TWI227319B - Method of measuring film thickness and microwave measuring unit - Google Patents

Method of measuring film thickness and microwave measuring unit Download PDF

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TWI227319B
TWI227319B TW92115651A TW92115651A TWI227319B TW I227319 B TWI227319 B TW I227319B TW 92115651 A TW92115651 A TW 92115651A TW 92115651 A TW92115651 A TW 92115651A TW I227319 B TWI227319 B TW I227319B
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signal
microwave
film thickness
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scope
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TW92115651A
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TW200427965A (en
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Bar-Long Deng
Kuang-Cheng Fan
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Compal Electronics Inc
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Abstract

A method of measuring film thickness and microwave measuring unit are provided. The method comprises providing an object and then measuring a needful time, t0, which a first signal of microwave region transmitting from a measuring point to the object surfaces. An object under test (OUT) that an object being took place a surface treatment is provided, wherein there is a surface treatment film on a surface of the object. A needful time, t1, which a second signal of microwave region transmitting from a measuring point to the OUT surfaces is measured, wherein the second signal is the same as the first signal. A film thickness of the surface treatment film of the OUT, d, is then calculated by the wavelength of the first signal, lambda, and time lag, t0-t1, wherein a calculating formula is d=lambda(t0-t1). Because of emission, reflection, and receiving of the signal and utilization of microwave region, it can easily and accurately measure thinner film thickness.

Description

1227319 _案號 92115651 五、發明說明(1) 93. 10. 1 5 年 月 曰 修正 發明所屬之技術領域 本發明是有關於一種膜厚量測方法及微波量測設 備,且特別是有關於一種可精確量測非平面之膜厚的量 測方法及微波量測設備。 先前技術1227319 _ Case No. 92115651 V. Description of the invention (1) 93. 10. The technical field to which the invention belongs in January 2015 The present invention relates to a film thickness measurement method and a microwave measurement device, and more particularly to a film thickness measurement method and a microwave measurement device. Measurement method and microwave measurement equipment capable of accurately measuring non-planar film thickness. Prior art

目前3 C產品的發展隨著客戶的需求,逐漸走向多元 化及外觀活潑發展,而在外殼上賦予不同的喷塗、濺 鍍、轉印、電鍍,甚至是含浸等技術。而這些技術對於 外殼的膜厚通常很難加以控制,因此容易造成產品的變 異性增加。這並不是產品本身有許多問題,而是對於膜 厚的分佈無法確實掌握,以便提供客戶設計指引。舉例 來說,手機的外殼膜厚會隨著治具旋轉速度、重力及喷 搶的特定因素(壓力、喷嘴形狀及方向等)影響,因而在 膜厚之最低與最高點的差異達7. 5微米以上,這相當於一 層漆的厚度。At present, the development of 3 C products is gradually diversified and the appearance is lively with the needs of customers, and different coating, sputtering, transfer, plating, and even impregnation technologies are given to the shell. These technologies are often difficult to control the film thickness of the shell, so it is easy to increase product variability. This is not that the product itself has many problems, but that the distribution of film thickness cannot be accurately grasped in order to provide customer design guidelines. 5 Above micron, this corresponds to the thickness of a layer of paint.

