TWI281192B - Power semiconductor structure capable of reducing on-state resistance and method of manufacturing the same - Google Patents

Power semiconductor structure capable of reducing on-state resistance and method of manufacturing the same Download PDF

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TWI281192B
TWI281192B TW94137626A TW94137626A TWI281192B TW I281192 B TWI281192 B TW I281192B TW 94137626 A TW94137626 A TW 94137626A TW 94137626 A TW94137626 A TW 94137626A TW I281192 B TWI281192 B TW I281192B
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region
type
resistance
impurity
channel region
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TW94137626A
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TW200717582A (en
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Yi-Yu Lin
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Dyna Image Corp
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Abstract

The present invention provides a power semiconductor (DMOS) structure capable of reducing on-state resistance (Ron) and method of manufacturing the same, which mainly employ an ion implantation means having a slanted implantation angle and enabling to select adequate implantation depth to directly implant impurity in a first conduction state into an epitaxial region affected by a junction field effect transistor (JFET) after completing etch of a polysilicon structure. The impurity in the first conduction state is blocked by the polysilicon structure and won't be directly implanted in a channel region; the channel region is immune to the influence of the increase amount of the impurity, and under the condition of a constant starting voltage, the length of the channel region can be shortened to reduce the resistance of the channel region; after increasing the amount of the impurity, the resistance on top of the epitaxial region can be further reduced.

Description

•1281192 -a 九、發明說明: 【發明所屬之技術領域】 ^ 本發明係關於—種功率半導體裝置的領域,尤其是指一 -·種可降低導通電阻(Ron)之功率半導體結構及其製造方法。 【先前技術】 ' 在半導體工業中,金氧半場效電晶體(MOS field effect φ tmnS1St〇r ’ M0SFET)是一種已知的功率半導體裝置,而該 金氧半場效電晶體的其中一種型態則是雙擴散型場效電晶 體’又稱作雙擴散金屬氧化半導體(D〇uble Diffused Metal</ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> <RTIgt; method. [Prior Art] In the semiconductor industry, a MOS field effect φ tmnS1 St〇r 'MOSS is a known power semiconductor device, and one of the types of the MOS field-effect transistor is Is a double diffused field effect transistor 'also known as double diffused metal oxide semiconductor (D〇uble Diffused Metal

