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CN1933098B - A mask for continuous lateral crystallization technology and a method for using the mask - Google Patents

A mask for continuous lateral crystallization technology and a method for using the mask Download PDF

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CN1933098B
CN1933098B CN2005101032405A CN200510103240A CN1933098B CN 1933098 B CN1933098 B CN 1933098B CN 2005101032405 A CN2005101032405 A CN 2005101032405A CN 200510103240 A CN200510103240 A CN 200510103240A CN 1933098 B CN1933098 B CN 1933098B
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mask
transparent grating
shaped
edge
lateral crystallization
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CN1933098A (en
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孙铭伟
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AUO Corp
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AU Optronics Corp
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Abstract

The invention provides a mask for a continuous lateral crystallization technology and a use method of the mask. The mask includes: the transparent grating comprises two long edges, a front edge and a rear edge, the two long edges are parallel to each other and have the same length, the front edge protrudes towards the outer side of the transparent grating, and the rear edge is recessed towards the inner part of the transparent grating. The invention can effectively eliminate the uneven area and avoid the problem of process speed reduction. With the improvement of the process speed, the continuous transverse crystallization process can simultaneously reduce the overlapping area of the melting area so as to prevent the polycrystalline silicon layer from absorbing excessive laser energy and reduce the possibility of the polycrystalline silicon layer breaking due to agglomeration.

Description

一种用于连续横向结晶技术的掩膜及使用该掩膜的方法A mask for continuous lateral crystallization technology and a method for using the mask

技术领域technical field

本发明涉及一种掩膜,尤其涉及一种用于连续横向结晶(SLS:SequentialLateral Solidification)技术的掩膜及使用该掩膜的方法。The present invention relates to a mask, in particular to a mask for SLS (Sequential Lateral Solidification) technology and a method for using the mask.

背景技术Background technique

近年来,液晶显示器(LCD:Liquid Crystal Display)因其轻薄、省电、无幅射的优点,逐渐取代了传统阴极射线管(CRT:Cathode Ray Tube)显示器,广泛应用于桌上型计算机、个人数字助理器、笔记型计算机、数字相机与行动电话等电子产品中。In recent years, liquid crystal displays (LCD: Liquid Crystal Display) have gradually replaced traditional cathode ray tube (CRT: Cathode Ray Tube) displays due to their advantages of thinness, power saving, and no radiation, and are widely used in desktop computers, personal In electronic products such as digital assistants, notebook computers, digital cameras and mobile phones.

如图1所示,为一种典型主动矩阵式液晶显示面板的示意图。此液晶显示面板10上具有多个像素元件12呈矩阵排列。每一个像素元件12均连接至一个薄膜晶体管(TFT:Thin Film Transistor)14,作为开关以控制像素元件12的充放电。此薄膜晶体管14的源极通过一信号线16电连接至一源极驱动电路(未图标),而其栅极通过一扫描线18电连接至一扫描驱动电路(未图标)。因此,外界输入的显示信号可以转换为源极驱动电压Vs与扫描驱动电压Vg分别输入各个薄膜晶体管14的源极与栅极以产生画面。As shown in FIG. 1 , it is a schematic diagram of a typical active matrix liquid crystal display panel. The liquid crystal display panel 10 has a plurality of pixel elements 12 arranged in a matrix. Each pixel element 12 is connected to a thin film transistor (TFT: Thin Film Transistor) 14 as a switch to control the charging and discharging of the pixel element 12 . The source of the thin film transistor 14 is electrically connected to a source driving circuit (not shown) through a signal line 16 , and its gate is electrically connected to a scanning driving circuit (not shown) through a scanning line 18 . Therefore, the display signal input from the outside can be converted into a source driving voltage Vs and a scanning driving voltage Vg respectively input to the source and gate of each thin film transistor 14 to generate a picture.

一般而言,受限于玻璃基板所能承受的温度,直接制作于液晶显示面板10上的薄膜晶体管14,采用非晶硅(Amorphous Silicon)的设计。然而,非晶硅薄膜晶体管(a-TFT:Amorphous This Film Transistor)的开关速度、电性效果以及可靠度,都不足以适应驱动电路所需的高运算速度。因此,驱动电路必须使用多晶硅薄膜晶体管作为开关元件,导致驱动电路必须制作于硅芯片上,并通过排线连接至液晶显示面板10以控制像素元件12的显示。Generally speaking, the TFT 14 directly fabricated on the liquid crystal display panel 10 adopts an amorphous silicon (Amorphous Silicon) design due to the limitation of the temperature that the glass substrate can withstand. However, the switching speed, electrical effect and reliability of the amorphous silicon thin film transistor (a-TFT: Amorphous This Film Transistor) are not enough to meet the high computing speed required by the driving circuit. Therefore, the driving circuit must use polysilicon thin film transistors as switching elements, so that the driving circuit must be fabricated on a silicon chip and connected to the liquid crystal display panel 10 through wiring to control the display of the pixel elements 12 .

