

12511081251108

向異性導電膜5〇 〇 其久’將壓著頭1 〇、基板1 4以及驅動器1 2之電極1 5之 位^對準。如上述所示,在壓著頭丨〇埋入形成了蛇行形狀 之V體1 7之導體基板16。首先,將壓著頭丨〇所含之導體基 板1 6之導體1 7之位置對準,使其被夾入到基板14和驅動器 12之電極15間。又,如後述所示,將壓著頭1〇和電極15之 位置對準,使得在導體17之間距線22上產生之磁場相加 強’間距線2 2和電極15之中心線大致重疊。 位置對準完了後,用壓著頭1 〇對驅動器丨2施加壓力, 用基板14及驅動器12夾入各向異悻導電臈5〇。可是,照這 f原封不動時因膠合劑52熔解及未凝固,依然未安裝馬區動 态1 2 〇 接著,使交流電流流向在壓著頭1 〇所埋入之導體基板 息上之導體1 7。結果,導體基板16產生動態磁場。該磁場 ^有與基板1 4及驅動器1 2垂直之磁力線。該交流磁場之磁 線受到包含鐵磁性層5 8之導電粒子54強力束縛,4 u ^ 戶斤一 •、可 如上連 1不’導電粒子54因渦電流及磁滯損失而發熱。 體 大 上 (〇 調 所 在此,將作用於導電粒子54之磁場調整為供給鐵磁性 之飽和磁化之強度,使得磁滯損失所引起之發熱變成旧 。設供給飽和磁化之外部磁化強度為H s時,在外却、, 她加H = Hs X SI Ν( ω t)。在此,t表示時間。關於頻率 ’考慮自鐵磁性體之粒子密度所計算之應供給之能量 整最佳值。由於溫度上升,飽和磁化量減少,罐^ $产 弓丨起之發熱量減少,但是例如在使用鎳之情況,/ t壞 囚居里Aligning the opposite polarity conductive film 5 for a long time 'aligns the head 1 〇, the substrate 14 and the electrode 15 of the driver 1 2 . As described above, the conductor substrate 16 of the V body 17 in which the meandering shape is formed is embedded in the pressing head. First, the position of the conductor 17 of the conductor substrate 16 included in the crimping head is aligned so as to be sandwiched between the substrate 14 and the electrode 15 of the driver 12. Further, as will be described later, the positions of the crimping head 1 and the electrode 15 are aligned such that the magnetic field generated between the conductors 17 from the line 22 is strongly increased. The pitch line 2 2 substantially overlaps the center line of the electrode 15. After the alignment is completed, pressure is applied to the actuator 丨2 by the pressing head 1 ,, and the opposite-direction conductive 臈 5 夹 is sandwiched between the substrate 14 and the driver 12. However, when the f is intact, the adhesive 52 is melted and not solidified, and the dynamics of the horse zone is still not installed. Then, the alternating current flows to the conductor 1 of the conductor substrate embedded in the crimping head 1 〇. 7. As a result, the conductor substrate 16 generates a dynamic magnetic field. The magnetic field has magnetic lines perpendicular to the substrate 14 and the driver 12. The magnetic field of the alternating magnetic field is strongly bound by the conductive particles 54 including the ferromagnetic layer 58, and can be heated as a result of eddy current and hysteresis loss. In the body, the magnetic field acting on the conductive particles 54 is adjusted to the intensity of the saturation magnetization of the ferromagnetic material, so that the heat generated by the hysteresis loss becomes old. The external magnetization for supplying the saturation magnetization is H s . At the time of the outside, she adds H = Hs X SI Ν( ω t). Here, t represents time. Regarding the frequency 'considered from the particle density of the ferromagnetic body, the energy optimum value should be supplied. As the temperature rises, the amount of saturation magnetization decreases, and the amount of heat generated by the cans is reduced, but for example, in the case of using nickel, / t is in a bad prison.