Oxide Semiconductor,DMOS)結構(下稱:DMOS 結構), 其中該DMOS結構係包括n型通道之DMOS結構及p型通 這之DMOS結構,另一種相似於該金氧半場效電晶體的功率 半$體叙置’即稱作絕緣閘雙極性電晶體(Insulate(j Gate • BlPolar Transistor,IGBT)(下稱:IGBT 結構),主要優點 在於其被驅動所消耗電功率非常小,故大多不需要另加散熱 裝置,即可小形化,俾符合現代電子產品愈來愈輕薄短小的 基本要求。但由於現今電子產品的日新月異,且對低消耗功 率及咼頻率化的要求也愈趨嚴格,故如何有效地改良功率半 導體裝置,使其擁有超低導通電阻,已成為該技術領域之重 點發展方向。 如第一圖所示,其為該n型通道之DM〇s結構的一般構 5 1281192 造圖。該DMOS結構係包括:η型汲極區域1 〇 a (矽晶圓 基板)、形成於該汲極區域1 〇 a上端之n型磊晶區域(層) (n-type epitaxial layer) 2 0 a、形成於該磊晶區域 2 〇 a 頂部之p型體區域(p-type body) 3 0 a、形成於該體區域 3 0 a頂部之源極區域(source regi〇ns) 4 〇 a,以及形成 於該磊晶區域2 0 a上端之閘極區域5〇a (其包括絕緣層 及多晶矽結構);其中,該閘極區域5 〇 a下端係部份重疊於 該源極區域40a,且延伸遮蔽於該體區域3〇a的部份表 面。另外’位於該閘極區域5 〇 a下端之該體區域3 〇 a的 表面可定義為通道區域3 :[ a,且該磊晶區域2 〇 a之頂部 的表面區域一般可稱為接面場效電晶體(Juncti〇n Field Effect Transistor,JFET)區域(下稱:JFET 區域)。 再者’該DMOS結構之源極區域4 〇 a到汲極區域1 〇 a間的阻抗稱為導通電阻(〇n_state resistance,R〇n),該導 通電阻主要包括:通道區域3丄a的電阻R1、JFET區域的 電阻R2、磊晶區域2 〇 a的電阻R3,以及汲極(基板)區 域1 0 a的電阻R4等;其中,對該j)MOS結構之整體導通 電阻(Ron)最具影響力的阻抗,乃在於該磊晶區域之頂部 的電阻(即指JFET區域或通道區域的電阻)。 如第二圖所示,係為_種習知為了降低該JFET區域之 電阻所發展出來的製造方法,即主要是在形成該閘極區域5 6 1281192 0 a之前’利用離子植入或其它擴散方式,將^型不純物垂 直向下植入至該磊晶區域頂部之JFET區域或通道區域,以 . 增加该JFET區域之η型摻質濃度,而降低該jfeT區域的電 • 阻R2 ’並達到降低該DMOS結構之導通電阻的目的者。 • 惟’利用上述方法,雖可降低該JFET區域的電阻,但 南劑虿之n型不純物亦將同時中和該體區域3 〇 a頂部之p _ 型不純物,而後降低該體區域3 〇 a頂部之p型摻質濃度, 即因该η型不純物直接植入該通道區域3 1 a所在的位置, 使得該通這區域3 1 a外緣向内推入(pushing_in)該體區域 30a (如第二圖之j部份所示);然而,隨著不純物之劑量 的增加,该通道區域3 1 a的濃度將逐漸變淡,同時開始降 低啟始電壓(Threshold Voltage,Vt),且使該結構更容易受 到擊穿(punch-through )效應的影響,而造成崩潰電壓 ·( Breakdown Voltage )降低的現象。 因此,上述方法將受限於JFET區域之離子植入摻質或 不純物(D0se)的增加量,以致於該JFET區域之電阻的降 …低是有限的,故如何更有效地降低該DM〇s結構之導通電 阻’即為長期以來所面臨並欲解決的課題之一。 有鑑於斯,發明人係根據「習知降mDMOS結構之導通 电阻(R〇n)的製造方法」的缺失,且基於不受該JFET區域 之離子植入摻質(Dose)增加量的影響為前提考量下,並累 7 1281192 積多年之試製與實作,終能發展出一種創新之「可降低導通 .電阻之雙擴散金屬氧化半導體的製造方法」,俾以解決上述之 , 缺失者。 【發明内容】 . 本發明之目的,在於提供一種可降低導通電阻(R0n) ⑩之功率半導體結構及其製造方法,其主要是為了降低肌丁 區域之離子植入(ion implantation)(下稱:jfet IMP)對 崩/貝電壓及啟始電壓(Vt)的影響,進而可增加該Oxide Semiconductor (DMOS) structure (hereinafter referred to as DMOS structure), wherein the DMOS structure includes a DMOS structure of an n-type channel and a DMOS structure of a p-type pass, and the other is similar to the power of the MOS half-effect transistor. The body is called 'Insulate (j Gate • BlPolar Transistor, IGBT) (hereinafter referred to as: IGBT structure), the main advantage is that the electric power consumed by it is very small, so most of them do not need to be added. The heat sink can be miniaturized, which meets the basic requirements of modern electronic products, which are becoming lighter, thinner and shorter. However, due to the rapid changes in electronic products today and the stricter requirements for low power consumption and frequency, how to effectively Improving the power semiconductor device to have ultra-low on-resistance has become a key development direction in the field of technology. As shown in the first figure, it is a general structure of the DM 〇s structure of the n-type channel 51281192. The DMOS structure includes an n-type drain region 1 〇a (矽 wafer substrate), and an n-type epitaxial region (layer) formed at the upper end of the drain region 1 〇a (n-type epitaxial la) Yer) 20 a, a p-type body formed at the top of the epitaxial region 2 〇a 3 0 a, a source region formed at the top of the body region 3 0 a (source regi〇ns) 4 〇a, and a gate region 5〇a (which includes an insulating layer and a polysilicon structure) formed at an upper end of the epitaxial region 20 a; wherein a lower portion of the gate region 5 〇a partially overlaps the source a region 40a extending over a portion of the surface of the body region 3a. Further, a surface of