TWI246194B - Self-aligned schottky-barrier clamped trench DMOS transistor structure and its manufacturing methods - Google Patents
Self-aligned schottky-barrier clamped trench DMOS transistor structure and its manufacturing methods Download PDFInfo
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1246194 五、發明說明(1) 【發明所屬之技術領域】 本發明與一種凹槽式(trench)雙擴散金氧半(DM〇s) 功率電晶體及其製造方法有關’特別是與一種自動對準蕭 特基能障(Schottky —barr ier)极位 (clamped)凹槽式 雙擴散金氧半電晶體結構及其製造方法有關。 【先前技術】1246194 V. Description of the invention (1) [Technical field to which the invention belongs] The present invention relates to a trench-type double-diffusion metal-oxide-semiconductor (DM0s) power transistor and a manufacturing method thereof, particularly to an automatic alignment A quasi-Schottky barrier (clamped) grooved double-diffusion metal-oxide semiconductor structure and its manufacturing method are related. [Prior art]
一個雙擴散(double-diffused)金氧半功率電晶體呈 有一個很低的導通電阻已成為應用於電池保護、切換、^ 性調壓器、放大器、及功率管理的一種重要半導體元件。A double-diffused metal-oxide half-power transistor with a very low on-resistance has become an important semiconductor element for battery protection, switching, voltage regulators, amplifiers, and power management.
圖一 A顯示先前技術之一種平面式雙擴散金氧半電晶 體的一種非自動對準源結構之一個簡要剖面圖,其中一: P-基擴散區1 04a係利用一個第一罩幕光阻步驟且透過一個 成形複晶矽閘層103a置於一個閘氧化物層1〇2a之上所包圍 的一個成形(patterned)窗口形成於一個高摻雜N+矽基 板1 0 0之上的一個淡摻雜N -磊晶矽層1 〇 1之内;一個高摻雜 P擴政區1 0 5 a藉由一個高能量離子佈植透過該成形窗口來 形成於,p -基擴散區1 〇 4 a之内;一個高摻雜n +源擴散環 1 0 6 a係藉由一個第二罩幕光阻步驟(未圖示)且透過位於 一個成形光阻層(未圖示)形成於該成形窗口的一個中間 部份之内及該成形複晶矽閘層丨〇 3a置於該閘氧化物層1 〇 2a 之上的一個非自動對準離子佈植窗口來形成於該p-基擴散FIG. 1A shows a schematic cross-sectional view of a non-auto-aligned source structure of a planar double-diffused metal-oxide semiconductor transistor of the prior art. One of them: the P-based diffusion region 104a uses a first mask photoresist Step and forming a lightly doped layer over a highly doped N + silicon substrate 100 through a patterned polysilicon gate layer 103a over a gate oxide layer 102a and a patterned window Within the hetero-N epitaxial silicon layer 1 〇1; a highly doped P diffusion region 1 0 5 a is formed by implanting a high energy ion through the forming window, the p-based diffusion region 1 〇 4 a Within; a highly doped n + source diffusion ring 1 0 6 a is formed in the forming window through a second mask photoresist step (not shown) and through a forming photoresist layer (not shown) A non-auto-aligned ion implantation window within the middle portion of the formed polycrystalline silicon gate layer and the gate oxide layer over the gate oxide layer 〇2a to form the p-based diffusion
1246194 五、發明說明(2) 區1 0 4a的一個表面部份且置於該高摻雜p 個側邊表面部份之上;一個非自動對準源 一個第三罩幕光阻步驟(未圖示)形成於 物層1 0 7 a所包圍的一個#刻洞;及一個源 係形成於該成形氧化物層 1 0 7 a之上且置 源擴散環1 0 6 a所包圍的該高摻雜p +擴散區 η +源擴散環1 0 6 a的一個側邊表面部份之上 平面式雙擴散金氧半功率電晶體的該非自 圖一 A所示係需要兩個嚴謹罩幕光阻步驟 幕光阻步驟)來製造。然而,該兩個嚴謹 產生的誤對準 (misalignments) 會產生 佈,進而造成嚴重的元件可靠性問題。 雙擴散金氧半功率電晶體的源區面積很難 外,若連接的電晶體細胞元相當多時,該 1 0 3 a作為一個閘連線導電層將具有一個較 電阻來降低切換速度。該平面式雙擴散金 的一個典型例子可以參見S. M u k h e r j e e e1 號碼5,2 6 8,5 8 6所揭示。 圖一 B顯示圖一 A所示之該平面式雙擴 晶體的一個等效元件代表符號,其中一個 (D1)係透過源及汲電極之間的該p-基擴 摻雜 N—磊晶矽層101之間的P-η接面來形天 極體(D1)在某些電路應用中會導通,而 體(D1)在順向偏壓之下的少數載子儲存 擴散區1 0 5 a的一 接觸窗口係透過 由一個成形氧化 接觸金屬層1 08a 於由該高摻雜η + 1 0 5 a及該高摻雜 ^ 。很明顯地,該 , 動對準源結構如 (第二及第三罩 罩幕光阻步驟所 不均勻的電流分〇 因此,該平面式 加予微縮化。另 成形複晶矽閘層 大的閘連線雜散 氧半功率電晶體 ^ :a 1.之美國專利 散金氧半功率電 ρ - η接面二極體 散區1 04a及該淡 I。該ρ-η接面二 該 ρ - η接面二極 會降低該平面式 1246194 五、發明說明(3) . 雙擴散金氧半功率電晶體的切換速度。因此,一個蕭特基 能障二極體被提出來置於該源及汲電極之間。 文獻中有不少的複雜方法曾被提出來同時將一個平面 式雙擴散金氧半電晶體及一個蕭特基二極體整合在一個電 晶體細胞元内。一個典型的例子可以參見 J . T i h a n j i所揭 示的美國專利號碼 6,6 8 6,6 1 4,如圖二A及圖二B所示,其 ‘ 中圖二A顯示一個簡要剖面圖而圖二B顯示一個等效元件代 》 表圖。由圖二A可知,一個蕭特基能障二極體 (Ds) 係透 過形成於一個P-基擴散區5 0之一個中間部份的一個非自動 對準凹槽窗口來形成於一個淡摻雜N —磊晶矽層2 0之上。這 裡可以清楚地看到,圖二A並沒有蕭特基能障接觸金屬9 0 ^ 所需的擴散保護環來消除邊緣漏電及軟性(so f t)崩潰; 該P-基擴散區5 0係漂浮且沒有與一個高摻雜η +源擴散環 6 0短路;該非自動對準凹槽窗口會使鄰近平面式雙擴散金 氧半電晶體細胞元產生不均勻的電流分佈,該蕭特基能障 二極體具有一個低值能障會在順向阻隔(b 1 ock i ng)狀態 ^ 下呈現一個較大的漏電電流。 因此,本發明的一個主要目的係提供一種自動對準蕭 特基能障嵌位凹槽式雙擴散金氧半電晶體結構且無需嚴謹 罩幕光阻步驟來製造。 本發明的另一個目的係提供一種自動對準蕭特基能障 省· 嵌位凹槽式雙擴散金氧半電晶體結構具有一個凹槽式雙擴 散金氧半電晶體細胞元之一個中度摻雜P-基擴散環作為一 個蕭特基能障二極體的一個擴散保護環來消除邊緣漏電電1246194 V. Description of the invention (2) A surface portion of the region 1 0 4a is placed on the highly doped p side surface portions; a non-automatic alignment source and a third mask photoresist step (not shown) (Pictured) is formed in a #etched hole surrounded by the object layer 1 0 7 a; and a source system is formed on the shaped oxide layer 10 7 a and the height surrounded by the source diffusion ring 1 0 6 a The doped p + diffusion region η + source diffusion ring 1 0 6 a on one side surface portion of the planar double-diffusion metal-oxide half-power transistor, which is not shown in Figure 1A, requires two rigorous curtain lights. Resistance step curtain photoresist step) to manufacture. However, these two rigorous misalignments can cause layout, which in turn can cause serious component reliability issues. The source area of a double-diffused metal-oxide half-power transistor is difficult. If there are a large number of transistor cells connected, the 103a as a gate conductive layer will have a higher resistance to reduce the switching speed. A typical example of the planar double-diffusion gold can be found in S. M u k h e r j e e e1 No. 5, 2 6 8, 5 8 6. FIG. 1B shows a representative symbol of an equivalent element of the planar double-expanded crystal shown in FIG. 1A. One (D1) is a p-based diffusion-doped N-epitaxial silicon through the source and the drain electrode. The P-η junction between layers 101 to shape the celestial body (D1) will be conductive in some circuit applications, while the body (D1) has a minority carrier storage diffusion region under forward bias 1 0 5 a A contact window passes through a shaped oxide contact metal layer 108a from the highly doped η + 105a and the highly doped ^. Obviously, the structure of the active alignment source is not equal to the current distribution in the second and third mask photoresist steps. Therefore, the planar type is further miniaturized. In addition, the formed polycrystalline silicon gate layer is large. Gate-connected stray oxygen half-power transistor ^: a 1. US patent bulk gold-oxygen half-power transistor ρ-η junction diode scattering region 104a and the light I. The ρ-η junction interface is the ρ -η junction diode will reduce the planar type 1246194 V. Description of the invention (3). The