TW454249B - Manufacturing method to form lightly doped region and heavily doped region of source/drain on transistor simultaneously - Google Patents
Manufacturing method to form lightly doped region and heavily doped region of source/drain on transistor simultaneously Download PDFInfo
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- TW454249B TW454249B TW88111583A TW88111583A TW454249B TW 454249 B TW454249 B TW 454249B TW 88111583 A TW88111583 A TW 88111583A TW 88111583 A TW88111583 A TW 88111583A TW 454249 B TW454249 B TW 454249B
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454g;49 7 五、發明說明(1) 法’ = 種=導體積體電路元件之製造方 摻雜=卩輕微摻;^淡 件數量不斷增加,電路之發展,日日日片中所含之元 來越小;以MOS電晶體^件之/寸也隨積集度之上升而越 之長度將隨之縮短,因兀/日越辨小’通道(Channel) 是,當_電晶體之通:上快了電晶體之操作速度。但 變,通道内之户6 長度縮短,若施加之電壓大小不 ie Α β & & &只σ電場將增加’這會使通道内的電子因電 \ . b、量上升,遂產生熱載子效應(h〇t carrier* (eCt ,以隨⑽電晶體為例,通道接近汲極區域之載子 工arrier)數目將上升,部分因載子數目增加而產生之電 則1¾入(trap)閘氧化層(gate 〇xide 内並破壞 之,因此影響元件之工作性能(perf〇rmance)。 為了抑制因通道縮短而產生之熱載子效應,目前有一 種廣為採用之解決方法’亦即於原來的M〇s電晶體之源極 與没極接近通道處’再增加一組摻雜程度較原來的源/汲 極為低的域稱之為”淡換雜的没極"(lightly doped drain) ’簡稱為LDD。在具有LDD之設計下,電場之大小將 較無LDD δ又§1*之M0S電晶體為低,因而減輕了熱載子效應。 然而’由於此種含LDD之源/汲極之製作必須透過兩次 的離子植入步驟’因此會使得㈣^電晶體之製程變得複 雜’且需要更多的時間來完成其製造,因而影響其生產速 率。454g; 49 7 V. Description of the invention (1) Method '= species = doped volume circuit element manufacturing method doping = 卩 slight doping; ^ The number of thin parts is increasing, the development of circuits, the daily The smaller the element is, the longer the size of the MOS transistor will increase with the increase of the accumulation degree. The smaller the channel is, the smaller the channel is. When the transistor is : Faster operation of the transistor. However, the length of the household 6 in the channel is shortened. If the magnitude of the applied voltage is not Α β & & & only the σ electric field will increase ', which will cause the electrons in the channel to generate heat due to electricity. The number of carrier effects (hOt carrier * (eCt), with the example of a tritium crystal, the number of carrier arriers in the channel close to the drain region) will rise, and some of the electricity generated by the increase in the number of carriers will be trapped (trap ) The gate oxide layer (which is inside gate 〇xide and destroys it, thus affecting the performance of the device (perfommance). In order to suppress the thermal carrier effect due to the shortening of the channel, there is currently a widely used solution ', that is, Adding a set of domains with a lower level of doping than the original source / drain extremely near the source and dead pole of the original Mos transistor is called "lightly doped" "Drain" is abbreviated as LDD. Under the design with LDD, the size of the electric field will be lower than that of the M0S transistor without LDD δ and §1 *, thus reducing the hot carrier effect. However, because of this source containing LDD The fabrication of the drain / drain must go through two ion implantation steps' Therefore, the process of the transistor is complicated, and it takes more time to complete its manufacture, which affects its production rate.