the body region 3a at the lower end of the gate region 5a can be defined as a channel region 3: [a, and The surface area at the top of the epitaxial region 2 〇a is generally referred to as a Junctified Field Effect Transistor (JFET) region (hereinafter referred to as the JFET region). Further, the source region of the DMOS structure 4 The impedance between 〇a and the drain region 1 〇a is called the on-resistance (〇n_state resistance, R〇n). The on-resistance mainly includes: the resistor R1 of the channel region 3丄a, the resistor R2 of the JFET region, and the epitaxial layer. a resistor R3 of the region 2 〇a, and a resistor R4 of the drain region (substrate) region 10 a; The most influential impedance of the overall on-resistance (Ron) of the j) MOS structure is the resistance at the top of the epitaxial region (i.e., the resistance of the JFET region or the channel region). As shown in the second figure, it is a conventional manufacturing method developed to reduce the resistance of the JFET region, that is, mainly by using ion implantation or other diffusion before forming the gate region 5 6 1281192 0 a. In a manner, the impurity is implanted vertically downward to the JFET region or the channel region at the top of the epitaxial region to increase the n-type dopant concentration of the JFET region, and reduce the electrical resistance R2' of the jfeT region and reach The purpose of reducing the on-resistance of the DMOS structure. • Only by using the above method, although the resistance of the JFET region can be reduced, the n-type impurity of the south agent will simultaneously neutralize the p _ type impurity at the top of the body region 3 〇a, and then lower the body region 3 〇a The p-type dopant concentration at the top, that is, because the n-type impurity is directly implanted in the position of the channel region 31a, such that the outer edge of the region 3p is pushed-inwardly (pushing_in) the body region 30a (eg As shown in part j of the second figure; however, as the dose of the impurity increases, the concentration of the channel region 3 1 a will gradually fade, and at the same time, the threshold voltage (Vt) will be lowered, and the The structure is more susceptible to the punch-through effect and causes a breakdown of the Breakdown Voltage. Therefore, the above method will be limited by the amount of ion implantation dopant or impurity (D0se) in the JFET region, so that the drop in the resistance of the JFET region is limited, so how to reduce the DM〇s more effectively. The on-resistance of the structure is one of the issues that have been faced and solved for a long time. In view of the fact, the inventors are missing from the "method of manufacturing the on-resistance (R〇n) of the conventional mDMOS structure, and are based on the influence of the increase in the ion implantation dopant (Dose) of the JFET region. Under the premise, and the accumulation of 7 1281192 years of trial production and implementation, we can finally develop an innovative "can reduce the conduction and resistance of the double-diffused metal oxide semiconductor manufacturing method", in order to solve the above, the missing. SUMMARY OF THE INVENTION An object of the present invention is to provide a power semiconductor structure capable of reducing on-resistance (R0n) 10 and a method of fabricating the same, which are mainly for reducing ion implantation in a muscle region (hereinafter referred to as: Jfet IMP) affects the collapse/beauty voltage and the starting voltage (Vt), which in turn increases

