TWI453834B - Semiconductor device and method for manufacturing semiconductor device - Google Patents
Semiconductor device and method for manufacturing semiconductor device Download PDFInfo
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- 239000004065 semiconductor Substances 0.000 title claims description 108
- 238000004519 manufacturing process Methods 0.000 title claims description 27
- 238000000034 method Methods 0.000 title claims description 13
- 239000012535 impurity Substances 0.000 claims description 67
- 230000002093 peripheral effect Effects 0.000 claims description 41
- 239000000758 substrate Substances 0.000 claims description 32
- 229910052732 germanium Inorganic materials 0.000 claims description 11
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 claims description 11
- KJTLSVCANCCWHF-UHFFFAOYSA-N Ruthenium Chemical compound [Ru] KJTLSVCANCCWHF-UHFFFAOYSA-N 0.000 claims description 4
- 229910052707 ruthenium Inorganic materials 0.000 claims description 4
- 238000009751 slip forming Methods 0.000 claims 1
- 229920002120 photoresistant polymer Polymers 0.000 description 12
- 238000000926 separation method Methods 0.000 description 7
- 230000000052 comparative effect Effects 0.000 description 6
- MZLGASXMSKOWSE-UHFFFAOYSA-N tantalum nitride Chemical compound [Ta]#N MZLGASXMSKOWSE-UHFFFAOYSA-N 0.000 description 6
- 238000005468 ion implantation Methods 0.000 description 4
- 238000000206 photolithography Methods 0.000 description 4
- 229910052796 boron Inorganic materials 0.000 description 3
- 150000002500 ions Chemical class 0.000 description 3
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 2
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 2
- 229910052785 arsenic Inorganic materials 0.000 description 2
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 description 2
- 238000005229 chemical vapour deposition Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 229910052698 phosphorus Inorganic materials 0.000 description 2
- 239000011574 phosphorus Substances 0.000 description 2
- 238000001020 plasma etching Methods 0.000 description 2
- 238000010276 construction Methods 0.000 description 1
- 239000007943 implant Substances 0.000 description 1
- 238000002513 implantation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000003647 oxidation Effects 0.000 description 1
- 238000007254 oxidation reaction Methods 0.000 description 1
- 238000000059 patterning Methods 0.000 description 1
- 229910001925 ruthenium oxide Inorganic materials 0.000 description 1
- WOCIAKWEIIZHES-UHFFFAOYSA-N ruthenium(iv) oxide Chemical compound O=[Ru]=O WOCIAKWEIIZHES-UHFFFAOYSA-N 0.000 description 1
- 229910052715 tantalum Inorganic materials 0.000 description 1
- GUVRBAGPIYLISA-UHFFFAOYSA-N tantalum atom Chemical compound [Ta] GUVRBAGPIYLISA-UHFFFAOYSA-N 0.000 description 1
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/60—Electrodes characterised by their materials
- H10D64/66—Electrodes having a conductor capacitively coupled to a semiconductor by an insulator, e.g. MIS electrodes
- H10D64/671—Electrodes having a conductor capacitively coupled to a semiconductor by an insulator, e.g. MIS electrodes the conductor having lateral variation in doping or structure
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/01—Manufacture or treatment
- H10D30/021—Manufacture or treatment of FETs having insulated gates [IGFET]
- H10D30/0221—Manufacture or treatment of FETs having insulated gates [IGFET] having asymmetry in the channel direction, e.g. lateral high-voltage MISFETs having drain offset region or extended-drain MOSFETs [EDMOS]
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/60—Insulated-gate field-effect transistors [IGFET]
- H10D30/601—Insulated-gate field-effect transistors [IGFET] having lightly-doped drain or source extensions, e.g. LDD IGFETs or DDD IGFETs
- H10D30/603—Insulated-gate field-effect transistors [IGFET] having lightly-doped drain or source extensions, e.g. LDD IGFETs or DDD IGFETs having asymmetry in the channel direction, e.g. lateral high-voltage MISFETs having drain offset region or extended drain IGFETs [EDMOS]
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/20—Electrodes characterised by their shapes, relative sizes or dispositions
- H10D64/27—Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
- H10D64/311—Gate electrodes for field-effect devices
- H10D64/411—Gate electrodes for field-effect devices for FETs
- H10D64/511—Gate electrodes for field-effect devices for FETs for IGFETs
- H10D64/514—Gate electrodes for field-effect devices for FETs for IGFETs characterised by the insulating layers
- H10D64/516—Gate electrodes for field-effect devices for FETs for IGFETs characterised by the insulating layers the thicknesses being non-uniform
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- Insulated Gate Type Field-Effect Transistor (AREA)
- Electrodes Of Semiconductors (AREA)
- Local Oxidation Of Silicon (AREA)
- Element Separation (AREA)
Description
本發明係關於一種具有LOCOS分離構造之MOS電晶體之半導體裝置及半導體裝置之製造方法。The present invention relates to a semiconductor device having a MOS transistor having a LOCOS separation structure and a method of fabricating the semiconductor device.
為了實現高耐壓之MOS電晶體,採用形成有與和汲極電極接觸之高雜質濃度之汲極區域相鄰且雜質濃度較此汲極區域低之區域(LDD區域)之構造。藉由形成LDD區域,能緩和在汲極區域附近之電場。又,使用LOCOS法形成較閘極絕緣膜厚之場絕緣膜(以下稱為「LOCOS絕緣膜」)以緩和閘極電極與汲極區域間之電場之方法已被探討(例如,參照專利文獻1)。具有形成為較閘極絕緣膜厚之LOCOS絕緣膜之構造,在以下稱為「LOCOS分離構造」。In order to realize a high withstand voltage MOS transistor, a structure is formed in which a region (LDD region) having a high impurity concentration in contact with the drain electrode and having a lower impurity concentration than the drain region is formed. By forming the LDD region, the electric field in the vicinity of the drain region can be alleviated. Further, a method of forming a field insulating film (hereinafter referred to as "LOCOS insulating film") having a gate insulating film thickness by the LOCOS method to alleviate the electric field between the gate electrode and the drain region has been discussed (for example, refer to Patent Document 1) ). The structure having the LOCOS insulating film formed to be thicker than the gate insulating film is hereinafter referred to as "LOCOS separation structure".
專利文獻1:日本特開2010-206163號公報Patent Document 1: Japanese Laid-Open Patent Publication No. 2010-206163
在LOCOS分離構造之MOS電晶體,有時會產生在較設計時之閘極閾值電壓低之閘極/源極間電壓之區域,洩漏電流流至源極區域與汲極區域間之現象。In the MOS transistor in which the LOCOS is separated, a phenomenon occurs in a region between the gate/source voltage at which the threshold voltage of the gate is lower than that at the time of design, and leakage current flows between the source region and the drain region.
本發明之目的在於提供一種抑制源極區域與汲極區域間之洩漏電流之產生之LOCOS分離構造之半導體裝置及半導體裝置之製造方法。It is an object of the present invention to provide a semiconductor device and a method of manufacturing a semiconductor device having a LOCOS separation structure for suppressing generation of a leakage current between a source region and a drain region.
