TWI311643B - Unevenness inspecting apparatus and unevenness inspecting method - Google Patents
Unevenness inspecting apparatus and unevenness inspecting method Download PDFInfo
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- PEDCQBHIVMGVHV-UHFFFAOYSA-N Glycerine Chemical compound OCC(O)CO PEDCQBHIVMGVHV-UHFFFAOYSA-N 0.000 description 1
- 241001465754 Metazoa Species 0.000 description 1
- KJTLSVCANCCWHF-UHFFFAOYSA-N Ruthenium Chemical compound [Ru] KJTLSVCANCCWHF-UHFFFAOYSA-N 0.000 description 1
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- G—PHYSICS
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- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/84—Systems specially adapted for particular applications
- G01N21/88—Investigating the presence of flaws or contamination
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B11/00—Measuring arrangements characterised by the use of optical techniques
- G01B11/30—Measuring arrangements characterised by the use of optical techniques for measuring roughness or irregularity of surfaces
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/02—Testing optical properties
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/1306—Details
- G02F1/1309—Repairing; Testing
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/84—Systems specially adapted for particular applications
- G01N21/88—Investigating the presence of flaws or contamination
- G01N21/95—Investigating the presence of flaws or contamination characterised by the material or shape of the object to be examined
- G01N2021/9513—Liquid crystal panels
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Description
1311643 九、發明說明: 【發明所屬之技術領域】 本發明關於-種檢查基板上所形成之膜之膜厚不均 (mura)的技術。 【先前技術】 習:’撿查顯示裝置用玻璃基板或半導體基板等(以 ㈣腔^「基板」)之主面上所形成之光賴等薄膜時, ,膜照射來自光源之光’並利用來自薄膜之反射光中的 ^干涉檢查膜厚不均。例如,日本專利特開測—194739 =報中揭示有如下技術:於藉由接受光源所照射之光之 ^基板上賴的反射光,於㈣部取得干涉景彡像,並藉 =對干涉影像施以影像處理來檢查基板上之膜厚不均的 I置中,藉由選擇性地變更攝影部所接受之光之波長,使 ,板上膜之厚度均—之部分與存在膜厚不均之部分間的 冗度差調整為所希望之大小。 再者,日本專利第3335503號公報中揭示有如下技術: 於彩色顯像管用遮蔽罩(shad〇w mask)之光透過率之膜厚 不均檢查中,對於自遮蔽罩之一個主面側照射光、自另— 2主面側攝影之影像之色調資料,利用中值濾波器進行平 ’月^處,並求出平滑化資料,並根據將灰階資料除以平滑 化資=算出之標準化資料顯示強調有應檢測之膜厚不均 蔽罩的影像’藉此實現目視檢查之簡化及檢查精度之 提高。 以而,藉由接党基板上的膜所反射之一個波長的干涉光 312XP/發明說明書(補件)/95-11/95127465 6 1311643 而取得膜之影像,並基於該影像檢查膜厚不均時,因干涉 光之強度相對於膜厚呈現週期之變化,故作為干涉光之強 度變動對膜厚變動之比例的靈敏度亦隨膜厚而變化。因 此,由於基板上的膜之厚度或膜厚不均之程度等由於受到 靈敏度之變化的影響,有時膜厚不均於影像中反映為濃淡 之程度會產生變動,而無法高精度地檢查膜厚不均。 【發明内容】 本發明適合檢查基板上所形成之膜之膜厚不均的膜厚 不均檢查裝置,其目的在於,高精度地檢查基板上所形成 之膜之膜厚不均。 本發明之膜厚不均檢查裝置包括:保持部,保持於主面 上形成有光透過性膜基板;光照射部,以特定射入角將光 照射至膜;攝影部,接受來自光照射部之光中由膜所反射 之特定波長的干涉光並取得膜之原影'像;以及膜厚不均檢 測部,一邊校正靈敏度依存於膜厚而變化的影響,上述靈 敏度係特定波長之干涉光的強度變動對於膜厚變動之比 例’一邊將原影像或自原影像導出之影像中之特定空間頻 帶振幅的程度作為膜厚不均而檢測。根據本發明,藉由校 正依存於膜厚而變化之靈敏度的影響,可高精度地檢查膜 厚不均。 本發明之一較佳實施形態中,膜厚不均檢查裝置進而包 括記憶部,記憶表示靈敏度與特定波長之干涉光之強度的 關係的靈敏度資§扎’且膜厚不均檢測部可藉由參照原影像 之各像素值及靈敏度資訊而一邊校正靈敏度變化之影 312χρ/發明說明書(補件)/95-11/95127465 7 1311643 ^響:邊檢測膜厚不均’從而可容易地校正靈敏度變化之 本發明之其他較佳實施形態中,攝影部包含多個攝影元 巧膜厚*均檢測部亦可藉由對於原影像或自原影像導出 声货^之各像素’進仃與對應的攝影元件相應之個別靈敏 ^化之影響的校正,校正攝影元件之輸出特性不同之影 谁:ΐ明之進而其他較佳實施形態中,膜厚不均檢查裝置 匕括記‘It部’記憶表示靈敏度與膜厚之關係之靈敏度 二且=厚t均檢測部參照主面上之膜之厚度及靈敏度 :邊板正靈敏度變化㈣響—邊檢賴料均。更佳 的疋,膜厚不均檢杳I晉彳隹 之膜厚測量部進而包括取得主面上之膜之厚度 部本:二之:形態中’膜厚不均檢測部包括:濾波器處理 衫像進行特定空間頻帶之帶通滤波器處理;以及 # #. 心波器處理部進行處理後之原影 声^田… 影響的校正藉由變更對比 X強凋邛中之對比度強調的程度而進行。 本發明亦適合檢查基板上所 厚不均檢查方法。—料成之膜之膜厚不均的膜 s ^他目的、特徵、形態及優點藉由參照隨附 圖式並可由以下本發明詳細的說明當中明白。 【實施方式】 圖1係表示臈之(絕對)反射率相對於膜厚而變化的 發明說明書(補件)/95-1】/95127465 8 1311643 圖,該變化係在以特定鉍 有光阻膜(以下,僅稱將「個波長的光照射至形成 膜」)之玻璃基板(以下,稱為 二」、月'兄。,1中’膜對於波長(正確地說,係半 見m左右之極乍波段之中央值)55G、600、650奈米 入光的反射率分別以圖1中賦予符號⑴、112、 113的線表不。此虛, 基板上之膜係存在於形成於基板之 = 圖1係將射人光之射人角S為60度、臈之折 為h 6、及鉻層之折射率設為(3. 77+4· 8i)通過運 =求得。再者’因求出反射率之運算係習知技術,故此 處省略說明。 如圖1所7F ’可知任—波長+膜之反射率均相對於膜厚 王週期的變化。該種反射率之變化之起因為,基板上之膜 之反射光實際上係射入光之基板上之膜的表面(上表面) 的反射光與基板上之膜之下表面(亦即,膜與基板本體之 ’面)的反射光的干涉光。此處,基板上之膜之反射率係 書干V光之強度對於射入光之強度的比率,從圖i中之縱軸 可瞭解為干涉光對於一定強度之射入光的強度,以下,就 反射率作為射入光之強度為!時之干涉光的強度(以下, 稱為「相對反射強度」)進行說明。此時,相對反射強度 h可如式(1)所示,將膜厚設為d並利用特定函數“。其 中,如上所述,基板上之膜之折射率及膜的下側之層的折 射率、以及光之射入角為固定。 R(d) …(1) 圖2係表示圖1中膜厚僅變動〗nm時之相對反射強度 312XP/_S^書(補件)/95-11/95127465 9 1311643 之變動的圖。圖2中,將干涉光的相對反射強度變動對於 膜厚之1 mn之變動的比例作為靈敏度並表示在縱軸,波 長為55G、6GG、65G nm之干涉光之靈敏度分別以圖ι中 賦予符號121、122、123的線表示。根據圖!及圖2,可 知:任-波長’於相對反射強度(或者反射率)之最大值附 近及最小值附近,靈敏度均變得非常小,因 膜料獲得充分的S/N比(訊號/雜訊比)。若將靈敏= 特疋值以下之膜厚範圍定義為死帶,則於相對反射強度之 最大值附近存在膜厚範圍較廣之死帶,於最小值附近存在 膑厚範圍較窄之死帶。再者’靈敏度&可如式⑵所示, 將膜厚設為d,並使用函數f,R,函數f,R係將式⑴中之 函數h對膜厚d微分而得。[Technical Field] The present invention relates to a technique for inspecting a film thickness unevenness (mura) of a film formed on a substrate. [Prior Art] When the film such as a glass substrate or a semiconductor substrate (for (4) cavity ^ "substrate") on the main surface of the display device is used, the film is irradiated with light from the light source and used. The interference from the reflected light of the film examined the film thickness unevenness. For example, Japanese Patent Laid-Open No. 194739=Report discloses a technique for obtaining an interference scene image in (4) by receiving light reflected from a substrate irradiated by a light source, and borrowing an interference image. By performing image processing to check the unevenness of the film thickness on the substrate, by selectively changing the wavelength of the light received by the image capturing portion, the thickness of the film on the substrate is uneven and the film thickness is uneven. The redundancy between the parts is adjusted to the desired size. Further, Japanese Patent No. 3335503 discloses a technique of irradiating light to one main surface side of a self-shielding film in a film thickness unevenness inspection of a light transmittance of a shading mask for a color picture tube. The tone data of the image taken from the other side of the main surface is measured by the median filter, and the smoothed data is obtained, and the standardized data is calculated by dividing the grayscale data by the smoothing resource= The display emphasizes the image of the film thickness unevenness mask to be detected', thereby achieving the simplification of the visual inspection and the improvement of the inspection accuracy. Therefore, the image of the film is obtained by the interference light 312XP/invention specification (supplement)/95-11/95127465 6 1311643 reflected by the film on the substrate of the party, and the film thickness is not detected based on the image. In the case where the intensity of the interference light changes with respect to the film thickness, the sensitivity as a ratio of the intensity variation of the interference light to the film thickness variation also varies depending on the film thickness. Therefore, the thickness of the film on the substrate or the degree of unevenness of the film thickness is affected by the change in sensitivity, and the film thickness unevenness may vary depending on the degree of lightness in the image, and the film may not be inspected with high precision. Uneven thickness. SUMMARY OF THE INVENTION The present invention is suitable for a film thickness unevenness inspection device for inspecting a film thickness unevenness of a film formed on a substrate, and an object thereof is to inspect a film thickness unevenness of a film formed on a substrate with high precision. The film thickness unevenness inspection apparatus according to the present invention includes: a holding portion that holds a light transmissive film substrate on a main surface; a light irradiation portion that irradiates light to the film at a specific incident angle; and a photographing portion that receives light from the light irradiation portion In the light, the interference light of the specific wavelength reflected by the film acquires the original image of the film; and the film thickness unevenness detecting portion changes the sensitivity depending on the film thickness, and the sensitivity is the interference light of a specific wavelength. The ratio of the change in intensity to the change in film thickness is detected as the film thickness unevenness of the original image or the amplitude of the specific spatial band in the image derived from the original image. According to the present invention, it is possible to accurately check the film thickness unevenness by correcting the influence of the sensitivity which varies depending on the film thickness. In a preferred embodiment of the present invention, the film thickness unevenness inspection device further includes a memory portion, and the sensitivity indicating the relationship between the sensitivity and the intensity of the interference light of the specific wavelength is memorable, and the film thickness unevenness detecting portion can be used by Correcting the change in sensitivity with reference to each pixel value and sensitivity information of the original image 312 χ ρ / invention manual (supplement) / 95-11/95127465 7 1311643 ^ Sound: uneven detection of film thickness can be easily corrected for sensitivity change In another preferred embodiment of the present invention, the photographing unit includes a plurality of photographing elements, and the detecting unit can also extract and correspond to each pixel of the original image or the original image. Correction of the influence of the individual sensitive sensitivity of the component, correcting the difference in the output characteristics of the photographic element. Whoever: In other preferred embodiments, the film thickness unevenness inspection device includes the 'It part' memory representation sensitivity and The sensitivity of the relationship between the film thickness and the thickness of the thickness detection unit refers to the thickness and sensitivity of the film on the main surface: the positive sensitivity of the side plate changes (four) ringing - both sides are checked. Better 疋, film thickness unevenness inspection 彳隹 I Jin 彳隹 film thickness measurement section further includes the thickness of the film on the main surface: two: in the form of the film thickness unevenness detection section includes: filter processing The shirt image is processed by a bandpass filter for a specific spatial frequency band; and ##. The original shadow sound after processing by the heartbeat processing unit... The correction of the influence is corrected by changing the contrast emphasis in the X strong fade get on. The present invention is also suitable for inspecting a method for inspecting uneven thickness on a substrate. — 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 [Embodiment] Fig. 1 is a diagram showing the (absolute) reflectance of ruthenium relative to the film thickness (Supplement) / 95-1] / 95127465 8 1311643, which is characterized by a specific photoresist film. (Hereinafter, the glass substrate (hereinafter referred to as "two-dimensional", "moon" brother, which is called "the light of one wavelength is irradiated to the film"), the film of "1" is the wavelength (correctly speaking, it is about half) The central value of the extreme chirp band) The reflectances of the incident light of 55G, 600, and 650 nm are respectively indicated by the lines given the symbols (1), 112, and 113 in Fig. 1. The virtual film on the substrate exists on the substrate. = Fig. 1 is to shoot the human light, the angle S is 60 degrees, the 臈 is folded to h 6 , and the refractive index of the chrome layer is set to (3. 77+4· 8i). Since the calculation technique of the reflectance is known, the description is omitted here. As shown in Fig. 1 and Fig. 7F, it can be seen that the reflectance of the wavelength-+ film is changed with respect to the film thickness, and the change of the reflectance Because the reflected light of the film on the substrate is actually the reflected light of the surface (upper surface) of the film incident on the substrate of the light and the film on the substrate The interference light of the reflected light on the lower surface (that is, the surface of the film and the substrate body). Here, the reflectance of the film on the substrate is the ratio of the intensity of the dry V light to the intensity of the incident light, from FIG. The vertical axis of the medium can be understood as the intensity of the incident light of the interference light for a certain intensity. Hereinafter, the reflectance is performed as the intensity of the interference light when the intensity of the incident light is ? (hereinafter referred to as "relative reflection intensity"). In this case, the relative reflection intensity h may be as shown in the formula (1), and the film thickness is set to d and a specific function is used. Here, as described above, the refractive index of the film on the substrate and the lower layer of the film The refractive index and the incident angle of light are fixed. R(d) (1) Fig. 2 is a graph showing the relative reflection intensity when the film thickness in Fig. 1 is only changed by 311XP/_S^(supplement)/95 -11/95127465 9 1311643 Variation diagram. In Figure 2, the ratio of the relative reflection intensity variation of the interference light to the variation of the film thickness of 1 mn is taken as the sensitivity and is shown on the vertical axis, and the wavelength is 55G, 6GG, 65G nm. The sensitivity of the interference light is represented by the line assigned to the symbols 121, 122, and 123 in Fig. 1, respectively. And Fig. 2, it can be seen that the sensitivity of the arbitrary-wavelength 'in the vicinity of the maximum value of the relative reflection intensity (or reflectance) and the minimum value becomes very small, because the film material obtains a sufficient S/N ratio (signal/miscellaneous) If the film thickness range below the sensitivity = characteristic value is defined as a dead band, there is a dead band with a wide film thickness near the maximum value of the relative reflection intensity, and the thickness range is narrow near the minimum value. In addition, the 'sensitivity' can be set to d as shown in equation (2), and the function f, R, function f, R is used to differentiate the function h in the formula (1) from the film thickness d. .
