TWI567937B - Active device and semiconductor device with the same - Google Patents

Active device and semiconductor device with the same Download PDF

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TWI567937B
TWI567937B TW103139461A TW103139461A TWI567937B TW I567937 B TWI567937 B TW I567937B TW 103139461 A TW103139461 A TW 103139461A TW 103139461 A TW103139461 A TW 103139461A TW I567937 B TWI567937 B TW I567937B
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region
contact
active
guard
intermediate portion
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TW201618277A (en
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呂函庭
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旺宏電子股份有限公司
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Description

主動元件及應用其之半導體元件 Active component and semiconductor component using the same

本發明是有關於一種主動元件及應用其之一半導體元件,且特別是有關於一種自隔離(self-isolated)的主動元件及一應用此主動元件的無淺溝渠隔離之半導體元件。 The present invention relates to an active component and a semiconductor component thereof, and more particularly to a self-isolated active component and a shallow trench isolation semiconductor component using the active component.

在超大型積體電路(Very-large-scale integration,VLSI)技術中,通常使用淺溝渠隔離(shallow-trench isolation,STI)隔絕主動元件(例如互補式金屬氧化物半導體之電晶體)而定義出通道寬度。然而,相關研究者已經發現STI邊緣會對應用元件造成許多嚴重問題。 In the Very-large-scale integration (VLSI) technology, shallow-trench isolation (STI) isolation active elements (such as complementary metal oxide semiconductor transistors) are usually defined. Channel width. However, researchers have found that STI edges can cause many serious problems for application components.

第1圖繪示一種半導體元件之傳統佈局。半導體元件包括多個主動元件10彼此相距地設置於一基板上,並皆位於具第一導電態之一第一井12中,例如NMOS元件的P型井中。再者,一輕摻雜區域(light doping region)具一第二導電態(例如N-)且位於P型井中並包圍所有的主動元件10和P型井接點(P-well contact)。相鄰的主動元件10係以STI電性隔離。各主動元件10包括具第一導電態之一擴散區域DIF,一第一接觸區域111(例如 一汲極區域)與一第二接觸區域113(例如一源極區域)分別位於擴散區域DIF內,以及一多晶矽閘極PG(其上具有一閘極接點115)形成在第一接觸區域111和第二接觸區域113之間。對傳統的半導體元件而言,存在於相鄰主動元件10之間的STI會造成不希望出現的STI邊緣效應(STI edge issues)。 Figure 1 illustrates a conventional layout of a semiconductor component. The semiconductor component includes a plurality of active components 10 disposed on a substrate at a distance from one another and both located in a first well 12 having a first conductivity state, such as a P-well of an NMOS component. Furthermore, a light doping region has a second conductive state (eg, N-) and is located in the P-well and surrounds all active components 10 and P-well contacts. Adjacent active components 10 are electrically isolated by STI. Each active component 10 includes a diffusion region DIF having a first conductive state, a first contact region 111 (eg, A drain region) and a second contact region 113 (eg, a source region) are respectively located in the diffusion region DIF, and a polysilicon gate PG (having a gate contact 115 thereon) is formed in the first contact region 111 And the second contact area 113. For conventional semiconductor components, STIs that exist between adjacent active components 10 can cause undesirable STI edge issues.

第2圖是繪示一傳統半導體元件之多晶矽閘極及兩側之絕緣物的剖面示意圖。一多晶矽閘極PG係形成於一閘極氧化層GOX,通道135則位於多晶矽閘極PG下方和絕緣物STI之間。第3A圖為一典型的低壓(LV)NMOS電晶體之ID-VG特性曲線,其中閘極氧化層GOX厚度為70Å,W/Lg=0.6μm/0.4μm,且該些曲線在一汲極偏壓(VD)0.1V下量測而得。第3B圖為一典型的高壓(HV)NMOS電晶體之ID-VG特性曲線,其中閘極氧化層GOX厚度為370Å,W/Lg=10μm/1.6μm,且該些曲線在一汲極偏壓(VD)0.1V下量測而得。請參照第1圖至第3B圖。STI邊緣通常是半導體元件的”弱點”(如第2圖中圈選處),會造成不正常的次臨界漏電流(subthreshold leakage current)和導致不希望出現的雙峰(double hump)次臨界ID-VG特性曲線(如第3A圖和第3B圖中的曲線Process-1所示)。第3A圖和第3B圖中,曲線Process-1代表具雙峰漏電流之典型NMOS電晶體的ID-VG特性曲線,曲線Process-2代表具有改良STI之典型NMOS電晶體的ID-VG特性曲線,曲線Process-3代表具有改良STI和STI邊牆口袋摻雜(sidewall STI pocket implant)之典型NMOS電晶體的ID-VG特性曲 線。 2 is a schematic cross-sectional view showing a polysilicon gate of a conventional semiconductor device and insulators on both sides. A polysilicon gate PG is formed in a gate oxide layer GOX, and a channel 135 is located under the polysilicon gate PG and between the insulators STI. Figure 3A is an I D -V G characteristic curve of a typical low voltage (LV) NMOS transistor in which the gate oxide layer GOX has a thickness of 70 Å, W/Lg = 0.6 μm / 0.4 μm, and the curves are in a The pole bias (V D ) is measured at 0.1V. Figure 3B is an I D -V G characteristic curve of a typical high voltage (HV) NMOS transistor, wherein the gate oxide layer GOX has a thickness of 370 Å, W/Lg = 10 μm / 1.6 μm, and the curves are in a bungee The bias voltage (V D ) was measured at 0.1 V. Please refer to Figures 1 to 3B. The STI edge is usually the "weakness" of the semiconductor component (as circled in Figure 2), causing an abnormal subthreshold leakage current and an undesired double hump subcritical I D- V G characteristic curve (as shown by curve Process-1 in Figures 3A and 3B). In Figs. 3A and 3B, the curve Process-1 represents the I D -V G characteristic curve of a typical NMOS transistor having a bimodal leakage current, and the curve Process-2 represents the I D of a typical NMOS transistor having an improved STI. The V G characteristic curve, curve Process-3, represents the I D -V G characteristic curve of a typical NMOS transistor with improved STI and STI sidewall STI pocket implants.

一般而言,STI邊緣通常會產生幾種非理想狀況,例如:(1)在STI邊牆上產生硼偏離(boron segregation)而導致P型井摻雜損失(p-well dosage loss);(2)STI引起的應力變化(STI induced stress)會影響臨界電壓(Vt)的穩定度;以及(3)一些界面陷阱(interface trap)或錯位會增加漏電流。這些狀況會造成不理想的次臨界特性和更高的漏電流問題。雖然,目前經常是應用一STI邊牆口袋摻雜(sidewall STI pocket implant)於結構的”弱點”處(如第2圖中圈選處),以在STI邊牆處提高局部的井摻雜並抑制雙峰漏電流(double-hump leakage)(曲線Process-3),結構仍有缺點,包括:(1)會降低高壓NMOS的接面崩潰(junction breakdown),因為接面(輕摻雜NM)在STI邊緣處會看到更多的P型井摻雜,以及(2)當通道寬度尺寸縮小會產生嚴重的窄通道寬度效應(snarrow-width effect)。因此,STI邊牆口袋摻雜仍然影響了通道摻雜和臨界電壓的控制。 In general, STI edges usually produce several non-ideal conditions, such as: (1) Boron segregation on the STI side wall leads to P-well dosage loss; (2) STI induced stress affects the stability of the threshold voltage (Vt); and (3) some interface traps or misalignments increase the leakage current. These conditions can cause undesirable subcritical properties and higher leakage current problems. Although it is often the case that a STI pocket implant is often applied to the "weakness" of the structure (as circled in Figure 2) to improve local well doping at the STI sidewall To suppress double-hump leakage (curve Process-3), the structure still has shortcomings, including: (1) it will reduce the junction breakdown of the high-voltage NMOS because of the junction (lightly doped NM) More P-well doping will be seen at the STI edge, and (2) a narrow narrow channel width effect will result when the channel width is reduced. Therefore, STI sidewall pocket doping still affects channel doping and threshold voltage control.

再者,由於主動元件10的傳統構型,如第1圖所示,其交疊的多晶矽閘極PG和擴散區域DIF之間的延伸方式,使相鄰主動元件10的間距會受到限制,特別是主動元件10在第1圖中x-方向上的排列。因此,由於必須考慮到擴散區域DIF的設計原則,這會對於傳統構型主動元件的一密集間距佈局的設計原則(tight-pitch layout design rule)產生限制。 Moreover, due to the conventional configuration of the active device 10, as shown in FIG. 1, the manner of extension between the overlapping polysilicon gate PG and the diffusion region DIF limits the spacing of adjacent active devices 10, in particular It is the arrangement of the active elements 10 in the x-direction in Fig. 1. Therefore, since the design principle of the diffusion region DIF must be taken into consideration, this imposes a limitation on a tight-pitch layout design rule of the conventional configuration active element.

本發明係有關於一種主動元件及應用其之一半導體元件。實施例之主動元件係利用一導電護欄結構而自隔離,而包括無淺溝渠隔離(STI-free)主動元件的實施例之半導體元件,可成功地解決傳統半導體元件遭遇到的STI邊緣效應(STI edge issues)問題。 The present invention relates to an active component and a semiconductor component using the same. The active components of the embodiments are self-isolated using a conductive barrier structure, and the semiconductor components of the embodiments including the shallow trench isolation (STI-free) active devices can successfully solve the STI edge effects encountered by conventional semiconductor components (STI Edge issues).