然而,随着液晶显示面板10尺寸增大,传统的非晶硅薄膜晶体管所提供的开关速度已逐渐不敷使用。为了提高液晶显示面板的显示效果,开且为了使驱动电路得以制作于显示面板上来达到轻薄化的需求,必须设法在玻璃基板上制作多晶硅薄膜晶体管。因此,必须设法在玻璃基板上制作高品质的多晶硅层。However, as the size of the liquid crystal display panel 10 increases, the switching speed provided by the traditional amorphous silicon thin film transistor is gradually insufficient. In order to improve the display effect of the liquid crystal display panel, and in order to make the driving circuit on the display panel to achieve light and thin requirements, it is necessary to try to fabricate polysilicon thin film transistors on the glass substrate. Therefore, it is necessary to try to make a high-quality polysilicon layer on the glass substrate.

如图2所示,为一典型低温多晶硅工艺的示意图。如图中所示,一非晶硅层120形成于一基板100表面,激光在非晶硅层120的表面形成一熔融层122。此熔融层122下方尚未熔融的非晶硅材料作为结晶所需的晶种,向上成长形成晶粒126。然而,此工艺所能提供的晶粒126尺寸往往不及一微米,无法有效提高薄膜晶体管的电性。As shown in FIG. 2 , it is a schematic diagram of a typical low temperature polysilicon process. As shown in the figure, an amorphous silicon layer 120 is formed on the surface of a substrate 100 , and a laser forms a molten layer 122 on the surface of the amorphous silicon layer 120 . The unmelted amorphous silicon material under the molten layer 122 acts as a seed crystal required for crystallization, and grows upward to form crystal grains 126 . However, the grain size 126 provided by this process is often less than one micron, which cannot effectively improve the electrical properties of the thin film transistor.

为了提高晶粒的尺寸,请参照图3,在一典型横向结晶(LateralSolidification)工艺中,激光通过掩膜200熔融非晶硅层120的特定区域A,同时,也在此熔融区域A中产生横向的热梯度。此熔融区域A侧边尚未熔融的非晶硅材料作为晶种,往熔融区域A的中央成长以产生较大尺寸的晶粒128。In order to increase the grain size, please refer to FIG. 3 , in a typical lateral crystallization (LateralSolidification) process, the laser passes through the mask 200 to melt the specific region A of the amorphous silicon layer 120, and at the same time, a lateral solidification is also produced in the molten region A. thermal gradient. The non-melted amorphous silicon material at the side of the molten region A acts as a seed crystal and grows toward the center of the molten region A to generate larger-sized crystal grains 128 .

如图4A所示,为典型用于连续横向结晶(SLS:Sequential LateralSolidification)工艺的掩膜300的示意图。如图中所示,此掩膜300具有多个第一透明光栅(slit)310与多个排列其上的第二透明光栅320。第一透明光栅310与第二透明光栅320的前缘与后缘分别采用三角形对称图案的设计。每一个第一透明光栅310对齐相邻二个第二透明光栅320间的不透光区。并且,第一透明光栅310的宽度大于相邻二个第二透明光栅320的间距。As shown in FIG. 4A , it is a schematic diagram of a mask 300 typically used in a sequential lateral solidification (SLS: Sequential Lateral Solidification) process. As shown in the figure, the mask 300 has a plurality of first transparent slits 310 and a plurality of second transparent slits 320 arranged thereon. The front edge and the rear edge of the first transparent grating 310 and the second transparent grating 320 adopt a triangular symmetrical pattern design respectively. Each first transparent grating 310 is aligned with the opaque area between two adjacent second transparent gratings 320 . Moreover, the width of the first transparent grating 310 is greater than the distance between two adjacent second transparent gratings 320 .

图4B与4C显示其它用于连续横向结晶工艺的掩膜301,302设计的示意图。相较于图4A的掩膜300设计,掩膜301,302上的透明光栅的前缘与后缘,分别采用矩形、半圆形对称图案的设计。4B and 4C show schematic diagrams of other mask 301, 302 designs for continuous lateral crystallization processes. Compared with the design of the mask 300 in FIG. 4A , the front and rear edges of the transparent gratings on the masks 301 and 302 respectively adopt rectangular and semicircular symmetrical patterns.