switching speed of the double-diffused metal-oxide half-power transistor. Therefore, a Schottky barrier diode is proposed to be placed in the source There are many complicated methods in the literature that have been proposed to integrate a planar double-diffused metal-oxide semiconductor and a Schottky diode into a transistor cell. A typical For an example, see US Patent No. 6,6 8 6, 6 1 4 disclosed by J. Tihanji, as shown in Figures 2A and 2B, where Figure 2A shows a brief cross-sectional view and Figure 2B shows An equivalent element is shown in the table. From Figure 2A, we can see that a Schottky barrier diode (Ds ) Is formed on a lightly doped N-epitaxial silicon layer 20 through a non-automatically aligned groove window formed in a middle portion of a P-based diffusion region 50. It can be clearly seen here Therefore, Figure 2A does not have the Schottky barrier to contact the metal 9 0 ^ required diffusion protection ring to eliminate edge leakage and soft (so ft) collapse; the P-based diffusion region 50 is floating and does not have a high The doped η + source diffusion ring 60 is short-circuited; the non-automatically aligned groove window will cause an uneven current distribution in the adjacent planar double-diffused metal-oxide semi-electric crystal cell. The Schottky barrier diode has one A low value energy barrier exhibits a large leakage current under a forward blocking (b 1 ock i ng) state. Therefore, a main object of the present invention is to provide an automatic alignment of Schottky barrier energy recesses. Type double-diffused metal-oxide-semiconductor structure without the need for rigorous masking photoresist steps. Another object of the present invention is to provide an automatic alignment Schottky barrier. Crystal structure has a grooved double-diffused metal-oxide semiconductor A moderately doped P-based diffusion ring in the somatic cell acts as a diffusion protection ring for a Schottky barrier diode to eliminate edge leakage
第9頁 1246194 五、發明說明(4) 流及軟性崩潰。 本發明的一個進 能障嵌位凹槽 p-基擴散環與 高摻雜η +源擴 本發明的 障嵌位凹槽式雙擴 二極體可以藉由該 晶石夕層之間所形成 消除在順向阻隔狀 能障二極體的逆向 【發明内容】 式雙 該凹 擴散 槽式 散環短路 重要 散金 中度 的一 態操 漏電 個 步目的 金氧半 雙擴散 來消除 目的係 氧半電 摻雜Ρ- 個 ρ - η 作下具 流0 係提供 電晶體 金氧半 結構具 電晶體 本體(body) 提供一種自動 種自動對準蕭特基 有該中度摻雜 細胞元的一個 晶體結 -基擴散 接面空乏區來 有一個低值能 效應。 對準蕭特基能 構具有該蕭特基能障 環與一個淡摻雜ΙΓ磊 加予擠止,以 障之該蕭特基 散金 二極 半電 位凹 源區 區所 散環 層之 散環 本發明揭示一種 氧半電晶 體係以一 晶體 槽式 及一 包圍 形成 内、 細胞 雙擴 個凹 〇該 於該 一個 的一個側 動對準蕭特基能障嵌 體結構及其製造方法 種自動對準的方式與 元積體化。本發明之 散金氧半電晶體結構 槽閘區,其中該自動對準源區 自動對準源區至少包含一個中 凹槽閘區所包圍的一個淡摻雜 高摻雜η +源擴散環形成於該中 邊表面部份之内、一個自動對 ,其中一 一個凹槽 自動對準 至少包含 位凹槽 個蕭特 式雙擴 蕭特基 一個自 式雙擴 基能障 散金氧 能障嵌 動對準 凹槽閘 Ρ-基擴 半導體 係由該 度摻雜 Ν 蠢晶 度摻雜Ρ -基擴 準源接觸窗口Page 9 1246194 V. Description of the invention (4) Flow and soft collapse. The p-based diffusion ring of an energy-inserting barrier recess of the present invention and a highly doped η + source expansion The barrier-recessing recessed double-expanding diode of the present invention can be formed between the crystal layers. Eliminate the reverse of the forward barrier-shaped energy-barrier diode. [Content of the invention] Double concave recessed groove type short-circuit short circuit important loose gold mode one state of electricity leakage step by step metal oxygen half-diffusion to eliminate the target oxygen The semi-electrically doped P- ρ-η is provided with a current of 0. The transistor is provided with a metal-oxygen semi-structured transistor body. An automatic seed is provided to automatically align the Schottky with one of the moderately doped cells. There is a low value energy effect in the empty region of the crystal junction-base diffusion interface. The Schottky energy structure has a scatter ring of the Schottky barrier ring and a lightly doped ΙΓ 磊 加 to stop the scattered ring layer of the Schottky scattered gold bipolar half-potential concave source region. The invention discloses an oxygen semi-electric crystal system with a crystal trough type and an enveloping formation, and the cells are double-expanded. The one side of the one is aligned with the Schottky barrier inlay structure and its manufacturing method. Alignment and meta-product integration. According to the present invention, the metal oxide semiconductor transistor structure trench gate region, wherein the automatic alignment source region includes at least one lightly doped and highly doped η + source diffusion ring surrounded by a middle groove gate region. Within the mid-surface portion, an automatic pair, one of the grooves is automatically aligned with at least one groove including Schott-type double-expanded Schottky, a self-type double-expanded energy barrier, and a gold-oxygen barrier. P-based expansion semiconductors with embedded alignment groove gates are doped with N-doped P-based expanded source contact windows
第10頁 1246194 五、發明說明 係形成於 半導體層 擴散環、 ί動對準 上的一個 及 之 於一 之上 一個 個自 矽閘 摻雜 該中 觸的 流及 槽式 雜質 槽式 能障 緣閘 個自 上。 個淺 且具 底部 動對 層覆 複晶 (5) 該中 、該 及形 源區 側邊 動對 該凹 凹槽 有或 凹槽 準高 度摻 高摻 成於 内之 牆介 準金 槽閘 内之 不具 表面 摻雜 雜Ρ -基擴散環所 雜η +源擴散環所 包圍的該淡 包圍的該中 該凹槽閘區的一個側邊牆之 的一個側邊 摻雜η 自動對 一個緩衝介電層 包圍的 電墊層所 屬矽化物層形成 區至少包含一個 一個凹槽 有一個厚 之上。該 複晶矽閘 半導體 隔離介 自動對 該面 於該 自動對準導 表面 電層 準導 上的一 個自 蓋有一個金屬碎化物層、或一 矽閘層填充有一個耐高溫 度推雜Ρ -基擴 一個擴散保護 軟性崩潰。上 雙擴散金氧半 型態的改變來 雙擴散金氧半 嵌位凹槽式雙 雙載子電晶體 散環係作 環來消除 述之自動 電晶體結 形成自動 電晶體結 擴散金氧 (IGBT) 為一個 該蕭特 對準蕭 構可以 對準蕭 構。另 半電晶 或金氧 金屬 自動 基二 特基 輕易 特基 外, 體結 半控 形成於 電閘層 動對準 個自動 或金屬 對準蕭 極體的 能障嵌 地將半 能障嵌 該自動 構可以 制閘流 摻雜 度摻 上且 表面 源擴 準源 電閘 個閘 該淺 至少 局換 對準 石夕化 特基 邊緣 位η-導體 位Ρ-對準 用來 體( 曰曰 雜Ρ-基 置於該 部份之 散環、 接觸窗 層形成 介電層 凹槽的 包含一 雜複晶 凹槽高 物層。 