根據一實施例,係提出一種半導體元件,包括一基板、一第一井具有一第一導電態並自基板之表面向下延伸、摻雜第一導電態之不純物之一擴散區域(diffusion region)並自第一井之表面向下延伸、以及複數個主動元件形成於擴散區域內。其中,這些主動元件係彼此相距地設置,並藉由擴散區域而彼此電性絕緣。 According to an embodiment, a semiconductor device includes a substrate, a first well having a first conductive state and extending downward from a surface of the substrate, and a diffusion region of the impurity doped with the first conductive state. And extending downward from the surface of the first well, and a plurality of active components are formed in the diffusion region. Wherein, the active components are disposed apart from each other and electrically insulated from each other by the diffusion region.

根據實施例,係提出一種主動元件,形成於一基板處之具有一第一導電態的一擴散區域內。主動元件包括一導電護欄結構(conductive guarding structure)、一第一接觸區域(first contact region)和一第二接觸區域(second contact region)。導電護欄結構包括一中間部(middle portion)、一第一護部(first guarding portion)和第二護部(second guarding portion)。第一護部連接中間部之一側以定義位於擴散區域之一第一區域,其中第一區域係由第一護部和中間部圍繞而成。一第二護部與第一護部相對並連接中間部之另一側以定義位於擴散區域之一第二區域,其中第二區域係由第二護部和中間部圍繞而成。第一接觸區域具有一第二 導電態並形成於導電護欄結構之第一區域內,且第一接觸區域係與第一護部和該中間部相距。第二接觸區域具有第二導電態並形成於導電護欄結構之第二區域內,且第二接觸區域係與第二護部和中間部相距。 According to an embodiment, an active device is formed in a diffusion region having a first conductive state at a substrate. The active component includes a conductive guarding structure, a first contact region, and a second contact region. The conductive barrier structure includes a middle portion, a first guarding portion, and a second guarding portion. The first guard portion is coupled to one side of the intermediate portion to define a first region located in one of the diffusion regions, wherein the first region is surrounded by the first guard portion and the intermediate portion. A second guard portion is opposite to the first guard portion and connects to the other side of the intermediate portion to define a second region located in one of the diffusion regions, wherein the second region is surrounded by the second guard portion and the intermediate portion. The first contact area has a second The conductive state is formed in the first region of the conductive barrier structure, and the first contact region is spaced from the first guard portion and the intermediate portion. The second contact region has a second conductive state and is formed in the second region of the conductive barrier structure, and the second contact region is spaced from the second guard portion and the intermediate portion.

為了對本發明之上述及其他方面有更佳的瞭解,下文特舉實施例,並配合所附圖式,作詳細說明如下。然而,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。 In order to better understand the above and other aspects of the present invention, the following detailed description of the embodiments and the accompanying drawings are set forth below. However, the scope of the invention is defined by the scope of the appended claims.

10、20‧‧‧主動元件 10, 20‧‧‧ active components

12、PW‧‧‧第一井 12. PW‧‧‧ first well

111‧‧‧第一接觸區域 111‧‧‧First contact area

113‧‧‧第二接觸區域 113‧‧‧Second contact area

115‧‧‧閘極接點 115‧‧‧gate contacts

135‧‧‧通道 135‧‧‧ channel

22‧‧‧輕摻雜區域 22‧‧‧Lightly doped areas

24‧‧‧間隔物 24‧‧‧ spacers

201‧‧‧導電護欄結構 201‧‧‧ Conductive guardrail structure

201m‧‧‧中間部 201m‧‧‧ middle part

2011‧‧‧第一護部 2011‧‧‧First Department

2012‧‧‧第二護部 2012‧‧‧Second Ministry

201a‧‧‧第一區域 201a‧‧‧First area

201b‧‧‧第二區域 201b‧‧‧Second area

211‧‧‧第一接觸區域 211‧‧‧First contact area

213‧‧‧第二接觸區域 213‧‧‧Second contact area

215‧‧‧第三接觸區域 215‧‧‧ Third contact area

251‧‧‧第一接點 251‧‧‧ first joint

253‧‧‧第二接點 253‧‧‧second junction

255‧‧‧閘極接點 255‧‧‧gate contacts

S‧‧‧基板 S‧‧‧Substrate

DIF‧‧‧擴散區域 DIF‧‧‧Diffusion area

PG‧‧‧多晶矽閘極 PG‧‧‧ polysilicon gate

STI‧‧‧絕緣物 STI‧‧‧Insulators

GOX‧‧‧閘極氧化層 GOX‧‧‧ gate oxide layer

S1‧‧‧第一隔離距離 S1‧‧‧first isolation distance

S2‧‧‧第二隔離距離 S2‧‧‧Second isolation distance

W’‧‧‧有效通道寬度 W’‧‧‧ effective channel width

W‧‧‧第一區域和第二區域之寬度 W‧‧‧Width of the first and second regions

W2‧‧‧第一護部和第二護部之寬度 W2‧‧‧Width of the first and second guards

Dp‧‧‧主動元件之間距 Dp‧‧‧ active component spacing

Lg‧‧‧通道長度 Lg‧‧‧ channel length

doffset‧‧‧接觸區域到第一護部/第二護部的最小距離 d offset ‧‧‧Minimum distance from the contact area to the first guard/second guard

第1圖繪示一種半導體元件之傳統佈局。 Figure 1 illustrates a conventional layout of a semiconductor component.

第2圖是繪示一傳統半導體元件之多晶矽閘極及兩側之絕緣物的剖面示意圖。 2 is a schematic cross-sectional view showing a polysilicon gate of a conventional semiconductor device and insulators on both sides.

第3A圖為一典型的低壓(LV)NMOS電晶體之ID-VG特性曲線,其中閘極氧化層GOX厚度為70Å,W/Lg=0.6μm/0.4μm,且該些曲線在一汲極偏壓(VD)0.1V下量測而得。 Figure 3A is an I D -V G characteristic curve of a typical low voltage (LV) NMOS transistor in which the gate oxide layer GOX has a thickness of 70 Å, W/Lg = 0.6 μm / 0.4 μm, and the curves are in a The pole bias (V D ) is measured at 0.1V.

第3B圖為一典型的高壓(HV)NMOS電晶體之ID-VG特性曲線,其中閘極氧化層GOX厚度為370Å,W/Lg=10μm/1.6μm,且該些曲線在一汲極偏壓(VD)0.1V下量測而得。 Figure 3B is an I D -V G characteristic curve of a typical high voltage (HV) NMOS transistor, wherein the gate oxide layer GOX has a thickness of 370 Å, W/Lg = 10 μm / 1.6 μm, and the curves are in a bungee The bias voltage (V D ) was measured at 0.1 V.

第4圖係為本揭露實施例之一半導體元件之佈局。 Figure 4 is a layout of a semiconductor device of one embodiment of the present disclosure.

第5A圖係為本揭露實施例之一半導體元件之一主動元件之示意圖。 FIG. 5A is a schematic view showing an active element of one of the semiconductor elements of the disclosed embodiment.

第5B圖為第5A圖中主動元件之一導電護欄結構的爆炸圖。 Figure 5B is an exploded view of the conductive barrier structure of one of the active components of Figure 5A.

第6圖係繪示第4圖之半導體元件中兩個相鄰主動元件之示意圖。 Figure 6 is a schematic view showing two adjacent active elements in the semiconductor device of Figure 4.

第7圖繪示本揭露實施例之第4圖中之兩個相鄰主動元件,以及在主動元件的源極和汲極之間汲極電流之示意圖。 FIG. 7 is a schematic diagram showing two adjacent active elements in FIG. 4 of the disclosed embodiment, and a drain current between the source and the drain of the active device.

第8圖係清楚顯示沒有雙峰漏電流產生,且實驗數值係與理論模型的模擬曲線理想重合。 Figure 8 clearly shows that there is no bimodal leakage current generation, and the experimental values are ideally coincident with the simulation curves of the theoretical model.

第9圖為具有箝制位元線元件(BL Clamp Devices)之NAND快閃記憶體之頁面緩衝電路設計。 Figure 9 is a page buffer circuit design of a NAND flash memory with a clamped line element (BL Clamp Devices).

第10圖係繪示一實施例中一高壓半導體元件之佈局。 Figure 10 is a diagram showing the layout of a high voltage semiconductor device in an embodiment.

第11圖係繪示本揭露一實施例之其中一種可應用之包括多個主動元件之CMOS的佈局。 FIG. 11 is a diagram showing a layout of a CMOS including a plurality of active elements, which is applicable to an embodiment of the present disclosure.

第12A-12D圖分別繪示根據TCAD模擬實驗之一實施例之無STI電晶體的立體圖、及沿YZ-平面、XZ-平面和XY-平面之剖面圖。 12A-12D are respectively a perspective view of the STI-free transistor according to an embodiment of the TCAD simulation experiment, and a cross-sectional view along the YZ-plane, the XZ-plane, and the XY-plane.

第13A圖繪示TCAD模擬實驗中實施例之無STI電晶體之ID-VG特性曲線,其中係施加電壓Vg1和Vg2於實施例之無STI電晶體“Gate 1”和“Gate 2”元件。 Figure 13A is a graph showing the I D -V G characteristic of the STI-free transistor of the embodiment in the TCAD simulation experiment, in which the voltages Vg1 and Vg2 are applied to the STI-free transistor "Gate 1" and "Gate 2" components of the embodiment. .