如图5所示,为使用图4A的掩膜进行连续横向结晶工艺的示意图。首先,在第一次激光熔融步骤中(如图中虚线所示),激光通过掩膜300上的第一透明光栅310与第二透明光栅320,以一定缩小比例,照射至非晶硅层,而在非晶硅层上形成熔融区域。同时如图6所示,为放大显示在此次激光熔融步骤中所形成的第一结晶区域A1。由于透明光栅310与320的周围处会因为光线的干涉与散射而产生结晶方向紊乱的不均匀区a,因此,只有第一结晶区域A1的中央部分可以为理想的均匀横向结晶区b。因此,图6A的横向结晶区b的长度L至多仅能与透明光栅的长边投射于此非晶硅层的长度L1相等。As shown in FIG. 5 , it is a schematic diagram of a continuous lateral crystallization process using the mask of FIG. 4A . First, in the first laser melting step (as shown by the dotted line in the figure), the laser passes through the first transparent grating 310 and the second transparent grating 320 on the mask 300, and irradiates the amorphous silicon layer at a certain reduction ratio. Instead, a molten region is formed on the amorphous silicon layer. Meanwhile, as shown in FIG. 6 , the first crystalline region A1 formed in this laser melting step is enlarged. Since the inhomogeneous region a with disordered crystal direction will be generated around the transparent gratings 310 and 320 due to light interference and scattering, only the central part of the first crystallization region A1 can be an ideal uniform lateral crystallization region b. Therefore, the length L of the lateral crystalline region b in FIG. 6A can only be at most equal to the length L1 of the projection of the long side of the transparent grating on the amorphous silicon layer.

在第二次激光熔融步骤中(如图5中实线部分),向右移动掩膜300,使第一透明光栅310对准第一结晶区域A1间尚未结晶的部分。由于第一透明光栅的宽度大于相邻二个第二透明光栅的间距,因此,如图6B所示,此次激光照射步骤中所产生的第二结晶区域A2与第一结晶区域A1的长边会有部分重叠。因此,位于第一结晶区域A1长边周围的不均匀区a,可通过此步骤重新熔融以改善其结晶效果。In the second laser melting step (as shown by the solid line in FIG. 5 ), the mask 300 is moved to the right, so that the first transparent grating 310 is aligned with the uncrystallized portion between the first crystallization regions A1 . Since the width of the first transparent grating is greater than the distance between two adjacent second transparent gratings, as shown in FIG. 6B, the second crystallization region A2 produced in this laser irradiation step and the long side of the first crystallization region A1 There will be some overlap. Therefore, the inhomogeneous region a located around the long side of the first crystallization region A1 can be re-melted through this step to improve its crystallization effect.

至于第一结晶区域A1前缘与后缘附近的不均匀区a,必须通过减少掩膜的移动距离来改善。进一步来说,如图6C所示,第一次激光熔融步骤所形成的第一结晶区域A1与第二次激光熔融步骤所形成的第三结晶区域A3的距离D必须小于横向结晶区b的长度L1,以确保第一结晶区域A1的前缘与第三结晶区域A3的后缘有充分的重叠,以有效消除不均匀区a。因此,此掩膜移动距离无法提高而导致工艺速度受到限制。同时,由于第一结晶区域A1与第三结晶区A3的重叠面积增加,会使得聚块作用(agglomeration)导致多晶硅层破洞的机会提高。As for the uneven region a near the leading edge and the trailing edge of the first crystalline region A1, it must be improved by reducing the moving distance of the mask. Further, as shown in FIG. 6C, the distance D between the first crystalline region A1 formed in the first laser melting step and the third crystalline region A3 formed in the second laser melting step must be smaller than the length of the lateral crystalline region b L1, to ensure that the leading edge of the first crystalline region A1 fully overlaps the trailing edge of the third crystalline region A3, so as to effectively eliminate the uneven region a. Therefore, the mask moving distance cannot be increased and the process speed is limited. At the same time, since the overlapping area of the first crystalline region A1 and the third crystalline region A3 increases, the possibility of agglomeration causing holes in the polysilicon layer increases.

发明内容Contents of the invention

本发明的目的在于提供一种应用于连续横向结晶的掩膜,除了可以有效消除不均匀区a外,并且还可以避免工艺速度下降的问题。The object of the present invention is to provide a mask applied to continuous lateral crystallization, which can effectively eliminate the non-uniform region a and avoid the problem of process speed reduction.

本发明提供一种用于连续横向结晶技术,将非晶硅层结晶形成多晶层的掩膜,包括:The present invention provides a continuous lateral crystallization technique for crystallizing an amorphous silicon layer to form a polycrystalline layer mask, comprising:

至少一透明光栅,该透明光栅包括二长边,一前缘与一后缘,所述二长边相互平行且长度相等,所述前缘朝向所述透明光栅的外侧突出,所述后缘朝向所述透明光栅的内部凹陷。At least one transparent grating, the transparent grating includes two long sides, a front edge and a rear edge, the two long sides are parallel to each other and have the same length, the front edge protrudes toward the outside of the transparent grating, and the rear edge faces The interior of the transparent grating is concave.

所述前缘的形状为V型、圆弧型或梯型。The shape of the front edge is V-shaped, arc-shaped or trapezoidal.

所述后缘的形状为V型、圆弧型或梯型。The shape of the trailing edge is V-shaped, arc-shaped or trapezoidal.