根據本發明一形態之半導體裝置,具備:(a)半導體基板;(b)第1導電型源極區域及汲極區域,彼此分離形成在半導體基板上部之一部分;(c)閘極絕緣膜,包含源極區域與汲極區域所夾之區域而配置在半導體基板上;(d)LOCOS絕緣膜,包圍形成於源極區域與汲極區域間之通道區域之周圍而與閘極絕緣膜連續地配置在半導體基板上,膜厚較閘極絕緣膜厚;以及(e)閘極電極,由多晶體矽膜構成,該多晶體矽膜在源極區域與汲極區域所夾之區域,連續地遍布配置在閘極絕緣膜上及閘極絕緣膜周圍之LOCOS絕緣膜上;在閘極電極之通道寬度方向之端部即周邊區域之閘極閾值電壓較在閘極電極之中央區域之閘極閾值電壓高。A semiconductor device according to an aspect of the present invention includes: (a) a semiconductor substrate; (b) a first conductive type source region and a drain region, which are formed apart from each other in a portion of the upper portion of the semiconductor substrate; and (c) a gate insulating film; a region sandwiched between the source region and the drain region is disposed on the semiconductor substrate; (d) a LOCOS insulating film surrounds the channel region formed between the source region and the drain region and is continuous with the gate insulating film Arranged on the semiconductor substrate, the film thickness is thicker than the gate insulating film; and (e) the gate electrode is composed of a polycrystalline germanium film continuously in the region sandwiched between the source region and the drain region It is distributed over the LOCOS insulating film disposed on the gate insulating film and around the gate insulating film; the gate threshold voltage at the end portion of the gate electrode in the channel width direction is a gate electrode in the central region of the gate electrode The threshold voltage is high.
根據本發明另一形態之半導體裝置之製造方法,包含:(a)在半導體基板之表面之一部分藉由LOCOS法形成LOCOS絕緣膜之步驟;(b)在形成有LOCOS絕緣膜之區域以外之區域,將膜厚較LOCOS絕緣膜薄之閘極絕緣膜以與LOCOS絕緣膜連續之方式形成在半導體基板之表面之步驟;(c)遍布在閘極絕緣膜上及閘極絕緣膜周圍之LOCOS絕緣膜上連續地形成由多晶體矽膜構成之閘極電極之步驟;(d)隔著形成有閘極電極之區域,在半導體基板之上部形成第1導電型源極區域與汲極區域之步驟;以及(e)使在閘極電極之通道寬度方向之端部即周邊區域之閘極閾值電壓較在閘極電極之中央區域之閘極閾值電壓高,從閘極絕緣膜與LOCOS絕緣膜之邊界朝向閘極電極之中央區域遍布一定之距離而將導電型雜質注入閘極絕緣膜上之閘極電極之步驟。A method of fabricating a semiconductor device according to another aspect of the present invention, comprising: (a) a step of forming a LOCOS insulating film by a LOCOS method on a portion of a surface of the semiconductor substrate; (b) a region other than a region where the LOCOS insulating film is formed; a step of forming a gate insulating film having a thinner film thickness than the LOCOS insulating film on the surface of the semiconductor substrate in a continuous manner with the LOCOS insulating film; (c) LOCOS insulating over the gate insulating film and around the gate insulating film a step of continuously forming a gate electrode composed of a polycrystalline germanium film on the film; (d) a step of forming a first conductivity type source region and a drain region on the upper portion of the semiconductor substrate via a region in which the gate electrode is formed And (e) making the gate threshold voltage at the end portion in the channel width direction of the gate electrode higher than the gate threshold voltage in the central region of the gate electrode, from the gate insulating film and the LOCOS insulating film A step of injecting a conductive type impurity into the gate electrode on the gate insulating film at a certain distance from the central region of the gate electrode toward the gate electrode.
根據本發明,可提供一種抑制源極區域與汲極區域間之洩漏電流之產生之LOCOS分離構造之半導體裝置及半導體裝置之製造方法。According to the present invention, it is possible to provide a semiconductor device and a method of manufacturing a semiconductor device having a LOCOS separation structure for suppressing generation of a leakage current between a source region and a drain region.
接著,參照圖式,說明本發明之第1及第2實施形態。在以下圖式之記載,對相同或類似之部分賦予相同或類似之符號。然而,圖式係以示意方式顯示,應留意厚度與平面尺寸之關係、各層之厚度之比率等與實際不同。是以,具體之厚度或尺寸應參酌以下之說明來判斷。又,圖式彼此間當然亦包含彼此之尺寸關係或比率不同之部分。Next, the first and second embodiments of the present invention will be described with reference to the drawings. In the following description, the same or similar parts are given the same or similar symbols. However, the drawings are shown in a schematic manner, and it should be noted that the relationship between the thickness and the plane size, the ratio of the thicknesses of the layers, and the like are different from the actual ones. Therefore, the specific thickness or size should be judged by considering the following instructions. Moreover, the drawings also of course include portions having different dimensional relationships or ratios from each other.
又,以下所示之第1及第2實施形態,係例示用以將本發明之技術思想具體化之裝置或方法,本發明之實施形態,構成零件之材質、形狀、構造、配置等並不限於下述說明。本發明之實施形態,在申請專利範圍內可追加各種變更。In addition, the first and second embodiments shown below exemplify an apparatus or method for embodying the technical idea of the present invention. In the embodiment of the present invention, the material, shape, structure, arrangement, and the like of the components are not Limited to the following instructions. In the embodiment of the present invention, various modifications can be added within the scope of the patent application.
(第1實施形態)(First embodiment)
圖1~圖3係顯示本發明第1實施形態之半導體裝置1。圖1係沿著圖2之I-I方向之剖面圖,顯示沿著半導體裝置1之閘極寬度方向之通道區域之切斷面。圖3係沿著圖2之III-III方向之剖面圖,顯示沿著半導體裝置1之閘極長度方向之閘極電極50之中央區域之切斷面。圖2之俯視圖中,省略閘極絕緣膜40。1 to 3 show a semiconductor device 1 according to a first embodiment of the present invention. 1 is a cross-sectional view taken along the line I-I of FIG. 2, showing a cut surface of a channel region along the gate width direction of the semiconductor device 1. 3 is a cross-sectional view taken along line III-III of FIG. 2, showing a cut surface of a central region of the gate electrode 50 along the gate length direction of the semiconductor device 1. In the plan view of Fig. 2, the gate insulating film 40 is omitted.
