TWI575220B - Thin-film curvature measurment apparatus and method thereof - Google Patents
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Description
本揭露係有關於一種薄膜曲率量測裝置及其方法。The present disclosure relates to a film curvature measuring device and method thereof.
半導體材料在磊晶沉積的過程中,若磊晶基板的晶格常數與沉積材料差異過大時,例如使氮化鎵(Ga l l ium ni t r ide , GaN)成長在矽(s i l i con, Si )基板上,兩材料之間會存在有內建應力,而使基板彎曲形成曲面。這樣的現象會使得磊晶品質降低而影響製程品質,並且造成製造成本的提高。因此,若能在磊晶過程中,即時監控基板的曲率變化,並藉此即時掌握內建應力在哪一層結構中最為明顯,進而調整相對應的參數以降低內建應力,實乃各家廠商皆在研究之課題。In the process of epitaxial deposition of a semiconductor material, if the lattice constant of the epitaxial substrate is too different from the deposited material, for example, gallium nitride (GaN) is grown on a sili con (Si) substrate. There is a built-in stress between the two materials, and the substrate is bent to form a curved surface. Such a phenomenon causes the epitaxial quality to be lowered to affect the process quality, and the manufacturing cost is increased. Therefore, if the curvature change of the substrate can be monitored in the epitaxial process, and the structure of the built-in stress is most obvious in the structure, and the corresponding parameters are adjusted to reduce the built-in stress, it is a manufacturer. All are in the subject of research.
根據本揭露一實施例中的一種薄膜曲率量測裝置,此薄膜曲率量測裝置包含發光模組、至少一第一光學模組、至少一第二光學模組與影像分析模組。發光模組用以發射至少一第一光線以作為入射光,入射光形成第一幾何圖形。至少一第一光學模組用以提供至少一第一光學路徑,以使入射光經由第一光學路徑入射至薄膜。至少一第二光學模組用以提供第二光學路徑,以使經薄膜反射的反射光沿第二光學路徑傳播。影像分析模組根據反射光所形成的第二幾何圖形,判斷出薄膜的曲率,第二幾何圖形具有至少一特徵。其中,第二幾何圖形的至少一特徵與第一幾何圖形不同,至少一特徵係為第二幾何圖形的長度、至少一對平行線間的距離、第二幾何圖形的周長與第二幾何圖形的面積中的至少其中之一。According to an embodiment of the present disclosure, a film curvature measuring device includes a light emitting module, at least one first optical module, at least one second optical module, and an image analyzing module. The light emitting module is configured to emit at least one first light as incident light, and the incident light forms a first geometric figure. The at least one first optical module is configured to provide at least one first optical path to cause incident light to be incident on the film via the first optical path. The at least one second optical module is configured to provide a second optical path to propagate the reflected light reflected by the thin film along the second optical path. The image analysis module determines the curvature of the film according to the second geometric shape formed by the reflected light, and the second geometric pattern has at least one feature. Wherein at least one feature of the second geometric figure is different from the first geometric figure, the at least one feature being a length of the second geometric figure, a distance between the at least one pair of parallel lines, a circumference of the second geometric figure, and a second geometric figure At least one of the areas.
根據本揭露一實施例中的一種薄膜曲率量測方法,此薄膜曲率量測方法適用於量測待測薄膜的曲率。薄膜曲率量測方法首先發射一第一光線以作為一入射光,該入射光的截面形狀係為一第一幾何圖形,並使入射光經由第一光學路徑傳播。再引導沿第一光學路徑傳播的入射光入射薄膜。引導經薄膜反射的反射光進入第二光學路徑,且反射光的截面形狀係為具有至少一特徵的第二幾何圖形。然後擷取傳播反射光,並根據反射光的截面形狀的具有至少一特徵的第二幾何圖形,判斷出薄膜的曲率。其中,第二幾何圖形包含矩形,至少一特徵包含矩形的長、寬或長寬的比值至少其中之一。According to a film curvature measuring method according to an embodiment of the present disclosure, the film curvature measuring method is suitable for measuring the curvature of the film to be tested. The film curvature measurement method first emits a first light as an incident light, and the cross-sectional shape of the incident light is a first geometric shape, and the incident light is propagated through the first optical path. The incident light propagating along the first optical path is then directed to the film. The reflected light reflected by the film is guided into the second optical path, and the cross-sectional shape of the reflected light is a second geometric figure having at least one feature. Then, the reflected light is extracted, and the curvature of the film is determined according to the second geometric shape having at least one feature of the cross-sectional shape of the reflected light. Wherein, the second geometric figure comprises a rectangle, and the at least one feature comprises at least one of a ratio of a length, a width or a length and a width of the rectangle.
以上關於本揭露的內容及以下關於實施方式的說明係用以示範與闡明本揭露的精神與原理,並提供對本揭露的申請專利範圍更進一步的解釋。The above description of the disclosure and the following description of the embodiments are intended to illustrate and clarify the spirit and principles of the disclosure, and to provide a further explanation of the scope of the disclosure.
以下在實施方式中敘述本揭露之詳細特徵,其內容足以使任何熟習相關技藝者瞭解本揭露之技術內容並據以實施,且依據本說明書所揭露之內容、申請專利範圍及圖式,任何熟習相關技藝者可輕易地理解本揭露相關之目的及優點。以下實施例係進一步說明本揭露之諸面向,但非以任何面向限制本揭露之範疇。The detailed features of the disclosure are described in the following description, which are sufficient for any person skilled in the art to understand the technical content of the disclosure and implement it according to the disclosure, the scope of the patent application and the drawings. The objects and advantages associated with the present disclosure can be readily understood by those skilled in the art. The following examples are intended to further illustrate the aspects of the disclosure, but are not intended to limit the scope of the disclosure.
需先一提的是,為使圖式簡明易懂,所附圖式均為簡化之示意圖,僅以示意方式說明本發明之基本結構與方法。因此,所顯示之元件並非以實際實施時之數目、形狀、尺寸比例等加以繪製,其實際實施時之規格尺寸實為一種選擇性之設計,且其元件佈局形態可能更為複雜,先于敘明。It is to be understood that the drawings are a simplified schematic and are merely illustrative of the basic structure and method of the invention. Therefore, the components shown are not drawn in the actual number, shape, size ratio, etc., and the actual size of the implementation is a selective design, and the component layout may be more complicated. Bright.
