TWI223284B - Method and system for high-speed, precise micromachining an array of devices - Google Patents

Method and system for high-speed, precise micromachining an array of devices Download PDF

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TWI223284B
TWI223284B TW092106952A TW92106952A TWI223284B TW I223284 B TWI223284 B TW I223284B TW 092106952 A TW092106952 A TW 092106952A TW 92106952 A TW92106952 A TW 92106952A TW I223284 B TWI223284 B TW I223284B
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Taiwan
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cutting
laser
micro
scope
patent application
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TW092106952A
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Chinese (zh)
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TW200305891A (en
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Bruce L Couch
Jonathan S Ehrmann
Yun Fee Chu
Joseph V Lento
Shepard D Johnson
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Gsi Lumonics Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01CRESISTORS
    • H01C17/00Apparatus or processes specially adapted for manufacturing resistors
    • H01C17/22Apparatus or processes specially adapted for manufacturing resistors adapted for trimming
    • H01C17/24Apparatus or processes specially adapted for manufacturing resistors adapted for trimming by removing or adding resistive material
    • H01C17/242Apparatus or processes specially adapted for manufacturing resistors adapted for trimming by removing or adding resistive material by laser
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B23MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
    • B23KSOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
    • B23K26/00Working by laser beam, e.g. welding, cutting or boring
    • B23K26/351Working by laser beam, e.g. welding, cutting or boring for trimming or tuning of electrical components

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Plasma & Fusion (AREA)
  • Manufacturing & Machinery (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Mechanical Engineering (AREA)
  • Laser Beam Processing (AREA)
  • Apparatuses And Processes For Manufacturing Resistors (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)

Abstract

A method and system for high-speed, precise micromachining an array of devices are disclosed wherein improved process throughput and accuracy, such as resistor trimming accuracy, are provided. The number of resistance measurements are limited by using non-measurement cuts, using non-sequential collinear cutting, using spot fan-out parallel cutting, and using a retrograde scanning technique for faster collinear cuts. Non-sequential cutting is also used to manage thermal effects and calibrated cuts are used for improved accuracy. Test voltage is controlled to avoid resistor damage.

Description

1223284 玖、發明說明 (發明說明應敘明:發明所屬之技術領域、先前技術、内容、實施方式及圖式簡單說明) L發明所屬技術領域]1 相關專利與申請案之交互參考1223284 发明 Description of the invention (The description of the invention should state: the technical field to which the invention belongs, the prior art, the content, the embodiments, and a brief description of the drawings) L The technical field to which the invention belongs] 1 Cross-reference of related patents and applications

本案對於2002年3月28日所提出申請之標題為’’Laser 5 Based micro-Machining Method And System ,and an Application To High Speed Laser Trimming Of Chip Components And Similar Structures”之美國專利臨時申請 案號No. 60/368,421作權利主張。本案亦對以下之專利案 作優先權主張並且為其後續申請案:於2002年3月27曰提 10 出申請其標題為”Method for Processing a Device,Method and System for Modeling Same and the Device”之美國專利 申請案號10/108,101,其現在公告為美國專利案號 2002/0162973。而具有共同發明人且受讓給本發明受讓人 之標題為”Method and Apparatus for Shaping a Laser_Beam 15 Intensity Profile by Dithering”之美國專利案號,其在此整 個併入作為參考。本申請案亦與受讓給本案受讓人之標題 為 “Pulse Control In Laser Systems” 之美國專利案號 6,339,604有關。本申請案亦與以下之專利案有關。2002年 3月27曰提出申請共同待審之申請案號為1〇/107,027且受讓 20 給本發明受讓人標題為“High Speed,Laser Based Method and System for Processing Material of One or More Targets Within a Field”而現在公告為美國專利案號 No.2002/0170898。 發明領域 6 1223284 玖、發明說明 本發明疋有關於以高速精密微切削陣列裝置之方法。 本發明亦有關於電阻器切削之範圍,尤其是在薄膜塊結構 上曲折彎曲電阻器之切削。雷射電阻器切削是關於右導體 之間電阻材料區域中以雷射處理之切割。 5 【】 發明背景 包阻器切削(以及其他電子元件與電路之切削與微切 肖’J)在過去20年演進發展,而現在使用於調整厚膜、薄膜 以及其他電子技術所用之電路。此2〇〇1年所出版之,,雷射 1〇材料處理LIA手冊,,第583-588頁第17章,,切削,,包含揭示, 其說明雷射切削之數個觀點。本案第^至卜圖是從該出版 刊物併入。第la圖說明未經切削電阻器之電流線,而第化 圖說明雷射切割對於電流線之影響。第1(:圖以各種電阻器 幾何形狀與切削型式總結數項結果(穩定度、速率以及公 15 差)。 以下之典範美國專利是與雷射切削系統與方法有關, 專利案號:6,510,605 ; 6,322,711 ·’ 5,796,392 ; 4,901,052 ,4,853,671 ; 4,647,899 ; 4,511,607以及4,428,298。 美國專利案號4,429,298是關於曲折切削之許多觀點。 20基本上,此曲折式電阻器是以連續進給切割形成,且此最 後切削切割是對上一次進給切割所產生電阻器之邊緣平行 而實施。其描述從一場交替地在電阻器上作,,連續,,的進給 刀而考慮到·此進給切割最大與最小長度,對於切削 刀。〗之進給切割之電阻^界值,用於進給切割之較快切割 7 1223284 玖、發明說明 ^ , 速率乂及具有各種電阻與切割長度測試之結構化處理流程。 、,對於例如在所有操作尺度之精準切削之改良式高速微 切削有持績之須求,其範圍從厚膜電路至晶圓切削。 【劈^明内容】 5 發明概要 本务明之目的為提供一種用於高速精準微切削陣列裳 置之改良式方法與系統。 在執仃本發明之以上以及其他目的中,提供一種用於 高速精準微切削陣列裝置之方法。各裝置具有至少一可測 10量之特性。此方法包括以下步驟··⑷將在陣列中之裝置選 擇性地微切削,以改變此可測量特性之值;(b)將此選擇性 微切削之步驟中止;(c)當此選擇性微切削步驟中止時,將 在此系列中至少另一裝置選擇性地微切割,以改變其可測 量特性之值;以及(d)將此所中止之選擇性微切削步驟恢復 15 ,以改變此裝置可測量之特性一直至此值是在所想要的範 圍中為止。 此裝置可以為電阻器。 此等電阻器可以薄膜電阻器。 此選擇性微切削步驟可以切割裝置之至少一雷射光線 20 實施。 此方法可更包括測量至少一此等裝置之可測量特性以 獲得可測量之值。 此方法可更包括·將所測量之值與預先設定之臨界值 比較而獲得比較結果,並根據此結果將至少另一此等裝置 8 玖、發明說明 微切削。 此方法可以更包括^艮據 丨巧里之值將至少另一此等 裝置選擇性地微切割。 此方法可更包括:根據所 里之值而決定,不測量至 少另一此等裝置之可測量之值。 此方法可用於高速精準φ 贯早田射切削電阻器陣列,此等可 測量特性之一可以為電阻。 步驟 各此等選擇性微切削步驟可以包括選擇性去除材料 之 此陣列可以包括一或多個列與_或多個行之至少一個。 至少-個此等選擇性微切削步驟可以用多個聚焦雷射 脈衝實質上同時照射多個裝置而實施。 〜至少-個選擇性微切削步驟可以用多個聚焦雷射脈衝 貫施。此方法可更包括分配此聚焦雷射脈衝。 此分配步驟可以包括㈣··產生具有多個雷射光線之 分配圖案,並將此雷射光線聚焦。 此雷射切削可以在電阻器之導體之間之電阻性材料區 域中產生一系列數字間切割。 至少一選擇性微切削步驟可以包括步驟··將雷射光線 定位在此各此時待微切削裝置之位置,並且以至少一雷射 脈衝選擇性地照射此各此等待微切削裝置之至少_個部份。 至少一此等選擇性切削步驟可以包括步驟··以產生雷 射光線並將其相對定位於在陣列範圍中之第一方向中傳送 ’且以至少一雷射脈衝選擇地照射此範圍中至少一裝置之 玖、發明說明 ’ ’ 至少一個部份。 此方法更包括產生雷射光線並將其相對定位於與此範 圍中第一方向實質上相反之第二方向十傳送,並且以至少 -雷射脈衝選擇性地照射在範圍中至少一裝置之至少一第 5 二部份。 至少一此等選擇性微切削步驟可以包括··產生雷射光 線並將其相對定位於跨此等裝置之第_掃_案中傳送, 將第二掃瞄圖案與第一掃瞄圖案重疊,且以至少一雷射脈 衝照射至少一裝置。 此第二掃瞄圖案可以為回復掃瞄,且此照射至少一裝 置之至少—雷射脈衝之掃瞄速度是低於第一掃瞄圖案之相 對應掃瞎速度。可以將雷射能量集巾於至少-裝置,其集中 期間是長於與僅第-掃瞎圖案有關之期間,因此增加產量。 此第二掃猫圖案可以包括從第一裝置跳至第二裝置。 此選擇性微切削步驟可以多個雷射脈衝實%,且至少 -雷射脈衝可以具有㈣指焦耳至25亳焦耳之能量。 此所測量值可以為所測量溫度之值。 此等裝置可以實質上相同。 20The title of this application for the application filed on March 28, 2002 is "Laser 5 Based micro-Machining Method And System, and an Application To High Speed Laser Trimming Of Chip Components And Similar Structures". 60 / 368,421 as a claim. This case also claims priority to the following patent cases and its subsequent applications: on March 27, 2002, filed 10 applications with the title "Method for Processing a Device, Method and System for Modeling Same and the Device "U.S. Patent Application No. 10 / 18,101, which is now published as U.S. Patent No. 2002/0162973. The title of" Method and Apparatus for Shaping a Laser_Beam 15 Intensity Profile by Dithering ", which is incorporated herein by reference in its entirety. This application is also related to the US patent case entitled" Pulse Control In Laser Systems "assigned to the assignee of this case No. 6,339,604. This application is also related to the following patents. Application was made on March 27, 2002 The pending application number is 10 / 107,027 and Assignee 20 gives the assignee of the present invention the title "High Speed, Laser Based Method and System for Processing Material of One or More Targets Within a Field" and is now announced as the United States Patent case No. 2002/0170898. Field of invention 6 1223284 (1). Description of the invention The invention relates to a method for high-speed precision micro-cutting array device. The invention also relates to the scope of resistor cutting, especially on thin film block structure Cutting of zigzag resistors. Laser resistor cutting refers to laser-cut cutting in the area of the resistive material between the right conductors. 5 [] BACKGROUND OF THE INVENTION Resistor cutting (and other electronic components and circuits cutting and micro-cutting) Xiao'J) has evolved over the past 20 years and is now used to adjust circuits used in thick films, thin films, and other electronic technologies. Published in 2001, the Laser 10 Material Handling LIA Handbook, No. Chapter 17, 583-588, Cutting, contains revelations that illustrate several points of laser cutting. Figures ^ to 卜 in this case are incorporated from that publication. Figure la illustrates the current lines without cutting resistors, and figure 1 illustrates the effect of laser cutting on the current lines. Figure 1 (: The figure summarizes several results (stability, rate, and tolerance) with various resistor geometries and cutting patterns. The following typical US patents are related to laser cutting systems and methods, patent case number: 6,510,605; 6,322,711 · '5,796,392; 4,901,052, 4,853,671; 4,647,899; 4,511,607 and 4,428,298. U.S. Patent No. 4,429,298 is about many viewpoints of zigzag cutting. 20 Basically, this zigzag resistor is formed by continuous feed cutting, and This final cutting is performed parallel to the edges of the resistor produced by the previous feed cutting. Its description starts from a field that is made on the resistor alternately, continuously, and feeds the knife into consideration. This feed cutting is the largest And the minimum length, for the cutting blade. 〖The cutting resistance of the feed cutting ^ cutoff value for faster cutting of feed cutting 7 1223284 发明, invention description ^, rate 乂 and structured processing with various resistance and cutting length test There are requirements for improved high-speed micro-cutting, such as precision cutting at all operating scales, ranging from thick films Circuit-to-wafer cutting. [Abstract] 5 Summary of the Invention The purpose of the present invention is to provide an improved method and system for high-speed and accurate micro-cutting arrays. In carrying out the above and other purposes of the present invention, Provide a method for high-speed and precise micro-cutting array device. Each device has at least a measurable 10-quantity characteristic. This method includes the following steps: • Selectively micro-cut the device in the array to change the measurable The value of the characteristic; (b) abort this selective micro-cutting step; (c) when this selective micro-cutting step is aborted, at least another device in the series will be selectively micro-cut to change its measurable The value of the characteristic; and (d) resume the discontinued selective microcutting step 15 to change the characteristic that the device can measure until the value is in the desired range. The device can be a resistor. This The resistor can be a thin film resistor. This selective micro-cutting step can be performed by cutting at least one laser ray 20 of the device. This method can further include measuring at least one of these devices. Measure the characteristics to obtain a measurable value. This method may further include: comparing the measured value with a preset threshold to obtain a comparison result, and based on the result, at least one of these other devices 8 玖, invention description micro-cutting This method may further include selectively micro-cutting at least one of these other devices according to the values in the table. This method may further include: deciding not to measure at least one of these other devices based on the values in the table. Measurable value. This method can be used for high-speed and accurate φ through Waseda cutting resistor arrays. One of these measurable characteristics can be resistance. Each of these selective micro-cutting steps can include selective removal of the material. Include at least one of one or more columns and / or multiple rows. At least one of these selective micro-cutting steps can be performed with multiple focusing laser pulses irradiating multiple devices substantially simultaneously. ~ At least one selective micro-cutting step can be performed with multiple focused laser pulses. This method may further include allocating the focused laser pulse. This distribution step may include generating a distribution pattern having a plurality of laser rays and focusing the laser rays. This laser cutting can produce a series of interdigital cuts in the area of resistive material between the conductors of the resistor. The at least one selective micro-cutting step may include the step of positioning the laser light at the position of each of the micro-cutting devices at this time, and selectively irradiating at least one of the micro-cutting devices with at least one laser pulse. Parts. At least one of these selective cutting steps may include a step of: generating laser rays and transmitting them relatively positioned in a first direction in the array range, and selectively illuminating at least one of the ranges with at least one laser pulse. Device description, invention description '' At least one part. The method further includes generating laser rays and transmitting them relative to a second direction substantially opposite to the first direction in the range, and selectively irradiating at least one device in the range with at least a laser pulse. One part five two. At least one of these selective micro-cutting steps may include generating laser light and transmitting it relative to the scan case across these devices, overlapping the second scan pattern with the first scan pattern, And at least one device is irradiated with at least one laser pulse. The second scanning pattern may be a rescanning scan, and at least the laser pulse scanning speed of the at least one device is lower than the corresponding scanning speed of the first scanning pattern. The laser energy can be concentrated on at least the device, and the concentration period is longer than the period related to the first-literacy pattern, thereby increasing the yield. This second cat sweep pattern may include jumping from the first device to the second device. This selective micro-cutting step may be performed with multiple laser pulses, and at least-the laser pulse may have an energy in the range of Joules to 25 Joules. This measured value can be the value of the measured temperature. These devices may be substantially the same. 20