如圖1~圖3所示,半導體裝置1,具備:半導體基板10;第1導電型源極區域20及汲極區域30,彼此分離形成在半導體基板10上部之一部分;閘極絕緣膜40,包含源極區域20與汲極區域30所夾之區域而配置在半導體基板10上;LOCOS絕緣膜60,膜厚較閘極絕緣膜40厚;以及閘極電極50,由第1導電型多晶體矽膜構成,該多晶體矽膜在源極區域20與汲極區域30所夾之區域,連續地遍布配置在閘極絕緣膜40上及閘極絕緣膜40周圍之LOCOS絕緣膜60上。LOCOS絕緣膜60,包圍形成於源極區域20與汲極區域30間之通道區域之周圍而與閘極絕緣膜40連續地配置在半導體基板10上。此外,第1導電型與第2導電型為彼此相反之導電型。亦即,若第1導電型為n型,則第2導電型為p型,半導體裝置1為n型通道MOS電晶體。又,若第1導電型為p型,則第2導電型為n型,半導體裝置1為p型通道MOS電晶體。As shown in FIGS. 1 to 3, the semiconductor device 1 includes a semiconductor substrate 10, a first conductive type source region 20 and a drain region 30, which are formed apart from each other in a portion of the upper portion of the semiconductor substrate 10, and a gate insulating film 40. The region including the source region 20 and the drain region 30 is disposed on the semiconductor substrate 10; the LOCOS insulating film 60 is thicker than the gate insulating film 40; and the gate electrode 50 is made of the first conductive type polycrystal In the ruthenium film, the polycrystalline ruthenium film is continuously spread over the LOCOS insulating film 60 disposed on the gate insulating film 40 and around the gate insulating film 40 in a region sandwiched between the source region 20 and the drain region 30. The LOCOS insulating film 60 surrounds the channel region formed between the source region 20 and the drain region 30, and is continuously disposed on the semiconductor substrate 10 with the gate insulating film 40. Further, the first conductivity type and the second conductivity type are opposite conductivity types. That is, when the first conductivity type is an n-type, the second conductivity type is a p-type, and the semiconductor device 1 is an n-channel MOS transistor. Further, when the first conductivity type is a p-type, the second conductivity type is an n-type, and the semiconductor device 1 is a p-channel MOS transistor.
半導體裝置1為在閘極電極50之通道寬度方向之端部即周邊區域S之閘極閾值電壓較在閘極電極50之中央區域之閘極閾值電壓高之MOS電晶體。此外,將周邊區域以外之區域作為閘極電極50之中央區域。此處,閘極閾值電壓為使半導體裝置1導通所需之施加於閘極電極50與源極區域20間之電壓。圖1及圖2中,以粗線包圍閘極電極50之周邊區域S來顯示(以下相同)。周邊區域S包含從閘極絕緣膜40與LOCOS絕緣膜60之邊界T朝向閘極電極50之中央區域距離w為止之配置在閘極絕緣膜40上之閘極電極50之區域。又,圖2中,以虛線顯示閘極電極50下方之LOCOS絕緣膜60之端部。The semiconductor device 1 is a MOS transistor having a gate threshold voltage at a terminal portion in the channel width direction of the gate electrode 50, that is, a gate threshold voltage higher than a gate threshold voltage in a central region of the gate electrode 50. Further, a region other than the peripheral region is referred to as a central region of the gate electrode 50. Here, the gate threshold voltage is a voltage applied between the gate electrode 50 and the source region 20 required to turn on the semiconductor device 1. In FIGS. 1 and 2, the peripheral region S of the gate electrode 50 is surrounded by a thick line to be displayed (the same applies hereinafter). The peripheral region S includes a region of the gate electrode 50 disposed on the gate insulating film 40 from the boundary T between the gate insulating film 40 and the LOCOS insulating film 60 toward the central portion of the gate electrode 50. Further, in Fig. 2, the end portions of the LOCOS insulating film 60 under the gate electrode 50 are shown by broken lines.
在半導體裝置1,詳細後述,閘極電極50之周邊區域S之第1導電型雜質之濃度形成為較閘極電極50之中央區域低。As will be described later in detail in the semiconductor device 1, the concentration of the first conductivity type impurity in the peripheral region S of the gate electrode 50 is formed to be lower than the central region of the gate electrode 50.
如圖1~圖3所示,半導體裝置1為具有LOCOS絕緣膜60之LOCOS分離構造。由於藉由LOCOS法形成LOCOS絕緣膜60,因此LOCOS絕緣膜60之下部埋入至半導體基板10上面之一部分。As shown in FIGS. 1 to 3, the semiconductor device 1 is a LOCOS separation structure having a LOCOS insulating film 60. Since the LOCOS insulating film 60 is formed by the LOCOS method, a lower portion of the LOCOS insulating film 60 is buried in a portion of the upper surface of the semiconductor substrate 10.
又,如圖1所示,閘極電極50之閘極寬度方向之兩端部係配置在LOCOS絕緣膜60上。又,與閘極電極50之側面接觸形成有側壁51。Further, as shown in FIG. 1, both ends of the gate electrode 50 in the gate width direction are disposed on the LOCOS insulating film 60. Further, a side wall 51 is formed in contact with the side surface of the gate electrode 50.
半導體裝置1之源極區域20具有形成在接近閘極電極50之區域之第1導電型低濃度源極區域21、與第1導電型雜質濃度較低濃度源極區域21高之高濃度源極區域22連結之LDS(lightly Doped Source)構造。汲極區域30具有形成在接近閘極電極50之區域之第1導電型低濃度汲極區域31、與第1導電型雜質濃度較低濃度汲極區域31高之高濃度汲極區域32連結之LDD(lightly Doped Drain)構造。The source region 20 of the semiconductor device 1 has a first conductivity type low concentration source region 21 formed in a region close to the gate electrode 50 and a high concentration source higher in the first conductivity type impurity concentration lower concentration source region 21. The LDS (lightly Doped Source) structure of the area 22 is connected. The drain region 30 has a first-conductivity-type low-concentration drain region 31 formed in a region close to the gate electrode 50, and is connected to the high-concentration drain region 32 having a higher first-concentration-type impurity concentration lower concentration drain region 31. LDD (lightly Doped Drain) construction.
如圖1~圖3所示,半導體基板10,係在第2導電型矽基板11上使第1導電型磊晶層12成長並在磊晶層12形成第2導電型井區域13之構造。在井區域13之被LOCOS絕緣膜60包圍之區域形成有半導體裝置1之所謂「活性區域」。As shown in FIG. 1 to FIG. 3, the semiconductor substrate 10 has a structure in which the first conductive type epitaxial layer 12 is grown on the second conductive type germanium substrate 11 and the second conductive type well region 13 is formed in the epitaxial layer 12. A so-called "active region" of the semiconductor device 1 is formed in a region of the well region 13 surrounded by the LOCOS insulating film 60.