1251108 五、發明說明(7) 溫度(Curie temperature)係385 t:,對於實際之 發揮效力。 ”文展充分 於是因利用導電粒子5 4 心局部的對膠合劑52加熱, 起之發熱將熱傳給膠合劑5 2 之發熱’能以導電粒子54為中 利用該導電粒子5 4之磁場戶^引 ’膠合劑5 2液化。 利用膠合劑52液化後至硬化之期間,例如約i秒鐘, 令在電極15上排列導電粒子。導體基板16如上述所示, 將導體17配線—成蛇行形狀,在各間距線22產生磁場強之邻 分。如圖5所示,將導體17配線使得預先在應連接之電極 15之部分產生磁場強之部分時,在導體17上方磁場變弱, 作用於膠合劑52之磁場具有圖6所示之磁場梯度。結果, 在電極1 5之部分產生朝導電粒子54集中之方向之力。 該力之原理係供給外部磁場時,導磁率大之物質(導 電粒子54)被導磁率小之物質吸引。因引力和磁場之平方 ^正比’猶微的磁場差異可產生大的引力。膠合細液化 h,導電粒子5 4變成易動,易集中於磁場強之電極工5之部 如上述所示,因可蚀^呈—$ ^ ^ t J便侍在電極15附近導電粒子54密 ΐ J相^之電極1 5間導電粒子5 4疏,電極間之連接變得 貝又因導電粒子54集中於各電極15,可防止導電 粒子54所引起之電極間之短路。 在圖7表不時間、磁摄 、, 、 磁穷以及壓力之關係。在上述之方 法利用溫升完成壓接時,昔土 ,m ^ ^ _ a 、 专 百先使作用磁場消失,接著除去 作用壓力後’元成安裝。佑储+ 、 依據品要,以低磁力退火。1251108 V. INSTRUCTIONS (7) Temperature (Curie temperature) is 385 t:, which is effective for practical use. "The exhibition is sufficient to heat the adhesive 52 by using the conductive particles 5 4, and the heat is transferred to the heat of the adhesive 5 2 ', and the conductive particles 54 can be used as the magnetic field of the conductive particles 54 The liquid crystal is liquefied by the binder 52. After the liquefaction with the binder 52 is liquefied, for example, for about i seconds, the conductive particles are arranged on the electrode 15. The conductor substrate 16 is wired as shown above. The shape generates a neighboring point of the magnetic field strength at each of the pitch lines 22. As shown in Fig. 5, when the conductor 17 is wired so that a portion of the electrode 15 to be connected is generated in advance, the magnetic field becomes weaker above the conductor 17, and the effect is weak. The magnetic field of the binder 52 has a magnetic field gradient as shown in Fig. 6. As a result, a force is generated in a portion of the electrode 15 toward the direction in which the conductive particles 54 are concentrated. The principle of the force is a substance having a large magnetic permeability when an external magnetic field is supplied ( The conductive particles 54) are attracted by a substance having a small magnetic permeability. Because the square of the gravitational force and the magnetic field is proportional to the magnetic field difference of the judging, a large gravitational force can be generated. The gluing is liquefied, the conductive particles 54 become easy to move, and are easily concentrated in the magnetic field. As shown above, the electrode 5 is as shown above, and the conductive particles 54 are in contact near the electrode 15 because of the etchable surface. The electrode of the J phase is 5, the conductive particles 5 4 are thin, and the electrodes are connected. It is also possible to prevent the short circuit between the electrodes caused by the conductive particles 54 because the conductive particles 54 are concentrated on the respective electrodes 15. The relationship between time, magnetic resonance, magnetic poorness, and pressure is shown in Fig. 7. When the temperature rise is used to complete the crimping, the soil, m ^ ^ _ a , and the special 100 first make the working magnetic field disappear, and then remove the working pressure and then 'yuan installation. You save +, according to the product, with low magnetic annealing.