JFET IMP 的办貝或不純物(Dose)量,並達到降低該DM〇s結構之導 ' 通電阻的目的者。 本發明之製造方法,主要在多㈣(p。㈣麵)結構 之餘刻(eteh)完成後,利用具傾斜角度之離子植入方式, φ 肸第傳$型恶(其中,在n型通道之DM〇s中,第一傳導 為η型’第—傳導型態為p型,·在p型通道之讀⑽中, 弟—傳導型態為p型,第二傳導型態為不純物傾斜地 植入該蟲晶區域頂部之;FET區域,此時該第—傳導型態之 不純物可選擇適當之植人深度,而直接植人(或擴散至)受 JFET影響之蠢晶區域,且該第—傳導型態之不純物將受到該 閘極區域的阻擋’而不會直接植人該低濃度的第二傳導型能 之體區域(即通道區域),故可維持原來的啟始電壓(Vt/ 8 1281192 且不致因擊穿(punch-through )效應的影響,而造成崩潰電 壓(Breakdown Voltage )降低的現象。 / 再者,利用本發明之製造方法所形成之一種功率半導體 - 結構,其可應用於DMOS結構或IGBT結構,包括一基板; 弟一傳導型悲之蟲晶區域’係形成於該基板的上端;一閑 . 極區域,係形成於該磊晶區域的上端;一個或複數個第二傳 鲁 導型態之體區域,係形成於該磊晶區域的頂部;複數個源極 區域,係形成於該體區域的頂部;其中該體區域的上表面設 有一通道區域,該通道區域係被遮蔽於該閘極區域的下端; 、 以及一第一傳導型態之中濃度磊晶區域,係利用具傾斜植入 角度及可選擇植入深度之離子植入方式,形成於受接面場效 電晶體(JFET )影響之蠢晶區域内。 藉此,該通道區域將不受該jFET IMP之摻質或不純物 _ J曰加里的影響’且崩潰電壓(Breakdown Voltage )及啟始電 壓(Vt)將不會改變,故可縮短該通道區域的長度,進而降 低該通道區域的電阻,同時當增加該JFET IMp之摻質或不 純物量時,則該磊晶區域頂部之JFET區域的電阻亦將會被 ' 降低。 【實施方式】 本發明係以η型通道之DMOS結構(即使用第一傳導型 9 1281192 _ 怨之基板,其中第一傳導型態為,第二傳導型態為p型) 為其中一種貫施態樣,而本發明亦應用於等效結構變化之p . 型通逼之DMOS結構(即使用第一傳導型態之基板,其中第 傳導型態為P型,第二傳導型態為^型),以及IGBt結構 : (即不同於該DMOS結構之處,僅在於使用第二傳導型態之 基板)。 _ 請參考第三A至三E圖,其為本發明之雙擴散金屬氧化 半導體(DMOS)的製造方法,依製造步驟描述如下: 如第二A圖所示,首先提供一矽晶圓(即為基板),其摻 減形成一第一傳導型態(n型)之高濃度汲極區域丄〇 ;利 用一反應氣體(由三氯矽烷及氫氣間的化學反應所產生)流 、’、I該基板的表面,以形成一邊界層;然後,該反應氣體會經 由邊邊界層而擴散,即利用m式,將單日日日⑦層成長於該 _ 基板之上端,以形成一第一傳導型態(η型)之低濃度蟲晶 區域2 0。 再者,如第三Β圖所示,利用薄膜、微影及蝕刻製程, 形成至少一閘極區域5 〇於該低濃度磊晶區域2 〇之上端; ”中该閘極區域5 〇係包括一多晶矽(p〇lysilic〇n)結構5 1及一絕緣層5 2。 如第三C圖所示,利用離子植入法或其它方式,將第二 傳&amp;型悲(P型)之不純物植入於該低濃度磊晶區域2 ◦的 10 -1281192 頂端’以形成一 p型之體(body )區域3〇 (其包括相鄰之 兩濃度體區域及低》辰度體區域)。 接者’如弟二D圖所不’再利用離子植入法或其它方式, 將第一傳導型態(η型)之不純物植入於該p型之體區域3 0的頂部,以形成至少二個η型之高濃度源極區域4 〇。其 中’於該Ρ型之體區域3 0的上表面,且於該高濃度源極區 域4 0與该體區域3 0邊緣内,形成有一通道區域3 1,其 長度為山,其中該通道區域3 1係被遮蔽於該閘極區域5 〇 的下端。 又,本發明最主要之技術手段,如第三Ε圖所示,進行 JFET 區域之離子植入(i〇I1 impiantati〇11)(下稱:JFET IMP),即利用具傾斜植入角度及可選擇適當植入深度之離子 植入方式,將第一傳導型態(η型)之不純物傾斜地植入該 φ DM0S結構的表面,然該η型不純物將受到該多晶矽結構5 1的阻擋,而不會直接植入該低濃度體區域(即為該 通道區域3 1 ),即直接進入該磊晶區域2 0頂部之JFET區 - 域(即受JFET影響之磊晶區域),以形成一第一傳導型態(η 型)之中/辰度蟲晶區域6 〇 (如第四圖所示)。藉此,可維持 原來的啟始電壓(Vt),且不致受到擊穿(pUnch-through)效 應的影V ’而造成崩潰電壓(Breakdown Voltage )降低的現 象。 11 1281192 一猎此,該通道區域3 1的長度可被縮短成d2,以降低該 通迢區域3 電阻;且當增加受JFET影響之蟲晶區域2 〇頂部的摻質量時(gp增加該JFET區域之n型摻 值),該JFET區域之雷阳介叮门斤、+牧y 又 P亦可同低’故透過該通道區 域3 1或該JFET區域夕+ ΛΑ攸化 $之電阻的降低,而可降低該DM〇S钍 構之導通餘(“),俾以細则知缺社目的者Γ &quot;綜上論述’本翻所提供之可降低導_岐雙 屬氧化半導體結構及其Ί i 衣k方法,確此有效地令該通道區域 父JFET IMP摻質量的影塑即為山 一 即在相潰fM及該啟始電 &amp;不會改變的條件下,而可以縮㈣通道區域的長度,^ 低通這區域的電阻,並在增加;FET跡之摻雜量的牛 亦可再降低該蟲晶區域頂部之肺τ區域的電阻;故其 可多得之發%,極具新祕及 /、' 請要件,爰依專利法提出巾,^心發明專利申 以保障創作者之權益。 木寻利, 惟以上料僅林糾之婦可行實 限本發明之專利範圍,故舉凡運用从m ^此即拘 運用本發明說明書及圖式内宏 予斤^等效結構變化,均同理皆包含於本發明之範圍内,合 1281192 【圖式簡單說明】 第一圖··係為習知雙擴散金屬氧化半導體(DMOS)結構的 \ 一般構造圖; ' 第二圖:係為習知受到JEFT IMP影響而使通道區域濃度變 、 淡的示意圖; 第—A圖至第二E圖:係根據本發明之製造方法,而降低雙 • 擴散金屬氧化半導體(DMOS)之導通電阻的製造 順序圖;以及 第四圖·係利用第三A圖至第三E圖所製造而成之可降低導 通電阻的雙擴散金屬氧化半導體結構。 