TWI267987B - Method for forming thin film transistor in an LCD device - Google Patents

Method for forming thin film transistor in an LCD device Download PDF

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TWI267987B
TWI267987B TW94102441A TW94102441A TWI267987B TW I267987 B TWI267987 B TW I267987B TW 94102441 A TW94102441 A TW 94102441A TW 94102441 A TW94102441 A TW 94102441A TW I267987 B TWI267987 B TW I267987B
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Taiwan
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layer
forming
thin film
gate insulating
film transistor
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TW94102441A
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TW200627645A (en
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Chin-Kuo Ting
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Quanta Display Inc
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Abstract

In a method for forming TFT in an LCD device, a buffer layer and a polysilicon layer are sequentially formed on a transparent substrate first. Then, a gate dielectric layer is formed on surface of the polysilicon layer by using plasma treatment, wherein the plasma contains oxygen, nitrogen, or both, and the treatment temperature is between about 300 to 600 DEG C. Next, a gate electrode layer is formed on the gate dielectric layer, and a source and a drain regions are formed on the opposite direction of the gate electrode layer.

Description

1267987 — 五、發明說明(1) 【發明所屬之技術領域】 本發明係有關於一種右、為曰 在/夜晶顯示哭中形成舊 法,特別是有關於一種在笔γ千。。中升y f缚嗅電晶體的方 山生命两叫k 在涛&電晶體液晶顯示突士 π丄 朋潰電壓閘極絕緣層之方法 卞杰中形成高 -【先前技術】 目前’在液晶顯示器中的驅動,一〜 ,,.日 > :日日具有反應快的特性使得顯示器的。併 較佳。Z則,缚膜電晶體的結構有底部閘極與頂二 尋。在第一圖中’介紹一種形成頂部閘極:在 $步驟的結構示意圖。 狀兒日日肢在 第一 A圖中,在一玻璃基板i 〇 〇上沉積一緩衝層i 〇 2以及一 •非晶石夕層1 0 4,其中緩衝層i 〇 2的材料可選擇氧化石夕或是i 化石夕。然後,如第一 B圖所示,經由準分子雷射退火 ·( Excimer Laser Annealing; ELA),或是連續結晶石夕 (Continuous Grain Silicon; CGS),連續伽j 邊固 ^匕 (Sequential Lateral Solidification; SLS),金屬今秀 發結晶(Metal Induced Crystallization; MIC),咬是 鲁屬誘發側邊結晶(M e 1: a 1 I n d u c e d L a t e r a 1 Crystallization; MILC)等方式將非晶矽層104形成複晶 矽層1 0 6。之後,在第一 C圖中,使用電漿增益化學氣相沉 積(PECVD)法或是低壓化學氣相沉積(LPCVD)方式沉積 閘極氧化層1 0 8在複晶矽層1 0 6上。沉積的方式有使用石夕甲1267987 - V. INSTRUCTION DESCRIPTION OF THE INVENTION (1) [Technical Field of the Invention] The present invention relates to a method for forming a cry in the right, 曰 in / night crystal display, and particularly relates to a pen γ thousand. . Fangshan life of the yf-bound scented crystal is called k. In Tao & crystal liquid crystal display, the method of the smashing voltage barrier gate insulation is formed in the high-previous [current technology] in the liquid crystal display Drive, one ~, ,.day >: The day has a fast response feature that makes the display. And better. Z, the structure of the bonded transistor has a bottom gate and a top dipole. In the first figure, a schematic diagram of the formation of the top gate is shown in the step: In the first A picture, a buffer layer i 〇 2 and an amorphous austenite layer 104 are deposited on a glass substrate i ,, wherein the material of the buffer layer i 〇 2 is selectively oxidized. Shi Xi or i fossil eve. Then, as shown in Figure B, Execmer Laser Annealing (ELA), or Continuous Grain Silicon (CGS), Sequential Lateral Solidification ; SLS), Metal Induced Crystallization (MIC), the formation of amorphous germanium layer 104 by means of Mean 1: a 1 I nduced L atera 1 Crystallization; MILC The polycrystalline layer is 1 0 6 . Thereafter, in the first C picture, a gate oxide layer 108 is deposited on the polysilicon layer 106 using a plasma gain chemical vapor deposition (PECVD) method or a low pressure chemical vapor deposition (LPCVD) method. The way of deposition is to use Shi Xijia

第6頁 1267987___ 五、發明說明(2) 烷與Ν 2 0或是Ο 2反應形成氧化矽,或是使用四乙基矽甲烷 (TEOS)分解成氧化矽。接著,如第一 D圖所示,在閘極 氧化層1 0 8上形成閘極金屬層1 1 0。形成的方式包含將金屬 層沉積在閘極氧化層上,然後使用光學微影以及餘刻的方 式將閘極的圖案轉移到金屬層上。在第一 Ε圖中,以離子 植入機(ion implant er)或是離子雲(ion shower)的 方式在複晶矽層1 〇 6内形成輕摻雜汲極區1 1 2在閘極金屬層 ]1 0的兩側。之後,如第一 F圖所示,在閘極層1 1 0的側壁 上形成間隙壁1 1 4。然後,在第一 G圖中,以離子植入的方 晶矽層1 0 6内形成源極與汲極區1 1 6域在閘極金屬層 兩側。 因為傳統使用化學氣相沉積法,不論是電漿增益化學氣相 沉積或是低壓化學氣相沉積,所沉積之閘極氧化(ga t e oxide)層,其崩潰電壓(breakdown voltage)通常比較 ,小而且複晶石夕與氧化層的界面缺陷(i n t e r f a c e d e f e c t) 會比較多,容易產生漏電流。這樣的閘極氧化層品質對於 未來元件的縮小與整合式無法達成其需求。因此,為了增 加閘極氧化層品質,需要解決崩潰電壓過低與漏電流的問 馨;亦即增加其崩潰電壓與減少閘極氧化層與複晶矽界面 缺陷。 【發明内容】 傳統以化學氣相沉積法形成的閘 鑒於上述之發明背景中Page 6 1267987___ V. INSTRUCTIONS (2) The alkane reacts with Ν 2 0 or Ο 2 to form cerium oxide or is decomposed into cerium oxide using tetraethyl hydrazine (TEOS). Next, as shown in Fig. D, a gate metal layer 110 is formed on the gate oxide layer 108. The manner of formation involves depositing a metal layer on the gate oxide layer and then transferring the pattern of the gate to the metal layer using optical lithography and a residual pattern. In the first diagram, a lightly doped bungee region 1 1 2 is formed in the polysilicon layer 1 〇6 by means of an ion implanter or an ion shower. Layer] 1 0 on both sides. Thereafter, as shown in the first F diagram, a spacer 1 1 4 is formed on the sidewall of the gate layer 110. Then, in the first G picture, the source and drain regions 1 1 6 are formed on both sides of the gate metal layer by ion implantation of the germanium layer 10.6. Because of the traditional use of chemical vapor deposition, whether it is plasma gain chemical vapor deposition or low pressure chemical vapor deposition, the deposited ga te oxide layer, its breakdown voltage is usually compared, small Moreover, the interface defects of the polycrystalline stone and the oxide layer will be more, and leakage current is likely to occur. Such gate oxide quality cannot meet the needs of future component shrinkage and integration. Therefore, in order to increase the quality of the gate oxide layer, it is necessary to solve the problem of low breakdown voltage and leakage current; that is, increase the breakdown voltage and reduce the interface defects between the gate oxide layer and the germanium oxide layer. SUMMARY OF THE INVENTION A gate formed by a chemical vapor deposition method in view of the above-described background of the invention

