TW402749B - Field effect transistor with self-aligned T-type gate - Google Patents
Field effect transistor with self-aligned T-type gate Download PDFInfo
- Publication number
- TW402749B TW402749B TW87118214A TW87118214A TW402749B TW 402749 B TW402749 B TW 402749B TW 87118214 A TW87118214 A TW 87118214A TW 87118214 A TW87118214 A TW 87118214A TW 402749 B TW402749 B TW 402749B
- Authority
- TW
- Taiwan
- Prior art keywords
- layer
- gate
- mentioned
- scope
- dielectric layer
- Prior art date
Links
Landscapes
- Insulated Gate Type Field-Effect Transistor (AREA)
Abstract
Description
五、發明說明(1) 本發明係有關於 極場效電晶體元件的 用,可用以降低電晶 寄生電容。 隨著半導體技術 進,所以元件之積集 體之閘極寄生電阻和 性。深次微米CMOS元 無線通訊技術的主流 後,元件將可滿足高 上述元件閘極之寄生 必須加以克服才行。 一種具有空氣邊隙之自我 製造方法’其製程新顆、簡單且實閑 體其閘極與源/汲極間之寄生電阻及 的進步’製程技術-直朝深次微米前 度增加而尺寸亦隨之減小,因此電晶 寄生電容亦開始料元件之傳輸特曰9 件與電路預計在未來數年,將會成為 ,因為當元件線寬小於〇. 25微米之 頻運作之需求,且其成本低廉。不過 電阻與其之寄生電容侧邊之問題點則 目前用以降低寄生電阻之方法,主要有自行對準金屬 矽化製程(salicide process)。然而,此一方式有其限制 而影響其應用。當製程技術再往深次微米縮小時,在以自 行對準金屬矽化製程形成極細線寬之傳導線時,傳導線之 片電阻會有急速上升的現象(稱為窄線寬效應,narrow 1 ine-width effect)。此外,因為熱而引起之聚合效應 (agglomeration effect)會使製程之整合更加困難。 就降低寄生電容之方式而言,T〇g〇等人於「A Gate-side Air-gap Structure (GAS) to Reduce the parasitic Capacitance in MOSFETs ; 1 996 Symposium on VLSI Technology Digest of Technical Papers 」中 有揭露利用數次成長不同材質的邊襯(spacer)與選擇性製5. Description of the invention (1) The present invention relates to the use of extremely field-effect transistor elements, which can be used to reduce the parasitic capacitance of the transistor. With the advancement of semiconductor technology, the gate parasitic resistance and characteristics of the integrated body of the components. After the mainstream of deep sub-micron CMOS wireless communication technology, components will be able to meet the high parasitics of the gates of these components, which must be overcome. A self-manufacturing method with an air gap 'its process is new, simple and practical, and its parasitic resistance between the gate and source / drain electrodes and its progress' process technology-increasing to the depth of the sub-micron, and the size is also With the reduction, the parasitic capacitance of the transistor has also begun to transfer the components. The 9 pieces and circuits are expected to become in the next few years, because when the line width of the components is less than 0.25 micrometers, the operation is required, and its low cost. However, the problem of the side of the resistor and its parasitic capacitance is the current method to reduce the parasitic resistance, which mainly includes self-aligned metal silicide process. However, this method has its limitations and affects its application. When the process technology is further reduced to the deep sub-micron, when the self-aligned metal silicidation process is used to form a very thin line width conductive line, the sheet resistance of the conductive line will increase rapidly (called the narrow line width effect, narrow 1 ine -width effect). In addition, agglomeration effects due to heat can make integration of the process more difficult. In terms of ways to reduce parasitic capacitance, Togo et al. Disclosed in "A Gate-side Air-gap Structure (GAS) to Reduce the parasitic Capacitance in MOSFETs; 1 996 Symposium on VLSI Technology Digest of Technical Papers" Use several times to grow the spacer and selective system of different materials