Sk= | f R(d) I ...(2) 於此’著眼於1個波長55〇 nm,就靈敏度與相對反射 強度之關係加以敍述。目3制以說明靈敏度與相對反射 強度U係的圖。圖3中之上層左側表示靈敏度相對於膜 厚之變化’上層右側表示靈敏度相對於相對反射強度之變 化,下層右側將膜厚作為縱軸表示相對反射強度相對於膜 厚之變化。 圖3中之上層右侧料符號13G之2條線分別對應於圖 3中之上層左侧中的隔著膜厚範圍寬度較窄之谷部分而存 在之2個山形的各組合的左側山形及右侧山形(圖3中之 下層右側’伴隨膜厚之增加,相對反射強度減小的部分、 及相對反射強度增加的部分),2條線13〇大致重疊。又, 312XP/發明說明書(補件)/9M 1/95127465 10 1311643 右於圖3中之上層左側中之2個山形的多個組合間加以比 較,則於分別對應於左側山形之靈敏度與相對反射強度之 f係、及對應於右侧山形之靈敏度與相對反射強度之關係 幾乎未產生差別。因此,靈敏度與相對反射強度之關 係可以說並非依存於膜厚而大致一定,其他波長情況亦相 同。 只際上,即使於彼此不同之波長間加以比較時,靈敏度 與相對反射強度之關係大致相同。因此,例如圖3中之上 •層右财2條線13〇之-條、或表示該等線13()之平均的 線等係如圖4所示表示各波長中之靈敏度與相對反射強 度之關係者。靈敏度與相對反射強度之關係中,若相對反 射強度之最大值為Rkmax、最小值為Rkmin,則相對反射強度 為Rk時之靈敏度sk可使用特定函數fs表示為式(3)。Sk = | f R(d) I (2) Here, focusing on one wavelength of 55 〇 nm, the relationship between sensitivity and relative reflection intensity will be described. The figure 3 is a diagram illustrating the sensitivity and the relative reflection intensity U. The left side of the upper layer in Fig. 3 indicates the change in sensitivity with respect to the film thickness. The right side of the upper layer indicates the change in sensitivity with respect to the relative reflection intensity, and the film thickness on the right side of the lower layer indicates the change in relative reflection intensity with respect to the film thickness. The two lines of the upper right symbol 13G in FIG. 3 correspond to the left side of each combination of two mountain shapes in the left side of the upper layer in FIG. 3 and the valley portion having a narrow width in the film thickness range. In the right mountain shape (the portion on the right side of the lower layer in Fig. 3 with an increase in film thickness, a portion where the relative reflection intensity decreases, and a portion where the relative reflection intensity increases), the two lines 13 〇 substantially overlap. Moreover, 312XP/invention specification (supplement)/9M 1/95127465 10 1311643 is compared with a plurality of combinations of two mountain shapes in the left side of the upper layer in FIG. 3, and then corresponds to the sensitivity and relative reflection of the left mountain shape respectively. There is almost no difference in the relationship between the intensity f-system and the sensitivity corresponding to the right mountain shape and the relative reflection intensity. Therefore, the relationship between the sensitivity and the relative reflection intensity can be said to be substantially constant depending on the film thickness, and the other wavelengths are also the same. In the meantime, even when compared between wavelengths different from each other, the relationship between sensitivity and relative reflection intensity is substantially the same. Therefore, for example, the upper line of the 2 layers of the right layer of Fig. 3, or the line indicating the average of the lines 13 (), etc., as shown in Fig. 4, indicate the sensitivity and relative reflection intensity in each wavelength. Relationship. In the relationship between the sensitivity and the relative reflection intensity, if the maximum value of the relative reflection intensity is Rkmax and the minimum value is Rkmin, the sensitivity sk when the relative reflection intensity is Rk can be expressed by the specific function fs as Equation (3).
Rk ~ Rkmin、 以下,就使用上述靈敏度與相對反射強度之關係之膜厚 不均檢查加以詳細說明。 圖5係表示本發明之第丨實施形態之膜厚不均檢查裝置 1的構成的圖。膜厚不均檢查裝置J係如下裝置,於用於 液晶顯示裝置等顯示裝置之玻璃基板9中,取得其中一個 主面91上所形成之圖案形成用光阻膜92之影像,並根據 該影像檢查膜厚不均。基板9上之膜92藉由於基板9之 上表面91上塗佈光阻液而形成。 312XP/發明說明書(補件)/95-11/95127465 11 1311643 此處’基板9上之膜92之膜 覺,因此定義不易,但例如縱及 ^依存於人類的視 且為i個顯示裝置之組裝零件之:長f士分別為大致h, 期之距離自數mm至數cm之膜之厚产’相當於1個週 厚不均的原因,該變動之振幅程;=均)係膜 即,膜厚不均之程度)。又,於 ^成膜异不均(亦 板9上對應於1個顯示|置 '夕個面板圖案之基 於膜之厚度變動之! 4固Hr板之區域内,未包含相當 子反义助心i 1固週期的距離時 丨膜厚不均。因此,對基板9上摄!,二,變動不構成 攸y上攝影膜92之影傻中一蛀— 空間頻帶之振幅程度(亦即,月邱μ bb & 〜像中特疋 為膜厚不均。 卩一明暗變動程幻可瞭解 如圖5所示,膜厚不均檢查裝置 有膜92之主面91(以下,稱為「上 2,形成 ρ ,.、 局上表面91」)朝向上側(圖 中之(+Ζ)側)保持基板9 ;光照射部3,以特定射入角將 光,射至㈣於平台2之基板9上之膜92;受光單元4, 接受自光照射部3照射並於基板9之上表面91上之膜92 反射的光;波長切換機構5,配置於基板9與受光單元4 之間並切換受光單it 4所接受的光的波長;移動機構21, Y』、兀…、耵4 d、文先早兀4及波長切換機構 5移動;膜厚不均檢測部7,根據受光單元4所接受之光 之強度分佈(對應於上表面91之區域之分佈)檢測膜92之 膜厚不均’·記憶部6 ’記憶膜厚不均檢測部7檢測膜厚不 均時所利用之特定資訊;以及控制部8,控制該等之構成。 平台2( + Z)侧之表面較佳的是黑色去光。移動機構u 31ZXP/發明說明書(補件mm丨奶⑵祕 12 1311643 ^成^珠螺桿(省略_與 ::旋轉,平台2沿導件212在基板=二= 圖5甲叉方向移動。 敎y之上表面91之 光照射部3包括:鹵音抨q .光(亦即,包含可見之:,作為光源’並射出白色 英棒犯,^1有波長之光的光)柱狀石 方6 。、平台2之移動方向垂直之圖5中的y 方向,以及圓柱透鏡33, 鹵素燈31安裝於石方向。光照射部3,’ Φ 〇1 M 、、棒32之( + Y)側之端部,且自鹵辛燈 響31射入至石英槔叨 曰图畜/立 即,# φ 、 轉換為於γ方向延伸之線狀光(亦 =❹於Υ方向成較長線狀之光)並自石英棒犯之 :面射出,經由圓柱透鏡33導向基板9之上表㈣卜換 棒32及圓柱透鏡33係光學系統,其等將來自 鹵素燈31之光轉換為與平台2之移動 並導向基板9的上表面9卜 罝的線狀先 “中’以一點鏈線表示自光照射部3至基板9之光路 鲁(自基板9至受光單元4之光路亦同)。自光照射部3射出 之光之-部分於基板9之上表面91上之膜92⑽側的上 表面反射。膜92對來自光照射部3之光具有光透過性, 來自光照射部3之光中未在膜92之上表面反射的光透過 膜92並於基板9之上表面91(亦即,膜92之下表面)反 射。膜厚不均檢查裝置丨中,於基板g中之膜92之上表 面反射的光與於基板9之上表面91反射的光的干涉光經 由波長切換機構5射入至受光單元4。 波長切換機構5包括:多個光學濾波器(例如,半寬為 312ΧΡ/發明說明書(補件)/95-11/95127465 13 1311643 nm之干涉濾波器)5卜選擇性地分別透過彼此不同的 多個波長之光’·圓板狀濾波器轉# 52,保持多個光學濾 波器51,以及滤波器旋轉馬達53,安裝於滤波器轉盤 之中〜用來使滤波器轉盤52旋轉。濾波器轉盤52以其法 線方向與自基板9至受光單元4之光路平行的方式配置。 、圖6係自基板9側沿與濾波器轉盤52垂直之方向觀察 波長切換機構5的圖。如圖6所示。慮波器轉盤52中,Rk ~ Rkmin, Hereinafter, the film thickness unevenness inspection using the relationship between the above sensitivity and the relative reflection intensity will be described in detail. Fig. 5 is a view showing the configuration of a film thickness unevenness inspection device 1 according to a third embodiment of the present invention. The film thickness unevenness inspection device J is an apparatus for obtaining an image of the pattern forming resist film 92 formed on one of the main faces 91 in a glass substrate 9 for a display device such as a liquid crystal display device, and based on the image Check for uneven film thickness. The film 92 on the substrate 9 is formed by applying a photoresist on the upper surface 91 of the substrate 9. 312XP/Invention Manual (Supplement)/95-11/95127465 11 1311643 Here, the film texture of the film 92 on the substrate 9 is not easy to define, but for example, the vertical and the ^ depend on human vision and are i display devices. As for the assembled parts, the length of the film is approximately h, and the period of the film is from the thickness of several mm to several cm. The thickness of the film is equivalent to one week thickness unevenness, the amplitude range of the change; , the degree of uneven film thickness). In addition, the film is unevenly formed (also corresponds to the thickness variation of the film on the plate 9 corresponding to one display|set of the 'seven panel pattern'! 4 The area of the solid Hr plate does not include the equivalent antisense helper When the distance of the solid cycle is i 1 , the film thickness is uneven. Therefore, the substrate 9 is photographed! Second, the variation does not constitute the shadow of the photographic film 92 on the 攸 y - the amplitude of the spatial band (ie, the month) Qiu μ bb & ~ The special film is uneven in film thickness. As shown in Fig. 5, the film thickness unevenness inspection device has the main surface 91 of the film 92 (hereinafter, referred to as "on" 2, forming ρ, ., the upper surface 91") toward the upper side (the (+ Ζ) side in the figure) holds the substrate 9; the light illuminating portion 3, the light is incident at a specific incident angle to the substrate of the platform 2 The upper film 92; the light receiving unit 4 receives light reflected from the film 92 on the upper surface 91 of the substrate 9 by the light irradiation unit 3; the wavelength switching mechanism 5 is disposed between the substrate 9 and the light receiving unit 4 and switches The wavelength of the light received by the light sheet it 4; the moving mechanism 21, Y 』, 兀..., 耵 4 d, the text early 4 and the wavelength switching mechanism 5; the film thickness is uneven The measuring unit 7 detects the film thickness unevenness of the film 92 based on the intensity distribution of the light received by the light receiving unit 4 (corresponding to the distribution of the region of the upper surface 91). The memory portion 6 'memory film thickness unevenness detecting portion 7 detects the film The specific information used when the thickness is uneven; and the control unit 8 controls the composition of the surface. The surface of the platform 2 (+Z) side is preferably black light. The moving mechanism u 31ZXP / invention manual (repair mm丨Milk (2) secret 12 1311643 ^ into the bead screw (omitted _ with:: rotation, the platform 2 moves along the guide 212 in the substrate = two = Fig. 5 in the direction of the fork. The light illuminating portion 3 of the upper surface 91 of the 敎y includes: halogen Sound 抨 q . Light (that is, including visible:, as a light source 'and emits a white sin, ^1 light with wavelength light) columnar stone 6 ., the direction of movement of platform 2 is vertical in Figure 5 The y direction, and the cylindrical lens 33, the halogen lamp 31 is mounted in the stone direction. The light irradiation portion 3, 'Φ 〇1 M , the end of the (+ Y) side of the rod 32, and is incident from the halogen lamp 31 To the quartz 槔叨曰 picture animal / immediately, # φ , converted to linear light extending in the γ direction (also = a longer linear light in the direction of the Υ And from the quartz rod: the surface is emitted, and guided through the cylindrical lens 33 to the upper surface of the substrate 9 (4), the replacement rod 32 and the cylindrical lens 33-based optical system, which convert the light from the halogen lamp 31 into the movement with the platform 2 And the upper surface of the guide substrate 9 is in the form of a line, and the "middle" indicates the light path from the light-irradiating portion 3 to the substrate 9 with a single chain line (the light path from the substrate 9 to the light-receiving unit 4 is also the same). The portion of the light emitted from the portion 3 is partially reflected on the upper surface of the film 92 (10) side on the upper surface 91 of the substrate 9. The film 92 is light transmissive to the light from the light irradiation portion 3, and the light from the light irradiation portion 3 is not in the light. Light reflected from the upper surface of the film 92 passes through the film 92 and is reflected on the upper surface 91 of the substrate 9 (i.e., the lower surface of the film 92). In the film thickness unevenness inspection device, the interference light of the light reflected on the surface of the film 92 in the substrate g and the light reflected on the upper surface 91 of the substrate 9 is incident on the light receiving unit 4 via the wavelength switching mechanism 5. The wavelength switching mechanism 5 includes: a plurality of optical filters (for example, an interference filter having a half width of 312 ΧΡ / invention specification (supplement) / 95-11/95127465 13 1311643 nm) 5 selectively selectively transmitted through each other The light of the wavelength '·the circular plate filter turns 52 52 holds the plurality of optical filters 51 and the filter rotating motor 53 and is mounted in the filter turntable - for rotating the filter turntable 52. The filter disk 52 is disposed such that its normal direction is parallel to the optical path from the substrate 9 to the light receiving unit 4. Fig. 6 is a view of the wavelength switching mechanism 5 viewed from the side of the substrate 9 in a direction perpendicular to the filter turntable 52. As shown in Figure 6. In the filter turntable 52,