第7頁 1267987 五、發明說明(3) 極氧化層所產生之諸多問題與缺點,本發明主要之目的在 於提供一種利用電漿處理的方式形成閘極絕緣層。主要是 利用已經形成之本質複晶矽(i n t r i n s i c ρ ο 1 y s i 1 i c ο η) 與包含氧氣或是氮氣的電漿在溫度3 0 0 - 6 0 0°C下反應成氧 化矽,氮化矽或是氮氧化矽等作為閘極絕緣層之介電材 料。 _本發明之另一目的為使用電漿處理所形成的閘極絕緣層具 備高的崩潰電壓。 t發明之又一目的為使用電漿處理所形成的閘極絕緣層較 低界面缺陷,因而有較低的漏電流。 本發明之再一目的為使用不同的反應氣體,在電漿處理的 過程中即可選擇需要成長的閘極絕緣層的材料。 根據以上所述之目的,本發明提供了 一種在液晶顯示器中 形成一薄膜電晶體的方法,其步驟包含在一透明基板上依 序形成一緩衝層與一複晶矽層。之後,在該複晶矽層表面 修以電漿處理複晶矽層以形成一閘極絕緣層。然後,在上 述之閘極絕緣層上形成一閘極層。接著,在上述之複晶矽 層内形成一源極與一没極區域在前述閘極層兩側。 本發明亦提供了 一種在薄膜電晶體液晶顯示器中形成高崩Page 7 1267987 V. DESCRIPTION OF THE INVENTION (3) A number of problems and disadvantages of the electrode layer are provided. The main object of the present invention is to provide a gate insulating layer by means of plasma processing. It is mainly formed by using the already formed intrinsic crystal enthalpy (intrinsic ρ ο 1 ysi 1 ic ο η) and a plasma containing oxygen or nitrogen to form cerium oxide and cerium nitride at a temperature of 300 to 600 ° C. Or a dielectric material such as ruthenium oxynitride as a gate insulating layer. Another object of the present invention is to provide a high breakdown voltage for the gate insulating layer formed by plasma treatment. A further object of the invention is that the gate insulating layer formed by the plasma treatment has lower interface defects and thus has a lower leakage current. A further object of the present invention is to use different reactive gases to select the material of the gate insulating layer that needs to be grown during the plasma processing. In accordance with the above objects, the present invention provides a method of forming a thin film transistor in a liquid crystal display, the method comprising the steps of sequentially forming a buffer layer and a polysilicon layer on a transparent substrate. Thereafter, the surface of the polysilicon layer is plasma-treated to treat the polysilicon layer to form a gate insulating layer. Then, a gate layer is formed on the gate insulating layer. Next, a source and a gate region are formed on both sides of the gate layer in the above-mentioned polysilicon layer. The invention also provides a high collapse in a thin film transistor liquid crystal display

第8頁 1267987 五、發明說明(4) t 潰電壓閘極絕緣層之方法,其步驟包含在一透明基板上形 成一複晶矽層。之後,在3 0 0 - 6 0 (TC之間以電漿處理上述 之複晶矽層以形成一閘極絕緣層,其中形成電漿之反應氣 體可包含氧氣或是氮氣,而上述閘極絕緣層可為氧化矽, 氮化矽,或是氮氧化矽。 【實施方式】 本發明的一些實施例會詳細描述如下。然而,除了詳細描 述的實施例外,本發明還可以廣泛地在其它的實施例中施 «,且本發明的範圍不受限定,其以之後的申請專利範圍 準。 再者,為提供更清楚的描述及更易理解本發明,圖示内各 部分並沒有依照其相對尺寸繪圖,某些尺寸與其他相關尺 度相比已經被誇張;不相關之細節部分也未完全繪出,以 味圖示的簡潔。 本發明係利用本質複晶石夕與包含氧或是氮等氣體之電聚’ 在溫度3 0 0 - 6 0 0°C下反應,然後形成閘極絕緣層。如果反 參氣體主要以氧氣為主,則閘極絕緣層為氧化矽。如果反 應氣體以氮氣為主,則閘極絕緣層為氮化矽。如果反應氣 體包含氧氣與氮氣,則閘極絕緣層可為氮氧化石夕。因為由 本質複晶矽所形成之閘極絕緣層,經過高溫處理後會變的 更緻密,因此也就可以得到更高的崩潰電壓。而且閘極絕Page 8 1267987 V. DESCRIPTION OF THE INVENTION (4) A method of breaking a voltage gate insulating layer, the method comprising forming a polysilicon layer on a transparent substrate. Thereafter, the above-mentioned polysilicon layer is plasma-treated between 300 and 60 (TC) to form a gate insulating layer, wherein the reaction gas forming the plasma may contain oxygen or nitrogen, and the gate is insulated. The layer may be tantalum oxide, tantalum nitride, or hafnium oxynitride. [Embodiment] Some embodiments of the present invention will be described in detail below. However, the present invention may be broadly applied to other embodiments except for the detailed description. The scope of the present invention is not limited by the scope of the following claims. Further, in order to provide a clearer description and a better understanding of the present invention, the various parts of the drawings are not drawn according to their relative sizes. Some dimensions have been exaggerated compared to other related scales; the unrelated details have not been fully drawn, and the succinct illustrations are simple. The present invention utilizes the essence of the polycrystalline stone and the electricity containing gases such as oxygen or nitrogen. The poly' reacts at a temperature of 300 to 600 ° C, and then forms a gate insulating layer. If the anti-gas is mainly oxygen, the gate insulating layer is cerium oxide. If the reaction gas is mainly nitrogen The gate insulating layer is tantalum nitride. If the reaction gas contains oxygen and nitrogen, the gate insulating layer may be nitrogen oxynitride. Because the gate insulating layer formed by the intrinsic polysilicon is processed after high temperature treatment It becomes denser, so you can get a higher breakdown voltage.