第4頁 2000. 04.15. 004 五、發明說明(1) 本發明係有關於 極場效電晶體元件的 用,可用以降低電晶 寄生電容。 隨著半導體技術 進,所以元件之積集 體之閘極寄生電阻和 性。深次微米CMOS元 無線通訊技術的主流 後,元件將可滿足高 上述元件閘極之寄生 必須加以克服才行。 一種具有空氣邊隙之自我 製造方法’其製程新顆、簡單且實閑 體其閘極與源/汲極間之寄生電阻及 的進步’製程技術-直朝深次微米前 度增加而尺寸亦隨之減小,因此電晶 寄生電容亦開始料元件之傳輸特曰9 件與電路預計在未來數年,將會成為 ,因為當元件線寬小於〇. 25微米之 頻運作之需求,且其成本低廉。不過 電阻與其之寄生電容侧邊之問題點則 目前用以降低寄生電阻之方法,主要有自行對準金屬 矽化製程(salicide process)。然而,此一方式有其限制 而影響其應用。當製程技術再往深次微米縮小時,在以自 行對準金屬矽化製程形成極細線寬之傳導線時,傳導線之 片電阻會有急速上升的現象(稱為窄線寬效應,narrow 1 ine-width effect)。此外,因為熱而引起之聚合效應 (agglomeration effect)會使製程之整合更加困難。 就降低寄生電容之方式而言,T〇g〇等人於「A Gate-side Air-gap Structure (GAS) to Reduce the parasitic Capacitance in MOSFETs ; 1 996 Symposium on VLSI Technology Digest of Technical Papers 」中 有揭露利用數次成長不同材質的邊襯(spacer)與選擇性製Page 4 2000. 04.15. 004 V. Description of the invention (1) The present invention relates to the use of an extremely field effect transistor element, which can be used to reduce the parasitic capacitance of the transistor. With the advancement of semiconductor technology, the gate parasitic resistance and characteristics of the integrated body of the components. After the mainstream of deep sub-micron CMOS wireless communication technology, components will be able to meet the high parasitics of the gates of these components, which must be overcome. A self-manufacturing method with an air gap 'its process is new, simple and practical, and its parasitic resistance between the gate and source / drain electrodes and its progress' process technology-increasing to the depth of the sub-micron, and the size is also With the reduction, the parasitic capacitance of the transistor has also begun to transfer the components. The 9 pieces and circuits are expected to become in the next few years, because when the line width of the components is less than 0.25 micrometers, the operation is required, and its low cost. However, the problem of the side of the resistor and its parasitic capacitance is the current method to reduce the parasitic resistance, which mainly includes self-aligned metal silicide process. However, this method has its limitations and affects its application. When the process technology is further reduced to the deep sub-micron, when the self-aligned metal silicidation process is used to form a very thin line width conductive line, the sheet resistance of the conductive line will increase rapidly (called the narrow line width effect, narrow 1 ine -width effect). In addition, agglomeration effects due to heat can make integration of the process more difficult. In terms of ways to reduce parasitic capacitance, Togo et al. Disclosed in "A Gate-side Air-gap Structure (GAS) to Reduce the parasitic Capacitance in MOSFETs; 1 996 Symposium on VLSI Technology Digest of Technical Papers" Use several times to grow the spacer and selective system of different materials
第4頁 2000. 04.15. 004 1Q2749 五、發明說明(2) 程而得到一空氣邊襯。由於空氣之八 a 使用之氧化層(介電常數4)或氮化^,常數為1,較傳統 可以降低寄生電容。但是,T〇g〇 介電常數7 )低,所以 複雜之製程(所以成本高),而且所彳ί不者需要使用到相當 所以降低寄生電容之效果有限,于=空氣邊襯並不大, 寄生電阻。 ,、也無法有效地改善 另外,編號32 7241之中華民國專利, Τ型閑極以降低寄生電阻,再以CVD ==形: 形成空氣邊隙,藉以降低寄匕層之方式 有.利用微衫蝕刻步驟定義該氮化矽層,形成一開口,,… =ί"…形成一多晶矽’並利用微影蝕刻步驟,在該開口 疋義出一寬度大於該開口之多晶矽閘極,因而兩端覆蓋 了部分的該氮化矽層”。所以,其形成τ型閘極至少須使用 兩道光罩並非為自動對準(self-aligned)之製程,而增 加製造之成本。而且,設計時須考慮對準之問題而必須增 加T型閘極側邊之寬度,如此將會使寄生電容增加,因而 降低了使用空氣邊隙之優點。 有鑑於此,本發明之主要目的為提供一種自我對準T 型閘極場效電晶體的製造方法,所製作之場效電晶體除了 可用以降低電晶體其閘極與源/汲極間之寄生電阻,可有 效解決上述窄線寬效應之問題,以及降低閘極與源/汲極 間之寄生電容,而且製程簡單,光罩數目少於上述之專 利’低成本,其與傳統製程相容所以更可以輕易應用在一 般之生產線上。Page 4 2000. 04.15. 