所述前缘的形状为V型,所述后缘的形状为V型,并且,所述V型前缘的顶角小于或等于所述V型后缘的顶角。The shape of the front edge is V-shaped, the shape of the trailing edge is V-shape, and the top angle of the V-shaped front edge is smaller than or equal to the top angle of the V-shaped trailing edge.

所述V型前缘的顶角介于10度至90度。The top angle of the V-shaped leading edge ranges from 10 degrees to 90 degrees.

所述V型后缘的顶角介于90度至170度。The top angle of the V-shaped trailing edge ranges from 90 degrees to 170 degrees.

本发明还提供一种用于横向结晶技术将非晶层结晶形成多晶层的掩膜,包括:The present invention also provides a mask for crystallizing an amorphous layer to form a polycrystalline layer by a lateral crystallization technique, comprising:

至少一透明光栅,该透明光栅包括二长边,一前缘与一后缘,所述二长边相互平行且长度相等,所述前缘朝向所述透明光栅的外侧突出,所述后缘成直线连接至所述二长边。At least one transparent grating, the transparent grating includes two long sides, a front edge and a rear edge, the two long sides are parallel to each other and have the same length, the front edge protrudes toward the outside of the transparent grating, and the rear edge forms a A straight line connects to the two long sides.

所述前缘的形状为V型、圆弧型或梯型。The shape of the front edge is V-shaped, arc-shaped or trapezoidal.

所述前缘呈V型且其顶角介于10度至90度。The front edge is V-shaped with a top angle ranging from 10° to 90°.

本发明还提供一种利用一掩膜结晶非晶硅层的方法,所述掩膜具有至少一透明光栅,该透明光栅具有二长边,一前缘与一后缘,所述前缘朝向所述透明光栅的外侧突出,所述后缘朝向所述透明光栅的内部凹陷,该方法至少包括下列步骤:The present invention also provides a method for crystallizing an amorphous silicon layer using a mask having at least one transparent grating with two long sides, a leading edge and a trailing edge, the leading edge facing the The outside of the transparent grating protrudes, and the trailing edge is recessed toward the inside of the transparent grating. The method at least includes the following steps:

提供一基板;providing a substrate;

制作一非晶硅层于所述基板上;making an amorphous silicon layer on the substrate;

将所述掩膜对准所述基板;aligning the mask to the substrate;

通过所述掩膜熔融所述非晶硅层,以在该非晶硅层中产生多个第一结晶区域分别对应至所述透明光栅;melting the amorphous silicon layer through the mask to generate a plurality of first crystalline regions in the amorphous silicon layer respectively corresponding to the transparent grating;

横向移动所述掩膜,使所述透明光栅的前缘或后缘与所述第一结晶区域重叠;laterally moving the mask such that a leading edge or a trailing edge of the transparent grating overlaps the first crystallized region;

通过所述掩膜熔融所述非晶硅层,以产生多个第二结晶区域。The amorphous silicon layer is melted through the mask to produce a plurality of second crystalline regions.

所述掩膜横向移动的距离小于所述透明光栅长边的长度。The distance that the mask moves laterally is less than the length of the long side of the transparent grating.

所述掩膜横向移动的距离大于所述透明光栅长边的长度减去所述后缘凹陷的距离。The distance that the mask moves laterally is greater than the length of the long side of the transparent grating minus the distance of the trailing edge depression.

本发明的有益之处在于,可以有效消除不均匀区,还可以避免工艺速度下降的问题。随着工艺速度的提高,本发明的连续横向结晶工艺可以同时减少熔融区域的重叠面积,以防止多晶硅层吸收过多激光能量,以降低多晶硅层因聚块作用而导致破洞的可能性。The advantage of the present invention is that it can effectively eliminate the non-uniform area, and also avoid the problem of process speed reduction. As the process speed increases, the continuous lateral crystallization process of the present invention can simultaneously reduce the overlapping area of the melting region, so as to prevent the polysilicon layer from absorbing too much laser energy and reduce the possibility of polysilicon layer being broken due to agglomeration.

附图说明Description of drawings

图1为一主动矩阵式液晶显示面板的示意图;1 is a schematic diagram of an active matrix liquid crystal display panel;

图2为一低温多晶硅工艺的示意图;2 is a schematic diagram of a low-temperature polysilicon process;

图3为一横向结晶工艺的示意图;3 is a schematic diagram of a lateral crystallization process;

图4A、图4B和图4C为用于连续横向结晶工艺的掩膜的示意图;4A, 4B and 4C are schematic diagrams of masks used in a continuous lateral crystallization process;

图5为使用图4A的掩膜进行连续横向结晶工艺的示意图;5 is a schematic diagram of a continuous lateral crystallization process using the mask of FIG. 4A;

图6A为放大显示在图5的连续横向结晶工艺中所形成的第一结晶区域;6A is an enlarged view of the first crystalline region formed in the continuous lateral crystallization process of FIG. 5;

