TW521351B - Fabrication method of semiconductor device with low resistivity/ultra-shallow junction - Google Patents

Fabrication method of semiconductor device with low resistivity/ultra-shallow junction Download PDF

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TW521351B
TW521351B TW88104555A TW88104555A TW521351B TW 521351 B TW521351 B TW 521351B TW 88104555 A TW88104555 A TW 88104555A TW 88104555 A TW88104555 A TW 88104555A TW 521351 B TW521351 B TW 521351B
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Jr-Hau Wang
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Taiwan Semiconductor Mfg
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Abstract

This invention provides a fabrication method of semiconductor device with low resistivity/ultra-shallow junction, which is characterized in: after implantation on the LDD region is carried out, performing an annealing treatment in a gas atmosphere containing NO, N2O or NH3 to drive in the implanted ions. The RTN process can improve the activation rate of the doped ions and concurrently reduce the transient enhance diffusion (TED) phenomenon during annealing treatment.

Description

521351521351

第4頁 五、發明說明(2) 一個亟待解決的課題。 明習明之背景,以下將配合第卜3圖說 以及其缺陷所在/n原極/汲極區(LDD)的製作流程, 首先請來日S繁丨圓 , 1 2用以界定^件區·。’乂夕基底1 0上形成一隔離氧化物 成一 n ? 二 在元件區表面上,則以熱氧化方形 積(cvfD^ S 14,並〃以一導電層16,例如是以化學氣相沈 ‘王、>υ積的複晶矽層’覆蓋在閘氧化層1 4上。然 後以议影成像和巍岁,丨雀。@ . '、、 丘 /私序疋義導電層16和閘氧化層14的圖 案,共冋構成一閘電極構造G。 口 底1 η ί ΐ 1如第2圖所示,在純氧的環境下,對裸露·的基 (底10與複晶石夕層16的表面進行氧化,形成-遮蔽氧化層18 :二=二由於在前述定義閉極結構所進行的钱刻 過私可此會導致閘氧化層與晶圓表面的一些缺陷,因此 ΐϊ :再Γ匕程序(re—oxidation)可以將蝕刻所造成的損 r遮蔽氧化層18,則是在後續咖離、 :佈=用來保護閉氧化層與基底避免受到離子A擊的破 二,同%可防止佈植離子在稍.後的回火程序中從表面流失 接下來,如第3圖所示,利用閘電極構造G當作 佈植適當劑量離子(例如硼、磷或砷離子)進入^基底 然後在氮氣環境下進行熱回火,將方才植人的離$ :丄 溫擴散而趨入(drlve-ιη)矽底材内,以形成一對淡摻 極/汲極區20。然而,由於在離子佈植時,或有部份離子、 521351 五、發明說明(3) 與石夕晶中的雜質結合成錯合物(c〇mplex),將會導致離子 在回火後的活化率降低,而使電阻偏高。 第4圖為硼佈植的投射距離(pro j ec ted range )與活化 率的關係圖;其中投射距離的大小可代表佈植所使用的能 量高低。該圖中,是將劑量1 X 1013/cm2的硼離子,以不同 的佈植能量(5〜160 keV)植入矽晶圓,然後在9〇〇。〇下回火 20秒。由圖中可發現,在低能量(〜5keV)佈植時,硼離子 的活化率明顯降低。由於硼離子的活化效應機制,乃取決 於棚離子從插空隙晶格位置進入取代性晶格位置,而在低 能量佈植時,由於接近表面處的空缺數量大大地減少,這 使朴雜質錯合物(B—impurity c〇mpiex),無法進入空 缺位置而達成活化。相關的文獻可參考F . pr i〇丨〇,e1: al· , APL 72(23), ρ·3011(1998)。 另一方面,在進行離子佈植時,根據佈植離子的種類 與/辰度’會在石夕晶内產生各種不同的缺陷,例如插空隙型 缺陷(Interstitial Type),空缺型缺陷(Vacancy Type) 等’其中自我插空隙(Self-Interstitial)型缺陷為引致 R T A處理時發生暫態加速擴散的主要原因之一。第5圖係以 離子佈植為例,說明暫態加速擴散現象,其顯示硼佈植 在經歷1 5秒、1 5分、1小時、2小時,8〇〇 °c下RTA回火處理 後的濃度縱深圖。如第5圖所示,爛離子在§ 〇 〇。〇下的暫態 加速槪散現象於1 5分鐘内即趨飽和,< 後,即使持續兩小 時的回火都不會再增加擴散深度,故稱為"暫態"加速擴散 。有關於暫態加速擴散的文獻請參考L · η . Z h a n g,e t 五、發明說明(4) al·,APL 67(14),ρ· 2〇25( 1 995 )。 一般而言,佈植離子在RTA處理日士 ^ 象,可藉由降低佈植時之能量來減麵才、暫悲加速擴散現 提及,降低佈植能量勢必會導致活^銮然而,如前文中所 偏高。因此,如何減輕暫態加速擴,降低,而使電限 接合面,並在同時降低其電阻率,象,以形成極淺之 在。 成為本發明之重點所 習知技術中的一種LDD改良製裎,B 層的成長,直接佈植離子於美底中 疋不經過遮蔽氧化 子的趨入。但此法少了遮蔽ί化層的f後以熱回火進行離 植時,將會造成閘氧化層的損壞,呆濩,不僅在離子佈 氧化層的覆蓋,也會造成離子彳^表且在回火時少了遮蔽 所示。[請參考Mark G. Stlns(; \流失,如第6圖中22 487 (1991)] ai· , ED-38(3), ρ· 習知技術中的另一種改良方 保護下進行LDD的離子佈植,然則是在遮蔽氧化層的 蔽氧化層剝除後,再進行換質的< 以渴蝕刻的方式將遮 氧化層受到離子佈植的破壞貝作入。此法雖然可避免間 當的覆蓋層,因此仍無法避免離 T在回火時依然沒有適 濕蝕刻法將遮蔽氧化層剝除時,勢從表面流失,·再者’以 刻,而蝕去部份的閘極氧化/,=也會因其等向性的蝕 這方法也有閘極氧化層完整^ 1第7圖中24所示,因此 有鑑於上述問題,本發明 的問題存在。 " 導體元件的製造、方法,苴 目的就是提供〆種半 /、了減輕摻雜離子在回火處理時的 521351 五、發明說明(5) 暫悲加速擴散現象,以形成極淺之接合面,並同時可辦 摻雜離子的活化率,以形成低電阻之接合面。 ' 本發明的另一目的在於提供一種半導體元件的製造方 法’其可避免摻雜區表面的摻質流失,並同時確 化層完整性。 < 為達上述目的,本發明的方法係在施行LDD佈植之後 ,在含有⑽,,或龍3的氣體環境下進行快速熱回火, 以取代傳統中在純氮氣(n2)下所進行的熱回火。 簡吕之’本發明的方法包括下列步驟:(a)提供一半 導體基底,其上形成有一閘極結構;(b)形成一遮蔽氧化 層於閘極結構兩側之基底;(c)施行一離子佈植,於閘極 結構兩側的基底中形成淡摻雜區;以及(d)施行一快 化製程。 