004 1Q2749 5. Description of the invention (2) process to obtain an air lining. Because of the oxide layer (dielectric constant 4) or nitriding ^ used for air eight a, the constant is 1, which can reduce the parasitic capacitance more traditionally. However, T0g0 has a low dielectric constant 7), so it has a complicated manufacturing process (so the cost is high), and it needs to be used quite, so the effect of reducing parasitic capacitance is limited. Parasitic resistance. In addition, it can not effectively improve. In addition, the Republic of China patent No. 32 7241, T-shaped pole to reduce parasitic resistance, and then CVD == shape: the formation of air gaps to reduce the dagger layer. The use of micro-shirt The etching step defines the silicon nitride layer to form an opening, ... = ί " ... forms a polycrystalline silicon 'and uses a lithographic etching step to define a polycrystalline silicon gate with a width larger than the opening in the opening, so that both ends are covered. Part of this silicon nitride layer ". Therefore, it is necessary to use at least two photomasks to form a τ-type gate, which is not a self-aligned process and increases the cost of manufacturing. Moreover, consideration must be given to the design It is necessary to increase the width of the side of the T-gate. This will increase the parasitic capacitance and reduce the advantage of using air gaps. In view of this, the main purpose of the present invention is to provide a self-aligned T-type A method for manufacturing a gate field effect transistor. In addition to reducing the parasitic resistance between the gate and source / drain of the transistor, the field effect transistor can effectively solve the problem of the narrow line width effect described above. And reduce the parasitic capacitance between the gate and source / drain, and the process is simple, the number of photomasks is less than the above patent 'low cost, it is compatible with the traditional process, so it can be easily applied to a general production line.
C:\ProgramFiles\Patent\0522-3940-E.ptd第 5 頁 40274aC: \ ProgramFiles \ Patent \ 0522-3940-E.ptd page 5 40274a
為了達到上述目的,本發明提供— 極場效電晶體電元件之製造方法, '自型閘 五、發明說明(3) _ 形成空氣邊隙,其包括以下之步驟 進而在閘極側邊 提供一半導體基底’依序於1 -第二介電層、以及一第三介電層;=:。介:層、 可由,硼磷矽玻璃、磷矽玻璃、硼矽玻二、仙第:,丨電層 選擇,上述第一介電層為墊氧化層0S::-者 化矽。 上述弟一介電層為氮 定義蝕刻上述第三、第二、第一In order to achieve the above object, the present invention provides a method for manufacturing a polarized field effect transistor electrical element, 'Self-shaped gate V. Description of the invention (3) _ forming an air gap, which includes the following steps to further provide a gate side The semiconductor substrate is sequentially formed by a 1-second dielectric layer and a third dielectric layer; = :. Dielectric layer: can be selected from borophosphosilicate glass, phosphosilicate glass, borosilicate glass, and selenium :, and the electrical layer is selected. The first dielectric layer is a pad oxide layer 0S ::-or silicon. The above-mentioned dielectric layer is nitrogen, which defines the third, second, and first etching.
D 以露出上述半導體基底。 β ,形成一開 形成一閘極氧化層於上述開口 .,.. 1 丞展上。 沈積一弟一導電層於上述開口中、 之上。 及上述第三介電層 使用例如CMP以便平坦化上述第一暮 -導電層僅存在於上述開口之中,弟以作導為電層:使上述第 -導電層例如為複Β曰… 以作為-閑極’上述第 使用例如為氫氟酸之蝕刻劑或是Β〇Ε, 介電層,以露出上述閘極之上端部分。 μ ; 一 施行第一次離子佈植,以形成第一 兩侧。 y战弟摻雜區於上述閘極 形成一堆疊導電層於上述閘極和上述入 藉以和上述閘極構成型閘極結構;上 —'層上, 材質係選自複晶矽、矽化金屬、摻雜複晶矽广電層之 鈦金屬之一者。 日7鎢、鈷、及D to expose the semiconductor substrate. β, forming an opening, forming a gate oxide layer on the opening ... 1 spread. A conductive layer is deposited on and above the openings. And the third dielectric layer uses, for example, CMP in order to planarize the first twilight-conducting layer existing only in the openings, and it is used as a conductive layer: the above-mentioned first conductive layer is, for example, a complex B ... -The electrode is used as an etchant such as hydrofluoric acid or BOE, a dielectric layer to expose the upper end portion of the gate electrode. μ; A first ion implantation was performed to form the first sides. The y-doped region forms a stacked conductive layer on the gate, and forms a gate structure with the gate and the gate; on the upper layer, the material is selected from polycrystalline silicon, silicon silicide, One of the titanium metals doped with a polycrystalline silicon broadcast layer. Japan 7 Tungsten, Cobalt, and