【主要元件符號說明】JFET IMP's amount of domicile or impurity (Dose), and achieve the purpose of reducing the conduction resistance of the DM〇s structure. The manufacturing method of the present invention mainly uses the ion implantation method with an oblique angle after the completion of the multiple (four) (p. (four) plane) structure (eteh), and the φ 肸 first transmission type 恶 (wherein the n-type channel) In DM〇s, the first conduction is η-type, the first-conductivity type is p-type, and in the reading of p-type channel (10), the di-conductive type is p-type, and the second conduction type is impurely inclined. Into the top of the wormhole region; the FET region, at which time the impurity of the first conductivity type can be selected to appropriately implant depth, and directly implant (or diffuse into) the stray region affected by the JFET, and the first The impurity of the conduction type will be blocked by the gate region and will not directly implant the low-concentration body region of the second conductivity type (ie, the channel region), so that the original starting voltage can be maintained (Vt/8). 1281192 does not cause a breakdown of the breakdown voltage due to the effect of the punch-through effect. / Further, a power semiconductor structure formed by the manufacturing method of the present invention can be applied to DMOS structure or IGBT structure, including one a substrate; a conductivity-type sorrowful crystal region is formed at an upper end of the substrate; a free region is formed at an upper end of the epitaxial region; and one or a plurality of second-passed-type regions Formed on top of the epitaxial region; a plurality of source regions are formed on top of the body region; wherein the upper surface of the body region is provided with a channel region, the channel region being shielded from the gate region The lower end; and the concentration epitaxial region of the first conductivity type are formed by the interfacial field effect transistor (JFET) by using an ion implantation method with an oblique implantation angle and a selectable implantation depth. In the stray area, the channel area will not be affected by the jFET IMP's dopant or impurity _J曰 Gary, and the breakdown voltage and the starting voltage (Vt) will not change. The length of the channel region is shortened, thereby reducing the resistance of the channel region, and when the amount of dopant or impurity of the JFET IMp is increased, the resistance of the JFET region at the top of the epitaxial region is also reduced. The present invention is a DMOS structure of an n-type channel (i.e., using a substrate of a first conductivity type 9 1281192 _ complaint, wherein the first conductivity type is a p-type of the second conductivity type) is one of the modes. The present invention is also applicable to the DMOS structure of the p-type equivalent of