、、Page 4 V. Description of the invention (2) A problem to be solved urgently. To understand the background of Ming and Ming, the following will cooperate with the illustration in Figure 3 and the production process of the / n source / drain region (LDD) where the defect is located. First, please come to Japan to make a circle, 1 2 to define the ^ area. 'Even on the substrate 10, an isolation oxide is formed to form an n? 2 on the surface of the element area, and then a square product (cvfD ^ S 14 is thermally oxidized, and a conductive layer 16 is used, for example, chemical vapor deposition is used.' Wang, > The stacked polycrystalline silicon layer 'covers on the gate oxide layer 14. Then it is imaged by the image and Wei Sui, que. @.',, Qiu / Private sequence conductive layer 16 and gate oxide The pattern of layer 14 together constitutes a gate electrode structure G. As shown in Fig. 2, the bottom of the mouth 1 η ί ΐ 1 on the exposed substrate (base 10 and polycrystalline spar layer 16 in a pure oxygen environment). The surface is oxidized to form-shield oxide layer 18: two = two. Due to the money engraved in the closed-polar structure defined above, it may cause some defects in the gate oxide layer and the wafer surface. Therefore: The procedure (re-oxidation) can shield the oxide layer 18 from the damage caused by the etching. It is used to protect the closed oxide layer and the substrate from ion A. The same% can prevent The implanted ions are lost from the surface during the subsequent tempering procedure. Next, as shown in FIG. 3, the gate electrode structure G is used as the cloth. An appropriate dose of ions (such as boron, phosphorus, or arsenic ions) is implanted into the substrate and then thermally tempered in a nitrogen environment to diffuse the human implanted ions into the drlve-silicon substrate. To form a pair of lightly doped / drain regions 20. However, since some ions may be implanted during ion implantation, 521351 V. Description of the invention (3) Combined with impurities in Shi Xijing to form a complex (c 〇mplex), will cause the activation rate of the ions after tempering to decrease, resulting in higher resistance. Figure 4 shows the relationship between the projection distance (pro j ec ted range) of boron implantation and the activation rate; The size can represent the level of energy used for implantation. In this figure, boron ions at a dose of 1 X 1013 / cm2 are implanted into a silicon wafer with different implantation energies (5 ~ 160 keV), and then at 90%. Tempering at 20 ° C for 20 seconds. It can be found from the figure that the activation rate of boron ions is significantly reduced when implanted at low energy (~ 5keV). Due to the activation effect mechanism of boron ions, it depends on the insertion of shed ions from the gap The lattice position enters the substitutional lattice position. The number of vacancies at the surface is greatly reduced, which makes B-impurity coompiex unable to enter the vacancies and achieve activation. Related literature can refer to F. pr i〇 丨 〇, e1: al · , APL 72 (23), ρ · 3011 (1998). On the other hand, when ion implantation is performed, various defects will be generated in Shi Xijing according to the type and degree of implanted ions, such as insertion. Interstitial Type, Vacancy Type, etc. 