於周方向等間隔形成有6個圓形開口 521,其中5個開口 521中安裝有透過波長彼此不同之5種光學滤波器51。 、,5所示之波長切換機構5中,被控制部8所控制之濾 波器旋轉馬達53使濾波器轉盤52旋轉,並於5個光學濾 波器51(參照圖6)中,選擇任一光學濾波器51(以下,為 〃其他光學;慮波器51相區別,稱為「選擇光學濾、波器 =a」),配置於自基板9至受光單元4之光路上。藉此, 來自基板9之反射光(亦即,包含對應於5個光學濾波器 51之5個透過波長之干涉光的白色光的反射光)中,僅與 光路上所配置之選擇光學濾波器51a相應之特定波長(= 下,稱為「特定波長」)的干涉光,透過選擇光學濾波器 51a並導向受光單元4。 並且,當濾波器旋轉馬達53使濾波器轉盤52旋轉時, 則多個光學濾波器51中配置於自光照射部3至受光單元 4之光路上之選擇光學濾波器5丨a切換為其他光學濾波器 51,且受光單元4所接受之干涉光之波長(亦即,特定波 長)變更。如此,波長切換機構5藉由於多個光學濾、波器 312XP/發明說明書(補件)/95-11/95127465 14 1311643 51間切換選擇光學濾波器51a,變為於多個光學濾波器 51之透過波長間切換與膜厚不均檢查有關之特定波長的 切換機構。 受光單元4包括:攝影部41 ;以及透鏡4 2,設置 影部41與波長切換機構5之選擇光學濾波器51a之間並 將來自基板9之反射光導向攝影部41。 圖7係表示攝影部41之受光面的圖。如圖7所示,攝 影部41中設置有線感測器41〇,該線感測器41〇含有於γ 方向排列為直線狀之多個攝影元件(例如,CCD(Charge Coupled Device,電荷耦合器件))411。圖5之攝影部4i 中,藉由光照射部3之照射並於基板9上之膜犯反射之 線狀光中,透過選擇光學遽波器51a之特定波長之干涉光 由攝影兀件411接受,從而可取得干涉光之強度分佈(亦 即,來自各攝影元件411之輸出值在γ方向上的分佈)。 實際上,伴隨基板9向X方向之移動攝影部41之 器仙重複取得干涉光之強度分佈,從而可板'上 之膜92之2維影像。 于土敬9上 4 = 7包括輸出受理部71,將來自攝影部 輸出作為基板9上之膜92之多色調影像 膜厚不均檢測冑7進而包括:缝器處理部72,對於於 出受理部71所受理之影像進行料 =理;對比度強調部73,強調由滤波 過後之影像對比度;以及評估值算出部74, /ψ72處理 據對比度強調後之^出用於根 V取马缺陷之膜厚不 312XP/發明說明書(補件)/95-⑽5】27你 μ 1311643 均)之有無的特定評估值。 〃、二就利用膜厚不均檢查裝置1檢查膜厚不均之流程 加以說明0圖β ± _ 圖係表示膜厚不均檢查裝置ί檢查基板g上 之、之膜厚不均的處理的流程圖。在檢查基板9上之 •膜92之膜厚不均時,作為事前準備,預先取得膜厚不均 •=人中之處理所利用之靈敏度資訊61,並記憶於記 L。卩6進行準備(步驟S10)。 靈敏度貧訊61係表示作為特定波長干涉光的相對反射 •強度變動對於膜厚變動之比例的靈敏度、與特定波長干涉 >光之相對反射強度的關係者(參照圖4),如剛參照圖3所 说明般,在求出膜厚與相對反射強度之關係、及膜厚與靈 敏度之關係後,根據該㈣係取得靈敏度資訊Η。如後 所述’因特定波長亦可切換為選擇光學滤波器仏以外之 -他光予m 51之透過波長,故必須有分別對應於多 個光學遽波器51之透過波長的靈敏度資訊6卜但如上所 修述’因靈敏度與干涉光之相對反射強度之關係於膜厚不均 檢查裝置1所利用之其他所有波長中均大致相同,故此 處’僅準備1個靈敏度資訊6卜再者,靈敏度資訊61只 要基板9上之膜92為光透過性膜’則不太過依存在膜之 材料等,而較大地依存於來自光照射部3之光之射入膜 92的射入角,故實際上’步驟训之處理於組裝膜厚不 均檢查裝置i時進行並記憶於記憶部6作為裝置固有資 訊,於膜厚不均檢查裝置i之通常使用時,由以下處 始。 312XP/發明說明書(補件)/95_ 11/% 127465 1311643 膜厚不均檢查裝置1中,基板9保持於位於圖5中實線 所示之檢查開始位置之平台2上後,基板9及平台2開始 朝(+X)方向之移動(步驟S11)。其次,自光照射部3射出 並對基板9之上表面91以射入角6〇。射入的線狀光,照 射於上表面91上之直線狀照射區域(以下,稱為「線狀 恥射區域」)(步驟S12),線狀照射區域相對於基板9移 動。 來自光照射部1之光於基板9之上表面91反射,並藉 •由透過波長切換機構5之選擇光學滤波器51a僅取出特定 波長的光(干涉光)後,導向攝影部41。攝影部41中,線 感測器410接受特定波長之干涉光,取得干涉光於基板9 j之線狀照射區域中的強度分佈(步驟13)。來自線感測 器410之各攝影元件4Π之輪出傳送至膜厚不均檢測部7 並由輸出受理部71所受理。 膜厚不均檢查裝置1中,藉由控制部8,於基板9之移 φ動中反覆確認基板9及平台2是否移動至圖5中以二點鍵 線所示之檢查結束位置(步驟su),在未移動至檢查結束 位置情=時,重複返回至步驟Sl3 #受特定波長之干涉 光,取得特定波長光於線狀照射區域中㈣度分佈。並 且,若基板9及平台2移動至檢查結束位置(步驟Sl4), 則停止移動機構21對基板9及平台2的移動,昭明光之 照射亦停止(步驟S15)。膜厚不均檢查裝置2 _,平” 方向移動期間,步驟S13之動作與平台2之移動° v並反覆進行,藉此可取得膜92在基板9之整體中的影 1 ^^#^^^#(^)/95.1^95127465 \1 1311643 像資料(亦即,進行攝影)。 右攝影基板9之上表面91整體之膜92(或與該動作 時進行)’則膜厚不均檢測部7之輸出受理部71中,來^ 所儲存之線感測器410之各攝影元件411的輸出根 轉換式轉換為例如8 bit(當然,8 bit以外亦可)之值 ,值)’並按時間順序排列。藉此,生成有膜厚不均檢測 部7中之處理用2維影像(實質係於攝影部41所取得 像,並為實施下述之處理前之影像,以下,稱為「原: 像」)並輸出至濾波器處理部72。如上所述,备膜q =度不同則膜92之反射率亦不同,故由線感測器、仙 、接文之反射光之強度亦不同。因此,於膜92之厚度 二膜厚不均時’較理想的是,原影像中亦產生像 二輸出受理部71t,對於各攝影元件4u,取得於 述處理所利用之相對反射強度之最大值及最小值。於 朝6 k舨而W基板9上之膜92之外緣部為膜92之厚度 二= 斬減少之傾斜部’取得攝影時之該部分之強度 =摄:常,取得分別對應於干涉光之最大強度及最小 如元件411的輸出的最大值及最小值。因此,例 抑像中攝影元件4U之輸“取得像素值的 =個:素:像:r最大值及最小值,並將此等i 參元件41 «而只貝地取得相对反射強度對應於該攝 n之最大值及最小值。再者,因相對反射強度於 312ΧΡ/發明說明書(補件)/95-11/95127465 18 1311643 各攝影兀件411中之最大值及最小值係依存於該攝影元 件411相對於光照射部3之配置,故可與靈敏度資訊相 同,於組裝膜厚不均檢查裳£ j時取得,該值記憶於記憶 部6並於檢查時使用。 其次’藉由濾波器處理部72壓縮原影像並生成第i影 像:於此’若將原影像t位於座標(χ,γ)之像素的像素值 表丁為Fxy則於以原影像為、像素X、像素之範圍為單位 f;而生成之第1影像中’位於座標(〜之注目像素之 像素值Axy可根據式(4 )求出。 A, #十"一iSa(y+W—lSix circular openings 521 are formed at equal intervals in the circumferential direction, and five kinds of optical filters 51 having different transmission wavelengths are mounted in the five openings 521. In the wavelength switching mechanism 5 shown in FIG. 5, the filter rotating motor 53 controlled by the control unit 8 rotates the filter dial 52, and selects either optical in the five optical filters 51 (see FIG. 6). The filter 51 (hereinafter, referred to as "other opticals; the filter 51 is distinguished from each other and referred to as "select optical filter, wave device = a") is disposed on the optical path from the substrate 9 to the light receiving unit 4. Thereby, among the reflected light from the substrate 9 (that is, the reflected light including the white light corresponding to the interference light of the five transmission wavelengths of the five optical filters 51), only the selective optical filter disposed on the optical path is provided. The interference light of the specific wavelength (=, referred to as "specific wavelength") corresponding to 51a is transmitted through the selection optical filter 51a and guided to the light receiving unit 4. Further, when the filter rotating motor 53 rotates the filter turntable 52, the selection optical filter 5A disposed on the optical path from the light-irradiating portion 3 to the light-receiving unit 4 among the plurality of optical filters 51 is switched to another optical The filter 51 is changed in wavelength (i.e., specific wavelength) of the interference light received by the light receiving unit 4. Thus, the wavelength switching mechanism 5 is changed to the plurality of optical filters 51 by switching between the plurality of optical filters, the filter 312XP, the invention specification (supplement)/95-11/95127465 14 1311643 51, and the optical filter 51a. A switching mechanism for a specific wavelength related to the inspection of the thickness difference by the switching between the wavelengths. The light receiving unit 4 includes a photographing unit 41 and a lens 42 which is disposed between the shadow unit 41 and the selection optical filter 51a of the wavelength switching mechanism 5 and guides the reflected light from the substrate 9 to the photographing unit 41. FIG. 7 is a view showing a light receiving surface of the photographing unit 41. As shown in FIG. 7, the imaging unit 41 is provided with a wired sensor 41A, and the line sensor 41 includes a plurality of imaging elements arranged in a line in the γ direction (for example, a CCD (Charge Coupled Device) )) 411. In the photographing unit 4i of Fig. 5, the interfering light of the specific wavelength of the selective optical chopper 51a is received by the photographing element 411 in the linear light reflected by the film on the substrate 9 by the irradiation of the light irradiation unit 3. Thereby, the intensity distribution of the interference light (that is, the distribution of the output values from the respective imaging elements 411 in the γ direction) can be obtained. Actually, the intensity distribution of the interference light is repeatedly obtained by moving the substrate 9 to the imaging unit 41 in the X direction, so that the two-dimensional image of the film 92 on the board ' can be obtained. 4: 7 includes the output accepting unit 71, and the multi-tone image thickness unevenness detecting unit 7 that outputs the film 92 on the substrate 9 from the photographing unit further includes a stitcher processing unit 72, and accepts the stitching processing unit 72. The image received by the unit 71 is subjected to the material control; the contrast enhancement unit 73 emphasizes the image contrast after the filtering; and the evaluation value calculation unit 74, /ψ72 processes the film for the root V to obtain the horse defect according to the contrast emphasis. Thick not 312XP / invention manual (supplement) / 95- (10) 5] 27 you μ 1311643 are specific evaluation values. 〃 and 2, the process of inspecting the film thickness unevenness by the film thickness unevenness inspection apparatus 1 is explained. FIG. β± _ The figure shows the film thickness unevenness inspection apparatus ί, and the film thickness unevenness on the substrate g is inspected. flow chart. When the thickness of the film 92 on the substrate 9 is uneven, the sensitivity information 61 used for the processing of the person is obtained in advance as a preparation for the film thickness.卩6 is prepared (step S10). The sensitivity information 61 indicates the relationship between the relative reflection intensity of the specific wavelength interference light and the sensitivity of the film thickness variation, and the interference with the specific wavelength and the relative reflection intensity of the light (see FIG. 4). As described in the third section, after determining the relationship between the film thickness and the relative reflection intensity and the relationship between the film thickness and the sensitivity, the sensitivity information is obtained based on the (4). As will be described later, 'because the specific wavelength can also be switched to select the optical filter - other than the transmission wavelength of m 51, it is necessary to have sensitivity information corresponding to the transmission wavelengths of the plurality of optical choppers 51 respectively. However, as described above, the relationship between the sensitivity and the relative reflection intensity of the interference light is substantially the same as that of all other wavelengths used by the film thickness unevenness inspection apparatus 1. Therefore, only one sensitivity information 6 is prepared here. As long as the film 92 on the substrate 9 is a light transmissive film, the sensitivity information 61 does not depend too much on the material of the film, but greatly depends on the incident angle of the incident film 92 from the light of the light irradiation unit 3. Actually, the process of the step-and-step process is performed when the film thickness unevenness inspection device i is assembled and is stored in the memory unit 6 as the device-specific information. When the film thickness unevenness inspection device i is normally used, the following is used. 312XP/Invention Manual (Replenishment)/95_11/% 127465 1311643 In the film thickness unevenness inspection device 1, after the substrate 9 is held on the stage 2 located at the inspection start position shown by the solid line in Fig. 5, the substrate 9 and the platform 2 starts moving in the (+X) direction (step S11). Next, the light-irradiating portion 3 is emitted and the upper surface 91 of the substrate 9 is incident at an angle of 6 。. The incident linear light is irradiated onto the linear irradiation region on the upper surface 91 (hereinafter referred to as "linear shame region") (step S12), and the linear irradiation region is moved relative to the substrate 9. The light