此外,在實施本發明之上述以及其他目的中,提供一 種系統用於高速雷射為主精準微切削陣列之裝置。各此等 裝置具有至少-可測量特性。此系統包括脈衝式雷射子系 統。將光學子系_合連接至脈衝式雷射系統,而以雷射 脈衝選擇性地照射此裝置之—部份。此搞合連接至子系統 控制控制此子系統以:(a)將在陣列中之裝置選擇性地 10 玖、發明說明In addition, in implementing the above and other objects of the present invention, a system for a high-speed laser-based precision micro-cutting array device is provided. Each of these devices has at least-measurable characteristics. This system includes a pulsed laser subsystem. The optical subsystem is connected to a pulsed laser system, and a part of the device is selectively illuminated with a laser pulse. This connection is connected to the subsystem. Control the subsystem to: (a) Select the devices in the array selectively.

微切削,以改變此可測量特性 > 佶,mI 付注之值,(b)中止此選擇性之微 切削;(C)當此選擇性微切削中止時,將此陣列中至少另一 裝置選擇性地微切削,以改變其可測量特性之值,以及⑷ 將此選擇性微切削恢復,以改變此裝置可測量之特性一直 5其值是在所想要的範圍中為止。 此光學子系統可以包括:偏光器與偏光控制器,用於 控制偏光器將雷射光線沿著第一掃猫圖案(其包括各此等 待微切削裝置)掃瞄。 此系統更包括測量子系統,以測量至少一此等裝置之 10 可測量特性之一。 此微切削可以為雷射切削,且此陣列可以為電阻器陣 列,且此測量子系統可以為探測器陣列。 此光學子系統可以包括第二偏光器,將高速第二掃瞄 圖案重璺至第一掃瞄圖案上,因此增加此系統之產量。 15 可以將控制器耦合連接至子系統,以致於可以控制此 子系統以產生用於至少一此等裝置之切削序列,其在微切 削期間降低裝置之溫度。 在發明上述以及其他之目的,特性與優點,將由以下 用於執行本發明之最佳模式之詳細說明並參考所附圖式而 20 為明顯。 圖式簡單說明 第la-lb圖為概要圖,其各說明在雷射切削之前與之 後之電流線; 第lc圖為圖表,其說明各種切割形成對數個切割參數 11 1223284 玖、發明說明 之影響; 第2a圖為配置成列與行之晶片電阻器陣列之概要圖, 其說明根據本發明實施例使用雷射切削步驟之結果; 第2b圖為進-步界定對應於第2a圖之切削步驟之方塊 5 流程圖; 第3圖為方塊流程圖,其進一步界定本發明系統中第 2a與2b圖之切削操作; 第4a圖為配置成列與行中之晶片電阻器陣列之概要圖 ,其說明根據本發明另一實施例使用雷射切削步驟之結果; 1〇 第朴圖為方塊流程圖,其進一步界定對應於第4a圖之 切削步驟; 第5圖為方塊流程圖;其進一步界定本發明系統中第 4a與4b圖之切削操作; 第6a圖為可以使用於本發明至少一實施例中雷射切削 15 系統之概要圖; 第6b圖為電阻器之概要圖,其具有尤其特別是電阻器 邊緣之可測量之幾何特性,可以使用以第63圖系統所獲得 之資料而測量; 第7圖為圖表其顯示在一實施例中電阻器陣列掃瞄期 2〇雷射光線之位置對(VS)時間之圖,其中將以固態偏光器之 快速掃瞄與電子機械線性掃瞄重疊,而以增加的速度選擇 性地形成第2圖或第4圖之切割。 第8圖為系統概要圖,其將多個聚焦光線傳送至至少 一電阻器以增加其切削速度;以及 12 玫、發明說明 第9圖為系統之概要圖,其在雷射切削系統中提供多 個光線給至少一電阻器。 C實施方式】 較佳實施例之詳細說明 高速曲折切削過程 在電阻器之切削中,此切割導引電流沿著電阻路徑流 經電阻材料。如同於第la至lc圖中說明,此切割尺寸與形 狀之精密控制與調整將電阻改變至所想要之值。此等晶片 電阻器典型地是在基板上配置成列與行。第2a圖顯示一種 配置其中處理電阻器R1、R2…RN之列。將此具有探測器 2〇〇且由第2a圖中箭頭所說明之探測器陣列與電阻器列之 導體帶至接觸202。矩陣開關將用於第一對導體之接觸(例 如,^ R1之接觸)定址,且實施一系列之切割與測量而將 介於導體#之間阻改變至所想要之值。#完成此電阻 器切削時,此矩陣切換至下一列元件(例如,R2)之第二組 接觸且重覆此切削過程。當已切削此等電阻器(以…rn)之 整個列時,將此介於接觸與探測器陣列之間之接觸斷開。 將此基板對另一列相對定位,將探測器陣與其接觸,並且 以如同先前列之方式處理第二列。 此例如在第lc圖中所說明之曲折薄膜電阻器之切削是 關於雷射處理,而在導體之間電阻材料區域中產生數字間 切割。此等數字間切割導引電流沿著此圍繞切割周圍曲折 路徑而流經電阻材料。其幾何形狀允許以單一區域薄膜/ 導體佈局產生廣大範圍之電阻。此上述方法將在電阻器位 1223284 玖、發明說明 置以測量步驟處理曲折切割之序列,並且然後移至下一個 電阻。Micro-cutting to change this measurable characteristic > 佶, the value of the mI injection, (b) abort this selective micro-cutting; (C) when this selective micro-cutting is aborted, at least another device in the array Selective micro-cutting to change the value of its measurable characteristics, and ⑷ Restore this selective micro-cutting to change the measurable characteristics of the device until its value is in the desired range. The optical subsystem may include a polarizer and a polarization controller for controlling the polarizer to scan the laser light along the first cat pattern (which includes each of the micro-cutting devices to be waited for). The system further includes a measurement subsystem to measure one of the 10 measurable characteristics of at least one of these devices. The microcutting can be laser cutting, the array can be a resistor array, and the measurement subsystem can be a detector array. The optical subsystem may include a second polarizer to re-focus the high-speed second scanning pattern onto the first scanning pattern, thereby increasing the output of the system. 15 A controller can be coupled to the subsystem so that the subsystem can be controlled to produce a cutting sequence for at least one of these devices, which reduces the temperature of the device during micro-cutting. The above and other objects, features and advantages of the invention will be apparent from the following detailed description of the best mode for carrying out the invention and with reference to the attached drawings. Brief description of the drawing The first la-lb diagram is a schematic diagram, each of which illustrates the current lines before and after laser cutting; the first lc diagram is a diagram illustrating the various cutting parameters on the number of cutting parameters 11 1223284 玖, the effect of the invention description Figure 2a is a schematic diagram of a chip resistor array arranged in rows and rows, which illustrates the results of using a laser cutting step according to an embodiment of the present invention; Figure 2b is a step-definition cutting step corresponding to Figure 2a Block 5 flowchart; Figure 3 is a block flowchart, which further defines the cutting operation of Figures 2a and 2b in the system of the present invention; Figure 4a is a schematic diagram of a chip resistor array arranged in columns and rows, which Describe the results of using laser cutting steps according to another embodiment of the present invention; 10th diagram is a block flow diagram, which further defines the cutting steps corresponding to FIG. 4a; FIG. 5 is a block flow diagram; The cutting operation of Figures 4a and 4b in the inventive system; Figure 6a is a schematic diagram of a laser cutting 15 system that can be used in at least one embodiment of the present invention; Figure 6b is a schematic diagram of a resistor, which The measurable geometric characteristics, especially the edges of the resistors, can be measured using the data obtained with the system in Figure 63; Figure 7 is a chart showing a laser array scan period of 20 in one embodiment A plot of the position of light versus time (VS), where a fast scan of a solid-state polarizer and an electro-mechanical linear scan are overlapped, and the cuts in Figure 2 or Figure 4 are selectively formed at an increased speed. FIG. 8 is a schematic diagram of the system, which transmits a plurality of focused rays to at least one resistor to increase its cutting speed; and FIG. 9 is a schematic diagram of the system, which provides multiple functions in a laser cutting system. Light to at least one resistor. Embodiment C] Detailed description of the preferred embodiment High-speed zigzag cutting process In the cutting of a resistor, this cutting guide current flows through the resistance material along the resistance path. As illustrated in Figures 1a to 1c, the precise control and adjustment of the cutting size and shape changes the resistance to the desired value. These chip resistors are typically arranged in columns and rows on a substrate. Figure 2a shows a configuration in which the processing resistors R1, R2 ... RN are arranged. Bring the conductor with the detector 200 and the array of resistors and resistor rows illustrated by the arrows in Figure 2a to the contact 202. The matrix switch will be used to address the contacts of the first pair of conductors (for example, the contact of ^ R1), and a series of cuts and measurements will be performed to change the resistance between the conductors # to the desired value. #When this resistor cutting is completed, the matrix switches to the second set of components in the next column (for example, R2) to contact and repeat the cutting process. When the entire column of these resistors (by ... rn) has been cut, the contact between this contact and the detector array is broken. Position this substrate relative to another column, contact the detector array with it, and process the second column in the same way as the previous column. The cutting of the zigzag thin film resistor as illustrated in Fig. 1c, for example, is related to laser processing, and an interdigital cut is generated in the area of the resistance material between the conductors. These inter-digital cutting guide currents flow through the resistive material along this tortuous path around the cutting. Its geometry allows a wide range of resistances to be produced in a single area thin film / conductor layout. This above method will place the zigzag cut sequence in the measurement step at the resistor position 1223284, description of the invention, and then move to the next resistor.

