TW525303B - MOS transistor and method for producing the same - Google Patents
MOS transistor and method for producing the same Download PDFInfo
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- TW525303B TW525303B TW90113682A TW90113682A TW525303B TW 525303 B TW525303 B TW 525303B TW 90113682 A TW90113682 A TW 90113682A TW 90113682 A TW90113682 A TW 90113682A TW 525303 B TW525303 B TW 525303B
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525303 ___案號 90113682_年月日__;_ 五、發明說明(1) 5 - 1發明領域: 本發明係有關於不需要淺接面(s h a 1 1 〇 w j u n c t i ο η )之 金氧半電晶體(metal oxide semiconductor, MOS),同時 也是有關於不需要使用低能量離子佈植程序之MOS的製造 方法。 5 - 2發明背景: M0S的基本構造包含了閘極、源極與汲極。如第一 a圖 所示’閘極1 1係位於底材1 〇上,而源極1 2與汲極1 3係位於 底材1 0内並分別位於閘極1 1相對的兩側。當然,如第一 B 圖所不’源極1 2與〉及極1 3也可以是位於井區14中而不是直 接位於未摻雜之底材1 〇中。 隨著半導體產品之輕薄短小的趨勢,Μ 〇 S的尺寸必須 持續地縮小。若保持整個半導體電晶體所有參數設計不變 僅是等比例的縮小尺寸,當源極丨2與汲極丨3間的距離短到 使得源極1 2之空乏區(^ e ρ 1 e ^丨〇 ^ r e g i ο η )與没極1 3之空乏 11¾生接近甚至重疊時,短通道效應(sh〇rt channel effect)便成為無法避免的問題,而會引發諸如起始電壓 下降、次啟始電流增加、熱電子效應與閘極氧化層退化等 等的缺失。525303 ___Case No. 90113682_year month __; _ V. Description of the invention (1) 5-1 Field of the invention: The present invention relates to a metal-oxygen half which does not require a shallow junction (sha 1 1 〇wjuncti ο η). A transistor (metal oxide semiconductor, MOS) is also a method for manufacturing a MOS that does not require a low-energy ion implantation process. 5-2 Background of the Invention: The basic structure of MOS includes a gate, a source, and a drain. As shown in Fig. 1a, the gate 12 is located on the substrate 10, and the source 12 and the drain 13 are located in the substrate 10 and located on opposite sides of the gate 11 respectively. Of course, as shown in the first B diagram, the source electrodes 12 and> and the electrodes 13 may also be located in the well region 14 instead of directly in the undoped substrate 10. With the trend of thinner, lighter and shorter semiconductor products, the size of MOS must continue to shrink. If the design of all parameters of the entire semiconductor transistor is kept unchanged, it is only a proportional reduction. When the distance between the source 丨 2 and the drain 丨 3 is short enough to make the empty region of the source 12 (^ e ρ 1 e ^ 丨〇 ^ regi ο η) When it is close to or even overlaps with the gap between 11 and 3 of the pole, the short channel effect becomes an unavoidable problem, which will cause the starting voltage to drop, and the secondary starting current. Increases, thermionic effects, and loss of gate oxide degradation.