請參照圖1,圖1係本揭露一實施例中薄膜曲率量測裝置的功能方塊示意圖。如圖1所示,本揭露的薄膜曲率量測裝置適用於量測待測薄膜4的曲率,且此薄膜曲率量測裝置包含發光模組1、第一光學模組2、第二光學模組3、第三光學模組5、影像擷取模組6以及影像分析模組7。其中影像擷取模組6電性連接影像分析模組7,其餘各功能模組1、2、3、4、5並無實質的連接關係,而是以發光模組1發出的入射光行經各功能模組2、3、4、5的順序,定義出各功能模組1、2、3、4、5的相對位置關係。Please refer to FIG. 1. FIG. 1 is a functional block diagram of a film curvature measuring device according to an embodiment of the present disclosure. As shown in FIG. 1 , the film curvature measuring device of the present disclosure is suitable for measuring the curvature of the film 4 to be tested, and the film curvature measuring device comprises the light emitting module 1 , the first optical module 2 , and the second optical module. 3. The third optical module 5, the image capturing module 6, and the image analyzing module 7. The image capturing module 6 is electrically connected to the image analyzing module 7, and the remaining functional modules 1, 2, 3, 4, and 5 have no substantial connection relationship, but the incident light emitted by the light emitting module 1 passes through each The order of the functional modules 2, 3, 4, 5 defines the relative positional relationship of each functional module 1, 2, 3, 4, 5.
簡單來說,本揭露的薄膜曲率量測裝置係先由發光模組1發射至少一條線雷射(line laser)以作為入射光,所述入射光的截面形狀係為第一幾何圖形。此入射光依序行經第一光學模組2所提供的第一光學路徑與第二光學模組3所提供的第二光學路徑,並根據第二光學模組3的引導而入射至待測薄膜4。接著,待測薄膜4會反射所接收到的入射光而形成反射光,此反射光再根據第二光學模組3的引導而進入第三光學模組5所提供的第三光學路徑,並被影像擷取模組6所接收。為求後續行文敘述簡明,在此根據反射光在各光學路徑中的傳播順序,定義影像擷取模組6所擷取得的反射光的截面係為第二幾何圖形。第二幾何圖形的形狀同樣為具有至少一特徵的幾何圖形。影像分析模組7則根據第二幾何圖形所包含的至少一特徵判斷出待測薄膜4的曲率。以下將分別根據薄膜曲率量測裝置中的各功能模組做詳細的說明。Briefly, the film curvature measuring device of the present disclosure first emits at least one line laser as the incident light by the light emitting module 1, and the cross-sectional shape of the incident light is the first geometric figure. The incident light is sequentially passed through the first optical path provided by the first optical module 2 and the second optical path provided by the second optical module 3, and is incident on the film to be tested according to the guiding of the second optical module 3. 4. Then, the film 4 to be tested reflects the received incident light to form reflected light, and the reflected light enters the third optical path provided by the third optical module 5 according to the guiding of the second optical module 3, and is The image capturing module 6 receives. In order to simplify the description of the subsequent text, the cross-section of the reflected light obtained by the image capturing module 6 is defined as the second geometric figure according to the propagation order of the reflected light in each optical path. The shape of the second geometric figure is also a geometric figure having at least one feature. The image analysis module 7 determines the curvature of the film 4 to be tested according to at least one feature included in the second geometric figure. The following will be explained in detail based on each functional module in the film curvature measuring device.
發光模組1用以發射至少一條線雷射(line laser)以作為入射光,此入射光的截面形狀係由至少一條直線所形成的第一幾何圖形。其中,上述的第一幾何圖形例如可為單一條直線、多條交錯直線(例如十字形狀、網狀)、多條平行線或多邊形(例如矩形、三角形),本揭露在此不加以限制。於實務上,發光模組1所發射的至少一條線雷射可以為一種固態雷射或氣態雷射,且每一條線雷射的波長範圍係為可見光波長,但本揭露在此僅為舉例示範並不加以限制。The light emitting module 1 is configured to emit at least one line laser as incident light, and the cross-sectional shape of the incident light is a first geometric shape formed by at least one straight line. The first geometric figure may be, for example, a single straight line, a plurality of staggered straight lines (for example, a cross shape, a mesh shape), a plurality of parallel lines or a polygon (for example, a rectangle or a triangle), and the disclosure is not limited herein. In practice, the at least one line of the laser emitted by the light-emitting module 1 may be a solid-state laser or a gaseous laser, and the wavelength range of each line of the laser is visible wavelength, but the disclosure is merely exemplary here. There are no restrictions.
第一光學模組2可以藉由配置不同的光學部件以形成第一光學路徑,以使入射光經由第一光學路徑傳播時,可以藉由這些光學部件調整入射光的光強度或截面形狀。光學部件例如為凹透鏡、凸透鏡、或中性衰減片(Neutral density filter, ND filter),在此僅為舉例示範但實際上並不以此為限。第二光學模組3用以提供第二光學路徑,其功能與第一光學路徑有所類似,但第二光學路徑更用以引導沿著第一光學路徑傳播的入射光入射待測薄膜4,並引導待測薄膜4反射所形成的反射光進入第三光學模組5所提供的第三光學路徑。第三光學模組5用以提供第三光學路徑,以使行經第二光學路徑的反射光可以沿著第三光學路徑傳播,且第三光學路徑同樣具有與第一光學路徑相似的功能。於實務上,待測薄膜4例如可以為一種發光二極體(light emitting diode, LED)的晶圓(wafer),但不以此為限。The first optical module 2 can adjust the light intensity or cross-sectional shape of the incident light by configuring the different optical components to form the first optical path so that the incident light propagates through the first optical path. The optical component is, for example, a concave lens, a convex lens, or a neutral density filter (ND filter), which is merely exemplary but not limited thereto. The second optical module 3 is configured to provide a second optical path, the function of which is similar to that of the first optical path, but the second optical path is further configured to guide incident light propagating along the first optical path to the film to be tested 4, And guiding the reflected light formed by the reflection of the film to be tested 4 into the third optical path provided by the third optical module 5. The third optical module 5 is configured to provide a third optical path such that the reflected light passing through the second optical path can propagate along the third optical path, and the third optical path also has a similar function as the first optical path. In practice, the film 4 to be tested may be, for example, a wafer of a light emitting diode (LED), but is not limited thereto.
影像擷取模組6用以擷取傳播至第三光學路徑終端的反射光,以擷取得前述的第二幾何圖形。此第二幾何圖形如前述係為具有至少一特徵的幾何圖形。於實務上,影像擷取模組6可例如是一種具有感光耦合元件(Charge-coupled Device, CCD)或是具有互補式金屬氧化物半導體(Complementary Metal Oxide Semiconductor, CMOS)的攝影機,本揭露在此不加以限制。The image capturing module 6 is configured to capture the reflected light that is transmitted to the terminal of the third optical path to obtain the second geometric pattern. This second geometric figure, as previously described, is a geometric figure having at least one feature. In practice, the image capturing module 6 can be, for example, a camera having a photosensitive-coupled device (CCD) or a complementary metal oxide semiconductor (CMOS). The disclosure is here. No restrictions.