the equivalent structural change (that is, the substrate using the first conductivity type, wherein the first conduction type is P type, and the second conduction type is ^ type), And the IGBt structure: (ie, different from the DMOS structure, only the substrate of the second conductivity type is used.) _ Please refer to the third to third E diagrams, which are double diffusion metal oxide semiconductors (DMOS) of the present invention. The manufacturing method is described as follows according to the manufacturing steps: As shown in FIG. 2A, a germanium wafer (ie, a substrate) is first provided, which is doped to form a high conductivity germanium region of a first conductivity type (n-type).丄〇; using a reaction gas (produced by a chemical reaction between trichlorosilane and hydrogen), ', I the surface of the substrate to form a boundary layer; then, the reaction gas will diffuse through the boundary layer, That is, using the m formula, the 7th floor of the day is grown in the day. _ The upper end of the substrate to form a low concentration insect crystal region 20 of a first conductivity type (n-type). Furthermore, as shown in the third figure, at least one gate region 5 is formed on the upper end of the low-concentration epitaxial region 2 利用 by a thin film, a lithography, and an etching process; "the gate region 5 includes a polycrystalline germanium (p〇lysilic) structure 5 1 and an insulating layer 5 2 . As shown in the third C diagram, the second pass &amp; type sad (P type) impurity is used by ion implantation or other means. Implanted in the top end of 10 -1281192 of the low-concentration epitaxial region 2 以 to form a p-type body region 3〇 (which includes two adjacent concentration regions and a low-length body region). The second conductivity type (n-type) impurity is implanted on the top of the p-type body region 30 to form at least two, as in the case of the second image, or by other methods. Η-type high-concentration source region 4 〇, wherein 'the upper surface of the body region 30 of the Ρ-type, and a channel region is formed in the high-concentration source region 40 and the edge of the body region 30 3 1, the length of which is a mountain, wherein the channel region 3 1 is shielded at the lower end of the gate region 5 。. Further, the present invention The main technical means, as shown in the third figure, is to perform ion implantation in the JFET region (i〇I1 impiantati〇11) (hereinafter referred to as JFET IMP), that is, using an inclined implantation angle and selecting an appropriate implantation depth. In the ion implantation mode, the impurity of the first conductivity type (n-type) is obliquely implanted on the surface of the φ DM0S structure, and the n-type impurity is blocked by the polysilicon