525303 _案號90113682 年月日 修正 五、發明說明(2) 由於以降低Μ 0 S之操作電壓來解決短通道效應的作法 ,無可避免地必須改變整個半導體元件的配置( conf iguration),成本高且牽連甚廣。因此習知技術通常 是以輕摻雜沒極(lightly doper drain,LDD)來防治短通 道效應。如第一 C圖與第一 d圖所示,在源極1 2面對汲極1 3 的側與/及極1 3面對源極1 2的一側都加入輕摻雜沒極1 5, 藉以改變空乏區的形成與分佈、改變電場的分佈與吸收熱 電子,進而減緩短通道效應。在此,輕摻雜汲極丨5形成了 厚度較源極1 2與沒極1 3之戶$ ϊ / u 1 1 _ 1 1 &与度小的淺接面(sha 1 1 ow junction)° 然論如何 -,« M0S. # V ^ # ^ 極1 5的摻雜程度較輕微合 于稷雜,另一方面輕摻雜汲 昇。而且隨著半導r ^:侍源極1 2到汲極1 3間之電阻上 過程會變得複雜且 < 需==2二寸的縮短,淺接面的形成 以最常用之低能量離子佈 ^心劇增加,不論淺接面是 法所形 <。 子佈才皇程序所形&或是以熱冑散等^ 習知技術對淺接面的 M0S的構造有許多的改/成方式以及具輕摻雜汲極之 輕摻雜區域,因此短 但^於仍使用以淺接面形成 些無法避免的缺失Γ通道效應的防治仍然總是會伴隨成著之_525303 _Case No. 90113682 Rev. V. Description of the invention (2) Due to the method of reducing the short-circuit effect by reducing the operating voltage of MOS, it is inevitable that the configuration of the entire semiconductor device must be changed (configuration), cost Tall and implicated. Therefore, conventional techniques usually use lightly doper drain (LDD) to prevent short channel effects. As shown in FIG. 1C and FIG. 1d, a lightly doped electrode 1 5 is added to the side of the source 12 facing the drain 1 3 and / or the side of the electrode 13 facing the source 12. In order to change the formation and distribution of the empty region, change the distribution of the electric field and absorb hot electrons, and then slow down the short channel effect. Here, the lightly doped drain 丨 5 forms a thicker layer than the source 12 and the electrode 1 3 ϊ / u 1 1 _ 1 1 & shallow junction (sha 1 1 ow junction) ° Of course, «M0S. # V ^ # ^ The degree of doping of pole 1 is slightly more doped, and lightly doped, on the other hand. And with the semiconducting r ^: the process of the resistance between the source 12 to the drain 13 will become complicated and < needs to be shortened by 2 = 2 inches, the formation of shallow junctions with the most commonly used low energy Ionic cloth ^ increase in drama, no matter the shallow interface is shaped by law <. The Zibucaihuang program is shaped by & thermal diffusion, etc. ^ The conventional technique has many modifications / changes to the structure of the shallow junction M0S and a lightly doped region with a lightly doped drain, so it is short. But ^ Yu still uses the shallow junction to form some unavoidable missing Γ channel effects. Prevention and control will always accompany the work.
525303 _案號90Π3682_年月日 修正 五、發明說明(3) 5 - 3發明目的及概述: 本發明之一主要目的為提出可以有效防治短通道效應 之M0S及其形成方法。 本發明的另一主要目的是提出不需要使用以淺接面形 成之輕摻雜汲極的M0S及其形成方法。 植 佈 子 As· 旦里 能 低 用 使 要 需 不 出 提 含 〇 J法 的方 J造 製 明S 〇 發Μ 本之 序 程 Μ 極 汲 種與 一極 為源 例、 施層 實雜 佳摻 較二 一第 之、 明層 發雜 本摻- 第 括 包 少 至 、材 極底 閘於 ••位 係 極 閘 摻於 一位 第係 , 層 方雜 下摻 的二 極第 間 ·, 於度 位濃 並雜 中摻 材一 底第 於與 位性 係電 層導 雜一 摻第 一有 第具 ; 上雜 下 的 層 AF 摻 1 第 於摻 大一 度第 濃到 雜觸 掺接 二接 第直性 ,並電 度側導 濃一二 雜的第 摻極有 二閘具 第於極 與位源 性極, 電源層 導·,雜 一度摻 第濃二 有雜第 具摻與 並一層 方第雜 到 觸 接 接 直 極。 