!2511〇8 兒明(8) ---- 在上述之實施例,將導體基板16埋入壓著頭i〇,但是 =可將導,基=16裝入基板14,將導體基板16放置於基板 之驅動器1 2裝载部分後,用絕緣層包覆導體基板1 6上, ,絕緣層上形成電極。或者,亦可將導體丨7直接配置於基 扳14之驅動器12裝載部分。 在基板1 4上所形成之導體1 7之形狀係蛇行形狀。導體 Η之蛇行形狀係,在絕緣層上形成電極15,使得間距線22 和電極15之中心線大致重疊。又,和上述之實施例一樣, 將基板1 4之電極1 5和驅動器1 2之電極1 5之位置對準,使得 在其中間夾住各向異性導電膜5 Q。 抑在本貫施例,也令各向異性導電膜5 〇介於基板丨4及驅 動器1 2之間後’用壓著頭1 〇施力口壓力。又,將驅動器1 2裝 ,基板14之機構和上述之實施例的一樣。可是,和上述之 貫施例不同,在基板1 4上形成之導體1 7產生磁場。又,也 =需要如上述之實施例所示之壓著頭1〇、基板丨4以及驅動 器12之電極15之精密之位置對準。 或者亦可將導體1 7直接配線於基板14中。在本實施 例’因基板1 4係絕緣體,不必新形成絕緣層。只要在基板 14形成導體基板16,使得係蛇行形狀之導體17之間距線22 和電極15之中心線大致重疊即可。以後和删才之該實施例 一樣,可將驅動器1 2安裝於基板丨4。 在本發明,在驅動器可包含晶元或TCP等全部之安裝 對象零件。又,在基板包含玻璃基板或PCB等全部之安裝 基板。又,導電粒子54只要包含鐵磁性體的形成,成分、!2511〇8 儿明(8) ---- In the above embodiment, the conductor substrate 16 is buried in the pressing head i〇, but = the guide, the base = 16 is placed in the substrate 14, and the conductor substrate 16 is placed. After the portion of the driver 12 of the substrate is loaded, the conductor substrate 16 is covered with an insulating layer, and an electrode is formed on the insulating layer. Alternatively, the conductor turns 7 may be disposed directly on the load portion of the driver 12 of the base 14. The shape of the conductor 17 formed on the substrate 14 is a serpentine shape. The serpentine shape of the conductor is such that the electrode 15 is formed on the insulating layer such that the pitch line 22 and the center line of the electrode 15 substantially overlap. Further, as in the above-described embodiment, the positions of the electrode 15 of the substrate 14 and the electrode 15 of the driver 12 are aligned so that the anisotropic conductive film 5 Q is sandwiched therebetween. In the present embodiment, the anisotropic conductive film 5 is also interposed between the substrate 丨4 and the actuator 12, and the pressure is applied by the pressing head 1. Further, the mechanism for mounting the driver 12 and the substrate 14 is the same as that of the above embodiment. However, unlike the above-described embodiments, the conductor 17 formed on the substrate 14 generates a magnetic field. Further, it is also necessary to precisely position the pressing head 1 〇, the substrate 丨 4, and the electrode 15 of the driver 12 as shown in the above embodiment. Alternatively, the conductors 17 may be directly wired in the substrate 14. In the present embodiment, it is not necessary to newly form an insulating layer due to the substrate 14-based insulator. As long as the conductor substrate 16 is formed on the substrate 14, the conductors 17 of the serpentine shape are substantially overlapped from the center line of the line 22 and the electrode 15. The driver 12 can be mounted on the substrate stack 4 in the same manner as this embodiment. In the present invention, all of the mounting object parts such as a wafer or a TCP may be included in the driver. Further, the substrate includes all of the mounting substrates such as a glass substrate or a PCB. Further, the conductive particles 54 include a ferromagnetic body, a composition, and