LOCOS絕緣膜60之形成時,在LOCOS絕緣膜60下方之井區域13擴散之雜質被LOCOS絕緣膜60之端部吸收。藉此,在LOCOS絕緣膜60之端部附近之井區域13之雜質濃度降低。其結果,在LOCOS絕緣膜60之端部,在較設計時之閘極閾值電壓低之閘極/源極間電壓(以下稱為「洩漏電壓V(leak)」)洩漏電流流至源極區域20與汲極區域30間。「設計時之閘極閾值」為沒有在LOCOS絕緣膜60之端部附近之井區域13之雜質濃度降低之情形之由預先設定之雜質濃度決定之既定閘極閾值電壓。When the LOCOS insulating film 60 is formed, impurities diffused in the well region 13 below the LOCOS insulating film 60 are absorbed by the ends of the LOCOS insulating film 60. Thereby, the impurity concentration of the well region 13 near the end portion of the LOCOS insulating film 60 is lowered. As a result, at the end of the LOCOS insulating film 60, the gate-source voltage (hereinafter referred to as "leakage voltage V (leak)") at a gate threshold voltage lower than the design threshold current flows to the source region. 20 and bungee area 30. The "gate threshold at design time" is a predetermined gate threshold voltage determined by a predetermined impurity concentration in the case where the impurity concentration of the well region 13 in the vicinity of the end portion of the LOCOS insulating film 60 is not lowered.
上述洩漏電流之產生,尤其在n型通道MOS電晶體觀測到較多。因此,以下,針對第1導電型為n型、第2導電型為p型之情形例示說明。The above leakage current is generated, especially in the n-channel MOS transistor. Therefore, the case where the first conductivity type is an n-type and the second conductivity type is a p-type is exemplified below.
在半導體裝置1,閘極絕緣膜40與LOCOS絕緣膜60之邊界T附近、亦即閘極電極50之周邊區域S之n型雜質濃度較閘極電極50之中央區域之n型雜質濃度低。因此,在位於閘極電極50之周邊區域S下方之LOCOS絕緣膜60之端部,相較於閘極電極50之中央區域不易產生通道反轉。亦即,在閘極電極50之周邊區域S局部地閘極閾值電壓上升。In the semiconductor device 1, the n-type impurity concentration in the vicinity of the boundary T between the gate insulating film 40 and the LOCOS insulating film 60, that is, in the peripheral region S of the gate electrode 50 is lower than the n-type impurity concentration in the central region of the gate electrode 50. Therefore, in the end portion of the LOCOS insulating film 60 located under the peripheral region S of the gate electrode 50, channel inversion is less likely to occur than in the central region of the gate electrode 50. That is, the gate threshold voltage rises locally in the peripheral region S of the gate electrode 50.
如上述,在半導體裝置1,在閘極電極50之周邊區域S之閘極閾值電壓(以下稱為「周邊閘極閾值電壓V(th)2」)較在閘極電極50之中央區域之閘極閾值電壓(以下稱為「中央閘極閾值電壓V(th)1」)高。在閘極電極50之周邊區域S以外之區域,閘極閾值電壓為中央閘極閾值電壓V(th)1。又,中央閘極閾值電壓V(th)1為設計時之閘極閾值電壓。As described above, in the semiconductor device 1, the gate threshold voltage (hereinafter referred to as "peripheral gate threshold voltage V(th) 2") in the peripheral region S of the gate electrode 50 is larger than that in the central region of the gate electrode 50. The pole threshold voltage (hereinafter referred to as "central gate threshold voltage V(th) 1") is high. In a region other than the peripheral region S of the gate electrode 50, the gate threshold voltage is the center gate threshold voltage V(th)1. Further, the central gate threshold voltage V(th)1 is the gate threshold voltage at the time of design.
此外,中央閘極閾值電壓V(th)1與周邊閘極閾值電壓V(th)2之差,較佳為,設定成閘極電極50之周邊區域S之n型雜質濃度與閘極電極50之中央區域之n型雜質濃度之差,以成為設計時之閘極閾值電壓與洩漏電壓V(leak)之差以上。Further, the difference between the central gate threshold voltage V(th)1 and the peripheral gate threshold voltage V(th)2 is preferably set to the n-type impurity concentration of the peripheral region S of the gate electrode 50 and the gate electrode 50. The difference in the n-type impurity concentration in the central region is equal to or greater than the difference between the gate threshold voltage and the leakage voltage V (leak) at the time of design.
是以,在半導體裝置1,在較設計時之閘極閾值電壓低之閘極/源極間電壓,在LOCOS絕緣膜60之端部不會產生在源極區域20與汲極區域30間之洩漏電流。Therefore, in the semiconductor device 1, the gate/source voltage at which the threshold voltage of the gate is lower than that of the design is not generated between the source region 20 and the drain region 30 at the end of the LOCOS insulating film 60. Leakage current.
此外,設閘極電極50之周邊區域S之導電型為p型、周邊區域S以外之區域之導電型為n型亦可。在此構造之半導體裝置1,亦能使半導體裝置1之周邊閘極閾值電壓V(th)2較中央閘極閾值電壓V(th)1高。Further, the conductivity type of the peripheral region S of the gate electrode 50 is p-type, and the conductivity type of the region other than the peripheral region S may be n-type. In the semiconductor device 1 constructed as described above, the peripheral gate threshold voltage V(th)2 of the semiconductor device 1 can be made higher than the center gate threshold voltage V(th)1.
圖4所示之特性A為表示第1實施形態之半導體裝置1之閘極/源極間電壓Vgs與汲極電流Ids之關係之電流電壓特性,特性B~特性C為比較例之電流電壓特性。The characteristic A shown in FIG. 4 is a current-voltage characteristic showing the relationship between the gate-source voltage Vgs and the drain current Ids of the semiconductor device 1 of the first embodiment, and the characteristic B to the characteristic C are current-voltage characteristics of the comparative example. .
亦即,特性A為從閘極絕緣膜40與LOCOS絕緣膜60之邊界T朝向閘極電極50之中央區域遍布一定之距離w閘極絕緣膜40上之閘極電極50之n型雜質濃度較在閘極電極50之中央區域之n型雜質濃度低之半導體裝置1之電流電壓特性。That is, the characteristic A is a n-type impurity concentration of the gate electrode 50 on the gate insulating film 40 from the boundary T of the gate insulating film 40 and the LOCOS insulating film 60 toward the central region of the gate electrode 50 over a certain distance. The current-voltage characteristics of the semiconductor device 1 having a low n-type impurity concentration in the central region of the gate electrode 50.
特性B為針對LOCOS絕緣膜60上之閘極電極50、在至閘極絕緣膜40與LOCOS絕緣膜60之邊界T為止之區域將p型雜質離子注入之比較例B之電流電壓特性。亦即,比較例B為至邊界T為止之LOCOS絕緣膜60上之閘極電極50之n型雜質濃度較在閘極電極50之中央區域之n型雜質濃度低之半導體裝置。The characteristic B is a current-voltage characteristic of Comparative Example B in which a p-type impurity is ion-implanted into the gate electrode 50 on the LOCOS insulating film 60 and in a region up to the boundary T between the gate insulating film 40 and the LOCOS insulating film 60. That is, Comparative Example B is a semiconductor device in which the n-type impurity concentration of the gate electrode 50 on the LOCOS insulating film 60 to the boundary T is lower than the n-type impurity concentration in the central region of the gate electrode 50.
特性C為對閘極電極50不將p型雜質離子注入、閘極電極50之n型雜質濃度在所有區域一樣之比較例C之電流電壓特性。The characteristic C is a current-voltage characteristic of Comparative Example C in which the gate electrode 50 is not implanted with p-type impurity ions and the n-type impurity concentration of the gate electrode 50 is the same in all regions.