from the light-irradiating portion 1 is reflected on the upper surface 91 of the substrate 9, and only the light of the specific wavelength (interference light) is taken out by the selective optical filter 51a of the transmission wavelength switching mechanism 5, and then guided to the imaging unit 41. In the photographing unit 41, the line sensor 410 receives the interference light of a specific wavelength, and acquires the intensity distribution of the interference light in the linear irradiation region of the substrate 9j (step 13). The photographic elements from the line sensor 410 are transferred to the film thickness unevenness detecting unit 7 and received by the output receiving unit 71. In the film thickness unevenness inspection apparatus 1, the control unit 8 repeatedly checks whether the substrate 9 and the stage 2 have moved to the inspection end position indicated by the two-point key line in FIG. 5 in the movement of the substrate 9 (step su When it is not moved to the inspection end position, the process returns to step S13, and the interference light of the specific wavelength is repeatedly obtained, and the (four) degree distribution of the specific wavelength light in the linear irradiation region is obtained. When the substrate 9 and the stage 2 are moved to the inspection end position (step S14), the movement of the substrate 9 and the stage 2 by the moving mechanism 21 is stopped, and the illumination of the light is also stopped (step S15). When the film thickness unevenness inspection device 2 moves in the "flat" direction, the operation of step S13 and the movement of the stage 2 are repeated, thereby obtaining the shadow of the film 92 in the entirety of the substrate 9 ^ ^^#^^ ^#(^)/95.1^95127465 \1 1311643 Image data (that is, photographing). The film 92 of the entire upper surface 91 of the right photographic substrate 9 (or during the operation) 'thickness unevenness detecting portion In the output receiving unit 71 of the seventh embodiment, the output of each of the imaging elements 411 of the line sensor 410 stored in the conversion sensor 410 is converted into a value of, for example, 8 bits (of course, 8 bits or more), and is pressed. In this way, the two-dimensional image for processing in the film thickness unevenness detecting unit 7 is generated (substantially the image obtained by the image capturing unit 41, and the image before the processing described below is performed, hereinafter referred to as " The original image is output to the filter processing unit 72. As described above, the reflectance of the film 92 is different when the preparation film q = degree is different, so the intensity of the reflected light by the line sensor, the fairy, and the article is also different. Therefore, when the film thickness of the film 92 is not uniform, it is preferable that the image output receiving portion 71t is also generated in the original image, and the maximum value of the relative reflection intensity used for the processing is obtained for each of the image forming elements 4u. And the minimum. The outer edge portion of the film 92 on the W substrate 9 is the thickness of the film 92. The thickness of the film 92 is reduced. The intensity of the portion at the time of photographing is taken as usual. The maximum intensity and minimum are the maximum and minimum values of the output of element 411. Therefore, the image of the photographic element 4U is "acquired by the pixel value = prime: image: r maximum and minimum values, and these i-parameter elements 41 « and only the relative reflection intensity of the shell corresponds to the The maximum and minimum values of n are taken. Furthermore, the maximum and minimum values of the respective photographic elements 411 depend on the relative reflection intensity at 312 ΧΡ / invention manual (supplement) / 95-11/95127465 18 1311643 Since the element 411 is disposed relative to the light-irradiating portion 3, it can be obtained in the same manner as the sensitivity information, and is acquired when the film thickness unevenness is detected. This value is stored in the memory unit 6 and used in the inspection. The processing unit 72 compresses the original image and generates an ith image: "If the pixel value of the pixel in which the original image t is located at the coordinates (χ, γ) is Fxy, the range of the original image, the pixel X, and the pixel is The unit f is generated in the first image, and the pixel value Axy of the pixel of interest is obtained according to the equation (4). A, #十"一iSa(y+W-1
Σ Σ fxA (4) X=sax Y=say =實㈣…3為4(像素),故藉由式⑷之運算, 衫像之S/N比提高為原影像之4倍。當 ί壓縮後之原影像),則對第1影像進行低㈣波像 並根據第1影像生成使高頻 理, 化之第2影像。決定低通據波器處理:;::=平滑 每個邊長綠…)像素之正方形,帛2:二之…系 (X,y)之注目像素之像素值 心象中位於座標 像素之第丨影像中的像素值‘^ 求出。 ‘、、、式(4))並猎由式(5)而 x+Sj y+sjΣ Σ fxA (4) X=sax Y=say = real (four)...3 is 4 (pixels), so the S/N ratio of the shirt image is increased to 4 times that of the original image by the operation of equation (4). When the original image is compressed, the low (four) wave image is imaged on the first image, and the second image is generated based on the first image. Decide the low-pass data processing: ;::= smooth each side of the green ...) the square of the pixel, 帛 2: two... the pixel value of the pixel of the (X, y) pixel is located in the third pixel of the coordinate pixel The pixel value '^ in the image is found. ‘, ,, (4)) and hunt by equation (5) and x+Sj y+sj
Lxy = Σ Σ Axy/(2si + l)2 X=X_Sj Y=y—sj 312XP/發明說明書(補件)/95-11/95127465 ...(5) 19 1311643 像影像進行高通濾波器處理,並根據第2影 ^ ,該第3影像係除去作為下述對比度強調 處理之p早礙之低頻的濃度變動者。此處,位於座標(x,y) 第2 之像素* Hxy,使用注目像素附近之各像素的 第2衫像中的像素值L(參照式⑸)並藉由式⑹而求出。Lxy = Σ Σ Axy/(2si + l)2 X=X_Sj Y=y_sj 312XP/Invention Manual (supplement)/95-11/95127465 ...(5) 19 1311643 Image-based high-pass filter processing, According to the second image, the third image system removes the density variation of the low frequency which is the early influence of the contrast enhancement processing described below. Here, the second pixel * Hxy located at the coordinates (x, y) is obtained by the equation (6) using the pixel value L (see equation (5)) in the second shirt image of each pixel in the vicinity of the pixel of interest.
HYV = LHYV = L
…(6) 瞀ί I!)表:如下之情形:作為決定高通濾波器處理之運 二丰之^ 口’使用以注目像素為中心之各邊、長為(2s2 + 厭々素之正方形窗口。如上所述,對m處理部72中 原:IV像之第1影像,實施低通濾波器處理後,藉由實 =牛通濾波器處理’來進行特定空間頻帶之帶通濾波器處 理(步驟S16)。 當遽波器處理部7 ? Φ # ϊ田# i 中處理、、,σ束,則藉由對比度強調 °子第影像進行對比度強調處理,從而生成強卿 像(步驟即。強調影像中位於座標(x,y)之注 像素值Exy使用以下值並利用式⑺而求 ^象素之像素仏,對比度係數(於此,為視覺化對象 -I之對比度寬度之相關係數)rc ’將帶通濾波器處理 」之1衫像之注目像素的像素值Α”除以255而標準化 =值k由輪出受理部71戶斤取得(或預先記憶於記憶 L、並且導出注目像素之像素值的攝影it件411之相對 射強度之最大值Rknux及最小值Rk基於圖4之靈敏度 3_發明說明書(補件)/95-11/95127465 20 1311643 資訊61而取得的函數fs(參照式(3)),以及背景值b r Η,1 +1、 ⑺ kmin...(6) 瞀ί I!) Table: The following situation: As the high-pass filter processing, the second port of the operation uses the pixel-centered sides and the length (2s2 + anamorphic square window) As described above, the low-pass filter processing is performed on the first video of the original image of the IV image in the m processing unit 72, and the band-pass filter processing in the specific spatial frequency band is performed by the real-nine pass filter processing (step). S16) When the chopper processing unit 7 ? Φ # ϊ田# i processes the σ beam, the contrast enhancement process is performed by the contrast enhancement sub-image, thereby generating a strong image (the step is to emphasize the image) The pixel value Exy located in the coordinate (x, y) uses the following values and uses the equation (7) to find the pixel 仏 of the pixel, and the contrast coefficient (here, the correlation coefficient of the contrast width of the visualization object -I) rc ' By dividing the pixel value Α of the pixel of interest of the one-shirt image of the band-pass filter processing by 255 and normalizing = the value k is obtained by the round-out receiving unit 71 (or pre-memorized in the memory L and deriving the pixel of the pixel of interest) The maximum value of the relative radiation intensity of the value of the photographing piece 411 Rk The nux and the minimum value Rk are based on the sensitivity of the figure 3_ invention specification (supplement)/95-11/95127465 20 1311643 information 61 obtained by the function fs (refer to equation (3)), and the background value br Η, 1 +1 , (7) kmin
Cvv-R 其中 ^"IcmaY -R- kmin 本實施形態中’對比度係數r。為0.05,背景值127。 又,因第3影像為壓縮影像,故實際上多個攝影元件^1 對應於注目影像,但利用式(7)運算時,使用任一攝影元 件411之相對反射強度的最大值^及最小值再 者’使像素值E”量子化時,值小於〇之情形,像素值l 為0 ’值大於255之情形’像素值Exy為255。 式⑺中’自原影像導出之第3影像之各像素的對比戶 係數η乘以由實質上為原影像之第(影像之對應的像; 的像素值Axy導出的靈敏度,藉此對第3影像之各像 施取得原影像時之靈敏度越高程度越小的對比度強調。、亦 7 ’對比度強調部73中’藉由與靈敏度相應變更相 =影像之各像素之對比度強調的程度,於強卿像中容 i权正原減中之靈敏度依存於膜厚而變化之影塑(降 :二Γ摄,⑺中,第3影像之各像素之像素值❹與 對應的攝影元# 411相應之相對反射強度之最大值 ::來校正’故亦可同時校正多個攝影元件4Π 特性不同之影響。 J出 當對比度強調處理結束,則由圖5所示之評估值算出部 31書(補件)/95-1 〗/95127465 21 1311643 74對強調影像進行特定運算處理,關於膜厚不均散佈於 基板9之整個表面之整體膜厚不均、膜厚不均部分地存在 於基板9上之一部分之部分膜厚不均、及線狀膜厚不均產 生於列方肖或行方向之條紋狀膜厚不均之各種膜厚不 均’使膜厚不均之程度(所謂膜厚不均強度)量化,並算出 乍為表示自@ 5周景象導出之膜厚不均之程度(振幅程度) 的值的評估值(步驟S18)。 乂而膜92對於特定波長之光的反射率,如圖1所示, 1對於臈厚具週期性地變動,如剛參照圖1及圖2所說明 二於反射率之最大值附近及最小值附近,靈敏度變得非 常小。因此,膜92之厚度為靈敏度變得微小之膜厚的附 近(亦即’包含於死帶)時’所取得之原影像中像素值幾乎 未變二動’臈厚不肖(亦即,膜厚之變動)之檢測之精度降低。 :假=基板9上之膜92之厚度於死帶中變動,則僅根據 該特定波長而要高精度地檢測此種膜厚不均甚為困難。因 鲁2膜厚不均檢查裝置丨中,如上所述將丨個光學渡波器 作為選擇光學濾波器51a,並進行將該選擇光學濾波器 Ha之透過波長作為特定波長之上述步驟sn〜si8的處 卯f ( V驟S1 9),藉由控制部8使波長切換機構5之濾波 =%轉馬達53驅動從而使濾波器轉盤52旋轉,使其他光 w皮器51配置於自基板g至受光單元4之光路上並變 ^波長切換機構5中之特定波長(步驟S2〇)。藉由變更特 疋波長,如圖2所示,膜厚之死帶亦移動。 之後,藉由移動機構21使平台2返回至檢查開始位置, 31助發明說明書(補件祕⑵你 1311643 並再次開始平台2 $ & & / μ t 1 φ ., 移動(步驟S11)。在膜厚不均檢查裝 接受來自光束位置為止’攝影部41 次進行膜厚不均檢列時t基;9反射的反射光中與第1 移動同牛拍拓费:寺不同之特定波長之光,與平台2之 射光的二庚人取得來自基才反9上之線狀照射區域之反 卜知X刀佈’發送至膜厚不均檢測部7後,平台2停 止移動(步驟S12〜S15)。 1 並且’對壓縮在變更德 a 原影像的第1影像,進ϋ 長之干涉光中所取得的 ςι 仃特疋空間頻帶之帶通濾波器處理 理並m田少對度強部73進行對比度強調處 妁夕,处枯^止 )异出強調影像中之膜厚不 ^之评估值(步驟Sl8)。當變更後之特定波長中 SU〜S18的處理結束時(牛驟 " 卞〇驟S19)’使與第1次及第2次 之處理不同之進而其他光皋啸 為伞一 “, 元予,慮波器51配置於自基板9至 =二的光路上並變更特定波長(步驟_,重複步 驟S11〜S18的處理。 膜厚不均檢查裝置1中, 袖、泰f E “ 右將5個光學濾波器51之各 個透過波長作為特定波長重 陇以0、, 反负重複步驟S11〜S18的處理(步 旦9) ’則選擇使用5個光學遽波器51所分別取得之5 個原衫像中與基板9上之膜g 2 f ^ , s 腰W之特定區域(相當於顯示裝 中之』不面的區域)對應的部分中所 Π準偏差較大的2個原影像作為對比度較2 : ^對比度較高之原影像之選擇亦可藉由其他方法而進 312XP/發明說明書(補件)/95-11/95127465 23 1311643 繼而’對於該等2㈣影像所取得之膜厚不均之評估值 中^較大值與特定臨限值相比較。並且,若該值大於臨限 值時於基板9上之膜92存在超過所允許範圍之膜厚不均 (以下’稱為「膜厚不均缺陷」)則檢測膜厚不均缺陷.若 該值為臨限值以下時於基板9上之膜犯未存在超過所允 許範圍之膜厚不均(膜厚不均缺陷)(步驟如),則結 用臈厚不均檢查裝置1進行的臈厚不均的檢查處理、: 再者:對與基板9相同份額(lot)之其他基板(亦即,認 之厚度與基板9相同之基板)繼續進行膜厚不均之檢 η’僅將與作為對比度較高者而選擇之2個影像相 進〜學滤波器51的各個透過波長作為特定波長 ? 〜S18的處理(下述第2實施形態中相同)。 4時’於基板9在X方向之往返移動的去路上將直中一 :光=器51之透過波長作為特定波長,一邊取得影 像一邊异出评估值(步驟S19);於基板9之回路上, 之透過波長作為特定波長進行同樣的處 ,,^ 】】〜S19)。然後’ 2個波長中所取得之評 測(步驟與臨限值相比較,進行膜4不均缺陷之檢 圖9係表示與各光學遽波器以相對應之波長之干涉光 的靈敏度與膜厚之關係的 長中之靈敏度與膜厚之關係的線上重中疊長:二 最:在各膜厚中根據特定標準而選擇之2個波二表;; 固’長之選擇標準’例如,於可能的範圍不屬於死帶,且, 312XP/_ 說明書(補件)/95-11/95127465 24 1311643 之靈敏度之傾斜為彼此相反者等。