汲性 , 電 極導 汲二 之第 侧有 二具 對並 相層 極雜 閘摻 於二 位第 極與 源層 與雜 及摻 以一 •,第 至 法 方 的 S 〇 Μ 成 形 種- 為 例 施 實 佳 較 一 另 的 明 發 本525303 _Case No. 90Π3682_ Year, Month, Day, and Amendment V. Description of the Invention (3) 5-3 Purpose and Summary of the Invention: One of the main purposes of the present invention is to propose a MOS that can effectively prevent and control the short channel effect and its forming method. Another main object of the present invention is to propose a MOS that does not require the use of a lightly doped drain formed with a shallow junction and a method of forming the same. As · Once implanted in the sub-cloth can be so low with no need to provide the J-containing side 〇J manufacturing method of square hair Μ S made out of sequence present process Μ drain electrode species and a source of extremely embodiment, application layer doped solid heteroaryl good Compared with the 21st, the mixed layer of the bright layer is mixed-the first includes the pole gate gate in the •• position system gate gate is mixed in the first phase system, and the layer electrode is mixed in the second electrode phase. In the degree of concentration, the dopants in the dopant are mixed first with the dopant of the paraelectric system. The doped layer is the first; the upper layer is doped with AF. Straightness, and the second dopant electrode with two side gates has two gates and the source source, the power source is conductive, and the first dopant is doped with the second and second gates. The first miscellaneous contact is straight. Absorptive, there are two pairs of parallel phase layer gates on the second side of the electrode guide, which are doped in the second position and the source layer and doped with one •, the first to the French S 〇 种 shaped species-as an example Shi Shijia compares with another Mingfa
第6頁 525303 五 、發明說明 ΛΜ 90113682 (4) Λ_3. 曰 修正 緊臨到第一摻雜層,第一換:位於第1雜 摻雜濃::並且第二摻雜層的摻雜濃度又ϊη:層的 比大认ί以形成源極與汲極在底材中,ί罩幕對材進行 白;第一摻雜層的厚度。一 /'、極與汲極的厚度 上 =沐這些實施例可以進一步包 亚且兩個摻雜層的寬度係與閘極;目上:在閘極之側壁 I R 田 0 的形Ϊ:Ϊ ί ”:成過程一定比厚度較大之源極與汲極 前述問i因此t發從另一個角度來解決 ?是否二执/口丑、L效應疋否一疋需要使用輕摻雜沒極 • 犯夠不使用輕摻雜汲極也不改變操作電壓,#沪右 效地防治短通道效應? 便此有 由於論文(IEEE Electron Device Letters, V〇i. 20, No· 2, ρ·95, Feb 1 9 9 9 )有提到對具有陡峭變化井區 (super steep retrograde well)之 MOS而言,當等效通道 長度大致相等時短通道效應基本上與接面厚度無關。本發Page 6 525303 V. Description of the invention ΛΜ 90113682 (4) Λ_3. The correction is close to the first doped layer, the first change: located at the first doped concentration :: and the doped concentration of the second doped layer is ϊη : The ratio of the layers is large to form the source and the drain in the substrate, and the mask is whitened; the thickness of the first doped layer. The thickness of the electrode and the drain electrode = these embodiments can be further included and the width of the two doped layers is related to the gate; for the purpose: the shape of the IR field 0 on the side wall of the gate: Ϊ ί ”: The formation process must be greater than the source and drain electrodes with a larger thickness. Therefore, the above problem should be solved from another angle? Is it the second implementation / ugliness, the L effect? Does it require the use of lightly doped electrodes? Do not use lightly doped drain and do not change the operating voltage, # Shanghai right to effectively prevent short channel effects? This is due to the paper (IEEE Electron Device Letters, V〇i. 20, No · 2, ρ · 95, Feb 1 9 9 9) It is mentioned that for MOS with super steep retrograde well, when the equivalent channel length is approximately equal, the short channel effect is basically independent of the interface thickness.
