TW200532164A - Film thickness measuring method and apparatus - Google Patents

Film thickness measuring method and apparatus Download PDF

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Publication number
TW200532164A
TW200532164A TW093136948A TW93136948A TW200532164A TW 200532164 A TW200532164 A TW 200532164A TW 093136948 A TW093136948 A TW 093136948A TW 93136948 A TW93136948 A TW 93136948A TW 200532164 A TW200532164 A TW 200532164A
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film thickness
film
reflectance
spectral
measured
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TW093136948A
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Chinese (zh)
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TWI275772B (en
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Nariaki Fujiwara
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Dainippon Screen Mfg
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    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01BNON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
    • C01B13/00Oxygen; Ozone; Oxides or hydroxides in general
    • C01B13/10Preparation of ozone
    • C01B13/11Preparation of ozone by electric discharge
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01BNON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
    • C01B2201/00Preparation of ozone by electrical discharge
    • C01B2201/20Electrodes used for obtaining electrical discharge
    • C01B2201/22Constructional details of the electrodes
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01BNON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
    • C01B2201/00Preparation of ozone by electrical discharge
    • C01B2201/20Electrodes used for obtaining electrical discharge
    • C01B2201/24Composition of the electrodes
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01BNON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
    • C01B2201/00Preparation of ozone by electrical discharge
    • C01B2201/60Feed streams for electrical dischargers
    • C01B2201/62Air
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01BNON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
    • C01B2201/00Preparation of ozone by electrical discharge
    • C01B2201/60Feed streams for electrical dischargers
    • C01B2201/64Oxygen

Abstract

To provide a film thickness measurement technique which can measure film thickness correctly, even for a transparent film which selectively transmits light of specific wavelength ranges such as a color filter. Theoretical spectral reflectance calculated as the spectral reflectance of a sample, in which a colorless transparent film having predetermined film thickness is formed on a substrate, is acquired a plurality of times for different film thickness. The spectral transmittance of a color filter, which is an object to be measured, is acquired. Concerning the spectral transmittance, a wavelength range providing transmittance of a predetermined value or more is selected as a measurement wavelength range. A plurality of theoretical spectral reflectance calculated for different film thickness are corrected by the spectral transmittance to determine corrected theoretical spectral reflectance. A sample, in which the color filter is formed on a substrate, is irradiated with light, and reflected light from the sample is spectrally separated to measure the spectral reflectance. The measured spectral reflectance is compared to the corrected theoretical spectral reflectance to calculate the film thickness of the color filter.

Description

200532164 九、發明說明: 【發明所屬之技術領域】 本發明係關於一種測定如同形成於半導體基板或液晶顯 不裝置用玻璃基板等之基板上之透明薄膜般,特別是如同 彩色濾光片般選擇性透過特定波長區域之光的透明薄膜之 膜厚的膜厚測定方法以及裝置。 【先前技術】 先前,例如於曰本專利公開平卜24962〇號公報(1994年) 中提出有使用光干擾法測定形成於如上述般之基板上的光 阻膜或氧化矽膜等之極薄之透明薄膜之膜厚的技術。於使 2光干擾法之膜厚測定中,於形成有膜厚為特定值d之透明 缚臈的基板光得以人射之條件下,㈣ !明薄膜之光干擾而規定之分光反射率。此時,=固 疋版厚乾圍以等間距設定之膜厚,則係將求得分光反射率 者作為複數個理論分光反射率而記憶於記憶體等之記憶裝 置中。 、 :繼而,將光照射於形成有測定對象之透明薄臈之基板, 精由分光器將自基板所反射之反射光分光從而實測分光反 射率。其後計算出該實測分光反射率與上述複數個理論分 光反射率之差值’藉由先前眾所周知的曲線擬合法求得該 差值為最小的膜厚值,並將所獲得之臈厚值作為測象 之透明薄膜的膜厚。 [發明所欲解決之問題] 近年來隨著數位照相機或附帶照相機之行動電話的迅逮 97436.doc 200532164 普及,彩色CCD之需求不斷增大。於彩色CCD之製造步驟 於矽晶圓上以矩陣狀貼附RGB 3色之彩色濾、光片 於放映機中使用於液晶玻璃基板上形成彩色濾光片者。於 此種基板上形成彩色濾光片之步驟中,嚴密管理濾光片膜 厚係較為重要,且要求正確測定彩色濾光片之膜厚。然而, 彩色濾光片僅透過特定波長區域之光,例如於綠色濾光片 之it形時僅透過大概480 nm〜600 nm之波長區域的光。圖9 係表示彩色濾光片之透光特性之圖。而將光照射至於基板 上形成具有同圖所示般之透光特性的彩色濾光片之試料時 所獲得之分光反射率(對於波長之反射率之分佈)則成為如 圖1〇所示般。再者,於圖1G中以實線表示自形成有彩色渡 光片之基板所獲得之分光反射率,替代彩色濾光片對於所 有的可視光區域之光為參考於基板上形成透明薄膜(即無 色之透明薄膜)時的分光反射率則以虛線表示。 士圖1 0所不’於無色之透明薄膜之情形時,於滿足薄膜200532164 IX. Description of the invention: [Technical field to which the invention belongs] The present invention relates to a kind of measurement, such as a transparent film formed on a substrate such as a semiconductor substrate or a glass substrate for a liquid crystal display device, and is particularly selected as a color filter. Film thickness measurement method and device for transparent film thickness that transparently transmits light in a specific wavelength region. [Prior Art] Previously, for example, in Japanese Patent Publication No. 249620 (1994), it has been proposed to use a light interference method to measure the extremely thin photoresist film or silicon oxide film formed on a substrate as described above. The technology of transparent film thickness. In the measurement of the film thickness of the two-light interference method, under the condition that the substrate formed with a transparent film having a film thickness of a specific value d can be radiated by humans, the specified spectral reflectance of the light interference of the thin film is determined. At this time, the film thickness set by the solid thickness of the solid plate at equal intervals is to store the scored light reflectance as a plurality of theoretical spectral reflectances in a memory device such as a memory. : Then, the light is irradiated on the substrate on which the transparent thin ridge of the measurement object is formed, and the spectroscope splits the reflected light reflected from the substrate to measure the spectral reflectance. Thereafter, the difference between the measured spectral reflectance and the above-mentioned theoretical spectral reflectances is calculated. 'The minimum film thickness value is obtained by the curve fitting method previously known, and the obtained thickness value is taken as The film thickness of the transparent film measured. [Problems to be Solved by the Invention] In recent years, with the rapid spread of digital cameras or mobile phones with cameras 97436.doc 200532164, the demand for color CCDs has been increasing. Manufacturing steps for color CCDs: Color filters and light filters of RGB 3 colors are pasted on a silicon wafer in a matrix. Those used in a projector are used to form color filters on a liquid crystal glass substrate. In the step of forming a color filter on such a substrate, it is important to closely manage the thickness of the filter film, and it is required to accurately measure the film thickness of the color filter. However, the color filter only transmits light in a specific wavelength region, for example, in the it shape of the green filter, it transmits only light in a wavelength region of about 480 nm to 600 nm. FIG. 9 is a diagram showing the light transmission characteristics of a color filter. The spectral reflectance (distribution of reflectance with respect to wavelength) obtained when the light is irradiated on the substrate to form a sample having a light-transmitting color filter as shown in the figure becomes as shown in FIG. 10 . Furthermore, in FIG. 1G, the solid reflectance obtained from the substrate on which the color light-emitting sheet is formed is represented by a solid line. Instead of using a color filter for all light in the visible light region, a transparent film (i.e., When the colorless transparent film is used, the spectral reflectance is indicated by a dotted line. What Figure 10 does not do in the case of a colorless transparent film