能障接 漏電電 通道凹 區之換 通道凹 蕭特基 製造絕 MCT) 實施方式Page 10, 1246194 V. Description of the invention is formed on the semiconductor layer diffusion ring, one on top of the other, and one on top of the other, one by one from the silicon gate doped with the middle flow and the trench impurity trench energy barrier edge The brakes come from the top. A shallow and bottom-moving layer is coated with a compound crystal (5) The side edges of the middle and the source regions are moved to the concave groove or the groove height is mixed into the inner wall of the gold groove gate. Without a surface doped hetero-p-based diffusion ring doped with η + a source diffusion ring surrounded by the lightly-enclosed one of the side walls of the recessed gate region, doped with η automatically to a buffer dielectric The silicide layer forming region of the electric pad layer surrounded by the layers includes at least one groove and a thickness above. The polycrystalline silicon gate semiconductor isolation medium automatically covers a self-covering metal chip layer on the surface of the self-aligned surface electric layer quasi-conductor, or a silicon gate layer is filled with a high temperature resistant impurity P- Basic expansion a soft collapse of diffusion protection. The double-diffused metal-oxygen half-type is changed to double-diffused metal-oxygen semi-clamped grooved double-battery transistor loose ring system as a ring to eliminate the described automatic transistor junction to form an automatic transistor junction diffused metal oxide (IGBT). Aligning Xiao Gou for one of these Schott can aim at Xiao Gou. In addition, the semi-transistor or metal oxide metal automatic base is easy to special, and the body junction semi-control is formed on the gate layer. The automatic barrier or the metal barrier is embedded in the energy barrier. The semi-energy barrier is embedded in the automatic barrier. The structure can be doped with the doping degree of the thyristor, and the gates of the surface source expansion and quasi-source switches should be at least partially exchanged and aligned at the edge of the lithographic base of the kiwi chemical base, the η-conductor position, and the P-alignment. The high-layer layer including a hetero-polycrystalline groove is formed in the loose ring and the contact window layer formed in this part, and the dielectric layer groove is formed. The barrier channel of the leakage channel of the electrical leakage channel can be changed. the way
第11頁 1246194 五、發明說明(6) 現請參見圖三A至圖三G,其中揭示製造本發明之一種 第一型自動對準蕭特基能障嵌位凹槽式雙擴散金氧半電晶 體結構的製程步驟及其簡要剖面圖。 圖三A顯示一個淡摻雜N —磊晶矽層 2 0 1形成一個高摻 雜 N +矽基板2 0 0之上;一個緩衝氧化物層 2 0 2係形成於該 < 淡摻雜N -磊晶矽層2 0 1之上;接著,一個罩幕介電層2 0 3係 , 形成於該緩衝氧化物層 2 0 2之上;然後,進行一個第一 罩幕光阻 (PR1)步驟來定義複數自動對準源區(SR) 及 一個凹槽閘區 (TGR),其中該複數自動對準源區(SR) 的每一個係由該凹槽閘區(TGR) 所包圍。該高摻雜N +矽 基板2 0 0係具有介於0 . 0 0 1歐姆·公分至 0 . 0 0 4歐姆·公分 之間的電阻係數及介於3 0 0微米至8 0 0微米之間的厚度, 並依晶圓尺寸來決定。該淡摻雜N —磊晶矽層 2 0 1係具有介 於1 0 0歐姆·公分至0 . 1歐姆·公分之間的電阻係數及介於 1 0 0微米至1微米之間的厚度。該緩衝氧化物層2 0 2係一個 4 熱二氧化矽層且其厚度介於2 0 0埃至1 0 0 0埃之間。這裡值 得注意的是,該複數自動對準源區(SR)之每一個的形狀 可以是正方形、長方形、六角形、圓形或柱狀等等。 圖三B顯示位於該凹槽閘區(TGR)之内的該罩幕介電 層 2 0 3係利用非等向乾式蝕刻法來加予去除,然後去除該 成形罩幕光阻(PR1);然後,透過該凹槽閘區(TGR)之 内的一個成形窗口進行硼離子佈植且接著加予驅入來形成 一個P-擴散區2 0 4a於該淡摻雜N—磊晶矽層 201之内;接著Page 11 1246194 V. Description of the invention (6) Please refer to FIG. 3A to FIG. 3G, which discloses the manufacture of a first type of self-aligned Schottky barrier with recessed double-diffusion metal-oxide halves of the present invention. The process steps of the transistor structure and its brief cross-sectional view. FIG. 3A shows a lightly doped N-epitaxial silicon layer 2 0 1 forming a highly doped N + silicon substrate 2 0 0; a buffer oxide layer 2 0 2 is formed on the < lightly doped N -Epitaxial silicon layer 201; then, a mask dielectric layer 203 is formed on the buffer oxide layer 202; then, a first mask photoresist (PR1) is performed Steps to define a complex automatic alignment source region (SR) and a groove gate region (TGR), wherein each of the complex automatic alignment source region (SR) is surrounded by the groove gate region (TGR). The highly doped N + silicon substrate 200 has a resistivity between 0.01 ohm · cm to 0.04 ohm · cm and a resistance coefficient between 300 micrometers and 800 micrometers. The thickness is determined by the wafer size. The lightly doped N-epitaxial silicon layer 201 has a resistivity between 100 ohm · cm to 0.1 ohm · cm and a thickness between 100 micrometers and 1 micrometer. The buffer oxide layer 202 is a 4 thermal silicon dioxide layer and has a thickness between 200 angstroms and 100 angstroms. It is important to note here that the shape of each of the complex auto-alignment source regions (SR) can be square, rectangular, hexagonal, circular or cylindrical, and so on. Figure three B shows that the mask dielectric layer 203 located in the groove gate region (TGR) is removed by anisotropic dry etching, and then the formed mask photoresist (PR1) is removed; Then, boron ion implantation is performed through a forming window in the groove gate region (TGR) and then driven to form a P-diffusion region 2 0 4a on the lightly doped N-epitaxial silicon layer 201 Within; then
第12頁 1246194 五、發明說明(7) ,透過相同的該成形窗口進行砷或磷離子佈植來形成一個 η +擴散區2 0 5 a於該p -擴散區2 0 4 a的一個表面部份之内。該 硼離子佈植的佈植劑量係介於1 0 13/平方公分及5 * 1 0 14/平方 公分之間,因而該p -擴散區2 0 4 a係中度摻雜(m 〇 d e r a t e 1 y -d o p e d)且具有一個接面深度介於0 . 8微米和3微米之間 。該磷或砷離子佈植劑量係介於1 0 15/平方公分和1 0 16/平方 公分,因此該η +擴散區 2 0 5 a係高摻雜(h e a v i 1 y d 〇 p e d) 且具有一個接面深度介於0 . 2微米和1微米之間。 圖三C顯示位於該凹槽閘區(TGR)之内的該緩衝氧化 物層 2 0 2係利用非等向乾式蝕刻法或濕式蝕刻法來加予去 除;接著,利用非等向乾式蝕刻法在該淡摻雜N -磊晶矽層 2 0 1之内形成一個淺凹槽;然後,進行一個清洗的步驟來 消除該淺凹槽之矽表面所產生的瑕疵;接著,一個閘介電 層2 0 6 a係形成於該淺凹槽的矽表面之上。這裡值得注意的 是,該清洗的步驟係先形成一個襯 (1 i n e r) 氧化物層於 該淺凹槽之矽表面之上再去除該襯氧化物層。該閘介電層 2 0 6 a係一個熱二氧化碎層或一個熱二氧化碎層在一個笑氣 (N 20)的環境下加予氮化且其厚度係介於1 0 0埃和1 0 0 0埃 之間。由圖三C可以清楚地看到,一個較厚的二氧化矽層 係形成於一個高摻雜N +源擴散環2 0 5 b之上,而圖三B内之 該P-擴散區2 0 4a係被該淺凹槽分離成位於該複數自動對準 源區(SR)的每一個之内的一個中度摻雜p-基擴散環2 04b 。另外,這裡可以清楚地看到,該淺凹槽的深度係比該p -擴散區2 0 4a的接面深度稍深。這裡值得強調的是,該較厚 1246194 五、發明說明(8) , 的二氧化矽層形成於該高摻雜η +源擴散環2 0 5b之上係有利 於提供該高摻雜η +源擴散環2 0 5b與後續所形成的導電閘層 之間具有一個良好的隔離層。 圖三D顯示一個回蝕複晶矽層2 0 7 a係形成於該凹槽閘 區(TGR)之内的該閘介電層 2 0 6a之上;然後,以一個自 動對準的方式佈植一個高劑量的磷或砷雜質。該回蝕複晶 f 矽層2 0 7a係先利用LPCVD法堆積一個厚度大約等於或大於 · 該凹槽閘區(TGR)的一半寬度之一個複晶矽層2 0 7 (未圖 示),然後回蝕所堆積之複晶矽層 2 0 7至稍高於該成形緩 衝氧化物層2 0 2 a的頂部水平。 圖三E顯示進行一個熱氧化製程來氧化該回蝕高摻雜 複晶矽層2 0 7a,以形成位於該凹槽閘區 (TGR)的一個平 面化覆蓋氧化物層2 0 8 a且同時重分佈一個自動對準高摻雜 複晶矽閘層2 0 7b之内的摻雜質。這裡值得注意的是,該平 < 面化覆蓋氧化物層2 0 8 a的頂部表面水平可以高於該複數自 動對準源區(SR)的每一個之内的該成形罩幕介電層2 0 3a ^ 的頂部表面水平,而該自動對準高摻雜複晶矽閘層2 0 7b的 一個頂部表面水平係位於該閘介電層2 0 6 a之該較厚的二氧 化物層的一個上方部份。 