第13B圖是“Gate 1”和“Gate 2”元件中施加Vg1=0.5V、Vg2=3.8V和Vds=0.1V之電流密度模擬示意圖。 Figure 13B is a schematic diagram showing the simulation of the current density of Vg1 = 0.5V, Vg2 = 3.8V, and Vds = 0.1V in the "Gate 1" and "Gate 2" elements.

第14A圖繪示TCAD模擬實驗中實施例之無STI電晶體之ID-VG特性曲線,其中係變化不同寬度W2為0.1μm、0.15μm和 0.2μm。 Fig. 14A is a graph showing the I D -V G characteristic of the STI-free transistor of the embodiment in the TCAD simulation experiment, wherein the system has different widths W2 of 0.1 μm, 0.15 μm and 0.2 μm.

第14B圖繪示TCAD模擬實驗中實施例之無STI電晶體之ID-VG特性曲線,其中係變化不同通道長度Lg為0.25μm、0.3μm和0.4μm。 Fig. 14B is a graph showing the I D -V G characteristic of the STI-free transistor of the embodiment in the TCAD simulation experiment, wherein the system changes the channel length Lg to 0.25 μm, 0.3 μm and 0.4 μm.

第15A圖為TCAD模擬實驗中,一實施例之無STI電晶體沿著XY-平面之剖面圖。 Figure 15A is a cross-sectional view of the STI-free transistor of the embodiment along the XY-plane in a TCAD simulation experiment.

第15B-15E圖繪示TCAD模擬實驗中實施例之無STI電晶體之ID-VG特性曲線,其中第15B圖之Vg2=0V和Vd1=0.1V,第15C圖之Vg2=0V和Vd1=3.8V,第15D圖之Vg2=3.8V和Vd1=0.1V,以及第15E圖之Vg2=3.8V和Vd1=3.8V。 15B-15E is a graph showing the I D -V G characteristic of the STI-free transistor of the embodiment in the TCAD simulation experiment, wherein Vg2=0V and Vd1=0.1V in Fig. 15B, Vg2=0V and Vd1 in Fig. 15C = 3.8 V, Vg2 = 3.8 V and Vd1 = 0.1 V in Fig. 15D, and Vg2 = 3.8 V and Vd1 = 3.8 V in Fig. 15E.

第16圖繪示TCAD模擬實驗中實施例之無STI電晶體中之I-Vd1特性曲線。 Figure 16 is a graph showing the IV d1 characteristic curve in the STI-free transistor of the embodiment in the TCAD simulation experiment.

在此揭露內容之實施例中,係提出一主動元件及應用其之一半導體元件。實施例之主動元件係以一導電護欄結構(conductive guarding structure)達到自隔離(self-isolated),例如是一多晶矽護欄結構也做為主動元件之閘極。而應用實施例之無STI主動元件的半導體元件可成功地解決傳統半導體元件所存在的STI邊緣效應(STI edge issues)。本揭露之實施例可應用於許多不同態樣之低壓(LV)半導體元件和高壓(HV)半導體元件,本揭露並不以某應用態樣為限。以下係提出實施例,配合圖示以詳細說 明本揭露所提出之其中一種主動元件及一半導體元件之新佈局。然而本揭露並不僅限於此。實施例中之敘述,如細部結構、相關元素之尺寸和材料選擇等等,僅為舉例說明之用,並非對本揭露欲保護之範圍做限縮。 In an embodiment of the present disclosure, an active component and one of the semiconductor components are applied. The active component of the embodiment is self-isolated with a conductive guarding structure, such as a polysilicon barrier structure also acting as a gate for the active component. The semiconductor component without the STI active device of the application embodiment can successfully solve the STI edge problem existing in the conventional semiconductor device. The embodiments of the present disclosure are applicable to many different aspects of low voltage (LV) semiconductor components and high voltage (HV) semiconductor components, and the disclosure is not limited to a certain application. The following is an embodiment, which is described in detail with the illustration. A new layout of one of the active components and a semiconductor component proposed is disclosed. However, the disclosure is not limited to this. The descriptions of the embodiments, such as the details of the details, the dimensions of the elements and the choice of materials, etc., are for illustrative purposes only and are not intended to limit the scope of the disclosure.

再者,本揭露並非顯示出所有可能的實施例。可在不脫離本揭露之精神和範圍內對結構和製程加以變化與修飾,以符合實際應用之需要。因此,未於本揭露提出的其他實施態樣也可能可以應用。再者,圖式上的尺寸比例並非按照實際產品等比例繪製。因此,說明書和圖示內容僅作敘述實施例之用,而非作為限縮本揭露保護範圍之用。 Furthermore, the disclosure does not show all possible embodiments. The structure and process may be modified and modified to meet the needs of the actual application without departing from the spirit and scope of the disclosure. Therefore, other implementations not presented in the present disclosure may also be applicable. Furthermore, the dimensional ratios on the drawings are not drawn in proportion to the actual product. Therefore, the description and illustration are for illustrative purposes only and are not intended to be limiting.

第4圖係為本揭露實施例之一半導體元件之佈局。第5A圖係為本揭露實施例之一半導體元件之一主動元件之示意圖。第5B圖為第5A圖中主動元件之一導電護欄結構的爆炸圖。第6圖係繪示第4圖之半導體元件中兩個相鄰主動元件之示意圖。請參照第4圖-第6圖。 Figure 4 is a layout of a semiconductor device of one embodiment of the present disclosure. FIG. 5A is a schematic view showing an active element of one of the semiconductor elements of the disclosed embodiment. Figure 5B is an exploded view of the conductive barrier structure of one of the active components of Figure 5A. Figure 6 is a schematic view showing two adjacent active elements in the semiconductor device of Figure 4. Please refer to Figure 4 - Figure 6.

實施例中,一半導體元件包括一基板S,具有一第一導電態(例如P型)之一第一井PW,一擴散區域DIF和和複數個主動元件20形成於擴散區域DIF內(第4圖和第6圖)。第一井PW係自基板S之一表面向下延伸,而具有第一導電態(例如P型)之擴散區域DIF係自第一井PW之一表面向下延伸(第6圖)。如第4圖所示,該些主動元件20係彼此相距地設置,且所有主動元件20皆形成於連續的一擴散區域DIF內,其中主動元件20係 藉由擴散區域DIF而彼此電性絕緣。沒有淺溝渠隔離(Shallow trench isolation,STI)存在於兩相鄰主動元件20之間。在一實施例中,擴散區域DIF係重度摻雜具第一導電態之不純物,如P+,以提供場絕緣(field isolation)。 In one embodiment, a semiconductor device includes a substrate S having a first well PW of a first conductive state (eg, P-type), a diffusion region DIF, and a plurality of active devices 20 formed in the diffusion region DIF (fourth Figure and Figure 6). The first well PW extends downward from one surface of the substrate S, and the diffusion region DIF having the first conductive state (e.g., P-type) extends downward from one surface of the first well PW (Fig. 6). As shown in FIG. 4, the active elements 20 are disposed at a distance from each other, and all the active elements 20 are formed in a continuous diffusion region DIF, wherein the active device 20 is They are electrically insulated from each other by the diffusion region DIF. No shallow trench isolation (STI) exists between two adjacent active elements 20. In one embodiment, the diffusion region DIF is heavily doped with impurities in a first conductivity state, such as P+, to provide field isolation.

再者,各主動元件20包括一導電護欄結構(conductive guarding structure)201形成於擴散區域DIF上,和一輕摻雜區域(light doping region)22具有一第二導電態(例如N-),且輕摻雜區域22自擴散區域DIF之一表面向下延伸並對應地位於導電護欄結構201之內。根據實施例,位於相鄰之主動元件20之間的一隔離區域(isolating region)(例如圖中標示隔離距離S1或S2之區域),係由相鄰主動元件20的導電護欄結構201所定義。如第4圖所示,沿著第一方向如x-方向排列的相鄰主動元件20係以具有第一隔離距離S1的隔離區域所隔絕,而沿著第二方向如y-方向排列的相鄰主動元件20係以具有第二隔離距離S2的隔離區域所隔絕。第一隔離距離S1和第二隔離距離S2可以不相等或相等。一實施例中,第一隔離距離S1係相等於第二隔離距離S2。根據實施例,相鄰之主動元件20之間的空間(S1/S2)係無淺溝渠隔離(STI)存在,因此實施例之設計可使半導體元件完全免除於任何STI邊緣效應(例如雙峰次臨界漏電流、崩潰電壓下降、不同STI佈局之差異,等等)。 Furthermore, each active component 20 includes a conductive guarding structure 201 formed on the diffusion region DIF, and a light doping region 22 having a second conductive state (eg, N-), and The lightly doped region 22 extends downwardly from one surface of the diffusion region DIF and is correspondingly located within the conductive barrier structure 201. According to an embodiment, an isolating region (e.g., an area labeled with an isolation distance S1 or S2) between adjacent active elements 20 is defined by conductive barrier structure 201 of adjacent active elements 20. As shown in FIG. 4, adjacent active elements 20 arranged along the first direction, such as the x-direction, are isolated by an isolation region having a first isolation distance S1, and phases arranged along a second direction, such as the y-direction. The adjacent active element 20 is isolated by an isolation region having a second isolation distance S2. The first isolation distance S1 and the second isolation distance S2 may not be equal or equal. In one embodiment, the first isolation distance S1 is equal to the second isolation distance S2. According to an embodiment, the space (S1/S2) between adjacent active elements 20 is free of shallow trench isolation (STI), so the embodiment is designed to completely eliminate the semiconductor components from any STI edge effects (eg, bimodal Critical leakage current, breakdown voltage drop, difference in different STI layouts, etc.).