图6B为放大显示在图5的连续横向结晶工艺中所形成的第二结晶区域与第一结晶区域;FIG. 6B is an enlarged view showing the second crystalline region and the first crystalline region formed in the continuous lateral crystallization process of FIG. 5;

图6C为放大显示在图5的连续横向结晶工艺中所形成的第一结晶区域与第三结晶区域;6C is an enlarged view of the first crystalline region and the third crystalline region formed in the continuous lateral crystallization process of FIG. 5;

图7A至图7I所示为本发明掩膜的透明光栅第一至第九实施例的示意图;7A to 7I are schematic diagrams of the first to ninth embodiments of the transparent grating of the mask of the present invention;

图8A为使用图7A的掩膜进行连续横向结晶工艺时掩膜移动的示意图;FIG. 8A is a schematic diagram of mask movement when using the mask of FIG. 7A for a continuous lateral crystallization process;

图8B与图8C图分别为显示在图8A的连续横向结晶工艺中所形成的第一结晶区域与第二结晶区域。8B and 8C are diagrams respectively showing the first crystallization region and the second crystallization region formed in the continuous lateral crystallization process of FIG. 8A .

图号说明:Description of figure number:

液晶显示面板10        像素元件12LCD panel 10 pixel element 12

薄膜晶体管14          信号线16Thin film transistor 14 Signal line 16

扫描线18              非晶硅层120Scanning line 18 Amorphous silicon layer 120

基板100               熔融层122Substrate 100 Fusion layer 122

晶粒126,128        掩膜200,300,301,302Die 126, 128 Mask 200, 300, 301, 302

第一透明光栅310     第二透明光栅320The first transparent grating 310 The second transparent grating 320

不均匀区a           均匀横向结晶区bInhomogeneous region a Uniform lateral crystallization region b

具体实施方式Detailed ways

如图7A所示,为本发明掩膜所具有的透明光栅第1实施例的示意图。如图中所示,此透明光栅具有二相对应长边、一前缘与一后缘。其中,二相对应长边相互平行且长度相等(长度均为X1)。前缘呈现V型,其尖端位于透明光栅的中心线上,并且朝向透明光栅的外侧(即图中的右侧)突出一预定距离F1。后缘呈现V型,其尖端位于透明光栅的中心线上,并且朝向透明光栅的内部(即图中的右侧)凹陷一预定距离R1。As shown in FIG. 7A , it is a schematic view of the first embodiment of the transparent grating included in the mask of the present invention. As shown in the figure, the transparent grating has two corresponding long sides, a leading edge and a trailing edge. Wherein, the two corresponding long sides are parallel to each other and have the same length (the lengths are both X1). The front edge is V-shaped, its tip is located on the center line of the transparent grating, and protrudes a predetermined distance F1 toward the outside of the transparent grating (ie, the right side in the figure). The trailing edge is V-shaped, its tip is located on the center line of the transparent grating, and is recessed toward the inside of the transparent grating (ie, the right side in the figure) for a predetermined distance R1.

虽然本实施例中,V型前缘与V型后缘具有相同的外型,而此V型前缘突出的距离F1与V型后缘凹陷的距离R1也相同。然而,本发明并不限于此。图7B所示,在本发明透明光栅的第二实施例中,V型前缘突出的距离F2大于V型后缘凹陷的距离R2。换言之,此透明光栅的V型前缘的顶角c小于V型后缘的顶角d。就一较佳实施例而言,V型前缘的顶角c最好介于10度至90度,而V型后缘的顶角d最好介于90度至170度。Although in this embodiment, the V-shaped front edge and the V-shaped trailing edge have the same shape, the protruding distance F1 of the V-shaped leading edge and the concave distance R1 of the V-shaped trailing edge are also the same. However, the present invention is not limited thereto. As shown in FIG. 7B , in the second embodiment of the transparent grating of the present invention, the protruding distance F2 of the V-shaped front edge is greater than the concave distance R2 of the V-shaped trailing edge. In other words, the apex angle c of the V-shaped leading edge of the transparent grating is smaller than the apex angle d of the V-shaped trailing edge. As for a preferred embodiment, the top angle c of the V-shaped leading edge is preferably between 10° and 90°, and the top angle d of the V-shaped trailing edge is preferably between 90° and 170°.

如图7A至图7F所示,显示本发明透明光栅第一至第六实施例。如图中所示,此透明光栅的前缘可以为V型(如图7A与图7B所示)、圆弧型(如图7C与图7D所示)或梯型(如图7E与图7F所示)等不同外型;而后缘也可以为V型(如图7A与图7B所示)、圆弧型(如图7C与图7D所示)或梯型(如图7E与图7F所示)等不同外型。As shown in FIG. 7A to FIG. 7F , the first to sixth embodiments of the transparent grating of the present invention are shown. As shown in the figure, the leading edge of the transparent grating can be V-shaped (as shown in Figure 7A and Figure 7B ), arc-shaped (as shown in Figure 7C and Figure 7D ), or trapezoidal (as shown in Figure 7E and Figure 7F shown) and other different shapes; and the trailing edge can also be V-shaped (as shown in Figure 7A and Figure 7B), arc-shaped (as shown in Figure 7C and Figure 7D) or trapezoidal (as shown in Figure 7E and Figure 7F Show) and other different appearance.