圖三F顯示位於該複數自動對準源區 (SR)的每一個 之内的該成形罩幕介電層2 0 3a係利用熱磷酸或非等向乾式 姓刻法來加予去除;一個側邊牆介電墊層2 0 9 a係形成於該 凹槽閘區(TGR)之内的該平面化覆蓋氧化物層 2 0 8a的一 個側邊牆之上且置於該複數自動對準源區(SR)的每一個Page 12 1246194 V. Description of the invention (7), arsenic or phosphorus ion implantation is performed through the same forming window to form an η + diffusion region 2 0 5 a at a surface portion of the p-diffusion region 2 0 4 a Within. The implantation dose of the boron ion implantation is between 10 13 / cm 2 and 5 * 1 0 14 / cm 2. Therefore, the p-diffusion region 2 0 4 a is moderately doped (m 〇derate 1). y-doped) and has a junction depth between 0.8 microns and 3 microns. The implantation dose of phosphorus or arsenic ions is between 10 15 / cm 2 and 10 16 / cm 2. Therefore, the η + diffusion region 2 0 5 a is highly doped (heavi 1 yd 〇ped) and has one The surface depth is between 0.2 micron and 1 micron. FIG. 3C shows that the buffer oxide layer 202 in the groove gate region (TGR) is removed by anisotropic dry etching or wet etching; then, anisotropic dry etching is used. A shallow groove is formed in the lightly doped N-epitaxial silicon layer 201; then, a cleaning step is performed to eliminate defects generated on the silicon surface of the shallow groove; then, a gate dielectric Layer 2 6 a is formed on the silicon surface of the shallow groove. It is worth noting here that the cleaning step is to form a liner (1 iner) oxide layer on the silicon surface of the shallow groove before removing the liner oxide layer. The gate dielectric layer 2 0 6 a is a thermal dioxide fragmentation layer or a thermal dioxide fragmentation layer which is pre-nitrided in a laughing gas (N 20) environment and its thickness is between 100 angstroms and 1 0 0 0 Angstroms. It can be clearly seen from FIG. 3C that a thicker silicon dioxide layer system is formed on a highly doped N + source diffusion ring 2 0 5 b, and the P-diffusion region 2 0 in FIG. 3B 4a is separated by the shallow groove into a moderately doped p-based diffusion ring 204b located within each of the plurality of auto-aligned source regions (SR). In addition, it can be clearly seen here that the depth of the shallow groove is slightly deeper than the junction depth of the p-diffusion region 204a. It is worth emphasizing here that the thicker 1246194 V. Invention Description (8), a silicon dioxide layer formed on the highly doped η + source diffusion ring 2 0 5b is conducive to providing the highly doped η + source There is a good isolation layer between the diffusion ring 2 0 5b and the conductive gate layer formed subsequently. FIG. 3D shows that an etch-back polycrystalline silicon layer 2 0 7a is formed on the gate dielectric layer 20 6a within the groove gate region (TGR); then, it is laid out in an automatic alignment manner. Plant a high dose of phosphorus or arsenic impurities. The etch-back polycrystalline silicon layer 2 7a is first deposited by a LPCVD method with a polycrystalline silicon layer 2 7 (not shown) having a thickness approximately equal to or greater than half the width of the groove gate region (TGR). Then, the stacked polycrystalline silicon layer 207 is etched back to a level slightly above the top of the shaped buffer oxide layer 202a. FIG. 3E shows that a thermal oxidation process is performed to oxidize the etch-back highly doped polycrystalline silicon layer 207a to form a planarized overlying oxide layer 208a located in the trench gate region (TGR) and at the same time Redistributes a dopant that automatically aligns within the highly doped complex silicon gate layer 207b. It is worth noting here that the top surface level of the planarized overlay oxide layer 208a may be higher than the shaped mask dielectric layer within each of the plurality of auto-aligned source regions (SR). The top surface level of 2 0 3a ^ is horizontal, and a top surface level of the auto-aligned highly doped complex crystalline silicon gate layer 2 7b is located at the thicker oxide layer of the gate dielectric layer 2 6 a An upper part of it. Figure 3F shows that the shaped mask dielectric layer 203a within each of the plurality of auto-aligned source regions (SR) is removed using hot phosphoric acid or anisotropic dry-type engraving; one side The side wall dielectric cushion layer 2 0 9 a is formed on a side wall of the planarized oxide layer 2 8 a within the groove gate region (TGR) and is placed on the plurality of automatic alignment sources. Every area (SR)
第14頁 1246194 五、發明說明(10) 一個擴散保護環來消除該蕭特基能障二極體的邊緣漏電電 流及軟性崩潰。另外,該中度摻雜P—擴散環2 04b係與該高 摻雜η +源擴散環2 0 5臟路來消除凹槽式雙擴散金氧半電晶 體細胞元之臨界電壓的本體(body)效應。另外,該中度 摻雜p -基基擴散環2 0 4 b所包圍的該淡摻雜n -磊晶矽層2 0 1 可以在一個順向阻隔 (forward blocking) 狀態下藉由Page 14 1246194 V. Description of the invention (10) A diffusion protection ring to eliminate the edge leakage current and soft breakdown of the Schottky barrier diode. In addition, the moderately doped P-diffusion ring 2 04b and the highly doped η + source diffusion ring 2 05 are dirty to eliminate the critical voltage body of the grooved double-diffused gold-oxide semi-electric crystal cell. )effect. In addition, the lightly doped n- epitaxial silicon layer 2 0 1 surrounded by the moderately doped p-based diffusion ring 2 0 4 b can be used in a forward blocking state by
該中度摻雜P-基擴散環6以U興琢淡摻^。π /w 之一個p - n接面所形成的一個空乏區來加予擠止,以消除 具有一個低值能障高度之該蕭特基能障二極體由於一種習 知的影像力降低效應 (image-force i〇wering effect) 所產生的一個較大逆向漏電電流。 — 現請參見圖四A至圖四E,其中揭示製造本發明之一種 第二型自動對準蕭特基能障嵌位凹槽式雙擴散金氧半電 體結構之接續圖圖三B的簡化製程步驟及其簡要剖面圖。 夕圖四A顯示一個厚隔離介電層2丨以係在形 ΐ層!=淺凹,的一個底部石夕表面之上。該厚= 先堆穑且右—虱化矽所組成且利用lpcvd法來堆積,4 )的」;f約等於或稍微大於該凹槽閘區(TR(The moderately doped P-based diffusion ring 6 is doped with U +. An empty area formed by a p-n junction of π / w is added to stop the elimination of the Schottky barrier diode with a low value barrier height due to a known image power reduction effect (Image-force i〇wering effect) A large reverse leakage current. — Please refer to FIG. 4A to FIG. 4E, which shows the continuation diagrams of the fabrication of a second type of self-aligned Schottky barrier double-diffusion metal-oxide semiconductor structure of the present invention. Simplified process steps and a brief cross-sectional view. Figure 4A shows a thick isolation dielectric layer 2 is tied to the shape of the layer 形! = Shallow concave, a bottom stone surface. The thickness = first piled up and right-lice silicon and stacked using lpcvd method, 4) "; f is approximately equal to or slightly larger than the groove gate area (TR (
淺凹槽的-d=石夕層212 (未圖示)來填滿i 積之二氧化矽;212至':蓉利^等向乾式蝕刻法回蝕所i 的-個底部表;if二於該中度摻 側邊=Z1顯二7 '閘介電層2 061)係形成於凹槽秒表面ί 相似地,一個較厚的二氧化矽層係形成於言-D = Shi Xi layer 212 (not shown) in the shallow groove to fill the silicon dioxide of i area; 212 to ': Rong Li ^ isotropic dry etching method to etch back the bottom of i; if two At this moderately doped side edge = Z1, 2′7 ′ gate dielectric layer 2 061) is formed on the second surface of the groove. Similarly, a thicker silicon dioxide layer is formed on the surface.