C:\Program Files\Patent\0522-3940-E.ptd第 6 頁 * -402749C: \ Program Files \ Patent \ 0522-3940-E.ptd page 6 * -402749
形成第一擦雜區 以作為源/ 進行第二次離子佈植 汲·極區。 从選擇性蝕刻,去除上述第二介電層。 上,:法Λ成一絕緣層於:述半導體基材之 一捧雜=於上述τ型閉極結構之堆疊導電層下方和上述第 摻雜區之間有空氣間隙(air space)存在。 其中上述堆疊導電層之形成方法有二: —為先行沈積一導電層於上述閘極和上述介電層之 非等向性蝕刻上述導電層,以形成導電間隔物於上 端之側壁上而作為上述堆疊導電層,藉以和上述 =構成T型間極結構,其中上述導電層之银刻係使用以 鹵,乳體、鹵素化合物、鹽酸、含溴化合物之一者、 混合物來進行非等向性乾式蝕刻。 …、 田二為針對上述閘極使用選擇性沈積法,以形成上述堆 豐導電層於上述閘極和介電層上,藉以和上述閘極 型閘極結構。 依據本發明之自我對準T型閘極場效電晶體電元件之 造方法,其製程簡單,且可與傳統製程相融合。由於本 明製造之T型閘極MOS電晶體,其閘兩側之邊襯均包含有办 氣間隙,所以可以降低閘極之寄生電容。又依據本發明= 製作之Τ型閘極場效電晶體電元件,由於形成一 τ型導電閘 極,使閘極之等效之寬度變大,故可以有效降低閘極 電阻之片電阻值。 t 圖式之簡單說明:A first impurity region is formed to serve as a source / drain ion region for the second ion implantation. From the selective etching, the above-mentioned second dielectric layer is removed. Above, an insulating layer is formed on the semiconductor substrate, and an air gap exists between the above-mentioned τ-type closed-pole structure under the stacked conductive layer and the above-mentioned doped region. There are two methods for forming the above-mentioned stacked conductive layers:-firstly deposit a conductive layer on the gate and the dielectric layer to anisotropically etch the conductive layer to form a conductive spacer on the upper side wall as the above The conductive layer is stacked to form a T-type interpolar structure. The silver engraving of the conductive layer is made of halogen, emulsion, halogen compound, hydrochloric acid, bromine-containing compound, or a mixture for anisotropic dry type. Etching. …, Tian Er used the selective deposition method for the above-mentioned gates to form the above-mentioned conductive layer on the above-mentioned gates and the dielectric layers, thereby the above-mentioned gate-type gate structure. According to the manufacturing method of the self-aligned T-gate field effect transistor according to the present invention, the manufacturing process is simple and can be integrated with the traditional manufacturing process. Since the T-gate MOS transistor manufactured by the present invention includes air gaps on both sides of the gate, the parasitic capacitance of the gate can be reduced. According to the present invention, the T-gate field-effect transistor is fabricated. Since a τ-type conductive gate is formed, the equivalent width of the gate becomes larger, so the sheet resistance value of the gate resistance can be effectively reduced. Brief description of t schema:
C:\Program Files\Patent\0522-3940-E.ptd第 7 頁 五 l〇W8 懂 發明說明(5) ,$讓本發明之上述目的、特徵、和優點能更明顯易 文特舉兩個較佳實施 附圖式,做詳細 丨月如下: σ / ’ 說明如下 例β 第1 Κ圖係顯示依據本發明製造方法之第一實施 1夕J之流程剖面圖; 第2 A 2 C圖係顯示第一實施例部份步驟之另一種選 以及 擇;以及 第3A〜3D圖係顯示本發明第 付琥說明: 1二半導體基材;2〜第—介電層(塾氧啤層);3翁I a鼠化矽層);4〜第三介電層(TE〇s);弓二開口; 閘極 证妯、曰.’ 7〜第一導電層(開極);8〜第一摻雜區(源/汲極區 ] ’9〜堆疊導電層;1〇〜第二摻雜區(深源/汲極區); 1 上氧化層…〜空氣間隙;1S〜堆疊導電層。 a施例一: 第1A至第1G圖係顯示依據本發明之製造方法之流程剖 w 。以下將配合圖式說明本發明之製 步驟一 例之部份流程圖 第二介 閘極 提供一半導體基材1, 其上依厲形成第一介電層2 4,如第1A圖所示。 上述基材1為.一般之石夕晶片, 、第二介電層3、及第三介電 在 層 上述第一介電層2為厚度介於5〇〜2〇〇埃之 (pad 0Xide);上述第二介電層3為使用低 (LPCVD)所形成之氮化矽層;上 _ 1 . 