如圖4所示,相較於特性B、C,特性A在閘極/源極間電壓Vgs低之區域汲極電流Ids小。亦即,可知藉由使在周邊區域S之閘極絕緣膜40上之閘極電極50之n型雜質濃度較在閘極電極50之中央區域之n型雜質濃度低,可抑制洩漏電流之產生。As shown in FIG. 4, compared with the characteristics B and C, the characteristic A has a small drain current Ids in a region where the gate-source voltage Vgs is low. That is, it can be seen that the occurrence of leakage current can be suppressed by making the n-type impurity concentration of the gate electrode 50 on the gate insulating film 40 in the peripheral region S lower than the n-type impurity concentration in the central region of the gate electrode 50. .
如特性B般,在閘極電極50之周邊區域S僅對LOCOS絕緣膜60上之閘極電極50注入p型雜質、對閘極絕緣膜40上之閘極電極50不注入p型雜質之比較例B之情形,相較於比較例C雖特性有若干改善,但無法抑制洩漏電流。是以,可知若從閘極絕緣膜40與LOCOS絕緣膜60之邊界T朝向閘極電極50之中央區域在一定之距離w不使閘極電極50之雜質濃度降低,則無法實現周邊閘極閾值電壓V(th)2較中央閘極閾值電壓V(th)1高之半導體裝置1。距離w為例如0.5μm程度。As in the case of the characteristic B, in the peripheral region S of the gate electrode 50, only the p-type impurity is implanted into the gate electrode 50 on the LOCOS insulating film 60, and the p-type impurity is not implanted into the gate electrode 50 on the gate insulating film 40. In the case of Example B, although the characteristics were somewhat improved as compared with Comparative Example C, the leakage current could not be suppressed. Therefore, it can be understood that the peripheral gate threshold cannot be achieved if the impurity concentration of the gate electrode 50 is not lowered from the boundary T between the gate insulating film 40 and the LOCOS insulating film 60 toward the central portion of the gate electrode 50 at a certain distance w. The semiconductor device 1 has a voltage V(th) 2 higher than the central gate threshold voltage V(th)1. The distance w is, for example, about 0.5 μm.
如以上說明,在本發明第1實施形態之半導體裝置1,在LOCOS絕緣膜60之端部附近即閘極電極50之周邊區域S之n型雜質濃度,較在閘極電極50之中央區域之n型雜質濃度低。因此,在閘極電極50之周邊區域S之周邊閘極閾值電壓V(th)2較在閘極電極50之中央區域之中央閘極閾值電壓V(th)1高。其結果,根據圖1所示之半導體裝置1,即使是LOCOS分離構造之MOS電晶體,亦可抑制在源極區域20與汲極區域30間之洩漏電流之產生。As described above, in the semiconductor device 1 according to the first embodiment of the present invention, the n-type impurity concentration in the vicinity of the end portion of the LOCOS insulating film 60, that is, in the peripheral region S of the gate electrode 50 is higher than that in the central portion of the gate electrode 50. The n-type impurity concentration is low. Therefore, the peripheral gate threshold voltage V(th)2 in the peripheral region S of the gate electrode 50 is higher than the central gate threshold voltage V(th)1 in the central region of the gate electrode 50. As a result, according to the semiconductor device 1 shown in FIG. 1, even in the MOS transistor of the LOCOS separation structure, generation of leakage current between the source region 20 and the drain region 30 can be suppressed.
此外,上述雖針對第1導電型為n型、第2導電型為p型之情形進行說明,但第1導電型為p型、第2導電型為n型之情形亦可獲得相同效果。亦即,針對在n型之井區域13形成p型之源極區域20及汲極區域30、由p型多晶體矽膜構成之閘極電極50配置在閘極絕緣膜40及LOCOS絕緣膜60上之半導體裝置1,使在閘極電極50之周邊區域S之p型雜質濃度,較在閘極電極50之中央區域之p型雜質濃度低。藉此,能使在閘極電極50之周邊區域S之閘極閾值電壓較在閘極電極50之中央區域之閘極閾值電壓高。又,上述實施形態中,為了獲得所欲特性,適當變更閘極電極之導電型及雜質濃度亦可。In addition, although the case where the first conductivity type is the n-type and the second conductivity type is the p-type is described above, the same effect can be obtained in the case where the first conductivity type is the p-type and the second conductivity type is the n-type. That is, the gate electrode 50 composed of the p-type polycrystalline germanium film is formed in the n-type well region 13 to form the p-type source region 20 and the drain region 30, and the gate insulating film 40 and the LOCOS insulating film 60 are disposed. In the above semiconductor device 1, the p-type impurity concentration in the peripheral region S of the gate electrode 50 is made lower than the p-type impurity concentration in the central region of the gate electrode 50. Thereby, the gate threshold voltage in the peripheral region S of the gate electrode 50 can be made higher than the gate threshold voltage in the central region of the gate electrode 50. Further, in the above embodiment, in order to obtain desired characteristics, the conductivity type and impurity concentration of the gate electrode may be appropriately changed.
以下,參照圖5~圖12說明在閘極電極50之周邊區域S之n型雜質濃度較在閘極電極50之中央區域之n型雜質濃度低之半導體裝置1之製造方法之例。以下所述之半導體裝置之製造方法為一例,包含其變形例當然可藉由除此以外之各種製造方法實現。此外,圖5~圖12之各圖中,圖(a)為沿著圖2之I-I方向之剖面圖,圖(b)為沿著III-III方向之剖面圖。Hereinafter, an example of a method of manufacturing the semiconductor device 1 in which the n-type impurity concentration in the peripheral region S of the gate electrode 50 is lower than the n-type impurity concentration in the central region of the gate electrode 50 will be described with reference to FIGS. 5 to 12. The method of manufacturing the semiconductor device described below is an example, and the modified example thereof can of course be realized by various other manufacturing methods. In addition, in each of FIGS. 5 to 12, (a) is a cross-sectional view taken along line I-I of FIG. 2, and (b) is a cross-sectional view taken along line III-III.
(a)如圖5所示,在於p型矽基板11上磊晶成長後之n型磊晶層12內形成p型井區域13。藉此,準備半導體基板10。井區域13係藉由例如以離子注入法將p型雜質離子注入至磊晶層12之既定位置後使p型雜質熱擴散形成。(a) As shown in FIG. 5, a p-type well region 13 is formed in the n-type epitaxial layer 12 after epitaxial growth on the p-type germanium substrate 11. Thereby, the semiconductor substrate 10 is prepared. The well region 13 is formed by thermally injecting a p-type impurity into a predetermined position of the epitaxial layer 12 by, for example, ion implantation.