影像分析模組7用以根據上述第二幾何圖形的至少一特徵,判斷出待測薄膜4的曲率。於實務上,影像分析模組7可例如是中央處理器(Central Processing Unit, CPU)或微控制器(microcontroller unit, MCU),但不以此為限。更具體地說,由於待測薄膜4並不一定是一個理想的平面,若待測薄膜4係為凹面或凸面時,則前述的入射光被待測薄膜4反射形成反射光的過程中,反射光的截面形狀係由入射光的截面形狀根據待測薄膜4的曲率對應地放大、縮小、歪斜或扭曲而形成。The image analysis module 7 is configured to determine the curvature of the film 4 to be tested according to at least one feature of the second geometric figure. In practice, the image analysis module 7 can be, for example, a central processing unit (CPU) or a microcontroller unit (MCU), but is not limited thereto. More specifically, since the film 4 to be tested is not necessarily an ideal plane, if the film 4 to be tested is concave or convex, the incident light is reflected by the film 4 to be tested to form a reflected light, and the reflection is performed. The cross-sectional shape of the light is formed by the cross-sectional shape of the incident light correspondingly enlarged, reduced, skewed, or twisted according to the curvature of the film 4 to be tested.
換句話說,入射光以及反射光具有的截面形狀會因待測薄膜4的反射而有所差異。且在待測薄膜4具有不同曲率的情況下,反射光會根據不同曲率形成相對應的截面形狀。是故,所述第二幾何圖形的至少一特徵也會根據曲率不同而有所變化。而影像分析模組7根據所述第二幾何圖形的至少一特徵與曲率的對應關係,由量測得的至少一特徵反推出待測薄膜4所具有的未知曲率。每一種幾何圖形分別具有不同的幾何定義並對應形成所述至少一特徵,故所述至少一特徵的第二幾何圖形可例如為至少一線雷射對應於不同軸向上的長度、至少一對平行線雷射間的距離、第二幾何圖形的周長與第二幾何圖形的面積至少其中之一。In other words, the cross-sectional shape of the incident light and the reflected light may differ depending on the reflection of the film 4 to be tested. And in the case where the film 4 to be tested has different curvatures, the reflected light will form a corresponding cross-sectional shape according to different curvatures. Therefore, at least one feature of the second geometric shape may also vary depending on the curvature. The image analysis module 7 derives the unknown curvature of the film 4 to be tested by the measured at least one feature according to the corresponding relationship between the at least one feature of the second geometric figure and the curvature. Each of the geometric shapes has a different geometric definition and correspondingly forms the at least one feature, so the second geometric shape of the at least one feature may be, for example, at least one line of laser corresponding to a length in different axial directions, at least one pair of parallel lines The distance between the lasers, the perimeter of the second geometric figure, and the area of the second geometric figure are at least one of.
在一實施例中,影像分析模組7可以根據多組相異的標準數據以及影像擷取模組6所擷取到的反射光的截面形狀,判斷出待測薄膜4的曲率。前述標準數據係為預先實驗得到的數據,每一組標準數據對應到特定曲率的薄膜。更詳細地說,每一組標準數據包含基板數據以及特徵數據,而且其中基板數據相關於一標準基板的曲率。例如基板數據可以指示此標準數據係關於具有某曲率的矽基板所形成的薄膜,或具有另一曲率的藍寶石基板所形成的薄膜;而特徵數據係相關於第二幾何圖形的至少一特徵。例如當第二幾何圖形係為一矩形時,特徵數據可以指示此矩形的長、寬或任何足以代表此矩形的特徵。是故,標準數據係用以指示:當由某材料形成的基板具有某曲率的時候,其對應第二幾何圖形係具有某特徵。In an embodiment, the image analysis module 7 can determine the curvature of the film 4 to be tested according to different sets of standard data and the cross-sectional shape of the reflected light captured by the image capturing module 6. The aforementioned standard data is pre-experimental data, and each set of standard data corresponds to a film of a specific curvature. In more detail, each set of standard data includes substrate data as well as feature data, and wherein the substrate data is related to the curvature of a standard substrate. For example, the substrate data may indicate that the standard data is a film formed by a germanium substrate having a certain curvature, or a thin film formed of a sapphire substrate having another curvature; and the feature data is related to at least one feature of the second geometric figure. For example, when the second geometric figure is a rectangle, the feature data can indicate the length, width, or any feature of the rectangle that is sufficient to represent the rectangle. Therefore, the standard data is used to indicate that when a substrate formed of a material has a certain curvature, it corresponds to the second geometric figure having a certain feature.
沿續前述實施例,影像分析模組7可自第二幾何圖形分析得一相關於待測薄膜4的第一特徵數據。此時,影像分析模組7可以根據多組已知的標準數據中所含的基板數據、特徵數據,連同第一特徵數據計算得待測薄膜的曲率。此計算方式可以是內插法、外插法或根據曲率以及第二幾何圖形之間的對應關係所設計的相對應演算法,例如以各已知資訊建立迴歸運算模型,此為所屬技術領域中具通常知識者可自由設計,在此並不以此為限。於此,所屬領域中具通常知識者當可明白,本揭露的精神即在於藉由以具有「特定截面形狀」的入射光入射待測薄膜4產生反射光,影像擷取模組6擷取反射光具有至少一特徵的第二幾何圖形。影像分析模組7則根據第二幾何圖形的至少一特徵,並輔以標準數據判斷出待測薄膜4的曲率。前述係為本揭露的薄膜曲率量測裝置的功能說明,然本揭露的薄膜曲率量測裝置實可具有以下的實施態樣。According to the foregoing embodiment, the image analysis module 7 can analyze the first feature data related to the film 4 to be tested from the second geometric figure. At this time, the image analysis module 7 can calculate the curvature of the film to be tested according to the substrate data and the feature data contained in the plurality of sets of known standard data together with the first feature data. The calculation may be an interpolation method, an extrapolation method or a corresponding algorithm designed according to the correspondence between the curvature and the second geometric figure, for example, establishing a regression operation model with each known information, which is in the technical field. Those with ordinary knowledge can design freely and are not limited to this. As can be understood by those of ordinary skill in the art, the spirit of the present disclosure is to generate reflected light by incident light having a "specific cross-sectional shape" incident on the film 4 to be tested, and the image capturing module 6 extracts the reflection. The light has a second geometric shape of at least one feature. The image analysis module 7 determines the curvature of the film 4 to be tested according to at least one feature of the second geometric figure and supplemented by standard data. The foregoing is a functional description of the disclosed film curvature measuring device. However, the film curvature measuring device disclosed herein may have the following embodiments.