第16頁 1246194 五、發明說明(11) β 高摻雜η+源擴散環2 0 5b的一個凹槽矽表面之上。這裡值得 注意的是,在形成該厚隔離介電層2 1 2 a之前或在形成該厚 隔離介電層2 1 2 a之後可以進行一個清洗的步驟來消除挖槽 所產生的瑕疵。 圖四C顯示一個回蝕複晶矽層2 0 7 a係形成於該閘介電 層206 b之上且置於該厚隔離介電層212 a之上;接著,以自 動對準的方式進行高劑量的磷或砷離子佈植來將該回蝕複 . 晶碎層2 0 7 a力π予高換雜。 圖四 D顯示進行一個熱氧化製程來形成位於該凹槽閘 區(TGR)之内的一個覆蓋氧化物層2 0 8a,如圖三E所示。 根據圖三F及圖三G所示之製程步驟,圖四E可以輕易 ® 地得到。很明顯地,除了一個厚隔離介電層 2 1 2係形成於 該淺凹槽之該底部矽表面之上來降低閘至汲極間的電容及 提高閘至汲極間的崩潰電壓之外,圖四E係與圖三G非常地 相似 。 現請參見圖五A及圖五B,其中揭示製造本發明之一種 ’ 第三型自動對準蕭特基嵌位凹槽式雙擴散金氧半電晶體結 構之接續圖三C的簡化製程步驟及其簡要剖面圖。 圖五A顯示一個自動對準複晶矽閘層2 0 7b係形成於該 閘介電層2 0 6 a之上;然後,一對覆蓋側邊牆介電墊層21 3a 係形成於該成形罩幕介電層2 0 3 a的側邊牆之上且置於該自 動對準高摻雜複晶矽閘層2 0 7b的側邊表面部份之上;接著 ,一個自動對準高導電層2 1 4a係形成於該對覆蓋側邊牆介 電墊層21 3a之間的該自動對準高摻雜複晶矽閘層2 0 7b之上Page 16 1246194 V. Description of the invention (11) A groove on the silicon surface of β highly doped η + source diffusion ring 2 0 5b. It is worth noting here that before the thick isolation dielectric layer 2 1 2 a is formed or after the thick isolation dielectric layer 2 1 2 a is formed, a cleaning step may be performed to eliminate defects caused by the trenching. FIG. 4C shows that an etch-back polycrystalline silicon layer 207a is formed on the gate dielectric layer 206b and is placed on the thick isolation dielectric layer 212a. Then, the automatic alignment is performed. The high-dose phosphorus or arsenic ions are implanted to restore the etch-back. The grain fragment layer 207 a force π gives high replacement. FIG. 4D shows that a thermal oxidation process is performed to form a cover oxide layer 208a located in the trench gate region (TGR), as shown in FIG. 3E. According to the process steps shown in Figure 3F and Figure 3G, Figure 4E can be easily obtained. Obviously, except that a thick isolation dielectric layer 2 1 2 is formed on the bottom silicon surface of the shallow groove to reduce the capacitance between the gate and the drain and increase the breakdown voltage between the gate and the drain. The four E series are very similar to the three G in FIG. Please refer to FIG. 5A and FIG. 5B, which discloses a method for manufacturing a third type of self-aligning Schottky-type recessed double-diffused metal-oxide semiconductor structure with self-aligning Schottky in accordance with the present invention. And its brief cross-section. FIG. 5A shows that an auto-aligned polycrystalline silicon gate layer 2 7b is formed on the gate dielectric layer 2 6a; then, a pair of side wall dielectric pad layers 21 3a is formed on the shape. The mask dielectric layer 2 0 3 a is on the side wall and is placed on the side surface portion of the self-aligned highly doped polycrystalline silicon gate layer 2 7b; then, an auto-aligned highly conductive A layer 2 1 4a is formed on the self-aligned highly doped complex crystalline silicon gate layer 2 0 7b between the pair of side wall dielectric pads 21 3a.
第17頁 1246194 五、發明說明(12) ;然後,一個平面化覆蓋氧化物層2 0 8b係形成於該自動對 準高導電層2 1 4 a之上。該對覆蓋側邊牆介電墊層2 1 3 a係由 二氧化矽所組成且利用 LPCVD法來堆積,係先堆積一個二 氧化矽層 21 3 (未圖示)於所形成的結構表面之上,然後 回蝕所堆積之二氧化矽層 2 1 3的一個厚度。該自動對準高 導電層2 1 4a可以是利用一種習知自動對準矽化製程所形成 的一個金屬矽化物層或藉由先堆積一個耐高溫金屬矽化物 或耐高溫金屬層來填滿位於該對覆蓋側邊牆介電墊層2 1 3 a 的一個空隙再回蝕所堆積之耐高溫金屬矽化物或耐高溫金 屬層至所預定之厚度的一個回蝕耐高溫金屬矽化物或耐高 溫金屬層所組成。該金屬石夕化物層係由石夕化鈦(T i S i 0 、 矽化鈷 (CoS i 2)或矽化鎳(NiSi 2)所組成。該耐高溫金 屬石夕化物層可以是由石夕化嫣 (W S i 0所組成而該耐高溫金 屬層是由鎢(W)所組成。該平面化覆蓋氧化物層 2 0 8b係 由二氧化矽所組成且利用 LPCVD法來堆積,係先堆積一個 二氧化矽層2 0 8 (未圖示)來填滿位於該對覆蓋側邊牆介 電墊層2 1 3 a之間的空隙,然後再回蝕所堆積之二氧化矽層 2 0 8的一個厚度;或利用化學-機械研磨法 (c h e m i c a 1 -mechanical polishing; CMP) 來平面化所堆積之二氧化 石夕層2 0 8且以該成形罩幕介電層 2 0 3 a作為一個磨平停止層 。這裡值得注意的是,該自動對準高摻雜複晶矽閘層2 0 7a 可以在形成該對覆蓋側邊牆介電墊層2 1 3 a之前或之後佈植 一個高劑量的磷或砷摻雜質來加予高摻雜。 根據圖三F及圖三G所示之相同製程步驟,圖五B可以Page 17 1246194 V. Description of the invention (12); Then, a planarized cover oxide layer 2 0b is formed on the auto-aligned highly conductive layer 2 1 4a. The pair of side wall dielectric pads 2 1 3 a are composed of silicon dioxide and are stacked by LPCVD. First, a silicon dioxide layer 21 3 (not shown) is deposited on the surface of the structure. And then etch back a thickness of the stacked silicon dioxide layer 2 1 3. The self-aligning highly conductive layer 2 1 4a may be a metal silicide layer formed by a conventional auto-alignment silicidation process or by filling a high-temperature-resistant metal silicide or high-temperature-resistant metal layer first to fill the area. Etching back the high temperature resistant metal silicide or high temperature metal layer deposited to a gap covering the side wall dielectric cushion layer 2 1 3 a to an etch back high temperature resistant metal silicide or high temperature resistant metal of a predetermined thickness Made up of layers. The metal petrified material layer is composed of titanium petrified material (T i S i 0, cobalt silicide (CoS i 2) or nickel silicide (NiSi 2). The high temperature resistant metal petrified material layer may be made from petrified material Yan (WS i 0 and the high-temperature-resistant metal layer is composed of tungsten (W). The planarized cover oxide layer 2 8b is composed of silicon dioxide and is deposited by LPCVD method. The silicon dioxide layer 2 0 8 (not shown) fills the gap between the pair of side wall dielectric pads 2 1 3 a, and then etches back the deposited silicon dioxide layer 2 0 8 A thickness; or use chemical-mechanical polishing (CMP) to planarize the stacked SiO 2 layer 2 0 8 and use the formed mask dielectric layer 2 0 3 a as a flat surface It is worth noting here that the auto-aligned highly doped polycrystalline silicon gate layer 2 7a can be implanted with a high dose before or after the pair of side wall dielectric pads 2 1 3 a is formed. Phosphorus or arsenic dopants are used to add high doping. According to the same process steps shown in Figure 3F and Figure 3G, Figure 5B can