(b)如圖6所示,在磊晶層12及井區域13之表面之一部分形成LOCOS絕緣膜60。例如,在磊晶層12及井區域13之表面整體形成氮化矽(SiN)膜後,使用光微影技術等除去形成LOCOS絕緣膜60之區域之氮化矽膜。接著,以圖案化後之氮化矽膜為光罩,藉由LOCOS法選擇性形成LOCOS絕緣膜60。LOCOS絕緣膜60之膜厚為例如300nm~600nm程度。(b) As shown in FIG. 6, a LOCOS insulating film 60 is formed on one of the surfaces of the epitaxial layer 12 and the well region 13. For example, after a tantalum nitride (SiN) film is formed on the entire surface of the epitaxial layer 12 and the well region 13, the tantalum nitride film in the region where the LOCOS insulating film 60 is formed is removed by photolithography or the like. Next, the patterned LONX insulating film 60 is selectively formed by the LOCOS method using the patterned tantalum nitride film as a photomask. The film thickness of the LOCOS insulating film 60 is, for example, about 300 nm to 600 nm.
(c)在除去半導體基板10上之氮化矽膜後,藉由熱氧化法等使露出之井區域13之表面氧化,形成膜厚較LOCOS絕緣膜60薄之閘極絕緣膜40。閘極絕緣膜40之膜厚為例如40nm~60nm程度。藉此,如圖7所示,在形成有LOCOS絕緣膜60之區域以外之區域,形成與LOCOS絕緣膜60連續之閘極絕緣膜40。(c) After removing the tantalum nitride film on the semiconductor substrate 10, the surface of the exposed well region 13 is oxidized by a thermal oxidation method or the like to form a gate insulating film 40 having a film thickness smaller than that of the LOCOS insulating film 60. The film thickness of the gate insulating film 40 is, for example, about 40 nm to 60 nm. Thereby, as shown in FIG. 7, a gate insulating film 40 continuous with the LOCOS insulating film 60 is formed in a region other than the region where the LOCOS insulating film 60 is formed.
(d)藉由化學氣相成長(CVD)法等,在整面形成n型多晶體矽膜。藉著,使用光微影技術等將n型多晶體矽膜圖案化,如圖8所示形成閘極電極50。亦即,連續遍布於閘極絕緣膜40上及閘極絕緣膜40周圍之LOCOS絕緣膜60上形成由n型多晶體矽膜構成之閘極電極50。此外,形成未摻雜多晶體矽膜後,藉由將n型雜質離子注入形成閘極電極50亦可。(d) An n-type polycrystalline ruthenium film is formed on the entire surface by a chemical vapor deposition (CVD) method or the like. The n-type polycrystalline tantalum film is patterned by photolithography or the like, and the gate electrode 50 is formed as shown in FIG. That is, the gate electrode 50 composed of the n-type polycrystalline germanium film is formed on the LOCOS insulating film 60 which is continuously spread over the gate insulating film 40 and around the gate insulating film 40. Further, after the undoped polycrystalline germanium film is formed, the gate electrode 50 may be formed by ion implantation of an n-type impurity.
(e)以閘極電極50為光罩將磷(P)或砷(As)等n型雜質離子注入至井區域13,如圖9所示,形成低濃度源極區域21與低濃度汲極區域31。低濃度源極區域21與低濃度汲極區域31之表面雜質濃度為例如1×1017 cm-3 程度。(e) ion-implanting n-type impurity such as phosphorus (P) or arsenic (As) into the well region 13 using the gate electrode 50 as a mask, as shown in FIG. 9, forming a low-concentration source region 21 and a low-concentration drain Area 31. The surface impurity concentration of the low-concentration source region 21 and the low-concentration drain region 31 is, for example, about 1 × 10 17 cm -3 .
(f)在整面形成氮化矽膜後,藉由反應性離子蝕刻(RIE)法等對該氮化矽膜進行異向性蝕刻。其結果,如圖10所示,與閘極電極50之側面接觸形成側壁51。在側壁51使用氧化矽膜等亦可(f) After the tantalum nitride film is formed over the entire surface, the tantalum nitride film is anisotropically etched by a reactive ion etching (RIE) method or the like. As a result, as shown in FIG. 10, the side wall 51 is formed in contact with the side surface of the gate electrode 50. A ruthenium oxide film or the like may be used for the side wall
(g)使用光微影技術以圖案化後之光阻膜或閘極電極50及側壁51為光罩,將磷或砷等n型雜質離子注入至井區域13之既定區域,如圖11所示,形成高濃度源極區域22與高濃度汲極區域32。高濃度源極區域22與高濃度汲極區域32之表面雜質濃度為例如2×1019 cm-3 程度。如圖11所示,低濃度源極區域21與高濃度源極區域22連結,低濃度汲極區域31與高濃度汲極區域32連結。(g) using the photolithography technique to pattern the photoresist film or the gate electrode 50 and the sidewall 51 as a mask, and implant an n-type impurity such as phosphorus or arsenic into a predetermined region of the well region 13, as shown in FIG. It is shown that a high concentration source region 22 and a high concentration drain region 32 are formed. The surface impurity concentration of the high-concentration source region 22 and the high-concentration drain region 32 is, for example, about 2 × 10 19 cm -3 . As shown in FIG. 11, the low-concentration source region 21 is connected to the high-concentration source region 22, and the low-concentration drain region 31 is connected to the high-concentration drain region 32.
(h)將光阻膜90塗布在整面後,如圖12所示,以在閘極絕緣膜40與LOCOS絕緣膜60之邊界T區域之上方閘極電極50露出之方式,使光阻膜90圖案化。此時,以在閘極電極50之通道寬度方向之端部、至少從閘極絕緣膜40與LOCOS絕緣膜60之邊界T朝向閘極電極50之中央區域遍布距離W閘極電極50露出之方式,使光阻膜90圖案化。接著,以光阻膜90為光罩,將硼(B)等p型雜質離子注入至閘極電極50。藉此,在閘極電極50之周邊區域S注入p型雜質。p型雜質之注入量為例如1×1016 cm-2 程度。其結果,閘極電極50之周邊區域S之n型雜質濃度較閘極電極50之中央區域之n型雜質濃度低。除去光阻膜90,完成圖1所示之半導體裝置1。(h) After the photoresist film 90 is applied over the entire surface, as shown in FIG. 12, the photoresist film is exposed in such a manner that the gate electrode 50 is exposed above the boundary T region of the gate insulating film 40 and the LOCOS insulating film 60. 90 patterning. At this time, at the end portion in the channel width direction of the gate electrode 50, at least from the boundary T between the gate insulating film 40 and the LOCOS insulating film 60 toward the central region of the gate electrode 50, the distance W is exposed to the gate electrode 50. The photoresist film 90 is patterned. Next, the photoresist film 90 is used as a mask, and p-type impurity ions such as boron (B) are implanted into the gate electrode 50. Thereby, a p-type impurity is implanted in the peripheral region S of the gate electrode 50. The implantation amount of the p-type impurity is, for example, about 1 × 10 16 cm -2 . As a result, the n-type impurity concentration in the peripheral region S of the gate electrode 50 is lower than the n-type impurity concentration in the central region of the gate electrode 50. The photoresist film 90 is removed, and the semiconductor device 1 shown in Fig. 1 is completed.