'Self-Interstitial Type Defects are one of the main causes of transient accelerated diffusion during RTA processing. Figure 5 illustrates the phenomenon of transient accelerated diffusion using ion implantation as an example. It shows that the boron implantation has undergone RTA tempering at 800 ° c for 15 seconds, 15 minutes, 1 hour, and 2 hours. Depth map. As shown in Figure 5, rotten ions are at § 〇 〇. The transient acceleration phenomenon below 〇 becomes saturated within 15 minutes, and after that, even if the tempering lasts for two hours, it will not increase the depth of diffusion, so it is called " transient " accelerated diffusion. For the literature on transient accelerated diffusion, please refer to L · η. Z h a n g, e t V. Description of the invention (4) al ·, APL 67 (14), ρ · 2052 (1 995). Generally speaking, the treatment of implantation ions in RTA by RTA can reduce the surface energy by reducing the energy at the time of implantation, and temporarily accelerate the spread of sorrow. It is mentioned that reducing the energy of implantation will inevitably lead to live ^^ High in the previous article. Therefore, how to mitigate the transient accelerated expansion and decrease the electrical limit of the junction surface and reduce its resistivity at the same time, so as to form a very shallow existence. It is a kind of improved LDD system in the conventional technology that has become the focus of the present invention. The growth of the B layer directly implants ions in the substrate, and does not pass through the shielding of the oxidants. However, when this method eliminates the f layer that shields the fluorinated layer and leaves it by thermal tempering, it will cause damage to the gate oxide layer, which will not only cover the oxide layer of the ion cloth, but also cause ionization. Less shadowing shown during tempering. [Please refer to Mark G. Stlns (; \ Lost, as shown in Figure 6 22 487 (1991)] ai ·, ED-38 (3), ρ · Ion under the protection of another improved method in the conventional technology The implantation, however, is performed after the masking oxide layer of the masking oxide layer is stripped off, and the masking oxide layer is destroyed by ion implantation in a thirsty etching manner. Although this method can avoid instability As a result, it is still unavoidable that when T is not tempered and the masking oxide layer is not stripped during tempering, the potential is lost from the surface, and in addition, a part of the gate oxide is etched in time. , = Also because of its isotropic etching, this method also has a complete gate oxide layer ^ 1 shown in Figure 7 at 24, so in view of the above problems, the problem of the present invention exists. &Quot; Manufacturing and methods of conductor elements, The purpose is to provide a kind of half // alleviation of 521351 during the tempering treatment of doped ions. V. Description of the invention (5) Temporarily accelerate the diffusion phenomenon to form a very shallow junction surface, and at the same time, doped ions Activation rate to form a low-resistance joint. 'Another object of the present invention is Provided is a method for manufacturing a semiconductor device, which can prevent dopant loss on the surface of a doped region, and at the same time ensure layer integrity. ≪ To achieve the above-mentioned object, the method of the present invention is performed after LDD implantation and contains rhenium. Or rapid thermal tempering under the gas environment of Dragon 3 to replace the traditional thermal tempering under pure nitrogen (n2). Jian Luzhi 'method of the present invention includes the following steps: (a) providing a semiconductor A substrate on which a gate structure is formed; (b) a substrate that shields an oxide layer on both sides of the gate structure; (c) performing an ion implantation to form a lightly doped region in the substrate on both sides of the gate structure ; And (d) implement a quickening process.