structure 51, and is not directly implanted. The low concentration body region (ie, the channel region 3 1 ), that is, the JFET region-domain (ie, the epitaxial region affected by the JFET) directly entering the top of the epitaxial region 20 to form a first conduction type (η) Type) Medium/Changing Insect Crystal Area 6 〇 (as shown in the fourth figure). By this, the original starting voltage (Vt) can be maintained without being affected by the pUnch-through effect. And the phenomenon that the breakdown voltage is reduced. 11 1281192 The length of the channel region 3 1 can be shortened to d2 to reduce the resistance of the wanted region 3; and when the crystal region affected by the JFET is increased 2 When the mass of the top of the 〇 is increased (gp increases the n of the JFET region) In addition, the JFET region of Leiyang Jieyumen, +mu y and P can also be low, so the resistance through the channel region 3 1 or the JFET region + + $ $ can be reduced, and can be reduced The DM〇S structure leads to the general ("), 俾 细则 细则 细则 细则 细则 细则 quot quot quot quot quot quot quot quot quot 综 综 综 综 综 综 综 综 综 综 综 综 综 综 综 综 综 综 综 本 本 本 本 本 本 本 本 本The method is effective to make the shadow of the parental JFET IMP doping quality of the channel region be that the mountain is in the condition that the phase collapse fM and the initiation power &amp; not change, and the length of the (four) channel region can be reduced. ^ The resistance of the low-pass region is increasing, and the doping amount of the FET trace can also reduce the resistance of the lung τ region at the top of the worm region; therefore, it can be used for a large amount of %. /, 'Please ask for a piece of paper, according to the patent law, and apply for a patent to protect the rights of the creator. Wood seeks profit, but only the above-mentioned materials are only applicable to the scope of patents of the present invention. Therefore, the application of the invention and the internal structure of the macro to the equivalent structure change are the same. All are included in the scope of the present invention, and 1281192 [Simplified description of the drawings] The first figure is a general structure diagram of a conventional double-diffused metal oxide semiconductor (DMOS) structure; 'Second figure: is a conventional Schematic diagram of the channel region concentration being changed by the influence of JEFT IMP; FIG. A to FIG. 2E: manufacturing order of reducing the on-resistance of double-diffused metal oxide semiconductor (DMOS) according to the manufacturing method of the present invention FIG. 4 is a double-diffused metal oxide semiconductor structure fabricated by using the third to third E-graphs to reduce the on-resistance. [Main component symbol description]