一實施例中,導電護欄結構201包括一中間部(middle portion)201m、一第一護部(first guarding portion)2011和 一第二護部(second guarding portion)2012,如第5A和5B圖所示。第一護部2011連接中間部201m之一側,以定義出位於擴散區域DIF之一第一區域(first region)201a。第二護部2012係與第一護部2011相對並連接中間部201m之另一側,以定義出位於擴散區域DIF之一第二區域(second region)201b。因此,第一區域201a是由第一護部2011和中間部201m圍繞而成,第二區域201b是由第二護部2012和中間部201圍繞而成。 In one embodiment, the conductive barrier structure 201 includes a middle portion 201m, a first guarding portion 2011, and A second guarding portion 2012, as shown in Figures 5A and 5B. The first guard portion 2011 is connected to one side of the intermediate portion 201m to define a first region 201a located in one of the diffusion regions DIF. The second guard portion 2012 is opposite to the first guard portion 2011 and is connected to the other side of the intermediate portion 201m to define a second region 201b located in one of the diffusion regions DIF. Therefore, the first region 201a is surrounded by the first guard portion 2011 and the intermediate portion 201m, and the second region 201b is surrounded by the second guard portion 2012 and the intermediate portion 201.

如第4圖所示,主動元件20中第一區域201a和第二區域201b係位於輕摻雜區域22內。輕摻雜區域22係包圍第一區域201a和第二區域201b但與其相隔一距離。一實施例中,輕摻雜區域22係位於對應第一護部2011和第二護部2012處。例如輕摻雜區域22的邊界(即第4圖和第5A圖中一主動元件20內的虛線所指)係實質上對應第一護部2011和第二護部2012邊寬的中間,如第4圖和第5A圖所示。 As shown in FIG. 4, the first region 201a and the second region 201b of the active device 20 are located within the lightly doped region 22. The lightly doped region 22 surrounds the first region 201a and the second region 201b but is spaced apart therefrom. In one embodiment, the lightly doped region 22 is located at the corresponding first guard portion 2011 and the second guard portion 2012. For example, the boundary of the lightly doped region 22 (ie, indicated by the broken line in the active element 20 in FIGS. 4 and 5A) substantially corresponds to the middle of the first guard portion 2011 and the second guard portion 2012, as in the first Figure 4 and Figure 5A show.

再者,各主動元件20更包括具有第二導電態(例如N+)並形成於導電護欄結構201之第一區域201a內的一第一接觸區域(firstcontact region)211,和具有第二導電態(例如N+)並形成於導電護欄結構201之第二區域201b內一第二接觸區域(second contact region)213。且第一接觸區域211係與第一護部2011和中間部201m相隔開來,第二接觸區域213係與第二護部2012和中間部201m相隔開來。一實施例中,第一接觸區域211和第二接觸區域213可分別做為主動元件20的一汲極區域(drain region) 和一源極區域(source region)。 Furthermore, each active component 20 further includes a first contact region 211 having a second conductive state (eg, N+) and formed in the first region 201a of the conductive barrier structure 201, and having a second conductive state ( For example, N+) is formed in a second contact region 213 in the second region 201b of the conductive barrier structure 201. The first contact region 211 is spaced apart from the first guard portion 2011 and the intermediate portion 201m, and the second contact region 213 is spaced apart from the second guard portion 2012 and the intermediate portion 201m. In an embodiment, the first contact region 211 and the second contact region 213 can be used as a drain region of the active device 20, respectively. And a source region.

如第6圖所示,各主動元件20更包括一第一接點(first contact)251(例如是做為汲極)形成於第一接觸區域211,以及一第二接點(second contact)253(例如是做為源極)形成於第二接觸區域213。再者,一閘極接點(gate contact)255係接觸導電護欄結構201。一實施例中,閘極接點255可以形成於導電護欄結構201的中間部201m之第三接觸區域215上,其中閘極接點255對應地位於輕摻雜區域22內。然而,閘極接點255並不限制於圖示中所繪示之位置,也可能形成於其他位置,只要閘極接點255能與導電護欄結構201電性連接即可。 As shown in FIG. 6, each active component 20 further includes a first contact 251 (for example, as a drain) formed in the first contact region 211, and a second contact 253. (for example, as a source) is formed in the second contact region 213. Furthermore, a gate contact 255 is in contact with the conductive barrier structure 201. In one embodiment, the gate contact 255 can be formed on the third contact region 215 of the intermediate portion 201m of the conductive barrier structure 201, wherein the gate contact 255 is correspondingly located within the lightly doped region 22. However, the gate contact 255 is not limited to the position shown in the drawing, and may be formed at other positions as long as the gate contact 255 can be electrically connected to the conductive barrier structure 201.

在製造過程中,導電護欄結構201的開口(對應第一區域201a和第二區域201b)形成後,係以摻雜少量第二導電態(如N-)不純物之方式於導電護欄結構201下方形成輕摻雜區域22,如第6圖所示。之後,於開口處形成適當尺寸的間隔物(spacers,如氧化物)24以定義出第一接觸區域211和第二接觸區域213。由於第一接觸區域211和第二接觸區域213的面積甚小(特別是對應用於小型電子產品之半導體元件),可先形成第一接點251、第二接點253和閘極接點255,再以插塞植入(plug implant)方式摻雜高濃度之第二導電態不純物(如N+)於該些接點下方。然而,本揭露並不限於此製造方式。如前敘述之步驟僅為舉例說明之用,可視實際應用之條件所需而做適當的調整或變化。 In the manufacturing process, the openings of the conductive barrier structure 201 (corresponding to the first region 201a and the second region 201b) are formed under the conductive barrier structure 201 by doping a small amount of second conductive state (such as N-) impurities. Lightly doped region 22, as shown in Figure 6. Thereafter, appropriately sized spacers (such as oxides) 24 are formed at the openings to define the first contact regions 211 and the second contact regions 213. Since the areas of the first contact region 211 and the second contact region 213 are very small (especially corresponding to semiconductor components for small electronic products), the first contact 251, the second contact 253, and the gate contact 255 may be formed first. Then, a high concentration of the second conductive state impurity (such as N+) is doped under the contacts by a plug implant. However, the disclosure is not limited to this manufacturing method. The steps as described above are for illustrative purposes only and may be appropriately adjusted or varied as needed for the actual application conditions.

根據一實施例,導電護欄結構201之材質可以是多 晶矽,而導電護欄結構201的中間部201m可做為主動元件20之閘極(即多晶矽閘極)。第7圖繪示本揭露實施例之第4圖中之兩個相鄰主動元件,以及在主動元件的源極和汲極之間汲極電流之示意圖。請同時參照第4圖和第7圖。做為主動元件20之閘極的導電護欄結構201之中間部201m,係在沿著第一方向(如x-方向)上具有一有效通道寬度(effective channel width)W’,在沿著第二方向(如y-方向)上具有一通道長度(channel length)Lg。 According to an embodiment, the material of the conductive guardrail structure 201 may be more The wafer, and the intermediate portion 201m of the conductive barrier structure 201 can serve as a gate of the active device 20 (i.e., a polysilicon gate). FIG. 7 is a schematic diagram showing two adjacent active elements in FIG. 4 of the disclosed embodiment, and a drain current between the source and the drain of the active device. Please refer to both Figure 4 and Figure 7. The intermediate portion 201m of the conductive barrier structure 201 as the gate of the active component 20 has an effective channel width W' along the first direction (eg, the x-direction), along the second The direction (such as the y-direction) has a channel length Lg.

一實施例中,第一方向(如x-方向)係垂直於第二方向(如y-方向)。如第4圖和第7圖所示,第一區域201a和第二區域201b係相隔了通道長度Lg之距離。再者,第一護部2011和第二護部2012沿著第一方向(如x-方向)各具有一寬度W2,第一區域201a和第二區域201b沿著第一方向各具有一寬度W。形成於第一接觸區域211之第一接點251和形成於第二接觸區域213之第二接點253可分別做為汲極和源極。如第7圖所示,在源極和汲極之間的汲極電流包括:在源極和汲極之間最短路徑流動的電流(即垂直線段),和流動路徑較最短路徑更長的側邊電流(sidewall current,即兩側之曲線)。因此,實施例中主動元件20之一有效通道寬度W’係大約等於寬度W和兩倍寬度W2之總和(記為W+2×W2)。側邊電流有較長的有效通道長度,即大於Lg,而沒有雙峰漏電流的問題產生。一實施例中,當擴散區域DIF包括高濃度的第一導電態摻雜物例如P+,在輕摻雜區域22外側則形成P+包圍閘極而達到場絕緣(field isolation)。根據實施例,兩 相鄰電晶體的寄生漏電流(parasitic leakage)可有效地被擴散區域DIF所抑制,而此抑制可因兩主動元件(如NMOS)之間的空間(Sl/S2)具有足夠濃度的P型摻雜(P+)而達成。第8圖為本揭露實施例之一MOSFET電晶體佈局的ID-VG特性曲線。第8圖係清楚顯示沒有雙峰漏電流產生,且實驗數值係與理論模型的模擬曲線理想重合。再者,當Vg低於0.7V時僅觀察到極低的漏電流值。 In one embodiment, the first direction (eg, the x-direction) is perpendicular to the second direction (eg, the y-direction). As shown in Figs. 4 and 7, the first region 201a and the second region 201b are separated by a channel length Lg. Furthermore, the first guard portion 2011 and the second guard portion 2012 each have a width W2 along the first direction (eg, the x-direction), and the first region 201a and the second region 201b each have a width W along the first direction. . The first contact 251 formed on the first contact region 211 and the second contact 253 formed on the second contact region 213 may serve as a drain and a source, respectively. As shown in Figure 7, the drain current between the source and the drain includes: the current flowing in the shortest path between the source and the drain (ie, the vertical line segment), and the side of the flow path that is longer than the shortest path. Sidewall current (the curve on both sides). Thus, the effective channel width W' of one of the active elements 20 in the embodiment is approximately equal to the sum of the width W and the double width W2 (denoted as W + 2 x W2). The side current has a longer effective channel length, ie greater than Lg, without the problem of bimodal leakage current. In one embodiment, when the diffusion region DIF includes a high concentration of the first conductive state dopant such as P+, and outside the lightly doped region 22, a P+ surrounding gate is formed to achieve field isolation. According to an embodiment, the parasitic leakage of two adjacent transistors can be effectively suppressed by the diffusion region DIF, and the suppression can be sufficient due to the space (S1/S2) between the two active devices (such as NMOS). The concentration of P-type doping (P+) is achieved. FIG. 8 is an I D -V G characteristic curve of a MOSFET transistor layout according to an embodiment of the present disclosure. Figure 8 clearly shows that there is no bimodal leakage current generation, and the experimental values are ideally coincident with the simulation curves of the theoretical model. Furthermore, only a very low leakage current value was observed when Vg was lower than 0.7V.