本發明在步驟(d)所進行的快速氮化製程(RapUThe rapid nitriding process (RapU) performed in step (d) of the present invention

Thermal Wtridatbn),係在含有 N〇,n2〇,或 Nh3 的氣體 環境下進行快速熱回火,例如可在N的混合氣體下収 以9 0 0〜1 050 °C進行回火5〜30秒鐘。此處的氮化製程可在石夕 晶格中放出空缺(inject vacancies),其兼具以下兩種 效: 功 (1 )氮化所放出的晶格空缺可幫助摻質—雜質錯合物 (dopant — impuritycomp lex)溶解,因 it 可增進〉、舌 ^ 匕率 如前文中所述,在低能量摻雜時,是因為靠近表面的* 密度不足,因此會有活化率偏低的問題,而本發明藉=, 化所放出的晶格空缺,正可用來彌補表面空缺數目^不鼠 521351 五、發明說明(6) ,因此可提高離子的活化率,形成一低電阻的接面。 (2)氮化所放出的晶格空缺可將位於插隙處的矽原子 重組,進入適當的空缺位置,因而減輕暫態加速擴散。如 前文中所述,離子佈植所引起的插空隙型缺陷是造成暫態 加速擴散的主要原因之一,而本發明藉由氮化所放出的晶 格空缺,可使得原本位於插隙處(i n t e r s t i t i a 1 )的石夕原子 經由晶格重組而進入適當的空缺,因此可減少插隙處的矽 原子數量,從而降低輕暫態加速擴散現象,形成一極淺的 接合面。 除此之外,在步驟(d)之後,熟習此技藝者可依習知 的製程技術製作絕緣側壁層與源極/汲極區,以完成具有 低電阻/極淺接面之場效電晶體的製作。 為讓本發明之上述和其他目的、特徵、和優點能更明 顯易懂,下文特舉一較佳實施例,並配合所附圖式,作詳 細說明如下: 圖式之簡單說明 第1〜3圖為一系列剖面圖,用以說明習知製作LDD的流 程。 第4圖為硼佈植的投射距離與活化率的關係圖。 第5圖為硼離子佈植在經歷不同時間RTA回火處理時的 濃度縱深圖,用以說明暫態加速擴散現象。 第6圖與第7圖為製程剖面圖,分別說明習知中的兩種 LDD改良製程。 第8〜1 0圖為一系列剖面圖,用以說明本發明之較佳實Thermal Wtridatbn), rapid thermal tempering in a gas environment containing N0, n2〇, or Nh3. For example, it can be tempered under a mixed gas of N at 90 0 ~ 1 050 ° C for 5 ~ 30 seconds. bell. The nitriding process here can release inject vacancies in the Shi Xi lattice, which has the following two effects: (1) lattice vacancies released by nitriding can help dopant-impurity complexes ( dopant — impuritycomp lex) dissolves, because it can be improved>, the rate of tongue ^ is as described above, when low energy doping, because the density near the surface is not enough, there will be a problem of low activation rate, and According to the present invention, the lattice vacancies released by the method can be used to make up the number of surface vacancies. ^ Bu 521351 5. Invention description (6), therefore, the activation rate of ions can be increased, and a low-resistance junction can be formed. (2) The lattice vacancies released by nitridation can recombine the silicon atoms located at the interstitial spaces and enter the appropriate vacancies, thereby reducing the transient accelerated diffusion. As mentioned above, the interstitial-type defects caused by ion implantation are one of the main reasons for the transient accelerated diffusion, and the lattice vacancies released by nitriding in the present invention can make the originals located at the interstitial spaces ( Interstitia 1) Shi Xi atoms enter the appropriate vacancies through lattice recombination, so the number of silicon atoms at the interstitial space can be reduced, thereby reducing the phenomenon of light transient accelerated diffusion and forming a very shallow junction. In addition, after step (d), those skilled in the art can make insulating sidewall layers and source / drain regions according to conventional process technologies to complete field effect transistors with low resistance / very shallow junctions. Making. In order to make the above and other objects, features, and advantages of the present invention more comprehensible, a preferred embodiment is given below in conjunction with the accompanying drawings for detailed description as follows: Brief description of the drawings 1 to 3 The figure is a series of cross-sectional views, which are used to explain the process of making LDD. Fig. 4 is a graph showing the relationship between the projection distance of boron implantation and the activation rate. Figure 5 is a concentration depth map of boron ion implantation after undergoing RTA tempering at different times to illustrate the phenomenon of transient accelerated diffusion. Figures 6 and 7 are cross-sectional views of the manufacturing process, respectively illustrating two conventional LDD improvement processes. Figures 8 to 10 are a series of cross-sectional views to illustrate the preferred embodiment of the present invention.