第4頁 454多49Page 4 454 and 49
五、發明說明(2) 法以:將舉習知之含LDD之源/汲極之CM〇s電晶體之製作 :石…針對問題而加以杳"斤;請參看第1八圖,係於-P 夕^板10上形成有數個場氧化層F〇x,用以隔離出主動V. Description of the invention (2) The method is: the production of a conventional CMOS transistor with a source / drain containing LDD: stone ... to solve the problem "jin; please refer to Figure 18 for the Several field oxide layers F0x are formed on the P-plate 10 to isolate the active
貝^場开』氧化層F〇X所隔離出之石夕基板1〇中之部分主動區 型離子而形成„N井區12,且於井區12 板1 〇 J面及該P㈣基板i 〇表面則分別形 :,其皆由閉氧化層,如二氧化石…、閑電極 PSome active-area ions in the Shixi substrate 10 isolated by the oxidized layer FOX are formed in the “N well area 12”, and on the 10 area of the plate 12 of the well area and the P㈣ substrate i 〇 The surfaces are respectively shaped, which are all made of a closed oxide layer, such as stone dioxide ..., the free electrode P
Is所:^用以降低金屬間極阻值之金屬破化物,如例 制下Ϊ下I,請參考第1,係於該閘極結構GP、Gn之兩 i L 板1G中形成LDD,如圖所示者係為於N井區中Is: ^ metal broken compounds used to reduce the intermetallic pole resistance value, such as the following I, for example, please refer to the first, is formed in the gate structure GP, Gn two i L plate 1G, such as The one shown in the figure is in the N well area
形成P型之淡摻雜區p-,且於p】 I 摻雜區N-。 且於P型石夕基板10内形成N型之淡A p-type lightly doped region p- is formed, and a p] I doped region N-. And an N-type light is formed in the P-type Shixi substrate 10
=’依據第以圖之圖示,在此二問極結構GP、GK 土上刀別形成絕緣側壁層i6p、i 6n,再以此閘極結構 P、Gn與絕緣側壁層丨6p v丨6n為罩幕,分別植入p型、N型 離子至該N井區12與P型石夕基板1〇中,以形成如第1]}圖所示 炎推雜區Π.與濃推雜之P+、N+區域之源/汲極的 CMOS電晶體。 但是,如上所述之習知之具有LDD之CM0S電晶體製程 由於兩階段性的離子植入’因此在其製程步驟上需要花費 更多時間;而為了抑制熱載子效應,LDD之形成又是重要 且不可或缺的。 有鑑於此,本發明之主要目的在於提供一種同時形成= 'According to the diagram in the first figure, the insulating sidewall layers i6p, i 6n are formed on the two interrogation structures GP and GK soil, and then the gate structures P, Gn and the insulating sidewall layers 6p v 6n For the mask, p-type and N-type ions are implanted into the N-well region 12 and the P-type stone substrate 10 respectively to form the inflammatory region Π as shown in Fig. 1) and the concentrated region. CMOS transistor with source / drain in P + and N + regions. However, the conventional CM0S transistor process with LDD as described above requires more time in its process steps due to the two-stage ion implantation; and in order to suppress the hot carrier effect, the formation of LDD is important. And indispensable. In view of this, the main object of the present invention is to provide a simultaneous formation
4 5 4^4 9 五、發明說明(3) 極阻之/摻雜區與遭摻雜區的方法,其藉由 度之先阻層之阻擋,而於 的万凌具错由__特定厚 電晶體之淡摻雜區與濃步η入離子以同時形成 應,更能減少製程步驟,可抑制熱載子效 為了達到本發明之主=於大$生產。 電晶體之源/汲極之淡#的,逐提供—種同時形成一 方法,包括+ 區域(LDD)與濃摻雜區域之製造 基板上形成H + ¥體基板’且於該半導體 體基板上。接著對此光阻層使覆蓋於此閑極與半導 程,以於間部分進行!光及顯影製 声;备始4* 、 壁形成一具有特疋厚度之光阻 ^阻芦下方=離子至該閘極兩側之半導體基板中,以於 (LDd/,廿之’導體基板中形成源/汲極之淡摻雜區域 1 /、,、且於未被該光阻層所覆蓋之半導體基板中形成 源/汲極之濃摻雜區域。 伋〒办玖 一 了達到本發明之主要目的,係提供另—種同時形成 &晶體之源/汲極之淡摻雜區域(LDD)與濃摻雜區域之製 二=法,包括下列步驟:提供—半導體基板’且於該半導 土板上形成一閘極;形成一光阻層使覆蓋於此閘極與半 體基板上。接著對此光阻層之一部分進行曝光,以於閘 極,側壁形成一具有特定厚度之光阻層;最後,植入離子 至該閘極兩側之半導體基板中,以於光阻層下方之半導體 基板中形成源/汲極之淡摻雜區域(LDD ),並且於未被該光 阻層所覆蓋之半導體基板中形成源/汲極之濃摻雜區域。 