根據上述,應用有實施例之主動元件的半導體元件係具有幾個特性,例如:(1)沒有分隔的擴散區域DIF(無STI存在於元件的主動區);(2)使用導電護欄結構(如多晶矽閘極)201本身來定義通道長度和通道寬度;(3)輕摻雜區域22(如N-)和摻雜區域22(如N+)(即第一接觸區域211、第二接觸區域213和閘極接觸區域215)係在各閘極區域裡隔絕;以及(4)在導電護欄結構201之間的隔離距離可用P+不純物而達到良好之場絕緣。相較於如第1圖所示之半導體元件的傳統佈局,實施例之半導體元件佈局(如第4圖所示)具有許多優點。例如,相鄰之主動元件20之間的空間(S1/S2)由於沒有淺溝渠隔離(STI)存在,因此實施例之設計可使半導體元件完全免除於任何STI邊緣效應(例如雙峰次臨界漏電流、崩潰電壓下降、不同STI佈局之差異等等)。再者,由於實施例的主動元件20特殊的構型,沒有如傳統之擴散區域DIF和多晶矽閘極之間交疊和延伸方式的存在,因此主動元件20之間的距離得以再縮減。 According to the above, the semiconductor element to which the active element of the embodiment is applied has several characteristics, such as: (1) a diffusion region DIF having no separation (no STI exists in the active region of the element); (2) using a conductive barrier structure (eg The polysilicon gate 201 itself defines the channel length and the channel width; (3) the lightly doped region 22 (eg, N-) and the doped region 22 (eg, N+) (ie, the first contact region 211, the second contact region 213, and The gate contact regions 215) are isolated in each gate region; and (4) the isolation distance between the conductive barrier structures 201 can be achieved with P+ impurities to achieve good field insulation. The semiconductor element layout of the embodiment (as shown in Fig. 4) has many advantages over the conventional layout of the semiconductor element as shown in Fig. 1. For example, the space between adjacent active elements 20 (S1/S2) is present because there is no shallow trench isolation (STI), so the embodiment is designed to completely eliminate the semiconductor components from any STI edge effects (eg, bimodal sub-critical leakage). Current, breakdown voltage drop, difference in different STI layouts, etc.). Moreover, due to the special configuration of the active element 20 of the embodiment, there is no overlap and extension between the conventional diffusion region DIF and the polysilicon gate, so the distance between the active elements 20 can be further reduced.

實施例之主動元件可應用於高壓(HV)半導體元件 或低壓(LV)半導體元件。以下係說明一高壓半導體元件或一低壓半導體元件之中可實行的其中一種設計規則。但,以下提出之相關參數數值係僅為例示之用,並非用以限制本揭露欲保護之範圍。 The active component of the embodiment can be applied to a high voltage (HV) semiconductor component Or low voltage (LV) semiconductor components. The following describes one of the design rules that can be implemented in a high voltage semiconductor element or a low voltage semiconductor element. However, the relevant parameter values set forth below are for illustrative purposes only and are not intended to limit the scope of the disclosure.

請參照第4圖,可代表一實施例中一低壓半導體元件之佈局。對於在3V下操作的一NAND快閃記憶體之元件來說,最大偏壓需約在3.8V左右。以下係提出在3V下操作之一低壓半導體元件的一組相關參數作說明。一實施例中,對在3V下操作之低壓半導體元件,其通道長度Lg可約0.3μm至約0.4μm以支撐最大偏壓3.8V。第一區域201a和第二區域201b的最小寬度W約0.2μm,第一接觸區域211和第二接觸區域213的其中之一(即每一汲極/源極)具有約0.1μm×0.1μm之面積。第一護部2011和第二護部2012的最小寬度W2約0.1μm至約0.15μm。相鄰主動元件20的空間(假設S1=S2=S)例如是約0.18μm至約0.28μm的距離。再者,主動元件20之間距(pitch)DP約0.68μm。由於實施例之主動元件間距DP達到約0.68μm,因此符合NAND快閃記憶體的頁面緩衝電路設計(page buffer circuit design)。 Referring to Figure 4, there may be shown a layout of a low voltage semiconductor component in an embodiment. For a NAND flash memory device operating at 3V, the maximum bias voltage is about 3.8V. The following is a description of a set of related parameters for operating a low voltage semiconductor component at 3V. In one embodiment, for a low voltage semiconductor device operating at 3V, the channel length Lg can be from about 0.3 [mu]m to about 0.4 [mu]m to support a maximum bias voltage of 3.8V. The minimum width W of the first region 201a and the second region 201b is about 0.2 μm, and one of the first contact region 211 and the second contact region 213 (ie, each drain/source) has about 0.1 μm×0.1 μm. area. The minimum width W2 of the first guard portion 2011 and the second guard portion 2012 is about 0.1 μm to about 0.15 μm. The space of adjacent active elements 20 (assuming S1 = S2 = S) is, for example, a distance of about 0.18 μm to about 0.28 μm. Furthermore, the active element 20 has a pitch DP of about 0.68 μm. Since the active device pitch DP of the embodiment reaches about 0.68 μm, it conforms to the page buffer circuit design of the NAND flash memory.

第9圖為具有箝制位元線元件(BL Clamp Devices)之NAND快閃記憶體之頁面緩衝電路設計。在NAND快閃記憶體頁面緩衝設計中,BLC、BLK和BLC_I元件(及三個圈選區域之元件)是很重要的。這些元件需要有緊的臨界電壓(Vt)分佈以在感測時可精確地控制位元線偏壓。再者,由於許多頁面緩衝電路 存在,因此需要一個可緊密配置元件的佈局規則存在。而實施例之元件特別符合此目的,其至少具有以下優點:包括(1)由於無須考慮擴散區域規則,因此實施例之佈局比傳統佈局可達到更緊密的配置間距;和(2)緊臨界電壓(Vt)分佈和沒有STI邊緣所引起的問題和變異。 Figure 9 is a page buffer circuit design of a NAND flash memory with a clamped line element (BL Clamp Devices). In NAND flash memory page buffer designs, the BLC, BLK, and BLC_I components (and the components of the three circled regions) are important. These components require a tight threshold voltage (Vt) distribution to accurately control the bit line bias during sensing. Furthermore, due to many page buffer circuits There is a need for a layout rule that tightly configurable components. While the elements of the embodiments are particularly suitable for this purpose, they have at least the following advantages: including (1) the layout of the embodiment can achieve a tighter arrangement spacing than the conventional layout since there is no need to consider the diffusion area rule; and (2) the tight threshold voltage (Vt) distribution and problems and variations caused by the absence of STI edges.

第10圖係繪示一實施例中一高壓半導體元件之佈局。請參照上述關於實施例之主動元件的相關部件內容說明。且第10圖與第4圖中相同的元件係沿用相同標號以清楚呈現實施例。其細節(例如在多晶矽閘極內之輕摻雜區域22(N-)、在第一區域201a/第二區域201b內之第一接觸區域211/第二接觸區域213)已經記述如前,在此不再贅述。低壓和高壓半導體元件的設計主要的不同在於,高壓半導體元件中第一接觸區域211及第二接觸區域213分別到第一護部2011及第二護部2012的距離必須增加,以支撐高壓操作。由於接觸區域(211/213/215)的N+是在接觸蝕刻後進行,重摻雜接觸區域(211/213/215)會被限制在小面積的接觸區域。 Figure 10 is a diagram showing the layout of a high voltage semiconductor device in an embodiment. Please refer to the description of the relevant components of the active components of the above embodiments. The same elements in the drawings of FIG. 10 and FIG. 4 are given the same reference numerals to clearly illustrate the embodiments. Details thereof (for example, the lightly doped region 22 (N-) in the polysilicon gate, the first contact region 211 / the second contact region 213 in the first region 201a / the second region 201b) have been described as before This will not be repeated here. The main difference between the design of the low voltage and high voltage semiconductor components is that the distance between the first contact region 211 and the second contact region 213 of the high voltage semiconductor component to the first guard portion 2011 and the second guard portion 2012 must be increased to support the high voltage operation. Since the N+ of the contact region (211/213/215) is performed after the contact etching, the heavily doped contact region (211/213/215) is confined to a small-area contact region.