而習知對於膜厚或膜厚分佈的量測,多半是利用所 謂的單點破壞或單點非破壞性量測以及超音波C掃描方 法,而得到膜厚或膜厚分佈。其最大的問題是就單點破 壞或單點非破壞性量測而言,所獲得的資料很少,故無 法提出準確的資訊,並造成量測點位置本身就變異很 大。而對於超音波C掃描方法而言,只能量測最小1 5微米 以上的膜厚(偏差值目前習知的精準度約在±1微米),因 此較難精準測得較薄的膜厚,而發生很大的問題,更遑 1227319 _案號92115651_年月日_« 五、發明說明(2) 量地 及準 法精 方可 測且 量, 厚厚 膜膜 種的。 一薄佈 供較分 提得厚 是測膜 的地之 目確上 之精面 明且表 發易體 本輕物 ,可面 此,平 因備非 設得 測測 測被 量間 及期 法厚 方膜 »MJ JnJ 涓涓 旦里旦里 厚在 膜物 種層 一理 供處 提面 是表 的之 目物 一測 另待 之止 明防 發可 本, 備 設 測 量收 及吸 法物 方層 測理 量處 厚面 膜表 種之 一物 供測 提待 是被 的號 目訊 一測 又量 之免 明避 發可 。本, 壞 備 破 設 掉 又 之 明 發 本 測 量 及 法 方 測 量 厚 膜 種 一 供 提 是 的 易 不 且 值 異 差 間 時 到 測 量 易 輕 器 收 接 iiuu # 訊。 使響 可影 ,界 備外 設受 方訊 測一 量的 厚段 膜波 種微 一在 出圍 提範 明長 發波 本測 ’ 量 ΓΤΠ , 它體 其物 與一 述供 上提 據先 根係 法 供體 提物 ,中 後其 然, c體 to物 間的 時過 的理 需處 所面 面表 表係 體物 物測 達待 到一 點此 測, 量物 一測 從待 號一 1 IHd. 段於。 波中樣 微其一 在,長 圍tl波 範間號 長時訊 波的的 源需用 量所使 ,面所 後表to 之物測 。測量 物待前 層達之 理到與 處點需 面測號 表量訊 一從的 有號用 具訊使 λ U文 d 波厚 之膜 號之 訊物 用層 JnJ £ ,處 著面 寺 日 與 為 式 公 算 估 中 其 表 的 體 物 出 算 估 用然 J表 彳品。 驟j射 步虎反 其flf一 訊 , 第 法I ' 的 方 射 ㈣Ϊ反 量 會 皮 厚h後 0 ^ ^ 置 一裝# * U達 提^ 再U號 明射訊 發發中 本波其 微, 一面For the measurement of film thickness or film thickness distribution, it is common to obtain the film thickness or film thickness distribution using the so-called single-point destruction or single-point non-destructive measurement and the ultrasonic C-scan method. The biggest problem is that as far as single-point damage or single-point non-destructive measurement is concerned, little data is obtained, so it is impossible to provide accurate information, and the position of the measurement point itself is greatly variably. For the ultrasonic C-scan method, it can only measure a minimum film thickness of 15 micrometers or more (the deviation value is currently known to about ± 1 micrometer), so it is difficult to accurately measure a thin film thickness. And a big problem occurred, even more so 1227319 _ case number 92115651_ year month day _ «V. Description of the invention (2) The quantity and accuracy of the method can be measured and measured, thick and thick film type. A thin cloth is provided for comparison. The thickness of the ground is the precise and clear surface of the test film and the light weight of the body. It can be faced with this method. Thick square film »MJ JnJ It is thick and thin in the film species layer. The surface is provided for the purpose of the surface. The test is to be performed until the light is released. It is equipped with a measurement and absorption method. One of the thick mask sheet species at the measurement point is for measurement and measurement. It is measured and measured to avoid the need to avoid light. If the device is broken, the device is broken, the device is clear, the method of measuring the thickness of the film, and the method of measuring the thickness of the film. It is easy to supply and withdraw. When the difference between the values is different, the device will receive the iiuu # message. Make the sound impactable, and the external receiver will measure a certain amount of thick film wave micro-micro-a measurement of the long-distance wave wave measurement ΓΤΠ, which is related to the substance and a description of the evidence. The method of extracting the donor, after the middle, then, the time-honored space between the body and the object, the surface and the surface of the object should be measured to the point, and the amount of the object should be measured from the number 1 to 1 IHd. . Duan Yu. The sample in the wave is slightly different. The source of the long-distance wave is the long-term wave. The source of the wave is required. It is measured by the following table. The object to be measured should be measured at the front layer, and the number should be measured on the meter. The number of the equipment used is λ U, d, and the thickness of the film is JnJ £. For the physical calculation of the formula in the formula, the estimated value of the table J is a fake. The step j shot the tiger against its flf, and the law of the square shot of the law I 'will be the thickness of the skin after 0 ^ ^ 置 一 装 # * U 达提 ^ and then the U-shot broadcast sends the middle wave Micro, one side

第8頁 1227319 案號 92115651 年 ία 月 曰 修正 五、發明說明(3) 後,利用微波發射/接收器接收第一反射訊號,以得到訊 號從微波發射/接收裝置到達樣品之所需時間%。接著, 利用微波發射/接收裝置發射波長同為λ的訊號到已進行 表面處理而具有一表面處理層物的樣品,其中訊號到達 表面處理層物之後會反射一第二反射訊號。隨後,利用 微波發射/接收器接收第二反射訊號,以得到訊號從微波 發射/接收裝置到達表面處理層物之所需時間t i。之後, 利用波長λ與反射接收時間差(tQ- h )估算出樣品的表面 處理層物之膜厚d,其中估算公式為d=A(tQ- h)。 另外,本發明又提出一種微波量測設備,適於量測 具有非平面表面之一待測物,再根據所得到的數據估算 待測物在表面處理前後之表面厚度差異。此一微波量測 設備至少包括一微波發射/接收裝置以及一處理裝置,其 中微波發射/接收裝置具有以陣列排列之數個發射器以及 數個接收器。微波發射/接收裝置是位於待測物上方,其 中的發射器係用以發射波長範圍在微波段的訊號到待測 物表面,而接收器則係用以經由‘待測物表面之反射,接 收發射器所發射出之訊號。而處理裝置則與微波發射/接 收裝置相連,以根據訊號之發射/接收時間差來測出訊號 到待測物之所需時間。 本發明因為透過訊號發射、反射及接收,並設定範 圍在短波高頻之微波段,所以可輕易地精確測得較薄的 膜厚。 為讓本發明之上述和其他目的、特徵、和優點能更 明顯易懂,下文特舉較佳實施例,並配合所附圖式,作Page 8 1227319 Case No. 92115651 ία Month Revision V. Description of the invention (3) After receiving the first reflection signal by using the microwave transmitting / receiving device to obtain the% of time required for the signal to reach the sample from the microwave transmitting / receiving device. Then, the microwave transmitting / receiving device is used to transmit a signal with the same wavelength to a sample that has been surface-treated and has a surface-treated layer, wherein a second reflection signal is reflected after the signal reaches the surface-treated layer. Subsequently, the microwave reflection / receiver is used to receive the second reflection signal to obtain the time t i required for the signal to reach the surface treatment layer from the microwave transmission / reception device. Then, the film thickness d of the surface treatment layer of the sample is estimated by using the difference between the wavelength λ and the reflection receiving time (tQ-h), where the estimation formula is d = A (tQ-h). In addition, the present invention also proposes a microwave measuring device, which is suitable for measuring a test object having a non-planar surface, and then estimates the difference in surface thickness of the test object before and after the surface treatment according to the obtained data. The microwave measuring device includes at least a microwave transmitting / receiving device and a processing device, wherein the microwave transmitting / receiving device has a plurality of transmitters and a plurality of receivers arranged in an array. The microwave transmitting / receiving device is located above the object under test. The transmitter is used to transmit signals in the microwave range to the surface of the object under test, and the receiver is used to receive the signal through the surface of the object under test The signal emitted by the transmitter. The processing device is connected to the microwave transmitting / receiving device to measure the time required for the signal to reach the object under test based on the difference between the transmitting / receiving time of the signal. Because the present invention transmits, reflects, and receives signals, and sets the microwave band in the short-wave high-frequency range, it can easily and accurately measure thinner film thicknesses. In order to make the above and other objects, features, and advantages of the present invention more comprehensible, preferred embodiments are described below with reference to the accompanying drawings.