如上所述, 、=檢查袋置1中選擇有與原影像中膜92之特定區 =之部t的像素值的標準偏差較大的2、個波長:該; 對2 /之膜厚不均之評估值係判斷有無膜厚不均缺陷的 亦叮箱t已知基板9之膜92之大概厚度時,如圖9所示, 最好各膜厚中選擇的2個波長,根據膜92 、古县2度特難定所使用之2個波長並分別僅將該等 波長作為特定波長進行上述處理。 人’就對測試影像進行與上述膜厚不均檢測部7相同 2理之情形加以敍述。首先’準備表示具有延伸於特定 向之條紋狀膜厚不均之基板上的膜的M列M行的膜厚 ^均影像。使膜厚不均影像中屬於同—列之像素之亮度為 目同’並將未包含膜厚不均成分及雜訊成分之基板上之理 〜=臈的固疋厚度(亦稱為背景膜厚)設為β,將膜厚不均 之:度5又為au’將膜厚不均之波長設為又u,將自膜厚不 :Ty像之第1列至第μ列之列號碼設為”將膜厚不均影 象之中央之列號碼设為yc,使用6 5 〇 nm之波長之干涉光 中的式(1)的函數5並利用式(8)求出表示包含膜厚不均 的膜厚不均影像的相對反射強度Gs。實際上,膜厚不均影 像係僅包含1個週期之膜厚不均者。Cvv-R where ^"IcmaY -R- kmin in the present embodiment 'contrast coefficient r. It is 0.05 and the background value is 127. Further, since the third image is a compressed image, actually, the plurality of imaging elements ^1 correspond to the attention image, but when calculating by the equation (7), the maximum and minimum values of the relative reflection intensities of any of the imaging elements 411 are used. Furthermore, when the pixel value E is quantized, the value is smaller than 〇, and the pixel value l is 0'. The value of the value is greater than 255. The pixel value Exy is 255. In the equation (7), each of the third images derived from the original image The contrast factor η of the pixel is multiplied by the sensitivity derived from the pixel value Axy of the image corresponding to the image (the corresponding image of the image), thereby increasing the sensitivity of the original image for each image of the third image. The smaller the contrast is emphasized, the 7 'contrast emphasis section 73' is based on the sensitivity of the phase change = the contrast of each pixel of the image, and the sensitivity of the strong image in the strong image is dependent on Film thickness and change of shadow (fall: two shots, (7), the pixel value of each pixel of the third image ❹ and the corresponding maximum intensity of the corresponding reflection intensity of the corresponding photographic element # 411:: to correct 'may also Simultaneous correction of multiple photographic elements 4Π When the contrast enhancement processing is completed, the evaluation value calculation unit 31 (supplement)/95-1 〗 / 95127465 21 1311643 74 shown in FIG. 5 performs specific arithmetic processing on the emphasized image, regarding the film thickness. The uneven thickness of the entire film which is unevenly spread over the entire surface of the substrate 9 and the unevenness of the film thickness partially present on a part of the substrate 9 are uneven, and the unevenness of the linear film thickness is generated in the column or the line The film thickness unevenness of the stripe film thickness in the direction is quantified, the degree of film thickness unevenness (so-called film thickness unevenness intensity) is quantified, and 乍 is calculated to indicate the degree of film thickness unevenness derived from the @5 week scene. The evaluation value of the value of the (amplitude level) (step S18). The reflectance of the film 92 for light of a specific wavelength is as shown in Fig. 1, and the periodic variation of the thickness of the film is as described with reference to Fig. 1 and 2 shows that the sensitivity is extremely small near the maximum value of the reflectance and the minimum value. Therefore, the thickness of the film 92 is near the film thickness where the sensitivity is small (that is, when it is included in the dead band). The pixel value in the original image obtained is almost unchanged. The accuracy of the detection of the discreet (that is, the variation of the film thickness) is lowered. False = the thickness of the film 92 on the substrate 9 varies in the dead band, and the film thickness is not accurately detected based on the specific wavelength. It is very difficult. In the Lu 2 film thickness unevenness inspection device, as described above, an optical wave filter is used as the selection optical filter 51a, and the transmission wavelength of the selective optical filter Ha is made as the specific wavelength. In the steps nn to si8, 卯f (V step S1 9), the control unit 8 drives the filter=%-turn motor 53 of the wavelength switching mechanism 5 to rotate the filter disk 52, and arranges the other light wrapper 51 on The specific wavelength in the wavelength switching mechanism 5 is changed from the substrate g to the optical path of the light receiving unit 4 (step S2). By changing the characteristic wavelength, as shown in Fig. 2, the dead band of the film thickness also moves. Thereafter, the platform 2 is returned to the inspection start position by the moving mechanism 21, and the instruction manual (Supplement Secret (2) 1311643 is restarted and the platform 2 $ && / μ t 1 φ . is moved again (step S11). In the case where the film thickness unevenness inspection package receives the position from the beam position, the imaging unit 41 performs the film thickness unevenness detection 41 times, and the 9-reflected reflected light is different from the first movement. The light, and the two Geng people who are irradiated with the platform 2 obtain the anti-discovering X-knife from the linear irradiation area on the base 9 and send it to the film thickness unevenness detecting unit 7, and then the platform 2 stops moving (step S12~) S15). 1 and 'Bypassing the band-pass filter processing of the ςι 仃 疋 疋 疋 疋 变更 变更 变更73, the contrast is emphasized, and the evaluation value of the film thickness in the image is emphasized (step S18). When the processing of SU to S18 is completed at the specific wavelength after the change (the bolus " step S19)', the other light is different from the processing of the first and second times, and the other light is screamed as an umbrella. The wave filter 51 is disposed on the optical path from the substrate 9 to the second and changes the specific wavelength (step _, the processing of steps S11 to S18 is repeated. In the film thickness unevenness inspection device 1, the sleeve, the Thai f E "right 5 Each of the optical filters 51 has a transmission wavelength of 0 as a specific wavelength, and repeats the processing of steps S11 to S18 by an inverse step (step 9). Then, 5 originals obtained by using the five optical choppers 51 are selected. Two original images with a large deviation from the portion corresponding to the specific area of the film g 2 f ^ , s waist W on the substrate 9 (corresponding to the area in the display device) are used as contrast 2: ^The choice of the original image with higher contrast can also be entered into the 312XP/invention manual (supplement)/95-11/95127465 23 1311643 by other methods, and then the film thickness unevenness obtained for the 2 (four) images The larger value of the evaluation value is compared with the specific threshold value, and if the value is greater than the threshold value When the film 92 on the substrate 9 has a film thickness unevenness exceeding the allowable range (hereinafter referred to as "film thickness unevenness defect"), the film thickness unevenness defect is detected. If the value is less than the threshold value, the substrate 9 is used. If there is no film thickness unevenness (film thickness unevenness defect) exceeding the allowable range (the step is as follows), the thickness unevenness inspection device 1 is used to check the thickness unevenness inspection: : The other substrate (i.e., the substrate having the same thickness as the substrate 9) which is the same as the substrate 9 is continuously subjected to the detection of the film thickness unevenness η', and only two selected as the higher contrast ratio Each of the transmission wavelengths of the image-to-sense filter 51 is a specific wavelength ~S18 (the same as in the second embodiment described below). At 4 o'clock, the path of the substrate 9 in the X direction is straight. : The transmission wavelength of the light=the device 51 is a specific wavelength, and the evaluation value is obtained while acquiring the image (step S19); on the circuit of the substrate 9, the transmission wavelength is the same as the specific wavelength, ^]]~S19) . Then, the evaluation obtained in the two wavelengths (the step of detecting the unevenness of the film 4 compared with the threshold value is shown in Fig. 9 is the sensitivity and film thickness of the interference light at the wavelength corresponding to each optical chopper. The relationship between the sensitivity of the relationship and the film thickness of the relationship between the length and the length of the film: two most: two wave two tables selected according to specific criteria in each film thickness;; the selection criteria of solid 'long', for example, The possible range is not a dead band, and the inclination of the sensitivity of the 312XP/_ specification (supplement)/95-11/95127465 24 1311643 is opposite to each other, etc. As described above, the check bag is set to 1 and has The specific area of the film 92 in the original image = the standard deviation of the pixel value of the part t is 2, the wavelength is: the evaluation value of the film thickness unevenness of 2 / is judged whether there is any film thickness unevenness defect When the thickness of the film 92 of the substrate 9 is known in the case t, as shown in FIG. 9, it is preferable to select two wavelengths of the respective film thicknesses, and according to the two wavelengths of the film 92 and the ancient county, it is difficult to determine the two wavelengths. The above-described processing is performed only by using the same wavelength as a specific wavelength. The person's test image is performed with the above film. The case where the unevenness detecting unit 7 is the same is described. First, the film thickness of the M rows and M lines having the film extending on the substrate having the stripe film thickness unevenness is specified. In the average image, the brightness of the pixels belonging to the same column is the same as that of the substrate on the substrate which does not include the film thickness unevenness component and the noise component, and the solid film thickness (also referred to as the background film thickness) is set to β, the film thickness is uneven: the degree 5 is au', the wavelength of the film thickness unevenness is set to u, and the film thickness is not: the number of the first column to the μ column of the Ty image is set to "will The center line number of the film thickness unevenness image is yc, and the film containing the film thickness unevenness is obtained by the equation (8) using the function 5 of the equation (1) in the interference light of the wavelength of 65 〇 nm. The relative reflection intensity Gs of the thickness unevenness image. Actually, the film thickness unevenness image system only includes the film thickness unevenness of one cycle.