3月參考第2 a圖’其將用於任何切割之最初雷射位置說 明為205,然後光線定位器導引光線沿著線性路徑通過電 5 阻器材料。根據本發明新的典範切削在第一電阻器上之一 支(例如,R1之切削切割204)並測量其電阻。如果其電阻 低於預先設定之臨界值,則跨止列中其他電阻器R2〜rn 實施類似之共線性切削。在第2a圖中之210說明沿著列之 所完成共線切削,而在第2b圖中進一步界定相對應之方塊 ίο 22〇。在本發明之至少一實施例中,可以測量電阻器之子 集合以確定跨此基板薄膜之均勻一致。如果此薄膜具有已 知之均勻一致,則測量一次就足夠。With reference to Figure 2a in March, it illustrates the initial laser position for any cutting as 205, and the light locator directs the light along the linear path through the electrical resistor material. A new model according to the present invention cuts a branch on the first resistor (e.g., cutting cut 204 of R1) and measures its resistance. If its resistance is lower than the preset threshold, similar collinear cutting is performed across the other resistors R2 ~ rn in the stop row. In Fig. 2a, 210 illustrates the collinear cutting performed along the column, and in Fig. 2b, the corresponding square is further defined. In at least one embodiment of the invention, a subset of the resistors can be measured to determine the uniformity of the film across the substrate. If the film has a known uniformity, one measurement is sufficient.

此沿著電阻器列之下一個共線切割組是以在第2a圖之 211所示相同的方式實施,且在第2b圖之方塊221進一步的 15 界定,電阻器RN首先被切削。此過程如同於第2a圖之212-213中所示地重覆、而在第2b圖方塊222-223進一步界定。 如果測量顯示其超過臨界值,則列R1…RN之切削以各電 阻器之測量進行,以致於在切換至下一個電阻器之前將各 電阻器切削至臨界值(如同在方塊224描述為214)。 20 將測量次數限制且維持共線切削軌跡均增加切削速度。 在第3圖之流程更進一步界定對應於第2a-2b圖之步驟 ,以及使用於切削系統中其他的處理步驟(例如:定址與 裝載)。 在至少一實施例中,可以根據預先設定之資訊實施切 14 1223284 玖、發明說明 割步驟。作為例子,對於某些電阻器型式而言,在測量電 阻之前可將第_系列元件切割,此序列是根據電阻器之預 先設:之參數(例如:幾何形狀)及/或已知之薄膜特性(例 如’薄膜電阻)。同樣的,可以在第一電阻器以學習模式 決定非測量式切割之次數(例如包括至少_次測量,或: 覆測幻。在學習模式中實施反覆測量,並且根據測量與 材料特性決定此非切削切割之次數。在至少一實施例中, 可以計算此非測量切割之次數。This collinear cutting group along the resistor column is implemented in the same manner as shown in 211 in Fig. 2a, and further defined by 15 in block 221 in Fig. 2b. The resistor RN is first cut. This process is repeated as shown in Figures 2a-212-213, and further defined in Figures 2b, blocks 222-223. If the measurement shows that it exceeds the critical value, the cutting of the columns R1 ... RN is performed with the measurement of each resistor, so that each resistor is cut to the critical value before switching to the next resistor (as described in block 224 as 214) . 20 Limit the number of measurements and maintain collinear cutting trajectories to increase cutting speed. The process in Figure 3 further defines the steps corresponding to Figures 2a-2b, as well as other processing steps used in the cutting system (such as addressing and loading). In at least one embodiment, the cutting step can be implemented according to preset information. As an example, for some resistor types, the _ series element can be cut before measuring the resistance. This sequence is based on the resistor's preset parameters: (such as: geometric shape) and / or known film characteristics ( (Eg 'thin film resistor). Similarly, the number of non-measuring cuts can be determined in the learning mode of the first resistor (for example, including at least _ measurements, or: repeat testing. Implement repeated measurements in the learning mode, and determine the non-measurement based on the measurement and material characteristics Number of times of cutting. In at least one embodiment, the number of times of non-measurement cutting can be calculated.

例如,可以不經測量作四次切割。請參考第钧圖其說 1〇明最初之情況410。其中如同於第2a圖中所示將探測器置 入與列接觸202。請參考第4b圖,在方塊420進一步界定此 最初情況。藉由例子,第4a-4b圖說明切割過程之實施例 ’其中未經任何測量而作最切四次切割4丨丨。如同於第朴 圖中所示,方塊421根據至少一切削前之值或條件未經測 15 $而界定預定設定之切割次數(例如:4次)。此用於完成四For example, four cuts can be made without measurement. Please refer to Di Juntu, whose statement 10 states 410 at the beginning. The detector is placed in contact with the column 202 as shown in Figure 2a. Referring to Figure 4b, this initial situation is further defined at block 420. By way of example, Figs. 4a-4b illustrate an embodiment of the cutting process, in which the most four cuts are made without any measurement. As shown in the figure, block 421 defines a predetermined set of cutting times (for example, 4 times) according to at least one value or condition before cutting without measuring 15 $. This is used to complete four

切割之掃瞒路徑是在405說明。然後在406數列中之第一電 阻器R1切削並測量以決定是否達成目標值。如果沒有,則 如同在412所描述且由方塊422進一步界定,則(例如,未 經測量)將剩餘電阻器R2…RN切割。 20 然後將此過程重覆,以RN之切削407開始,且然後如 同在413所示且由方塊423進一步界定將R(N-l)至切割。 因此,以各方向中之改變而將R1或RN切割,並且如果未 達到目標值,則各將剩餘之電阻器R2 切割。在R1或RN達到目標值後則產生最後步驟。如同在 15 1223284 玖、發明說明 414說明且由方塊424進一步界定,將各電阻器連接且依序 切削。 第5圖之流程圖進一步界定對應於第4a_4b圖之步驟, 以及使用於切削系統中額外的處理步驟(例如,其包括定 5 址與裝載之步驟)。 在一實施例中,其中使用反覆測量而獲得預先設定之 資訊以提供切削前之值。此等值可由操作人員或製程工程 師規疋,或以其他方式獲得。轉體提供能力用以規定或使 用此切削前之目標值,以致於可以控制所施加之測試電壓 10及/或電流。此特性是有用於在與此曲折切削有關之電阻 改變之寬度範圍中避免足以損害此部份之高電壓。當在本 發明實施例中使用快速電阻H測量系統時,將用於最初低 電阻切害J之施加用於測量電阻器之電壓降低,以限制流經 電阻器之電流與對其可能之損害。在作隨後實施切割時電 15 阻增加,而將測量電壓增加。 20The Sweep Conceal Path is illustrated at 405. The first resistor R1 in the 406 series is then cut and measured to determine whether the target value is reached. If not, as described at 412 and further defined by block 422, then (e.g., not measured) the remaining resistors R2 ... RN are cut. 20 This process is then repeated, starting with RN's cutting 407, and then as shown at 413 and further defined by block 423 from R (N-1) to cutting. Therefore, R1 or RN is cut with a change in each direction, and if the target value is not reached, each of the remaining resistors R2 is cut. The final step occurs after R1 or RN reaches the target value. As in 15 1223284 (1), the description of the invention 414 and further defined by block 424, the resistors are connected and sequentially cut. The flowchart of Figure 5 further defines the steps corresponding to Figures 4a_4b and additional processing steps used in the cutting system (for example, it includes steps of addressing and loading). In one embodiment, iterative measurements are used to obtain pre-set information to provide values before cutting. These values can be specified by the operator or process engineer, or otherwise obtained. The swivel provides the ability to specify or use the target value before cutting so that the applied test voltage 10 and / or current can be controlled. This characteristic is useful for avoiding high voltages that are sufficient to damage this part in the range of resistance changes associated with this zigzag cutting. When a fast resistance H measurement system is used in the embodiment of the present invention, the application of the initial low resistance cut J to the voltage drop of the measurement resistor is used to limit the current flowing through the resistor and the possible damage to it. During subsequent cutting, the electrical resistance increases and the measurement voltage increases. 20