以下係說明在30V下操作的一NAND快閃記憶體之高壓元件的其中一種設計規則。但,以下提出之相關參數數值係僅為例示之用,並非限制保護範圍之用。如第10圖所示,一實施例之一高壓半導體元件中,其通道長度Lg可約1.2μm至約2μm以支撐最大操作電壓30V。一實施例中,從接觸區域(即N+,第一接觸區域211及第二接觸區域213)到多晶矽閘極(即第一護部 2011及第二護部2012)的最小距離係記為doffset,其距離doffset係約0.5μm至約1μm以提供足夠的N+汲極偏移(N+drain offset),因而降低GIDL(gate induced drain leakage)引起的崩潰。一實施例中,距離doffset係約0.8μm。再者,一實施例中,第一接觸區域211和/或第二接觸區域213其中之一(即每一汲極/源極)具有約0.1μm×0.1μm之面積。一實施例中,第一護部2011和第二護部2012的最小寬度W2約0.2μm。因此,對一實施例之高壓半導體元件而言,距離doffset(約0.5μm至1μm)與寬度W2(約0.2μm)的關係可表示為2.5×W2doffset 5×W2。一實施例中,最小通道寬度W’約2.1μm。再者,相鄰主動元件20的空間(具有P型摻雜達到場絕緣)(假設S1=S2=S)係具有最小距離約1μm。 The following is a description of one of the design rules for a high voltage component of a NAND flash memory operating at 30V. However, the relevant parameter values set forth below are for illustrative purposes only and are not intended to limit the scope of protection. As shown in Fig. 10, in a high voltage semiconductor device of an embodiment, the channel length Lg may be about 1.2 μm to about 2 μm to support a maximum operating voltage of 30V. In one embodiment, the minimum distance from the contact regions (ie, N+, first contact region 211 and second contact region 213) to the polysilicon gate (ie, the first guard portion 2011 and the second guard portion 2012) is denoted by d offset The distance d offset is about 0.5 μm to about 1 μm to provide a sufficient N+drain offset, thus reducing the collapse caused by GEDL (gate induced drain leakage). In one embodiment, the distance d offset is about 0.8 μm. Moreover, in one embodiment, one of the first contact regions 211 and/or the second contact regions 213 (ie, each drain/source) has an area of about 0.1 μm×0.1 μm. In one embodiment, the minimum width W2 of the first guard portion 2011 and the second guard portion 2012 is about 0.2 μm. Therefore, for the high voltage semiconductor device of an embodiment, the relationship of the distance d offset (about 0.5 μm to 1 μm) and the width W2 (about 0.2 μm) can be expressed as 2.5 × W 2 . d offset 5 × W2. In one embodiment, the minimum channel width W' is about 2.1 [mu]m. Furthermore, the space of adjacent active elements 20 (with P-type doping to achieve field insulation) (assuming S1 = S2 = S) has a minimum distance of about 1 [mu]m.

雖然上述實施例中係以第一井具有P型導電態和輕摻雜區域22具有N-導電態,但本揭露並不以此為限。對一PMOS製程,亦可應用本揭露,只要反轉井和接面的摻雜導電態即可。例如NMOS元件的P型井和N型輕摻雜區域22,在PMOS元件時取代為N型井和P型輕摻雜區域。因此,一CMOS中可包括共享一P型井之多個NMOS元件,和共享一N型井之多個PMOS元件。第11圖係繪示本揭露一實施例之其中一種可應用之包括多個主動元件之CMOS的佈局。對大型元件的一CMOS佈局設計,可將共享一P型井之多個NMOS元件和共享一N型井之多個PMOS元件分隔開來,如第11圖所示。 Although the first well has a P-type conductive state and the lightly doped region 22 has an N-conductive state in the above embodiment, the disclosure is not limited thereto. For a PMOS process, the present disclosure can also be applied as long as the doped conductive state of the well and the junction is reversed. For example, the P-well of the NMOS device and the N-type lightly doped region 22 are replaced by an N-well and a P-type lightly doped region in the PMOS device. Therefore, a CMOS may include a plurality of NMOS devices sharing a P-type well, and a plurality of PMOS devices sharing an N-type well. FIG. 11 is a diagram showing a layout of a CMOS including a plurality of active elements, which is applicable to an embodiment of the present disclosure. A CMOS layout design for large components separates multiple NMOS components sharing a P-well from multiple PMOS components sharing an N-well, as shown in Figure 11.

再者,實施例之主動元件亦可容易地形成於薄主體 的矽覆絕緣(SOI,silicon-on-insulation)晶圓上。 Furthermore, the active component of the embodiment can also be easily formed on a thin body On silicon-on-insulation (SOI) wafers.

擴散區域隔離(DIF isolation)可以在多晶矽蝕刻(自對準蝕刻)以形成導電護欄結構201時製作,因此,空間(S1/S2)可以進一步縮小。由於沒有井分離(well isolation)的考量,有可能可以在鄰近區域設計N/P MOSFET以使佈局最佳化。再者,由於缺少體接觸(body contact)而屬浮動基體(floating-body)MOSFET。 DIF isolation can be fabricated during polysilicon etch (self-aligned etch) to form the conductive barrier structure 201, and thus the space (S1/S2) can be further reduced. Since there is no well isolation considerations, it is possible to design N/P MOSFETs in adjacent areas to optimize the layout. Furthermore, it is a floating-body MOSFET due to the lack of body contact.

<相關實驗、模擬和結果> <Related experiments, simulations and results>

許多相關實驗和模擬(例如電腦輔助設計與模擬軟體Technology Computer Aided Design,“TCAD”)係用來觀察實施例佈局設計之結果,以下係提出其中幾種證明實施例之佈局設計具有優異效果(例如主動元件之間具有良好的場絕緣,無STI電晶體的極微量之汲極電流等)。第12A-12D圖分別繪示根據TCAD模擬實驗之一實施例之無STI電晶體的立體圖、及沿YZ-平面、XZ-平面和XY-平面之剖面圖。請同時參照第4圖和前述相關參數之內容說明。在TCAD模擬實驗中,以“Gate 1”和“Gate 2”代表兩相鄰主動元件,且相關參數包括:GOX(閘極氧化物)=7nm,SPR=60nm,Lg(通道長度)=0.4μm,W1=0.2μm,W2=0.1μm,擴散接點(即N+,第一接觸區域211和第二接觸區域213)=0.1μm×0.1μm,P型丼到主動區域(AA)之距離=0.5μm,重摻雜濃度(HDD)=1×1020cm-3,輕摻雜濃度(LDD)=5×1018cm-3,N+閘極摻雜濃度=1×1020cm-3,P型丼摻雜濃度=6×1017cm-3,以及主動元件之間距(pitch)DP=0.68μm。 Many related experiments and simulations (such as Computer Aided Design, "TCAD") are used to observe the results of the layout design of the embodiment. The following is a summary of the layout design of several of the proven embodiments (eg Good field insulation between active components, no traces of silicon current in STI transistors, etc.). 12A-12D are respectively a perspective view of the STI-free transistor according to an embodiment of the TCAD simulation experiment, and a cross-sectional view along the YZ-plane, the XZ-plane, and the XY-plane. Please also refer to Figure 4 and the description of the relevant parameters. In the TCAD simulation experiment, "Gate 1" and "Gate 2" represent two adjacent active components, and related parameters include: GOX (gate oxide) = 7 nm, SPR = 60 nm, Lg (channel length) = 0.4 μm , W1=0.2 μm, W2=0.1 μm, diffusion contact (ie, N+, first contact region 211 and second contact region 213)=0.1 μm×0.1 μm, distance of P-type 主动 to active region (AA)=0.5 Μm, heavy doping concentration (HDD) = 1 × 10 20 cm -3 , light doping concentration (LDD) = 5 × 10 18 cm -3 , N + gate doping concentration = 1 × 10 20 cm -3 , P The erbium doping concentration = 6 × 10 17 cm -3 , and the active element pitch (pitch) = 0.68 μm.

第13A圖繪示TCAD模擬實驗中實施例之無STI電晶體之ID-VG特性曲線。其中,係施加電壓Vg1和Vg2於實施例之無STI電晶體“Gate 1”和“Gate 2”元件。第13A圖中,兩TID-VG特性曲線係分別由施加0V之Vg1和3.8V之Vg2的電壓而得。根據第13A圖的結果,變化施加於標示“Gate 2”之元件的偏壓並不會改變標示“Gate 1”之元件的ID-VG特性曲線,因此可證明實施例提供了良好的場絕緣。第13B圖是“Gate 1”和“Gate 2”元件中施加Vg1=0.5V、Vg2=3.8V和Vds=0.1V之電流密度模擬示意圖。從第13B圖之電流密度模擬可知,汲極電流大部分是沿最短距離之路徑流動,因此也可以將有效通道寬度視為等於W1。 Fig. 13A is a graph showing the I D -V G characteristic curve of the STI-free transistor of the embodiment in the TCAD simulation experiment. Among them, the voltages Vg1 and Vg2 are applied to the STI-free transistor "Gate 1" and "Gate 2" elements of the embodiment. In Fig. 13A, the two TI D - V G characteristic curves are obtained by applying a voltage of Vg1 of 0V and Vg2 of 3.8V, respectively. According to the result of Fig. 13A, the variation of the bias applied to the element labeled "Gate 2" does not change the I D - V G characteristic of the element labeled "Gate 1", thus demonstrating that the embodiment provides a good field insulation. Figure 13B is a schematic diagram showing the simulation of the current density of Vg1 = 0.5V, Vg2 = 3.8V, and Vds = 0.1V in the "Gate 1" and "Gate 2" elements. From the current density simulation of Fig. 13B, it is known that most of the drain current flows along the path of the shortest distance, so the effective channel width can also be regarded as equal to W1.