第7頁 525303 _案號90113682_年月曰 修正_ i、發明說明(5) 明的發明人進一步推導此概念而指出,當等效通道長度可 以有效地控制與固定時,使用陡峭變化井區可以使短通道 效應的防治並不需要使用淺接面或改變操作電壓。進一步 地,本發明之發明人指出由於源極與汲極各自之空乏區的 擴張與接觸會引發短通道效應,因此可以使用位於源極與 汲極間之陡峭變化井區來控制源極與汲極間之空乏區的分 佈,進而取代未使用陡峨變化井區之M0S中輕摻雜没極的 功能。換句話說,可以用陡峭變化井區取代以淺接面形成 之輕摻雜汲極,進而避免淺接面形成過程的困難。 為具體實踐上述之以陡峭變化井區取代以淺接面形成 之輕摻雜沒極的概念,本發明之一較佳實施例為一種使用 陡峭變化井區之M0S,如第二A圖與第二B圖所示,至少包 括:閘極2卜第一摻雜層2 2、第二摻雜層2 3、源極2 4與汲 極2 5。 閘極2 1係位於底材2 0上,並且尚可包含間隙壁在閘極 21的侧壁上。 第一摻雜層22係位於底材20中並位於閘極21的下方, 第一摻雜層2 2具有第一導電性與第一掺雜濃度,並且第一 摻雜層2 2通常係緊臨到底材2 0之表面。 第二摻雜層2 3係位於第一摻雜層2 2的下方並具有第二Page 7 525303 _Case No. 90113682_ Modification of the month of the year _ i. Description of the invention (5) The inventor of the invention further deduced this concept and pointed out that when the equivalent channel length can be effectively controlled and fixed, use a steeply varying well area The prevention of short channel effects can be achieved without using shallow junctions or changing the operating voltage. Further, the inventor of the present invention pointed out that because the expansion and contact between the empty regions of the source and the drain will cause a short channel effect, a steeply varying well region between the source and the drain can be used to control the source and the The distribution of the empty regions between the drain electrodes further replaces the function of lightly doped non-electrodes in the MOS that do not use the steeply-elevated well area. In other words, a steeply varying well region can be used instead of a lightly doped drain formed with a shallow junction, thereby avoiding the difficulty of forming the shallow junction. In order to specifically implement the above-mentioned concept of replacing the lightly doped non-polar electrode formed by a shallow junction with a steeply varying well area, a preferred embodiment of the present invention is a MOS using a steeply varying well area, as shown in Figure A and Figure 2 As shown in FIG. 2B, at least: a gate electrode 2, a first doped layer 2 2, a second doped layer 2 3, a source electrode 24, and a drain electrode 25. The gate electrode 21 is located on the substrate 20, and may further include a gap wall on the side wall of the gate electrode 21. The first doped layer 22 is located in the substrate 20 and below the gate electrode 21. The first doped layer 22 has a first conductivity and a first doping concentration, and the first doped layer 22 is usually fastened. Facing the surface of the base material 20. The second doped layer 2 3 is located below the first doped layer 2 2 and has a second
525303 _案號90113682_年月日_^_ 五、發明說明(6) 導電性與第二摻雜濃度,第二摻雜濃度大於第一摻雜濃度 。在此第一導電性與第二導電性通常是相同的,而第一摻 雜層2 2的寬度與第二摻雜層2 3的寬度通常與閘極2 1的寬度 大致相等。 源極2 4位於底材2 0内並位於閘極2 1的一側,源極2 4直 接接觸到第一摻雜層2 2與第二摻雜層2 3,源極2 4具有第二 導電性。 没極2 5係與源極2 4位於閘極2 1相對之二侧,沒極2 5直 接接觸到第一摻雜層2 2與第二摻雜層2 3並具有第二導電性 。源極2 4與汲極2 5的厚度通常皆大於第一摻雜層2 2的厚度 ,並且第一摻雜層2 2與源極2 4之界面與第一摻雜層2 2與汲 極2 5之界面的輪廓可以為與底材2 0之表面幾乎垂直之直線 也可以為彎曲的線段,基本上係取決於源極2 4與汲極2 5的 形成過程,本發明並不受限於此細節。 顯然地,藉由比較第二A圖至第二D圖以及第一 A圖與 第一 D圖,可以看出本實施例的一大特徵是源極與没極之 間並沒有輕摻雜汲極,而另一大特徵是在閘極下方與源極 及汲極之間不是單一摻雜濃度的井區或底材,而是同時存 在濃度不同之第一摻雜層2 2與第二摻雜層2 3。