97436.doc 200532164 衫色濾光片之分光透過率(對於波長之透過率之分佈)並非 表不為矩形波形而是表示為台形狀波形。即,即使於產生 透光的特定波長區域中,於其之邊界附近透過率亦會類比 性變化。因此’於透過率分佈之傾斜部的波長區域中反射 率會變得低於理論值,故而若將該波長區域包含於測定波 長區域則膜厚測定之可靠性將明顯降低。 、為此,雖亦可考隸將去除於透過率分料之傾斜部之 波長區域的波長範圍,即僅將於如圖9之透過率分佈中之峰 頂平坦部之波長區域設為測定波長區域,藉此提高測定精 度’然而該情形時測定波長區域之寬度變得非f狹窄為4q 細至5〇 nm,因此擔心由此種情況造成敎可靠性之降低。 特別是彩色渡光片之膜厚越薄反射率分佈之波形越會變成 低周波波m會產生心収波長區域之寬度變得較窄 則膜厚測定自身將難以進行之問題。 本發明係#於上述課題開發而成者,其目的在於提供一 種即使如彩色渡光片般選擇性透過特定波長區域之光的透 明薄膜亦可正確測定其膜厚之臈厚測定技術。 【發明内容】 為解決上述課題,請求们之發明係自將光照射至於基板 上形成有透明薄膜之試料而獲得之分光反射率敎上述透 明薄膜之膜厚的膜厚敎方法,其包含:分光透過率取得 步驟,其取得上述透明薄膜之分光透㈣;分光反射率測 定步驟’其將光照射至上述試料,並將自上述試料所反射 之反射光分光從而實測分光反射率;校正步驟,其藉由上 97436.doc 200532164 = 先得以算定作為於基板上形成具有特 率一二==::,射 正之校正後理論分光反射率▲二:中付以校 中得以測…測分光反射;,、從而算==定步驟 薄膜之膜厚。 叨斤出涮疋對象之透明 其於上二請求項1之發明之膜_方法, 旦廿^ V驟中附加對應於上述分光透過率之重 里"匕較上述校正後理論 射率從^出測定對象之透明薄膜之膜羊厚,这實測分光反 測二係請求項1或請求項她^ 臨限值以上定具有於上述分光透過率之特定 之測定波長區域之步驟域作為上述臈厚算出步驟中 透明薄臈:::4之發:’係自將光照射至於基板上形成有 ==測定方法’其包含:分光透過率取得步驟,其 二述透明薄臈之分光透過率’·分光反射率測定步驟, 照㈣上述試料,並將自上述試料所反射之反射光 = 分光反射率;校正步驟,其藉由上述分光透 y又正於上述分光反射率測定步驟中 膜厚算出步驟,其比較作為於基板上形= 特疋版厚之透明薄膜之試料的分光反射率而預先得以 异定之理論分光反射率與於上述校正步驟中得以校正之校 97436.doc 200532164 ,實:=反射率,算出測定對象之透明薄臈之膜厚。 明薄膜之試料而獲得之分光反射率測定上:= 厚的膜厚測定裝置,其包含:第,記 产: 裘7 過率’·第2記憶機構’其記憶理論分光反射 率’该理論分光反射率作為 之透明餐㈣ 手料於練场切W特定膜厚 臈之試料的分光反射率而預先得以算定;光源, 其將光照射至測定對象n “、 象之从,77 μ料敎機構,其 峨,且將藉由測定對象之試料而反射之反 光透、射率;校正機構’其藉由上述分 述理論分光反射率;以及臈厚算出機構, 率η 機構中得讀正之校正後理論分光反射 、、猎上述分光反射率測定機構而得以測定之實測分光 反射率’從而算出測定對象之透明薄膜之膜厚。 又,請求項6之發明,係請求項5之發明之膜厚測定裝置, 其=上述第2記憶機構中記憶對應於不同膜厚之透明薄膜 的複數個理淪分光反射率,並於上述校正機構將各上述複 數個理論分光反射率乘以上述分光透過率從而算出複數個 校正後理論分光反射率,而於上述膜厚算出機構,求得各 上述複數個校正後理論分光反射率與上述實測分光反射率 之f值’使表示將所獲得之複數個差值近似為二次曲線時 之最小值的膜厚值為測定對象之透明薄膜之膜厚。 又,請求項7之發明,係請求項6之發明之膜厚測定裝置, 其於上述膜厚算出機構,將上述分光透過率越高則會變得 97436.doc 200532164 (重之重减加至各個上述複數 與上述實測分光反射率之差值,使先反射率 附加有重量之差j吏表不將所獲得之複數個 測定對象之透明薄臈之膜厚。 丨值的膜尽值為 求項8之發明,係請求項5至請求項7之任一項發明 之特1 #進而包含將具有於上述分光透過率處 之特疋臣品限值以上之透 時之測定、、由且,、 域選定作為膜厚算出 ❿ 、/長區域的波長區域選定機構。 又、月求項9之發明,係自將光照射至 明薄膜之試料而㈣旱夕八丄c… 土板上形成有透 B月薄膣夕a S :第1記憶機構,其記憶上述透 率,兮料、 ¥ 4機構,其纪憶理論分光反射 ^㈣光反射率係作為於基板上形成有 厚之透明薄膜之#极从\ 八有特疋膜 、Μ ^斗的勿光反射率而預先得以瞀定· 源,其將光照射至測定對象之試料·八于^斤疋,光 其自上述光源照射光,且葬 再 射之反射光分光從而、_卜 象之試料而得以反 、 測定分光反射率;校正機構,其藉由 4先透過率校正藉由上述分光反射率測 測定之實測分歧射m膜厚算出_,其比較^ 述&正機構得以校正之校正後實測分光反射率八 为光反射率,從而算出測定對象之透明薄膜之膜厚;1里响 又,凊求項H)之發明’係自將光照射至 透明薄膜之續料而猶〜 &上^成有 *輪之从而獲得之分光反射率測定上述 膜厚的膜厚測定裝置,1七八.斤彳丨 '' 置其包含.第1光源,其將光照射至上 97436.doc -10- 200532164 2 膜形成面;第2光源’其將光照射至與上述試料 〜、形成面相反側面;分光機構,其將自上97436.doc 200532164 The spectral transmittance (distribution of transmittance to wavelength) of the color filter is not shown as a rectangular waveform but as a table-shaped waveform. That is, even in a specific wavelength region where light is transmitted, the transmittance changes analogously near its boundary. Therefore, the reflectance in the wavelength region of the inclined portion of the transmittance distribution becomes lower than the theoretical value. Therefore, if the wavelength region is included in the measurement wavelength region, the reliability of the film thickness measurement will be significantly reduced. For this reason, although the wavelength range of the wavelength region removed from the inclined portion of the transmittance material can be tested, that is, only the wavelength region of the peak top flat portion in the transmittance distribution shown in FIG. 9 is set as the measurement wavelength. In this case, the width of the measurement wavelength region becomes non-narrow to 4q to 50 nm, so there is a concern that the reliability may be reduced in this case. In particular, the thinner the film thickness of the color light-transmitting sheet is, the lower the waveform of the reflectance distribution becomes. The lower the frequency m, the narrower the width of the wavelength range of the epicenter, the narrower the film thickness measurement itself becomes. The present invention was developed based on the above-mentioned subject, and its object is to provide a thickness measurement technology that can accurately measure the thickness of a transparent thin film that can selectively transmit light in a specific wavelength region, such as a color light sheet. [Summary of the Invention] In order to solve the above-mentioned problem, the invention of the applicant is a spectral reflectance obtained by irradiating light to a sample having a transparent film formed on a substrate (a film thickness of the above-mentioned transparent film), a method including: A transmittance obtaining step, which obtains the spectral transmittance of the transparent film; a spectroscopic reflectance measuring step, which irradiates light onto the sample, and separates the reflected light reflected from the sample to measure the spectroscopic reflectance; a calibration step, which Based on 97436.doc 200532164 = first it can be calculated as the formation on the substrate with a specific rate of one == ::, the theoretical spectral reflectance after correction is correct ▲ two: Zhongfu can be measured in the middle of the measurement ... , So that == film thickness of a fixed step film. The object ’s transparency is based on the film_method of the invention claimed in item 2 of the previous two claims. Once the V step is added, the weight corresponding to the above-mentioned spectral transmittance is added. The film thickness of the transparent film of the measurement object is measured by the spectroscopic reflection measurement of the second item of the request item 1 or the item ^ above the threshold. The step range determined to have a specific measurement wavelength region of the above-mentioned spectral transmittance is calculated as the above thickness. In the step, the transparent thin film ::: 4 is issued: 'It is formed by irradiating light on the substrate == measuring method', which includes: the step of obtaining the spectral transmittance, and the second is the spectral transmittance of the transparent thin film. The reflectance measurement step is based on the above sample, and the reflected light reflected from the sample is equal to the spectral reflectance; the correction step is the step of calculating the film thickness in the spectral reflectance measurement step by the spectroscopic transmission y, It compares the theoretical spectral reflectance, which was previously determined as the spectral reflectance of the sample on the substrate = special thick transparent film, and the calibration corrected in the above-mentioned calibration step 97436.doc 2005321 64, real: = reflectance, calculate the film thickness of the transparent thin object to be measured. Measurement of the spectral reflectance obtained from a sample of a thin film: = Thick film thickness measuring device, which includes: First, recorded production: Qiu 7 Excess rate '· 2nd memory mechanism' Theoretical spectroscopic reflectance of its memory 'The theoretical spectroscopic The reflectance is calculated as a transparent meal. The spectroscopic reflectance of a sample with a specific film thickness is cut in the training area. The light source irradiates light to the measurement object n, the image is from the 77 μ material. The correction mechanism will reflect the reflectance and transmittance of the light reflected by the sample of the measurement object; the correction mechanism 'its spectroscopic reflectance based on the above-mentioned theory; and the thickness calculation mechanism, after reading the correct correction in the η mechanism The theoretical spectral reflection and the actual spectral reflectance measured by hunting the above-mentioned spectral reflectance measuring mechanism can be used to calculate the film thickness of the transparent film to be measured. The invention of claim 6 is the film thickness measurement of the invention of claim 5. Device, which stores a plurality of theoretical spectral reflectances of transparent films corresponding to different film thicknesses in the second memory mechanism, and reflects each of the plurality of theoretical spectral reflections in the correction mechanism Multiplying the above-mentioned spectral transmittance to calculate a plurality of corrected theoretical spectral reflectances, and in the film thickness calculating mechanism, the f-values of each of the above-mentioned corrected theoretical spectral reflectances and the actual measured spectral reflectances are calculated so that The film thickness obtained when the plurality of obtained differences are approximately the minimum when the quadratic curve is the film thickness of the transparent film to be measured. The invention of claim 7 is a film thickness measuring device of the invention of claim 6. In the above-mentioned film thickness calculation mechanism, the higher the spectral transmittance becomes 97436.doc 200532164 (the weight reduction is added to the difference between each of the complex number and the measured spectral reflectance, so that the first reflectance is added with weight The difference j indicates that the obtained film thicknesses of the plurality of transparent thin objects to be measured are not included. The value of the film is the invention of item 8, which is a feature of any one of claims 5 to 7. 1 # In addition, it includes a wavelength region selection mechanism for measuring when there is a transmittance above the threshold value of the special optical transmittance at the above-mentioned spectral transmittance, and selecting a region as a film thickness to calculate ❿ and // long regions. The invention of claim 9 is obtained by irradiating light to the sample of the thin film and drying it on the ground. C ... A transparent plate is formed on the soil plate. S: The first memory mechanism, which memorizes the above-mentioned transmittance. Material, ¥ 4 mechanism, its Ji Yi theory spectroscopic reflection ^ ㈣ light reflectance is as a thick transparent film formed on the substrate # 极 从 \ Eight special film, M ^ Do not reflect light reflectance in advance A fixed source, which irradiates light to the sample to be measured. The palladium is irradiated with light from the above-mentioned light source, and the reflected light emitted from the light source is spectroscopically separated to measure the spectrophotometry. Reflectivity; a correction mechanism that calculates the measured birefringence m film thickness from the measured spectral reflectance measured by the above-mentioned spectral reflectance measurement with 4 first transmittance corrections, a comparison ^ described & the actual measured spectral reflectance after the correction is corrected by the positive mechanism Is the light reflectance, so that the film thickness of the transparent film to be measured is calculated; the invention of 1 mile, and the search term H) is based on the continuation of irradiating light to the transparent film ~ & 上 ^ 成 有 * The film thickness measurement device for measuring the above-mentioned film thickness by measuring the spectral reflectance thus obtained The first light source, which irradiates light to the above 97436.doc -10- 200532164 2 film formation surface; the second light source 'which irradiates light to the above sample ~, forming Opposite side; beam splitter, which will be from top