此外,上述各个实施例的透明光栅,其前缘与后缘均采用相同的形状类型。也就是说,若是透明光栅的前缘为V型,其后缘也采用V型(如图7A与图7B所示);若是透明光栅的前缘为圆弧型,其后缘也采用圆弧型(如图7C与图7D所示),而若是透明光栅的前缘为梯型,其后缘也采用梯型(如图7E与图7F所示)。In addition, the transparent gratings in each of the above embodiments adopt the same shape type at the leading edge and the trailing edge. That is to say, if the front edge of the transparent grating is V-shaped, its trailing edge is also V-shaped (as shown in FIGS. 7A and 7B ); if the front edge of the transparent grating is arc-shaped, its trailing edge is also arc-shaped. type (as shown in FIG. 7C and FIG. 7D ), and if the front edge of the transparent grating is trapezoidal, its trailing edge is also trapezoidal (as shown in FIG. 7E and FIG. 7F ).

其次,本发明透明光栅的前缘突出的距离与后缘凹陷的距离,可以相同(如图7A、图7C和图7E所示),也可以不同(如图7B、图7D与图7F所示)。前缘突出的距离最好是大于后缘凹陷的距离。此外,请参照图7G至图7I,在本发明透明光栅第七至九实施例中,透明光栅的前缘分别为V型、圆弧型或梯型,然而,其后缘凹陷的距离减少至零,也就是后缘采用直线的形状。Secondly, the protruding distance of the leading edge and the concave distance of the trailing edge of the transparent grating of the present invention can be the same (as shown in Figure 7A, Figure 7C and Figure 7E), or different (as shown in Figure 7B, Figure 7D and Figure 7F ). The distance by which the leading edge protrudes is preferably greater than the distance by which the trailing edge is recessed. In addition, please refer to FIG. 7G to FIG. 7I. In the seventh to ninth embodiments of the transparent grating of the present invention, the front edges of the transparent grating are respectively V-shaped, arc-shaped or trapezoidal, however, the distance of the trailing edge depression is reduced to Zero, that is, the trailing edge adopts the shape of a straight line.

如图8A所示,为使用本发明的掩膜进行连续横向结晶工艺的示意图。图中是以图7A的透明光栅为例进行说明。在此连续横向结晶工艺中,首先,提供一基板,并且制作一非晶硅层于此基板上(请同时参照图2)。随后,如图8A中虚线所示,在第一次激光熔融步骤中,将掩膜对准基板。激光透过掩膜上的透明光栅,以一定的缩放比例投射于非晶硅层,而在非晶硅层中产生多个第一结晶区B1(请参照第图8B)。随后,如图8A中实线所示,横向移动掩膜,以进行后续的第二次激光熔融步骤。激光透过掩膜熔融非晶硅层,以产生多个第二结晶区域B2(请参照图8C图)。As shown in FIG. 8A , it is a schematic diagram of a continuous lateral crystallization process using the mask of the present invention. In the figure, the transparent grating shown in FIG. 7A is taken as an example for illustration. In the continuous lateral crystallization process, firstly, a substrate is provided, and an amorphous silicon layer is formed on the substrate (please also refer to FIG. 2 ). Subsequently, the mask is aligned to the substrate in the first laser melting step, as indicated by the dotted line in FIG. 8A. The laser beam passes through the transparent grating on the mask and projects on the amorphous silicon layer with a certain scaling ratio, so as to generate a plurality of first crystalline regions B1 in the amorphous silicon layer (please refer to FIG. 8B ). Subsequently, as shown by the solid line in FIG. 8A , the mask is moved laterally for a subsequent second laser melting step. The laser passes through the mask to melt the amorphous silicon layer to generate a plurality of second crystalline regions B2 (please refer to FIG. 8C ).