第9頁 1267987 五、發明說明(5) 緣層與複晶石夕之間的界面特性也較佳,漏電流因而可以降 低。再者’將透明基板放置在可旋轉之平台(Table) 上,可以增加閘極絕緣層薄膜薄膜厚度之均勻性。 本發明提供一種在液晶顯示器中形成一薄膜電晶體的方 法’其步驟包含在一透明基板上依序形成一緩衝層與一複 晶石夕層,其中之透明基板可為玻璃基板或是其他的高分子 聚合物。上述之複晶碎層的形成方式可為先沉積非晶矽層 在上述緩衝層上,然後以退火的方式將非晶矽層轉換成複 •石夕層。上述之退火的方式可為準分子雷射退火 (Exc i mer Laser Annealing; ELA)。然而,亦有其他的 方式直接形成複晶石夕層’例如連續結晶石夕(C ο n t i n u o u sPage 9 1267987 V. INSTRUCTIONS (5) The interface between the edge layer and the polycrystalline stone is also better, and the leakage current can be reduced. Furthermore, placing the transparent substrate on a rotatable table can increase the uniformity of the thickness of the gate insulating film film. The invention provides a method for forming a thin film transistor in a liquid crystal display, the step of which comprises sequentially forming a buffer layer and a polycrystalline layer on a transparent substrate, wherein the transparent substrate can be a glass substrate or the like. High molecular polymer. The above-mentioned polycrystalline fracture layer may be formed by depositing an amorphous germanium layer on the buffer layer and then annealing the amorphous germanium layer into a complex layer. The above annealing method may be Eximmer Laser Annealing (ELA). However, there are other ways to directly form a polycrystalline stone layer, such as continuous crystalline stone (C ο n t i n u o u s

Grain Silicon; CGS),連續側邊固化(sequential Lateral Solidification; SLS),金屬誘發結晶(Meta 1 Induced Crystallization; MIC),金屬誘發側邊結晶 T( Metal Induced Lateral Crystallization; MILC), 或是固相結晶化(Solid Phase Crystallization; SPC )。之後,在該複晶矽層表面上以電漿處理複晶矽層以形 成一閘極絕緣層。然後,在上述之閘極絕緣層上形成一閘 修層。在複晶矽層内形成輕摻雜汲極區域在閘極層兩側, 並且在閘極層側壁上形成間隙壁。接著,在上述之複晶石夕 層内形成一源極與一 ί及極區域在前述閘極層兩側。 其中電漿處理步驟係在溫度3 0 0 - 6 0 0°C之間,而上述成為Grain Silicon; CGS), Sequential Lateral Solidification (SLS), Metal Induced Crystallization (MIC), Metal Induced Lateral Crystallization (MILC), or Solid Phase Crystallization Solid Phase Crystallization (SPC). Thereafter, the polysilicon layer is treated by plasma on the surface of the polysilicon layer to form a gate insulating layer. Then, a gate layer is formed on the above-mentioned gate insulating layer. A lightly doped drain region is formed on both sides of the gate layer in the polysilicon layer, and a spacer is formed on the sidewall of the gate layer. Next, a source and a NMOS region are formed on both sides of the gate layer in the above-mentioned single crystal layer. Wherein the plasma treatment step is between 30 and 60 ° C, and the above