==且透過上述基板以及上述透明薄膜之透過光分 *、、:疋上述透明薄膜之分光透過率,且將自上述p 、列,=射且藉由上述試料而得以反射之反射光分光從而 呈二刀先反射率;記憶機構,其記憶作為於基板上形成有 2特定膜厚之透㈣叙試㈣分歧射“預先得以 理論分光反射率;校正機構,其藉由以上述分光機 传以敎之上述分光透過率校正上述理論分光反射 率,=及膜厚算出機構,其比較於上述校正機構中得以校 =之权正後理論分光反射率與藉由上述分光機構而得以測 =之貫測分光反射率,從而算出測定對象之透明薄膜之膜 厚0 [發明之效果] 依據請求項1之發明,由於比較藉由分光透過率校正作為 於基板上形成有具有特定膜厚之透明薄膜之試料的分光反 射率而預先得以算定的校正後理論分歧㈣與實測分光 反射率絲&敎料之透㈣膜之膜厚,㈣理論分光 二射率與實測分光反射率之背離將得以解除,所以即使如 彩色渡光片般選擇性透過特枝長區域之光的透明薄膜亦 可正確地測定其膜厚。 又’依據請求項2之發明,由於附加對應於分光透過率之 重量’並比較校正後理論分光反射率與實測分光反射率從 而算出測定對象之透明薄膜之膜厚1而可進行增強了對 97436.doc -11 - 200532164 應於分光透過率之可靠性的比較,從而可實行更正確之膜 厚測定。 ' 矿據月长項3之發明,由於選定具有於分光透過率處 之特定臨限值以上之读# .旁&、士 εl 之透過率的波長區域作為測定波長區 域,故而可擴大測定波長區域提高膜厚測定精度。 又依據°月求項4之發明,由於比較作為於基板上形成有 具有特定膜厚之透明薄膜之試料的分光反射率而預先得以 异定之理論分光反射率與藉由分光透過率而得以校正之校 正後貝測分光反射率,從而算出測定對象之透明薄膜之膜 厚,故而理論分光反射率與實測分光反射率之背離得以解 除,所以即使如彩色濾光片般選擇性透過特定波長區域之 光的透明薄膜亦可正確測定其膜厚。 又’依據請求項5之發明,由於比較藉由分光透過率校正 作為於基板上形成有具有特定膜厚之透明薄膜之試料的分 光反射率而預先^異丨v+ 八m+i s 4之理論分光反射率之校正後理論 =射率與貫測分光反射率’從而算出測定對象之透明 :得=,故而理論分光反射率與實測分光反射率之背 二"即使如彩色濾光片般選擇性透過特定波 °° 3 、’透明薄膜亦可正確測定其膜厚。 又’依據請求項6之發明,將各個複數個 乘以分光透過車你;^ ^ 甘屯〜 κ而异出複數個校正後理論分敍射率, 亚求侍各個該等複數個校正後理#八#应&# ^ 反射率m, x纟理-刀先反射率與實測分光 Λ φ 吏表示將所獲得之複數個差值近似為二次 最小值的臈厚值為測定對象之透明薄膜之膜厚, 97436.doc 200532164 故而理論分光反射率與實測分光反射率之背離將得以解除 且含於兩者之差值的誤差會大幅度降低,所以二次曲線近 似之精度變高,因而即使如彩色濾光片般選擇性透過特定 波長區域之光的透明薄膜亦可正確測定其膜厚。 又,依據請求項7之發明,將分光透過率越高則越重之重 量附加至各個複數個校正後理論分光反射率與實測分光反== and transmitted light transmitted through the substrate and the transparent film, *, :: 疋 the spectral transmittance of the transparent film, and will be reflected from the p, column, = and reflected light reflected by the sample to split the light so that It has a two-knife first reflectance; the memory mechanism stores its memory as a transparent film with a specific film thickness of 2 on the substrate. The "differential projection" allows the theoretical spectral reflectance to be obtained in advance; the correction mechanism uses the above-mentioned spectrometer to transmit The above-mentioned spectral transmittance corrects the above-mentioned theoretical spectral reflectance, and the film thickness calculation mechanism, which is compared with the above-mentioned correcting mechanism to correct the theoretical spectral reflectance after being corrected with the above-mentioned spectroscopic mechanism to measure = Measure the spectral reflectance to calculate the film thickness of the transparent film to be measured. 0 [Effect of the invention] According to the invention of claim 1, the spectral transmittance correction is used to compare the thickness of a transparent film with a specific film thickness on the substrate. Spectral reflectance of the sample can be calculated in advance after the theoretical difference between correction and the measured spectral reflectance wire & the thickness of the transparent film of the material. The deviation between the reflectance and the measured spectral reflectance will be eliminated, so that even a transparent thin film that selectively transmits light in the special branch long area like a color light sheet can accurately measure its film thickness. Also according to the invention of claim 2, because The weight corresponding to the spectral transmittance is added, and the theoretical spectral reflectance after correction is compared with the measured spectral reflectance to calculate the film thickness 1 of the transparent thin film to be measured, which can be enhanced. 97436.doc -11-200532164 should be used for spectral transmission The comparison of the reliability of the transmission rate enables a more accurate measurement of the film thickness. According to the invention of the item 3 of the monthly length, the reading having a specific threshold value above the spectral transmittance is selected. The wavelength region of the transmittance of εl is used as the measurement wavelength region. Therefore, the measurement wavelength region can be enlarged to improve the measurement accuracy of the film thickness. According to the invention of the item 4 in °°, it is compared with the case where a transparent film with a specific film thickness is formed on the substrate. Spectral reflectance of the sample, the theoretical spectroscopic reflectance that can be determined in advance, and the corrected spectroscopic reflectance that is corrected by the spectral transmittance In order to calculate the film thickness of the transparent film to be measured, the deviation between the theoretical spectral reflectance and the measured spectral reflectance can be eliminated, so even a transparent film that selectively transmits light in a specific wavelength region like a color filter can be accurately measured. Its film thickness. According to the invention of claim 5, according to the comparison of the spectral reflectance of a sample having a transparent film with a specific film thickness formed on the substrate by spectral transmittance correction, it is different in advance. V + eight m + is The theoretical spectral reflectance of 4 is corrected after the theory = emissivity and measured spectral reflectance 'to calculate the transparency of the measurement object: get =, so the theoretical spectral reflectance and the measured spectral reflectance are the second two "even if the color filter Selective transmission through a specific wave °° 3, 'transparent film can also accurately determine its film thickness.' Also according to the invention of claim 6, multiply each of the multiple by the spectroscopic transmission through the car; ^ ^ Gantun ~ κ varies A plurality of corrected theoretical spectroscopic emissivities are produced, and Ya Qiushi each of these plural corrected post-correction principles # 八 # 应 &# ^ Reflectivity m, x 纟 -the first reflectance of the knife and the measured spectrometry Λ φ The thickness that indicates that the obtained multiple differences are approximated to the second minimum value is the film thickness of the transparent film to be measured. 97436.doc 200532164 Therefore, the deviation between the theoretical spectral reflectance and the measured spectral reflectance will be removed and included. The error in the difference between the two will be greatly reduced, so the accuracy of the quadratic curve approximation is increased, so that even a transparent thin film that selectively transmits light in a specific wavelength region like a color filter can accurately measure its film thickness. In addition, according to the invention of claim 7, the higher the spectral transmittance, the heavier the weight is added to each of the plurality of corrected theoretical spectral reflectances and measured spectral reflectances.

射率之差值,並使表示將所獲得之複數個附有重量之差值 近似為二次曲線時之最小值的膜厚值為測定對象之透明薄 膜之膜厚,故而越是透過率較高且可#性較高之差值則評 價越鬲,故可實行更正確之膜厚測定。 定精度 又,依據請求項8之發明,由於選定具有於分光透過率處 之特定臨限值以上之透過㈣波長區域作為膜厚算出時的 測定波長區域,故而可擴大測定波長區域從而提高膜厚測 又,依據請求項9之發明,由於比較作為於基板上形成有 ΐ有特定膜厚之透明薄膜之試料的分光反射“預先得以 异又之理論分歧料㈣由分紐過㈣得以校正 ;後實測分光反射率,並算出測定對象之透明薄膜之膜 Χ 故而料分歧料與實齡光反㈣之㈣得以解 所以即使如彩μ光片般選擇性透過特定波長 光的透明薄膜亦可正確測定其膜厚。 次之 正二依:請求項1〇之發明,由於比較藉由分光透過率校 ’、、、於土板上形成有具有特定膜厚之透 的 分光反射率而預先得以算定之理論分光反射 97436.doc 200532164 論分光反射率與實測分光反射率,並算出測定對象之透明 薄膜之膜厚,故而理論分光反射率與實測分光反射率之背 離將得以解除,所以即使如彩色濾光片般選擇性透過特定 波長區域之光的透明薄膜亦可正確測定其膜厚。 【實施方式】 以下,一面參照圖式一面就本發明之實施形態加以詳細 說明。 ' < 1 ·苐1實施形態> 圖1係表示本發明之膜厚測定裝置之構成的圖。該膜厚測 定裝置包含第1照明光學系統10、第2照明光學系統2〇以及 成像光學系統30。第1照明光學系統10包含出射白色光之鹵 素燈11以及照明透鏡12。照明透鏡12以例如聚光鏡之組合 構成,於該聚光鏡附設有省略圖示之視場光闌等。自鹵素 燈11出射之光經由照明透鏡12入射至成像光學系統。 成像光學系統30包含物鏡31、半反射鏡32以及成像透鏡 33。來自第i照明光學系統1〇之照明光藉由半反射鏡似The difference between the emissivity and the minimum film thickness when the difference between the obtained weights with the approximated quadratic curve is approximated as the film thickness of the transparent film to be measured. The higher and the higher the difference, the more the evaluation becomes, so that a more accurate film thickness measurement can be performed. In addition, according to the invention of claim 8, since a transmission wavelength region having a specific threshold value above the spectral transmittance is selected as the measurement wavelength region when the film thickness is calculated, the measurement wavelength region can be enlarged to increase the film thickness. According to the invention of claim 9, because the spectroscopic reflection of a sample formed with a transparent film with a specific film thickness on a substrate is compared, "theoretical divergence material that is different in advance can be corrected by the branch transition"; Measure the spectral reflectance and calculate the film of the transparent film to be measured. Therefore, the difference between the material and the actual age light can be resolved. Therefore, even a transparent film that selectively transmits light with a specific wavelength like a color μ-light sheet can be accurately measured. The thickness of the film is second. The invention of claim 10 is based on the theory that the spectroscopic reflectance of a specific film thickness is formed on the soil plate by comparing the spectral transmittance with the spectral transmittance calibration. Spectral reflection 97436.doc 200532164 The spectroscopic reflectance and the measured spectroscopic reflectance are calculated, and the film thickness of the transparent film to be measured is calculated. The deviation between the emissivity and the measured spectral reflectance will be eliminated, so even a transparent film that selectively transmits light in a specific wavelength region like a color filter can accurately measure its thickness. [Embodiment] Hereinafter, referring to the drawings An embodiment of the present invention will be described in detail. '≪ 1 · 1 embodiment > Fig. 1 is a diagram showing a configuration of a film thickness measuring device of the present invention. The film thickness measuring device includes a first illumination optical system 10 The second illumination optical system 20 and the imaging optical system 30. The first illumination optical system 10 includes a halogen lamp 11 that emits white light and an illumination lens 12. The illumination lens 12 is constituted by a combination of, for example, a condenser, and an omitted figure is attached to the condenser. The field of view diaphragm, etc. The light emitted from the halogen lamp 11 is incident on the imaging optical system through the illumination lens 12. The imaging optical system 30 includes an objective lens 31, a half mirror 32, and an imaging lens 33. From the i-th illumination optical system 1〇 The illumination light looks like a half mirror

射,且經由物鏡3 1照射至載置於樣口 A 么银σ口台5上之試料丨之上 面。再者,試料1係於半導體基板或液曰 双乂,夜日日顯不裝置用玻璃基 板等之基板上形成有作為有色之读 巴之透明溥膜的彩色濾光片 者。即,光可自第1照明光學李蛴〗0旧& 予糸、·先10妝射至試料1之薄膜形 成面。 樣品台5係於其中央部具有開口 載置台。於樣品台 5附設有省略圖示之ΧΥ驅動機構, 執置試料1且移動於水 平面内之X方向以及Υ方向。再者, 作為樣品台5可為於中 97436.doc -14- 200532164 央4具有開口且可載置試料!者,亦可為如同例如保持試料 1之周緣部的框體般者。 另一方面,第2照明光學系統2〇失著樣品台5配置於與成 像光學系統30相反側。第2照明光學系統2〇含有出射白色光 之齒素燈21以及照明透鏡22。較好的是鹵素燈以之出射光 之分光特性與il素燈11相同。或者亦可以—個齒素燈構成 i素燈11以及21,並藉由光纖等分別導光。又,照明透鏡 22係具有聚光功能之透鏡系統,自_素燈21所出射之光經 由妝明透鏡22聚光,並通過樣品台5之開口照射至試料丨之 背面,即與試料1之薄膜形成面相反側之面。 自第1照明光學系統10照射且於試料丨之上面反射之光以 及自第2照明光學系統2〇照射且透過試料1之光經由物鏡 31、半反射鏡32以及成像透鏡33而聚光於成像光學系統3〇 之光軸上之特定位置。以分光單元4〇之入射用針孔位於該 聚光位置之附近之方式,配置有分光單元4〇。 分光單元40包含將入射光分光之凹面繞射光柵41以及檢 測藉由凹面繞射光柵41所繞射之繞射光之分光光譜的光檢 測為42。光檢測器42包含例如光電二極體陣列或ccd等。 藉此,藉由成像光學系統30聚光,且入射至分光單元4〇之 光藉由凹面繞射光柵41分光,對應於該光之分光光譜之信 號自光檢測器42傳達至運算部50。 圖2係表示運算部5〇之構成的方塊圖。運算部5〇基於自分 光單元40所接受之分光光譜資訊算出試料1之彩色濾光片 之膜厚。運算部50具有與一般性電腦同樣之硬體構成,並 97436.doc -15- 200532164 包含執行各種運算處理之CPU51、作為記憶基本程式等之 讀出專用之記憶體的ROM52、作為CPU51之作業區域而發 揮功能之自由讀寫之記憶體的RAM53及記憶程式或各種資 料之磁碟54。又,CPU51經由省略圖示之輸人輸出介面連 接有鍵盤60、CRT61、列印機62以及上述之光檢測器42。 膜厚測定裝置之操作員可自鍵盤6G將各種指令或參數輸人 至運算部50,且可確認自CRT 61或打印機以所輸出之運算Is irradiated and irradiated onto the sample 丨 placed on the sample port A and the silver σ port table 5 through the objective lens 31. In addition, the sample 1 is a color filter formed on a semiconductor substrate or a liquid crystal substrate, and a glass substrate such as a glass substrate, which is a device for colored display, is formed on a substrate every day. In other words, light can be emitted from the first illumination optics 蛴 旧 0 old & Yu 先, · 10 makeup first to the film forming surface of sample 1. The sample stage 5 has an opening mounting stage at the center. An XY drive mechanism (not shown) is attached to the sample stage 5, and the sample 1 is placed and moved in the X direction and the Y direction in the horizontal plane. In addition, the sample stage 5 may be a center 97436.doc -14- 200532164. The center 4 has an opening and can mount a sample! Alternatively, it may be, for example, a frame that holds the peripheral portion of the sample 1. On the other hand, the second illumination optical system 20 is disposed on the opposite side from the imaging optical system 30 without the sample stage 5. The second illumination optical system 20 includes a tooth lamp 21 and an illumination lens 22 which emit white light. It is preferable that the spectral characteristics of the light emitted by the halogen lamp are the same as those of the illuminator lamp 11. Alternatively, one element lamp may be used to form the element lamps 11 and 21, and the light is guided by an optical fiber or the like. In addition, the illumination lens 22 is a lens system having a focusing function. The light emitted from the prime lamp 21 is condensed through the makeup lens 22 and is irradiated to the back of the sample 丨 through the opening of the sample stage 5, that is, the same as the sample 1 The surface on the opposite side of the film formation surface. The light irradiated from the first illumination optical system 10 and reflected on the sample 丨 and the light irradiated from the second illumination optical system 20 and transmitted through the sample 1 are collected by the objective lens 31, the half mirror 32, and the imaging lens 33 to be focused on the imaging A specific position on the optical axis of the optical system 30. The spectroscopic unit 40 is arranged such that the entrance pinhole of the spectroscopic unit 40 is located near the light-condensing position. The spectroscopic unit 40 includes a concave diffraction grating 41 that splits incident light and a light detection 42 that detects a spectral spectrum of the diffraction light diffracted by the concave diffraction grating 41. The photodetector 42 includes, for example, a photodiode array or ccd. Thereby, the light condensed by the imaging optical system 30 and incident on the spectroscopic unit 40 is split by the concave diffraction grating 41, and a signal corresponding to the spectroscopic spectrum of the light is transmitted from the photodetector 42 to the arithmetic unit 50. FIG. 2 is a block diagram showing the configuration of the arithmetic unit 50. The calculation unit 50 calculates the film thickness of the color filter of the sample 1 based on the spectral spectrum information received from the spectroscopic unit 40. The arithmetic unit 50 has the same hardware configuration as a general computer, and 97436.doc -15- 200532164 includes a CPU 51 for performing various arithmetic processes, a ROM 52 as read-only memory for storing basic programs and the like, and a work area for the CPU 51 RAM53, which is a freely readable and writable memory, and disk 54 for storing programs or various data. The CPU 51 is connected to a keyboard 60, a CRT 61, a printer 62, and the photodetector 42 described above via an input / output interface (not shown). The operator of the film thickness measuring device can input various instructions or parameters from the keyboard 6G to the calculation section 50, and can confirm the calculations output from the CRT 61 or the printer