第9頁 1227319 __ 案號 92115651_±_9 _ 五、發明說明(4) 詳細說明如下: 實施方式Page 9 1227319 __ Case No. 92115651_ ± _9 _ V. Description of the invention (4) The detailed description is as follows:

第1 A圖與第1 B圖係依照本發明之膜厚量測的原理示 意簡圖。請參照第1 A圖,假設要量測一具有不規則平面 的物體100上之表面處理層物的厚度時,可先提供—物體 1 〇 〇 ,其係未經表面處理過,主要是作為背景值的量測。 然後,由一發射器l〇2a發射一訊號104到未表面處理過的 物體1 0 0上,並設定訊號1 〇 4之波長範圍在短波高頻之微 波段,譬如訊號1 0 4的波長在〇 · 〇 1〜1 0公分之間、頻率在 3 G Η z〜3 0 0 0 G Η z之間。當訊號1 〇 4到達物體1 〇 〇表面後,會 反射一反射訊號1 〇 6。此時,可利用一接收器1 〇 2 b接收此 反射訊號1 0 6,因而量測出波長範圍在微波段的訊號丨〇 4 從發射器1 0 2 a (即量測點)到物體1 〇 0表面所需的時間。 此外,在利用發射器1 0 2 a發射訊號1 〇 4到物體1 〇 〇時,可 先固定物體1 0 0,再相對於物體1 0 0將發射器1 0 2 a往一移 動方向1 08移動。 之後,請參照第1 B圖,利甫與第1 A圖相同的原理,Figures 1A and 1B are schematic diagrams illustrating the principle of film thickness measurement according to the present invention. Please refer to Figure 1A. Assuming that the thickness of the surface treatment layer on an object 100 with an irregular plane is to be measured, it can be provided first-object 100, which has not been surface-treated and is mainly used as a background. Measurement of values. Then, a transmitter 104 transmits a signal 104 to an unsurfaced object 100, and sets the wavelength range of the signal 104 to the short-wave and high-frequency microwave band, such as the wavelength of the signal 104 〇 · 〇 1 ~ 10 cm, the frequency is between 3 G Η z ~ 3 0 0 0 G Η z. When the signal 104 reaches the surface of the object 100, a reflected signal 106 will be reflected. At this time, a receiver 1 〇 2 b can be used to receive this reflected signal 10 6, so the signal with a wavelength range in the microwave band can be measured. 〇 4 from the transmitter 1 0 2 a (that is, the measurement point) to the object 1 〇0 surface required time. In addition, when the transmitter 10 2 a is used to transmit the signal 1 〇 04 to the object 100, the object 1 0 can be fixed first, and then the transmitter 1 0 2 a can be moved in a moving direction 1 08 relative to the object 1 0 0. mobile. After that, please refer to Figure 1B. Lifu has the same principle as Figure 1A.

對表面處理過而具有一表面處理層物110的物體1〇〇(即一 待測物1 2 0 )作量測,其中待測物1 2 0例如是經過嘴塗、錢 鍍、轉印、電鍍或含浸而於物體100表面形成表面處理層 物1 1 0 。而這裡的量測原理與第1 A圖相同包括由發射器 1 0 2 a發射訊號1 〇 4到待測物1 2 〇上,其中訊號1 〇 4的波長需 與之前第1 A圖所使用的一樣。此外,在利用發射器丨〇 2 a 發射訊號1 〇 4到待測物丨2 〇時,可先固定待測物1 2 〇,再相 對於待測物1 2 0將發射器丨〇 2 a往一移動方向1 〇 8移動。當Measure an object 100 (that is, a test object 120) that has been surface-treated and has a surface treatment layer 110, where the test object 120 is, for example, subjected to mouth coating, money plating, transfer printing, A surface treatment layer 1 1 0 is formed on the surface of the object 100 by plating or impregnation. The measurement principle here is the same as that in Figure 1A. The transmitter 1 0 2 a emits a signal 10 4 to the object to be measured 120. The wavelength of the signal 1 04 must be the same as that used in Figure 1 A. The same. In addition, when using the transmitter 丨 〇2 a to transmit the signal 104 to the test object 丨 2 〇, the test object 1 2 〇 can be fixed first, and then the transmitter 丨 〇 2 a Move in a direction of 1.08. when

第10頁 1227319 _案號 92115B51_年月日_ 五、發明說明(5) 訊號1 0 4到達待測物1 2 0表面後,會從表面處理層物1 1 0表 面反射另一反射訊號1 〇 6 a。此時,可利用接收器1 0 2 b接 收此反射訊號1 0 6 a,因而量測出波長範圍在微波段的訊 號1 0 4從發射器1 〇 2 a到待測物1 2 0表面所需的時間b。因 此,可利用訊號1 0 4之波長;I與反射接收時間差(tG- I ) 估算出物體100的表面處理層物110之膜厚d,其中估算公 式如下:Page 10 1227319 _ Case No. 92115B51_ Year Month and Day _ V. Description of the invention (5) When the signal 1 0 4 reaches the surface of the object 1 2 0 to be measured, it will reflect another reflection signal 1 from the surface of the surface treatment layer 1 1 0 〇6 a. At this time, the receiver 1 0 2 b can be used to receive this reflected signal 1 0 6 a, so the measured signal 1 0 4 in the microwave range is measured from the transmitter 1 0 2 a to the surface of the object to be measured. The time required b. Therefore, the wavelength of the signal 104 can be used; the time difference (tG-I) between I and the reflection receiving time (tG-I) can be used to estimate the film thickness d of the surface treatment layer 110 of the object 100. The estimation formula is as follows:

另外,以微波量測物體1 0 0之表面處理層物1 1 0的整 體膜厚分佈計算,除可利用前述訊號的一接一收特性 外’尚可透過快速傅立葉轉換(Fast Fourier Transform,簡稱FFT)方式加以獲得。 而依據上述原理,本發明可應用於以下實施例。 第一實施例 第 圖。請 裝置發 表面處 號,而 3GHz 〜 發射波 對於樣 微波發 軸。之 第一反 2圖係依照本發明之第一實施例之膜厚量測步驟 t τ d’於步驟2 0 0中’利用一微波發射/接斗 ϊ以號樣:r,而ί品係未經In addition, by measuring the overall film thickness distribution of the surface treatment layer object 110 of the object 100 with microwave measurement, in addition to using the one-by-one receiving characteristics of the aforementioned signals, it can also be performed by Fast Fourier Transform (Fast Fourier Transform, for short) FFT). According to the above principle, the present invention can be applied to the following embodiments. First Embodiment Figure. Please send the surface number of the device, and 3GHz ~ the emitted wave for the sample microwave axis. The first inverse 2 diagram is a film thickness measurement step t τ d according to the first embodiment of the present invention. In step 2 0 ', a microwave transmission / bucket is used. Without

訊號的波長;I譬如二之後a反射第反射汛 3 0 0 0 GHz之間)。此1〇.〇1〜10公分之間(頻率則^ 長又的訊號到樣品在利用微波發射/接收裝: 品將微波發射/接收面時,可先固定樣品,再相 射/接收裝置例如是又置往一移動方向移動,其11 後,於步驟2 0 2中含有多個微波發射器之移動 射訊號,以得到訊/用微波發射/接收裝置接收 戒從微波發射/接收裝置到達书The wavelength of the signal; I, for example, the second reflection a after the second reflection flood between 3 0 0 0 GHz). This 10.01 ~ 10 cm (frequency is ^ long and long signal to the sample when using the microwave transmitting / receiving device: When the microwave transmitting / receiving surface, the sample can be fixed before the phase transmitting / receiving device such as It is set to move in a moving direction again. After that, in step 202, the mobile radio signals containing multiple microwave transmitters are received to obtain the information / received by the microwave transmitting / receiving device or the arrival book from the microwave transmitting / receiving device.

第11頁 1227319Page 11 1227319

:i<3. lU. 1 D _案號 92115651_年月日__ 五、發明說明(6) 品之所需時間tD。 然後,請繼續參照第2圖,於步驟2 0 4中,利用微波 發射/接收裝置發射波長為λ的訊號到已進行表面處理而 具有一表面處理層物的樣品,其中訊號到達表面處理層 物之後會反射一第二反射訊號,而於此發射之訊號的波 長需與步驟2 0 0中所發射的訊號的波長一樣。再者,對樣 品所進行之表面處理包括噴塗、丨賤鍍、轉印、電鑛或含 浸。此外,在利用微波發射/接收裝置發射訊號到表面處 理層物表面時,可先固定樣品,再相對於樣品將微波發 射/接收裝置往一移動方向移動,其中微波發射/接收裝 置例如是含有多個微波發射器之移動軸。接著,於步驟 2 0 6中,利用微波發射/接收裝置接收第二反射訊號,以 得到訊號從微波發射/接收裝置到達表面處理層物之所需 時間t i。 請再參照第2圖,進行步驟2 0 8,利用波長;I與反射 接收時間差(tQ- td估算出樣品之表面處理層物的膜厚 d,其中估算公式為d= λ (tQ- D。另外,以微波量測樣 品之表面處理層物的整體膜厚分佈計算,除可利用訊號 的一接一收特性外,尚可透過快速傅立葉轉換方式加以 獲得。以下為應用本發明的兩個範例: 1 ·以3 G Η z (波長相當於1 0公分或1 0 0 0 0 0微米)之微波 發射/接收裝置,利用本發明之方法量測預估膜厚為1 0微 米之塗料,則所需之時間差只要有達0 . 1 ms,微波發射/ 接收器相對精準度在0 . 0 1 m s以内,則在同步掃描過程, 即可獲得曲面表面的整體膜厚分佈。: I < 3. LU. 1 D _ case number 92115651_ year month day __ 5. Description of the invention (6) The time required for the product tD. Then, please continue to refer to FIG. 2. In step 204, the microwave transmitting / receiving device is used to transmit a signal with a wavelength of λ to a sample that has undergone surface treatment and has a surface treatment layer, and the signal reaches the surface treatment layer. After that, a second reflection signal is reflected, and the wavelength of the signal transmitted here needs to be the same as the wavelength of the signal transmitted in step 200. In addition, the surface treatment of the sample includes spray coating, low-plating, transfer printing, electric ore mining or impregnation. In addition, when using the microwave transmitting / receiving device to transmit a signal to the surface of the surface treatment layer, the sample can be fixed first, and then the microwave transmitting / receiving device can be moved in a moving direction relative to the sample. The microwave transmitting / receiving device contains The axis of the microwave transmitter. Next, in step 206, the microwave reflection / reception device is used to receive the second reflection signal to obtain the time t i required for the signal to reach the surface treatment layer from the microwave transmission / reception device. Please refer to FIG. 2 again, and perform step 208, using the wavelength; I and the reflection receiving time difference (tQ- td to estimate the film thickness d of the surface treatment layer of the sample, where the estimation formula is d = λ (tQ- D. In addition, the overall film thickness distribution calculation of the surface treatment layer of the sample measured by microwave measurement can be obtained through fast Fourier transform in addition to the one-by-one reception characteristics of the signal. The following are two examples of applying the present invention : 1 · Using a microwave transmitting / receiving device with a wavelength of 3 G 波长 z (wavelength equivalent to 10 cm or 100 micrometers), using the method of the present invention to measure a coating with an estimated film thickness of 10 micrometers, then As long as the required time difference is 0.1 ms and the relative accuracy of the microwave transmitter / receiver is within 0.1 ms, the overall film thickness distribution on the curved surface can be obtained during the synchronous scanning process.