第17頁 1251108 五、發明說明(9) 材料、構造等未特別限定。此外,導體1 7之形成形狀未限 定為蛇行形狀,包含使電流流動後產生之磁場局部的發生 強弱之全部之形狀。 :此外,本發明在未超出其主旨之範圍内,能以依照該 素者之知識進行各種改良、修正、變更之形態實施。 發明之效果 如以上所示,因利用磁場將包含鐵磁性體之導電粒子 加熱,產生之熱係局部性的。因此,不會將不需要基板之 位置加熱•冷卻,可防止熱所引起之應力發生。 又,利用磁場梯度可令在電極上排列導電粒子,可將 導電粒子集中於連接之電極間。因此,電極間之連接變成 更確實。而,在相鄰之電極間因導電粒子疏,可防止經由 導電粒子之相鄰之電極間之短路。 利用如上述之局部性之加熱及導電粒子之局部化,可 實現驅動器之超高密度及高可靠性之安裝。Page 17 1251108 V. INSTRUCTIONS (9) Materials, structures, etc. are not particularly limited. Further, the shape of the conductor 17 is not limited to a meandering shape, and includes a shape in which all of the magnetic field generated by the current flow is generated. In addition, the present invention can be implemented in various modifications, corrections, and changes in accordance with the knowledge of the subject matter within the scope of the invention. Advantageous Effects of Invention As described above, the conductive particles containing the ferromagnetic material are heated by the magnetic field, and the heat generated locally is localized. Therefore, the position of the substrate is not required to be heated and cooled, and the stress caused by heat can be prevented. Further, by using a magnetic field gradient, conductive particles can be arranged on the electrodes, and the conductive particles can be concentrated between the connected electrodes. Therefore, the connection between the electrodes becomes more certain. Further, since the conductive particles are sparse between the adjacent electrodes, the short circuit between the adjacent electrodes passing through the conductive particles can be prevented. The localized heating as described above and the localization of the conductive particles enable ultra-high density and high reliability mounting of the driver.

1251108 圖式簡單說明 五、【圖式簡單說明】 圖1係表示本發明之安裝方法之示意圖。 圖2係本發明之ACF(各向異性導電膜)、導電粒子以及 導電粒子之剖面圖。 圖3 (a)係本發明之導體基板之平面圖。 圖3(b)係本發明之導體基板之導體部分之放大圖。 圖4係表示鐵磁性體在磁場中之磁場和磁通密度之關 係之磁滯。1251108 Brief description of the drawings V. [Simple description of the drawings] Fig. 1 is a schematic view showing the mounting method of the present invention. Fig. 2 is a cross-sectional view showing an ACF (anisotropic conductive film), conductive particles, and conductive particles of the present invention. Figure 3 (a) is a plan view of a conductor substrate of the present invention. Fig. 3 (b) is an enlarged view of a conductor portion of the conductor substrate of the present invention. Fig. 4 is a graph showing the hysteresis of the relationship between the magnetic field of the ferromagnetic body in the magnetic field and the magnetic flux density.

圖5係表不本發明之安裝方法之不意圖之放大圖。 圖6係在本發明之安裝方法表不磁場梯度和作用於導 電粒子之力之示意圖。 圖7係表示在本發明之安裝方法之時間和壓力以及磁 場之關係之關係圖。 圖8 (a)係各向異性導電膜之剖面圖。 圖8(b)係經由各向異性導電膜將TCP裝在陣歹,J基板之 狀況之示意圖。 圖8 (c )係經由各向異性導電膜令TCP和陣列基板連接 之狀況之示意圖。Fig. 5 is an enlarged view showing an unintentional installation method of the present invention. Fig. 6 is a schematic view showing the magnetic field gradient and the force acting on the conductive particles in the mounting method of the present invention. Fig. 7 is a graph showing the relationship between time and pressure and magnetic field in the mounting method of the present invention. Fig. 8(a) is a cross-sectional view showing an anisotropic conductive film. Fig. 8(b) is a view showing a state in which TCP is mounted on a matrix and a J substrate via an anisotropic conductive film. Fig. 8(c) is a view showing a state in which TCP and an array substrate are connected via an anisotropic conductive film.