第10頁 1267987 五、發明說明(6) 電漿之反應氣體可包含氧氣或是氮氣,例如02,N2, H20,NH3,N20。當反應氣體主要為氧氣時,例如02,N20 或是Η 2 0,上述之閘極絕緣層為氧化矽。當反應氣體主要 為氮氣時,例如Ν20,Ν2或是ΝΗ3,上述之閘極絕緣層為氮 化矽。當反應氣體包含氧氣與氮氣時,例如0 2,Ν 2, Ή 2 0,Ν 2 0,與Ν Η 3,上述之閘極絕緣層可為氮氧化矽。 本發明同時提供一種在薄膜電晶體液晶顯示器中形成高崩 潰電壓閘極絕緣層之方法,其步驟包含在一透明基板上形 g —複晶矽層。之後,在3 0 0 - 6 0 0°C之間以電漿處理上述 之複晶矽層以形成一閘極絕緣層,其中形成電漿之反應氣 體可包含氧氣或是氮氣或是兩者都包含,例如氧化氫,氧 氣,或是氧化氮。上述閘極絕緣層可為氧化矽,氮化矽, 氮氣,或是氮氧化矽。 在上述電漿處理步驟中較佳的溫度在4 5 0 - 5 5 0°C之間。上 述之透明基板在電漿處理步驟中會旋轉。在電漿處理步驟 之前可引入惰性氣體清潔並去除複晶矽層表面之倶生氧化 層。 本發明之一較佳實施方式,將會參照第二圖所顯示之各步 驟之結構示意圖作一詳細說明。 如第二A圖所示,在一透明基板2 0 0上形成一緩衝層2 0 2。Page 10 1267987 V. INSTRUCTIONS (6) The reactive gas of the plasma may contain oxygen or nitrogen, such as 02, N2, H20, NH3, N20. When the reaction gas is mainly oxygen, such as 02, N20 or Η20, the above-mentioned gate insulating layer is yttrium oxide. When the reaction gas is mainly nitrogen, such as ruthenium 20, ruthenium 2 or ruthenium 3, the above-mentioned gate insulating layer is ruthenium nitride. When the reaction gas contains oxygen and nitrogen, such as 0 2, Ν 2, Ή 2 0, Ν 2 0, and Ν Η 3, the above-mentioned gate insulating layer may be yttrium oxynitride. The present invention also provides a method of forming a high breakdown voltage gate insulating layer in a thin film transistor liquid crystal display, the method comprising forming a g-polysilicon layer on a transparent substrate. Thereafter, the above-mentioned polysilicon layer is plasma-treated between 300 and 600 ° C to form a gate insulating layer, wherein the reaction gas forming the plasma may contain oxygen or nitrogen or both Contains, for example, hydrogen peroxide, oxygen, or nitrogen oxides. The gate insulating layer may be tantalum oxide, tantalum nitride, nitrogen, or hafnium oxynitride. The preferred temperature in the above plasma treatment step is between 4 50 - 5 50 ° C. The transparent substrate described above rotates during the plasma processing step. An inert gas may be introduced to clean and remove the twin oxide layer on the surface of the polysilicon layer prior to the plasma treatment step. A preferred embodiment of the present invention will be described in detail with reference to the structural diagrams of the steps shown in the second figure. As shown in FIG. 2A, a buffer layer 220 is formed on a transparent substrate 200.

第11頁 1267987 五、發明說明(7) 透明基板2 0 0的材質可以使用玻璃基板,壓克力,或是透 明塑膠等高分子聚合物。緩衝層2 0 2可以使用氧化矽或是 氮化矽。緩衝層2 0 2的材質選擇,會使用與矽晶格的晶格 常數相匹配的材料為主,並且需要考慮光線的通透性’製 程的簡易與良率等。一般而言,氧化石夕是很好的一個材 質,因為現有氧化矽的沉積,例如電漿增益化學氣相沉積 法或是低壓化學氣相沉積法,都是是很成熟的製程。再 者,緩衝層2 0 2還可以防止透明基板2 0 0的金屬離子跑進非 晶矽層中,造成元件漏電流的產生。在一實施例中,緩衝 g 2 0 2的厚度約為1 0 0 0 - 4 0 0 0埃。 本實施例對於形成複晶矽的方式是以先形成非晶矽然後經 由退火的方式形成複晶矽作為說明。然而,亦可以直接形 成複晶矽層,其形成的方式有連續結晶矽,連續側邊固 化,金屬誘發結晶,金屬誘發側邊結晶,或是固相結晶 ,化。 接著,形成一非晶矽層2 0 4在緩衝層上。非晶矽層2 0 4的形 成方式可以使用目前成熟的電漿增益化學氣相沉積法或是 _壓化學氣相沉積法。一方式是使用氫氣去分解作為矽的 前驅物的矽甲烷,或是矽乙烷。以電漿增益化學氣相沉積 法為例,製程的溫度約為2 0 0 - 6 0 0 °C ,反應室的壓力約為 0.1-2000 mtorr,氫氣的流量約為20-1000 SCCM而石夕曱炫 的流量約為5 0 - 1 0 0 0 SCCM。沉積的非晶矽層1 0 4的厚度約Page 11 1267987 V. INSTRUCTIONS (7) The material of the transparent substrate 200 can be a high molecular polymer such as a glass substrate, acrylic, or transparent plastic. As the buffer layer 220, ruthenium oxide or tantalum nitride can be used. The material selection of the buffer layer 2 0 2 is mainly based on the material matching the lattice constant of the germanium lattice, and the transparency of the light needs to be considered, and the process is simple and good. In general, oxidized stone is a good material because the deposition of existing cerium oxide, such as plasma gain chemical vapor deposition or low pressure chemical vapor deposition, is a very mature process. Further, the buffer layer 202 can also prevent metal ions of the transparent substrate 200 from running into the amorphous layer, causing leakage current of the element. In one embodiment, the buffer g 2 0 2 has a thickness of about 1 0 0 0 - 4 0 0 angstroms. The manner in which the present embodiment is formed for forming a germanium is described by forming an amorphous germanium first and then forming a germanium by annealing. However, it is also possible to form a polycrystalline germanium layer directly in the form of continuous crystalline germanium, continuous side solidification, metal induced crystallization, metal induced side crystallization, or solid phase crystallization. Next, an amorphous germanium layer 220 is formed on the buffer layer. The amorphous germanium layer 204 can be formed by using the currently mature plasma gain chemical vapor deposition method or the _ pressure chemical vapor deposition method. One way is to use hydrogen to decompose methane as a precursor to helium, or helium. Taking the plasma gain chemical vapor deposition method as an example, the process temperature is about 200-600 ° C, the pressure in the reaction chamber is about 0.1-2000 mtorr, and the flow rate of hydrogen is about 20-1000 SCCM. The traffic of 曱炫 is about 50 - 1 0 0 0 SCCM. The thickness of the deposited amorphous germanium layer 104 is about