第18頁 1246194 五、發明說明(13) 輕易地得到。由圖五B可以清楚地看到,該自動對準高導 電層2 1 4 a係形成於該對覆蓋側邊牆介電墊層2 1 3 a之間的該 自動對準高摻雜複晶矽閘層2 0 7 b之上,因而比圖三G更有 效地降低閘連線的雜散電阻。另外,圖五B所示之該對覆 蓋側邊牆介電墊層2 1 3 a可以消除該高摻雜η +擴散環2 0 5 b與 該導電閘層 2 0 7b/ 2 1 4a之間的可能漏電路徑並同時降低源 ^ 與閘間的電容。 _ 現請參見圖六A及圖六B,其中揭示製造本發明之一種 第四型自動對準蕭特基能障嵌位凹槽式雙擴散金氧半電晶 體結構之接續圖三C的簡化製程步驟及其簡要剖面圖。 圖六A顯示一個自動對準高摻雜複晶矽閘層2 0 7b係形 p 成於該閘介電層2 0 6 a之上,然後形成一對覆蓋側邊牆介電 墊層2 1 3 a,如圖五A所示;接著,位於該對覆蓋側邊牆介 電墊層21 3a之間的該自動對準高摻雜複晶矽閘層2 0 7b係利 用非等向乾式蝕刻法加予蝕刻來形成一個凹槽高摻雜複晶 矽閘層2 0 7c;然後,一個回蝕導電層21 5a係填充位於該對 覆蓋側邊牆介電墊層2 1 3 a之間的一部份空隙;接著,一個 平面化覆蓋氧化物層2 0 8b係形成於該回蝕導電層21 5a之上 。該回蝕導電層 2 1 5 a係由矽化鎢 (WS i 2)或鎢(W)所組 成,係先堆積一個導電層 2 1 5 (未圖示)來填滿位於該對 覆蓋側邊牆介電墊層2 1 3 a之間的一個空隙,然後,回蝕所 _ 堆積之導電層 2 1 5至一個預定的厚度。相似地,該平面化 覆蓋氧化物層2 0 8b係如圖五A所描述的相同步驟來形成。 根據圖三F及圖三G所描述的相同製程步驟,圖六B可Page 18 1246194 V. Description of the invention (13) Easily available. It can be clearly seen from FIG. 5B that the auto-aligned highly conductive layer 2 1 4 a is the auto-aligned highly doped complex crystal formed between the pair of side wall dielectric pads 2 1 3 a The silicon gate layer is above 207b, so the stray resistance of the gate connection is more effectively reduced than that shown in Fig. 3G. In addition, the pair of side wall dielectric pads 2 1 3 a shown in FIG. 5B can eliminate the highly doped η + diffusion ring 2 0 5 b and the conductive gate layer 2 0 7b / 2 1 4a Possible leakage path and reduce the capacitance between the source ^ and the gate. _ Now refer to FIG. 6A and FIG. 6B, which discloses a continuation of the fabrication of a fourth type of self-aligned Schottky barrier barrier recessed double-diffused metal-oxide semiconductor structure of the present invention. Process steps and their brief cross-sectional views. FIG. 6A shows a self-aligned highly doped compound silicon gate layer 2 0 7b system p formed on the gate dielectric layer 2 0 6 a, and then a pair of side wall dielectric pad layers 2 1 is formed. 3 a, as shown in FIG. 5A; then, the self-aligned highly doped complex crystalline silicon gate layer 2 7b located between the pair of overlying side wall dielectric pads 21 3a uses anisotropic dry etching Farad pre-etching is used to form a groove highly doped polycrystalline silicon gate layer 2 0c; then, an etch-back conductive layer 21 5a is filled between the pair of side wall dielectric pad layers 2 1 3 a A part of the void is formed. Then, a planarized cover oxide layer 2 0b is formed on the etch-back conductive layer 21 5a. The etch-back conductive layer 2 1 5 a is composed of tungsten silicide (WS i 2) or tungsten (W), and a conductive layer 2 1 5 (not shown) is first stacked to fill the pair of side walls. A gap between the dielectric pad layers 2 1 3 a is then etched back to the stacked conductive layers 2 1 5 to a predetermined thickness. Similarly, the planarized capping oxide layer 208b is formed by the same steps as described in FIG. 5A. According to the same process steps described in FIG. 3F and FIG. 3G, FIG. 6B may
第19頁 1246194 五、發明說明 以輕易地 2 1 5 a可以 現請 第五型自 體結構之 圖七 成於該閘 一對覆蓋 2 0 3 a的側 2 0 7b的側 2 14a係形 對準高摻 氧化物層 本上,除 底部矽表 的製程步 根據 地得到。 該自動對 現請 型自動對 構之接續 圖八 成於該閘 (14) 得到。由圖六B可以清楚地看到,該回蝕導電層 比圖五B更能降低閘連線的雜散電阻。 參見圖七A及圖七B,其中揭示製造本發明之一種 動對準蕭特基能障嵌位凹槽式雙擴散金氧半電晶 接續圖四B的簡化製程步驟及其簡要剖面圖。 A顯示一個自動對準高摻雜複晶矽閘層2 0 7b係形 介電層2 0 6 b及該厚隔離介電層2 1 2 a之上;然後, 側邊牆介電墊層2 1 3 a係形成於該成形罩幕介電層 邊牆之上且形成於該自動對準高摻雜複晶矽閘層 邊表面部份之上;接著,一個自動對準高導電層 成於該對覆蓋側邊牆介電墊層2 1 3 a之間的該自動 雜複晶矽閘層2 0 7b之上;然後,一個平面化覆蓋 2 0 8b係形成於該自動對準高導電層2 14a之上。基 了一個厚隔離介電層2 1 2 a係形成於該淺凹槽的該 面之上外,形成圖七A的製程步驟係與形成圖六A 驟相同,因此進一步的描述可以省略。 圖三F及圖三G的相同製程步驟,圖七B可以輕易 比較圖七B及圖四E可以清楚地看到,圖七B提供 準高導電層2 1 4a來降低閘連線的雜散電阻。 參見圖八A及圖八B,其中揭示製造本發明之第六 準蕭特基能障嵌位凹槽式雙擴散金氧半電晶體結 圖四B的簡化製程步驟及其簡要剖面圖。 B顯示一個自動對準高摻雜複晶矽閘層2 0 7b係形 介電層2 0 6 b及該厚隔離介電層 2 1 2之上;然後,Page 19, 1246194 V. Description of the invention to easily 2 1 5 a can now invite the figure of the fifth type of self-structure 70% on the gate to cover the side of 2 0 3 a 2 0 7b side 2 14a series The quasi-highly-doped oxide layer is obtained in accordance with the process steps except for the bottom silicon surface. The continuation of the auto-match on-demand auto-configuration Figure 8 is obtained from the gate (14). It can be clearly seen from FIG. 6B that the etch-back conductive layer can reduce the stray resistance of the gate connection more than that of FIG. 5B. Referring to FIG. 7A and FIG. 7B, it is disclosed that the manufacturing method of a dynamically aligned Schottky barrier barrier-type recessed double-diffusion metal-oxide semiconductor transistor is continued from FIG. 4B and a simplified cross-sectional view thereof. A shows an automatic alignment of a highly doped complex crystalline silicon gate layer 2 0 7b series dielectric layer 2 6 6 b and the thick isolation dielectric layer 2 1 2 a; then, a side wall dielectric pad layer 2 1 3 a is formed on the side wall of the dielectric layer of the forming mask and is formed on the edge surface portion of the self-aligned highly-doped polycrystalline silicon gate layer; then, an auto-aligned highly conductive layer is formed on The pair covers the self-hybrid polysilicon gate layer 2 7b between the side wall dielectric pads 2 1 3 a; then, a planarized cover 2 8b is formed on the auto-aligned highly conductive layer 2 14a above. A thick isolation dielectric layer 2 1 2 a is formed on the surface of the shallow groove. The process steps for forming FIG. 7A are the same as the steps for forming FIG. 6A, so further description may be omitted. Figure 7F and Figure 3G have the same process steps. Figure 7B can be easily compared with Figure 7B and Figure 4E. It can be clearly seen that Figure 7B provides a quasi-high conductive layer 2 1 4a to reduce the spurious of the gate connection. resistance. Referring to FIG. 8A and FIG. 8B, it is disclosed that the sixth quasi-Schottky barrier-type recessed double-diffused metal-oxide semiconductor transistor of the present invention is fabricated. FIG. 4B is a simplified process step and a schematic cross-sectional view thereof. B shows an automatic alignment of the highly doped complex crystalline silicon gate layer 2 0 7b series dielectric layer 2 6 b and the thick isolation dielectric layer 2 1 2; then,