在此,第二 摻雜濃度與第一摻雜濃度的差距,必須大到使得當位於閘 極2 1下方之第一摻雜層2 2被閘極之電壓(操作電壓)反轉而525303 _Case No. 90113682_Year Month Day _ ^ _ V. Description of the Invention (6) Electrical conductivity and second doping concentration, the second doping concentration is greater than the first doping concentration. Here, the first conductivity and the second conductivity are generally the same, and the width of the first doped layer 22 and the width of the second doped layer 23 are generally approximately the same as the width of the gate electrode 21. The source electrode 24 is located in the substrate 20 and on one side of the gate electrode 21. The source electrode 24 is directly in contact with the first doped layer 22 and the second doped layer 23, and the source electrode 24 has a second Conductivity. The pole electrode 2 5 and the source electrode 24 are located on opposite sides of the gate electrode 21, and the pole electrode 2 5 is in direct contact with the first doped layer 22 and the second doped layer 23 and has a second conductivity. The thicknesses of the source 24 and the drain 25 are generally larger than those of the first doped layer 22, and the interface between the first doped layer 2 2 and the source 24 and the first doped layer 22 and the drain The contour of the interface of 25 can be a straight line that is almost perpendicular to the surface of the substrate 20 or a curved line segment, which basically depends on the formation process of the source 24 and the drain 25, and the present invention is not limited. In this detail. Obviously, by comparing the second A-picture to the second D-picture and the first A-picture and the first D-picture, it can be seen that a major feature of this embodiment is that there is no lightly doped drain between the source and the non-electrode. Another major feature is that there is not a well region or substrate with a single doping concentration under the gate and between the source and the drain, but there are a first doped layer 22 and a second doped layer with different concentrations at the same time. Miscellaneous layers 2 3. Here, the difference between the second doping concentration and the first doping concentration must be so large that when the first doping layer 22 below the gate 21 is reversed by the gate voltage (operating voltage),
525303 年 修正 月 曰 案號 90113682 五、發明說明(7) 形成連接源極24與汲極25之通道(channel>^,第二摻雜 層2 3並不會被反轉。 一第三A圖與第三B圖顯示了使用陡峭變化井區之M0S中 短通道效應的變化。第三A圖顯示此類使用陡峭變化井區 之M〇2的基本架構’在此第一摻雜層2 2的厚度被設定為2 〇 〇 埃,第一摻雜濃度為lx l〇i6/cm^第二摻雜濃度為5χ 1〇 1S /cm3’模擬的變數是源極24與汲極25的厚度,在此分別模 擬了 0.06um、0.12Um和0.18_三種厚度,並計算等效通道 長度與起始電壓間的關係。 第二B圖顯不了模擬的結果,很明顯地,除了短通道 效應所引發之當等效通道長度過短時起始電壓會下降外, =同源極2 4 /沒極2 5厚度所引發的短通道效應幾乎完全一 j:樣。⑨句話說’使用本實施例,不只不需用使用以淺 ,面所形成之輕摻雜汲極,而且源極24與汲極25的厚度也 I以任意的調整變厚’並不需要隨著半導體元件之臨界尺 =縮短,而減少源極24與汲極25的厚度或甚至使用 形成源,24與汲極25。也因此,源極24與汲極 成過程可以簡化,並不需要使用低能量離子佈植程序。 ^然’本貫施例雖不需要使用輕摻雜沒極,但如第二 1圖<與第二F圖所示之例子,本實施例仍可以進一步地包含 摻雜袋27 ( implantation pocket)來增強本實施例防治短 通道效應的Revised 525303 Case No. 90113682 V. Description of the invention (7) Forming a channel connecting the source 24 and the drain 25 (channel) ^, the second doped layer 23 will not be reversed. A third A picture Figure 3 and Figure B show the change in short channel effects in MOS using steeply varying wells. Figure 3 A shows the basic architecture of this type of MO using steeply varying wells' here the first doped layer 2 2 The thickness is set to 2000 angstroms, the first doping concentration is lx l0i6 / cm ^, and the second doping concentration is 5x10S / cm3. The simulated variable is the thickness of the source 24 and the drain 25, Three thicknesses of 0.06um, 0.12Um, and 0.18_ are simulated here, and