第12頁 1267987__ 五、發明說明(8) 為 5 0 - 5 0 0埃。 ^ 如第二B圖所示,將非晶矽層1 0 4退火形成複晶矽層1 0 6。 複晶矽層1 0 6的半導體特性較非晶矽好,因此需要將非晶 矽轉換成複晶矽。最簡單的轉換方式是直接升溫退火的方 式,但是必須考慮到透明基板2 0 0所能承受的溫度。在本 發明中,較佳退火的方式可以為準分子雷射退火方式。 接著,如第二C圖所示,以電漿2 2 0處理複晶矽層2 0 6的表 «在3 0 0 - 6 0 0°C之間以形成閘極絕緣層2 0 8。電漿2 2 0的選 主要由閘極絕緣層2 0 8的材料所決定。這裏使用的電漿 2 2 0可以使用包含氧的電漿,以形成氧化矽的閘極絕緣層 2 0 8,亦可以使用含氮的電漿以形成氮化矽的閘極絕緣層 2 0 8。再者,亦可以同時使用含有氧與氮的電漿以形成氮 氧化矽的閘極絕緣層2 0 8。 如果閘極絕緣層2 0 8為氧化矽,則電漿2 2 0的輸入氣體可以 為02, H20,或是N20,輸入氣體的流量約為2 0 - 5 0 0 0 SCCM, 反應室壓力約為1 - 1 0 0 0 m t 〇 r r,較佳的溫度約為4 5 0 - 5 5 0 _。以上述的條件,形成的氧化矽的厚度約為1 0 0 - 1 0 0 0 埃。如果閘極絕緣層為氮化矽,則電漿2 2 0的輸入氣體可 以為N2, N3H,N20,輸入氣體的流量約為2 0 - 5 0 0 0 SCCM,反 應室壓力約為1 - 1 0 0 0 m t 〇 r r,較佳的溫度約為4 5 0 - 5 5 0 °C 。以上述的條件,形成的氮化矽的厚度約為1 〇 〇 - 1 〇 〇 〇Page 12 1267987__ V. The invention description (8) is 5 0 - 500 angstroms. ^ As shown in the second B-graph, the amorphous germanium layer 104 is annealed to form a polycrystalline germanium layer 106. The semiconductor characteristics of the polycrystalline germanium layer 106 are better than those of the amorphous germanium, so it is necessary to convert the amorphous germanium into a germanium germanium. The simplest way to convert is to directly heat up the anneal, but the temperature at which the transparent substrate 2000 can withstand must be considered. In the present invention, the preferred annealing method may be an excimer laser annealing method. Next, as shown in the second C diagram, the table of the polysilicon layer 206 is treated with the plasma 2 2 0 «between 300-600 ° C to form the gate insulating layer 208. The selection of the plasma 2 2 0 is mainly determined by the material of the gate insulating layer 208. The plasma 2 2 0 used herein may use a plasma containing oxygen to form a gate insulating layer of ruthenium oxide 2 0 8. A plasma containing nitrogen may also be used to form a gate insulating layer of tantalum nitride. . Further, it is also possible to simultaneously use a plasma containing oxygen and nitrogen to form a gate insulating layer 208 of ruthenium oxynitride. If the gate insulating layer 20 8 is yttrium oxide, the input gas of the plasma 2 2 0 may be 02, H20, or N20, and the flow rate of the input gas is about 2 0 - 5 0 0 0 SCCM, and the reaction chamber pressure is about For 1 - 1 0 0 0 mt rr, the preferred temperature is about 4 50 - 5 5 0 _. Under the above conditions, the thickness of the yttrium oxide formed is about 1 0 0 - 1 0 0 angstrom. If the gate insulating layer is tantalum nitride, the input gas of the plasma 220 may be N2, N3H, N20, the flow rate of the input gas is about 2 0 - 5 0 0 SCCM, and the reaction chamber pressure is about 1-1. 0 0 0 mt 〇rr, the preferred temperature is about 4 5 0 - 5 5 0 °C. Under the above conditions, the thickness of the tantalum nitride formed is about 1 〇 〇 - 1 〇 〇 〇

第13頁 1267987__ 五、發明說明(9) 埃。如果閘極絕緣層為氮氧化石夕,則電漿2 2 0的輸入氣體 可以為02, H20, N20, N3H,NO,輸入氣體的流量約為2 0 - 5 0 0 0 SCCM,反應室壓力約為1 - 1 0 0 0 mtorr,較佳的溫度約為 4 5 0 - 5 5 0°C。以上述的條件,形成的氮氧化矽的厚度約為 1 0 0 - 1 0 0 0埃。 之後,如第二D圖所示,在閘極絕緣層2 0 8上形成閘極層 ’2 1 0。形成的方式包含了幾個步驟:沉積金屬層在閘極絕 緣層2 0 8上,形成光阻層在金屬層上,以光學微影的方式 «閘極的圖案轉移到光阻層上,以光阻層為遮罩蝕刻金屬 _ ,以及移除光阻層。在上述的製程中,金屬的材質可為 銘,鉻,鎮,編,或是上述其中的合金。金屬層的沉積方 式可為化學氣相沉積或是物理氣相沉積。光阻層可以使用 正光阻或是負光阻,其材料的使用係取決於曝光的光線頻 率。钱刻的方式可以是等向性餘刻或是非等向性I虫刻。 如第二E圖所示,接下來的步驟可以是選擇性的。因為有 輕扭雜〉及極區212的電晶體有較佳的元件特性。以離子植 入機或是離子雲的方式將摻雜子植入到複晶矽層2 0 6中。 ⑩裏摻雜的粒子主要是以可以提供電子作為導電載子的元 素,一般會是五價的元素,例如磷,或是砷。輕摻雜的意 思是指摻雜的濃度較源極及極低,大約較低每平方公分 1 0 3個。Page 13 1267987__ V. Description of invention (9) Egypt. If the gate insulating layer is arsenic oxide, the input gas of the plasma 2 2 0 may be 02, H20, N20, N3H, NO, and the flow rate of the input gas is about 2 0 - 5 0 0 0 SCCM, the reaction chamber pressure It is about 1 - 1 0 0 mtorr, and the preferred temperature is about 4 50 - 5 50 °C. Under the above conditions, the thickness of yttrium oxynitride formed is about 1 0 0 - 1 0 0 angstrom. Thereafter, as shown in the second D diagram, a gate layer '2 1 0 is formed on the gate insulating layer 208. The formation method comprises several steps: depositing a metal layer on the gate insulating layer 202, forming a photoresist layer on the metal layer, and transferring the pattern of the gate to the photoresist layer by optical lithography to The photoresist layer is a mask etch metal _ and the photoresist layer is removed. In the above process, the material of the metal may be Ming, chrome, town, braid, or the alloy described above. The metal layer can be deposited by chemical vapor deposition or physical vapor deposition. The photoresist layer can use either positive or negative photoresist, and the material used depends on the frequency of the light being exposed. The way of engraving money can be an isotropic remnant or an anisotropic I insect. As shown in the second E diagram, the next steps may be optional. Because of the lightly twisted and polar regions 212, the transistors have better component characteristics. The dopants are implanted into the polycrystalline germanium layer 206 by means of an ion implanter or an ion cloud. The 10 doped particles are mainly elements which can provide electrons as a conductive carrier, and are generally pentavalent elements such as phosphorus or arsenic. The meaning of light doping means that the doping concentration is lower than the source and is extremely low, about 1 3 3 per square centimeter.