第12頁 1227319 _案號92115651_年月日__ 五、發明說明(7) 2.以3 0 0 0 GHz(波長相當於0. 01公分或100微米)之微 波發射/接收裝置,利用本發明之方法量測預估膜厚為1 0 微米之塗料,則所需之時間差只要有達1 0 0 m s,微波發射 接收器相對精準度在1 0 m s以内,則在同步掃描過程,即 可獲得曲面表面的整體膜厚分佈。 由上述範例可知,本發明利用波長範圍在微波段的 訊號進行量測,即可搭配現有的接收器,而輕易獲致待 測物體之膜厚。此外,為說明本發明之優勢,請見表 表 一 範圔 波長(cm) 頻率(Hz) 能量(eV) 無線電磁波 >10 <3xl〇9 <105 微波 10 〜0.01 3xl〇P 〜3xl〇12 10·5 〜0.01 紅外線 ο·οι 〜7xio.5 3xl〇12 〜4.3xl〇14 0.01 〜2· 可見光 7X1CT5 〜4X1CT5 4.3M014 〜7.5X1014 2〜3 紫外線 4xl0·5 〜ΙΟ.7 7.5xl〇14 〜3xl〇17 3 〜103 X射線 ίο·7 〜10·9 3xl〇17 〜3xl〇19 103〜ίο5 伽瑪射線 <10·9 >3x1019 >ισ51227319 on page 12 _Case No. 92115651_Year Month Date__ V. Description of the invention (7) 2. A microwave transmitting / receiving device with a wavelength of 3 0 0 0 GHz (wavelength equivalent to 0.01 cm or 100 micrometers), using this The method of the invention measures a coating with an estimated film thickness of 10 microns, so long as the required time difference is 100 ms, and the relative accuracy of the microwave transmitter and receiver is within 10 ms, then the synchronous scanning process can be used. The overall film thickness distribution on the curved surface is obtained. It can be known from the above examples that the present invention uses signals in the microwave range for measurement, and can be used with existing receivers to easily obtain the film thickness of the object to be measured. In addition, in order to illustrate the advantages of the present invention, please refer to the table below. The range of wavelengths (cm), frequency (Hz), energy (eV), wireless electromagnetic waves > 10 < 3xl09, < 105 microwaves 10 to 0.01 3xlOP to 3xl 〇12 10 · 5 ~ 0.01 Infrared ο · οι ~ 7xio.5 3xl〇12 ~ 4.3xl〇14 0.01 ~ 2 · Visible light 7X1CT5 ~ 4X1CT5 4.3M014 ~ 7.5X1014 2 ~ 3 Ultraviolet light 4x100.5 ~ 10.7 7.5xl〇 14 ~ 3xl〇17 3 ~ 103 X-ray ίο · 7 ~ 10 · 9 3xl〇17 ~ 3xl〇19 103 ~ ίο5 Gamma ray < 10 · 9 > 3x1019 > ισ5

表一為一般訊號輻射頻譜,透過表一可知,本發明 不選用X射線、伽瑪射線主要原因在於其所夾帶的能量很 大,容易造成操作者基因病變等問題。若選用紫外線、Table 1 shows the general signal radiation spectrum. According to Table 1, it can be known that the main reason for not using X-rays and gamma rays in the present invention is that the energy entrained by them is very large, which may easily cause problems such as genetic diseases of the operator. If you choose UV,