請參照圖2,圖2係本揭露一實施例中薄膜曲率量測裝置的第一實施態樣。在圖2所代表的實施態樣中,更以實際的光學部件實做出如圖1所示的各功能方塊。如圖2所示,第一光學模組2包含第一透鏡21以及第一濾鏡23,藉以形成第一光學路徑,使入射光在第一光學路徑中依序經過第一透鏡21以及第一濾鏡23。第二光學模組3包含第一全反射鏡31以及分光鏡33,藉以形成第二光學路徑,使得入射光在第二光學路徑中依序經過第一全反射鏡31與分光鏡33,且使由待測薄膜4反射形成的反射光在第二光學路徑中藉由分光鏡33的引導進入前述第三光學路徑。第三光學模組5包含第二濾鏡51以及第二透鏡53,藉以形成第三光學路徑,使入射光在第一光學路徑中依序經過第二濾鏡51以及第二透鏡53。Please refer to FIG. 2. FIG. 2 is a first embodiment of a film curvature measuring device according to an embodiment of the present disclosure. In the embodiment represented by Fig. 2, the functional blocks shown in Fig. 1 are actually made with actual optical components. As shown in FIG. 2, the first optical module 2 includes a first lens 21 and a first filter 23, thereby forming a first optical path for sequentially passing incident light through the first lens 21 and the first in the first optical path. Filter 23. The second optical module 3 includes a first total reflection mirror 31 and a beam splitter 33, thereby forming a second optical path, so that the incident light sequentially passes through the first total reflection mirror 31 and the beam splitter 33 in the second optical path, and The reflected light formed by the reflection of the film to be tested 4 is guided into the third optical path by the beam splitter 33 in the second optical path. The third optical module 5 includes a second filter 51 and a second lens 53 to form a third optical path for sequentially passing the incident light through the second filter 51 and the second lens 53 in the first optical path.
其中,前述的第一透鏡21、第二透鏡53係為凸透鏡,用以聚焦入射光與反射光,藉此微調出具有所欲特徵的入射光或反射光。而於實務上,第一透鏡21、第二透鏡53也可以是凹透鏡,用以發散入射光或反射光,而使其具有所欲的特徵。前述的第一濾鏡23、第二濾鏡51可以是中性衰減片,用以控制入射光與反射光的光強度。是故,可以明白由第一透鏡21、第一濾鏡23組成的第一光學模組2以及由第二濾鏡51、第二透鏡53組成的第三光學模組5,在圖2所對應實施例中係用以微調入射光及反射光的態樣。而第一全反射鏡31用以反射沿第一方向傳播的入射光,使其改沿第二方向傳播;分光鏡33的第一面用以供沿第二方向的入射光穿透,而分光鏡33的第二面則反射沿第二方向傳播的反射光,使其改沿第一方向傳播。是故,可以明白由第一全反射鏡31、分光鏡33組成的第二光學模組2係用以控制入射光與反射光的方向,使其偏向所欲的角度並傳播於所欲的路徑。The first lens 21 and the second lens 53 are convex lenses for focusing incident light and reflected light, thereby finely adjusting incident light or reflected light having a desired characteristic. In practice, the first lens 21 and the second lens 53 may also be concave lenses for diverging incident light or reflected light to have desired characteristics. The first filter 23 and the second filter 51 may be neutral attenuators for controlling the light intensity of the incident light and the reflected light. Therefore, it can be understood that the first optical module 2 composed of the first lens 21 and the first filter 23 and the third optical module 5 composed of the second filter 51 and the second lens 53 are corresponding to FIG. In the embodiment, the aspect of the incident light and the reflected light is finely adjusted. The first total reflection mirror 31 is configured to reflect the incident light propagating in the first direction to propagate in the second direction; the first surface of the beam splitter 33 is used for the incident light in the second direction to penetrate, and the light splitting The second side of the mirror 33 reflects the reflected light propagating in the second direction, causing it to propagate in the first direction. Therefore, it can be understood that the second optical module 2 composed of the first total reflection mirror 31 and the beam splitter 33 is used to control the direction of the incident light and the reflected light to be biased to a desired angle and propagated to a desired path. .
請同時參照圖1及圖2,在圖2的對應實施例中,發光模組1發射至少一條線雷射以做為一入射光,此入射光如前所述地依序經過第一光學模組2提供的第一光學路徑及第二光學模組3提供的第二光學路徑,其中入射光與反射光更受第二光學模組3的引導而轉換傳播方向。更詳細地說,入射光在第一光學路徑中沿第一方向(例如X軸方向)傳播,並受第二光學模組3引導而沿第二方向(例如Y軸方向)垂直入射待測薄膜4並被垂直反射而形成反射光。接著,反射光會先沿第二方向傳播於第二光學路徑中,再透過第二光學模組3之反射而轉沿第一方向進入第三光學模組5所提供的第三光學路徑。其中,如圖2所示,第一方向係垂直於第二方向。而影像擷取模組6接收第三光學路徑終端的反射光,並擷取得如前述的第二幾何圖形。影像分析模組7根據此第二幾何圖形的至少一特徵以及前述的多個標準數據進行分析,並判斷得待測薄膜4的曲率。Referring to FIG. 1 and FIG. 2 simultaneously, in the corresponding embodiment of FIG. 2, the light-emitting module 1 emits at least one line of laser light as an incident light, and the incident light passes through the first optical mode in sequence as described above. The first optical path provided by the group 2 and the second optical path provided by the second optical module 3, wherein the incident light and the reflected light are further guided by the second optical module 3 to switch the propagation direction. In more detail, the incident light propagates in the first direction (for example, the X-axis direction) in the first optical path, and is guided by the second optical module 3 to vertically enter the film to be tested in the second direction (for example, the Y-axis direction). 4 is reflected vertically to form reflected light. Then, the reflected light first propagates in the second optical path along the second direction, and then passes through the reflection of the second optical module 3 to enter the third optical path provided by the third optical module 5 in the first direction. Wherein, as shown in FIG. 2, the first direction is perpendicular to the second direction. The image capturing module 6 receives the reflected light of the third optical path terminal and obtains the second geometric figure as described above. The image analysis module 7 analyzes according to at least one feature of the second geometric figure and the plurality of standard data, and determines the curvature of the film 4 to be tested.