示一;丨電層4可由硼磷矽C: \ Program Files \ Patent \ 0522-3940-E.ptd Page 7 5 10W8 Understand the description of the invention (5), so that the above-mentioned objects, features, and advantages of the present invention can be more obvious. The preferred implementation drawings are detailed below as follows: σ / 'The following example is explained. Β Figure 1K is a cross-sectional view showing the flow chart of the first implementation of the manufacturing method according to the present invention; Figure 2A 2C Shows another option and choice of some steps of the first embodiment; and the 3A to 3D diagrams show the description of the first embodiment of the present invention: 12 semiconductor substrates; 2 to the first-dielectric layer (kraft beer layer); 3 Won I a ratified silicon layer); 4 to the third dielectric layer (TE0s); bow two openings; gate card 妯, said. 7 ~ the first conductive layer (open pole); 8 ~ the first Doped region (source / drain region) '9 ~ stacked conductive layer; 10 ~ second doped region (deep source / drain region); 1 upper oxide layer ... ~ air gap; 1S ~ stacked conductive layer. A Embodiment 1: Figures 1A to 1G are flow charts of the manufacturing method according to the present invention. The following is a part of a flowchart illustrating an example of the manufacturing steps of the present invention with drawings. The gate provides a semiconductor substrate 1 on which a first dielectric layer 24 is formed, as shown in FIG. 1A. The above substrate 1 is a general Shi Xi wafer, a second dielectric layer 3, and The third dielectric layer is the first dielectric layer 2 with a thickness of 50 ~ 200 angstroms (pad 0Xide); the second dielectric layer 3 is a silicon nitride layer formed using low (LPCVD) ; On _ 1. Show one; 丨 the electrical layer 4 can be borophosphosilicate
402749402749
玻璃、磷矽破填 施例為使用氣象 步驟二 、蝴矽玻璃、TE0S中之一者選擇,在此 沈積法(CVD)而得之TE0S。The glass and phosphorous silicon underfilling example is selected by using one of the meteorological step 2, butterfly glass, and TE0S, and the TE0S obtained by the deposition method (CVD).
開口 5,:露義::述Τ導第體U 第-介電層’形成 干¥體基底1 ’結果如第1B圖所示。 . ^ 了避免短通道效應(short channel effect )之 ^ . ’ 5中所路出之基底1進行必要之通道離 子佈植。 步驟三 閘極氧化層6於上述開口 5中之基底 以熱氧化法形成一 1上’如第1 c圖所示。 步驟四 沈積第—導電層7於上述開口5中和上述第三介電層 4之上,如第1D圖所示。 此貝施例中,上述第一導電層7為複晶矽,其厚度必 須大於上述開口5寬度之半’以確保能夠將上述開的填 步驟五 使用化學機械研磨法(CMP),平坦化上述第一導電層 7,使上述第一導電層僅存在於上述開口 5之中以作為_ 閘極7 ’結果如第1E圖所示。 … 步驟六 使用例如含氫氟酸或是Β0Ε,對上述第三介電層4 (TE0S)進行選擇性蝕刻,去除上述第三介電層$,而露出Opening 5 :: Lu Yi :: Describing the T-th body U-dielectric layer 'to form a dry body substrate 1' The results are shown in Figure 1B. ^ To avoid the short channel effect (^.), The substrate 1 that is routed out in 5 is used for necessary channel ion implantation. Step 3 The substrate of the gate oxide layer 6 in the opening 5 is formed on the substrate 1 by thermal oxidation as shown in FIG. 1c. Step 4: A first conductive layer 7 is deposited in the opening 5 and above the third dielectric layer 4, as shown in FIG. 1D. In this example, the first conductive layer 7 is polycrystalline silicon, and its thickness must be greater than half of the width of the opening 5 to ensure that the above-mentioned filling step 5 can be planarized using chemical mechanical polishing (CMP). The first conductive layer 7 allows the first conductive layer to exist only in the opening 5 as the gate electrode 7 ′. The result is shown in FIG. 1E. … Step 6 Use, for example, hydrofluoric acid or BOE to selectively etch the third dielectric layer 4 (TE0S) to remove the third dielectric layer $ and expose