為讓本發明之上述目的、特徵、和優點能更明顯易4 5 4 ^ 4 9 V. Description of the invention (3) The method of the extremely resistive / doped region and the doped region, which is blocked by the first resistance layer, and Wan Ling has the wrong reason. The lightly doped region of the thick transistor and the concentrated step η are used to form ions at the same time, which can further reduce the process steps, and can suppress the hot carrier effect. The source of the transistor / 极 极 之 淡 # is provided one by one-a method for simultaneously forming, including forming a H + ¥ bulk substrate on a manufacturing substrate of a + region (LDD) and a heavily doped region, and on the semiconductor substrate . Then cover this photoresist layer with this free electrode and semiconductor, so as to do it in between! Light and developing sound; 4 *, the wall forms a photoresistor with a special thickness ^ the bottom of the barrier = ions into the semiconductor substrate on both sides of the gate, in (LDd /, 廿 之 'conductor substrate A lightly doped region 1 / of the source / drain is formed, and a heavily doped region of the source / drain is formed in a semiconductor substrate that is not covered by the photoresist layer. The main purpose is to provide another method for simultaneously forming a & crystal source / drain lightly doped region (LDD) and a heavily doped region = 2 method, including the following steps: provide-a semiconductor substrate 'and A gate is formed on the earth guide plate; a photoresist layer is formed so as to cover the gate and the half-body substrate. Then a part of this photoresist layer is exposed to form a light with a specific thickness on the gate and the sidewall. Finally, ions are implanted into the semiconductor substrate on both sides of the gate to form a lightly doped region (LDD) of the source / drain in the semiconductor substrate below the photoresist layer, and the photoresist is not exposed to the photoresist. A heavily doped region of the source / drain is formed in the semiconductor substrate covered by the layer. The above object of the present invention, features, and advantages can be more easily
第6頁 4 5 4 9 ΎPage 6 4 5 4 9 Ύ
’:如;文特舉—較佳實施例,1配合所附圖式’作詳細說 圖式之簡單說明: 第1A〜1D圖顯示習知之具有ldd結構之CM〇s電晶體之流 程剖面圖;以及 第2 A〜2 J圖顯示依據本發明之同時形成源/汲極之淡摻 雜區域(LDD)與濃摻雜區域之流程剖面圖。 符號說明 1 〇矽基板 1 3二氧化矽 1 5矽化鎢 F Ο X場氧化層 16ρ、16η絕緣侧壁層 20矽基板 ^ 2 2二氧化矽 24矽化鎢': Such as; Wen Teju-preferred embodiment, 1 with the attached drawings' for a brief description of the drawings in detail: Figures 1A to 1D show a cross-sectional view of a conventional CMOS transistor with an ldd structure And FIGS. 2A to 2J show cross-sectional views of a process for simultaneously forming a lightly doped region (LDD) and a heavily doped region of a source / drain in accordance with the present invention. Explanation of symbols 1 〇 silicon substrate 1 3 silicon dioxide 1 5 tungsten silicide F 〇 X-field oxide layer 16ρ, 16η insulating sidewall layer 20 silicon substrate ^ 2 2 silicon dioxide 24 tungsten silicide
El、Ε2 電子束(E —beam) 29a 、 29b 開口 Ml、M2金屬检 實施例 12 N型井區 1 4複晶碎El, Ε2 Electron beam (E-beam) 29a, 29b opening Ml, M2 metal inspection Example 12 N-type well area
Gp、Gn閘極結構 P-、N-淡摻雜區域(LDD) P+、N+濃掺雜區域 21 N型井區 2 3複晶碎 25、25a、27、27a 光阻層 2 6、2 8 凹口 29 、 3〇 BPSG 層Gp, Gn gate structure P-, N- lightly doped region (LDD) P +, N + heavily doped region 21 N-type well region 2 3 polycrystalline broken 25, 25a, 27, 27a photoresist layer 2 6, 2 8 Notch 29, 30BPSG layer
參圖:係提供一半導體基板,例如是P型与 ^元件在软苴=形成有隔離用之場氣化層F0X,以界突 出疋件在矽基板20之主動區a與B ;而 利用單井製程來形成互補式金氧半導例中Refer to the figure: a semiconductor substrate is provided, for example, a P-type element is formed on the soft substrate = a field gasification layer F0X for isolation is formed to protrude the substrate in the active areas a and B of the silicon substrate 20; Well process to form complementary metal-oxide semiconductors