五、發明說明(7) 施例製作LDD的流程 符號說明 10、3〇~矽基底;12 化層;1 6、3 6〜導電層· 以〜隔絕氧化物;14、34〜閘氧 摻植源極/汲極區;&18、38〜遮蔽氧化層;20、40〜淡 陷;4 2〜側壁間隔層·表面摻質流失;2 4〜閘氧化層缺 曰’ 4〜源極/汲極區;G〜閘極結構。 —實施例 本發明之實施例 如下,由於在本實於' 3第8圖至第10圖作一詳細敘述 施以N型離子的淡摻雜τ①形成PMOS元件,因此將基底3〇 盲先 Μ得統的Ρ β斤 程(STI )形成隔離氡/域軋化法(L0C0S)或淺溝槽隔離製 元件區上形成一閑極:32 ’用以界定出元件區’然後在 ,如第8圖所示。構G,包括閘極氧化層34與閘極36 化層,通常是以乾Λ化層34是一層很薄’且無污染的氧 诵堂s 、,儿粗-式或濕式熱氧化法緩慢形成;問極3 6, 疋L /予氣相沈積法(CVD)或類似方法所形成的複晶 與二。、在形成堆疊的問氧化層34與閘複晶矽層36後,便^ Ρ衫成像與#刻技術將之定義成第8圖所示的閘極結構G。 請參照第9圖,於閘極結構g兩側之基底形成一遮蔽氧 化層38 °在純氧環境下以9 0 0〜1〇〇〇 °C的溫度成長一遮蔽氧 化層,厚度約2 0〜7 0埃。此時,在基底3 0裸露的表面與複 晶矽層36上會形成一遮蔽氧化層38,如第9圖所示。由於V. Description of the invention (7) Example of symbolic flow chart for making LDD in the examples 10, 30 ~ silicon substrate; 12 layers; 16 and 36 ~ conductive layers to isolate oxides; 14, 34 ~ gate oxygen doping Source / drain region; & 18, 38 ~ shielding oxide layer; 20, 40 ~ fading; 4 2 ~ sidewall spacers · surface dopant loss; 2 4 ~ gate oxide layer missing '4 ~ source / Drain region; G ~ gate structure. —Example The following is an example of the present invention. As described in detail in FIG. 8 to FIG. 10, a detailed description is given by applying a lightly doped τ① of an N-type ion to form a PMOS element. The system's P β catastrophe (STI) is used to form an isolation / field rolling method (LOC0S) or a shallow trench isolation device area to form a free pole: 32 'to define the device area' and then, as in Section 8 As shown. Structure G, including the gate oxide layer 34 and the gate 36 layer, is usually a dry thin layer 34 is a thin layer of non-pollution oxygen, and the coarse-type or wet thermal oxidation method is slow Formation; interfacial electrodes 36, 疋 L / pre-vapour deposition (CVD) or similar methods, and multiple crystals. After forming the stacked interlayer oxide layer 34 and the gate compound silicon layer 36, they are defined as the gate structure G shown in FIG. Referring to FIG. 9, a shielding oxide layer is formed on the substrates on both sides of the gate structure g. 38 ° A shielding oxide layer is grown at a temperature of 900-1000 ° C in a pure oxygen environment, with a thickness of about 20 ~ 70 0 Angstroms. At this time, a masking oxide layer 38 will be formed on the exposed surface of the substrate 30 and the polycrystalline silicon layer 36, as shown in FIG. due to