第14A圖繪示TCAD模擬實驗中實施例之無STI電晶體之ID-VG特性曲線,其中係變化不同寬度W2為0.1μm、0.15μm和0.2μm。第14A圖中,無STI電晶體之相關參數包括:Vds=0.1V,Vg2=3.8V,W1=0.2μm,Lg=0.4μm和P型丼摻雜濃度=6×1017cm-3。第14B圖繪示TCAD模擬實驗中實施例之無STI電晶體之ID-VG特性曲線,其中係變化不同通道長度Lg為0.25μm、0.3μm和0.4μm。第14B圖中,無STI電晶體之相關參數包括Vds=0.1V,Vg2=3.8V,W1=0.2μm,W2=0.1μm,和P型丼摻雜濃度=6×1017cm-3。第14A圖和第14B圖之結果係指出窄通道(narrow-width)效應和短通道(short-channel)效應是鏡向的。再者,當W2=0.2um,主動元件之間的空間距離可以減縮至僅0.08μm,且也沒有觀察到會引起注意的漏電流增加幅度。 Fig. 14A is a graph showing the I D -V G characteristic of the STI-free transistor of the embodiment in the TCAD simulation experiment, wherein the system has different widths W2 of 0.1 μm, 0.15 μm and 0.2 μm. In Fig. 14A, the relevant parameters of the STI-free transistor include: Vds = 0.1 V, Vg2 = 3.8 V, W1 = 0.2 μm, Lg = 0.4 μm, and P-type erbium doping concentration = 6 × 10 17 cm -3 . Fig. 14B is a graph showing the I D -V G characteristic of the STI-free transistor of the embodiment in the TCAD simulation experiment, wherein the system changes the channel length Lg to 0.25 μm, 0.3 μm and 0.4 μm. In Fig. 14B, the relevant parameters of the STI-free transistor include Vds = 0.1 V, Vg2 = 3.8 V, W1 = 0.2 μm, W2 = 0.1 μm, and P-type erbium doping concentration = 6 × 10 17 cm -3 . The results of Figures 14A and 14B indicate that the narrow-width effect and the short-channel effect are mirrored. Furthermore, when W2 = 0.2 um, the spatial distance between the active elements can be reduced to only 0.08 μm, and no increase in the leakage current that causes attention is observed.

第15A圖為TCAD模擬實驗中,一實施例之無STI電晶體沿著XY-平面之剖面圖,其中係在主動元件的接觸區域上標示施加電壓。第15B-15D圖繪示TCAD模擬實驗中實施例之無STI電晶體之ID-VG特性曲線,其中第15B圖之Vg2=0V和Vd1=0.1V,第15C圖之Vg2=0V和Vd1=3.8V,第15D圖之Vg2=3.8V和Vd1=0.1V,以及第15E圖之Vg2=3.8V和Vd1=3.8V。根據第15B-15D圖之模擬實驗結果顯示,不論偏壓狀況,電晶體”Gate-2”的都維持極微小的汲極電流,表示有優異的場絕緣效果。 Figure 15A is a cross-sectional view of the STI-free transistor of the embodiment along the XY-plane in a TCAD simulation experiment in which the applied voltage is indicated on the contact area of the active device. 15B-15D are diagrams showing the I D -V G characteristic curve of the STI-free transistor of the embodiment in the TCAD simulation experiment, wherein Vg2=0V and Vd1=0.1V in Fig. 15B, Vg2=0V and Vd1 in Fig. 15C = 3.8 V, Vg2 = 3.8 V and Vd1 = 0.1 V in Fig. 15D, and Vg2 = 3.8 V and Vd1 = 3.8 V in Fig. 15E. According to the simulation results of Fig. 15B-15D, the transistor "Gate-2" maintains a very small drain current regardless of the bias condition, indicating excellent field insulation effect.

第16圖繪示TCAD模擬實驗中實施例之無STI電晶體中之I-Vd1特性曲線,其中Vg2=3.8V和Vg1=3.8V,且Id1曲線代表電晶體”Gate-1”的汲極電流,Id2曲線代表電晶體”Gate-2”的汲極電流,以及Ip-well曲線代表P型井的電流。根據第16圖之模擬實驗結果顯示,當Vd1增加時,P型井電流也隨之上升。但即使當Vd1增加至8V時,電晶體”Gate-2”的汲極電流Id2仍維持無限小。 Figure 16 is a graph showing the IV d1 characteristic curve in the STI-free transistor of the embodiment in the TCAD simulation experiment, wherein Vg2 = 3.8V and Vg1 = 3.8V, and the Id1 curve represents the drain current of the transistor "Gate-1". The Id2 curve represents the drain current of the transistor "Gate-2" and the Ip-well curve represents the current of the P-well. According to the simulation experiment shown in Fig. 16, when the Vd1 is increased, the P-type well current also rises. But even when Vd1 is increased to 8V, the gate current Id2 of the transistor "Gate-2" remains infinitely small.

綜上所述,應用實施例之主動元件的半導體元件中,其各主動元件係利用一導電護欄結構(如多晶矽閘極)來定義通道長度和寬度。實施例之半導體元件可包括NMOS、PMOS或CMOS。對NMOS,N+接面係被導電護欄結構(如多晶矽閘極)包圍,因此使主動元件(無STI)可被導電護欄結構(如多晶矽閘極)而自隔離(self-isolated)。再者,導電護欄結構外側的區域(即擴散 區域DIF)可以摻雜P型不純物以達到場絕緣。實施例之半導體佈局設計可使半導體元件完全免除於任何STI邊緣效應,例如雙峰次臨界漏電流、崩潰電壓下降、不同STI佈局之差異等等,而可成功地解決傳統半導體元件會遭遇到STI邊緣效應的問題。再者,由於實施例的主動元件沒有如傳統之擴散區域DIF和多晶矽閘極之間交疊和延伸方式的存在,因此主動元件的設置間距(pitch)得以再進一步縮減。另外,模擬實驗的結果也證明了實施例之半導體元件可達到良好的場絕緣以及無法引起注意的漏電流增幅。 In summary, in the semiconductor device of the active device of the embodiment, each active device uses a conductive barrier structure (such as a polysilicon gate) to define the channel length and width. The semiconductor component of an embodiment may include NMOS, PMOS, or CMOS. For NMOS, the N+ junction is surrounded by a conductive barrier structure (such as a polysilicon gate), thus allowing the active component (without STI) to be self-isolated by a conductive barrier structure (such as a polysilicon gate). Furthermore, the area outside the conductive barrier structure (ie, diffusion) The region DIF) can be doped with P-type impurities to achieve field insulation. The semiconductor layout design of the embodiment can completely eliminate the semiconductor components from any STI edge effects, such as bimodal sub-critical leakage current, breakdown voltage drop, difference in different STI layouts, etc., and can successfully solve the traditional semiconductor components encounter STI The problem of edge effects. Moreover, since the active elements of the embodiment do not overlap and extend as in the conventional diffusion region DIF and the polysilicon gate, the pitch of the active elements is further reduced. In addition, the results of the simulation experiments also demonstrate that the semiconductor component of the embodiment can achieve good field insulation and an increase in leakage current that cannot be noticed.

綜上所述,雖然本發明已以實施例揭露如上,然其並非用以限定本發明。本發明所屬技術領域中具有通常知識者,在不脫離本發明之精神和範圍內,當可作各種之更動與潤飾。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。 In conclusion, the present invention has been disclosed in the above embodiments, but it is not intended to limit the present invention. A person skilled in the art can make various changes and modifications without departing from the spirit and scope of the invention. Therefore, the scope of the invention is defined by the scope of the appended claims.