力以將第2a、2b、4a以及4b圖之典型之切削與㈣ 列修正’以允許材制性與其他製程參數與公差中之變 :例如’在本發明之至少_實施例中,當所測量之切削 剔達到目標值且其長度是在所允許最大切割長度之預先 定邊緣中時,則可以使用額外之步驟。在此邊緣中材料 性中之改變可以使得某些切削切割無法達到目標值且須 額外的切割。 在第一模式中,在元件之初丨由 ^ 千之歹j中依序貫施切削切割, 將未達到目標值之元件位置俘 罝保存。而以隨後之切削切割 16 1223284 玖、發明說明 將在所保存位置之其餘元件切削至目標值。 在第二模式中,根據此第一元件被切削長度之值,而 減少此切割長度以防止達到目標值,並實施非測量式切割 以完成此列之切割。此等隨後之切削切割將在列中所有元 5 件帶至目標值。 在第二模式中,將在元件上至少一預先切割的長度修 正以防止隨後之切割落入邊緣情況中。 在至少一實施例中,當此經測量切削切割之值是在目 標值之預先設定邊緣中時,可以使用額外之步驟。在此緣 10中材料特性中之改變可以使得某些元件超過使用完全非測 量式切割之目標值。 在第一模式中,在此等元件之列中依序實施切削切割 ,且將未達到目標值元件之位置保存。而以隨後之切削切 割’將在所保存位置之其餘元件切削至目標值。 15 在第二模式中,根據在第一元件中所測量之值將切割 長度減少以防止達到目標值,並實施非測量式切割以完成 此列之切割。隨後之切削切割將在列中所有元件帶至目標 值。 τ 在第二模式中,將在元件上至少一先前切割之長度修 20正以防止隨後之切割落入邊緣情況中。 不同於傳統單一電阻器切削技術,而如同在第2至4圖 中所不之實驗資料顯示,藉由將在列中所有電阻器切割而 產里增加。作為例子,在以下表中顯示大致之結果: 17 1223284 玖、發明說明Force to modify the typical cutting and queuing of Figures 2a, 2b, 4a, and 4b to allow changes in material properties and other process parameters and tolerances: for example, in at least An additional step can be used when the measured chipping reaches the target value and its length is within a predetermined edge of the maximum allowable cutting length. Changes in material properties in this edge can make some cutting cuts fail to reach the target value and require additional cuts. In the first mode, at the beginning of the component, cutting and cutting are sequentially performed from ^ thousand of 歹 j, and the component positions that have not reached the target value are captured and saved. And subsequent cutting and cutting 16 1223284 玖, description of the invention The remaining components in the saved position are cut to the target value. In the second mode, according to the value of the cut length of the first component, the cut length is reduced to prevent reaching the target value, and a non-measurement cut is performed to complete the cut of the column. These subsequent cuts will bring all 5 pieces in the column to the target value. In the second mode, at least one pre-cut length on the component is corrected to prevent subsequent cuts from falling into the edge case. In at least one embodiment, an additional step may be used when the measured cutting cut value is in a predetermined edge of the target value. Changes in material properties in this margin 10 can cause some components to exceed the target value of using completely non-measurement cutting. In the first mode, cutting and cutting are performed in sequence among these components, and the locations of components that have not reached the target value are saved. Then, the remaining components in the saved position are cut to the target value by subsequent cutting. 15 In the second mode, the cutting length is reduced according to the value measured in the first component to prevent the target value from being reached, and a non-measurement cutting is performed to complete the cutting of the column. Subsequent cutting cuts bring all components in the column to the target value. τ In the second mode, the length of at least one previous cut on the component is adjusted to prevent subsequent cuts from falling into the edge condition. Different from the traditional single resistor cutting technique, as shown in the experimental data in Figures 2 to 4, the yield is increased by cutting all the resistors in the row. As an example, the approximate results are shown in the following table: 17 1223284 玖, Description of the invention