第7頁 五、發明說明(5) - (Complementary Metal Oxide Semiconductor Transistor) ’簡稱為CMOS電晶體,因此先在該p型;5夕基板 20之部分主動區B内形成一井區’例如是N型井區21,且在 該P型矽基板2 0與N型井區21之表面並依序形成一閘氧化 層’如二氧化矽層22、一閘電極,如複晶矽層23以及一用 以降低閘極阻值之金屬石夕化物層,如石夕化鶴層2 4。 之後,要於該半導體基板之表面形成一閘極結構;例 如’依據第2B圖之圖示,係利用光學微影術 (photolithography)及蝕刻製程(etching),以定義出間 極結構之圖案;於此實施例中,位於N型井區21上方之^ ( 極結構標號係為Gp ’而位於p型矽基板2〇表面之閘極結構 標號則為Gn。 ° 接下來要進行之步驟係為形成一光阻層使覆蓋於該閑 極與該半導體基板上;在此,請先參照第2C圖,係塗佈 (coating) —層光阻層25於該矽基板2〇之表面,其厚度約 在1 0000〜1 2000埃之間;接下來,要對該部分之光阻層進 行曝光及顯影製程以於該閘極結構之頂部 側壁上)形成-具有特定厚度之光阻層;如第2:圖(;=其 係以月b里強度為E2之電子束(E-beam)掃射閘極Gn及周圍所 在區域之光阻層25,並以能量強度為£1之電子束掃射閘極^ Gn及周圍以外之主動區A上之光阻層25使其曝光,而在n井 區^之光阻層則未予以曝光;在此應注意兩點,其一為: 使光阻層25曝光之方式尚可利用雷射光(laser)或是χ光 (X-ray)掃射而成;另3點必須特慕注意都 A § 44 3 發明說明⑹ ' ^ " 係丸於E 2 5 ’且E 2所照射之脅雷勢翁哪極:結構如^ 之主動區A土之光阻層、範圍,由於翁量強度之差異,該光 阻層25在經曝光及顯影製程之後,係於閉極結構以之頂部 及侧邊形成如第2D圖所示之光阻層pR1與一凹口26,其厚 度約在3 0 0 0〜400 0埃之間;或者以之能量強度更加強些, 因此於閘極結構Gn之頂部及其側邊曝光較多,於是在經顯 衫之後’遂形成了如第2E圖所示之光阻層?1^2與一凹口 26 ’其厚度約在1〇〇〜500埃之間。 然後,請同時參看第2D、2£:圖,利用光阻層25a與 PR1(或是PR2)為罩幕,以! xl〇15巧 χ1〇15 at〇ms/cm2 間之( 離子濃度植入離子,例如是砷離子至該矽基板2〇中;由於 先珂對光阻層PR1 (或是PR2)之厚度控制,因此在植入離子 日可,光阻層PR1(或是PR2)會對植入之離子產生阻擋之效 果,因而在閘極結構Gn下方兩側之p型矽基板中,於該光 阻層PR1 (或疋PR2)之下方形成一對淡摻雜(亦即區域 N-,並且於凹口26中未被光阻層PR1 (或是pR2)覆蓋之矽基 板20中形成一對濃摻雜區,而完成源/汲極之結構。 —=後,塗佈另一光阻層27,如第2F圖所示;接著,進 行與前述相同之步驟,例如,請參看第2F圖,先以兩種強 度不同之能量E1與E2(例如是E-beam)照射N型井區21上方\ 之部分光阻使其曝光,然後如第2G圖所示,在經顯影之後 係形成一凹口 28,以及一未被顯影掉之光阻層pR3與位於 主動區A上方之光阻層27a,再以該光阻層27a與PR3為罩 幕,以1 X 1〇15〜5 X i〇i5 atoms/cni2間之離子濃度植入離 4S4^4 9 五、發明說明(7) ^ ^ 子’例如是硼離子至該矽基板2〇中,而於該光阻層pR3之 下方形成一對淡摻雜(亦即LDD)區域p—,並且於該凹口 Μ 中之未被光阻層PR3覆蓋之矽基板2〇中形成一對濃摻雜區 域p以作為源/没極區。 如同前述’於第2G圖中,此光阻層27經曝光、顯影之 結果可以因E1、E2強度之不同而形成不同情況之光阻層 PR4 ’如第2H圖所示’若E2之能量強度更高,則於閑極結 構Gp之頂部及側邊曝光較多,因此在顯影後係形成如第 圖所示之PR4。 最後’必須於該等閘極之表面形成一絕緣層,始完成| 一CMOS電晶體之製作,此外,若欲與其他元件做電性接 觸’則尚須以下步驟;例如,請先參考第2〖圖,移除該光 阻層27a與PR3使露出閘極結構Gp、Gn及該矽基板2〇之表面 (未顯不);再利用沈積與蝕刻製程,於該矽基板2 〇與該等 閘極結構Gp、Gn上形成一具有二開口 29a、29b之第一絕緣 層’例如是侧磷矽玻璃(BPSG)層29。其中,開口 29a、29b 係形成於該BPSG層29中,並分別露出Gp、Gn所屬電晶體之 源/没極的其中之一之矽基板2 〇表面。 接下來’請參看第2 j圖,沈積並回蝕刻一金屬層,例 如是複晶石夕層(未標號)於BPSG層29之表面,以於開口 ( 29a、29b中形成金屬栓们與站2。最後,於該心%層29之表 面再形成一第二絕緣層,例如是BPSG層3〇,以完成一半導 體元件之製造。 本發明利用控制光阻層之厚度而將形成電晶體源/汲Page 7 V. Description of the invention (5)-(Complementary Metal Oxide Semiconductor Transistor) 'referred to as CMOS transistor, so first in the p-type; a well region is formed in part of the active area B of the substrate 20', for example N Type well region 21, and a gate oxide layer such as a silicon dioxide layer 22, a gate electrode such as a polycrystalline silicon layer 23, and a gate oxide layer are sequentially formed on the surfaces of the P-type silicon substrate 20 and the N-type well region 21. Metallic oxide layers used to reduce gate resistance, such as Shixi Chemical Crane Layer 2 4. After that, a gate structure is to be formed on the surface of the semiconductor substrate; for example, according to the diagram in FIG. 2B, a pattern of the interelectrode structure is defined by using photolithography and etching; In this embodiment, the ^ (pole structure number is located above the N-type well region 21 is Gp 'and the gate structure number is located on the surface of the p-type silicon substrate 20 is Gn. ° The next step is Forming a photoresist layer to cover the free electrode and the semiconductor substrate; here, please refer to FIG. 2C