20‧‧‧主動元件 20‧‧‧Active components

PW‧‧‧第一井 PW‧‧‧First Well

22‧‧‧輕摻雜區域 22‧‧‧Lightly doped areas

201‧‧‧導電護欄結構 201‧‧‧ Conductive guardrail structure

201m‧‧‧中間部 201m‧‧‧ middle part

2011‧‧‧第一護部 2011‧‧‧First Department

2012‧‧‧第二護部 2012‧‧‧Second Ministry

201a‧‧‧第一區域 201a‧‧‧First area

201b‧‧‧第二區域 201b‧‧‧Second area

211‧‧‧第一接觸區域 211‧‧‧First contact area

213‧‧‧第二接觸區域 213‧‧‧Second contact area

215‧‧‧第三接觸區域 215‧‧‧ Third contact area

S1‧‧‧第一隔離距離 S1‧‧‧first isolation distance

S2‧‧‧第二隔離距離 S2‧‧‧Second isolation distance

Dp‧‧‧主動元件之間距 Dp‧‧‧ active component spacing

Lg‧‧‧通道長度 Lg‧‧‧ channel length

W2‧‧‧第一護部和第二護部之寬度 W2‧‧‧Width of the first and second guards

W‧‧‧第一區域和第二區域之寬度 W‧‧‧Width of the first and second regions

Claims (10)

一種半導體元件,包括:一基板;一第一井具有一第一導電態並自該基板之一表面向下延伸;一擴散區域(diffusion region)摻雜該第一導電態之不純物並自該第一井之一表面向下延伸;複數個主動元件形成於該擴散區域內,且該些主動元件係彼此相距地設置,其中該些主動元件係藉由該擴散區域而彼此電性絕緣。 A semiconductor device comprising: a substrate; a first well having a first conductive state and extending downward from a surface of the substrate; a diffusion region doping the impurity of the first conductive state and from the first One of the wells extends downwardly; a plurality of active components are formed in the diffusion region, and the active components are disposed apart from each other, wherein the active components are electrically insulated from each other by the diffusion region. 如申請專利範圍第1項所述之半導體元件,其中該些主動元件之一包括:一導電護欄結構(conductive guarding structure)形成於該擴散區域上;和一輕摻雜區域(light doping region)具有一第二導電態,且該輕摻雜區域自該擴散區域之一表面向下延伸並對應地位於該導電護欄結構之內,其中相鄰之該些主動元件各包括該導電護欄結構,位於相鄰之該些主動元件之間的一隔離區域(isolating region)係由該些相鄰主動元件的該些導電護欄結構所定義。 The semiconductor component of claim 1, wherein one of the active components comprises: a conductive guarding structure formed on the diffusion region; and a light doping region a second conductive state, wherein the lightly doped region extends downward from a surface of the diffusion region and is correspondingly located within the conductive barrier structure, wherein the adjacent active components each comprise the conductive barrier structure An isolating region between the adjacent active components is defined by the conductive barrier structures of the adjacent active components. 如申請專利範圍第2項所述之半導體元件,其中該導電護欄結構包括:一中間部(middle portion),其中該中間部係作為該主動元件之一閘極,且該中間部沿著一第一方向具有一通道寬度(channel width,W’)和沿著一第二方向具有一通道長度(channel length,Lg);一第一護部(first guarding portion),連接該中間部之一側以定義位於該擴散區域之一第一區域(first region),其中該第一區域係由該第一護部和該中間部圍繞而成;和一第二護部(second guarding portion),與該第一護部相對並連接該中間部之另一側以定義位於該擴散區域之一第二區域(second region),其中該第二區域係由該第二護部和該中間部圍繞而成,其中該第一區域和該第二區域係位於該輕摻雜區域內,而該第一區域和該第二區域係相隔開該通道長度之一距離。 The semiconductor device of claim 2, wherein the conductive barrier structure comprises: a middle portion, wherein the intermediate portion serves as a gate of the active device, and the intermediate portion is along a first One direction has a channel width (channel Width, W') and having a channel length (Lg) along a second direction; a first guarding portion connecting one side of the intermediate portion to define one of the diffusion regions a first region, wherein the first region is surrounded by the first guard portion and the intermediate portion; and a second guarding portion opposite to the first guard portion and connected to the middle portion The other side of the portion is defined as a second region of the diffusion region, wherein the second region is surrounded by the second guard portion and the intermediate portion, wherein the first region and the second region The region is located within the lightly doped region, and the first region and the second region are separated by a distance from the length of the channel. 如申請專利範圍第3項所述之半導體元件,其中該些主動元件所述之一更包括:一第一接觸區域(first contact region)具有該第二導電態並形成於該導電護欄結構之該第一區域內,且該第一接觸區域係與該第一護部和該中間部相距;一第二接觸區域(second contact region)具有該第二導電態並形成於該導電護欄結構之該第二區域內,且該第二接觸區域係與該第二護部和該中間部相距;和一第一接點(first contact)形成於該第一接觸區域,以及一第二接點(second contact)形成於該第二接觸區域。 The semiconductor device of claim 3, wherein one of the active elements further comprises: a first contact region having the second conductive state and formed on the conductive barrier structure In the first region, the first contact region is spaced apart from the first guard portion and the intermediate portion; a second contact region has the second conductive state and is formed in the conductive fence structure In the two regions, the second contact region is spaced apart from the second guard portion and the intermediate portion; and a first contact is formed in the first contact region, and a second contact (second contact) ) formed in the second contact region. 如申請專利範圍第1項所述之半導體元件,其中當該半導體元件為一低壓(LV)元件時,相鄰之該些主動元件之間的一間 距(space,S)係在0.18μm to 0.28μm之範圍內;當該半導體元件為一高壓(HV)元件時,相鄰之該些主動元件之間的一間距(space,S)係在0.8μm to 1.2μm之範圍內。 The semiconductor device of claim 1, wherein when the semiconductor device is a low voltage (LV) device, a space between adjacent ones of the active devices The space (S) is in the range of 0.18 μm to 0.28 μm; when the semiconductor component is a high voltage (HV) component, a space (S) between adjacent active components is 0.8. Within the range of μm to 1.2μm. 如申請專利範圍第1項所述之半導體元件,其中相鄰之該些主動元件之間的一間距(space,S)處係無淺溝渠隔離(Shallow trench isolation,STI)。 The semiconductor device according to claim 1, wherein a space (S) between adjacent ones of the active elements is not shallow trench isolation (STI). 一主動元件,形成於一基板處之具有一第一導電態的一擴散區域內,該主動元件包括:一導電護欄結構(conductive guarding structure),包括:一中間部(middle portion);一第一護部(first guarding portion),連接該中間部之一側以定義位於該擴散區域之一第一區域(first region),其中該第一區域係由該第一護部和該中間部圍繞而成;和一第二護部(second guarding portion),與該第一護部相對並連接該中間部之另一側以定義位於該擴散區域之一第二區域(second region),其中該第二區域係由該第二護部和該中間部圍繞而成;一第一接觸區域(first contact region)具有一第二導電態並形成於該導電護欄結構之該第一區域內,且該第一接觸區域係與該第一護部和該中間部相距;和一第二接觸區域(second contact region)具有該第二導電態並 形成於該導電護欄結構之該第二區域內,且該第二接觸區域係與該第二護部和該中間部相距。 An active component is formed in a diffusion region of a substrate having a first conductive state, the active component comprising: a conductive guarding structure, including: a middle portion; a first a first guarding portion, connected to one side of the intermediate portion to define a first region located in the diffusion region, wherein the first region is surrounded by the first guard portion and the intermediate portion And a second guarding portion opposite to the first guard and connected to the other side of the intermediate portion to define a second region of the diffusion region, wherein the second region Formed by the second guard portion and the intermediate portion; a first contact region has a second conductive state and is formed in the first region of the conductive fence structure, and the first contact The region is spaced apart from the first guard and the intermediate portion; and a second contact region has the second conductive state and Formed in the second region of the conductive barrier structure, and the second contact region is spaced from the second guard portion and the intermediate portion. 如申請專利範圍第7項所述之主動元件,其中該中間部係作為該主動元件之一閘極,且該中間部沿著一第一方向具有一通道寬度(channel width,W’)和沿著一第二方向具有一通道長度(channel length,Lg),而該第一區域和該第二區域係相隔開該通道長度之一距離;而該主動元件更包括:一輕摻雜區域(light doping region)具有該第二導電態,且該輕摻雜區域自該擴散區域之一表面向下延伸並位於對應該導電護欄結構之內,其中該第一區域和該第二區域係位於該輕摻雜區域內;一第一接點(first contact)形成於該第一接觸區域,以及一第二接點(second contact)形成於該第二接觸區域,其中圍繞該主動元件之一周邊區域(peripheral area)係為重摻雜該第一導電態的該擴散區域且無淺溝渠隔離(Shallow trench isolation,STI)。 The active component of claim 7, wherein the intermediate portion serves as a gate of the active component, and the intermediate portion has a channel width (W') and along a first direction. The second direction has a channel length (Lg), and the first area and the second area are separated by a distance of the length of the channel; and the active component further comprises: a lightly doped area (light The doping region has the second conductive state, and the lightly doped region extends downward from a surface of the diffusion region and is located within the corresponding conductive barrier structure, wherein the first region and the second region are located in the light a doped region; a first contact is formed in the first contact region, and a second contact is formed in the second contact region, wherein a peripheral region of the active component is surrounded ( The peripheral region is a heavily doped diffusion region of the first conductive state and has no shallow trench isolation (STI). 如申請專利範圍第7項所述之主動元件,其中該第一區域和該第二區域沿著一第一方向各具有一寬度W,和該第一護部和該第二護部沿著該第一方向各具有一寬度W2,而該主動元件之一有效通道寬度(effective channel width)係為W+2×W2。 The active element of claim 7, wherein the first area and the second area each have a width W along a first direction, and the first guard and the second guard follow the The first direction has a width W2, and one of the active elements has an effective channel width of W+2×W2. 如申請專利範圍第7項所述之主動元件,係為一高壓(HV)元件,其中該第一護部和該第二護部各具有一寬度W2,該 第一接觸區域和該第二接觸區域分別與該第一護部和該第二護部各相隔一距離doffset,其中2.5×W2doffset 5×W2。 The active component as described in claim 7 is a high voltage (HV) component, wherein the first guard portion and the second guard portion each have a width W2, the first contact region and the second contact The area is separated from the first guard part and the second guard part by a distance d offset , wherein 2.5×W2 d offset 5 × W2.
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US20110237035A1 (en) * 2004-07-15 2011-09-29 Jiang Yan Formation of Active Area Using Semiconductor Growth Process without STI Integration

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