此整體之切削速率隨著:在列中電阻器數目的增加, 較少的測量,以及隨著用於最後(即,精密)切削時間之減 5 少而增加。 此外,各電阻器須有額外的時間從雷射所產生的能量 恢復。可以確定切割之順序以管理在元件中溫度之改變( 例如,降低在切割期間之最大元件溫度)。例如參考第 4a圖’可以將順序405反轉,以致於從接近元件中央開始 1〇實施一組切割,並進行至接近導體與探測器之元件之一端 。可以使用其他適當順序之序列(例如,任何非相鄰式切 割之順序具有用於熱量管理之優點)。在另外的測量步驟 之前較佳可以切割第二元件。 用於曲折切割之電阻改變範圍,以目前的材料而言從 15大約一個數量級(例如10X),典型的兩個數量級(1〇〇χ), 改變至大約500Χ之數量級。 雷射切削系統 在本發明之至少一實施例中,可以使用在美國專利案 號 N0.4,918,284,,CalibratingLaserTrimmingApparatus,i 20所描述之方法首先將雷射切削系統校準。此,2料專利揭示 藉由控制雷射光線定位機構而校準雷射切削裝置,此定位 18 1223284 玖、發明說明 機構將雷射光線移動至在基板區域上所想要的額定雷射位 置,在媒體上印上記號(例如,切割一線)以建立實際之雷 射位置,掃瞄此印上的記號以偵測實際的雷射位置,並將 實際的雷射位置與所想要之額定位置比較。較佳在一個波 5長上操作雷射光線,並且在不同波長上操作之偵測裝置掃 瞄此記號。此偵測裝置所觀看之範圍包栝整個基板區域之 一部份,並決定在此範圍中記號的位置。此,284專利更揭 示確定相對於攝影機觀看範圍之雷射光線之位置。 可以單獨地使用其他的校準技術或與此,284方法組合 1〇使用。例如,美國專利案號NO, 6,501,061,,Laser Calibration Apparatus and Method,”揭示一種方法以決定掃 猫器座標,而將經聚焦之雷射光線準確地定位。由此雷射 掃瞄器將所聚焦之雷射光線在工作平面上之所關切區域( 例如,孔徑)上掃瞄。此所聚焦雷射光線之位置是由光偵 15測為以預先設定之時間或空間之間隔或當此經聚焦之雷射 光線經由工作平面中孔徑出現時偵測。使用此經聚焦雷射 光線之經偵測之位置根據在偵測到聚焦雷射光線時雷射掃 瞎器之位置,而產生掃瞄器位置對於(vs)光線位置之資料 。可以使用此掃瞄器對於(VS)光線位置之資料;以決定與 20此聚焦雷射光線所想要位置對應之孔徑中央或掃瞄器位置 座標。 在將系統校準(其較佳包括多種其他系統元件之校準) 之後’將具有被切削裝置之至少一基板裝載入切削台中。 請參考第6a圖,其部份來自1284專利,此改良之雷射 19 1223284 玖、發明說明 切削系統可以包括紅外線雷射602,其典型地具有從1.047 微米至大約1.32微米之波長’其沿著光學路控604輸出雷 射光線603經由雷射光線定位機構605至基板區域606。為 了應用至薄膜陣列之切削,可以藉由使用在此技術中所知 5 且在商業上可供使用之各種技術,將IR雷射之輸出頻率加 倍而可以獲得大約0.532微米之較佳波長。 此雷射光線定位機構605,較佳包括一對鏡子與所裝 附之各電流計607與608(可從本案受讓人獲得而可供使用) 。此光線定位機構605導引雷射光線603經由透鏡609(其可 10 為遠心式或非遠心式,且在此兩波長較佳為無色化)而至 於範圍上之基板區域606。如果維持足夠之準確度,此χ_γ 電流計鏡系統可以提供整個基板之角度涵蓋。否則,可以 使用各種定位機構以提供基板與雷射光線之間之相對移動 。例如,可以使用在617所圖示說明之雙軸準確步進與重 15複轉發器,而將基板定位於此以電流計為主的鏡子系統 607、608之範圍(例如:於χ_γ平面中)中。此雷射光線定 位機構605將雷射光線603沿著兩個垂直軸移動,因此提供 雷射光線603跨基板區域606之兩因次定位。各鏡子與有關 的電流計607、608在電腦610控制下,將雷射光線沿著其 20各X或Υ軸移動。照射裝置6Π可以為鹵素燈或發光二極體 其產生可見光以照射基板區域606。 分光器612(—種部份反射鏡)是位於光學路徑6〇4中以 導引光線能量沿著路徑604,從基板區域6〇6反射回偵測裝 置614。此偵測裝置614包括··攝影機615,其可以為數位 20 1223284 玖、發明說明 CCD攝影板(例如··彩色或黑/白)與相關晝面擷取器616(或 此攝影機所提供之數位晝面緩衝器),此裝置將來自電視 攝影機615之影像輸入數位化,以獲得代表基板區域6〇6之 一部份之二因次影像。此像素資料是儲存於畫面擷取器 5 616之記憶體中,或例如由高速連接直接傳送至電腦61〇而 處理。 此光線定位子系統可以包括其他的光學元件,例如電 腦控制之光學子系統,用於調整在基板位置之雷射光點大 小及/或雷射光點之自動聚焦。 10 在將本發明應用至電阻器陣列之薄膜切削中,至少一 薄膜陣列是由基板支持。此如同以上所獲得之校準資料較 佳與自動切削視界算法組合使用而將陣列之元件(例如, 電阻器R1)定位,並且測量第讣圖之元件62〇之至少一幾何 特徵之位置。此特徵例如可以為藉由使用多個可供使用之 15邊緣偵測算法之一而分析在記憶體中像素資料所發現之: 水平邊緣621(例如,平行於又_方向之邊緣)之一,以及垂 直邊緣622(例如,平行於γ_方向之邊緣)之一。此邊緣可 以包括·沿著電阻裔整個周圍之多個邊緣測量,像本之邊 緣、或來自此陣列多個電阻器之邊緣。然後可以決定電阻 -之見度’纟可被使用典型地作為寬度之預先設定之百分 比以界定切割長度。此邊緣資訊較佳自動地獲得,且例如 校準資料一起使用,以控制列ri "rn中各切割之長度。 亦可使用其他合適之測量算法,例如影像相關算法或斑點 偵測方法。 21 1223284 玫、發明說明 可將校準應用至沿著切割之一或多個點。在至少一實 施例中可以用权準資料修正至少一切割之開始點。 幸乂佳可以修正在第2與4圖中多個切割之長度與開始點。 取較佳的是可以修正在第2&與4a圖中所有切割之長度 5 與開始點。 在一實施例中,可以將第一電阻器(例如:…或關交 準,然後對此列之所有電阻器(例如:R1,〜,RN)實施相對 應之修正。 幸乂佳疋作凡全的自動化。然而,可以使用具有操作人 10員介入之半自動算法,例如當將電流計定位以致於陣列元 件是在此範圍中,然後將光線沿著元件依序以交互方式定 位’然後由操作人員在顯示器630上觀察強度輪廊(或強度 之衍生物)。 此使用才乂準身訊以調整在陣列區域中之座標對於改善 15雷射光線定位之準確度是有價值的而不會造成產量之下降 。電阻器寬度之測量與對準資料對於以下之情形是有用的 ••用於控制㈣之長度,與用於修正對線性之偏差,以及 用於修正對於掃聪器Χ、γ座標系統之非正交性。此用於 修正成何形狀之校準資料之使用,是特別適用於具有一或 20多個線性轉換台之雷射切削系統。 幾何修正並無必要取代其他有用的系統設計特微,包 括:f-theta透鏡之線性,扇出光線補償等。通常可以使用 此系統公差<合計根據所期望之位置誤差而決定在切割校 準位置數月之間之抵換。當將光線扇出(fan 〇ut)時尤其 22 1223284 坎、發明說明 是對於具有跨越許多電阻器之大的間隔時,只有一個被校 準與對準。例如,當電阻器之間之間隔非常大時,可以將 單一的切割校準與對準。而在此等元件所產生位置之偏差 為可預期的,其部份由於系統設計,f_theta線性、扇出擴 5散補償等而緩和減輕。緊密間隔切割之橫向擴扇(fan)較在 轴上之擴扇被認為具有較小之誤差。 產量進一步的改善一光學技術 在本發明之至少一實施例中,可以藉由使用一或多個 以下技術以增加有效掃瞄率而進一步增加產量。 1〇 可以跨越此列之電阻器之間之切隙間隙較快之跳躍而 達成具有共線切削處理速率進一步的增加。此種間隙顯示 於第2a圖中。請參考第7圖,在本發明之至少一實施例中 ,當電流計以恆定速度702跨列掃瞄時,此單軸聲光光線 偏轉器(AOBD)將踞齒形線性掃瞄圖案7〇1重疊。在切削期 15間此A〇BD在逆向移動703中掃瞄,並且在切削之間提供快 速跳躍704至下一個切割。此允許電流計以恆定速度掃瞒 ,且將整個處理時間中跳躍所占比例減至最小。 此使用聲光偏轉器與電流計組合用於速率之改善在此 技術中為人所知。例如’美國專利案號N〇, 5,837,962揭示 20 -種改良式裝置用於將卫作加熱、溶化、蒸發或切割。此 種二因次聲光偏轉器提供標記速率大約5倍之改善。 美國專利案號NO 6,341,G29將其整個併人作為參考, 而在第5圖中顯示其實施例具有數個元件,其在當以逆向 模式實施本發明以增加速率時可以使用於整個系統中。在 23 玖、發明說明 此’029美國專利中,顯示具有相關控制器之聲光偏轉器與 電流計,其用於脈動之CW光線以形成雷射圖案。關於系 統結構之額外細節,亦請參考此,029專利案說明書之第3 攔第47行與第4欄。 藉由使用可應用之技術,可以輕易地調整地,〇29專利 案之配置,以便提供光學元件與掃瞄控制輪廓之修正,較 佳以額外之硬體校準程序以實施本發明之逆向掃瞄技術。 在本發明之另一實施例中,在此曲折電阻器上共線切 削可以用沿著此列之多個光點以平行方式達成。使用一種 扇出光柵或其他多光線產生裝置以產生光點陣列,以致於 根據沿著此列電阻器間距形成兩個或更多光點並將其對準 。例如,美國專利案號^^〇, 5,521,628揭示使用繞射光學裝 置以同時標記數個部份。此等多個光線可以為從更強而有 力之雷射源所產生之較低功率光線,或是來自多個來源之 組合光線。此掃瞄系統掃瞄多個光線,並經由同時跨多個 電阻器之共同掃瞄透鏡形成光點。此切削過程類似於在非 測量式切割步驟期間具有兩個或更多平行切割之單一光點 法。當達到臨界值時,此系統轉變成單一光點模式依序將 各電阻器切削成所想要之值。 同樣的,此在曲折電阻器上共線切削可以在目標上形 成多個光點以平行方式實施平行切割而達成。使用扇出光 栅或其他多光線產生裝置以產生光點陣列,以形成兩個或 更多個光點,將此光點與元件對準,其具有在切割之間預 先設定之間隙。如果實施預先設定次數之切割(例如,在 玖、發明說明 第4a圖中所不之4次),則在一實施例中可將通過之次數減 少5〇%(例如,在各方向中單次通過)。如果良好建立電阻 “製私臭化與公差,則此實施例最為有用。此光栅可以在 光予切換路徑中,以致於選擇性地形成多個光點或單一光 5 點。 此所公佈之美國專利申請案號N0,2002/0162973說明 種系統與方法用以產生多㈤光點以處理記憶體維修所用 之半導體連接。可以使用在透鏡系統與偏光器系統中各種 修正’以產生使用於本發明中之多個光點。 1〇 在一貫施例中,使用單一雷射脈衝同時切割一直至兩 個電阻器(例如:沒有,一或兩個切割)。請參考第8圖,藉 由將單對準之雷射光線803空間分解成兩個發散對準之 光線804 805,而在兩個切割上形成兩個聚焦光點、 802。此差異頻率精密之調整控制光點之分離。此使用聲 b光裝置用於在材料處理應用中以空間方式分解光線在此技 術中為人所知。例如日本專利摘要JP 53152662顯示一種配 置用於使用具有可選擇頻率之多頻率偏光器以鑽微 形孔。 第8圖之雷射806以預先設定之重覆率脈動。此雷射光 20線經由傳送光學裝置807 ,其形成雷射光線腰之中間影像 而進入聲光調變器(AOM)之孔徑中。較佳使用在Brag^^ 況中操作之AOM 808,以可控制地產生兩個稍微發散而對 準之弟一專級繞射雷射光線’且控制各光線中之能量。此 AOM是由兩個頻率fi、f2驅動,而fi=f〇+df且f2:=f〇_df,而 25 1223284 玖、發明說明 df為原來RF信號頻率fO之一小百分率。兩個光線之間之角 度大約等於用於fO之Bragg角度乘以2(df/f0)。此AOM藉由 調變在R F信號f 12中兩個頻率成份f 1與f 2之信號振幅以及 調整光線之交互耦合,而控制在各雷射光線中之能量。 5 在離開AOM 808之後,此光線經由選擇性光線旋轉控 制模組809將光線旋轉90度,以致於此光線是在又或丫方向 。在一實施例中使用稜鏡用於此旋轉,雖然如同在相關的 美國專利公告案號NO· 2002/0170898中說明之許多旋轉技 術是為人所熟知。 10 其次,此光線經由一組光學裝置將光線腰部定位,並 且將光線之大小設定成適用於調整焦距光學裝置與物鏡 810。此調整焦距光學裝置亦修正兩個光線之間之角度, 因此取決於此調整焦距之調整,此等離開A〇M 8〇8之兩個 光線之間之角度必須調整,以造成在焦點平面所想要之光 15點分離。其次,此雷射光線進入物鏡81〇,其在兩個電阻 器上提供一對聚焦光點801、8〇2。此兩個光點所分開之距 離大約等於透鏡810之焦距長度乘以兩個光線之間的角度 可將此逆向與平行方法組合用於在曲折電阻器上之共線 切肖]例如,此光線由AOBD掃瞄,然後分解成一對且跨 20此粑圍而掃描。將兩個相鄰電阻器同時切削,且此跳躍是 從電阻器N至電阻器N+2而至下一對電阻器。 以替代之方式或以二因次偏光器,可以在垂直於曲折 掃目苗方向之方向產生-對光點。例如,以-因次八咖之 相當間早之控制與程式化,可以使用(具有適當輸出功率 26 1223284 玖、發明說明 控制之)偏光器以同時產生如同於第4a圖中所示實施四個 切割所用四個光線之至少兩個。因此,此用於切割之掃瞄 時間可以減少50%。由於其可程式之偏轉,此A〇BD是優 於扇出光栅而被偏好。此等多個光點亦可如同所須在粗略 5 或精細切削期間產生。 第9圖概要說明改良式雷射切削系統之典範實施例, 其具有加上來自第8圖之模組901,而用於逆向掃瞄,平行 處理、或其組合。例如,可以使用來自電腦61〇之信號9〇2 ,以控制在一或多軸中之A〇BD或其他固態偏光器8〇8,以 1〇及(如果提供的話)光線旋轉模組809。模組901可以包括傳 送光學裝置807與其他的光線成形元件。較佳使用至少一 AOBD以提供相當大的彈性與容易使用,例如,以數位尺^^ 產生器提供來自電腦61 〇之控制信號812。 此外,此用於形成延長或橢圓光點之技術可以與本發 15明一起使用,以進一步增加處理速度與品質。此與光點成 形有關之切削速率之改善,是在經公佈共同待審之美國專 利申請案號NO. 2002/0170898中說明。 在本發明至少一實施例中,可以使用多種其他設計替 代方式,用於加強系統表現與使用之容易。例如,此等替 20代方式包括但不受限於以下: 1·此系統可以提供電腦控制之光點大小及/或焦點調整 。在讓與本發明受讓人之美國專利案號NO. M83,G7m明 -種光學m其提供光點大小控制與用於以雷射為主 之冗憶體維修之動態焦點。 27 1223284 玖、發明說明 2 ·另一替代方式是以可變光線衰減器控制光線之能量 。此衰減态可以為聲光偏轉器(或調變器)。可以使用不論 是手工調整或自動調整之中性密度濾波器或是以偏極化為 主之衰減器。作為例子,在美國專利案號Ν〇· 6,518,54〇中 5顯示一種合適之可變衰減器,具有旋轉半波片以及對偏極 化敏感之分光器。 3 ·可以使用為熟習此技術人士所知之方法改變脈衝寬 度,而具有此瞭解:此q-切換雷射之能量會隨著重覆速率 而改變(尤其是在高重覆速度時)。對於動態切削,其中在 10脈衝之間實施測量,其較佳可以維持實質上恆定之脈衝能 量。此用於脈衝能量控制之方法是揭示於6,339,1〇4專利中 ’其在當電阻值接近預先設定之目標值時對應於精準測量 期間,隨著切削速帛降低(例如:較大之脈衝時間間隔)而 減少在目標能量中的變化。 15 (在至少—實施例中,使用-種以二極體為泵頻率加 倍之YAG雷射以㈣電阻料列。#與其他波長比較時, 此種532nm之輸出波長導致低移動、無微破裂,且可忽略 熱影響之區域。較佳使用大約⑸化之脈衝寬度,而典 型是小於3〇ns之寬度。此較佳最大雷射重覆速率至少為 20 ΙΟΚΗζ。此脈衝寬度是較典型詩厚膜系統者小許多,而 提供相當高之重覆速率用於移除薄膜材料。此在減少之脈 衝寬度與高重覆率之最大可供使用脈衝能量,允許與繞射 光學裝置(例如,光柵或A〇BD)有關之損耗,因此可以提 供多個光點。 28 玖、發明說明 5·可以將雷射聚焦至受繞射限制大約光點之大 大小Γ型是小於大⑽微米或更小,而較佳光點大 15:半2〇微米’並且最較佳之光點大小是在大約6-〜米之範圍中,例如是10-15微米。 5 一在所說明的本發明實施例中,將曲折切割說明成為 糸列之平行數字間切割。然而,應瞭解本發明之應用並 不受限於形成平行切割。此種切削或微切削是用以產生具This overall cutting rate increases as the number of resistors in the column increases, fewer measurements, and as the final (i.e., precision) cutting time decreases by 5 times. In addition, each resistor must have additional time to recover from the energy generated by the laser. The order of the cuts can be determined to manage temperature changes in the component (for example, reducing the maximum component temperature during cutting). For example, referring to Figure 4a ', the sequence 405 can be reversed, so that a group of cuts is performed starting from the center of the approaching element 10 and proceeding to one end of the element approaching the conductor and the detector. Other suitable sequences can be used (for example, any non-adjacent cutting sequence has the advantage of being used for thermal management). The second element may preferably be cut before the further measuring step. The range of resistance change for zigzag cutting ranges from about 15 orders of magnitude (for example, 10X), typically two orders of magnitude (100x), to about 500X for current materials. Laser Cutting System In at least one embodiment of the present invention, the laser cutting system can be first calibrated using the method described in U.S. Pat. No. 4,918,284, Calibrating Laser Trimming Apparatus, i 20. Therefore, the two patents disclose that the laser cutting device is calibrated by controlling the laser light positioning mechanism. This positioning 18 1223284 玖, the invention description mechanism moves the laser light to the desired rated laser position on the substrate area. Print a mark on the media (for example, cut a line) to establish the actual laser position, scan the printed mark to detect the actual laser position, and compare the actual laser position with the desired rated position . It is preferable to operate the laser light on one wave length, and the detection device operating on different wavelengths scans this mark. The range viewed by this detection device covers a part of the entire substrate area, and determines the position of the mark in this range. Therefore, the 284 patent further discloses determining the position of the laser ray relative to the viewing range of the camera. Other calibration techniques can be used alone or in combination with this 284 method. For example, US Patent No. 6,501,061, Laser Calibration Apparatus and Method, "discloses a method to determine the coordinates of the cat scanner and accurately locate the focused laser light. The laser scanner will therefore The focused laser ray is scanned over the area of interest (eg, aperture) on the work plane. The position of the focused laser ray is measured by light detection 15 at a preset time or space interval or when The focused laser light is detected when it appears through the aperture in the work plane. The detected position using this focused laser light is generated based on the position of the laser scanner when the focused laser light is detected. The data of the position of the scanner vs. the position of the light. You can use the data of the position of the scanner (VS) to determine the center of the aperture or the position of the scanner corresponding to the desired position of the focused laser ray 20 After the system is calibrated (which preferably includes the calibration of various other system components), 'at least one substrate with the device to be cut is loaded into the cutting table. Please refer to Figure 6a, part of which Since the 1284 patent, this improved laser 19 1223284 玖, description of the cutting system may include an infrared laser 602, which typically has a wavelength from 1.047 microns to about 1.32 microns' which outputs laser light 603 along the optical path control 604 Via the laser light positioning mechanism 605 to the substrate area 606. In order to apply to the cutting of the thin film array, the output frequency of the IR laser can be doubled by using various technologies known in the art5 and commercially available A better wavelength of about 0.532 microns can be obtained. The laser light positioning mechanism 605 preferably includes a pair of mirrors and attached galvanometers 607 and 608 (available from the assignee of the present case and available for use). This light positioning mechanism 605 guides the laser light 603 through the lens 609 (which may be telecentric or non-telecentric, and the two wavelengths are preferably colorless) to the substrate region 606 in the range. If it is maintained sufficiently Accuracy, this χ_γ galvanometer mirror system can provide the angle coverage of the entire substrate. Otherwise, various positioning mechanisms can be used to provide the relative between the substrate and the laser light For example, you can use the dual-axis accurate step and repeat 15 repeater illustrated in 617 to position the substrate in the range of the galvanometer-based mirror system 607 and 608 (for example, in the χ_γ plane). (Middle). This laser ray positioning mechanism 605 moves the laser ray 603 along two vertical axes, thus providing two-dimensional positioning of the laser ray 603 across the substrate area 606. Each mirror and the relevant galvanometer 607, 608 Under the control of the computer 610, the laser light is moved along its X or Y axis. The irradiation device 6II can be a halogen lamp or a light emitting diode, which generates visible light to illuminate the substrate area 606. The beam splitter 612 (a kind of part The reflector is located in the optical path 604 to guide the light energy along the path 604, and is reflected from the substrate area 606 back to the detection device 614. This detection device 614 includes a camera 615, which can be a digital 20 1223284, a CCD camera plate (such as a color or black / white) and an associated daylight extractor 616 (or a digital camera provided by this camera) Daytime buffer), this device digitizes the image input from the television camera 615 to obtain a two-dimensional image representing a portion of the substrate area 606. This pixel data is stored in the memory of the frame grabber 5 616, or is directly transmitted to the computer 61 for processing via a high-speed connection, for example. The light positioning subsystem may include other optical components, such as a computer-controlled optical subsystem, for adjusting the laser spot size and / or autofocus of the laser spot at the substrate position. 10 In the application of the present invention to thin film cutting of a resistor array, at least one thin film array is supported by a substrate. This calibration data, as obtained above, is preferably used in combination with the automatic cutting horizon algorithm to position the array element (for example, resistor R1) and measure the position of at least one geometric feature of element 62 in the second figure. This feature can be found, for example, by analyzing pixel data in memory by using one of the 15 available edge detection algorithms: one of horizontal edges 621 (eg, edges parallel to the _ direction), And one of the vertical edges 622 (eg, edges parallel to the γ_ direction). This edge may include multiple edges measured along the entire periphery of the resistor, such as the edge of the original, or the edge of multiple resistors from the array. The resistance-visibility 'can then be determined and can be used as a pre-set percentage of the width to define the cut length. This edge information is preferably obtained automatically and used, for example, with calibration data to control the length of each cut in the row ri " rn. Other suitable measurement algorithms can also be used, such as image correlation algorithms or speckle detection methods. 