元件符號說明: 10壓著頭 12 驅動器 14 基板 15 電極Component symbol description: 10 pressing head 12 driver 14 substrate 15 electrode

第19頁 1251108 圖式簡單說明 16導體基板 17導體 1 8 將導體配線之基板 2 0 折回部 2 2 間距線 50 本發明之各向異性導電膜 Μ 膠合劑 54 導電粒子 56 核心 5 8 鐵磁性層 60 殼 100 各向異性導電膜 102 膠合劑 104 導電粒子Page 19 1251108 Schematic description of 16 conductor substrate 17 conductor 1 8 Conductor wiring substrate 20 0 folded back portion 2 2 pitch line 50 Anisotropic conductive film of the present invention 胶 Glue 54 Conductive particles 56 Core 5 8 Ferromagnetic layer 60 shell 100 anisotropic conductive film 102 adhesive 104 conductive particles

106 TCP 108 電極 11 0 陣列基板106 TCP 108 electrode 11 0 array substrate

第20頁Page 20

Claims (1)

12511081251108 電膜將驅動 六、申請專利範圍 1 · 一種驅動器安裝方法 器安裝在基板,包含如下步驟: 以該基板和驅動器夾住各向異性導電膜之步驟· 對該各向異性導電膜所含之導電粒子施加磁場i 導電粒子產生渦電流及磁滯損失之步驟; ’而使 利用因該渴電流及磁滯損失而產生之導電粒子 令該各向異性導電膜所含之樹脂液化之步驟;及 …、’ 令液化之該樹脂硬化,而以導電粒子連接其./ 和驅動器之電極之步驟。 2 ·如申睛專利範圍第1項之驅動器安裝方法,其中 包含利用该磁場之梯度將該導電粒子收集於基板之電極和 驅動器之電極之間的步驟。 3· —種基板,在驅動器裝載部上疊設導體、在該導體 亡所形成之絕緣層、及用以和在該絕緣層上所形成之驅動 器連接之電極,藉著使電流流向該導體而於該電極上產生 磁場。 、4 · 一種基板,於其内部形成導體,在驅動器裝載部形 成用以和驅動器連接之電極,藉著使電流流向該導體而於 該電極上產生磁場^ 5·如申請專利範圍第3或4項之基板,其中,該導體之 形狀係蛇行形狀。 、6 · —種各向異性導電膜,包含導電粒子和膠合劑,而 该導電粒子包含鐵磁性體。The electric film will drive the sixth. Patent application 1 1. A driver mounting method is mounted on a substrate, and includes the following steps: a step of sandwiching the anisotropic conductive film with the substrate and the driver · Conducting the anisotropic conductive film a step of applying a magnetic field i to the particles to generate eddy current and hysteresis loss; and a step of liquefying the resin contained in the anisotropic conductive film by using conductive particles generated by the thirst current and hysteresis loss; and... , 'The step of hardening the liquefied resin and connecting the electrodes with the conductive particles and/or the driver. 2. The driver mounting method of claim 1, wherein the step of collecting the conductive particles between the electrodes of the substrate and the electrodes of the driver by using the gradient of the magnetic field. 3. A substrate on which a conductor is stacked, an insulating layer formed on the conductor, and an electrode connected to a driver formed on the insulating layer, by causing a current to flow to the conductor. A magnetic field is generated on the electrode. And a substrate in which a conductor is formed, and an electrode for connecting to the driver is formed at the driver loading portion, and a magnetic field is generated on the electrode by causing a current to flow to the conductor. 5, as claimed in claim 3 or 4 The substrate of the item, wherein the shape of the conductor is a serpentine shape. An anisotropic conductive film comprising conductive particles and a binder, and the conductive particles comprise a ferromagnetic body.
TW92123060A 2003-03-18 2003-08-21 Driver mounting method using hysteresis loss, and substrate and anisotropic conductive film TWI251108B (en)

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