第13頁 1227319 _案號 92115651 车 月 9_^__ 五、發明說明(8) 可見光的話,雖然其能量不高,但是容易將表面處理層 物破壞。而紅外線則是會被表面處理層物分子以旋轉、 震盪與剪諧運動方式吸收。至於無線訊號則是波長太 長,目前接收器不容易量測到時間差異值,且易受外界 影響。總而言之,本發明選用波長範圍在微波段的訊號 來量測膜厚,不但可輕易地精確測得較薄的膜厚,而且 能避免前述的缺點。 第二實施例 本發明還提出一種微波量測設備,可用以達成本發 明之膜厚量測方法,請見第3圖。 第3圖係依照本發明之第二實施例之微波量測設備的 示意圖。請參照第3圖,本發明之微波量測設備3 0 0,適 於量測具非平面表面之一待測物3丨〇,此一微波量測設備 300包括一微波發射/接收裝置3〇2以及一處理裝置3〇8。 微波發射/接收裝置3 0 2係位於待測物3 1 0上方,其中微波 發射/接收裝置3 0 2具有以陣列排列之數個發射器3 〇 4與數 個接收器3 0 6 ’其中發射器3 〇 4係用以發射波長範圍在微 波段的訊號到待測物3 1 〇表面,而接收器3 〇 6則係用以經 由待測物3 1 0表面之反射,接收發射器3 〇 4所發射出之訊 號。而處理裝置3 0 8則與微波發射/接收裝置3 〇 2相連,並 根f訊號之發射/接收時間差來測出訊號到待測物3丨〇之 所需時-間。此外,本發明之設備3 〇 〇更可包括一移動軸 (未繪不),連接微波發射/接收裝置3 〇 2之發射器3 〇 4及/ 或接收器306 ,用以同時移動發射器3〇4及/或接收器 3 0 6。另外,本發明之設備3〇〇還可以加上一定位裝°置(未Page 13 1227319 _ Case No. 92115651 Car month 9 _ ^ __ V. Description of the invention (8) Although visible energy, although its energy is not high, it is easy to damage the surface treatment layer. Infrared rays are absorbed by the molecules of the surface treatment layer by means of rotation, vibration and shear harmonic motion. As for the wireless signal, the wavelength is too long. At present, it is not easy for the receiver to measure the time difference and it is susceptible to external influences. In summary, the present invention uses a signal in the microwave range to measure the film thickness, which can not only easily and accurately measure a thinner film thickness, but also avoid the aforementioned disadvantages. Second Embodiment The present invention also proposes a microwave measurement device, which can be used to achieve the film thickness measurement method of the present invention, as shown in FIG. 3. Fig. 3 is a schematic diagram of a microwave measuring device according to a second embodiment of the present invention. Referring to FIG. 3, the microwave measuring device 300 of the present invention is suitable for measuring an object to be measured 3 on a non-planar surface of the tool. The microwave measuring device 300 includes a microwave transmitting / receiving device 3o. 2 and a processing device 308. The microwave transmitting / receiving device 3 0 2 is located above the test object 3 1 0. The microwave transmitting / receiving device 3 0 2 has a plurality of transmitters 3 04 and a plurality of receivers 3 0 6 arranged in an array. The receiver 3 〇4 is used to transmit the signal in the wavelength range of the microwave band to the surface of the DUT 3 1 〇, and the receiver 3 〇6 is used to reflect the surface of the DUT 3 1 0 to receive the transmitter 3 〇 4 emitted signals. The processing device 3 0 8 is connected to the microwave transmitting / receiving device 3 02 and measures the time required between the signal and the object to be measured 3 based on the difference between the transmitting / receiving time of the f signal. In addition, the device 300 of the present invention may further include a moving shaft (not shown), a transmitter 3 04 and / or a receiver 306 connected to the microwave transmitting / receiving device 3 02, for simultaneously moving the transmitter 3 〇4 and / or receiver 3 06. In addition, the device 300 of the present invention can also be added with a positioning device (not

第14頁 1227319 _案號 92115651 五、發明說明(9) 9:ι ία ί 〇 年月曰_ 繪示),用以定位待測物3 1 0。 綜上所述,本發明之特點在於透過訊號發射、反射 及接收,並設定其波長範圍在微波段,所以可輕易地精 確測得較薄的膜厚。另外,本發明上提出一種具有以陣 列排列的微波發射器,可更有效地量測出曲面之待測 物。 雖然本發明已以較佳實施例揭露如上,然其並非用 以限定本發明,任何熟習此技藝者,在不脫離本發明之 精神和範圍内,當可作各種之更動與潤飾,因此本發明 之保護範圍當視後附之申請專利範圍所界定者為準。Page 14 1227319 _ Case No. 92115651 V. Description of the invention (9) 9: ι Αα ί 〇 _ _ (shown), used to locate the test object 3 1 0. In summary, the present invention is characterized by transmitting, reflecting, and receiving signals, and setting its wavelength range in the microwave range, so that thinner film thicknesses can be easily and accurately measured. In addition, the present invention proposes a microwave transmitter with an array, which can more effectively measure curved objects to be measured. Although the present invention has been disclosed as above with preferred embodiments, it is not intended to limit the present invention. Any person skilled in the art can make various modifications and retouches without departing from the spirit and scope of the present invention. Therefore, the present invention The scope of protection shall be determined by the scope of the attached patent application.

第15頁 1227319 _案號92115651_年月日_iti_ 圖式簡單說明 第1 A圖與第1 B圖係依照本發明之膜厚量測的原理示意 簡圖; 第2圖係依照本發明之第一實施例之膜厚量測步驟 圖,以及 第3圖係依照本發明之第二實施例之微波量測設備的 示意圖。 圖式標示說明 1 0 0 :物體 10 2a,3 0 4 ··發射器 10 2b,3 0 6 :接收器 1 0 4 :訊號 1 0 6,1 0 6 a :反射訊號 1 0 8 :移動方向 1 1 0 ··表面處理層物 1 2 0,3 1 0 :待測物 2 0 0 :利用一微波發射/接收裝置發射波長;I的一訊號 到一樣品表面,而樣品係未經表‘面處理,其中訊號到達樣 品之後會反射一第一反射訊號Page 15 1227319 _Case No. 92115651_ 年月 日 _iti_ Schematic illustrations Figures 1A and 1B are schematic diagrams of the principle of film thickness measurement according to the present invention; Figure 2 is a diagram according to the present invention The film thickness measurement step diagram of the first embodiment, and FIG. 3 are schematic diagrams of a microwave measurement device according to a second embodiment of the present invention. Description of the diagrams 1 0 0: Object 10 2a, 3 0 4 ·· Transmitter 10 2b, 3 0 6: Receiver 1 0 4: Signal 1 0 6, 1 0 6 a: Reflected signal 1 0 8: Movement direction 1 1 0 ·· Surface treatment layer 1 2 0, 3 1 0: object to be measured 2 0 0: using a microwave transmitting / receiving device to emit wavelength; a signal of I to a sample surface, and the sample is not shown Surface processing, where a first reflected signal is reflected after the signal reaches the sample