請參照圖3,圖3係本揭露圖1之薄膜曲率量測裝置的第二實施態樣。如圖示,第一光學模組2以第一透鏡21與第一濾鏡23形成第一光學路徑。第二光學模組3以第一全反射鏡31與第二全反射鏡35形成第二光學路徑。第三光學模組5以第二濾鏡51與第二透鏡53形成第三光學路徑。入射光在第一光學路徑係沿第一方向傳播,接著進入第二光學路徑。入射光在第二光學路徑中被第一全反射鏡31反射至第二方向,並沿第二方向入射待測薄膜4。待測薄膜4反射入射光形成反射光,此反射光係沿第三方向傳播。反射光會被第二全反射鏡35反射至第一方向,並沿第一方向進入第三光學路徑。接著如前述,影像截取模組6在第三光學路徑的終端接收反射光,並擷取得如前述的第二幾何圖形,供影像分析模組7據以分析。Please refer to FIG. 3. FIG. 3 is a second embodiment of the film curvature measuring device of FIG. As shown, the first optical module 2 forms a first optical path with the first lens 21 and the first filter 23. The second optical module 3 forms a second optical path with the first total reflection mirror 31 and the second total reflection mirror 35. The third optical module 5 forms a third optical path with the second filter 51 and the second lens 53. The incident light propagates in the first direction along the first optical path and then into the second optical path. The incident light is reflected by the first total reflection mirror 31 to the second direction in the second optical path, and is incident on the film 4 to be tested in the second direction. The film to be tested 4 reflects the incident light to form reflected light, and the reflected light propagates in the third direction. The reflected light is reflected by the second total reflection mirror 35 to the first direction and enters the third optical path in the first direction. Then, as described above, the image capture module 6 receives the reflected light at the terminal of the third optical path, and obtains the second geometric pattern as described above for analysis by the image analysis module 7.
第2、3圖分別揭示了本揭露的薄膜曲率量測裝置實際上的實施態樣,惟以光學模組形成光學路徑係為所屬技術領域具有通常知識者可以根據薄膜類型、機台設計、配置位置等實際考量自由安排設計,在此並不以此為限。而如前述,本揭露的精神在於以線雷射形成具有特定截面形狀的入射光,並以此入射光入射待測薄膜4並被反射形成反射光,再自反射光擷取出具有至少一特徵的第二幾何圖形,且輔以標準數據判斷出待測薄膜4的曲率。以下將以具體實施例詳細說明。2 and 3 respectively disclose the actual implementation of the film curvature measuring device of the present disclosure, but the optical path system formed by the optical module is generally known to those skilled in the art, and can be designed and configured according to the type of the film, the machine, and the configuration. The actual considerations such as location are free to arrange the design, which is not limited to this. As described above, the spirit of the present disclosure is to form incident light having a specific cross-sectional shape by a line laser, and the incident light is incident on the film to be tested 4 and reflected to form reflected light, and then the self-reflecting light picks up at least one feature. The second geometric figure is supplemented by standard data to determine the curvature of the film 4 to be tested. The details will be described in detail below with reference to specific embodiments.
請參照圖4A、4B、4C,圖4A、4B、4C係本揭露一實施例中以線雷射光源產生不同標準數據及其相對應的第二幾何圖形示意圖。得先注意的是,圖4A、4B、4C係對應於不同的標準數據,亦即圖4A、4B、4C係以發光模組1發射同樣形狀的線雷射,經前述光學路徑以及具不同「已知」曲率的凸面薄膜的反射,被影像擷取模組6擷取的第二幾何圖形示意圖。是故,圖4A、4B、4C所示意的每一第二幾何圖形都對應於具有相異且已知懸浮高度的薄膜,如圖所示,圖4A、4B、4C分別對應的懸浮高度依序為100µm、70µm、65µm。而除了從理論推得外,更可以由圖4A、4B、4C明白,以相同的光學路徑發射相同形狀的入射光至具有不同懸浮高度的薄膜,其對應產生的反射光會分別具有不同形狀的第二幾何圖形。4A, 4B, and 4C, FIG. 4A, FIG. 4B and FIG. 4C are diagrams showing different standard data generated by a line laser source and corresponding second geometric patterns in an embodiment of the present disclosure. It should be noted that FIGS. 4A, 4B, and 4C correspond to different standard data, that is, FIG. 4A, FIG. 4B, and FIG. 4C are used to emit the same shape of the line laser by the light-emitting module 1, and the optical path and the difference are different. The reflection of the convex film of curvature is known as a schematic diagram of the second geometry captured by the image capture module 6. Therefore, each of the second geometric figures illustrated in FIGS. 4A, 4B, and 4C corresponds to a film having a different and known levitation height. As shown in the figure, the corresponding sag heights of FIGS. 4A, 4B, and 4C are sequentially followed. It is 100 μm, 70 μm, and 65 μm. In addition to being derived from the theory, it can be further understood from FIGS. 4A, 4B, and 4C that the same shape of incident light is emitted to the film having different levitation heights in the same optical path, and the corresponding reflected light respectively has different shapes. The second geometry.
前述懸浮高度係為待測薄膜的最高點與一水平面的距離,而當固定待測薄膜與水平面的接面面積時,懸浮高度可以對應於待測薄膜的曲率以及曲率半徑。更具體地以一凸面待測薄膜來說,當懸浮高度越大時,對應的凸面待測薄膜的曲率越大、曲率半徑越小;反過來說,當懸浮高度越小時,對應的凸面待測薄膜的曲率越小、曲率半徑越大。基於實際應用上的考量,本揭露係以懸浮高度為基準對第二幾何圖形的至少一特徵進行分析。但如前述所屬領域具通常知識者應該可以理解懸浮高度、曲率、曲率半徑三者實質上係可透過運算互換。The aforementioned suspension height is the distance between the highest point of the film to be tested and a horizontal plane, and when the junction area of the film to be tested and the horizontal plane is fixed, the suspension height may correspond to the curvature of the film to be tested and the radius of curvature. More specifically, in a convex film to be tested, when the flying height is larger, the curvature of the corresponding convex film to be tested is larger and the radius of curvature is smaller; conversely, when the flying height is smaller, the corresponding convex surface is to be tested. The smaller the curvature of the film, the larger the radius of curvature. Based on practical considerations, the present disclosure analyzes at least one feature of the second geometric figure based on the levitation height. However, those skilled in the art should understand that the levitation height, curvature, and radius of curvature are substantially interchangeable through the operation.
請再參照圖4A、4B、4C,在圖4A、4B、4C對應實施例中,前述發光模組1係發射一條線雷射做為入射光。在適當的單位級距下觀之,此入射光的截面形狀接近一矩形。此具有矩形截面形狀的入射光經前述各「具有已知懸浮高度的凸面薄膜」反射時,其矩形截面形狀的長、寬對應各懸浮高度縮小或放大,故反射光截面形狀雖仍是矩形,但其長與寬已與入射光的截面形狀有所不同,且每一反射光的截面形狀也對應待測薄膜4的曲率而有所不同。最後分別對應形成如圖4A、4B、4C的第二幾何圖形。4A, 4B, and 4C, in the corresponding embodiment of FIGS. 4A, 4B, and 4C, the light-emitting module 1 emits a line of laser light as incident light. The cross-sectional shape of the incident light is close to a rectangle under the appropriate unit pitch. When the incident light having a rectangular cross-sectional shape is reflected by the above-mentioned "convex film having a known levitation height", the length and width of the rectangular cross-sectional shape are reduced or enlarged corresponding to the respective levitation heights, so that the cross-sectional shape of the reflected light is still rectangular. However, the length and width thereof are different from the cross-sectional shape of the incident light, and the cross-sectional shape of each reflected light also differs depending on the curvature of the film 4 to be tested. Finally, the second geometric figures as shown in FIGS. 4A, 4B, and 4C are respectively formed.