521351 五、發明說明521351 V. Description of the invention

前述定義閘極結構所進 面的一些缺陷,因此這裡的j過程,可能會導致晶圓表 30與複晶矽層36的表面谁三;:、虱化程序可以對裸露的基底 復元。 仃氧化,以將蝕刻所造成的損壞 請繼續參照第9圖 構造G當作罩幕,對其 進仃LDD的佈植。利用閘電極 的基底中形成源極/ ::植入,在閘極相對兩側 氧化層38所提供的保護 ?雜區42,此時,由於遮蔽 為釗籬不I箭 一又 侍閘氧化層3 4的邊緣處可免於The aforementioned definition of some defects on the surface of the gate structure, so the process j here may lead to the surface of the wafer table 30 and the polycrystalline silicon layer 36. The lice process can recover the bare substrate. It is oxidized to damage the etching. Please continue to refer to Fig. 9. Structure G is used as a mask, and it is implanted with LDD. Use the gate electrode to form the source / :: implant, the protection provided by the oxide layer 38 on opposite sides of the gate? Miscellaneous area 42, at this time, the edge of the oxide layer 3 4 can be avoided due to the shadowing.

二植入可W破壞,確保閘氧化層完整性。pm〇s元件的 LDD植入了使用二氟化硼(Bf2)離子,在劑量約 1013〜1015/cnr2,能量約3〜15keV的條件下進行植入。 接下來’進行本發明的關鍵步驟,在含有N 〇,κ 〇或 ΜΙ的氣體環境下進行快速熱回火。在本實施例中,2是以 n2/nh3的混合氣體(氣體流量比:nH3/N疒0· ι〜80%),在9〇〇 〜1050 C的溫度下持續回火5〜30秒鐘,完成佈植離子的趨 入。此時’氮化製程所放出的晶格空缺可增加離子的活化 率’並同時降低暫態加速擴散現象,因此在回火後可形成 一低電阻且深度極淺的接合面。另一方面,由於此回火程The two implants can be destroyed to ensure the integrity of the gate oxide layer. The LDD of the PMOS element was implanted using boron difluoride (Bf2) ions at a dose of about 1013 to 1015 / cnr2 and an energy of about 3 to 15 keV. Next, the key step of the present invention is performed, and rapid thermal tempering is performed in a gas environment containing N 0, κ 0 or MI. In this embodiment, 2 is a mixed gas of n2 / nh3 (gas flow ratio: nH3 / N 疒 0 · ι ~ 80%), and is continuously tempered at a temperature of 900 ~ 1050 C for 5 ~ 30 seconds. To complete the implantation of ions. At this time, 'lattice vacancies released by the nitridation process can increase the activation rate of ions' and at the same time reduce the phenomenon of transient accelerated diffusion, so a low-resistance and extremely shallow junction surface can be formed after tempering. On the other hand, due to this tempering process

序是在遮蔽氧化層的覆蓋下進行,因此可避免摻質從表面 流失 ° 請參照第1 0圖,之後的步驟,熟習此技藝者可依傳統 製程技術,製作側壁間隔層4 2與源極/没極區4 4,以完成 PM0S電晶體的製作。例如可先沈積一層厚約1 0 0 0〜2 5 0 0埃 的氧化層在基底3 〇與閘極結構G上,然後以電漿蝕刻法,The sequence is performed under the covering of an oxide layer, so that the dopant can be prevented from being lost from the surface. Please refer to Figure 10, and the following steps. Those skilled in this art can make the sidewall spacer 42 and the source electrode according to the traditional process technology. / Pole area 4 4 to complete the fabrication of PM0S transistor. For example, an oxide layer having a thickness of about 1000 to 2500 angstroms can be deposited on the substrate 30 and the gate structure G first, and then plasma etching is used.