21 1223284 Rose, invention description Calibration can be applied to one or more points along the cut. In at least one embodiment, the starting data of at least one cut can be corrected by the weight data. Fortunately, the length and starting point of multiple cuts in Figures 2 and 4 can be corrected. It is preferable that the lengths 5 and the starting points of all the cuts in Figs. 2 & 4a can be corrected. In an embodiment, the first resistor (for example: ... or Guan Jiaozheng) can be corrected correspondingly to all resistors in the column (for example: R1, ~, RN). Fully automated. However, a semi-automatic algorithm with the intervention of 10 operators can be used, for example, when positioning the galvanometer so that the array elements are in this range, and then sequentially positioning the light along the elements in an interactive manner, then by operation A person observes the intensity contour (or a derivative of intensity) on the display 630. This use is only necessary to adjust the coordinates in the array area to improve the accuracy of the 15 laser light positioning without causing damage. Yield reduction. The measurement and alignment data of the resistor width is useful for the following situations: • For controlling the length of ㈣, and for correcting the deviation from linearity, and for correcting the X and γ coordinates of the sweeper Non-orthogonality of the system. The use of this calibration data to correct the shape is particularly suitable for laser cutting systems with one or more linear conversion tables. Geometric correction There is no need to replace other useful system design features, including: linearity of the f-theta lens, fan-out light compensation, etc. Usually this system tolerance can be used < Total based on the expected position error for a few months at the cutting calibration position When the light is fanned out (fan 〇ut), especially 22 1223284, the invention description is for a large gap across many resistors, only one is calibrated and aligned. For example, when the resistor When the interval is very large, a single cut can be calibrated and aligned. The position deviation of these components can be expected, and part of it is due to the system design, f_theta linearity, fan-out expansion and 5 dispersion compensation. Mitigation. Closely spaced horizontal fans are considered to have smaller errors than axial fans. Yield is further improved. Optical technology In at least one embodiment of the present invention, one can use a Or more of the following technologies to increase the effective scanning rate to further increase the yield. 10 can jump across the gap between the resistors in this column to achieve a faster The collinear cutting processing rate is further increased. This gap is shown in Figure 2a. Please refer to Figure 7, in at least one embodiment of the present invention, when the galvanometer is scanned at a constant speed of 702 across the column, this single The axio-optic light deflector (AOBD) overlaps the 踞 -tooth linear scanning pattern 701. During the cutting period, this AOBD scans in the reverse movement 703 and provides a rapid jump 704 to the next between cuttings. One cut. This allows the galvanometer to evade at a constant speed and minimizes the proportion of jumps in the overall processing time. This uses acousto-optic deflectors in combination with galvanometers for speed improvement is known in this technology For example, 'U.S. Patent No. 5,837,962 discloses 20 improved devices for heating, melting, evaporating, or cutting the crop. This two-dimensional acousto-optic deflector provides about a five-fold improvement in the marking rate. U.S. Patent No. 6,341, G29 takes the entirety as a reference, and Figure 5 shows that its embodiment has several elements that can be used in the entire system when the invention is implemented in reverse mode to increase the rate . In '23. Description of the invention, this' 029 U.S. patent shows an acousto-optic deflector and a galvanometer with associated controllers for pulsating CW light to form a laser pattern. For additional details of the system structure, please also refer to this, line 3, line 47 and column 4 of the 029 patent specification. By using the applicable technology, the configuration of the 〇29 patent case can be easily adjusted in order to provide the correction of the optical element and the scanning control contour. It is preferable to implement the reverse scanning of the present invention with an additional hardware calibration procedure. technology. In another embodiment of the present invention, collinear cutting on the meandering resistor can be achieved in parallel with a plurality of light spots along the column. A fan-out grating or other multi-light generating device is used to generate an array of light spots, so that two or more light spots are formed and aligned according to the resistor pitch along this column. For example, U.S. Patent No. ^^ 0, 5,521,628 discloses the use of diffractive optical devices to mark several portions simultaneously. These multiple rays can be lower power rays from a more powerful laser source, or a combination of rays from multiple sources. This scanning system scans multiple light rays and forms a light spot through a common scanning lens across multiple resistors simultaneously. This cutting process is similar to a single light spot method with two or more parallel cuts during a non-measurement cutting step. When the critical value is reached, the system transforms into a single spot pattern and sequentially cuts each resistor to the desired value. Similarly, this collinear cutting on the zigzag resistor can be achieved by forming multiple light spots on the target and performing parallel cutting in a parallel manner. A fan-out grid or other multi-light generating device is used to generate an array of light spots to form two or more light spots, and align this light spot with the component with a gap set in advance between cuts. If a predetermined number of cuts are performed (for example, 4 times shown in Fig. 4a of the invention description), the number of passes can be reduced by 50% in one embodiment (for example, a single pass in each direction) by). This embodiment is most useful if the resistance "smell resistance and tolerance are well established. This grating can be in the light pre-switching path so that multiple light spots or a single light spot can be selectively formed. This published United States Patent application No. 2002/0162973 describes a system and method for generating multiple light spots to handle semiconductor connections used for memory maintenance. Various modifications can be used in the lens system and polarizer system to produce the use in the present invention 10. In a consistent embodiment, a single laser pulse is used to cut up to two resistors at the same time (for example: no, one or two cuts). Please refer to Figure 8 by The aligned laser light 803 is spatially decomposed into two divergent aligned rays 804 805, and two focused light spots, 802 are formed on the two cuts. This difference frequency is precisely adjusted to control the separation of light spots. This uses sound The b-light device for spatially decomposing light in material processing applications is known in this technology. For example, Japanese Patent Abstract JP 53152662 shows a configuration for using Multi-frequency polarizer to drill micro-shaped holes. Laser 806 in Figure 8 pulsates at a preset repetition rate. This 20-ray laser light passes through the transmission optical device 807, which forms the middle image of the laser light waist and enters In the aperture of the acousto-optic modulator (AOM), it is better to use the AOM 808 operated in the Brag ^^ condition to controllably produce two slightly divergent and aligned brothers, a special-level diffraction laser light 'and Control the energy in each light. This AOM is driven by two frequencies fi, f2, and fi = f〇 + df and f2: = f〇_df, and 25 1223284 发明, invention description df is the original RF signal frequency fO A small percentage. The angle between the two rays is approximately equal to the Bragg angle used for fO times 2 (df / f0). This AOM modulates the two frequency components f 1 and f 2 in the RF signal f 12 The signal amplitude and the interactive coupling of the adjustment light control the energy in each laser light. 5 After leaving the AOM 808, this light rotates the light 90 degrees through the selective light rotation control module 809, so that the light is at Or ah direction. In one embodiment, 稜鏡 is used for this rotation, although as in Many of the rotation techniques described in the related U.S. Patent Publication No. 2002/0170898 are well known. 10 Second, the light is positioned at the waist of the light via a set of optical devices, and the size of the light is set to be suitable for adjusting the focal length Optical device and objective lens 810. The focus-adjusting optical device also corrects the angle between the two rays, so depending on the adjustment of the focus adjustment, the angle between the two rays leaving the AOM 808 must be adjusted. In order to cause the desired light at the focal plane to be separated by 15 points. Second, this laser light enters the objective lens 81o, which provides a pair of focused light spots 801, 802 on two resistors. The distance between these two light spots is approximately equal to the focal length of the lens 810 times the angle between the two rays. This inverse and parallel method can be combined for collinear tangent on a tortuous resistor.] For example, this ray Scan by AOBD, then break down into a pair and scan across 20 perimeters. Cut two adjacent resistors at the same time, and this jump is from resistor N to resistor N + 2 and to the next pair of resistors. Alternatively, or with a two-dimensional polarizer, a spot-point can be created in a direction perpendicular to the direction of the zigzag scan. For example, with the very early control and stylization of the eight factors, you can use a polarizer (with appropriate output power 26 1223284 玖, controlled by the description of the invention) to simultaneously produce four implementations as shown in Figure 4a. Cut at least two of the four rays used. Therefore, the scanning time for cutting can be reduced by 50%. Because of its programmable deflection, this AOBD is preferred over the fan-out grating. These multiple light spots can also be generated as required during rough 5 or fine cutting. Fig. 9 outlines an exemplary embodiment of an improved laser cutting system having a module 901 from Fig. 8 for reverse scanning, parallel processing, or a combination thereof. For example, a signal 902 from a computer 61 can be used to control AOBD or other solid-state polarizer 808 in one or more axes, rotating the module 809 with 10 and (if provided) light. The module 901 may include a transmission optical device 807 and other light shaping elements. It is preferred to use at least one AOBD to provide considerable flexibility and ease of use. For example, a digital ruler ^^ generator is used to provide a control signal 812 from a computer 61 °. In addition, this technique for forming extended or elliptical light spots can be used with the present invention to further increase processing speed and quality. The improvement of the cutting rate related to the formation of light spots is described in US Patent Application No. 2002/0170898, which has been published and pending. In at least one embodiment of the present invention, a variety of other design alternatives may be used to enhance system performance and ease of use. For example, these 20 generation methods include but are not limited to the following: 1. This system can provide computer-controlled light spot size and / or focus adjustment. In the US Patent No. M83, G7m, which is assigned to the assignee of the present invention, a kind of optical m which provides the control of the spot size and the dynamic focus for laser-based maintenance of redundant memory. 27 1223284 发明, description of the invention 2 · Another alternative is to control the energy of light with a variable light attenuator. This attenuation state can be an acousto-optic deflector (or modulator). You can use either a manual or automatic adjustment of a neutral density filter or an attenuator based on polarization. As an example, U.S. Patent No. 6,518,54 5 shows a suitable variable attenuator with a rotating half-wave plate and a beam splitter sensitive to polarization. 3. The pulse width can be changed using methods known to those skilled in the art, with the understanding that the energy of this q-switched laser changes with the repetition rate (especially at high repetition rates). For dynamic cutting, where measurements are performed between 10 pulses, it is preferred to maintain a substantially constant pulse energy. This method for pulse energy control is disclosed in the 6,339,104 patent 'It corresponds to the precise measurement period when the resistance value approaches a preset target value, and decreases with the cutting speed (for example: a larger pulse Time interval) while reducing changes in target energy. 15 (In at least the embodiment, a kind of YAG laser with diode as the pump frequency doubled is used as the rubidium resistance material. #Compared with other wavelengths, this output wavelength of 532nm results in low movement and no micro-fracture And can ignore the area affected by heat. It is better to use a pulse width of approximately ⑸, but typically a width less than 30ns. This preferred maximum laser repetition rate is at least 20 ΙΟΚΗζ. This pulse width is more typical. Thick-film systems are much smaller and provide a fairly high repetition rate for removing thin film materials. This reduces the pulse width and high repetition rate to the maximum available pulse energy, allowing and diffractive optical devices (eg, Gratings or AOBD), so multiple light spots can be provided. 28 玖, description of the invention 5. The laser can be focused to a large size limited by the diffraction limit about the light spot Γ type is less than large ⑽ microns or more It is small, and the preferred light spot is 15: half 20 micrometers' in size, and the most preferable light spot size is in the range of about 6 to ~ meters, for example, 10-15 micrometers. 5-In the illustrated embodiment of the present invention In the description of zigzag cutting The listed parallel numbers are cut. However, it should be understood that the application of the present invention is not limited to the formation of parallel cuts. Such cutting or micro-cutting is used to produce