C:\Program Fi les\Patent\0522_3940-E· ptd第 9 頁 、、 五、發明說明(7] ' ---— --- 閘極7上端之局部,如第1F圖所示。 步驟七 進行離子佈植,形成第一摻雜區8於上述閘極7之兩 :挪而作為MOS電晶體之源/汲極區延伸,如第( 示。 ,驟八 先行沈積一第二導電層於上述閘極7和上述第二介電 層3之上,其厚度介於5〇〇〜2〇〇〇埃之間,可依實際需要來 配合調整,以本實施例而言厚度為15〇〇埃。再對丁上述第二 導電層進行非等向性.银刻,以形成堆疊導電層間隔物 (spacer) 9於上述閘極7之側壁上,藉以和上述閘極7構成 T型閘極結構’如第丨H圖所示。 其中,上述第二導電層之材質係選自複晶矽、矽化金 屬、摻雜複晶矽、鎢、鈷、及鈦金屬之一者,或選自複晶 矽蝕刻後施以自我校準矽化金屬(salicide)程序形成之矽 化金屬,以及與閘極3之界面情形良好之材質者為佳。上 述導電層之蝕刻係使用以鹵素氣體、函素化合物、鹽酸、 含溴化合物之一者、或其混合物,例如Cl2/HBr/SF6之混合 氣體來進行非等向性乾式蝕刻。 步驟九 使用神離子進行離子佈植,形成第二摻雜區1〇於T型 閘極之兩側,作為MOS電晶體之深源/汲極區,如第丨丨圖所 示’如此即完成自我對準T型閘極場效電晶體之製作。 更可繼續以下之步驟十〜十一,以便形成具有空氣間 隙之T型閘極MOSFET.。C: \ Program Files \ Patent \ 0522_3940-E · ptd Page 9, 5, V. Description of Invention (7) '----- --- Part of the upper end of gate 7, as shown in Figure 1F. Step 7 Ion implantation is performed to form a first doped region 8 on the two of the above gates 7: as a source / drain region extension of the MOS transistor, as shown in (). In step 8, a second conductive layer is deposited in advance. The thickness of the gate electrode 7 and the second dielectric layer 3 is between 5000 and 2000 angstroms, and can be adjusted according to actual needs. In this embodiment, the thickness is 1 500. A. The second conductive layer D is anisotropic. Silver is engraved to form a stacked conductive layer spacer 9 on the side wall of the gate electrode 7 to form a T-gate with the gate electrode 7 The structure 'is shown in Figure 丨 H. The material of the second conductive layer is selected from one of polycrystalline silicon, silicided metal, doped polycrystalline silicon, tungsten, cobalt, and titanium, or a compound After the silicon is etched, a silicon silicide formed by a self-calibrating salicide process and a material with a good interface with the gate 3 are preferred. The conductive layer is etched with anisotropic dry etching using a halogen gas, a halide compound, hydrochloric acid, one of the bromine-containing compounds, or a mixture thereof, such as a mixed gas of Cl2 / HBr / SF6. Ions are implanted to form a second doped region 10 on both sides of the T-type gate, which serves as the deep source / drain region of the MOS transistor. Fabrication of gate-type field-effect transistor. The following steps 10 ~ 11 can be continued to form a T-gate MOSFET with air gap.
C:\Program Files\Patent\0522-3940-E.pt(i第 10 頁 402749C: \ Program Files \ Patent \ 0522-3940-E.pt (i page 10 402749
五、發明說明(8) 步驟十 以選擇性蝕刻法去除 以露出T型閘極,且”=逑弟二介電層3 (氮化石夕層), 方,不會有氮化石夕層“ ίϊ疊導電層間隔物9之下 步驟十一 ” 果如第1 J圖所示。 層厚度介於4〇°"_埃之氧化 蓋,在本實施例中Γ氧化;^型閉極完全加以覆 Τ型閘極結構之堆疊導電声曰^度為5500埃。其中於上述 間有空氣邊隙存在。 S 和上述源/汲極區延伸8之 本實施例中,在(步驟八) ( 可以先濕式钱刻法去除上述第甲和u後,亦 (第2A圖;原來之步驟十) u露出T型閘極 /汲極區10(第2B圖;原來 '離子π佈植’卩形成深源 沈積法形成氧化層丨丨於上述半後,以化學氣相 極完全加以覆蓋(第2(:圖)。太:體基材1之上’ @將Τ型閘 跡2C圖所示(第⑻本實施例可變化之流程部分如 實施例二: 如上述第一實施例之方法, 七,如第1G圖所示。 由步驟—至完成上述步驟 步驟八 針對上述閘極7使甩選擇性嗜接、土 , 層丄3於上述閘極7和第二介電層3\積/ 形成堆疊導電 構成Τ型問極結構,如第^圖所述之上’藉以和上述問極7V. Description of the invention (8) Step 10 is removed by selective etching to expose the T-type gate, and "= the second dielectric layer 3 (nitride stone layer), and there will be no nitride stone layer". Step 11 below the stacked conductive layer spacer 9 is shown in FIG. 1J. The layer thickness is between 40 ° " Angstrom oxide cap, in this embodiment, Γ oxidation; The stacked conductive sound structure of the T-type gate structure is 5500 angstroms. There is an air gap between the above. S and the source / drain region extension 8 in this embodiment, in (step eight) (can be After the first money and u are removed by wet coin engraving, (Figure 2A; the original step 10) u exposes the T-gate / drain region 10 (Figure 2B; the original 'ion π implanting') is formed. The deep source deposition method forms an oxide layer. After the above half, it is completely covered with a chemical vapor phase electrode (Part 2 (: Figure). Too: on the bulk substrate 1 '@ 将 Τ 型 开关 迹 2C shown ( The second part of the process that can be changed in this embodiment is as in the second embodiment: as in the method of the first embodiment above, seven, as shown in Figure 1G. From step to completion The step 8 is described as follows: the gate 7 is selectively attracted to the gate 7, and the layer 3 is formed on the gate 7 and the second dielectric layer 3 to form a stacked conductive structure to form a T-type electrode structure, as shown in FIG. The above 'and the above question 7