上述針對形成LDS區域及LDD區域之情形例示說明。然而,半導體裝置1為不具有LDS區域及LDD區域之構造亦可。The above description is directed to the case of forming an LDS region and an LDD region. However, the semiconductor device 1 may have a structure that does not have an LDS region and an LDD region.
又,將p型雜質注入至閘極電極50之周邊區域S之步驟,作為單獨步驟進行亦可,與其他半導體元件之製造步驟同時進行亦可。例如,將省略圖示之p型通道MOS電晶體與半導體裝置1同時形成在半導體基板10上之情形,在形成p型通道MOS電晶體之源極區域或汲極區域之離子注入步驟,將p型雜質注入至閘極電極50之周邊區域S亦可。Further, the step of implanting the p-type impurity into the peripheral region S of the gate electrode 50 may be performed as a separate step, and may be performed simultaneously with the manufacturing steps of other semiconductor elements. For example, in the case where the p-channel MOS transistor (not shown) is formed on the semiconductor substrate 10 simultaneously with the semiconductor device 1, in the ion implantation step of forming the source region or the drain region of the p-channel MOS transistor, p The type impurity may be implanted into the peripheral region S of the gate electrode 50.
此外,藉由使注入至閘極電極50之周邊區域S之p型雜質之濃度變高,在閘極電極50之中央區域之導電型維持n型之狀態下,使閘極電極50之周邊區域S之導電型為p型亦可。Further, by increasing the concentration of the p-type impurity implanted in the peripheral region S of the gate electrode 50, the peripheral region of the gate electrode 50 is maintained in a state where the conductivity type in the central portion of the gate electrode 50 is maintained in the n-type. The conductivity type of S may be p-type.
如以上說明,根據本發明第1實施形態之半導體裝置1之製造方法,能使閘極電極50之周邊區域S之n型雜質濃度較閘極電極50之中央區域之n型雜質濃度低。其結果,能將在半導體裝置1之閘極絕緣膜40與LOCOS絕緣膜60之邊界區域附近之周邊閘極閾值電壓V(th)2設定成較在閘極電極50之中央區域之中央閘極閾值電壓V(th)1高。因此,能提供抑制源極區域20與汲極區域30間之洩漏電流之產生之LOCOS分離構造之半導體裝置1。As described above, according to the method of manufacturing the semiconductor device 1 of the first embodiment of the present invention, the n-type impurity concentration in the peripheral region S of the gate electrode 50 can be made lower than the n-type impurity concentration in the central region of the gate electrode 50. As a result, the peripheral gate threshold voltage V(th) 2 in the vicinity of the boundary region between the gate insulating film 40 of the semiconductor device 1 and the LOCOS insulating film 60 can be set to be the center gate of the central region of the gate electrode 50. The threshold voltage V(th)1 is high. Therefore, the semiconductor device 1 of the LOCOS separation structure which suppresses the generation of the leakage current between the source region 20 and the drain region 30 can be provided.
(第2實施形態)(Second embodiment)
本發明第2實施形態之半導體裝置1,如圖13所示,不僅井區域13之周邊,在低濃度源極區域21上與低濃度汲極區域31上形成有LOCOS絕緣膜60之點與圖1所示之半導體裝置1不同。圖13所示之閘極電極50,從閘極絕緣膜40上連續遍布配置在形成於低濃度源極區域21上與低濃度汲極區域31上之LOCOS絕緣膜60上。In the semiconductor device 1 according to the second embodiment of the present invention, as shown in FIG. 13, not only the periphery of the well region 13, but also the LOCOS insulating film 60 is formed on the low-concentration source region 21 and the low-concentration drain region 31. The semiconductor device 1 shown in Fig. 1 is different. The gate electrode 50 shown in FIG. 13 is continuously spread over the gate insulating film 40 over the LOCOS insulating film 60 formed on the low-concentration source region 21 and the low-concentration drain region 31.
圖14係顯示圖13所示之半導體裝置1之俯視圖。圖13係顯示圖14之XIII-XIII方向、亦即沿著半導體裝置1之閘極長度方向之閘極電極50之中央區域之切斷面。圖14中,以虛線顯示閘極電極50下方之LOCOS絕緣膜60之端部,省略閘極絕緣膜40。Fig. 14 is a plan view showing the semiconductor device 1 shown in Fig. 13. Fig. 13 is a view showing a cut surface of the central region of the gate electrode 50 in the XIII-XIII direction of Fig. 14, that is, along the gate length direction of the semiconductor device 1. In Fig. 14, the end portion of the LOCOS insulating film 60 under the gate electrode 50 is indicated by a broken line, and the gate insulating film 40 is omitted.
如圖14所示,高濃度源極區域22上與高濃度汲極區域32被LOCOS絕緣膜60包圍在周圍。藉由在低濃度汲極區域31上形成LOCOS絕緣膜60,可達到提升閘極電極50與汲極區域30間之耐壓之效果。As shown in FIG. 14, the high-concentration source region 22 and the high-concentration drain region 32 are surrounded by the LOCOS insulating film 60. By forming the LOCOS insulating film 60 on the low-concentration drain region 31, the effect of increasing the withstand voltage between the gate electrode 50 and the drain region 30 can be achieved.
圖15係顯示圖14之XV-XV方向、亦即沿著半導體裝置1之閘極寬度方向之通道區域之切斷面。圖15所示之剖面圖顯示與圖1所示之剖面圖相同之構造。Fig. 15 is a view showing a cut surface of the channel region in the XV-XV direction of Fig. 14, that is, along the gate width direction of the semiconductor device 1. The cross-sectional view shown in Fig. 15 shows the same configuration as the cross-sectional view shown in Fig. 1.
在圖13~圖15所示之半導體裝置1,在閘極絕緣膜40與形成在低濃度源極區域21上及低濃度汲極區域31上之LOCOS絕緣膜60之邊界附近之閘極電極50之周邊區域S之n型雜質濃度形成為較在閘極電極50之中央區域之n型雜質濃度低。因此,在閘極電極50之周邊區域S下方之LOCOS絕緣膜60之端部,相較於閘極電極50之中央區域不易產生通道反轉。亦即,在閘極電極50之周邊區域S閾值電壓局部上升。In the semiconductor device 1 shown in FIGS. 13 to 15, the gate electrode 50 is in the vicinity of the boundary between the gate insulating film 40 and the LOCOS insulating film 60 formed on the low-concentration source region 21 and the low-concentration drain region 31. The n-type impurity concentration of the peripheral region S is formed to be lower than the n-type impurity concentration in the central region of the gate electrode 50. Therefore, in the end portion of the LOCOS insulating film 60 under the peripheral region S of the gate electrode 50, channel inversion is less likely to occur than in the central region of the gate electrode 50. That is, the threshold voltage locally rises in the peripheral region S of the gate electrode 50.