有減少測量數目之多個不相交切割,而這被認為是在本發 明之範圍中。 X 7·此外,本發明之實施例並不限於薄膜電阻器測量, 而是可以使用於其他之微切削應用,其中之物理特性為可 測量。此測量不限於電氣測量,而是可以為(例如,以紅 外線感測器)之溫度監視、壓力、振動、或其他特性之測 量0 15 雖然以上已經描述與說明了本發明之實施例,但其用 意並非為此等實施例描述且說明本發明所有可能之形式。 而是在本發明書中所使用之字句是說明字句而非限制字句 ,且應瞭解在不偏離本發明之精神與範圍之前題下可以對 它作各種改變。 20 【圖式簡單說明】 第la-lb圖為概要圖,其各說明在雷射切削之前與之 後之電流線; 第lc圖為圖表,其說明各種切割形成對數個切割參數 之影響; 29 1223284 玖、發明說明 第2a圖為配置成列與行之晶片電阻器陣列之概要圖, 其說明根據本發明實施例使用雷射切削步驟之結果; 第2b圖為進一步界定對應於第2a圖之切削步驟之方塊 流程圖; 5 第3圖為方塊流程圖,其進一步界定本發明系統中第 2a與2b圖之切削操作; 第4a圖為配置成列與行中之晶片電阻器陣列之概要圖 ,其說明根據本發明另一實施例使用雷射切削步驟之結果; 第4b圖為方塊流程圖,其進一步界定對應於第如圖之 10 切削步驟; 第5圖為方塊流程圖;其進一步界定本發明系統中第 4a與4b圖之切削操作; 第6a圖為可以使用於本發明至少一實施例中雷射切削 系統之概要圖; 15 第6b圖為電阻器之概要圖,其具有尤其特別是電阻器 邊緣之可測量之幾何特性,可以使用以第以圖系統所獲得 之資料而測量; 第7圖為圖表其顯示在一實施例中電阻器陣列掃瞄期 雷射光線之位置對(VS)時間之圖,其中將以固態偏光器之 20快速掃瞄與電子機械線性掃瞄重疊,而以增加的速度選擇 性地形成第2圖或第4圖之切割。 第8圖為系統概要圖,其將多個聚焦光線傳送至至少 一電阻器以增加其切削速度;以及 第9圖為系統之概要圖’其在雷射切削系統中提供多 30 1223284 玖、發明說明 個光線給至少一電阻器。 【圖式之主要元件代表符號表】 617…轉發器 620…元件 200···探測器 202…接觸 204,205···切割 210···共線切削 211,212,213,214—切割 R1,R2〜RN…電阻器 405…掃瞒路徑 406,407,408…切削 410···最切情況 411,412,413,414…切割 602…紅外線 603···雷射線 604···光學路徑 605···雷射光線·定位機構 606···基板區域 607,608···電流計 609…透鏡 610…電腦 611…照射裝置 614…偵測裝置 615…攝影機 616…書面擷取器 62卜··水平邊緣 622···垂直邊緣 630…顯示器 702…怪定速度 703…逆向移動 704…跳躍 801,802···光點 803···雷射光線 804,805··.光線 806…雷射 807···傳送光學裝置 808···聲光調變器 809···光線旋轉控制模組 810…物鏡 812···射頻信號 822···折疊鏡 901···模組 902…信號 220,221,222,223,224,420, 421,422,423,424〜方塊There are multiple disjoint cuts that reduce the number of measurements, and this is considered to be within the scope of the present invention. X 7 · In addition, the embodiments of the present invention are not limited to the measurement of thin film resistors, but can be used in other micro-cutting applications where the physical characteristics are measurable. This measurement is not limited to electrical measurement, but may be (for example, an infrared sensor) temperature monitoring, pressure, vibration, or other characteristic measurements. 0 15 Although the embodiments of the present invention have been described and illustrated above, It is not intended to describe and illustrate all possible forms of the invention for these embodiments. Instead, the words used in the present invention are explanatory words rather than restrictive words, and it should be understood that various changes can be made to the subject without departing from the spirit and scope of the invention. 20 [Schematic description] Figures la-lb are schematic diagrams, each of which illustrates current lines before and after laser cutting; Figure lc is a diagram, which illustrates the effect of various cutting formations on several cutting parameters; 29 1223284发明 Description of the invention Figure 2a is a schematic diagram of a chip resistor array arranged in rows and rows, which illustrates the results of using a laser cutting step according to an embodiment of the invention; Figure 2b is a further definition of the cutting corresponding to Figure 2a Block diagram of steps; 5 FIG. 3 is a block diagram that further defines the cutting operation of FIGS. 2a and 2b in the system of the present invention; FIG. 4a is a schematic diagram of a chip resistor array arranged in columns and rows, It illustrates the result of using a laser cutting step according to another embodiment of the present invention; FIG. 4b is a block flow chart, which further defines the cutting step corresponding to FIG. 10; FIG. 5 is a block flow chart; The cutting operation of Figures 4a and 4b in the invention system; Figure 6a is a schematic diagram of a laser cutting system that can be used in at least one embodiment of the present invention; 15 Figure 6b is a summary of a resistor Figure, which has measurable geometric characteristics, especially the edge of the resistor, which can be measured using the data obtained with the graph system; Figure 7 is a graph showing the resistor array scanning period in one embodiment The plot of the position of the light rays versus time (VS), in which the fast scanning of the solid-state polarizer 20 and the electromechanical linear scanning are superimposed, and the cutting of Figure 2 or Figure 4 is selectively formed at an increased speed. Fig. 8 is a schematic diagram of the system, which transmits a plurality of focused rays to at least one resistor to increase its cutting speed; and Fig. 9 is a schematic diagram of the system 'which provides more 30 1223284 in a laser cutting system. Explain a light to at least one resistor. [Representative symbol table of main components of the figure] 617 ... transponder 620 ... element 200 ... detector 202 ... contact 204,205 ... cut 210 ... collinear cut 211,212,213,214—cut R1, R2 ~ RN ... resistor 405 ... Sweep path 406,407,408 ... Cut 410 ... Cut most cases 411,412,413,414 ... Cut 602 ... Infrared 603 ... Ray path 604 ... Optical path 605 ... Laser beam positioning mechanism 606 ... Substrate area 607, 608 ... Galvanometer 609 ... Lens 610 ... Computer 611 ... Illuminating device 614 ... Detection device 615 ... Camera 616 ... Writer 62 ... Horizontal edge 622 ... Vertical edge 630 ... Monitor 702 ... Constant speed 703 ... Reverse movement 704 ... Jump 801,802 ... Light spot 803 ... Laser light 804,805 ... Light 806 ... Laser 807 ... Transmission optics 808 ... Acoustooptic modulator 809 ... · Light rotation control module 810 ... Objective lens 812 ... RF signal 822 ... Folding lens 901 ... Module 902 ... Signal 220, 221, 222, 223, 224, 420, 421, 422, 423, 424 ~ block