402749 五、發明說明(9) 要來之度介於埃之間可依需 層之材質係選自複晶;:::ί”]5〇°埃。上述導電 銘、及鈦金屬之一者,以=金屬、摻雜複晶石夕、鶴、 質為佳。 及與閉極3之界面情形良好之材 步驟九 使用坤離子進行離子備始 =極=二作為M〇s電晶體之深源 極場效電晶心 隙之τ型閑極M0SFET。驟十〜十一,以便形成具有空氣間 步驟十 以濕式钱刻法去除上述第二 露出T型閉極,且T型閑極之堆;;(〜化㈣)會二 鼠化石夕層存在,其結果如第3C圖所示。曰3之下方’不會有 步驟十一 以化學氣相沈積法形成厚度介於4000〜7 層11於上述丰導,美;^ 埃之乳化 芸,右太Ϊ 將τ型閘極完全加以覆 1在本實鉍例中,氧化層之厚度為55〇〇埃。豆 τ型閘極結構之堆疊導電層i 3下方和上述源/汲&延 之間有空氣邊隙存在;如第3 D圖所示。、 °° 第二實施例如同第一實施例所述,亦可 第二介電層,之後再使用例如石申離子實 ^ 源/汲極區10。 料實鉍佈植,以形成深 C:\Program Files\Patent\0522-3940-E.ptd第 12 頁 402749 五、發明說明(10) _ 傳統之T型閘極與源/汲極間存 而以本發明製其 $ ^化層等介電質, 隙。由室—氣之介電常數為i小於氧 (約4左、右)’因此本發明製作 二又氧:匕層之介電常數 間之寄生雷交骆备 电日日體,其閘極與源/汲極 之效能表現上較為優異。 斤乂在回速傳輸 綜上所述,依據本發明 電元件,係利用自動對準製 度、並節省成本。此外,所 效之寬度變大,故可以有效 利用空氣邊隙之形成,使閘 降低。 所製作之T型閘極場效電晶體 程’所以可以降低製程之複雜 形成之T型導電閘極,使其等 地降低閘極間之寄生電阻,且 極與源/汲極間之寄生電容值 雖然本發明已以兩個較佳實施例揭露如上,然其並非 用以限定本發明,任何熟悉本項技藝者,在不脫離本發明 之精神和範圍内,當可做些許之更動和潤飾,因此本發明 之保護範圍當視後附之申請專利範圍所界定者為準。402749 V. Description of the invention (9) The material of the on-demand layer that is between Angstrom and Angstrom is selected from the compound crystal; ::: ί "] 50 ° Angstrom. One of the above conductive inscriptions and titanium It is better to use = metal, doped compound spar, crane, and quality. And the interface with the closed electrode 3 is in good condition. Step 9 Use Kun ion for ion preparation. = Pole = 2 as the depth of the M0s transistor. The τ-type idler M0SFET of the source field effect transistor's core gap. Steps ten to eleven, so as to form an air-to-air step, the wet exposed method is used to remove the second exposed T-type closed pole, and the T-type idler (~ 化 ㈣) There will be two rat fossil layers, and the result is shown in Figure 3C. Below 3, there will be no eleven steps to form a layer with a thickness of 4000 ~ 7 by chemical vapor deposition. 11 In the above guide, beauty; ^ Emulsified Yun, right Taiji completely cover the τ-type gate 1 In this example of bismuth, the thickness of the oxide layer is 5500 Angstroms. There is an air gap below the stacked conductive layer i 3 and between the above source / sink &extension; as shown in Figure 3D., ° ° The second embodiment is the same as the first embodiment As described in the example, the second dielectric layer can also be used afterwards, such as Shishen ion source / drain region 10. Material bismuth is implanted to form a deep C: \ Program Files \ Patent \ 0522-3940-E .ptd page 12 402749 V. Description of the invention (10) _ The traditional T-gate and source / drain are interposed, and the present invention is used to make dielectric layers and gaps, such as layers, from the chamber to the gas. The electric constant is smaller than oxygen (about 4 left and right). Therefore, the present invention makes two oxygen: parasitic lightning between the dielectric constants of the dagger layer. The performance of the gate and source / drain The performance is superior. According to the summary of the return speed transmission, according to the electrical component of the present invention, the automatic alignment system is used, and the cost is saved. In addition, the effective width becomes larger, so the air gap can be effectively used. The formation of the T-gate field-effect transistor can reduce the complexity of the T-shaped conductive gate formed in the process, so as to reduce the parasitic resistance between the gate and the electrode / source / Parasitic capacitance value between the drain electrodes Although the present invention has been disclosed above in two preferred embodiments, it is not limited The present invention, any Skilled persons, without departing from the spirit and scope of the present invention, it can still make cover modifications and variations, so as to define the attachment of the scope of the invention when view patent, whichever range.