值得注意的是,如图8C所示,第二次激光熔融步骤所形成的第二结晶区域B2,其前缘必须与第一结晶区域B1后缘有充分的重叠,以确保产生于第一结晶区域B1后缘结晶方向紊乱的不均匀区,可经此熔融步骤得到修补。由此可见,为了确保良好的结晶效果,第一结晶区域B1与第二结晶区域B2的间距D1,必须小于第一结晶区域B1的长边的长度S1。因此,此间距D1必须小于透明光栅长边的长度X1(如图8A所示)乘上此透明光栅投射至非晶硅层的缩小比例。此外,虽然在上述连续横向结晶工艺中,如图8A所示,掩膜向图中右方移动,以进行后续的激光熔融步骤;然而,本发明并不限于此。如前所述,只要确保相邻二次激光熔融步骤的距离D1小于结晶区域的长边长度S1,至于掩膜的移动方向,并没有限制。It is worth noting that, as shown in Figure 8C, the leading edge of the second crystalline region B2 formed in the second laser melting step must fully overlap with the trailing edge of the first crystalline region B1, so as to ensure that the first crystalline The inhomogeneous region with disordered crystal direction at the trailing edge of region B1 can be repaired through this melting step. It can be seen that, in order to ensure a good crystallization effect, the distance D1 between the first crystalline region B1 and the second crystalline region B2 must be smaller than the length S1 of the long side of the first crystalline region B1. Therefore, the distance D1 must be smaller than the length X1 of the long side of the transparent grating (as shown in FIG. 8A ) multiplied by the reduction ratio of the projection of the transparent grating to the amorphous silicon layer. In addition, although in the above continuous lateral crystallization process, as shown in FIG. 8A , the mask is moved to the right in the figure to perform the subsequent laser melting step; however, the present invention is not limited thereto. As mentioned above, as long as the distance D1 between adjacent secondary laser melting steps is less than the length S1 of the long side of the crystallized region, there is no limitation on the moving direction of the mask.

相较于图6C的传统连续横向结晶工艺中,第一结晶区域A1与第三结晶区域A3的距离必须小于横向结晶区b的长度L1,以获得良好的结晶效果。如图8B所示,本发明的连续横向结晶工艺,在连续两次激光熔融步骤中所形成的第一结晶区域B1与第二结晶区域B2,其间距D1的大小则无此限制。Compared with the conventional continuous lateral crystallization process in FIG. 6C , the distance between the first crystallization region A1 and the third crystallization region A3 must be smaller than the length L1 of the lateral crystallization region b to obtain a good crystallization effect. As shown in FIG. 8B , in the continuous lateral crystallization process of the present invention, the distance D1 between the first crystallization region B1 and the second crystallization region B2 formed in two consecutive laser melting steps is not limited.

进一步来说,假定本发明的透明光栅与图4A传统透明光栅具有相同长度,本发明透明光栅与此传统透明光栅前缘突出的距离相同,并且,本发明透明光栅后缘凹陷的距离等同于此传统透明光栅的三角型后缘突出的距离。请参照图6A与图8A,透过传统透明光栅所形成的第一结晶区域A1的侧边长度L,等于透过本发明透明光栅所形成的第一结晶区域B1的长边长度S1减去后缘凹陷的距离r。如图8A所示,本发明的连续横向结晶工艺,显然容许第一结晶区域B1与第二结晶区域B2的间隔距离D1,提高至大于第一结晶区域B1的长边长度S1减去后缘凹陷的距离r。因此,本发明的连续横向结晶工艺的连续二次激光熔融步骤,所容许的掩膜移动距离大于传统连续横向结晶工艺所容许的移动距离。因此,相较于采用传统掩膜设计的连续横向结晶工艺,本发明的连续横向结晶工艺可以达到较高的工艺速度。随着工艺速度的提高,本发明的连续横向结晶工艺可以同时减少熔融区域的重叠面积,以防止多晶硅层吸收过多激光能量,以降低多晶硅层因聚块作用而导致破洞的可能性。Further, assuming that the transparent grating of the present invention has the same length as the traditional transparent grating of FIG. The distance by which the triangular trailing edge of a conventional transparent grating protrudes. Please refer to FIG. 6A and FIG. 8A, the side length L of the first crystalline region A1 formed through the conventional transparent grating is equal to the long side length S1 of the first crystalline region B1 formed through the transparent grating of the present invention after subtraction The distance r of the edge depression. As shown in FIG. 8A, the continuous lateral crystallization process of the present invention obviously allows the separation distance D1 between the first crystallization region B1 and the second crystallization region B2 to be increased to be greater than the long side length S1 of the first crystallization region B1 minus the trailing edge depression The distance r. Therefore, the allowable moving distance of the mask in the continuous secondary laser melting step of the continuous lateral crystallization process of the present invention is greater than the allowable moving distance of the traditional continuous lateral crystallization process. Therefore, compared with the continuous lateral crystallization process using traditional mask design, the continuous lateral crystallization process of the present invention can achieve a higher process speed. As the process speed increases, the continuous lateral crystallization process of the present invention can simultaneously reduce the overlapping area of the melting region, so as to prevent the polysilicon layer from absorbing too much laser energy and reduce the possibility of polysilicon layer being broken due to agglomeration.

以上具体实施例仅用于说明本发明,而非用于限定本发明。The above specific embodiments are only used to illustrate the present invention, but not to limit the present invention.