結果。進而於鹵素燈U以及鹵素燈12分別設有燈電源,: 樣品台5設有XY驅動電路(均省略圖示),運算部5〇iCpu5i 亦與該等電性連接。再者,於圖2所示之校正部&膜厚算 出部56以及測定波長區域敎部㈣為藉由cpu5i實行特 ^之處理程序而得以實現之處理部,關於該處理之詳細内 谷下面將作進一步敍述。result. Further, the halogen lamp U and the halogen lamp 12 are respectively provided with lamp power sources: the sample stage 5 is provided with an XY driving circuit (both are not shown), and the computing unit 50iCpu5i is also electrically connected to these. Furthermore, the correction section & film thickness calculation section 56 and the measurement wavelength region 敎 section shown in FIG. 2 are processing sections which are realized by implementing a special processing program by cpu5i. Details of the processing are described below. This will be described further.

其次,就本發明之臈厚測定方法之處理步驟加以㈣ 圖3係表示本發明之膜厚測定方法之處理步驟的流程i 此處’說明自將光照射至試則所獲得之分光反射率測变 :色遽光片之臈厚的步驟,上述試料^於基板上形成有作 ==膜的綠色彩色渡光片。再者,當然並非僅限 、=:,㈣光片或紅色遽光片等之其他顏色的 巴/愿光片亦可以相同步驟測定膜厚。 首先,取得作為於基板上形 膜之試料的分光反射率而得以定厚之透明 驟si)。該理論分光反射率係 f +反射^ 尸夕八^ 如下之條件下藉由計算所 件之分光反射率,該條件為於與形成有成為測定對象之 97436.doc -16- 200532164 色濾光片之基板相同之基板上形成有特定膜厚d之 明薄膜,且白色光自第(照明光學系統1〇入射至該無色透明 缚膜之上面。再者,於本說明書中所謂之「反射率」係對 於於嚴格地在基板上未形成透明薄膜(膜厚為零)時之反射 強度的反射強度比率,即相對反射率。 :里論分光反射率係就不同膜厚4之無色透明薄膜分別得 以算定’此等不同膜厚d之無色透明薄膜於相應成為測定對 象之彩色滤光片的膜厚之要求的固定範圍内(例如假設測 疋對象β色遽光片之膜厚為數百咖時為1〇〇細至丨_咖 之範圍)以等間距(例如10 nm間距)而設定。由於於透明薄膜 會產生光干擾’故而光於相互加強之波長反射率變高,於 相互減弱之波長反射率降低。且產生光干擾之條件依據透 明薄膜之膜厚而決定,故而依據膜厚理論分光反射率之圖 案不同。所以’基於就各個不同膜厚之光干擾條件,理論 分光反射率可得以算定。 圖4係例示就不同膜厚之無色透明薄膜而得以算定之理 淪分光反射率的圖。圖4(a)係膜厚較厚之透明薄膜的理論分 光反射率,(b)係膜厚較薄之透明薄膜的理論分光反射率。 如圖4所示,膜厚越薄理論分光反射率之圖案週期越低。 即,固定波長區域内之理論分光反射率之峰穀將減少。相 應此種預先算定之不同膜厚之透明薄膜的理論分光反射率 之資料將記憶於磁碟54。 其次’進入步驟S2,取得作為測定對象之彩色濾光片的 刀光透過率。彩色濾光片之分光透過率亦可於圖1之膜厚測 97436.doc 200532164 定裝置直接測定,或亦可使用預先測定者。即,於對於可 視光整個區域透明之玻璃基板上形成有彩色濾光片之情形 時,直接測定利用第2照明光學系統2〇之分光透過率,於對 於可視光不透明之矽基板上形成有彩色濾光片之情形時使 用預先測定之分光透過率。 於玻璃基板上形成有彩色濾光片之情形時該基板自身基 本完全透過光故而可直接測定分光透過率,此時自第2照明 光學系統20所照射並透過試料丨(即基板以及彩色濾光片)之 光藉由成像光學系統30得以聚光,並藉由分光單元4〇將該 光分光,藉此測定彩色濾光片之分光透過率。藉由分光單 元40所測定之分光透過率將傳達至運算部5〇,並記憶於磁 碟54 〇 另一方面,於矽基板上形成彩色濾光片之情形時,由於 基板自身不透過光故而無法直接測定分光透過率,使用形 成有具有與測定對象之彩色濾光片相同之材質且同等程度 之厚度的彩色濾光片之透明基板(例如玻璃基板)預先測定 分光透過率。亦可藉由本實施形態之膜厚測定裝置實行使 用有此種li視器用試料之彩色濾、光片之分光透過率的測 定’亦可使用其他分光透過率測定專用裝置。測定方法與 上述直接測定相同,將所獲得之分光透過率之資料經由特 定之通信電路或記錄媒體輸入至運算部50,並記憶於磁碟 54 °再者,於本實施形態中係使複數個理論分光反射率之 資料以及分光透過率之資料之兩者記憶於磁碟5 4,亦可使 其中任一者記憶於不同之記憶裝置(例如RAM53)。 97436.doc -18- 200532164 圖5係例不衫色攄光片之分光透過率之圖。彩色滤光片基 本具有僅選擇性透過特定波長區域之光的特性,如圖5所 ;彔色之衫色濾光片之情形時透過大概48〇 nms 6〇〇 聰之波長區域的光。即使於該波長區域中亦基本完全透過 (透過率約贈。)光之峰頂平坦部之波長區域寬度為4〇麵 /、他#刀成為透光量衰減(透過率於〇%至1〇〇%之 ^推移)之傾斜部。再者,於本說明書中之分光透過率係將 分=之測定範圍内之最大值設為100%時的相對值。 虽於如傾斜部之透光量較低之波長區域測定膜厚時,則 理論分光反射率與實測分光反射率之背離將變大,故而會 成為心&差之原因。於本發明中’雖然藉由如下述之方 法該背離會減小,然而較好的是即使如此般處理亦應儘量 於透過率較大之波長區域實行測定。為此,於如圖5之分光 透過率中選定具有固定臨限值以上之透過率的波長區域作 為用以膜厚測定之測定波長區域(步驟S3)。 /則疋波長區域之選定亦可藉由膜厚測定裝置之操作員 手動操作而實行,亦可基於預先所設定之臨限值由裝置自 動操作。於手動操作之情形時操作員觀察CRT 61所示之如 圖5之分光透過率選定適當之測定波長區域,並自鍵盤⑼ 輸入該波長區域。此情形時,可考慮測定波長區域之寬度 〇透匕率之平衡而進行選定。另一方面於自動選定之情形 時,敎波長區域選定部57自如圖5之分光透過率之資料求 得成為預先設定之臨限值以上的透過率資料,並選定與此 對應之波長區域作為測定波長區域。又,亦可使操作員觀 97436.doc -19- 200532164 察CRT61所不之如圖5之分光透過率,自鍵盤60輸入適告的 臨限值,從而測定波長區域選定部57選定對應於成為^ 限值以上之透過率資料的波長區域作為測定波長區域。 測定波長區域之寬度越大理論分歧射率與 射率之差值算定之精度越高,而另一方面由透過= ,之誤差將增大。為此,不論選定手動或自動中之任: ㈣ΓΙ慮此等之平衡而選定測定波長區域。於本實施 〜中’基於預先所収之臨限值,測定波長區域選定部 57自動選定有測定波長區域,並選定圖5之分光透過率中透 過率為70%以上的波長區域(大概5〇〇⑽至㈣ 以膜厚測定之測定浊县卩只,. 為用 _ ± 収波長&域。再者,所選定之敎波長區 域暫時記憶於例如RAM 53。 祖其次’進入步驟S4’藉由圖1所示之膜厚測定裝置實測試 料1之分光反射率。此時,自第 射於試料!之上面之: 統〇照射且反 一 面之反射光精由成像光學系統30得以聚 亚猎由分光單元40將該光分光,藉此測定試料!之分光 反射率。藉由分光單元40所測定之實測分光透過率將傳達 至運算部50。 干肘得運 :係表示試料!之實測分光反射率之一例的圖。於實測 射二:出現由透明薄膜處之光干擾所引起之反射 值右试m之透明薄膜並非彩色渡光 於實測分光反射率亦應出現如圖4所示二= 率般之㈣性峰值之重複,然而由於彩色遽光片僅 過特疋波長區域之光,故而僅於如圖6所示之特定 97436.doc -20- 200532164 波長區域出現反射率之峰值。又,即使為特定波長區域内 於透過率幾乎為100%之波長區域亦可獲得與理論分光反 射率相同之反射率特性,然而於除此以外的波長區域隨著 透過率之降低理論分光反射率與實測分光反射率之背離將 、大所’則定之試料1之實測分光反射率暫時記憶於例如 RAM 53。㈣,於本實施形態中係經過可視光整個區域之 較廣波長區域測定實測分光反射率,然而亦可僅就基於上 述分光透過率而選定的測定波長區域測定實測分光反射 率。 其次,進入步驟S5,藉由分光透過率校正儲存於磁碟54 之理論分光反射率。此時,於基於上述分光透過率而選定 之測定波長區域之範圍内實行校正。χ,就各個相應於不 同膜厚之透明薄膜之複數個理論分光反射率實行校正。具 體的是校正部55按照以下之算式1校正理論分光反射率,、 [算式1] R,(X)=T(X)-R(X) 、於异式1中,Ι1(λ)為波長λ處之理論分光反射率之值,τ(λ) 為波長入處之分光透過率之值(嚴格而言係將透過率画設 為而正規化之值),R⑻為校丨後之波長入處之理論分光反 射率之值即m卩將理論分光反射率r⑻乘以分光 透過率τ(λ),藉此算出校正後理論分光反射率rw。 圖7係概㈣說明由分光透過率而得出之理論分光反射 率的校正之圖。同圖中上側圖之實線表示校正前之理論分 先反射率,虛線表示校正後之理論分光反射率。如上所述, 97436.doc -21 - 200532164 於刀光透過率存在透過率幾乎為的峰頂平坦部以及 透、率於0/〇至100%之間推移的傾斜部,於對應於蜂頂平坦 部之波長區域理論分光反射率與校正後理論分光反射率為 大致相同的值。而另-方面,於對應於分光透過率之傾斜 部的波長區域,校正後理論分光反射率相應於分光透過率 之值亦將低於校正前。校正部55就相應於不同膜厚之透明 缚膜所求得之各個複數個理論分光反射率實行此種校正,Next, the processing steps of the 臈 thickness measuring method of the present invention are added. Fig. 3 shows the flow of the processing steps of the film thickness measuring method of the present invention. Here, 'the spectroscopic reflectance measurement obtained by irradiating light to the test is described. The step of changing the thickness of the color phosphor film, the above-mentioned sample ^ is formed on the substrate with a green color light film as a film. In addition, of course, it is not limited to, and = :, the film thickness of other colors such as phosphor film or red phosphor film can also be measured in the same procedure. First, a transparent step (si) is obtained in which the spectral reflectance of a sample formed on a substrate is set to a thickness. The theoretical spectral reflectance is f + reflection ^ Shi Xiba ^ Calculate the spectral reflectance of the article under the following conditions, and this condition is formed with the 97436.doc -16- 200532164 color filter as the measurement object A bright film having a specific film thickness d is formed on the same substrate as the substrate, and white light is incident on the colorless transparent film from the (lighting optical system 10). Furthermore, the so-called "reflectance" in this specification It is the ratio of the reflection intensity to the reflection intensity when the transparent film is not strictly formed on the substrate (the film thickness is zero), that is, the relative reflectance.: The spectroscopic reflectance is based on the colorless transparent films with different film thicknesses. Calculate 'these colorless transparent films with different film thicknesses d are within a fixed range corresponding to the film thickness of the color filter to be measured (for example, if the film thickness of the beta color calender of the measurement target is hundreds of coffees) The range is from 100μ to 丨 _c) is set at equal intervals (for example, 10 nm pitch). Because light interference occurs in the transparent film, the reflectance of the wavelengths where the light strengthens with each other becomes higher, and the mutual reflection decreases. The wavelength reflectance is reduced. The conditions for generating light interference are determined by the film thickness of the transparent film, so the pattern of the spectral reflectance is different based on the film thickness theory. Therefore, 'the theoretical spectral reflectance can be based on the light interference conditions for different film thicknesses. Figure 4 is a graph illustrating the theoretical spectral reflectance of colorless transparent films with different film thicknesses. Figure 4 (a) is the theoretical spectral reflectance of transparent films with thicker films, and (b) is the The theoretical spectral reflectance of a transparent film with a thinner film thickness. As shown in Figure 4, the thinner the film thickness, the lower the pattern period of the theoretical spectral reflectance. That is, the peaks and valleys of the theoretical spectral reflectance in a fixed wavelength region will decrease. Data corresponding to the theoretical spectral reflectance of such transparent films with different film thicknesses calculated in advance will be stored in the magnetic disk 54. Next, the process proceeds to step S2 to obtain the knife light transmittance of the color filter as the measurement target. Color filter The spectral transmittance of the film can also be measured directly in the film thickness measurement of 97436.doc 200532164 set in Figure 1, or it can also be measured in advance. That is, it can transmit the entire area of visible light. When a color filter is formed on a glass substrate, directly measure the spectral transmittance of 20 using the second illumination optical system, and use a pre-measurement when a color filter is formed on a silicon substrate that is opaque to visible light. When the color filter is formed on the glass substrate, the substrate itself can transmit light directly, so the spectral transmittance can be measured directly. At this time, the sample is irradiated from the second illumination optical system 20 and transmitted through the sample. The substrate and the color filter) are focused by the imaging optical system 30, and the light is split by the spectroscopic unit 40 to determine the spectral transmittance of the color filter. Measured by the spectroscopic unit 40 The spectral transmittance will be transmitted to the calculation unit 50 and stored in the magnetic disk 54. On the other hand, when a color filter is formed on a silicon substrate, the substrate itself cannot transmit light, so the spectral transmittance cannot be directly measured. Use a transparent substrate (such as a glass substrate) formed with a color filter that has the same material and the same thickness as the color filter to be measured. ) Previously measured spectral transmittance. The film thickness measuring device of this embodiment can also be used to measure the spectral transmittance of a color filter and a light sheet using such a sample for a vision device ', or other devices for measuring the spectral transmittance can be used. The measurement method is the same as the above-mentioned direct measurement. The obtained spectral transmittance data is input to the calculation unit 50 through a specific communication circuit or recording medium, and is stored in the magnetic disk 54 °. Furthermore, in this embodiment, a plurality of data are used. Both the theoretical spectral reflectance data and the spectral transmittance data are stored in the magnetic disk 54, and either of them can be stored in a different memory device (such as RAM53). 