第14頁 1267987 五、發明說明(10) 如第二F圖所示’之德从* ^ θθ 瓦的步驟是在閘極金屬層2 1 0的側壁形 成間隙壁214。形成的方人 , conformal)介電層 人〜万式包含,先沉積一層共形的 然後以非等向性蝕刻的方式進行 名虫刻。這個步驟有幾_復 α " 戍们k點,在之後的離子植入以形成源 S /及極區中遮j住輕摻雜汲極區2 1 2,以及提供閘極與源 極/没極區之間的較佳的電性隔離。 如第一 G圖所不’以離子植入機或是以離子雲的方式將摻 雜子植入到複晶石夕層2 〇 6中形成源極與汲極區域2 1 6。這裏 f雜的粒子與之前輕摻雜汲極區2丨2植入的摻雜子可以相 或是不相同。摻雜的濃度較輕摻雜汲極區2 1 2高。 第三圖顯示電漿處理步驟的反應室的結構示意圖。導管 3 0 2將反應氣體3 0 4與載流氣體引入到反應室3 〇 〇中,基板 2 0 0放置在托架平台(table) 3 2 0上。在反應室3 0 0中提供 谢頻電源3 0 6,讓反應氣體3 0 4形成電漿。反應室3 0 0靠近 托架平台3 2 0有一加熱器3 0 8,將基板2 0 0加熱至適當的溫 度,反應氣體即可以在基板2 0 0上與複晶矽反應成為閘極 絕緣層。托架平台2 0 0可以旋轉,使得在複晶矽的表面可 籲均勻的與反應氣體反應,使得成長的閘極絕緣層的厚度 均勻。另外,一閥門3 1 0將反應室3 0 0内的氣體抽出。 在這個步驟中,先是在開始的時候先將惰性氣體,例如氬 氣,導入到反應室3 0 0中,進行清潔的動作,並且可以去Page 14 1267987 V. INSTRUCTION DESCRIPTION (10) As shown in the second F diagram, the step from the *^ θθ watt is to form the spacer 214 on the sidewall of the gate metal layer 2 10 . The formed person, conformal) dielectric layer, the human-type 10,000-type inclusion, first deposits a layer of conformal and then anisotropic etching. This step has a few _ complex α " we k points, after the ion implantation to form the source S / and the polar region to cover the lightly doped bungee region 2 1 2, and provide the gate and source / Better electrical isolation between the immersion zones. The source and drain regions 2 1 6 are formed by implanting dopants into the polycrystalline layer 2 〇 6 as an ion implanter or as an ion cloud, as in the first G diagram. Here, the doped particles may or may not be the same as the dopants implanted in the previously lightly doped bungee region 2丨2. The doping concentration is higher than the lightly doped bungee region 2 1 2 . The third figure shows a schematic structural view of the reaction chamber of the plasma treatment step. The conduit 3 0 2 introduces the reaction gas 340 and the carrier gas into the reaction chamber 3 〇 , and the substrate 200 is placed on the tray table 320 . A frequency power supply 3 0 6 is provided in the reaction chamber 300 to allow the reaction gas 3 0 4 to form a plasma. The reaction chamber 300 is close to the carrier platform 3 2 0 and has a heater 3 0 8 to heat the substrate 200 to a suitable temperature, and the reaction gas can react with the polysilicon on the substrate 200 to become a gate insulating layer. . The carriage platform 200 can be rotated so that the surface of the polysilicon can be uniformly reacted with the reaction gas, so that the thickness of the grown gate insulating layer is uniform. In addition, a valve 310 charges the gas in the reaction chamber 300. In this step, the inert gas, such as argon, is first introduced into the reaction chamber 300 at the beginning to perform the cleaning action, and can go