且由圖4A、4B、4C可知,當凸面薄膜的懸浮高度越大,相對應矩形第二幾何圖形的長與寬越大。更具體地以懸浮高度為100µm的薄膜所對應的矩形第二幾何圖形來說,其長與寬會較懸浮高度為70µm或65µm的薄膜所對應者來得大。儘管以同樣單一線雷射做為入射光,由圖可明白各矩形第二幾何圖形的長m1、m2、m3之間存在有m1>m2>m3的相對關係,且各矩形第二幾何圖形的寬n1、n2、n3之間存在有n1>n2>n3的相對關係。所屬技術領域具通常知識者應可以此類推,當待測薄膜4為一凹面薄膜時,上述的特性將會因此有所不同,於此則不再重複贅述。4A, 4B, 4C, the larger the levitation height of the convex film, the larger the length and width of the corresponding second geometric figure. More specifically, in the rectangular second geometry corresponding to the film having a suspension height of 100 μm, the length and width are larger than those corresponding to the film having a suspension height of 70 μm or 65 μm. Although the same single-line laser is used as the incident light, it can be understood from the figure that there is a relative relationship between m1>m2>m3 between the lengths m1, m2 and m3 of the second geometric figure of each rectangle, and the second geometric figure of each rectangle There is a relative relationship between n1>n2>n3 between the widths n1, n2, and n3. Those skilled in the art should be able to deduce that when the film 4 to be tested is a concave film, the above characteristics will be different, and the details will not be repeated here.
當本揭露的薄膜曲率量測裝置用以量測具有未知曲率的薄膜時,亦即待測薄膜4具有未知的曲率或者可以說是未知的懸浮高度,前述影像擷取模組6擷取得一對應於此具未知懸浮高度的待測薄膜4的矩形之第二幾何圖形。前述影像分析模組7可根據此對應於未知懸浮高度的矩形之第二幾何圖形,以及前述相對應已知懸浮高度的矩形之第二幾何圖形,根據其長或寬的對應關係,利用內插法、外插法或根據其對應關係設計分析演算法,據以計算並判斷出待測薄膜4的懸浮高度,亦即待測薄膜4的曲率。When the film curvature measuring device of the present disclosure is used to measure a film having an unknown curvature, that is, the film 4 to be tested has an unknown curvature or an unknown levitation height, the image capturing module 6 撷 obtains a corresponding The second geometric shape of the rectangle of the film 4 to be tested having an unknown levitation height. The image analysis module 7 can use the second geometric figure corresponding to the rectangle of the unknown levitation height and the second geometric shape of the rectangle corresponding to the known levitation height, and use the interpolation according to the correspondence of the length or the width thereof. The method, the extrapolation method or the analysis algorithm is designed according to the corresponding relationship, and the levitation height of the film 4 to be tested, that is, the curvature of the film 4 to be tested is calculated and judged.
請參照圖5A、5B、5C,圖5A、5B、5C係本揭露一實施例中以十字雷射光源產生不同標準數據及其相對應的第二幾何圖形示意圖。在此實施例中,發光模組1發射兩條線雷射做為入射光,此兩條線雷射交錯形成一十字,此時入射光的截面形狀係為所述十字形,前述影像擷取模組6可對應擷取得一十字形的第二幾何圖形。影像分析模組7則根據此十字型之第二幾何圖形以及多個如圖5A、5B、5C代表的已知的標準數據,藉由反射光的兩個線雷射在不同軸向上的長度變化,判斷得待測薄膜4的懸浮高度及曲率。5A, 5B, and 5C, FIG. 5A, FIG. 5B, and FIG. 5C are schematic diagrams showing different standard data generated by a cross laser light source and corresponding second geometric patterns in an embodiment of the present disclosure. In this embodiment, the light-emitting module 1 emits two lines of laser light as incident light, and the two lines of laser light are staggered to form a cross. At this time, the cross-sectional shape of the incident light is the cross shape, and the image capturing is performed. The module 6 can be adapted to obtain a second geometric shape of a cross. The image analysis module 7 changes the length of the two lines of the reflected light in different axial directions according to the second geometry of the cross and a plurality of known standard data as shown in FIGS. 5A, 5B, and 5C. The suspension height and curvature of the film 4 to be tested are determined.
圖5A、5B、5C所對應實施例與圖4A、4B、4C對應實施例分析第二幾何圖形的概念有所類似,兩者皆是根據第二幾何圖形在兩個軸向上的形狀、長度變化以判斷出待測薄膜4的懸浮高度。但需注意的是,圖4A、4B、4C所對應實施例係以單一條線雷射入射待測薄膜4,並根據其對應形成的第二幾何圖形的長或寬進行判斷。而圖5A、5B、5C對應實施例係以兩條線雷射對應於不同薄膜曲率的長度變化進行判斷,故圖5A、5B、5C對應實施例係應用了比圖4A、4B、4C對應實施例更多的資訊進行判斷,因此可以更精確地測量得待測薄膜4的懸浮高度和曲率。5A, 5B, and 5C correspond to the concepts of analyzing the second geometric figure in the corresponding embodiments of FIGS. 4A, 4B, and 4C, and both are in accordance with the shape and length of the second geometric figure in two axial directions. The suspension height of the film 4 to be tested is judged. It should be noted, however, that the embodiment corresponding to FIGS. 4A, 4B, and 4C is incident on the film 4 to be tested with a single line of laser light, and is judged according to the length or width of the corresponding second geometric figure. 5A, 5B, and 5C correspond to the embodiment in which the two line lasers are determined according to the change in the length of the curvature of the different films. Therefore, the corresponding embodiments of FIGS. 5A, 5B, and 5C are applied in accordance with FIGS. 4A, 4B, and 4C. For example, more information is judged, so that the levitation height and curvature of the film 4 to be tested can be measured more accurately.