汲極區域Bungee area

蟲晶區域Insect crystal region

4〇a 體區域4〇a body area

源極區域 閘極區域Source region gate region

没極區域 體區域 源極區域 4 0 多晶石夕結構Osmotic region body region source region 4 0 polycrystalline stone structure

蟲晶區域 通道區域 閘極區域 絕緣層Insect crystal region channel region gate region insulation layer

13 1281192 中濃度磊晶區域13 1281192 medium concentration epitaxial region

Claims (1)

1281192 十、申請專利範圍: 1、 一種可降低導通電阻之功率半導體結構的製造方 ' 法,包括下列步驟: ' 提供一基板; 形成一第一傳導型態之磊晶區域於該基板的上端; • 形成一閘極區域於該磊晶區域的上端; • 形成一個或複數個第二傳導型態之體區域於該磊晶區域的頂 部; 形成複數個源極區域於該體區域的頂部;其中該體區域 的上表面設有一通道區域,該通道區域係被遮蔽於該閘極區 域的下端;以及 利用具傾斜植入角度及可選擇植入深度之離子植入方 式’將第一傳導型態之不純物傾斜植入(或擴散至)受接面 ♦場效兒晶體(JFET)影響之蟲晶區域内,以形成一第一傳導 型恶之中濃度遙晶區域,且該不純物將受到該閘極區域的阻 擋,而不會直接植入該通道區域; - 轉此’該通道區域將不受該不純物增加量的影響,且在 啟始電壓不會改變的條件下,可縮短該通道區域的長度,並 了牦力u該蠢晶區域頂部的濃度。 2、 如申請專利範圍第1項所述之可降低導通電阻之功 卞半‘體結構的製造方法,其中該功率半導體結構係為η型 15 1281192 通道之雙擴散金屬氧化半導體(DMQS)結構,且讀夷板為 第—傳導型態之高濃度祕區域,該第—傳導·為:^、 第二傳導型態為p型。 3、如中請專利範圍第i項所述之可降低導通^ =半導體結構的製造方法,其中該功率半導體結構 ㈣之雙擴散金屬氧化半導體(DMqS)結構,_ =傳導型態之高濃纽極區域,該第—傳導型態為;型: 遠弟二傳導型態為η型。 Ρ 泡本2如巾請專利範圍第1項所述之可降低導通電阻之功 千半‘體結構的製造方法,並中 間隹μ + · ,、中如力4 +賴結構係為絕緣 閘又極性電晶體(IGB丁)結構, 高濃度沒極區域。 且縣板為弟二傳導型態之 5、-種可降低導通電阻之功率半導體結構,包括: 一基板; 昂-傳導型悲之悬晶區域,係形成於該基板的上端; —閘極區域,係形成於該磊晶區域的上端; —個或複數個第二傳導麵之體區域,係形成於該遙晶區域 的丁頁部; 品/夂數個源極區域’係形成於該體區域的頂部;其中該體 Μ的上表面$道區域,該通道區域係被遮蔽於該閑 極區域的下端;以及 161281192 X. Patent Application Range: 1. A method for fabricating a power semiconductor structure capable of reducing on-resistance, comprising the steps of: 'providing a substrate; forming an epitaxial region of a first conductivity type at an upper end of the substrate; • forming a gate region at an upper end of the epitaxial region; • forming a body region of one or more second conductivity types at the top of the epitaxial region; forming a plurality of source regions at the top of the body region; The upper surface of the body region is provided with a channel region which is shielded at the lower end of the gate region; and the first conductivity type is utilized by an ion implantation method with an oblique implantation angle and a selectable implant depth The impurity is obliquely implanted (or diffused) into the area of the insect crystal affected by the field effector crystal (JFET) to form a first conduction type of medium concentration concentration crystallite region, and the impurity will be subjected to the gate Blocking of the pole region, and not directly implanting the channel region; - Turning this channel region will not be affected by the increase in the impurity, and the starting voltage will not Under varying conditions, and can shorten the length of the channel region, and the concentration at the top of the Yak force u stupid crystal region. 2. The method for manufacturing a half-body structure capable of reducing on-resistance as described in claim 1, wherein the power semiconductor structure is a double-diffused metal oxide semiconductor (DMQS) structure of an n-type 15 1281192 channel, And the reading plate is a high-concentration secret region of the first-conducting type, the first-conducting is: ^, and the second conducting type is p-type. 3. The manufacturing method for reducing the conduction of a semiconductor structure as described in the item i of the patent scope, wherein the power semiconductor structure (4) is a double-diffused metal oxide semiconductor (DMqS) structure, _ = a high-density type of conduction type In the polar region, the first conduction type is; type: the far two conductivity type is η type.泡 Bubble 2, such as the towel, please refer to the manufacturing method of the structure of the first half of the patent, which can reduce the on-resistance, and the middle 隹μ + · , the middle force 4 + Lai structure is the insulation gate Polar transistor (IGB) structure, high concentration immersion region. And the county board is the second conductivity type of the second, a power semiconductor structure that can reduce the on-resistance, including: a substrate; an ang-conductive type of suspended crystal region formed on the upper end of the substrate; Formed in the upper end of the epitaxial region; a body region of one or a plurality of second conductive faces is formed in the smectic portion of the telecrystalline region; and a plurality of source regions are formed in the body a top portion of the region; wherein the upper surface of the body is a $way region, the channel region is shielded at a lower end of the idler region; and 16
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