97436.doc -18- 200532164 Fig. 5 is a graph showing the spectral transmittance of an example of a non-shirt colored calender. The color filter basically has the characteristic of selectively transmitting only light in a specific wavelength region, as shown in FIG. 5; in the case of a black shirt color filter, it transmits light in a wavelength region of about 48 nms to 600 cong. Even in this wavelength region, it is almost completely transmitted (transmittance is about free.) The width of the wavelength region of the flat portion of the peak of light is 40 planes, and the light transmission is attenuated (the transmittance is between 0% and 10%. 〇% 之 推移) the inclined portion. In addition, the spectral transmittance in this specification is a relative value when the maximum value in the measurement range of minutes = is set to 100%. When the film thickness is measured in a wavelength region where the light transmittance of the inclined portion is relatively low, the deviation between the theoretical spectral reflectance and the actual spectral reflectance will increase, and this will be the cause of poor heart & In the present invention, although the deviation is reduced by the method described below, it is preferable that the measurement should be performed in a wavelength region with a large transmittance as much as possible even in such a treatment. For this reason, in the spectral transmittance shown in Fig. 5, a wavelength region having a transmittance of a fixed threshold value or more is selected as a measurement wavelength region for film thickness measurement (step S3). / The selection of the 疋 wavelength region can also be performed manually by the operator of the film thickness measuring device, or it can be automatically operated by the device based on a preset threshold. In the case of manual operation, the operator observes the spectral transmittance shown in CRT 61 as shown in Figure 5 and selects an appropriate measurement wavelength region, and enters the wavelength region from the keyboard ⑼. In this case, the measurement can be made by considering the balance of the wavelength range and the transmittance. On the other hand, in the case of automatic selection, the chirped-wavelength region selection unit 57 obtains transmittance data that is greater than a predetermined threshold from the data of the spectral transmittance in FIG. 5, and selects the corresponding wavelength region as the measurement Wavelength region. In addition, the operator can observe 97436.doc -19- 200532164 to observe the spectral transmittance of CRT61, as shown in FIG. 5, and input the appropriate threshold value from the keyboard 60 to measure the wavelength region selection unit 57 corresponding to the ^ The wavelength region of the transmittance data above the limit is used as the measurement wavelength region. The greater the width of the measurement wavelength range, the higher the accuracy of the theoretical difference between the emissivity and the emissivity. On the other hand, if the transmission =, the error will increase. To this end, regardless of whether manual or automatic is selected: ㈣ΓΙ selects the measurement wavelength region in consideration of these balances. In this implementation, the measurement wavelength region selection unit 57 automatically selects the measurement wavelength region based on the threshold value received in advance, and selects a wavelength region with a transmittance of 70% or more (approximately 50%) in the spectral transmittance of FIG. 5. ⑽ to ㈣ The measurement of the film thickness in Zhuxian County is based on the measurement of the film thickness. The wavelength range of 波长 ± is used to capture the wavelength & domain. Furthermore, the selected wavelength range of 暂时 is temporarily stored in, for example, RAM 53. The next step is to proceed to step S4 by The specular reflectance of the test material 1 of the film thickness measuring device shown in FIG. 1 at this time. Since the first shot on the sample! Above: The reflected light from the other side is illuminated by the imaging optical system 30. The spectroscopic unit 40 splits the light, thereby measuring the spectroscopic reflectance of the sample. The measured spectroscopic transmittance measured by the spectroscopic unit 40 is transmitted to the computing unit 50. The dry elbow is transported: the measured spectroscopic reflection indicating the sample! An example of the rate. In the actual measurement shot two: the reflection value caused by the light interference at the transparent film appears. The transparent film of the right test m is not colored. The measured spectral reflectance should also appear as shown in Figure 4. Two = rate Like The peaks are repeated. However, since the color phosphor film only passes light in the special wavelength region, the reflectance peak appears only in the specific 97436.doc -20-200532164 wavelength region shown in FIG. 6. Also, even for a specific wavelength In the region where the transmittance is almost 100%, the same reflectance characteristics as the theoretical spectral reflectance can be obtained. However, in other wavelength regions, the transmittance decreases with the decrease of the theoretical spectral reflectance and the measured spectral reflectance. The measured spectral reflectance of sample 1 which deviates from the general rule, is temporarily stored in, for example, RAM 53. Alas, in this embodiment, the measured spectral reflectance is measured through a wider wavelength region of the entire area of visible light, but it may be only The measured spectral reflectance is measured based on the measurement wavelength region selected based on the aforementioned spectral transmittance. Next, the process proceeds to step S5 to correct the theoretical spectral reflectance stored in the magnetic disk 54 by the spectral transmittance. At this time, based on the aforementioned spectral transmittance The calibration is performed within the selected measurement wavelength range. Χ, a plurality of principles for each transparent film corresponding to a different film thickness On the implementation of correction of the spectral reflectance. Specifically, the correction unit 55 corrects the theoretical spectral reflectance according to the following formula 1. [Equation 1] R, (X) = T (X) -R (X) , I1 (λ) is the value of the theoretical spectral reflectance at the wavelength λ, τ (λ) is the value of the spectral transmittance at the wavelength input (strictly speaking, the transmittance is plotted as the normalized value), R⑻ The value of the theoretical spectral reflectance at the wavelength after calibration is m 卩. The theoretical spectral reflectance r 反射 is multiplied by the spectral transmittance τ (λ) to calculate the theoretical theoretical spectral reflectance rw after correction. Figure 7 is a summary A graph illustrating the correction of the theoretical spectral reflectance derived from the spectral transmittance. The solid line in the upper side of the same figure indicates the theoretical spectral reflectance before correction, and the dashed line indicates the theoretical spectral reflectance after correction. As mentioned above, 97436.doc -21-200532164 has a peak top flat portion with almost the transmittance and a slant portion whose transmittance shifts between 0/0 and 100% in the knife light transmittance, corresponding to the flat top. The theoretical spectral reflectance of the wavelength region is approximately the same as the theoretical spectral reflectance after correction. On the other hand, in the wavelength region of the inclined portion corresponding to the spectral transmittance, the value of the theoretical spectral reflectance corresponding to the spectral transmittance after correction will also be lower than that before the correction. The correction section 55 performs such correction on each of a plurality of theoretical spectral reflectances obtained corresponding to transparent film with different film thicknesses.

=异定複數個校正後理論分光反射率。再者,於本實施形 恶中由於選定分光透過率中透過率為70%以上的波長區域 作為用以膜厚測定的測定波長區域,故而由校正所引起之 降低率的最大值為30%左右。 、其次’進入步驟S6,膜厚算出部56藉由比較校正後理論 二反射率與Λ測分光反射率,算出成為測定對象之彩色 f光片的膜厚。具體的是,首先膜厚算出部56依據其次之 异W算出於步驟以所測定之實測分光反射率與膜厚廿之透= Theoretical spectroscopic reflectance after correction. Furthermore, in this embodiment, a wavelength region having a transmittance of 70% or more in the spectral transmittance is selected as a measurement wavelength region for film thickness measurement. Therefore, the maximum value of the reduction rate due to correction is about 30%. . Next, the process proceeds to step S6, and the film thickness calculating unit 56 calculates the film thickness of the color f-light sheet to be measured by comparing the corrected theoretical second reflectance with the Δ spectroscopic reflectance. Specifically, first, the film thickness calculation unit 56 calculates the transmission of the measured spectral reflectance and the thickness of the film according to the difference in the next step.