C:\ProgramFiles\Patent\0522-3940-E.ptd第 13 頁C: \ ProgramFiles \ Patent \ 0522-3940-E.ptd page 13
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW87118214A TW402749B (en) | 1998-11-02 | 1998-11-02 | Field effect transistor with self-aligned T-type gate |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW87118214A TW402749B (en) | 1998-11-02 | 1998-11-02 | Field effect transistor with self-aligned T-type gate |
Publications (1)
Publication Number | Publication Date |
---|---|
TW402749B true TW402749B (en) | 2000-08-21 |
Family
ID=21631858
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
TW87118214A TW402749B (en) | 1998-11-02 | 1998-11-02 | Field effect transistor with self-aligned T-type gate |
Country Status (1)
Country | Link |
---|---|
TW (1) | TW402749B (en) |
-
1998
- 1998-11-02 TW TW87118214A patent/TW402749B/en not_active IP Right Cessation
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US6780694B2 (en) | MOS transistor | |
TWI536462B (en) | Integrated circuits having protruding source and drain regions and methods for forming integrated circuits | |
JP4430669B2 (en) | Method of manufacturing a transistor having an asymmetric conductive spacer | |
TW408424B (en) | Semiconductor device with silicon replacing structure on the insulated layer and the manufacture method thereof | |
JP4299791B2 (en) | Method for fabricating a gate structure of a CMOS device | |
TWI402984B (en) | Self-aligned planar double-gate process by self-aligned oxidation | |
US20070215951A1 (en) | Semiconductor devices having silicided electrodes | |
TW201013758A (en) | Semiconductor device and method for making semiconductor device having metal gate stack | |
JP2003017710A (en) | Double gate/double channel mosfet | |
TW200425519A (en) | Self-aligned isolation double-gate FET | |
US20070187774A1 (en) | Manufacturing method for an integrated semiconductor structure and corresponding integrated semiconductor structure | |
US6403485B1 (en) | Method to form a low parasitic capacitance pseudo-SOI CMOS device | |
US7169676B1 (en) | Semiconductor devices and methods for forming the same including contacting gate to source | |
US20060134874A1 (en) | Manufacture method of MOS semiconductor device having extension and pocket | |
US6225175B1 (en) | Process for defining ultra-thin geometries | |
JP4086099B2 (en) | Method for forming semiconductor device | |
US5970331A (en) | Method of making a plug transistor | |
US6146952A (en) | Semiconductor device having self-aligned asymmetric source/drain regions and method of fabrication thereof | |
JP2005340782A (en) | Semiconductor device and manufacturing method of same | |
US6228729B1 (en) | MOS transistors having raised source and drain and interconnects | |
JP3990858B2 (en) | Semiconductor device | |
US6780691B2 (en) | Method to fabricate elevated source/drain transistor with large area for silicidation | |
TW402749B (en) | Field effect transistor with self-aligned T-type gate | |
JPH09289249A (en) | Fabrication method of semiconductor device | |
JP3680417B2 (en) | Semiconductor device |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
GD4A | Issue of patent certificate for granted invention patent | ||
MM4A | Annulment or lapse of patent due to non-payment of fees |