the relationship between the equivalent channel length and the starting voltage is calculated. Figure 2B does not show the results of the simulation. Obviously, except for the short channel effect When the equivalent channel length is too short, the starting voltage will decrease, and the short-channel effect caused by the thickness of the homologous pole 2 4 / not pole 25 will be almost exactly the same. Say, 'Using this embodiment, Not only do you need to use lightly doped drains formed on the surface, but also the thickness of the source 24 and drain 25 I thicken with an arbitrary adjustment 'does not need to reduce the thickness of the source 24 and the drain 25 or even use the source 24 and the drain 25 as the critical dimension of the semiconductor element is shortened. Therefore, the source 24 The formation process with the drain electrode can be simplified, and it is not necessary to use a low-energy ion implantation procedure. ^ However, although this embodiment does not require the use of a lightly doped electrode, as shown in Figure 2 < and Figure 2 F As shown in the example, this embodiment may further include an implantation pocket 27 (implantation pocket) to enhance the prevention and control of the short channel effect of this embodiment.
第10頁 525303 _案號90113682_年月日__ 玉、發明說明(8) 能力。但必須強調的是摻雜袋的細節如輪廓與濃度等並不 是本實施例的重點。 本發明的另一較佳實施例為一種形成MOS的方法,特 別是形成使用陡峭變化井區之MOS的方法,如第四A圖所示 ,至少包含下列步驟: 如底材方塊4 1所示,提供具有第一摻雜層與第二摻雜 層的底材,第一摻雜層係緊鄰到底材表面,而第二摻雜層 係位於第一摻雜層下方並緊臨到第一掺雜層,第一摻雜層 與第二摻雜層的電性相同,並且第二摻雜層的摻雜濃度大 於第一摻雜層的摻雜濃度。在此第一摻雜層與第二摻雜層 是的形成過程並不是本實施例的重點,本實施例亦不受限 於此。 如閘極方塊4 2所示,形成閘極在底材上。 如摻雜方塊4 3所示,以閘極為罩幕對底材進行摻雜程 序以形成源極與汲極在底材中,源極與汲極的厚度皆大於 第,一摻雜層的厚度。 當然,由於間隙壁可以用來保護閘極側壁與改變源極 與汲極之間的距離,本實施例也可以修改為如第四B圖所 示之情形。Page 10 525303 _Case No. 90113682_Year Month and Day__ Jade, description of invention (8) Ability. It must be emphasized that the details of the doping bag, such as the profile and concentration, are not the focus of this embodiment. Another preferred embodiment of the present invention is a method for forming a MOS, especially a method for forming a MOS using a steeply varying well area. As shown in FIG. 4A, at least the following steps are included: As shown in the substrate block 41 A substrate with a first doped layer and a second doped layer is provided. The first doped layer is immediately adjacent to the surface of the substrate, and the second doped layer is located below the first doped layer and immediately adjacent to the first doped layer. Layer, the first doped layer has the same electrical properties as the second doped layer, and the doped concentration of the second doped layer is greater than the doped concentration of the first doped layer. The formation process of the first doped layer and the second doped layer is not the focus of this embodiment, and the embodiment is not limited thereto. As shown in the gate block 42, the gate is formed on the substrate. As shown in the doping block 4 3, the substrate is doped with a gate electrode mask to form a source and a drain. In the substrate, the thickness of the source and the drain is greater than that of the first and the thickness of a doped layer. . Of course, since the gap wall can be used to protect the gate sidewall and change the distance between the source and the drain, this embodiment can also be modified to the situation shown in Figure 4B.