Gs=fR^B + ^(c〇s(^(y.(yc 2 (8) 然後’使式(8)所示之膜厚不均影像之各像素加上雜訊 312沿/發明說明書(補件)/95-11/95127465 25 Ϊ311643 用ns將雜訊成分大小之標準偏差設為 n亚使用0.0〜1.0之亂數rnd以式(9)表 65〇nm之波長之,、 後作為 我之卞,步先中的測試影像而準備。 ns V~^l°Se(l ~-nid} · sin(2x · md) ’…(9) 如此,測試影像簡化為背景膜厚、膜厚不均及雜气 ^備有組合各種背景膜厚及膜厚不均深度之多個測試影 。實際上’測試影像之大小為12〇〇χ12〇〇像素⑻ 中之膜厚不均之波長λ A . ”式(8) 之沪!&兰士 "為64,式(9)中之雜訊成分大小 之“準偏差ση為1.〇。 ^測試影像轉換為8 bit之原影像後,❹式⑷以$ 像素X、像素之範圍為單位實施壓縮處理,從而取ι 為4。繼而,對第1影像使用 式(5)並實施低通濾波器處理取得第2影像後,藉由 2影像實施使用式⑻之高通濾波器處理,來取得第b 像。並且’藉由對第3影像實施使用式⑺之對比度強調二 取得強調影像。再者’式⑺中,相對反射強度之最大值 及最小值Rkmin利用任意攝影元件411中者,對比产 數 r。為 〇.〇5。 ,、 此處’如式(1 〇)所示’分別對各強調影像中所有列,求 出像素值與背景值b之差之絕對值的、屬於該列的多個像 素中的平均值除以背景值b的值,並將最大值作為相對檢 測強度m。而算出,_L述相對檢測強度m。係相對於條紋狀 膜厚不均之評估值。此處,f景值b與式⑺同樣為⑵, 312XP/發明說明書(補件)/95-11/95127465 26 1311643 hei及wid分別為m/4 wid b xy max- (l,hei) = Σ|ε b.Wld -(10) 上述處理將膜厚不均深度變更為卜2、5、、別 100 nm’針對各财不均深度,分料㈣. 個值之多個測試影像進行上述虛 、 為各 同處取得相對檢測強度。 圖10 #、表示自多㈣料彡像所取得之相對 >對於背景膜厚變化的圖。又,圖 又相 !。之比較例,於上二二強=示作為相對於圖 k町比度強5周處理中,將式(7)中之 f机Μ定設為!時(亦即,使對比度強調 斤取得之相對檢測強度相對於背景膜厚變: 的圖。再者’目Η)及圖U(以及,下述圖⑵中,將值為 以上之相對檢測強度作為1來圖示。 景:周:度固定時,如圖11所示,對於例如背 mId / nm深度之膜厚不均之相對檢測強度 =,0.2’即使於背景膜厚刪⑽附近為5Qnm深度 ㈣㈣強度檢測均為以下。此係因為 :又#於膜厚變化,此時,難以高精度地取得膜厚不 =”此相對’將對比度強調程度對應於靈敏度變更時, 所示’對於膜厚不均深度小於5_之膜厚不均, 于 卜’相對檢測強度相對於膜厚之變化大致平坦化 (幾乎為固定)。 '厚不均檢查裳置i中,因利用如上所述之5種波長之 312XP/發明說明書(補件)/95 11/95ΐ27465 η 1311643 干涉光’故藉由選擇有忒呰旦 之屌岑後“上 纟“、臈厗申較佳波長之干涉光令 ^像,並對該原影像進行將對比度強調 =:變更的處理,如圖〗2所示,各膜厚不均深;中: 對檢測強度相對於臈厚之變化進而平坦化。圖12中, 日二1下之膜厚不均深度中’相對檢測強度大致固定並 ^對檢測強度與膜厚不均深度大致成比例,· 20及50 nm =二:不均深度中’相對檢測強度之最大值為最小值 右且相對檢測強度之變動寬度變小。又,100nm ^膜=均殊度中’大部分f景膜厚中相對檢測強度飽 I疋,故可謂能檢測膜厚不均。 ,10至圖12中之各膜厚不均深度之相對檢 於背景膜厚變化中,Μ於咎旦胳后^ η 旦旦 子於h膜尽的砣圍的整體(準備有 川忒衫像之月厅、膜厚之全範圍)的比率(以下,稱為「 :測範圍之比率」)表示於λ i,上述背景膜厚^ 2厚不均深度中之相對檢測強度之平均值,強 度細範圍内者。再者,如上所述,圖u在單一: 中所取得,表示未進行靈敏度變化之影響之校正的、 的相對檢測強度;圖1G在單—波長中所取得,表 靈敏度變化之影響之校正後的影像㈣相對檢測強度;S 12係由自多個波長與膜厚相應而選擇之波長中所取得 者’表示進行靈敏度變化之影響之校正後的影像中的相 铋測強度,表1中’將表示圖u中之穩定檢測範圍之比 率的項目名表示為「未進行校正之情形」,將表示圖10中 之穩定檢測範圍之比率的項目名表示為「進行校正之情 312XP/發明說明書(補件)/95-11/95127465 28 1311643 形」將表不圖12中之穩定檢測範圍 示 盔「、社,e 礼因 < 此旱的項目名表 為「進行波長選擇及校正之情形」。 衣 表1 未進行校正之情形 — 進行校正之情形 進行波長選擇及校正之情形 gjl·不均深度[η 79 ----- | | fu ° 00 4 8 8 9 5 如表1所示’ 靈敲 =二響’相對檢測強度為較大不均-之膜厚範圍大幅J 減> (亦即,穩定檢測範圍之比率增大)。又,可知, 之”並自多個波長對應於膜厚選㈣ 穩定檢測範圍之比率約為9Q%,並可於更廣膜 厗辄圍中進行高精度的膜厚不均之檢測。 -' 产!說明’膜厚不均檢查裝置1中,藉由參照靈敏 又貝讯61及原影像之各像素之像素值,容 ^ H#41中·^原影像時靈敏度依存於膜厚而變化之^ ;作為膜像導出之影像中之特定空間頻帶的振幅程 可=度地檢查基板9上 •^联y予不均。又’可實現,藉 均檢測部7中對自原影像導出之第3影像之各像辛進Γ盘 2應=影元彳411相應之㈣靈敏度變化^校 二亦可同時校正多個攝影元件411間之輸出特性不二 又’亦可於膜厚不均檢查裝置1中,僅使用2、3或4 312XP/__書(補件)/95-11/95127465 29 1311643 個光學濾波器51,且圖8之步驟S19、S2〇中,於特定波 長彼此不同之2、3或4種波長間切換,並重複步驟S11 〜S18(下述第2實施形態中亦同樣)。藉此,可實現,於 膜厚不均檢查裝置1中,比上述處理例更高速地進行膜厚 不均檢查處理,上述處理例係使用5個光學濾波器51重 複5 -人基板9向X方向之移動,從而於膜之厚度之較廣範 圍内高精度地檢查膜厚不均。 圖13係表示第2實施形態之臈厚不均檢查裝置la之結 鲁構的圖。圖13之膜厚不均檢查褽置la係於圖5之膜厚不 均檢查裝置1中追加例如白色干涉式膜厚測量部丨丨者。 膜厚測量部11可藉由測量部移動機構12向沿基板9之主 面之圖13中γ方向移動。其他結構與圖5之膜厚不均檢 查裝置1相同,因此賦予相同符號。 圖14係表示膜厚不均檢查裝置la檢查基板9上之臈 92之膜厚不均的處理流程的一部分的圖,其表示於圖8 鲁中之步驟S10與步驟S11之間進行的處理。膜厚不均檢查 裝置la檢查基板9上之膜92之膜厚不均時,作為事前準 備,準備表示靈敏度與膜厚關係之靈敏度資訊61a並記情 於記憶部6(圖8:步驟S1〇)。於此,本實施形態中,靈 敏度資訊61a如圖2所示,係表示各個多個光學遽波器 51中之透過波長之干涉光的靈敏度與膜厚的關係者(直 中,圖2表示僅3種透過波長之靈敏度與膜厚之關係/、 繼而,控制移動機構21及測量部移動機構12,並使臈 厚測量部11之測量位置一致於基板9上之膜92的特定位 312XP/發明說明書(補件)/95-11/95127465 3〇 1311643 置,取得該位置上之膜92之 測量於基板9上之膜92中夫/士驟S31)。實際上, 上之膜92中大致一樣地 如,25點)的膜92的厚直(夕個位置(例 夕Μ η 予度仗而取得膜92之厚度之分佈。 半二2門2移動機構21平台2返回至檢查開始位置, 二=移動(圖8:步驟su)。膜厚不均檢查裝置h 中丄兵平。2之移動同步,藉由 :=並反覆取得來自基板9上之線狀照射區域;;= 的強度为佈,當平台2到 之移動(步驟Sl2〜S15)。 °束位置時1止平台2 於膜厚不均檢測部7中壓縮原影像後,對於作為 壓縮後之原影像之第i畢—麥促対於作為 波器處理,從而取得第間頻帶的帶通遽 比度強調處理從而生成;步:S16) ’之後’進行對 利用膜厚測量部i i =,:像(步驟S17)。此時’根據 於注目像♦的 仵之膜92之厚度的分佈導出對應 表干靈敏μ ㈣92的厚度,根據該厚度藉由參照 = = 係之靈敏度資…獲得的靈 換η(崎:用;且之注二,^^ 評估值(步驟厚不均在強調影像中之 右於膜厚不均檢魯扭¥, 各個透Μ 將⑽料缝⑽之 (牛驟ςι〇乍為特疋波長重複步驟S11〜S18之處理 :之5個原::中則f使用5個光學濾波器51所分別取 於节等擇有對比度較高的2個原影像,對 於以2個原影像所取得之膜厚不均之評估值中,較大值 3咖_說明書_)/95 11/9512· 31 1311643 與特定臨限值相比較。然後,該值切臨限值時,在 9上之膜Θ2存在超過所允許範圍之膜 土 不均缺陷;該值為臨限值以下時λ _、&測膜厚 . 丁牡巷板9上之膜去 ,在^斤允許範圍之膜厚不均(步驟㈣心 ;不均檢查裝置la進行的膜厚不均的檢查處理 、 ^圖9所示’預先蚊最好於各膜厚中而選擇之2個波長 時’根據於所取得之膜92之厚度可特別指 、 ^波長,並分別僅將該等波長作㈣定波㈣行上= 如以上所說明,圖13之膜厚不均檢查裝置_ :!严:之厚度及靈敏度資訊6卜容易地校正取得“影 之原影像時靈敏度依存於膜厚變化之影響,並將 二、影像導出之影像中之特定空間頻帶的 膜::均而檢測。藉此,可高精度地檢查基板9上所= 之之膜厚不均。再者,亦於膜厚不均檢查裝置la中, ^於元件411準備表示靈敏度與膜厚之關係之表 專,於膜厚不均檢測部7中,對於自原影像導出之第& 像之各像素,進行與撕庫之摄旦y — 年’ 度變化的影響的1Γ!攝“件411相應之個別靈敏 定二ί二:發明之實施形態加以說明,但本發明並非限 疋於上述實施形態者,可有各種變形。 上述第1及第2實施形態中,為使干涉光之強度一般化 =:強:用射入光之強度為1時之干涉光的強度、即相 射強度進行了說明,但因特定波長之相對反射強度與 312XP/發明說明書(補件)/95·11/95ΐ27465 ^ 1311643 度:解a 4 '歩光的強度實質上係相同含義’故可將靈敏 I寺定波長之干涉光之強度變動對膜厚變動的比 L::::上述第1實施形態中之靈敏度資…示靈 又/、寺疋波長之干涉光之強度的關係。 根=辛41 原影像之各像素’ 值(或者,根據膜92對應位置的厚度)參照靈敏 二二去出對應的靈敏度’並將與該靈敏度相應之係數乘 :素值’取得使$敏度變化之影響降低之影像亦可。 2時,對於原影像之各像素進行與對應之攝影元件411相 ;::固:靈敏度變化的影響的校正。然後,藉由僅使帶通 亥影像,使表示特定空間頻帶之振幅程度之 不:的檢測結果而輸出。此時,膜厚不均檢 獨立的處理而進行,並利;表干%二::對比度強調處理 和用表不原影像中之特定空間頻帶 振幅之程度的影像來檢測膜厚不均。如上所述,當 =敏度依存於膜厚變化之影響,一邊將原影像或自原影 影像中之特定空間頻帶振幅的程度作為膜厚不 均而檢測,則既於膜展兀从、如 %膜厚不均檢測部中進行各種處理,膜 不均之檢縣果亦可為除評估值料表㈣均 影像。 j <Gs=fR^B + ^(c〇s(^(y.(yc 2 (8) Then 'make each pixel of the film thickness unevenness image shown by the formula (8) plus the noise 312 edge/invention specification ( Supplement) /95-11/95127465 25 Ϊ311643 Use ns to set the standard deviation of the noise component size to n. Use 0.0~1.0 random number rnd to the wavelength of 65〇nm of equation (9), and then as me Then, prepare for the test image in the first step. ns V~^l°Se(l ~-nid} · sin(2x · md) '...(9) Thus, the test image is simplified to the background film thickness and film thickness. Both the heterogeneous and the heterogeneous gas have a plurality of test shadows combining various background film thicknesses and uneven thicknesses of the film thickness. Actually, the size of the test image is 12 〇〇χ 12 〇〇 pixels (8), and the film thickness is uneven λ A The "quasi-deviation ση of the size of the noise component in the equation (8) is 64. The amplitude of the noise component in the equation (9) is 1. 〇. ^ After the test image is converted into the original image of 8 bits, The formula (4) performs compression processing in units of a range of pixels X and pixels, thereby obtaining ι of 4. Then, using the equation (5) for the first image and performing low-pass filter processing to obtain the second image, the second image is obtained by 2 Image implementation using the height of (8) The filter process is performed to obtain the b-th image, and 'the emphasized image is obtained by using the contrast enhancement 2 of the equation (7) for the third image. Further, in the equation (7), the maximum value and the minimum value Rkmin of the relative reflection intensity are used for arbitrary photography. In the element 411, the comparison yield r is 〇.〇5. , and here, as shown in the equation (1 〇), respectively, for each column in each emphasized image, the difference between the pixel value and the background value b is obtained. The absolute value of the average of the plurality of pixels belonging to the column is divided by the value of the background value b, and the maximum value is used as the relative detection intensity m. The relative detection intensity m is calculated as _L. The evaluation value of the unevenness. Here, the f-value b is the same as the formula (7), (2), 312XP/invention specification (supplement)/95-11/95127465 26 1311643 hei and wid are m/4 wid b xy max- ( l,hei) = Σ|ε b.Wld -(10) The above treatment changes the film thickness unevenness depth to 2, 5, and 100 nm' for each financial uneven depth, and the material is divided (4). The test images are subjected to the above-mentioned imaginary, and the relative detection strengths are obtained for the same place. Fig. 10 #, which is obtained from the multiple (four) material image The relative image of the background film thickness change. In addition, the figure is again! In the comparative example, the upper two and two strong = show as a strong comparison with the figure k, 5 weeks of processing, in the formula (7) When the f-machine setting is set to ! (that is, the contrast detection intensity obtained by the contrast emphasis is changed with respect to the background film thickness: in addition to the 'visual view' and the figure U (and, in the following figure (2), The relative detection intensity of the above value is shown as 1. Scene: Week: When the degree is fixed, as shown in Fig. 11, the relative detection intensity of the film thickness unevenness such as the back mId / nm depth = 0.2', even if the background film thickness is deleted (10), the depth is 5Qnm (four) (four) the intensity test is the following. This is because the thickness of the film is changed. In this case, it is difficult to obtain the film thickness with high precision. "This relative" corresponds to the change in sensitivity when the contrast is emphasized. The thickness of the film thickness is less than 5 mm. The thickness of the film is not uniform, and the relative detection intensity is substantially flat (almost fixed) with respect to the change in film thickness. 'The thickness unevenness is checked in the case i, because the five wavelengths of the above-mentioned 312XP/invention specification are utilized. (supplement) /95 11/95ΐ27465 η 1311643 Interfering light', so by selecting the "upper", the best wavelength of the interference light, and the original image Contrast emphasis =: change processing, as shown in Fig. 2, the thickness of each film is not uniform; medium: The detection intensity is flattened with respect to the change in thickness. In Fig. 12, the film thickness of day 2 is not In the mean depth, the relative detection intensity is approximately fixed and the detection intensity is approximately proportional to the depth of the film thickness unevenness. · 20 and 50 nm = two: the maximum value of the relative detection intensity in the uneven depth is the minimum value and the relative detection The variation width of the intensity becomes smaller. Also, 100 nm ^ film = uniformity 'Most of the thickness of the film is relatively high, so it can be detected that the film thickness is uneven. The relative thickness of each film thickness in 10 to 12 is detected in the background film thickness change. The ratio (hereinafter, referred to as "the ratio of the measurement range") of λ 旦 旦 ^ 于 于 于 于 于 于 于 于 h h h h λ λ λ λ λ λ λ λ λ λ λ λ λ λ λ λ λ i, the average of the relative detection intensities in the above-mentioned background film thickness ^ 2 thickness unevenness depth, and the intensity is within a fine range. Further, as described above, the graph u is obtained in a single: indicating the relative detection intensity of the correction without the influence of the sensitivity change; FIG. 1G is obtained in the single-wavelength, and the influence of the change in the sensitivity of the table is corrected. (4) Relative detection intensity; S 12 is the phase-measured intensity in the image obtained by correcting the influence of sensitivity change from the wavelength selected from the multiple wavelengths and the film thickness, in Table 1 ' The item name indicating the ratio of the stable detection range in the graph u is expressed as "the case where the correction is not performed", and the item name indicating the ratio of the stable detection range in Fig. 10 is expressed as "the correction 312XP/invention specification ( The patch) /95-11/95127465 28 1311643 will not show the stable detection range in Figure 12, "she, e, et al." This dry item name list is "the case of wavelength selection and correction". Closing table 1 is not corrected - the case of wavelength correction and correction in the case of correction gjl · uneven depth [η 79 ----- | | fu ° 00 4 8 8 9 5 as shown in Table 1 'Ling Knock = two rings' relative detection intensity is large unevenness - the film thickness range is greatly reduced by J (that is, the ratio of the stable detection range is increased). Further, it can be seen that the ratio of the plurality of wavelengths corresponding to the film thickness selection (four) stable detection range is about 9%, and high-precision film thickness unevenness can be detected in a wider film circumference. Product Description: In the film thickness unevenness inspection device 1, by referring to the pixel values of each pixel of the sensitive and the Bayer 61 and the original image, the sensitivity of the original image in the H#41 is changed depending on the film thickness. ^; The amplitude range of a specific spatial frequency band in the image derived from the film image can be used to check the substrate 9 on the surface of the substrate 9 to be uneven. Further, it can be realized, and the first detection unit 7 derives the image from the original image. 