第15頁 1267987____ 五、發明說明(11) 除在複晶石夕表面的倶生氧化(na t i ve ox i de)層。氣體輸 入的流量約為1 0 0 0 -8 0 0 0 SC CM,持續時間約為1 Ο-6 0秒。 然後關閉惰性氣體,輸入反應氣體,並且調整射頻的功 率,以調整所產生的電漿濃度。對反應室3 0 0加熱至適當 的溫度。將反應平台進行旋轉,旋轉的頻率約為每分鐘 1-10 0#。反應室的壓力約為1 - 1 0 0 0 m t 〇 r r。 由電漿處理的方式所形成的閘極絕緣層,不論是矽的氧化 物,氮化物或是氮氧化物,都是由複晶石夕層與電漿反應所 &生的。以這種方式形成的閘極絕緣層相較於先前的化學 冒相沉積法有較佳的品質,材質的緻密性高,因此可以有 較高的崩潰電壓。另外,由複晶石夕層與電梁反應所產生的 閘極絕緣層與複晶矽之間的缺陷相較於先前的化學氣相沉 積法較少,因此可以降低漏電流。 對熟悉此領域技藝者,本發明雖以一較佳實例闡明如上, 然其並非用以限定本發明精神。在不脫離本發明之精神與 範圍内所作之修改與類似的安排,均應包含在下述之申請 專利範圍内,這樣的範圍應該與覆蓋在所有修改與類似結 _的最寬廣的詮釋一致。因此,闡明如上的本發明一較佳 實例,可用來鑑別不脫離本發明之精神與範圍内所作之各 種改變。Page 15 1267987____ V. INSTRUCTIONS (11) In addition to the layer of neo-oxidation (na t i ve ox i de) on the surface of the ceramsite. The gas input flow is approximately 1 0 0 -8 0 0 0 SC CM and lasts approximately 1 Ο -6 seconds. The inert gas is then turned off, the reaction gas is input, and the power of the radio frequency is adjusted to adjust the plasma concentration produced. The reaction chamber 300 was heated to an appropriate temperature. The reaction platform is rotated at a frequency of approximately 1-10 0# per minute. The pressure in the reaction chamber is approximately 1 - 1 0 0 m t 〇 r r. The gate insulating layer formed by the plasma treatment method, whether it is a cerium oxide, a nitride or an oxynitride, is produced by a combination of a smectite layer and a plasma. The gate insulating layer formed in this manner has better quality than the prior chemical vapor deposition method, and the material has high compactness, so that a high breakdown voltage can be obtained. In addition, the defect between the gate insulating layer and the polycrystalline silicon produced by the reaction of the double crystal layer and the electric beam is less than that of the previous chemical vapor deposition method, so that the leakage current can be reduced. The present invention has been described above by way of a preferred example, and is not intended to limit the scope of the invention. Modifications and similar arrangements made within the spirit and scope of the invention are intended to be included within the scope of the appended claims. Therefore, a preferred embodiment of the invention as set forth above may be used to identify various modifications within the spirit and scope of the invention.

IIIIII

第16頁 1267987___ 圖式簡單說明 【圖式簡單說明】 * 第一圖顯示一種以傳統的方式形成頂部閘極的薄膜電晶體 在各步驟的結構不意圖, 第二圖顯示一種以本發明的方法形成頂部閘極的薄膜電晶 體在各步驟的結構示意圖;以及 第三圖顯示以電漿處理形成閘極絕緣層的設備之結構示意 圖。 ,主要元件符號說明】 100 玻璃基板 1 02 \ 202 緩衝層 104、 204 非晶矽層 106> 206 複晶矽層 108 閘極氧化層 1 1 0〜 210 閘極金屬層 112、 212 輕摻雜汲極 區 114、 214 間隙壁 籲1 6、 216 源極與汲極 區 200 透明基板 208 閘極絕緣層 220 電漿 300 反應 室Page 16 1267987___ Schematic description of the drawing [Simple description of the drawing] * The first figure shows the structure of a thin film transistor forming a top gate in a conventional manner, and the second figure shows a method according to the present invention. A schematic view of the structure of the thin film transistor forming the top gate at each step; and the third diagram showing the structure of the device for forming the gate insulating layer by plasma treatment. , the main component symbol description] 100 glass substrate 1 02 \ 202 buffer layer 104, 204 amorphous germanium layer 106 > 206 polysilicon layer 108 gate oxide layer 1 1 0 ~ 210 gate metal layer 112, 212 lightly doped Polar region 114, 214 gap wall 16 6 216 source and drain region 200 transparent substrate 208 gate insulating layer 220 plasma 300 reaction chamber

第17頁 1267987 圖式簡單說明 3 0 2 導管 3 0 4 反應氣體 3 0 6 射頻電源 3 0 8 加熱器 3 10 閥門 3 2 0 托架平台Page 17 1267987 Schematic description 3 0 2 Conduit 3 0 4 Reactive gas 3 0 6 RF power supply 3 0 8 Heater 3 10 Valve 3 2 0 Bracket platform

第18頁Page 18

Claims (1)