2 0 2 :利用微波發射/接收裝置接收第一反射訊號,以 得到訊號從微波發射/接收裝置到達樣品之所需時間tQ 2 0 4 :利用微波發射/接收裝置發射波長為λ的訊號到 已進行表面處理而具有一表面處理層物的樣品,其中訊號 到達表面處理層物之後會反射一第二反射訊號 2 0 6 :利用微波發射/接收裝置接收第二反射訊號,以2 0 2: Use the microwave transmitting / receiving device to receive the first reflection signal to obtain the time required for the signal to reach the sample from the microwave transmitting / receiving device tQ 2 0 4: Use the microwave transmitting / receiving device to transmit a signal with a wavelength of λ to A sample having a surface treatment layer subjected to a surface treatment, in which a signal reflects a second reflection signal after reaching the surface treatment layer 2 06: the second reflection signal is received by a microwave transmitting / receiving device, and

第16頁 1227319Page 16 1227319

第17頁Page 17

Claims (1)

1227319 _案號92115651_年月日_Iti_ 六、申請專利範圍 1 . 一種膜厚量測方法,包括: 提供一物體; 量測波長範圍在微波段的一訊號從一量測點到達該物 體表面所需的時間tQ ; 提供一待測物,該待測物係表面處理過的該物體,其 中該物體具有一表面處理層物; 量測波長範圍在微波段的該訊號從該量測點到達該待 測物表面所需的時間t i ;以及 利用該訊號之波長λ與時間差(tQ-估算出該物體 的該表面處理層物之膜厚d,其中估算公式為dzACtf ti )° 2 .如申請專利範圍第1項所述之膜厚量測方法,其中 該訊號的波長在0 . 0 1〜1 0公分之間,該訊號的頻率在3 G Η z 〜3 0 0 0 G Η ζ之間。 3 .如申請專利範圍第1項所述之膜厚量測方法,其中 提供該待測物之步驟包括對該物體進行喷塗、濺鍍、轉 印、電鍍或含浸,以於該物體表面形成該表面處理層物。 4.如申請專利範圍第1項所述之膜厚量測方法,其中 該物體包括具有不規則平面。 5 .如申請專利範圍第1項所述之膜厚量測方法,其中 更包括利用快速傅立葉轉換計算出整體膜厚分佈。 6 . —種膜厚量測方法,適於量測需進行一表面處理之 一樣品,其步驟包括: 利用一微波發射/接收裝置發射波長λ的一訊號到一1227319 _Case No. 92115651_ 年月 日 _Iti_ VI. Application for Patent Scope 1. A method for measuring film thickness, including: providing an object; measuring a signal in the microwave range from a measurement point to the surface of the object Required time tQ; provide a test object, the test object is a surface-treated object, wherein the object has a surface treatment layer; the signal with a measurement wavelength range in the microwave range arrives from the measurement point The time ti required for the surface of the object to be measured; and the difference between the wavelength λ and the time of the signal (tQ- to estimate the film thickness d of the surface treatment layer of the object, where the estimation formula is dzACtf ti) ° 2. The film thickness measurement method according to item 1 of the patent scope, wherein the wavelength of the signal is between 0.01 and 10 cm, and the frequency of the signal is between 3 G Η z and 3 0 0 0 G Η ζ . 3. The film thickness measurement method according to item 1 of the scope of patent application, wherein the step of providing the object to be tested includes spraying, sputtering, transferring, plating or impregnating the object to form the surface of the object This surface treatment layer. 4. The film thickness measurement method according to item 1 of the scope of patent application, wherein the object includes an irregular plane. 5. The film thickness measurement method as described in item 1 of the scope of patent application, which further comprises calculating the overall film thickness distribution using a fast Fourier transform. 6. A film thickness measurement method, suitable for measuring a sample requiring a surface treatment, the steps include: using a microwave transmitting / receiving device to transmit a signal of wavelength λ to a 第18頁 1227319 _案號92115651_年月日_«_ 六、申請專利範圍 樣品表面,其中該訊號到達該樣品之後會反射一第一反射 訊號; 利用該微波發射/接收器接收該第一反射訊號,以得 到該訊號從該微波發射/接收裝置到達該樣品之所需時間t 〇 , 利用該微波發射/接收裝置發射波長為λ的該訊號到 已進行該表面處理而具有一表面處理層物的該樣品,其中 該訊號到達該表面處理層物之後會反射一第二反射訊號; 利用該微波發射/接收器接收該第二反射訊號,以得 到該訊號從該微波發射/接收裝置到達該表面處理層物之 所需時間t丨;以及 利用波長λ與反射接收時間差(h )估算出該樣品 的該表面處理層物之膜厚d,其中估算公式為d=A(t〇- 1 7 .如申請專利範圍第6項所述之膜厚量測方法,其中 該訊號的波長在1 0 0微米〜1 0 0 0 0 0微米之間,該訊號的頻 率在3 G Η z〜3 0 0 0 G Η z之間。 4 8 .如申請專利範圍第6項所述之膜厚量測方法,其中 利用該微波發射/接收裝置發射波長λ的該訊號到該樣品 表面之步驟,包括: 固定該樣品;以及 相對於該樣品移動該微波發射/接收裝置。 9 ·如申請專利範圍第8項所述之膜厚量測方法,其中 該微波發射/接收裝置包括含有多個微波發射器之移動Page 18 1227319 _Case No. 92115651_Year Month Date _ «_ VI. Patent application sample surface, where the signal will reflect a first reflection signal after reaching the sample; use the microwave transmitter / receiver to receive the first reflection Signal to obtain the time required for the signal to reach the sample from the microwave transmitting / receiving device, and to use the microwave transmitting / receiving device to emit the signal having a wavelength of λ until the surface treatment has been performed to have a surface treatment layer The sample, wherein the signal reflects a second reflection signal after reaching the surface treatment layer; the second reflection signal is received by the microwave transmitting / receiving device to obtain the signal reaching the surface from the microwave transmitting / receiving device The time t 丨 required to process the layered object; and the film thickness d of the surface treated layered object of the sample was