3131

Claims (1)

拾、申請專利範圍 1 · ~種用於高速精密微切削陣列裝置之方法,各穿置具 有至少一可測量特性,其特徵為包括以下步驟: 選擇性地將陣列中之裝置微切削,以改變其可測 量特性之值; 中止此選擇性微切削步驟; 當此選擇性微切削步驟中止時,將此陣列中至少 另一裝置選擇性地微切削,以改變此可測量特性之值 ;以及Scope of patent application 1. A method for high-speed precision micro-cutting array devices, each of which has at least one measurable characteristic, which is characterized by the following steps: Selectively micro-cutting the devices in the array to change The value of its measurable characteristic; discontinuing the selective microcutting step; and when the selective microcutting step is aborted, selectively microcutting at least another device in the array to change the value of the measurable characteristic; and 恢復此經中止選擇性微切削步驟以改變此裝置可 測量之特性,一直至其值在所想要之範圍中為止。 如申請專利範圍第1項之方法,其中此裝置是電阻器。 如申明專利範圍第2項之方法,其中此電阻器是薄膜電 阻器。 4·如申請專利範圍第!項之方法,其中此選擇性微切削之 步驟是以切割地等裝置之至少一雷射光線實施。 5·如申請專利範圍第!項之方法,更包括測量至少—此等 裝置之可測量特性,以獲得經測量之值。 6·如申請專利範圍第5項之方法,更包括將此經測量值與 預先設定之臨界值比較以獲得比較結果,且根據此比 較結果將至少另一此等裝置微切削。 7·如申請專利範圍第5項之方法,更包括根據所測量之值 ’將至少此等裝置選擇性地微切削。 8·如申請專利範圍第5項之方法,更包括根據所測量之值 決定不測量至少另-此等裝置之可測量特性。 32 fe、申請專利範厪 如申請專利範圍第〗項之方法 精準雷射切削陣列之電阻器 電阻。 0·如申請專利範圍第〗項 、 法,其中各此等選擇性微切 ^步驟包括:選擇性地去除材料之步驟。 u•如申請專利範圍第丨項 _ 、 法,其中此陣列包括··此等 —或多列之至少之一,盥 ”此等一或多行之至少之一。 2·如申請專利範圍第〗項 之方法,其中至少一此等選擇性 微切削步驟,是以多個細取 10 v'工來“、、μ射脈衝實質上同時昭 射多個裝置而實施。 … 13·如申請專利範圍第1項之方法,其中至少-此等選擇性 微切削步驟,是以多個經聚焦雷射脈衝實施,且其中 此方法更包括分配此等經聚焦雷射脈衝。 Κ如申請專利範圍第 15 貝之方法,其中此分配步驟包括 ’驟·產生具有多個雷射光線之分配圖案,並且將 此等雷射光線聚焦。 15·如申請專利範圍第9項之方法,其中此雷射切削在此等 電阻器之導體之間電阻材料區域中產生一系列數字間 之切割。 20 9. 其中此方法是用於高速 且其中一可測量特性為Resume this aborted selective microcutting step to change the measurable characteristics of the device until its value is within the desired range. For example, the method of claim 1 in which the device is a resistor. For example, the method of claim 2 of the patent scope is declared, wherein the resistor is a thin film resistor. 4 · If the scope of patent application is the first! The method of claim 4, wherein the step of selective micro-cutting is performed by at least one laser light of a device such as a cutting ground. 5 · If the scope of patent application is the first! The method further includes measuring at least the measurable characteristics of these devices to obtain a measured value. 6. The method of claim 5, further comprising comparing the measured value with a preset threshold to obtain a comparison result, and micro-cutting at least one of these other devices based on the comparison result. 7. The method of claim 5, further comprising selectively micro-cutting at least these devices according to the measured value '. 8. The method of item 5 of the scope of patent application, further comprising deciding not to measure at least the measurable characteristics of these devices based on the measured values. 32 fe. Application for patent: The method of item No. 17 of the scope of patent application. Precision laser cutting array resistor. 0. As described in the scope of patent application, each of these selective micro-cutting steps includes: a step of selectively removing material. u • If the scope of the patent application item 丨, method, where the array includes ... these—at least one of the plurality of columns, the "at least one of these one or more rows. 2 The method of item 其中, in which at least one of these selective micro-cutting steps, is carried out by using a plurality of 10 v ′ fine-cutting pulses to substantially simultaneously shoot multiple devices. … 13. The method according to item 1 of the scope of patent application, wherein at least-these selective micro-cutting steps are performed with a plurality of focused laser pulses, and wherein the method further includes allocating the focused laser pulses. The method of claim 15 is patent application method, wherein the distribution step includes a step of generating a distribution pattern having a plurality of laser rays, and focusing the laser rays. 15. The method of claim 9 in the scope of patent application, wherein the laser cutting produces a series of digital cuts in the area of the resistive material between the conductors of these resistors. 20 9. Where this method is used for high speed and one of the measurable characteristics is 16. 如申請專利範圍第1項之方法,其中至少一此等選擇性 U切削步驟包括此步驟:將雷射光線定位於各此等待 微切削裝置之位置,且以至少一雷射脈衝選擇性地照 射各此等待微切削裝置之至少一部份。 17. 如申請專利範圍第β之方法,其中至少一此等選擇性 33 拾、申請專利範匱 ^切削步驟包括此等步驟:產生雷射光線並將其相對 疋位於在此陣列範圍φ筮 . 』靶闺中弟一方向中傳送,I以至少一 雷射脈衝選擇地照射在此範圍中至少一裝置之至少一 部份。 18.如申請專利範圍第17項之方法,卩包括產生雷射光線 並=其相對定位於在此範圍中實質上與第一方向相反 、第方向中傳送’且以至少_雷射脈衝選擇性地照 射在此範圍中至少-裝置之至少-第二部份。 、 10 19·如申請專圍第lJS之方法,其中至少—此等選擇性 微切削步驟包括此等步驟: 產生田射光線並將其相對定位於跨此等裝置之第 一:猫圖案中傳送,將第二掃晦圖案與第-掃瞒圖案 重$ ’且以至少一雷射脈衝照射至少一裝置。 15 申請專利範圍第19項之方法,其中此第二掃瞒圖案 是逆向掃晦,且其中照射此至少一裝置之至少一雷射 脈衝之掃瞒速率是低於第-掃晦圖案之相對應掃瞎速 率’其中雷射能量是集中於至少一裝置一段期間,其 長於只與第一掃瞄圖案有關之期間,因此增量增加。 20 •如申4專利範圍第19項之方法,其中第二掃描圖案包 括從第一裝置跳至第二裝置。 22.如申請專利範圍第1項之方法,其中此等選擇性微切削 步驟是以多個雷射脈衝實施,且其中至少一此等脈衝 所具有能量是在❻·1微焦耳至25毫焦耳之範圍中。 23·如申請專利範圍第7項之方法,其中此所測量值是所測 34 拾、申請專利範圍 量之溫度值。 24·如申凊專利範圍第1項之方法,其中此等裝置實質上相 同。 25. —種用於高速以雷射為主精密微切削陣列裝置之系統 ’各此等裝置具有至少—可測量特十生,其特徵為包括: 脈衝雷射子系統; 耦合連接至脈衝雷射子系統之一光學子系統,以 雷射脈衝選擇性地照射此裝置之一部份;以及 耦合連接至此等子系統之控制器,以控制此等子 糸統: 選擇性地微切削陣列中之裝置,以改變可測量特 性之值; 中止此選擇性的微切削; 當此選擇性微切削中止時,選擇性地微切削此陣 列中至少另一裝置’以改變其可測量特性之值;以及 恢復此選擇性微切削以改變此裝置可測量之特性 ,一直至其值是在所想要之範圍中為止。 26·如申請專利範圍第25項之系統,其中光學子系統包括 :偏光器與偏光器控制器,其用於控制偏光器將雷射 光線沿著第一掃瞄圖案掃瞄,此圖案包括待微切削之 各此等裝置。 27·如申請專利範圍第25項之系統,更包括測量子系統以 測量至少一此等裝置之一此等可測量特性。 28·如申請專利範圍第27項之系統,其中此微切削是雷射 1223284 拾、申請專利範圍 切削’且此陣列為電阻器之陣列,以及其中此測量子 系統是探測器陣列。 29·如申請專利範圍第26項之系統,其中此光學子系統包 括第二偏光器,其將高速第二掃瞄圖案重疊至第一掃 瞄圖案上,因此系統產量增加。 30.如申請專利範圍第25項之系統,其中將此控制器耦合 連接至此等子系統,以致控制此等子系統,以產生用 於至少一此等裝置之切削序列,其在微切削期間降低 裝置之溫度。16. The method of claim 1 in patent application, wherein at least one of these selective U-cutting steps includes the step of positioning laser light at each of the positions waiting for the micro-cutting device, and selectively using at least one laser pulse The ground is irradiated with at least a part of each of the waiting micro-cutting devices. 17. If the method of applying patent scope β, at least one of which is selective 33, the patent application Fan ^ cutting step includes these steps: generating laser light and relatively 疋 located in this array range φ 筮. "The target girl's younger brother transmits in one direction. I selectively irradiate at least a part of at least one device in this range with at least one laser pulse. 18. The method of claim 17 in the scope of patent application, comprising generating laser light and its relative positioning in this range is substantially opposite to the first direction, transmitted in the first direction ', and at least _ laser pulse selectivity The ground radiates at least-at least-the second part of the device in this range. 10 10 If you are applying for a method specifically for lJS, at least-these selective micro-cutting steps include these steps: Generate field shots and position them relative to the first across these devices: cat pattern transmission , The second scan pattern and the first scan pattern are repeated, and at least one device is illuminated with at least one laser pulse. 15. The method of claim 19 in the patent application range, wherein the second concealment pattern is a reverse concealment pattern, and wherein the concealment rate of at least one laser pulse irradiating the at least one device is lower than that corresponding to the-concealment pattern The "blind rate", in which the laser energy is concentrated in at least one device for a period of time, which is longer than the period related only to the first scanning pattern, and thus the increase is increased. 20 • The method of item 19 in the scope of claim 4, wherein the second scanning pattern includes a jump from the first device to the second device. 22. The method of claim 1, wherein the selective micro-cutting steps are performed with a plurality of laser pulses, and at least one of these pulses has an energy in the range of ❻ · 1 microjoule to 25 millijoules In the range. 23. The method of item 7 in the scope of patent application, wherein the measured value is the temperature value measured in the scope of patent application and scope of patent application. 24. The method of claim 1 in the patent scope, wherein these devices are substantially the same. 25. —A system for high-speed laser-based precision micro-cutting array devices' Each of these devices has at least a measurable feature, which is characterized by: a pulsed laser subsystem; coupled to a pulsed laser One of the subsystems is an optical subsystem that selectively irradiates a part of the device with laser pulses; and a controller coupled to these subsystems to control these subsystems: Means to change the value of the measurable characteristic; to suspend the selective micro-cutting; to selectively micro-cut at least one other device in the array to change the value of the measurable characteristic when the selective micro-cutting is stopped; and The selective microcutting is resumed to change the measurable characteristics of the device until its value is in the desired range. 26. The system of claim 25, wherein the optical subsystem includes a polarizer and a polarizer controller, which are used to control the polarizer to scan the laser light along the first scanning pattern, and the pattern includes Each of these devices for micro-cutting. 27. The system of claim 25, further comprising a measurement subsystem to measure these measurable characteristics of at least one of these devices. 28. The system of item 27 in the scope of patent application, wherein the micro-cutting is laser 1223284, the scope of patent-application cutting ', and the array is an array of resistors, and wherein the measurement subsystem is a detector array. 29. The system of claim 26, wherein the optical subsystem includes a second polarizer that superimposes the high-speed second scanning pattern on the first scanning pattern, thereby increasing the system output. 30. The system of claim 25, wherein the controller is coupled to these subsystems so as to control the subsystems to produce a cutting sequence for at least one of these devices, which is reduced during micro-cutting Device temperature. 3636
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