1267987__ 六、申請專利範圍 1. 一種在液晶顯示器中形成一薄膜電晶體的方法 '包 含: 依序沉積一緩衝層與一複晶矽層在一透明基板上; 以電漿處理該複晶矽層以形成一閘極絕緣層; 形成一閘極層在該閘極絕緣層上;以及 在該複晶矽層内形成一源極與一汲極區域在該閘極層兩 侧0 2. 如申請專利範圍第1項之形成薄膜電晶體的方法,其中 j述之電漿處理步驟係在溫度3 0 0 - 6 0 0°C之間。 3. 如申請專利範圍第2項之形成薄膜電晶體的方法,其中 上述之電聚包含氧。 4. 如申請專利範圍第3項之形成薄膜電晶體的方法,其中 土述之電漿包含氮。 5.如申請專利範圍第3項之形成薄膜電晶體的方法,其中 上述之閘極絕緣層為氧化矽。 6.如申請專利範圍弟4項之形成薄膜電晶體的方法’其中 上述之閘極絕緣層為氧化矽。 7.如申請專利範圍第2項之形成薄膜電晶體的方法,其中 1267987___ 六、申請專利範圍 上述之電漿包含氮。 8V/如申請專利範圍第7項之形成薄膜電晶體的方法,其中 上述之閘極絕緣層為氮化矽。 .如申請專利範圍第4項之形成薄膜電晶體的方法,其中 上述之閘極絕緣層包含氧化矽與氮化矽。 1 0.如申請專利範圍第1項之形成薄膜電晶體的方法,其 g上述之緩衝層為氧化石夕或氮化碎。 1 1 .如申請專利範圍第1項之形成薄膜電晶體的方法,其 中上述形成該複晶矽層之方法包含: 沉積一非晶矽層在該緩衝層上;以及 對該非晶矽層以準分子雷射退火方式轉換成該複晶矽層。 1 2.如申請專利範圍第1項之形成薄膜電晶體的方法,其 中上述形成該複晶矽層之方法為連續結晶矽,連續側邊固 化,金屬誘發結晶,金屬誘發側邊結晶,或是固相結晶化 φ中之一。 1 3.如申請專利範圍第1項之形成薄膜電晶體的方法,在 該形成源極汲極區域步驟之前更包含: 在該複晶矽層内形成輕摻雜汲極區域在該閘極層兩側;以 1267987 六、申請專利範圍 及 在該閘極層側壁上形成間隙壁。 1 4.如申請專利範圍第1項之形成薄膜電晶體的方法,其 中上述之透明基板為玻璃基板。 1 5. —種在薄膜電晶體液晶顯示器中形成高崩潰電壓閘極 絕緣層之方法,包含: 提供一透明基板; ▲該 管3( 基板上形成一複晶石夕層; 0 0 - 6 0 0°C之間以電漿處理該複晶矽層以形成一閘極絕 緣層,其中上述之電漿為包含氧或是包含氮,而該閘極絕 緣層為氧化矽,氮化矽,或是氮氧化矽。 1 6.如申請專利範圍第1 5項之形成高崩潰電壓閘極絕緣層 之方法,其中上述以電漿處理之步驟的溫度係在4 5 0 - 5 5 0 °C之間。 1 7.如申請專利範圍第1 6項之形成高崩潰電壓閘極絕緣層 •方法,其中上述之電漿包含氧與氮。 1 8.如申請專利範圍第1 7項之形成高崩潰電壓閘極絕緣層 之方法,其中上述之透明基板在該電漿處理步驟中旋轉。 1267987 六、申請專利範圍 1 9.如申請專利範圍第1 8項之形成高崩潰電壓閘極絕緣層 之方法,其中上述以電漿處理之步驟所引入的氣體為氧化 氫,氧氣,氮氣,或是氧化氮。 層 緣 絕 極 閘 壓 電 〇 潰矽 崩化 高氧 成為 形層 之緣 項絕 9 1極 第閘 圍之 範述 利上 專中 請其 中, 如法 •方 ο 2 之 層並 緣潔 絕清 極體 閘氣 壓 ιέί! 電隋 潰入 山朋弓 高含。 成包層 形更化 之前氧 g之生 15驟倶 第步之 圍理面 範處表 利漿層 專電梦 請在晶 申,複 如法該 •方除 TX 2之1267987__ VI. Patent Application Range 1. A method for forming a thin film transistor in a liquid crystal display' includes: sequentially depositing a buffer layer and a polysilicon layer on a transparent substrate; treating the polysilicon layer by plasma Forming a gate insulating layer; forming a gate layer on the gate insulating layer; and forming a source and a drain region in the polysilicon layer on both sides of the gate layer. The method for forming a thin film transistor according to the first aspect of the patent, wherein the plasma processing step is a temperature between 300 and 60 °C. 3. The method of forming a thin film transistor according to claim 2, wherein the electropolymerization comprises oxygen. 4. The method of forming a thin film transistor according to claim 3, wherein the slurry of the earth contains nitrogen. 5. The method of forming a thin film transistor according to claim 3, wherein the gate insulating layer is yttrium oxide. 6. The method of forming a thin film transistor according to the fourth aspect of the patent application, wherein the gate insulating layer is yttrium oxide. 7. The method of forming a thin film transistor according to the second aspect of the patent application, wherein: 1267987___, the patent scope of the invention comprises nitrogen. 8V/ A method of forming a thin film transistor according to claim 7, wherein the gate insulating layer is tantalum nitride. The method of forming a thin film transistor according to claim 4, wherein the gate insulating layer comprises ruthenium oxide and tantalum nitride. 10. The method of forming a thin film transistor according to claim 1, wherein the buffer layer is oxidized or oxidized. 1 1. The method of forming a thin film transistor according to claim 1, wherein the method for forming the polysilicon layer comprises: depositing an amorphous germanium layer on the buffer layer; and quantifying the amorphous germanium layer The molecular laser annealing method is converted into the polycrystalline germanium layer. 1 2. The method for forming a thin film transistor according to claim 1, wherein the method for forming the polycrystalline germanium layer is continuous crystallization, continuous side solidification, metal induced crystallization, metal induced side crystallization, or One of solid phase crystallization φ. 1 . The method of forming a thin film transistor according to claim 1 , before the step of forming the source drain region further comprises: forming a lightly doped drain region in the gate layer in the polysilicon layer Both sides; to 1267987, the patent application scope and the formation of a spacer on the sidewall of the gate layer. A method of forming a thin film transistor according to the first aspect of the invention, wherein the transparent substrate is a glass substrate. 1 5. A method for forming a high breakdown voltage gate insulating layer in a thin film transistor liquid crystal display, comprising: providing a transparent substrate; ▲ the tube 3 (forming a polycrystalline layer on the substrate; 0 0 - 60) The polysilicon layer is treated by plasma treatment between 0 ° C to form a gate insulating layer, wherein the plasma comprises oxygen or contains nitrogen, and the gate insulating layer is tantalum oxide, tantalum nitride, or Is a bismuth oxynitride. 1 6. A method of forming a high breakdown voltage gate insulating layer according to claim 15 of the patent application, wherein the temperature of the step of treating the plasma is at 455 - 550 °C 1. The method of forming a high-crash voltage gate insulating layer according to claim 16 of the patent application, wherein the above-mentioned plasma contains oxygen and nitrogen. 1 8. The high breakdown occurs in the case of claim 17 A method of voltage gate insulating layer, wherein the transparent substrate is rotated in the plasma processing step. 1267987 6. Patent application scope 1. 9. Method for forming high breakdown voltage gate insulating layer according to claim 18 Where the above is introduced by the step of plasma treatment The gas is hydrogen oxide, oxygen, nitrogen, or nitrogen oxide. The layered pole-extinguishing gate is broken, the high-oxygen is formed into the edge of the layer, and the 9th pole is the first step. , such as the law • Fang ο 2 layer and the edge of the cleansing of the body brake pressure ιέί! Electric 隋 入 山 山 朋 弓 弓 弓 高 高 成 成 成 成 成 成 成 成 成 成 成 成 成 成 成 成 成 成 成 成 成 氧 氧 氧 氧 氧 氧 氧At the table, the plasma layer of the special electric dream, please be in the crystal Shen, the same as the method of the party except the TX 2
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