first, coating—a layer of photoresist 25 on the surface of the silicon substrate 20, and its thickness About 10,000 ~ 12000 angstroms; next, the part of the photoresist layer is exposed and developed to form on the top side wall of the gate structure)-a photoresist layer with a specific thickness; 2: Figure (; = It uses the electron beam (E-beam) with intensity E2 in month b to scan the gate Gn and the photoresist layer 25 in the surrounding area, and the electron beam with an energy intensity of £ 1 to scan the gate ^ Gn and the photoresist layer 25 on the active area A other than the surrounding area to expose it, and light in the n-well area ^ The resist layer is not exposed; two points should be noted here. One is: the method of exposing the photoresist layer 25 can still be made by laser or X-ray scanning; the other 3 points Attention must be paid to all A § 44 3 Description of the invention ⑹ '^ " It is pill on E 2 5 ′ and E 2 is exposed to the thunder potential: which structure is the photoresist layer and range of A in the active area of ^ Due to the difference in intensity, the photoresist layer 25 is formed on the top and sides of the closed electrode structure after exposure and development processes to form a photoresist layer pR1 and a notch 26 as shown in FIG. 2D. Its thickness is between 300 and 400 angstroms; or its energy intensity is strengthened, so it exposes more on the top of the gate structure Gn and its sides, so it is formed after passing through the shirt. The photoresist layer shown in Fig. 2E? 1 ^ 2 and a notch 26 'have a thickness of about 100 ~ 500 Angstroms. Then, please refer to Figs. 2D and 2 £ at the same time: Use the photoresist layer 25a and PR1 (or PR2) are used as the curtain, and the ion concentration is implanted between! Xl015 and x1015 at 0ms / cm2 (the ion concentration is implanted into the silicon substrate 20, for example, arsenic ions; because Secco controls the thickness of the photoresist layer PR1 (or PR2), so it can be used when implanting ions. The photoresist layer PR1 (or PR2) will block the implanted ions. Therefore, the gate structure Gn In the p-type silicon substrates on the lower sides, a pair of lightly doped (ie, region N-) is formed under the photoresist layer PR1 (or 疋 PR2), and the photoresist layer PR1 (or A pair of heavily doped regions is formed in the silicon substrate 20 covered by pR2) to complete the source / drain structure. — = After that, apply another photoresist layer 27, as shown in FIG. 2F; then, perform the same steps as before, for example, refer to FIG. 2F, and first use two different energies E1 and E2 (eg (E-beam) irradiate a part of the photoresist above the N-type well area 21 to expose it, and then as shown in Figure 2G, after the development, a notch 28 is formed, and a photoresist layer that is not developed is developed. pR3 and the photoresist layer 27a located above the active area A, and then using the photoresist layer 27a and PR3 as a mask, an ion concentration between 1 X 1〇15 ~ 5 X i〇i5 atoms / cni2 is implanted from 4S4 ^ 4 9 V. Description of the invention (7) ^ ^ "The element" is, for example, boron ions into the silicon substrate 20, and a pair of lightly doped (ie, LDD) regions p- are formed below the photoresist layer pR3, and A pair of heavily doped regions p are formed in the notch M in the silicon substrate 20 not covered by