Claims (10)

1.一种用于连续横向结晶技术的掩膜,其特征在于,包括:1. A mask for continuous lateral crystallization technology, characterized in that it comprises: 至少一透明光栅,该透明光栅包括二长边,一前缘与一后缘,所述二长边相互平行且长度相等,所述前缘朝向所述透明光栅的外侧突出,所述后缘朝向所述透明光栅的内部凹陷。At least one transparent grating, the transparent grating includes two long sides, a front edge and a rear edge, the two long sides are parallel to each other and have the same length, the front edge protrudes toward the outside of the transparent grating, and the rear edge faces The interior of the transparent grating is concave. 2.如权利要求1所述的用于连续横向结晶技术的掩膜,其特征在于,所述前缘的形状为V型、圆弧型或梯型。2. The mask for continuous lateral crystallization according to claim 1, wherein the shape of the front edge is V-shaped, arc-shaped or trapezoidal. 3.如权利要求1所述的用于连续横向结晶技术的掩膜,其特征在于,所述后缘的形状为V型、圆弧型或梯型。3. The mask for continuous lateral crystallization according to claim 1, wherein the shape of the trailing edge is V-shaped, arc-shaped or trapezoidal. 4.如权利要求1所述的用于连续横向结晶技术的掩膜,其特征在于,所述前缘的形状为V型,所述后缘的形状为V型,并且,所述V型前缘的顶角小于或等于所述V型后缘的顶角。4. The mask for continuous lateral crystallization technology according to claim 1, wherein the shape of the leading edge is V-shaped, the shape of the trailing edge is V-shaped, and the V-shaped front The apex angle of the edge is less than or equal to the apex angle of the V-shaped trailing edge. 5.如权利要求4所述的用于连续横向结晶技术的掩膜,其特征在于,所述V型前缘的顶角介于10度至90度。5 . The mask for continuous lateral crystallization as claimed in claim 4 , wherein the top angle of the V-shaped front edge ranges from 10° to 90°. 6.如权利要求4所述的用于连续横向结晶技术的掩膜,其特征在于,所述V型后缘的顶角介于90度至170度。6 . The mask for continuous lateral crystallization as claimed in claim 4 , wherein the top angle of the V-shaped trailing edge is between 90° and 170°. 7.一种用于连续横向结晶技术的掩膜,其特征在于,包括:7. A mask for continuous lateral crystallization technology, comprising: 至少一透明光栅,该透明光栅包括二长边,一前缘与一后缘,所述二长边相互平行且长度相等,所述前缘朝向所述透明光栅的外侧突出,所述后缘成直线连接至所述二长边。At least one transparent grating, the transparent grating includes two long sides, a front edge and a rear edge, the two long sides are parallel to each other and have the same length, the front edge protrudes toward the outside of the transparent grating, and the rear edge forms a A straight line connects to the two long sides. 8.如权利要求7所述的用于连续横向结晶技术的掩膜,其特征在于,所述前缘的形状为V型、圆弧型或梯型。8. The mask for continuous lateral crystallization according to claim 7, wherein the shape of the front edge is V-shaped, arc-shaped or trapezoidal. 9.如权利要求8所述的用于连续横向结晶技术的掩膜,其特征在于,所述前缘呈V型且其顶角介于10度至90度。9 . The mask for continuous lateral crystallization as claimed in claim 8 , wherein the leading edge is V-shaped and its top angle is between 10° and 90°. 10.一种利用一掩膜结晶非晶硅层的方法,其特征在于,所述掩膜具有至少一透明光栅,该透明光栅具有二长边,一前缘与一后缘,所述前缘朝向所述透明光栅的外侧突出,所述后缘朝向所述透明光栅的内部凹陷,该方法至少包括下列步骤:10. A method for crystallizing an amorphous silicon layer using a mask, wherein the mask has at least one transparent grating, the transparent grating has two long sides, a leading edge and a trailing edge, the leading edge protruding toward the outside of the transparent grating, and the trailing edge is recessed toward the inside of the transparent grating, the method at least includes the following steps: 提供一基板;providing a substrate; 制作一非晶硅层于所述基板上;making an amorphous silicon layer on the substrate; 将所述掩膜对准所述基板;aligning the mask to the substrate; 通过所述掩膜熔融所述非晶硅层,以在该非晶硅层中产生多个第一结晶区域分别对应至所述透明光栅;melting the amorphous silicon layer through the mask to generate a plurality of first crystalline regions in the amorphous silicon layer respectively corresponding to the transparent grating; 横向移动所述掩膜,使所述透明光栅的前缘或后缘与所述第一结晶区域重叠,其中所述掩膜横向移动的距离小于所述透明光栅长边的长度且大于所述透明光栅长边的长度减去所述后缘凹陷的距离;moving the mask laterally so that the leading edge or the trailing edge of the transparent grating overlaps the first crystallized region, wherein the distance the mask moves laterally is less than the length of the long side of the transparent grating and greater than the length of the transparent grating the length of the long side of the grating minus the distance of the trailing edge depression; 通过所述掩膜熔融所述非晶硅层,以产生多个第二结晶区域。The amorphous silicon layer is melted through the mask to produce a plurality of second crystalline regions.
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