請參照圖6A、6B、6C,圖6A、6B、6C係本揭露一實施例中以一對平行雷射光源產生不同標準數據及其相對應的第二幾何圖形示意圖。在此實施例中,發光模組1同樣發射兩條線雷射做為入射光,與圖5A、5B、5C所對應的實施例不同的是,此兩條線雷射平行排列形成一對平行線。故此時入射光的截面形狀係為一對平行線,影像分析模組7則根據第二幾何圖形所包含的平行線間的距離變化判斷得待測薄膜4的懸浮高度及曲率。更詳細地說,影像分析模組7已知如各圖中的平行線距離d1、d2、d3以及每一平行線距離所對應的懸浮高度,且影像分析模組7再自對應於待測薄膜4的第二幾何圖形取得另一個對應於未知懸浮高度的平行線距離,並根據這些資訊分析判斷得待測薄膜4的懸浮高度和曲率。6A, 6B, and 6C, FIG. 6A, 6B, and 6C are schematic diagrams showing different standard data and corresponding second geometric patterns generated by a pair of parallel laser light sources in an embodiment of the present disclosure. In this embodiment, the light-emitting module 1 also emits two lines of laser light as incident light. Unlike the embodiment corresponding to FIGS. 5A, 5B, and 5C, the two lines of lasers are arranged in parallel to form a pair of parallel lines. line. Therefore, the cross-sectional shape of the incident light is a pair of parallel lines, and the image analysis module 7 determines the levitation height and curvature of the film 4 to be tested according to the change of the distance between the parallel lines included in the second geometric figure. In more detail, the image analysis module 7 knows the parallel line distances d1, d2, d3 and the distance corresponding to each parallel line distance in each figure, and the image analysis module 7 corresponds to the film to be tested. The second geometry of 4 takes another parallel line distance corresponding to the unknown levitation height, and based on these information analysis, determines the levitation height and curvature of the film 4 to be tested.
請參照圖7A、7B、7C,圖7A、7B、7C係本揭露一實施例中以網格雷射光源產生不同標準數據及其相對應的第二幾何圖形示意圖。在此實施例中,發光模組1發射多條線雷射做為入射光,此多條線雷射交錯排列形成網格。故此時入射光的截面形狀係為前述的網格形狀,前述影像擷取模組6可對應擷取得網格之第二幾何圖形。影像分析模組7則根據此網格之第二幾何圖形以及多個如圖7A、7B、7C代表的已知的標準數據,藉由網格中某一特定區域的面積或其周長與不同懸浮高度的對應關係,判斷得待測薄膜4的懸浮高度及曲率。更詳細地說,影像分析模組7已知如各圖中的特定區塊的面積a1、a2、a3或其周長以及每一特定區塊所對應的懸浮高度,且影像分析模組7再自對應於待測薄膜4的第二幾何圖形取得另一個對應於未知懸浮高度的特定區塊面積或其周長,根據這些資訊分析判斷得待測薄膜4的懸浮高度和曲率。7A, 7B, and 7C, FIG. 7A, FIG. 7B, and FIG. 7C are diagrams showing different standard data generated by a grid laser light source and corresponding second geometric patterns in an embodiment of the present disclosure. In this embodiment, the light-emitting module 1 emits a plurality of line lasers as incident light, and the plurality of line lasers are staggered to form a grid. Therefore, the cross-sectional shape of the incident light is the mesh shape described above, and the image capturing module 6 can correspondingly acquire the second geometric figure of the mesh. The image analysis module 7 is based on the second geometry of the grid and a plurality of known standard data as represented by FIGS. 7A, 7B, and 7C, by the area of a specific area in the grid or its perimeter. The corresponding relationship of the levitation height determines the levitation height and curvature of the film 4 to be tested. In more detail, the image analysis module 7 knows the area a1, a2, a3 or its circumference of a specific block in each figure and the levitation height corresponding to each specific block, and the image analysis module 7 From the second geometric figure corresponding to the film 4 to be tested, another specific block area corresponding to the unknown levitation height or its circumference is taken, and the levitation height and curvature of the film 4 to be tested are judged based on the analysis of the information.
對應上述,本揭露也提供了一種薄膜曲率量測方法,適用於量測待測薄膜的曲率。請參照圖8,圖8係本揭露一實施例中薄膜曲率量測方法的步驟流程圖。須先一提的是,本揭露實施例所述的薄膜曲率量測方法中的第一、第二、第三光學路徑均可對應於第1、2、3圖的相關實施例,以前述的第一、第二、第三光學模組2、3、5分別形成所述的第一、第二、第三光學路徑。本揭露的薄膜曲率量測方法同時適用於前述的薄膜曲率量測裝置,故請同時參照第1、2、3圖配合說明。在步驟S801中,本揭露的薄膜曲率量測方法先發射至少一條線雷射以作為入射光,其中此入射光的截面形狀係由至少一條直線所形成的第一幾何圖形。而同時對應第4~8圖相關實施例,此幾何形狀可例如為單一條直線、多條交錯直線、多條平行線或多邊形。Corresponding to the above, the present disclosure also provides a film curvature measuring method suitable for measuring the curvature of a film to be tested. Please refer to FIG. 8. FIG. 8 is a flow chart showing the steps of the method for measuring the curvature of a film according to an embodiment of the present disclosure. It should be noted that the first, second, and third optical paths in the film curvature measurement method according to the embodiment may correspond to the related embodiments of the first, second, and third figures, The first, second, and third optical modules 2, 3, and 5 respectively form the first, second, and third optical paths. The film curvature measuring method disclosed in the present invention is also applicable to the above-mentioned film curvature measuring device, so please refer to the first, second, and third figures at the same time. In step S801, the film curvature measurement method of the present disclosure first emits at least one line of laser light as incident light, wherein the cross-sectional shape of the incident light is a first geometric figure formed by at least one straight line. While corresponding to the related embodiments of FIGS. 4-8, the geometric shape may be, for example, a single straight line, a plurality of staggered straight lines, a plurality of parallel lines or a polygon.
接著在步驟S803中,使入射光經由第一光學路徑傳播,並引導沿第一光學路徑傳播的入射光經由第二光學路徑入射待測薄膜。然後在步驟S805中,引導行經第二光學路徑的反射光進入第三光學路徑,並使反射光沿第三光學路徑傳播,其中所述反射光係由待測薄膜反射入射光所形成,且反射光的截面形狀係為具有至少一特徵的第二幾何圖形。而在步驟S807中,擷取傳播至第三光學路徑終端的反射光。最後在步驟S809中,根據擷取得的反射光的至少一特徵的第二幾何圖形,判斷出待測薄膜的曲率。Next, in step S803, incident light is propagated through the first optical path, and incident light propagating along the first optical path is guided to enter the film to be tested via the second optical path. Then, in step S805, the reflected light passing through the second optical path is guided into the third optical path, and the reflected light is propagated along the third optical path, wherein the reflected light is formed by the incident light reflected by the film to be tested, and the reflection is The cross-sectional shape of the light is a second geometric figure having at least one feature. In step S807, the reflected light propagating to the third optical path terminal is extracted. Finally, in step S809, the curvature of the film to be tested is determined based on the second geometric pattern of at least one characteristic of the reflected light obtained by the 撷.