the photoresist layer PR3 as the source / inverted regions. As in the aforementioned 'Figure 2G, the result of this photoresist layer 27 after exposure and development can form a photoresist layer PR4 with different conditions due to the difference in intensity of E1 and E2' as shown in Figure 2H 'if the energy intensity of E2 Higher, there is more exposure on the top and sides of the idle electrode structure Gp, so after development, PR4 is formed as shown in the figure. Finally, 'an insulating layer must be formed on the surface of these gates before the completion of the production of a CMOS transistor; in addition, if you want to make electrical contact with other components', the following steps are required; for example, please refer to Section 2 first [Figure, removing the photoresist layer 27a and PR3 to expose the gate structure Gp, Gn and the surface of the silicon substrate 20 (not shown); and then using a deposition and etching process on the silicon substrate 20 and the A first insulating layer ′ having two openings 29 a and 29 b is formed on the gate structures Gp and Gn. For example, the first insulating layer is a side phosphosilicate glass (BPSG) layer 29. The openings 29a and 29b are formed in the BPSG layer 29, and the surfaces of the silicon substrate 20, one of the source / inverter of the transistor to which Gp and Gn belong, are exposed, respectively. Next, please refer to FIG. 2j, deposit and etch back a metal layer, such as a polycrystalline stone layer (not labeled) on the surface of the BPSG layer 29, so as to form metal plugs and stations in the openings (29a, 29b). 2. Finally, a second insulating layer, such as a BPSG layer 30, is formed on the surface of the core% layer 29 to complete the manufacture of a semiconductor device. The present invention utilizes controlling the thickness of the photoresist layer to form a transistor source / Draw
第10頁 :秀9_^__ 五、發明說明(8) 極之淡摻雜區域與濃掺雜區域合併於一個步驟内完成,不 僅改善了以往為了形成LDD而分成兩階段性之離子植入, 簡化其製程步驟,更減少製作元件時所花費的時間,符合 經濟效應。 雖然本發明已以較佳實施例揭露如上,然其並非用以 限定本發明,任何熟習此項技藝者,在不脫離本發明之精 神和範圍内,當可作更動與潤飾,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。Page 10: Show 9 _ ^ __ 5. Description of the invention (8) The combination of extremely lightly doped regions and heavily doped regions is completed in one step, which not only improves the two-stage ion implantation in the past to form LDD, It simplifies its manufacturing steps and reduces the time it takes to make components, which is in line with economic effects. Although the present invention has been disclosed as above with preferred embodiments, it is not intended to limit the present invention. Any person skilled in the art can make changes and retouching without departing from the spirit and scope of the present invention. The scope of protection shall be determined by the scope of the attached patent application.
第11頁Page 11
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TW88111583A TW454249B (en) | 1999-07-08 | 1999-07-08 | Manufacturing method to form lightly doped region and heavily doped region of source/drain on transistor simultaneously |
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TW88111583A TW454249B (en) | 1999-07-08 | 1999-07-08 | Manufacturing method to form lightly doped region and heavily doped region of source/drain on transistor simultaneously |
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