明薄膜之校正後理論分光反射率的差值D(d)。 [算式2]The difference D (d) of the corrected theoretical spectral reflectance of the thin film. [Equation 2]

叫)=]*{11’(入,d)-S〇)}2cR ;#式2中,r (λ,d)為就膜厚d之透明薄膜之波長人處之 ^^後理論分光反射率的值,δ(λ)為波長λ處之實測分光反 、、率的值再者,异式2之積分範圍係基於上述分光透過率 ;ν驟S3所迠定之測定波長區域。又,亦可代替計算y (入, )二、(λ)之差的平方而計异絕對值。膜厚算出部56依據算式 2异出各個不同膜厚之透明薄膜之複數個校正後理論分光 97436.doc -22- 200532164 反射率與實測分光反射率之差值。 繼而,膜厚算出部56於以上述方式所獲得之複數個差值 適用曲線擬合法求得差值為最小的膜厚值,並將該膜厚值· β又為測疋對象之彩色濾光片之膜厚。具體的是膜厚算出部 56使表不將實測分光反射率與各個不同膜厚之透明薄膜之 複數個校正後理論分光反射率之差值近似為二次曲線時之 最小值的膜厚值為測定對象之彩色濾光片的膜厚。 圖8係概念性表示用以膜厚測定之近似二次曲線的圖。於 圖8之例中,將實測分光反射率與各個膜厚七至&之透明薄 膜之複數個杈正後理論分光反射率之差值D(di)至〇(心)近 似為二次曲線,藉此求得最小差值Dmin,從而算出對應於 。亥取小差值Dmin之膜厚值1。繼而,膜厚算出部%將該膜厚 值dx設為測定對象之彩色濾光片的膜厚。所算定之膜厚值 為、】疋、、Ό果表示於CRT 61,並根據必要可自打印機μ輸 出。 一如上於第1實施形態中,比較藉由分光透過率校正理論分鲁 光反射率之权正後理論分光反射率與實測分光反射率,並 ^疋測疋對象之彩色濾光片之膜厚。如上所述,彩色濾光 系僅擇丨生透過特定波長區域之光者,若於膜厚值相同 之條件下,則於透過率幾乎為1〇〇%之峰頂平坦部之波長區 域理論分光反射率與實測分光反射率-致,然而於除I卩, 外的波長區域隨著透過率降低理論分光反射率與實測分光 , 反射率之背離將增大。,於透過率幾乎為1〇〇%之峰頂平 一 °卩之波長區域理論分光反射率與實測分光反射率之差值 97436.doc -23- 200532164 將成為正確者’而隨著透過率降低則於該波長區域處之理 論分光反射率與實測分光反射率的差值中將會含有較多誤、 差。隨之,為降低此種誤差,較好的是盡可能僅將透過率. 幾乎為_%之峰頂平坦部設為測定波長區域。另一方面, 為提高用以膜厚算定之曲線擬合法的精度,較好的是以盡 可能擴大測定波長區域之方式計算理論分光反射率愈實測 分光反射率的差值。特別是於彩色渡光片之膜厚較薄之情 形時由於分光反射率之波形較為平緩(低頻波形),故而盡可 能擴大測定波長區域之處理係提高曲線擬合法之精度# 鍵點。 於第i實施形態中’藉由分光透過率校正理論分光反射 率’藉此滿足類似如上述之相矛盾的兩個要求。即,若實 行理論分光反射率乘以分光透過率之校正,則可於實行該 校正的波長區域理論分光反射率與實測分光反射率的背離 得以解除且含於兩者之差的誤差會大幅度降低,並且可以 超過峰頂平坦部之方式較廣地設定測定波長區域。其結果· 用以膜厚算定之曲線擬合法之精度將變高,故可實行更正 確的膜厚測定。 、 若進而詳細說明此情形,則係藉由使用加有分光透過率 之理論分光反射率,即使如彩色遽光片般選擇性透過特定 波長區域之光的透明薄膜亦可正確測定其膜厚。尤其即使 . 於彩色濾光片之膜厚變薄之情形時,亦可較廣地設定敎 · 波長區域’故而可提高用以膜厚算m線擬合法的精产。 <2.第2實施形態 > 又 97436.doc -24- 200532164 其次,就本發明之第2實施形態加以說明。第2實施形態 之膜厚測定裝置之裝置構成係與圖卜2所示之p實施形態, 者相同纟膜厚測定方法之處理步驟亦大致與第丄實施形態 相同。第2實施形態與第❻施形態之不同點在於,於算出 彩色濾光片之膜厚時將相應於分光透過率之重量附加至理 論分光反射率與實測分光反射率之差。 於第2實施形態中,於測定彩色渡光片之膜厚時亦實行與 上述圖3之步驟81至85完全相同之處理。繼而,進入步驟 S6膜厚t出# 56藉由比較校正後理論分光反射率與實測 分光反射率’算出成為測定對象之彩色濾光片的膜厚,此 時附加相應於分光透過率之重量。具體的是,膜厚算出部 56依據以下之开式3异出實測分光反射率與關於膜厚d之透 明薄膜之校正後理論分光反射率的附有重量之差值D,⑷。 [算式3] D^d)= iT(X){RXX,d)«S(\)}2d\ 於#式3中R (λ ’ d)為於膜厚d之透明薄膜之波長入處的鲁 校正後理論分s反射率之值,s(x)為波長4之實測分光反 射率的值’ τ(λ)為波長4之分光透過率的值。再者,如上 所述刀光透過率τ(λ)為將透過率100%設為i而正規化之 值。又’算式3之積分範圍係於步驟S3所敎之測定波長區 域。 · 依據算式3,膜厚算出部_分有如下之值,即將校正後· 理响刀光反射率R (λ ’ d)與實測分光反射率⑽)之差的平方 值進而乘以刀光透過率τ(λ)的值。分光透過率τ(χ)為將透過 97436.doc •25- 200532164 率100%設為!而正規化之值,故而於算式3中,係將分光透 過率Τ(λ)越高則會越重之重量附加至校正後理論分光反射 率(d)契只測分光反射率S⑻之差值。_ ,可認為對應 於透過率幾乎為職之峰頂平坦部的波長區域之差優於 對應於透過率於跑嶋之間推移之傾斜部的波長區域 之差。再者’膜厚算出部56與上述^實施形態相同地依據 算式3算出各個不同膜厚之透明薄膜之複數個校正後理論 分光反射率與實測分光反射率的附有重量之差。 膜厚算出部56 ’於以上述方式所獲得之複數個附有重量 之差值使用曲線擬合法求得差為最小的膜厚值,並將該臈 厚值設為測定對象之彩色濾'光片的膜厚1,與上述第! 實施形態同樣’使表示將所獲得之複數個附有重量之差近 似為二次曲線時之最小值的膜厚值作為測定對象之彩色濾 光片的膜厚。 & 於第2實施形態中,將分光透過率越高則越重之重量附加 至校正後理論分光反射率與實測分光反射率之差值。若如 第1實施形態般處理,則可於分光透過率中大幅度降低含於 透過率變低之波長區域處之理論分光反射率與實測分光反 射率的差之誤差,然而即便如此,依然係透過率幾乎為 100%之岭頂平坦部之波長區域處之理論分歧射率與實 測分光反射率的差可靠性較高。故而,於第2實施形離中, 可較高評價此種可靠性較高之差,且透過率越低可靠性越 低之差評價較低。若如第2實施形態般處理,則用以膜厚算 定之曲線擬合法的精度將進—步提高,即使如彩色渡光7 97436.doc -26- 200532164 般選擇性透過特定波長區域之光 測定其膜厚。 月潯朕亦可更為正確 <3·變形例> 二二本發明之實施形態加以了說明,然而本發明並 非僅限於上述之例者。例如於上述各 由分光透過率校正各個複數個理論分光二中,:為: 代此處理藉由分光透過率校正實測^先反^主但亦可替 、、刀光反射率。且體的 二校正部55藉由分㈣過率除去實测分光反射率'、藉此 异出杈正後實測分光反射率。其 曰 认八氺& “ t 膜;π出部56比較理 =反射率與校正後實測分光反射率,藉此算出成為測 :=彩色遽光片的膜厚。此時之比較方法與上述實施 :同。即使以此方式處理,於實行該校正之波長區域 於理論分光反射率與實測分光反射率之差的誤差將 士幅度降低,且用以膜厚算定之曲線擬合法的精度會變 尚,所以可實行更正確的膜厚測定。 即,隨著彩色遽光片之透過率降低m解除變大之 理論分光反射率與實測分光反射率之背離之方式,籍由分 光透過率校正理論分光反射率或實測分光反射率之任— 者,則含於理論分光反射率與實測分光反射率之差的誤差 將得以降低’因此即使如彩色據光片般選擇性透過特定波 長區域之光的透明薄膜亦可正確測定其膜厚。 又,於上述實施形態中,設為分別取得分光透過率盘理 論分光反射率而校正,然而若已知彩色遽光片之種類:、且 已求得該分光透過率以及理論分光反射率,則亦可使預先 97436.doc >27- 200532164 記憶 藉由分光透過率而得以校 仪止之杈正後理論分光反射率 於磁碟54。 、,又,於上述實施形態巾,測定彩色濾、光片之膜厚,然而 並非僅限於$色濾、光片,即使於可視光區域中測定透過率 為非均之透明薄膜之膜厚的情形亦可使用本發明之技 術。 [產業上之可利用性] 作為本發明之活用例,列舉有於彩色CCD之製造步驟中 測定形成於半㈣基板上之彩色濾光片的膜厚之處理或於 放映機之製造步驟中敎形成於液晶玻璃基板上之彩色滤 光片的膜厚之處理等。 【圖式簡單說明】 圖1係表示本發明之膜厚測定裝置之構成的圖。 圖2係表示圖丨之膜厚測定裝置之運算部之構成的方塊 圖3係表示本發明之膜厚測定方法之處理步驟的流程圖。 圖4(a)至(b)係例示就不同膜厚之透明薄膜得以算定之理 論分光反射率的圖。 圖5係例示彩色濾光片之分光透過率的圖。 圖6係表示測定對象之試料之實測分光反射率之一例的 圖0 圖7係概念性說明由分光透過率而得出之理論分光反射 率之校正的圖。 圖8係概念性表示用以膜厚測定之近似二次曲線的圖。 97436.doc -28 - 200532164 圖9係表示彩色濾光片之透光特性的圖。 圖10係表示自形成有圖9之彩色濾光片的基板所獲得之 分光反射率的圖。 【主要元件符號說明】 1 試料 5 樣品台 10 第1照明光學系統 11,21 鹵素燈 20 第2照明光學系統 30 成像光學系統 32 半反射鏡 40 分光單元 50 運算部 54 磁碟 55 校正部 56 膜厚算出部 57 測定波長區域選定部 97436.doc - 29 -(Named) =] * {11 '(in, d) -S〇)} 2cR; # In Formula 2, r (λ, d) is the theoretical spectral reflection of the wavelength of the transparent film with a thickness of d. The value of the ratio, δ (λ) is the measured spectral reflectance at the wavelength λ, and the value of the ratio. Furthermore, the integration range of the heterogeneous equation 2 is based on the above-mentioned spectral transmittance; the measurement wavelength region determined by the step S3. Alternatively, instead of calculating the square of the difference between y (in,) and (λ), an absolute value may be calculated. The film thickness calculating unit 56 differs from the corrected theoretical spectroscopic 97436.doc -22- 200532164 of each of the transparent films of different film thicknesses according to the formula 2 and calculates the difference between the reflectance and the measured spectral reflectance. Then, the film thickness calculation unit 56 applies a curve fitting method to the plurality of difference values obtained in the above manner to obtain a film thickness value with the smallest difference value, and sets the film thickness value β as the color filter of the measurement target. The film thickness of the sheet. Specifically, the film thickness calculation unit 56 makes the difference between the measured spectral reflectance and the corrected theoretical spectral reflectance of each transparent film with different film thicknesses approximate the minimum film thickness value when the quadratic curve is approximated. The thickness of the target color filter is measured. FIG. 8 is a diagram conceptually showing an approximate quadratic curve for film thickness measurement. In the example of FIG. 8, the difference D (di) to 〇 (heart) of the measured spectral reflectance and the theoretical spectral reflectance of a plurality of transparent films with a thickness of seven to & From this, the minimum difference Dmin is obtained, and the correspondence is calculated. Take the film thickness value 1 with a small difference Dmin. Then, the film thickness calculation section% sets the film thickness value dx as the film thickness of the color filter to be measured. The calculated film thickness values are, 疋, Ό, and Ό are shown in the CRT 61 and can be output from the printer μ if necessary. As described above in the first embodiment, the theoretical spectral reflectance and the measured spectral reflectance are compared by correcting the theoretical spectral reflectance of the theoretical optical reflectance by correcting the spectral transmittance and measuring the film thickness of the target color filter. . As mentioned above, the color filter only selects the light that transmits through a specific wavelength region. If the film thickness is the same, the theoretical spectral splitting is performed in the wavelength region of the flat top of the peak with a transmittance of almost 100%. The reflectance is consistent with the measured spectral reflectance. However, in the wavelength region other than I 随着, as the transmittance decreases, the theoretical spectral reflectance and measured spectral reflectance divergence will increase. The difference between the theoretical spectral reflectance and the measured spectral reflectance in the wavelength region with a transmittance of almost 100% at the peak peak level of 1 ° 卩 will become the correct one. 'As the transmittance decreases, the The difference between the theoretical spectral reflectance and the measured spectral reflectance at this wavelength region will contain more errors and differences. Accordingly, in order to reduce such an error, it is preferable to set only a peak top flat portion of the transmittance as much as possible to the measurement wavelength region. On the other hand, in order to improve the accuracy of the curve fitting method used for film thickness calculation, it is better to calculate the difference between the theoretical spectral reflectance and the actual measured spectral reflectance in such a way that the measurement wavelength region is enlarged as much as possible. Especially in the case of thin film thickness of the color crossing sheet, the spectral reflectance waveform is smoother (low-frequency waveform), so the processing of expanding the measurement wavelength region as much as possible is to improve the accuracy of the curve fitting method # key point. In the i-th embodiment, 'the theoretical spectral reflectance is corrected by the spectral transmittance', thereby satisfying two contradictory requirements similar to those described above. That is, if the correction of the theoretical spectral reflectance times the spectral transmittance is implemented, the deviation between the theoretical spectral reflectance and the measured spectral reflectance in the wavelength region where the correction is performed can be removed, and the error included in the difference between the two will be greatly increased. The measurement wavelength region can be set in a wide manner so as to exceed the flat portion of the peak top. As a result, the accuracy of the curve fitting method used to calculate the film thickness will be higher, so more accurate film thickness measurement can be performed. If this situation is explained in more detail, it is possible to accurately measure the thickness of a transparent film that selectively transmits light in a specific wavelength region like a color phosphor, by using a theoretical spectral reflectance with a spectral transmittance added. In particular, even when the film thickness of the color filter becomes thin, it is possible to widely set the 敎 · wavelength region ', so that it is possible to improve the precision of the m-line fitting method for film thickness calculation. < 2. Second Embodiment > Another 97436.doc -24- 