在前述薄膜曲率量測方法的步驟中,所述至少一特徵的第二幾何圖形對應於先前第4A至第7C圖所述,包含至少一線雷射對應於在不同軸向上的長度、至少一對平行線雷射間的距離、第二幾何圖形的周長與第二幾何圖形的面積至少其中之一。且除了擷取得的至少一特徵更可輔以多個已知的標準數據,據以判斷得待測薄膜的懸浮高度和曲率。In the step of the film curvature measuring method, the second geometric shape of the at least one feature corresponds to the previous 4A to 7C, and includes at least one line of laser corresponding to the length in different axial directions, at least one pair The distance between the parallel line lasers, at least one of the perimeter of the second geometric figure and the area of the second geometric figure. And the at least one feature obtained in addition to the 更 can be supplemented with a plurality of known standard data to determine the levitation height and curvature of the film to be tested.
綜合以上所述,本揭露提供了一種薄膜曲率量測裝置以及薄膜曲率量測方法,藉由發光模組發射至少一線雷射以形成入射光,並經由各光學模組形成各光學路徑,來引導入射光入射一具有未知曲率的待測薄膜,並引導待測薄膜反射形成的反射光被影像擷取裝置接收。影像擷取模組反射光,以供影像分析模組進行分析判斷出待測薄膜的曲率。其中影像分析模組可以藉由反射光的至少一特徵的第二幾何圖形輔以相對應的標準數據,判斷出待測薄膜的懸浮高度,再經簡單運算得到其曲率。藉此,本接露之薄膜曲率量測裝置以及薄膜曲率量測方法可以在各磊晶製程中,即時地監控各晶圓的曲率變化,以協助廠商明確辨認造成基板彎曲的主要因素是在哪一道製程中,進而調整參數以提高製程的良率並據以降低成本,十分具有實用性。In summary, the present disclosure provides a film curvature measuring device and a film curvature measuring method, wherein at least one line of laser light is emitted by the light emitting module to form incident light, and optical paths are formed through the optical modules. The incident light is incident on a film to be tested having an unknown curvature, and the reflected light formed by the reflection of the film to be tested is received by the image capturing device. The image capturing module reflects the light for analysis by the image analysis module to determine the curvature of the film to be tested. The image analysis module can determine the levitation height of the film to be tested by using the second geometric figure of the at least one feature of the reflected light, and the corresponding standard data, and then obtain the curvature by a simple operation. Therefore, the exposed film curvature measuring device and the film curvature measuring method can monitor the curvature change of each wafer in each epitaxial process in order to assist the manufacturer to clearly identify the main factor causing the substrate to bend. In a process, the parameters are adjusted to improve the yield of the process and reduce the cost, which is very practical.
雖然本揭露以前述之實施例揭露如上,然其並非用以限定本揭露。在不脫離本揭露之精神和範圍內,所為之更動與潤飾,均屬本揭露之專利保護範圍。關於本揭露所界定之保護範圍請參考所附之申請專利範圍。Although the disclosure is disclosed above in the foregoing embodiments, it is not intended to limit the disclosure. All changes and refinements are beyond the scope of this disclosure. Please refer to the attached patent application for the scope of protection defined by this disclosure.
1‧‧‧發光模組
2‧‧‧第一光學模組
21‧‧‧第一透鏡
23‧‧‧第一濾鏡
3‧‧‧第二光學模組
31‧‧‧第一全反射鏡
33‧‧‧分光鏡
35‧‧‧第二全反射鏡
4‧‧‧待測薄膜
5‧‧‧第三光學模組
51‧‧‧第二濾鏡
53‧‧‧第二透鏡
6‧‧‧影像擷取模組
7‧‧‧影像分析模組
m1~m3‧‧‧矩形之第二幾何圖形的長度
n1~n3‧‧‧矩形之第二幾何圖形的寬度
d1~d3‧‧‧平行線之第二幾何圖形中的兩平行線的距離
a1~a3‧‧‧網格之第二幾何圖形某一特定區域的面積
S801~S809‧‧‧步驟流程1‧‧‧Lighting module
2‧‧‧First optical module
21‧‧‧ first lens
23‧‧‧First filter
3‧‧‧Second optical module
31‧‧‧First total reflection mirror
33‧‧‧beam splitter
35‧‧‧Second total reflection mirror
4‧‧‧ film to be tested
5‧‧‧ Third optical module
51‧‧‧Second filter
53‧‧‧second lens
6‧‧‧Image capture module
7‧‧‧Image Analysis Module
The length of the second geometric figure of the m1~m3‧‧‧ rectangle
Width of the second geometry of the rectangle n1~n3‧‧‧
Distance between two parallel lines in the second geometry of the d1~d3‧‧‧ parallel lines
The area of a particular area of the second geometry of the a1~a3‧‧‧ grid
S801~S809‧‧‧Step procedure
圖1 係本揭露一實施例中薄膜曲率量測裝置的功能方塊示意圖。 圖2 係本揭露圖1 之薄膜曲率量測裝置的第一實施態樣。 圖3 係本揭露圖1 之薄膜曲率量測裝置的第二實施態樣。 圖4A、4B、4C 係本揭露一實施例中以線雷射光源產生不同標準數據及其相對應的第二幾何圖形的示意圖。 第5A、5B、5C 圖係本揭露一實施例中以十字雷射光源產生不同標準數據及其相對應的第二幾何圖形的示意圖。 第6A、6B、6C 圖係本揭露一實施例中以一對平行線雷射光源產生不同標準數據及其相對應的第二幾何圖形的示意圖。 第7A、7B、7C 圖係本揭露一實施例中以網格雷射光源產生不同標準數據及其相對應的第二幾何圖形的示意圖。 圖8 係本揭露一實施例中薄膜曲率量測方法的步驟流程圖。1 is a functional block diagram of a film curvature measuring device according to an embodiment of the present invention. 2 is a first embodiment of the film curvature measuring device of FIG. 1. 3 is a second embodiment of the film curvature measuring device of FIG. 1. 4A, 4B, and 4C are schematic diagrams showing different standard data and corresponding second geometric patterns produced by a line laser source in an embodiment of the present disclosure. 5A, 5B, and 5C are schematic views showing the generation of different standard data and corresponding second geometric patterns by a cross laser light source in an embodiment. 6A, 6B, and 6C are schematic views showing the generation of different standard data and corresponding second geometric patterns by a pair of parallel line laser light sources in an embodiment. 7A, 7B, and 7C are schematic diagrams showing different standard data and corresponding second geometric patterns produced by a grid laser light source in an embodiment. FIG. 8 is a flow chart showing the steps of a method for measuring curvature of a film in an embodiment.
Claims (13)
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