第11頁 521351 五、發明說明(9) 將這層氧化層非等向性地蝕刻成側壁間隔層4 2。然後,利 用=電極構造G和側壁間隔層42共同當作罩幕,佈植較高 劑量離子進入基底中,用以形成濃摻植源極和汲極區44, 便完成如第1 〇圖所示的M〇s電晶體。 上呪明可知,本發明提供了 一個簡單而有效的方 造成:ΪΪ暫態加速擴散現象,時解決低能量佈植所 於習知製程率Ϊ Ϊ的問題。綜上所述,本發明的製程相較 白知衣权,具有下列優點: 千乂 ΐ f活化率以得到一低電阻之接合面。 子佈植破壞戶"發的暫態加速擴散。 ν ύ八避免表面摻質流失。 < [肽 (4 )·確保閘氧化層完整性。 以阳ί然本發明已以一較佳實施例揭㊉^ 抽又疋本發明,任何熟習此技藝者ι =上,然其並非用 謹t範圍内,當可作各種之更動與、'門f不脫離本發明之精 又乾圍當視後附之申請專利範圍 ,因此本發明之保 %界定者為準。Page 11 521351 V. Description of the invention (9) The oxide layer is anisotropically etched into a sidewall spacer layer 42. Then, using the electrode structure G and the sidewall spacer 42 together as a mask, implanting a higher dose of ions into the substrate to form a strongly doped source and drain region 44 is completed as shown in FIG. 10 The shown Mos transistor. It can be seen from the above description that the present invention provides a simple and effective solution to the problem: the transient acceleration of the phenomenon of ΪΪ, which can solve the problem of low-energy implantation in the conventional process rate Ϊ 时. To sum up, the process of the present invention has the following advantages compared with Bai Zhiyi, which has the following advantages: The activation rate can be reduced to obtain a low-resistance joint surface. The sub-plant destroys the transient state of households and accelerates the spread. ν ύ 八 Avoid the loss of adulteration on the surface. < [Peptide (4) · Ensure gate oxide integrity. The present invention has been disclosed in a preferred embodiment. Anyone skilled in the art is familiar with the above, but it is not within the range of t. It can be used to make various changes. f Without departing from the spirit and scope of the present invention, the scope of the patent application attached hereto shall be regarded as the definition of the guarantee of the present invention shall prevail.

第12頁Page 12

Claims (1)

521351 六、申請專利範圍 1. 一種低電阻/極淺接面之半導體元件的製造方法, 包括下列步驟: (a)提供一半導體基底,其上形成有一閘極結構; (b )形成一遮蔽氧化層於該閘極結構兩側之基底; (c) 施行一離子佈植,於該閘極結構兩側的基底中形 成淡推雜區,以及 (d) 施行一快速氮化製程。 2. 如申請專利範圍第1項所述之製造方法,其中該閘 極結構包括一導電層及一閘氧化層。 3. 如申請專利範圍第1項所述之製造方法,其中該遮 蔽氧化層的厚度為20〜70埃。 4. 如申請專利範圍第3項所述之製造方法,其中該遮 蔽氧化層係在9 0 0〜1 0 0 0 °C的溫度下以熱氧化法形成。 5. 如申請專利範圍第1項所述之製造方法,其中步驟 (d)係在含有NO,N20,或NH3的氣體環境下進行快速熱回火 〇 6. 如申請專利範圍第5項所述之製造方法,其中步驟 (d)係在9 0 0〜1 0 5 0 °C下持續回火5〜3 0秒鐘。 7. 如申請專利範圍第6項所述之製造方法,其中步驟 (d)係在含有N2與NH3的氣體環境下進行快速熱回火。 8. 如申請專利範圍第7項所述之製造方法,其中氣體 流量比:ΝΗ3/Ν2 = 0· 1 〜80%。521351 6. Scope of patent application 1. A method for manufacturing a low-resistance / very shallow junction semiconductor device, including the following steps: (a) providing a semiconductor substrate having a gate structure formed thereon; (b) forming a masking oxide A substrate layered on both sides of the gate structure; (c) performing an ion implantation to form a doped impurity region in the substrate on both sides of the gate structure; and (d) performing a rapid nitriding process. 2. The manufacturing method according to item 1 of the scope of patent application, wherein the gate structure includes a conductive layer and a gate oxide layer. 3. The manufacturing method according to item 1 of the scope of patent application, wherein the thickness of the shielding oxide layer is 20 to 70 angstroms. 4. The manufacturing method as described in item 3 of the scope of patent application, wherein the shielding oxide layer is formed by a thermal oxidation method at a temperature of 900 to 100 ° C. 5. The manufacturing method described in item 1 of the scope of patent application, wherein step (d) is rapid thermal tempering in a gas environment containing NO, N20, or NH3. 6. As described in item 5 of the scope of patent application The manufacturing method, wherein the step (d) is continuously tempered for 5 to 30 seconds at 900 to 105 ° C. 7. The manufacturing method as described in item 6 of the scope of patent application, wherein step (d) is performed by rapid thermal tempering in a gas environment containing N2 and NH3. 8. The manufacturing method as described in item 7 of the scope of patent application, wherein the gas flow ratio: ΝΗ3 / Ν2 = 0.1 to 80%. 第13頁Page 13
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