200532164 Next, a second embodiment of the present invention will be described. The device configuration of the film thickness measuring device of the second embodiment is the same as that of the p embodiment shown in Fig. 2; the processing steps of the film thickness measurement method are also substantially the same as those of the second embodiment. The difference between the second embodiment and the second embodiment is that the weight corresponding to the spectral transmittance is added to the difference between the theoretical spectral reflectance and the measured spectral reflectance when calculating the film thickness of the color filter. In the second embodiment, when measuring the film thickness of the color doped sheet, the same processing as that of steps 81 to 85 in Fig. 3 described above is performed. Then, the process proceeds to step S6, and the film thickness tout # 56 is calculated by comparing the theoretical spectral reflectance after the correction with the measured spectral reflectance 'to calculate the film thickness of the color filter to be measured. At this time, a weight corresponding to the spectral transmittance is added. Specifically, the film thickness calculation unit 56 differs from the measured spectral reflectance based on the following Equation 3 and the difference D, ⑷ with the weight of the theoretical spectral reflectance after correction of the transparent film with respect to the film thickness d. [Equation 3] D ^ d) = iT (X) {RXX, d) «S (\)} 2d \ In # 3, R (λ 'd) is at the wavelength of the transparent thin film with the thickness d. The corrected theoretical reflectance value of s, s (x) is the measured spectral reflectance value of wavelength 4 'τ (λ) is the spectral transmittance value of wavelength 4. In addition, as described above, the knife light transmittance τ (λ) is a value normalized by setting 100% of the transmittance to i. The integral range of the equation 3 is the measurement wavelength region in step S3. · According to Equation 3, the film thickness calculation unit _ points has the following values, which are about to be corrected. · The squared value of the difference between the R-blade light reflectance R (λ 'd) and the measured specular reflectance ⑽) is multiplied by the knife light transmission. Value of the rate τ (λ). The spectral transmittance τ (χ) is to set the transmittance to 97436.doc • 25- 200532164 as 100%! And the normalized value, so in Equation 3, the higher the spectral transmittance T (λ), the heavier the weight will be added to the corrected theoretical spectral reflectance (d), and only the difference between the spectral reflectance S⑻ will be measured. . It can be considered that the difference in the wavelength region corresponding to the flat portion of the peak top where the transmittance is almost the same is better than the difference in the wavelength region corresponding to the inclined portion where the transmittance shifts between running. In addition, the 'film thickness calculation unit 56 calculates the difference between the weights of the theoretical spectral reflectance and the measured spectral reflectance of each transparent film with different film thicknesses based on Equation 3 in the same manner as in the above-mentioned embodiment. The film thickness calculation unit 56 ′ uses the curve fitting method to obtain the film thickness value with the smallest difference from the plurality of weighted values obtained in the manner described above, and sets the thickness value as the color filter to be measured. The film thickness of the sheet is the same as above! The same applies to the embodiment. The film thickness of the color filter to be measured is a film thickness value obtained when a plurality of the obtained weight differences are close to the minimum value when the quadratic curve is obtained. & In the second embodiment, the higher the spectral transmittance, the heavier the weight is added to the difference between the corrected theoretical spectral reflectance and the measured spectral reflectance. If processed as in the first embodiment, the difference between the theoretical spectral reflectance and the measured spectral reflectance contained in the wavelength region where the transmittance is low can be greatly reduced in the spectral transmittance. However, even this is still the case. The reliability of the difference between the theoretical branched emissivity and the measured spectral reflectance at the wavelength region of the flat portion of the ridge top with a transmittance of almost 100% is high. Therefore, in the second embodiment, such a difference with higher reliability can be evaluated higher, and the lower the transmittance, the lower the difference between reliability and lower evaluation. If it is processed as in the second embodiment, the accuracy of the curve fitting method used for film thickness calculation will be further improved, even if it is selectively transmitted through a specific wavelength region, as in the case of color cross light 7 97436.doc -26- 200532164. Its film thickness. The moon can also be more accurate < 3 · Modifications > The embodiment of the present invention has been described, but the present invention is not limited to the above-mentioned examples. For example, in each of the above two theoretical spectral corrections by the spectral transmittance correction, the following is: Instead of this, the measured optical transmittance correction is used to measure the measured reflectance ^ first, but can also be used instead of, or the knife light reflectance. The two correcting sections 55 of the body remove the measured spectral reflectances' by the splitting pass ratio, thereby measuring the actual spectral reflectances after the difference. It is said that the eight films & "t film; π out section 56 comparison principle = reflectance and the measured spectral reflectance after correction, from which the calculation becomes: = film thickness of the color phosphor film. The comparison method at this time is the same as above Implementation: Same. Even if processed in this way, the error of the difference between the theoretical spectral reflectance and the measured spectral reflectance in the wavelength region where the correction is performed will reduce the amplitude, and the accuracy of the curve fitting method used to calculate the film thickness will remain Therefore, a more accurate measurement of the film thickness can be implemented. That is, as the transmittance of the color phosphor film decreases, the deviation between the theoretical spectral reflectance and the measured spectral reflectance that deviates becomes larger, and the theoretical spectral reflectance is corrected by the spectral transmittance. Any of the reflectance or the measured spectral reflectance, the error contained in the difference between the theoretical spectral reflectance and the measured spectral reflectance will be reduced. Therefore, even as a color data sheet, the transparency of light that selectively transmits through a specific wavelength region is transparent. The thickness of the thin film can also be measured accurately. In the above embodiment, it is assumed that the theoretical spectral reflectance of the spectral transmittance disk is obtained and corrected, however, if the color is known, Type of film: and the spectral transmittance and theoretical spectral reflectance have been obtained, the 97476.doc > 27- 200532164 memory can also be memorized by the spectral transmittance, the theoretical theoretical specular reflection The rate is on the magnetic disk 54. In the above embodiment, the film thickness of the color filter and the light sheet is measured, but it is not limited to the color filter and the light sheet. Even if the transmittance is measured in the visible light region, the transmittance is non-uniform. The technology of the present invention can also be used in the case of the film thickness of a transparent thin film. [Industrial Applicability] As a practical example of the present invention, the color filter formed on the half-half substrate is measured during the manufacturing steps of the color CCD. The processing of the film thickness of the sheet or the processing of the film thickness of the color filter formed on the liquid crystal glass substrate in the manufacturing process of the projector. [Brief Description of the Drawings] FIG. 1 shows a film thickness measuring device of the present invention. Figure 2 is a block diagram showing the structure of the calculation section of the film thickness measuring device of Figure 丨 Figure 3 is a flowchart showing the processing steps of the film thickness measuring method of the present invention. Figures 4 (a) to (b) are Instantiating different films A graph showing the theoretical spectral reflectance of a thick transparent film. Figure 5 is a graph illustrating the spectral transmittance of a color filter. Figure 6 is an example of the actual spectral reflectance of a sample to be measured. Figure 7 A conceptual illustration of the correction of the theoretical spectral reflectance derived from the spectral transmittance. Figure 8 is a conceptual representation of an approximate quadratic curve for film thickness measurement. 97436.doc -28-200532164 Figure 9 shows A diagram showing the light transmission characteristics of a color filter. Fig. 10 is a diagram showing the spectral reflectance obtained from a substrate on which the color filter of Fig. 9 is formed. [Description of Symbols of Main Components] 1 Sample 5 Sample Stage 10 First Illumination optical system 11, 21 Halogen lamp 20 Second illumination optical system 30 Imaging optical system 32 Half mirror 40 Spectral unit 50 Calculation section 54 Disk 55 Calibration section 56 Film thickness calculation section 57 Measurement wavelength region selection section 97436.doc-29 -