3 images of each image of the singular disk 2 should be = shadow 彳 411 corresponding (four) sensitivity change ^ school 2 can also simultaneously correct the output characteristics of multiple photographic elements 411 and can also be used in the film thickness unevenness inspection device In 1 , only 2, 3 or 4 312XP/__ book (supplement) / 95-11/95127465 29 1311643 optical filters 51 are used, and in steps S19 and S2 of Fig. 8, the specific wavelengths are different from each other. Switching between 2, 3 or 4 wavelengths, and repeating steps S11 to S18 (the same applies to the second embodiment described below). In the thickness unevenness inspection apparatus 1, the film thickness unevenness inspection process is performed at a higher speed than the above-described process example, and the above-described process example repeats the movement of the 5-man substrate 9 in the X direction by using five optical filters 51, thereby The film thickness unevenness is inspected with high precision in a wide range of thicknesses. Fig. 13 is a view showing the structure of the thickness unevenness inspection device 1a of the second embodiment. For example, a white interference type film thickness measuring unit is added to the film thickness unevenness inspection device 1 of Fig. 5. The film thickness measuring unit 11 can be moved to the main surface of the substrate 9 by the measuring unit moving mechanism 12 by γ. The other structure is the same as that of the film thickness unevenness inspection device 1 of Fig. 5, and therefore the same reference numerals are given. Fig. 14 is a view showing a process flow for inspecting the film thickness unevenness of the crucible 92 on the substrate 9 by the film thickness unevenness inspection device 1a. A part of the figure is shown in the process between step S10 and step S11 in Fig. 8. When the film thickness unevenness inspection device 1a checks the film thickness unevenness of the film 92 on the substrate 9, it is prepared as a preparation. Sensitivity information and film thickness sensitivity information 61a and remember The memory unit 6 (Fig. 8: Step S1). Here, in the present embodiment, the sensitivity information 61a indicates the sensitivity and film of the interference light of the transmission wavelength in each of the plurality of optical choppers 51 as shown in Fig. 2 . In the case of a thick relationship, FIG. 2 shows the relationship between the sensitivity of only three kinds of transmission wavelengths and the film thickness, and then controls the moving mechanism 21 and the measuring unit moving mechanism 12, and the measurement positions of the thickness measuring unit 11 are made uniform. The specific position 312XP of the film 92 on the substrate 9/invention specification (supplement)/95-11/95127465 3〇1311643 is taken, and the film 92 at the position is measured on the substrate 92 in the film 92. ). Actually, the film 92 in the upper film 92 is substantially the same as the thickness of the film 92 at 25 o'clock. (The position of the film 92 is obtained by 予 位置 予 予 。 。 。 。 。 。 。 。 。 。 。 。 半 半 半 半 半 半 半21 platform 2 returns to the inspection start position, and two = movement (Fig. 8: step su). The film thickness unevenness inspection device h is in the middle of the movement. The movement of the movement is synchronized by: = and repeatedly obtaining the line from the substrate 9. The intensity of the illuminating area;; = is the cloth, when the platform 2 moves (steps S1 to S15). At the beam position, the platform 2 is compressed in the film thickness unevenness detecting portion 7 and then compressed as the original image. The first image of the original image is processed by the waver to obtain the band pass ratio enhancement processing of the first frequency band, and is generated; step: S16) 'after' is performed on the utilized film thickness measuring unit ii =, : image (step S17). At this time, the thickness of the corresponding surface sensitive sensitivity μ (four) 92 is derived from the distribution of the thickness of the film 92 of the image of the image of the object ♦, and the spirit obtained by referring to the sensitivity of the reference == Change η (saki: use; and note 2, ^^ evaluation value (step thickness unevenness in the emphasis on the image to the right of the film Uneven inspection, twisting, and each of the (10) material slits (10) (the process of repeating steps S11 to S18 for the special wavelength: 5 originals:: medium f uses 5 optical filters 51 The two original images with higher contrast are selected from the section, and the larger the value of the film thickness unevenness obtained by the two original images, the larger value 3 coffee _ manual _) / 95 11 / 9512 · 31 1311643 compared with the specific threshold value. Then, when the value is cut to the limit value, the membrane defect 2 on the 9 has a membrane soil unevenness exceeding the allowable range; when the value is below the threshold value, λ _, & The thickness of the film is measured. The film on the plate of the Dingmu Lane is removed, and the film thickness is uneven in the allowable range of the kg (step (4) heart; the inspection of the film thickness unevenness by the unevenness inspection device la, ^ Figure 9 'When the pre-mosquito is preferably selected at two wavelengths of each film thickness', the thickness of the film 92 obtained may be specifically referred to as ^ wavelength, and only the wavelengths are (4) fixed wave (four) lines = As described above, the film thickness unevenness inspection device of Fig. 13 is _: strict: the thickness and sensitivity information 6 is easily corrected to obtain the sensitivity of the original image of the shadow The effect of the film thickness change is detected, and the film of the specific spatial frequency band in the image derived from the image is detected. The film thickness unevenness on the substrate 9 can be inspected with high precision. In the film thickness unevenness inspection device 1a, the element 411 is prepared to indicate the relationship between the sensitivity and the film thickness, and in the film thickness unevenness detecting portion 7, the image is derived from the original image. For each pixel, the effect of the change in the degree of change of the y y y y y y 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 The form can have various deformations. In the first and second embodiments, the intensity of the interference light is generalized: strong: the intensity of the interference light when the intensity of the incident light is 1, that is, the intensity of the incident light is described, but the specific wavelength is Relative reflection intensity and 312XP / invention manual (supplement) / 95 · 11 / 95 ΐ 27465 ^ 1311643 degrees: solution a 4 'the intensity of the 歩 light is essentially the same meaning', so the intensity of the interference light of the wavelength of the sensitive I Temple can be changed Ratio of film thickness variation L:::: The relationship between the sensitivity of the first embodiment and the intensity of the interference light of the temple wavelength. Root = Xin 41 original image of each pixel 'value (or, according to the thickness of the corresponding position of the film 92) with reference to the sensitivity of the second to remove the corresponding sensitivity 'and multiply the coefficient corresponding to the sensitivity: the prime value 'obtained to make the sensitivity Images with reduced effects of change can also be used. At 2 o'clock, each pixel of the original image is subjected to correction corresponding to the corresponding imaging element 411;:: solid: the influence of the sensitivity change. Then, by only taking the image with the pass, the detection result indicating the degree of the amplitude of the specific spatial frequency band is output. At this time, the film thickness unevenness detection is performed independently, and the surface dryness %:: contrast enhancement processing and image density of the specific spatial frequency band amplitude in the original image are used to detect film thickness unevenness. As described above, when the sensitivity is affected by the change in the film thickness, and the degree of the amplitude of the specific spatial frequency band in the original image or the original image is detected as the film thickness unevenness, the film is stretched out, for example. Various treatments are performed in the % film thickness unevenness detecting portion, and the inspection result of the film unevenness may be the image of the evaluation value table (4). j <