第20頁 1246194 五、發明說明(15) 幕介電層 晶矽閘層 側邊牆介 2 0 7b係利 摻雜複晶 於該對覆 接著,一 層2 1 5 a之 成有該厚 與形成圖 ,圖八B可 到,圖八 的雜散電 加予歸納 一對覆蓋側邊牆介電墊層2 1 3 a係形成於該成形罩 2 0 3 a的側邊牆之上且形成於該自動對準高摻雜複 2 0 7b的側邊表面部份之上;接著,位於該對覆蓋 電墊層2 1 3 a之間的該自動對準高摻雜複晶矽閘層 用非等向乾式蝕刻法來蝕刻,以形成一個凹槽高 矽閘層2 0 7 c ;然後,一個回蝕導電層2 1 5 a係形成 蓋側邊牆介電墊層2 1 3 a間之空隙的一部份之上; 個平面化覆蓋氧化物層2 0 8 b係形成於該回蝕導電 上。基本上,除了該淺凹槽的底部石夕表面之上形 隔離介電層2 1 2之外,形成該圖八A的製程步驟係 六A相同,因此更進一步的描述可以省略。 根據圖三F及圖三G所描述的相同製程步驟 以輕易地得到。比較圖八B及圖七B可以清楚地看 B具有該回#導電層2 1 5 a來進一步降低該閘連線 阻。 根據前面的描述,本發明的優點及特色可以 如下 : (a) 本發明之自動對準蕭特基能障嵌位凹槽式雙擴散金 氧半電晶體結構提供一個自動對準源區内之一個中間半導 體部份的一個自動對準蕭特基能障二極體且其製造無需嚴 謹罩幕光阻步驟。 (b) 本發明之自動對準蕭特基能障嵌位凹槽式雙擴散金Page 20, 1246194 V. Description of the invention (15) Screen dielectric layer, crystalline silicon gate layer, side wall dielectric 2 0 7b is doped with multiple crystals, and then a layer of 2 1 5 a has the thickness and formation. As shown in FIG. 8B, the stray electricity in FIG. 8 can be summarized. A pair of dielectric layer 2 1 3 a covering the side wall is formed on the side wall of the forming cover 2 0 3 a and is formed on The auto-aligned highly doped complex 207b is above the side surface portion; then, the auto-aligned highly-doped complex crystalline silicon gate layer is located between the pair of overlying electrical pads 2 1 3 a. Isotropic dry etching is used to etch to form a grooved high silicon gate layer 2 0 7 c; then, an etch-back conductive layer 2 1 5 a is formed to form a gap between the side wall dielectric pad 2 1 3 a A part of the planarized oxide layer 2 0 b is formed on the etch-back conductive layer. Basically, the process steps for forming FIG. 8A are the same as in FIG. 8A, except that the isolation dielectric layer 2 1 2 is formed on the surface of the bottom of the shallow groove, so further description can be omitted. It can be easily obtained according to the same process steps described in FIG. 3F and FIG. 3G. Comparing FIG. 8B and FIG. 7B, it can be clearly seen that B has the conductive layer 2 1 5 a to further reduce the gate connection resistance. According to the foregoing description, the advantages and features of the present invention can be as follows: (a) The self-aligning Schottky barrier recessed double-diffusion metal-oxide semiconductor structure of the present invention provides an automatic alignment in the source region. One of the intermediate semiconductor parts is automatically aligned with the Schottky barrier diode and its fabrication does not require a rigorous masking photoresist step. (b) The self-aligning Schottky barrier type recessed double-diffusion gold of the present invention
第21頁 1246194 五、發明說明(16) 氧半電晶體結構提供一個自動對準蕭特基能障二極體具有 -個中度摻雜P-基擴散環作為一個擴散保護環來消除該自 動對準蕭特基二極體的邊緣漏電電流及軟性崩潰。 (c) 本發明之自動對準蕭特基能障嵌位凹槽式雙擴散金 氧半電晶體結構提供一個自動對準源金屬矽化物層將一個 高摻雜η +源擴散環與一個中度摻雜p-基擴散環加予短路來 消除凹槽式雙擴散金氧半電晶體細胞元的本體效應且同時 作為一個自動對準蕭特基能障接觸金屬層。 (d) 本發明之自動對準蕭特基能障嵌位凹槽式雙擴散金 氧半電晶體結構提供位於一個中度摻雜P-基擴散環及一個 淡摻雜N-磊晶半導體層之間的一個逆向偏壓p-n接面來擠 止位於該自動對準蕭特基接觸金屬層之下的該淡摻雜N —磊 晶半導體層,因而由於影像力降低效應所產生的低值能障 高度之一個高逆向漏電電流可以消除。 (e) 本發明之自動對準蕭特基能障嵌位凹槽式雙擴散金 氧半電晶體結構提供一對覆蓋側邊牆介電墊層形成於一個 自動對準高摻雜複晶矽閘層的側邊表面部份之上來消除位 於一個自動對準高摻雜η +源擴散環與該自動對準高摻雜複 晶矽閘層之間的漏電電流路徑。 (f) 本發明之自動對準蕭特基能障嵌位凹槽式雙擴散金Page 21 1246194 V. Description of the invention (16) The oxygen semi-electric crystal structure provides an auto-aligned Schottky barrier diode with a moderately doped P-based diffusion ring as a diffusion protection ring to eliminate the automatic Leakage current and soft breakdown at the edge of the Schottky diode. (c) The self-aligning Schottky barrier barrier recessed double-diffused metal-oxide semiconductor structure of the present invention provides an auto-aligned source metal silicide layer that combines a highly doped η + source diffusion ring with a middle The degree-doped p-based diffusion ring is short-circuited to eliminate the bulk effect of the grooved double-diffused metal-oxide semi-electric crystal cell and at the same time act as an auto-alignment Schottky barrier to contact the metal layer. (d) The self-aligning Schottky barrier barrier recessed double-diffused metal-oxide semiconductor structure of the present invention provides a moderately doped P-based diffusion ring and a lightly doped N-epitaxial semiconductor layer. A reverse-biased pn junction is used to squeeze the lightly doped N-epitaxial semiconductor layer under the self-aligning Schottky contact metal layer, so the low-value energy due to the image power reduction effect is generated. A high reverse leakage current at the barrier height can be eliminated. (e) The self-aligning Schottky barrier barrier recessed double-diffusion metal-oxide semiconductor structure of the present invention provides a pair of side wall dielectric pads formed on an auto-aligned highly doped polycrystalline silicon The side surface portion of the gate layer is overlying to eliminate a leakage current path between an auto-aligned highly-doped η + source diffusion ring and the auto-aligned highly-doped complex silicon gate layer. (f) The self-aligning Schottky barrier type recessed double-diffusion gold of the present invention
第22頁 1246194 五、發明說明(17) 氧半電晶體結構提供一個自動對準高導電層形成於該對覆 蓋側邊牆介電墊層之間的該自動對準高掺雜複晶矽閘層之 上或位於該對覆蓋側邊牆介電墊層之間的一個凹槽高摻雜 複晶矽閘層内的一個回蝕導電層來降低閘連線的雜散電阻 (g) 本發明之自動對準蕭特基能障嵌位凹槽式雙擴散金 氧半電晶體結構提供一個厚隔離介電層形成於該淺凹槽的 一個底部半導體表面之上來降低閘至汲極間的電容及提高 位於閘至沒極間的崩潰電壓。 前述之自動對準蕭特基能障嵌位凹槽式η-通道雙擴散 金氧半電晶體結構可以經由改變半導體區的摻雜質型態來 輕易地製造自動對準蕭特基能障嵌位凹槽式Ρ-通道雙擴散 金氧半電晶體結構。相似地,該自動對準蕭特基能障嵌位 凹槽式雙擴散金氧半電晶體結構可以加予延伸來製造絕緣 閘雙載子電晶體(IGBT)及金氧半控制閘流體(MCT)。 本發明雖特別以參考所附的例子或内涵來圖示及描述 ,但僅是代表陳述而非限制。再者,本發明不侷限於所列 之細節,對於熟知此種技術的人亦可瞭解,各種不同形狀 或細節的更動在不脫離本發明的真實精神和範疇下均可製 造,但亦屬本發明的範疇。Page 22 1246194 V. Description of the invention (17) The oxygen semi-electric crystal structure provides an auto-aligned high-conductivity layer formed between the pair of side wall dielectric pads. A etch-back conductive layer in a groove in a highly-doped polycrystalline silicon gate layer above the layer or between the pair of covering side wall dielectric pads to reduce stray resistance of the gate line (g) The self-aligning Schottky barrier barrier recessed double-diffused metal-oxide semiconductor structure provides a thick isolation dielectric layer formed on a bottom semiconductor surface of the shallow recess to reduce the gate-to-drain capacitance. And increase the breakdown voltage between the gate and the pole. The aforementioned self-aligned Schottky barrier barrier recessed η-channel double-diffused metal-oxide semiconductor structure can be easily fabricated by changing the dopant type of the semiconductor region. Bit-groove P-channel double-diffused metal-oxide semiconductor structure. Similarly, the self-aligning Schottky barrier barrier recessed double-diffusion metal-oxide semi-transistor structure can be extended to manufacture insulated gate bipolar transistor (IGBT) and metal-oxide semi-controlled gate fluid (MCT). ). Although the present invention is particularly illustrated and described with reference to the attached examples or connotations, it is only a representative statement and not a limitation. Furthermore, the present invention is not limited to the listed details. Those skilled in the art can also understand that changes of various shapes or details can be made without departing from the true spirit and scope of the present invention, but also belong to the present invention. The category of invention.