Claims (1)

200532164 十、申請專利範圍·· Κ板定方法,其特徵在於:其係自照射光至於基 透^ 有透明薄膜之試料而獲得之分光反射率,測定 上述透明溥膜之膜厚者,且包含·· 過^光透過率取得步驟,其取得上述透明薄膜之分光透 分光反射率测定步驟,其照射光於上述試料,將自上 相料所反射之反射光分光而實測分光反射率. 其藉由上述分光透過率校正作為於基板上 預有特定膜厚之透明薄膜之試料的分光反射率而 預先^疋之理論分光反射率;及 2. 3. 4· 腠厚算出步驟,其比較於上述校正步驟校正之校正後 光反射率'於上述分光反射率測定步驟測定之實 “1刀"反射率’而算出測定對象之透明薄膜之膜厚。、 如請求項1之膜厚測定方法,其中上述臈厚算出步驟,係 附加相應於上述> & ϋ μ $ > p # ’、 边刀先透過率之相值,比較上述校正後理 射率與上述實測分光反射率而算出測定對象之 透明4膜的膜厚。 如請求項⑷之膜厚敎方法,其中進而包含選定上述 ::透過=有特定臨限值以上之透過率的波長區域 ’’、、上述肤厚异出步驟中之測定波長區域之步驟。 一種膜厚測定方法,其特徵在於:其係自照射光至於基 板上形成有透明薄膜之試料而獲得之分光反射率,測定 上述透明薄膜之膜厚者,且包含·· 97436.doc 200532164 分光透過率取得步驟,其取得上述透明薄膜之分光透 過率; 分光反射率測定步驟,其照射光於上述試料,將自上 述试料所反射之反射光分光而實測分光反射率; 杈正步驟’其藉由上述分光透過率校正由上述分光反 射率測定步驟測定之實測分光反射率;及 膜厚异出步驟,其比較作為於基板上形成有具有特定 膜厚之透明薄膜之試料的分光反射率而預先算定之理論 分光反射率與,於上述校正步驟校正之校正後實測分光 反射率,而算出測定對象之透明薄膜之膜厚。 5·種膜厚測疋裝置,其特徵在於:其係自照射光至於基 板上形成有透明薄膜之試料而獲得之分光反射率,測定 上述透明薄膜之膜厚者,且包含: 第。己隐機構,其§己憶上述透明薄膜之分光透過率; θ第2記憶機構,其記憶作為於基板上形成有具有特定膜 厚之透明溥膜之試料的分光反射率而預先算定之理論分 光反射率; 光源,其照射光於測定對象之試料; #光反射率測定機構,其自上述光源被照射光,且將 =測疋對象之試料所反射之反射光分光而測定分光反 ::機構’其藉由上述分光透過率校正上述理論分光 反射率;及 膜厚算出機構,豆比魴 /、比枚於上述校正機構校正之校正後 97436.doc 200532164 6. :光反射率與藉由上述分光反射率測定機構測定之 貫測分光反射率,而算出測定對象之透明薄膜之膜厚。 如請求項5之膜厚測定裝置,其中上述第2記憶機構係記 憶相應於不同膜厘夕;# @ γ J胰与之透明溥胲的禝數個理論分光反射 率; 、上述校正機構係上述複數個理論分光反射率之各個乘 以上述分光透過率而算出複數個校正後理論分光反射 率; J 上述膜厚算出機構係求得上述複數個校正後理論分光 反射=之各個與上述實測分光反射率之差,並使表示將 所獲传之複數個差近似二次曲線時之最小值的膜厚值作 為測定對象之透明薄膜之膜厚。 如請求項6之膜厚測定装置,其中上述膜厚算出機構係對 數個校正後理論分光反射率之各個與上述實測分 光反射率之差進行上述分光透過率越高則越重之類的加 H ’亚使表示將所獲得之複數個加權差近似二次曲線時 8. 9· 之最小值_厚值作為敎對象之透㈣膜之膜厚。 如請求項5至7中任一 夕赠陪、丨 ^ 、之膑厗測定裝置,其中進而包含 選定上述分光透過率之具有特定臨限值以上之透過率的 2區域作為膜厚算出時之測定波長區域之 定機構。 一種膜厚測定裝置,並 4 _ ,、特敛在於··其係自照射光至於基 ^ :成有透明㈣之試料而獲得之分光反射率,測定 上述透明薄膜之膜厚者,且包含·· 97436.doc 200532164 第1記憶機構,其記憶上述透明薄膜之分光透過率; 第2記憶機構,其記憶作為於基板上形成有具有特定膜 厚之透H膜之試料的分光反射率而預先算定之理論分 光反射率; 光源,其照射光於測定對象之試料; 由 率 分光反射率測定機構,纟自上述光源照射光,且將藉 測疋對象之5式料所反射之反射光分光而測定分光反射200532164 10. Scope of application for patents ... The K plate method is characterized in that it is the spectral reflectance obtained from irradiating light to a base transparent sample with a transparent film, and measuring the film thickness of the above transparent cymbal film, and includes The light-transmittance obtaining step obtains the spectroscopic and spectral reflectance measurement steps of the transparent film, which irradiates light onto the sample, and spectroscopically reflects the reflected light reflected from the upper phase material to measure the spectral reflectance. The theoretical spectral reflectance corrected in advance as the spectral reflectance of a sample of a transparent film having a specific film thickness on the substrate is corrected from the above spectral transmittance; and 2.3.4. The thickness calculation step, which is compared with the above The corrected light reflectance after correction in the correction step is calculated as "1 knife" and "reflectance" measured in the above-mentioned spectral reflectance measurement step to calculate the film thickness of the transparent film to be measured. For the method for measuring the film thickness of item 1, Wherein, the above-mentioned thickness calculation step is added with a phase value corresponding to the above-mentioned > & ϋ μ $ > p # ', first edge transmittance, and comparing the corrected emissivity Based on the above-mentioned measured spectral reflectance, the film thickness of the transparent 4 film to be measured is calculated. If the method of the film thickness of the item 请求 is requested, it further includes the selection of the above: :: transmission = wavelength region with a transmittance above a certain threshold value " A method for measuring a wavelength region in the above-mentioned skin thickness difference step. A method for measuring a film thickness, characterized in that it is a spectral reflectance obtained by irradiating light to a sample having a transparent film formed on a substrate, and measuring the transparency The thickness of the thin film includes: 97436.doc 200532164 Spectral transmittance obtaining step, which obtains the spectral transmittance of the transparent film; Spectral reflectance measuring step, which irradiates light onto the sample, and reflects from the sample The spectroscopic reflectance is measured by reflecting the reflected light; the positive step 'corrects the measured spectral reflectance measured by the above-mentioned spectral reflectance measuring step by the above-mentioned spectral transmittance; and the film thickness difference step, which is compared as forming on the substrate Spectral reflectance of a sample with a specific thickness of a transparent film After measuring the spectral reflectance after the correction in the above-mentioned correction step, calculate the film thickness of the transparent film to be measured. 5. A film thickness measuring device, which is characterized in that it irradiates light to a transparent film formed on the substrate Spectral reflectance obtained from the sample, the thickness of the transparent film is measured, and includes: the first hidden mechanism, which § recalls the spectral transmittance of the transparent film; θ second memory mechanism, whose memory is used as the substrate A theoretical spectroscopic reflectance calculated in advance on a spectroscopic reflectance of a sample having a transparent film with a specific film thickness is formed thereon; a light source that irradiates light to a sample to be measured; # a light reflectance measuring mechanism that is irradiated from the light source Light, and spectroscopic reflection is measured by splitting the reflected light reflected from the sample of the measuring object :: mechanism 'which corrects the above-mentioned theoretical spectral reflectance by the above-mentioned spectral transmittance; and the film thickness calculation mechanism, bean ratio / ratio After correction by the above-mentioned correction mechanism 97436.doc 200532164 6 .: Light reflectance and continuous measurement by the above-mentioned spectral reflectance measurement mechanism Light reflectance, calculates the thickness of the transparent film of the object to be measured. For example, the film thickness measuring device of claim 5, wherein the second memory mechanism stores a number of theoretical spectral reflectances corresponding to different film thicknesses; # @ γ J Multiplying each of the plurality of theoretical spectral reflectances by the above-mentioned spectral transmittance to calculate a plurality of corrected theoretical spectral reflectances; J The film thickness calculation mechanism obtains each of the plurality of corrected theoretical spectral reflectances = and each of the above-mentioned measured spectral reflections The film thickness of the transparent film to be measured is the film thickness value that represents the minimum value when the obtained plural differences approximate the quadratic curve. For example, the film thickness measuring device according to claim 6, wherein the film thickness calculation mechanism performs the addition of H to the above-mentioned spectral transmittance for the difference between each of the corrected theoretical spectral reflectances and the measured spectral reflectance. 'Asian' represents the minimum value of 8. 9 · _thickness when the obtained multiple weighted differences approximate the quadratic curve as the film thickness of the transparent membrane of the object. For example, if any of the items 5 to 7 is included in the measurement device, it further includes the measurement of the film thickness when the 2 regions having the above-mentioned spectral transmittance having a specific threshold value or higher are selected as the film thickness calculation. The fixed mechanism of the wavelength region. A film thickness measuring device is specifically designed to measure the film thickness of the above-mentioned transparent thin film, including the spectral reflectance obtained by irradiating light onto the substrate ^: a sample with a transparent tincture, and including · 97436.doc 200532164 The first memory mechanism memorizes the spectral transmittance of the transparent film; the second memory mechanism memorizes the spectroscopic reflectance of a sample having a specific film thickness of a transparent H film formed on the substrate. Theoretical spectral reflectance; light source, which irradiates light to the sample to be measured; a spectroscopic reflectance measuring mechanism, irradiates light from the light source, and spectrophotometrically measures the reflected light reflected from the 5th material of the target Spectral reflection 校正機構,其藉由上述分光透過率校正藉由上述分光 反射率敎機構所敎之㈣分光反射率;及 —膜厚算出機構’其比較於上述校正機構校正之校正後 只測刀光反射率與上述理論分光反射率,而算出測定對 象之透明薄膜之膜厚。 ίοA correction mechanism that corrects the spectral reflectance determined by the spectral reflectance measurement mechanism described above with the spectral transmittance; and a film thickness calculation mechanism that measures only the light reflectance of the knife after the correction corrected by the correction mechanism described above Calculate the film thickness of the transparent thin film to be measured with the theoretical spectral reflectance. ίο -徑…疋裝置,其特徵在於:其係自照射光至於 板上形成有透明薄膜之試料而獲得之分光反射率,測 上述透明薄臈之臈厚者,且包含: 第1光源,纟照射光至上述試料之薄膜形成面; 第2光源,其照射光至與上述試料之上述薄膜形成面 反側之面; 分光機構,i將白μ、+、结。 、 、、/、、 述第2光源所照射且透過上述基板 八ΠΓ Γ明:專膜的透過光分光而測定上述透明薄膜之 二所反:之’並且將自上述第1光源所照射且藉由上述試 " 、之反射光分光而測定分光反射率; L機構’其€憶作為於基板上形成有具有特定膜厚 97436.doc 200532164 之透明薄膜之試料的分光反射率而預先算定之理論分光 反射率; 校正機構,其藉由以上述分光機構所測定之上述分光 透過率校正上述理論分光反射率;及 理,出機構’其比較於上述校正機構校正之校正後 :刀光反射率與藉由上述分光機構敎之實測分光反 射率,而算出測定對象之透明薄膜之膜厚。 97436.doc-A diameter ... thickness device, characterized in that it is a spectral reflectance obtained from irradiating light to a sample on which a transparent film is formed on the board, and the thickness of the above-mentioned transparent thin film is measured, and includes: a first light source, thallium radiation Light is applied to the film formation surface of the sample; a second light source irradiates light to a surface opposite to the film formation surface of the sample; a spectroscopic mechanism, i will be white, μ, and +. ,,, / ,, and the second light source is irradiated and transmitted through the substrate Π Γ Γ Γ: the spectroscopic transmission of the light is measured to determine the second and the opposite of the transparent film: '' and will be irradiated from the first light source and borrowed The spectroscopic reflectance is measured from the above-mentioned test by spectroscopic reflection of light; the L mechanism is a theory that is calculated in advance as the spectroscopic reflectance of a sample having a transparent film with a specific film thickness of 97436.doc 200532164 formed on a substrate. Spectral reflectance; a correction mechanism that corrects the theoretical spectral reflectance by using the spectroscopic transmittance measured by the spectroscopic mechanism; and a mechanism that compares the correction with the correction by the correction mechanism: Based on the actual spectral reflectance measured by the spectroscopic mechanism, the film thickness of the transparent thin film to be measured is calculated. 97436.doc
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