525303525303
叫乐一修雜 一摻雜層,第一株 =雜層的摻雜濃度 一払$層與第二摻雜 ’本貫施例亦不受限 如底材方塊4 1所示,提供具有 層的底材,第一摻雜層係緊鄰到底 係位於第一摻雜層下方並緊臨到第 與第二摻雜層的電性相同,並且第 於第/摻雜層的摻雜濃度。在此第 的形成過程並不是本實施例的重點 此0 如閘極方塊4 2所示,形成閘極在底材上。 如間隙壁方塊44所示,形成間隙壁在閘極之側壁。 如接雜方塊43所示,以閘極與間隙壁為罩幕對底材進 行摻雜程序以形成源極與汲極在底材中,源極與汲極 度皆大於第一摻雜層的厚度。 子 以上所述僅為本發明之較佳實施例而已,並非用以限 定本發明之申請專利範圍;凡其它未脫離本發明所揭示之 精神下所完成之等效改變或修飾,均應包含在下述之申請 專利範圍中。 °It is called Leyi repairing a doped layer, the first strain = the doping concentration of the doped layer, the first layer and the second doping layer. This embodiment is also not limited. For the substrate, the first doped layer is located immediately below the first doped layer and immediately adjacent to the second and second doped layers, and has the same doping concentration as the first / doped layer. The formation process here is not the focus of this embodiment. As shown in the gate block 42, the gate is formed on the substrate. As shown by the spacer wall block 44, a spacer wall is formed on the side wall of the gate. As shown in block 43, the gate and the spacer are used as a mask to perform a doping process on the substrate to form a source and a drain. In the substrate, the source and the drain are both larger than the thickness of the first doped layer. . The above description is only a preferred embodiment of the present invention, and is not intended to limit the scope of patent application for the present invention; all other equivalent changes or modifications made without departing from the spirit disclosed by the present invention shall be included in the following Within the scope of the patent application. °
525303 _案號90113682_年月曰 修正_ 圖式簡單說明 第一 A圖至第一 D圖為習知之使用與未使用輕摻雜汲極 之M0S的基本構造: 第二A圖至第二F圖為本發明之一較佳實施例之幾種可 能橫截面示意圖; 第三A圖與第三B圖為本發明之一模擬例子的示意圖; 以及 第四A圖與第四B圖為本發明之另一較佳實施例的基本 流程圖。 主要部分之代表符號: 10 底材 11 閘極 12 源極 13 汲極 14 井區 15 輕摻雜没極 20 底材 21 閘極 22 第一掺雜層 23 第二摻雜層 24 源極 25 汲極525303 _Case No. 90113682_ Year Month Revised _ The diagrams briefly illustrate the first A to D diagrams are the basic structure of the MOS with the conventional use and without using lightly doped drains: the second A to the second F Figures are schematic diagrams of several possible cross-sections of a preferred embodiment of the present invention; Figures A and B are schematic diagrams of a simulation example of the present invention; and Figures A and B are the present invention A basic flowchart of another preferred embodiment. Representative symbols of the main parts: 10 substrate 11 gate 12 source 13 drain 14 well region 15 lightly doped electrode 20 substrate 21 gate 22 first doped layer 23 second doped layer 24 source 25 drain pole
筹 第13頁 525303 案號90113682 年月日 修正Prepared Page 13 525303 Case No. 90113682 Revised
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