上述第1實施形態中,表示靈敏度與相對反射強度 係之靈敏度錢61並非必彡請料算求出,例如 準備各種膜厚之基板,並利用實際測量求出相對反射強戶 與膜厚之卿’亦可導出靈敏度與相對反射強度之關係T 312XP/發明說明書(補件)/95-11/95127465 1311643 進而’可將近似於圖4所示之靈敏度與相對反射強度之關 係的作為形狀的函數作為靈敏度資訊而取得,基於該函數 來靈敏度於校正原影像中變化的影響。此時,亦可於某種 程度校正依存於膜厚變化之靈敏度之影響。 ' 〃 上述第i及第2實施形態中’藉由變更對比度強調部 73中之對比度強調之程度,對於由攝影部41所取得之自 原影像導ii]之影像高料地特$敏度變化的影響的校 正,但如上所述,靈敏度變化之影響之校正作為自對比度 強調處理而獨立的處理而進行時,作為影像對比度之強調 處理’亦可部分使用上述日本專利第33355()3號公報之方 法。該方法中,對於原影像,利用中值滤波器進行平滑化 處理從而求出平滑化影像,並取 將原影像之各像素之料值㈣調影像 参i值除以干滑化影像之對應像素 值而強調出應檢測的膜厚不均強調。 一膜厚不均檢查裝置卜la中,藉由波長㈣機構5於受 光單元4之基板9側切換光學滤波器⑴使特定波長於 彼此不同之多個波長間切換,例如,於光照射部3設置有 :出彼此各不相同之單一波長之光的多個光源,藉由切換 :控制部8之控制而主動化的光源(亦即,藉由控制部8 作為切換機構),可使作為由攝影部41所接受之干涉光之 波長的特定波長於彼此不同的多個波長間切換。 =射出部t ’可代替石英棒32設置多個光纖排列為直 ,狀之光纖陣列’來自幽素燈31之光藉由通過光纖陣列 換為線狀光。又’可代替齒素燈31及石英棒32,將排 312XP/__書(補件)/95-11/95127465 34 1311643 $為直線狀之多個發光二級體作為射出線狀光之光源而 °又^ I =,攝影部41中,在必須縮短基板9之攝影時間 ^ ^形等時,亦可代替線感測器410設置有2維CCD感測 器。 保持基板9之保持部除與基板9之下表面抵接並支持基 板9之平台2以外,亦可係藉由把持例如基板9之外緣部 而保持基板9者等。 上述實施形態之膜厚不均檢查裝置亦可用於除光阻膜 以外之其他臈、例如基板9上所形成之絕緣膜或導電膜之 膜厚,均的檢測。又,膜厚不均檢查裝置亦可用於半導體 基板等其他基板上所形成之膜之膜厚不均的檢查。 …以上洋細描寫了本發明,但所述之說明係為示例並非限 疋者。因此,於未脫離本發明之範圍内,可有多種變形或 形態當可理解。 【圖式簡單說明】 圖1係表示膜之反射率相對於膜厚變化的圖。 圖2係表示靈敏度相對於膜厚變化的圖。 圖3係用以說明靈敏度與相對反射強度之間關係的圖。 圖4係表示靈敏度與相對反射強度之間關係的圖。 圖5係表示第1實施形態之膜厚不均檢查裝置之構成的 圖。 圖6係表示波長切換機構的圖。 圖7係表示攝影部之受光面的圖。 圖8係表示檢查基板上之膜之膜厚不均之處理流程的 3J1/95127465 35 1311643 圖。 ,圖9係表示多個波長之干涉光之靈敏度與膜厚之間關 係的圖。 圖10係表示相對檢測強度相對於背景膜厚之變化的 圖。 圖11係表示相對檢測強度相對於背景膜厚之變化的 圖。 圖12係表示相對檢測強度相對於背景膜厚之變化的 圖。 圖13係表示第2實施形態之膜厚不均檢查裝置之構成 的圖。In the first embodiment, the sensitivity 61 and the sensitivity of the relative reflection intensity are not necessarily calculated. For example, a substrate having various film thicknesses is prepared, and the relative reflection strong family and the film thickness are obtained by actual measurement. 'The relationship between sensitivity and relative reflection intensity can also be derived. T 312XP/Invention Manual (Supplement)/95-11/95127465 1311643 Further, a function similar to the relationship between the sensitivity and the relative reflection intensity shown in Fig. 4 can be obtained. Obtained as sensitivity information, based on this function, sensitivity is used to correct the effects of changes in the original image. At this time, the influence of the sensitivity depending on the change in film thickness can also be corrected to some extent. In the above-described i-th and second embodiments, the degree of contrast enhancement in the contrast enhancement unit 73 is changed, and the image of the original image guide ii obtained by the imaging unit 41 is highly sensitive. Correction of the influence of the effect, but as described above, when the correction of the influence of the sensitivity change is performed as an independent process from the contrast enhancement processing, the above-mentioned Japanese Patent No. 33355() No. 3 may be partially used as the emphasis processing of the image contrast. The method. In the method, the smoothed image is obtained by using a median filter to obtain a smoothed image, and the material value of each pixel of the original image is divided by the image value of the image and the corresponding pixel of the image of the dry-sliding image. The value emphasizes the uneven thickness of the film to be detected. In the film thickness unevenness inspection device, the optical filter (1) is switched by the wavelength (4) mechanism 5 on the substrate 9 side of the light receiving unit 4 so that the specific wavelength is switched between a plurality of wavelengths different from each other, for example, in the light irradiation portion 3. A plurality of light sources that emit light of a single wavelength different from each other are provided, and a light source that is activated by switching control of the control unit 8 (that is, the control unit 8 is used as a switching mechanism) can be used as a The specific wavelength of the wavelength of the interference light received by the imaging unit 41 is switched between a plurality of wavelengths different from each other. The injection portion t' can be provided in place of the quartz rod 32. The plurality of optical fibers are arranged in a straight line, and the optical fiber array from the nucleus lamp 31 is replaced by linear light through the optical fiber array. In addition, instead of the tooth lamp 31 and the quartz rod 32, the row 312XP/__ book (supplement)/95-11/95127465 34 1311643 $ is a linear plurality of light-emitting diodes as a light source for emitting linear light. Further, in the photographing unit 41, when it is necessary to shorten the photographing time of the substrate 9, etc., a two-dimensional CCD sensor may be provided instead of the line sensor 410. The holding portion of the holding substrate 9 may hold the substrate 9 by holding the outer edge portion of the substrate 9, for example, in addition to the lower surface of the substrate 9 and supporting the substrate 2 of the substrate 9. The film thickness unevenness inspection apparatus according to the above embodiment can also be used for detecting the thickness of the insulating film or the conductive film formed on the substrate 9 other than the photoresist film. Further, the film thickness unevenness inspection device can also be used for inspection of film thickness unevenness of a film formed on another substrate such as a semiconductor substrate. The invention has been described above in detail, but the description is by way of example and not limitation. Therefore, various modifications or forms are possible without departing from the scope of the invention. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a view showing a change in reflectance of a film with respect to a film thickness. Fig. 2 is a graph showing the change in sensitivity with respect to film thickness. Figure 3 is a graph for explaining the relationship between sensitivity and relative reflection intensity. Figure 4 is a graph showing the relationship between sensitivity and relative reflection intensity. Fig. 5 is a view showing the configuration of a film thickness unevenness inspection device according to the first embodiment. Fig. 6 is a view showing a wavelength switching mechanism. Fig. 7 is a view showing a light receiving surface of a photographing unit. Fig. 8 is a view showing a process flow for inspecting the film thickness unevenness of the film on the substrate, 3J1/95127465 35 1311643. Fig. 9 is a view showing the relationship between the sensitivity of the interference light of a plurality of wavelengths and the film thickness. Fig. 10 is a graph showing changes in relative detection intensity with respect to background film thickness. Fig. 11 is a graph showing changes in relative detection intensity with respect to background film thickness. Fig. 12 is a graph showing changes in relative detection intensity with respect to background film thickness. Fig. 13 is a view showing the configuration of a film thickness unevenness inspection device according to a second embodiment.
圖14係表示檢查基板上之膜之膜厚不均之處理流程的 一部分的圖。 【主要元件符號說明】 1、la 膜厚不均檢查裝置 2 平台 3 光照射部 4 受光單元 5 波長切換機構 6 記憶部 7 膜厚不均檢測部 8 控制部 9 基板 11 膜厚測量部 312XP/發明說明書(補件)/95-11/95127465 36 1311643 12 測量部移動機構 21 移動機構 31 鹵素燈 32 圓柱狀石英棒 33 圓柱透鏡 41 攝影部 42 透鏡 51 光學濾波器 51a 選擇光學濾波器 52 圓板狀濾波器轉盤 53 濾波器旋轉馬達 61 ' 61a 靈敏度資訊 71 輸出受理部 72 濾波器處理部 73 對比度強調部 74 評估值算出部 91 主面 92 膜 111 、112 、 113 、 m 、 122 、 123 、 130 線 211 旋轉馬達 212 導件 410 線感測器 411 攝影元件 521 開口 312XP/發明說明書(補件)/95-11/95127465 37Fig. 14 is a view showing a part of a processing flow for inspecting the film thickness unevenness of the film on the substrate. [Description of main component symbols] 1. la film thickness unevenness inspection device 2 platform 3 light irradiation unit 4 light receiving unit 5 wavelength switching mechanism 6 memory portion 7 film thickness unevenness detecting portion 8 control portion 9 substrate 11 film thickness measuring portion 312XP/ Disclosure of Invention (Supplement)/95-11/95127465 36 1311643 12 Measuring section moving mechanism 21 Moving mechanism 31 Halogen lamp 32 Cylindrical quartz rod 33 Cylindrical lens 41 Photo section 42 Lens 51 Optical filter 51a Selection optical filter 52 Disc Filter wheel 53 Filter rotation motor 61 ' 61a Sensitivity information 71 Output reception unit 72 Filter processing unit 73 Contrast enhancement unit 74 Evaluation value calculation unit 91 Main surface 92 Membrane 111, 112, 113, m, 122, 123, 130 Line 211 Rotary motor 212 Guide 410 Line sensor 411 Photographic element 521 Opening 312XP / Invention specification (supplement) / 95-11/95127465 37
Claims (1)
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| Application Number | Priority Date | Filing Date | Title |
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| JP2005220098 | 2005-07-29 | ||
| JP2006139938A JP4799268B2 (en) | 2005-07-29 | 2006-05-19 | Unevenness inspection apparatus and unevenness inspection method |
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| TW200712480A TW200712480A (en) | 2007-04-01 |
| TWI311643B true TWI311643B (en) | 2009-07-01 |
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| JP4523516B2 (en) * | 2005-08-08 | 2010-08-11 | 東京エレクトロン株式会社 | Coating film unevenness detection method, coating film unevenness detection program, substrate processing method, and substrate processing apparatus |
| EP2128701A1 (en) * | 2008-05-30 | 2009-12-02 | ASML Netherlands BV | Method of determining defects in a substrate and apparatus for exposing a substrate in a lithographic process |
| JP5255342B2 (en) * | 2008-06-25 | 2013-08-07 | パナソニック株式会社 | Defect detection device for light transmissive film |
| JP5305792B2 (en) * | 2008-08-29 | 2013-10-02 | 芝浦メカトロニクス株式会社 | Substrate processing apparatus and substrate processing method |
| JP5410212B2 (en) * | 2009-09-15 | 2014-02-05 | 株式会社Sokudo | Substrate processing apparatus, substrate processing system, and inspection peripheral exposure apparatus |
| DE102012002174B4 (en) | 2012-02-07 | 2014-05-15 | Schott Ag | Apparatus and method for detecting defects within the volume of a transparent pane and using the apparatus |
| TWI477766B (en) * | 2012-12-18 | 2015-03-21 | 財團法人工業技術研究院 | Detection device and detection method |
| KR20140112230A (en) | 2013-03-13 | 2014-09-23 | 삼성전자주식회사 | Method of detecting inhomogeneity of a layer and apparatus for performing the same |
| JP6079697B2 (en) * | 2013-07-11 | 2017-02-15 | 株式会社村田製作所 | Method for measuring thickness of electronic component, method for manufacturing electronic component series using the same, electronic component series manufactured thereby, and electronic component inspection apparatus |
| CN114487046A (en) * | 2022-01-29 | 2022-05-13 | 中国科学技术大学 | An imaging method for determining the surface charge density distribution of two-dimensional materials |
| CN119936060B (en) * | 2025-04-09 | 2025-07-18 | 泉州天娇妇幼卫生用品有限公司 | Baby diaper stain detecting system based on image recognition |
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| JP2577960B2 (en) * | 1988-06-17 | 1997-02-05 | 株式会社ニデック | Specular surface inspection equipment |
| JP3322034B2 (en) * | 1994-10-24 | 2002-09-09 | 日産自動車株式会社 | Paint quality analyzer |
| JP2000055627A (en) * | 1998-08-07 | 2000-02-25 | Dainippon Screen Mfg Co Ltd | Film thickness measuring method and device |
| JP3508589B2 (en) | 1998-11-27 | 2004-03-22 | Jfeスチール株式会社 | Surface flaw inspection equipment |
| JP4162319B2 (en) * | 1999-03-10 | 2008-10-08 | 株式会社ニデック | Defect inspection equipment |
| JP3263931B2 (en) * | 1999-09-22 | 2002-03-11 | 富士重工業株式会社 | Stereo matching device |
| JP3520910B2 (en) * | 1999-12-20 | 2004-04-19 | 株式会社ニコン | Optical element thickness measurement method and optical element manufacturing method |
| JP4418078B2 (en) * | 2000-04-03 | 2010-02-17 | 株式会社トプコン | Surface inspection device |
| JP2001330566A (en) * | 2000-05-23 | 2001-11-30 | Kawasaki Steel Corp | Surface flaw inspection method using CCD camera |
| JP4632564B2 (en) * | 2001-03-08 | 2011-02-16 | オリンパス株式会社 | Surface defect inspection equipment |
| JP4474795B2 (en) * | 2001-04-26 | 2010-06-09 | 株式会社デンソー | Film thickness measuring method, measuring apparatus and semiconductor device manufacturing method |
| JP3928478B2 (en) * | 2002-05-22 | 2007-06-13 | 株式会社島津製作所 | Film thickness measuring method and film thickness measuring apparatus |
| JP3742801B2 (en) * | 2003-03-18 | 2006-02-08 | 独立行政法人科学技術振興機構 | Film thickness acquisition method |
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| JP2007057521A (en) | 2007-03-08 |
| TW200712480A (en) | 2007-04-01 |
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