estimated by using the difference between the wavelength λ and the reflection receiving time (h), where the estimation formula was d = A (t〇-1 7. The film thickness measurement method according to item 6 of the scope of patent application, wherein the wavelength of the signal is between 100 μm and 100 μm and the frequency of the signal is 3 G Η z 3 0 0 0 G Η z. 4 8. The film thickness measurement method according to item 6 of the patent application scope, wherein the step of transmitting the signal of wavelength λ to the surface of the sample using the microwave transmitting / receiving device, The method includes: fixing the sample; and moving the microwave transmitting / receiving device relative to the sample. 9 · The film thickness measurement method according to item 8 of the patent application scope, wherein the microwave transmitting / receiving device includes a plurality of microwave transmitting devices. Device movement 第19頁 1227319 案號 92115651 93. 10.±_Ά 修正 六、申請專利範圍 轴0 1 0 .如申請專利範圍第6項所述之膜厚量測方法,其中 該表面處理包括喷塗、濺鍍、轉印、電鍍或含浸。 1 1 .如申請專利範圍第6項所述之膜厚量測方法,其中 該物體包括具有不規則平面。 1 2 .如申請專利範圍第6項所述之膜厚量測方法,其中 更包括利用快速傅立葉轉換計算出整體膜厚分佈。 1 3 . —種微波量測設備,適於量測具非平面表面之一 待測物,該微波量測設備至少包括: 一微波發射/接收裝置,位於該待測物上方,其中該 微波發射/接收裝置具有以陣列排列之複數個發射器以及 複數個接收器,其中 該些發射器係用以發射波長範圍在微波段的複 數個訊號到該待測物表面; 該些接收器係用以經由該待測物表面之反射, 接收該些發射器所發射出之該些訊號;以及 一處理裝置,與該微波發射7接收裝置相連,並根據 該些訊號之發射/接收時間差來測出該些訊號到該待測物 之所需時間。 1 4.如申請專利範圍第1 3項所述之微波量測設備,其 中更包括一移動軸,連接該微波發射/接收裝置之該些發 射器,用以同時移動該些發射器。 1 5 .如申請專利範圍第1 3項所述之微波量測設備,其 中更包括一移動軸,連接該微波發射/接收裝置之該些接Page 19 1227319 Case No. 92115651 93. 10. ± _Ά Amendment VI. Patent Application Axis 0 1 0. The film thickness measurement method described in Item 6 of the Patent Application Scope, where the surface treatment includes spray coating, sputtering , Transfer, plating or impregnation. 1 1. The film thickness measurement method according to item 6 of the scope of patent application, wherein the object includes an irregular plane. 12. The method for measuring the film thickness as described in item 6 of the scope of the patent application, which further includes calculating the overall film thickness distribution using a fast Fourier transform. 1 3. A microwave measuring device suitable for measuring an object to be measured on a non-planar surface of the tool. The microwave measuring device includes at least: a microwave transmitting / receiving device located above the object to be measured, wherein the microwave emission The receiving device has a plurality of transmitters and a plurality of receivers arranged in an array, wherein the transmitters are used to transmit a plurality of signals in a microwave range to the surface of the object to be measured; the receivers are used to Receiving the signals emitted by the transmitters through the reflection of the surface of the object to be measured; and a processing device connected to the microwave transmitting 7 receiving device, and measuring the signals according to the transmission / reception time difference of the signals The time required for these signals to reach the DUT. 14. The microwave measuring device as described in item 13 of the scope of the patent application, further comprising a moving shaft connected to the transmitters of the microwave transmitting / receiving device for simultaneously moving the transmitters. 15. The microwave measuring device as described in item 13 of the scope of the patent application, which further includes a moving shaft connected to the microwave transmitting / receiving devices. 第20頁 1227319 9ό. i _案號 92115651_年月日__ 六、申請專利範圍 收器,用以同時移動該些接收器。 1 6 .如申請專利範圍第1 3項所述之微波量測設備,其 中更包括一定位裝置,用以定位該待測物。 1 7 .如申請專利範圍第1 3項所述之微波量測設備,其 中該些訊號的波長在1 0 0微米〜1 0 0 0 0 0微米之間,該些訊 號的頻率在3GHz〜3000GHz之間。Page 20 1227319 9ό. I _ case number 92115651 _ year month day __ Sixth, the scope of the patent application, used to move these receivers at the same time. 16. The microwave measuring device according to item 13 of the scope of patent application, further comprising a positioning device for positioning the object to be measured. 17. The microwave measuring device according to item 13 of the scope of patent application, wherein the wavelengths of these signals are between 100 microns and 100 micrometers, and the frequencies of these signals are between 3GHz and 3000GHz. between.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI386617B (en) * 2007-12-31 2013-02-21 Ind Tech Res Inst Reflective measurement method of film thickness by spectral image system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI386617B (en) * 2007-12-31 2013-02-21 Ind Tech Res Inst Reflective measurement method of film thickness by spectral image system

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