第23頁 1246194 圖式簡單說明 圖一 A及圖一 B顯示先前技術之一種平面式雙擴散金氧 半功率電晶體的簡要圖示,其中圖一 A顯示它的簡要剖面 圖而圖一 B顯示它的等效元件代表圖。 圖二A及圖二B顯示先前技術的一種平面式雙擴散金氧 半電晶體結構與一個蕭特基能障二極體積體化的簡要圖示 ,其中圖二A顯示它的簡要剖面圖而圖二B顯示它的等效元 件代表圖。 圖三A至圖三G揭示製造本發明之一種第一型自動對準 蕭特基能障嵌位凹槽式雙擴散金氧半電晶體結構的製程步 驟及其簡要剖面圖。 圖四A至圖四E揭示製造本發明之一種第二型自動對準 蕭特基能障嵌位凹槽式雙擴散金氧半電晶體結構之接續圖 三B的簡化製程步驟及其簡剖面圖。 圖五A及圖五B揭示製造本發明之一種第三型自動對準 蕭特基能障嵌位凹槽式雙擴散金氧半電晶體結構之接續圖 三C的簡化製程步驟及其簡剖面圖。 圖六A及圖六B揭示製造本發明之一種第四型自動對準 蕭特基能障嵌位凹槽式雙擴散金氧半電晶體結構之接續圖 三C的簡化製程步驟及其簡要剖面圖。 圖七A及圖七B揭示製造本發明之一種第五型自動對準 蕭特基能障嵌位凹槽式雙擴散金氧半電晶體結構之接續圖 四 A的簡化製程步驟及其簡要剖面圖。 圖八A及圖八B揭示製造本發明之一種第六型自動對準 蕭特基能障嵌位凹槽式雙擴散金氧半電晶體結構之接續圖Page 1246194 Brief Description of Drawings Figures 1A and 1B show a schematic diagram of a planar double-diffusion metal-oxide half-power transistor of the prior art, wherein Figure 1A shows a schematic cross-sectional view thereof and Figure 1B shows Its equivalent element represents the drawing. FIG. 2A and FIG. 2B are schematic diagrams showing a planar double-diffused metal-oxide semi-electric crystal structure and a Schottky barrier diode bipolar volume structure of the prior art. FIG. 2A shows a schematic cross-sectional view thereof. Figure 2B shows its equivalent component representation. Figures 3A to 3G show the manufacturing steps and a schematic cross-sectional view of manufacturing a first type of self-aligning Schottky barrier double-diffusion metal-oxide semiconductor structure with Schottky barriers. FIGS. 4A to 4E show the continuation of manufacturing a second type of self-aligned Schottky barrier barrier recessed double-diffused metal-oxide semiconductor structure in accordance with the present invention. FIG. Illustration. FIG. 5A and FIG. 5B show the continuation of manufacturing a third type of self-aligning Schottky barrier barrier recessed double-diffusion metal-oxide semiconductor structure of the present invention. FIG. Illustration. FIG. 6A and FIG. 6B show the continuation of manufacturing a fourth type of self-aligning Schottky barrier barrier recessed double-diffused metal-oxide semiconductor structure in accordance with the present invention. FIG. Illustration. FIG. 7A and FIG. 7B show the continuation of manufacturing a fifth type of self-aligned Schottky barrier barrier recessed double-diffused metal-oxide semiconductor structure in accordance with the present invention. FIG. Illustration. FIG. 8A and FIG. 8B show the continuation diagrams of the manufacture of a sixth type of self-alignment Schottky energy barrier recessed double-diffused metal-oxide semiconductor crystal structure of the present invention.
第24頁 1246194 圖式簡單說明 四 A的簡化製程步驟及其簡要剖面圖 代表圖號說明: 201 淡摻雜N-磊晶矽層 2 0 0 高摻雜N+矽基板 2 0 2 緩衝氧化物層 2 0 2a/ 2 0 2b成形緩衝氧化物層 2 0 3 罩幕介電層 203a成形罩幕介電層 2 0 4a P-擴散區 2 0 4b中度摻雜p-基擴散環 2 0 5 a高摻雜η +擴散區 2 0 5 b高摻雜η +源擴散環 2 0 6a/ 2 0 6b閘介電層 20 7a回蝕高摻雜複晶矽層 2 0 7b自動對準高摻雜複晶矽閘層 2 0 7c自動對準凹槽高摻雜複晶矽閘層 2 0 8 a平面化氧化物層 208b平面化覆蓋氧化物層 209a側邊牆介電墊層 2 1 0 a蕭特基接觸金屬層 211 源金屬層 212a厚隔離介電層 213a覆蓋側邊牆介電墊層 2 1 4 a自動對準财高溫金屬或金屬石夕化物層 215a回蝕導電層 _Page 24 1246194 The diagram briefly illustrates the simplified process steps of four A and its brief cross-sectional view represents the figure number description: 201 Lightly doped N- epitaxial silicon layer 2 0 0 Highly doped N + silicon substrate 2 0 2 Buffer oxide layer 2 0 2a / 2 0 2b Shaped buffer oxide layer 2 0 3 Mask dielectric layer 203a Shape mask dielectric layer 2 0 4a P-diffusion region 2 0 4b Moderately doped p-based diffusion ring 2 0 5 a Highly doped η + diffusion region 2 0 5 b Highly doped η + source diffusion ring 2 0 6a / 2 0 6b gate dielectric layer 20 7a etch back highly doped polycrystalline silicon layer 2 0 7b automatically aligned with high doping Complex silicon gate layer 2 0 7c Automatically aligned grooves Highly doped compound silicon gate layer 2 0 8a Planarized oxide layer 208b Planarized oxide layer 209a Side wall dielectric pad 2 1 0 a Tiki contact metal layer 211 source metal layer 212a thick isolation dielectric layer 213a covers side wall dielectric pad layer 2 1 4 a Automatically aligns high temperature metal or metal oxide layer 215a etch back conductive layer _
第25頁Page 25
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TWI743818B (en) * | 2020-06-02 | 2021-10-21 | 台灣半導體股份有限公司 | Schottky diode with multiple guard ring structures |
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TWI397154B (en) * | 2010-01-21 | 2013-05-21 | Great Power Semiconductor Corp | Trenched power semiconductor structure with schottky diode and fabrication method thereof |
TWI743818B (en) * | 2020-06-02 | 2021-10-21 | 台灣半導體股份有限公司 | Schottky diode with multiple guard ring structures |
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