是以,根據本發明第2實施形態之半導體裝置1,在閘極電極50之周邊區域S之周邊閘極閾值電壓V(th)2設定成較在閘極電極50之中央區域之中央閘極閾值電壓V(th)1高。其結果,根據第2實施形態之半導體裝置1,即使是LOCOS偏置構造之MOS電晶體,亦能抑制源極區域20與汲極區域30間之洩漏電流之產生。其他與第1實施形態實質上相同,省略重複之記載。According to the semiconductor device 1 of the second embodiment of the present invention, the gate threshold voltage V(th) 2 in the peripheral region S of the gate electrode 50 is set to be the center gate of the central region of the gate electrode 50. The threshold voltage V(th)1 is high. As a result, according to the semiconductor device 1 of the second embodiment, even in the MOS transistor of the LOCOS bias structure, the occurrence of leakage current between the source region 20 and the drain region 30 can be suppressed. Others are substantially the same as those of the first embodiment, and the description thereof will be omitted.
圖16係顯示第2實施形態之半導體裝置1之另一例。圖13~圖15所示之半導體裝置1,在形成在低濃度源極區域21上及低濃度汲極區域31上之LOCOS絕緣膜60與閘極絕緣膜40之所有邊界區域上,閘極電極50之n型雜質濃度較在中央區域之n型雜質濃度低。然而,如圖16所示,僅在閘極電極50之通道寬度方向之端部,從閘極絕緣膜40與LOCOS絕緣膜60之邊界T朝向閘極電極50之中央區域遍布距離w,閘極電極50之n型雜質濃度較在中央區域之n型雜質濃度低亦可。Fig. 16 is a view showing another example of the semiconductor device 1 of the second embodiment. The semiconductor device 1 shown in FIGS. 13 to 15 is formed on the low-concentration source region 21 and the low-concentration drain region 31 on all boundary regions of the LOCOS insulating film 60 and the gate insulating film 40, and the gate electrode The n-type impurity concentration of 50 is lower than the n-type impurity concentration in the central region. However, as shown in FIG. 16, only the end portion of the gate electrode 50 in the channel width direction is spread from the boundary T of the gate insulating film 40 and the LOCOS insulating film 60 toward the central portion of the gate electrode 50 by a distance w, the gate The n-type impurity concentration of the electrode 50 may be lower than the n-type impurity concentration in the central region.
為了製造圖13~圖15所示之半導體裝置1,可採用例如以下之製造方法。亦即,如圖17所示,在井區域13形成低濃度源極區域21及低濃度汲極區域31。低濃度源極區域21及低濃度汲極區域31係藉由以例如使用光微影技術形成之光阻膜為光罩進行離子注入形成。In order to manufacture the semiconductor device 1 shown in FIGS. 13 to 15, for example, the following manufacturing method can be employed. That is, as shown in FIG. 17, the low concentration source region 21 and the low concentration drain region 31 are formed in the well region 13. The low-concentration source region 21 and the low-concentration drain region 31 are formed by ion implantation using a photoresist film formed by, for example, photolithography.
接著,如圖18所示,形成LOCOS絕緣膜60之情形,在低濃度源極區域21上及低濃度汲極區域31上形成LOCOS絕緣膜60。Next, as shown in FIG. 18, in the case where the LOCOS insulating film 60 is formed, the LOCOS insulating film 60 is formed on the low-concentration source region 21 and the low-concentration drain region 31.
之後,如圖7~圖8所說明,形成閘極絕緣膜40、閘極電極50。接著,如圖10~圖11所說明,形成側壁51、高濃度源極區域22及高濃度汲極區域32。Thereafter, as shown in FIGS. 7 to 8, a gate insulating film 40 and a gate electrode 50 are formed. Next, as illustrated in FIGS. 10 to 11, the side wall 51, the high concentration source region 22, and the high concentration drain region 32 are formed.
再者,將光阻膜91整面塗布後,如圖19所示,以在形成於低濃度源極區域21上及低濃度汲極區域31上之LOCOS絕緣膜60與閘極絕緣膜40之邊界區域之上方閘極電極50露出之方式,使光阻膜91圖案化。此時,以在閘極電極50之通道寬度方向之端部、至少從閘極絕緣膜40與LOCOS絕緣膜60之邊界T朝向閘極電極50之中央區域遍布距離w閘極電極50露出之方式,使光阻膜91圖案化。Further, after the entire surface of the photoresist film 91 is applied, as shown in FIG. 19, the LOCOS insulating film 60 and the gate insulating film 40 are formed on the low-concentration source region 21 and the low-concentration drain region 31. The photoresist film 91 is patterned in such a manner that the gate electrode 50 is exposed above the boundary region. At this time, at the end portion in the channel width direction of the gate electrode 50, at least from the boundary T between the gate insulating film 40 and the LOCOS insulating film 60 toward the central portion of the gate electrode 50, the distance w is exposed to the gate electrode 50. The photoresist film 91 is patterned.
接著,以光阻膜91為光罩,將硼(B)等p型雜質離子注入至閘極電極50。藉此,在閘極電極50之周邊區域S注入p型雜質。其結果,閘極電極50之周邊區域S之n型雜質濃度較閘極電極50之中央區域之n型雜質濃度低。除去光阻膜91,完成圖13~圖15所示之半導體裝置1。Next, the photoresist film 91 is used as a mask, and p-type impurity ions such as boron (B) are implanted into the gate electrode 50. Thereby, a p-type impurity is implanted in the peripheral region S of the gate electrode 50. As a result, the n-type impurity concentration in the peripheral region S of the gate electrode 50 is lower than the n-type impurity concentration in the central region of the gate electrode 50. The photoresist film 91 is removed, and the semiconductor device 1 shown in FIGS. 13 to 15 is completed.
根據以上說明之第2實施形態之半導體裝置1之製造方法,能將在半導體裝置1之閘極絕緣膜40與形成於低濃度源極區域21上及低濃度汲極區域31上之LOCOS絕緣膜60之邊界區域附近之周邊閘極閾值電壓V(th)2設定成較在閘極電極50之中央區域之中央閘極閾值電壓V(th)1高。因此,能提供抑制源極區域20與汲極區域30間之洩漏電流之產生之LOCOS偏置構造之半導體裝置1。According to the method of manufacturing the semiconductor device 1 of the second embodiment described above, the gate insulating film 40 of the semiconductor device 1 and the LOCOS insulating film formed on the low-concentration source region 21 and the low-concentration drain region 31 can be formed. The peripheral gate threshold voltage V(th)2 near the boundary region of 60 is set to be higher than the central gate threshold voltage V(th)1 in the central region of the gate electrode 50. Therefore, the semiconductor device 1 having the LOCOS bias structure for suppressing the occurrence of leakage current between the source region 20 and the drain region 30 can be provided.
(其他實施形態)(Other embodiments)
如上述,雖以第1及第2實施形態記載本發明,但不應理解成構成此揭示一部分之論述及圖式係用以限定本發明。本發明所屬技術領域中具有通常知識者從此揭示應當理解各種替代實施形態、實施例及運用技術。As described above, the present invention is described in the first and second embodiments, and the description and drawings which form a part of this disclosure are not to be construed as limiting the invention. Those skilled in the art to which the present invention pertains will be apparent from the disclosure that various alternative embodiments, embodiments, and operational techniques.
例如,作為半導體基板10採用未形成磊晶層12及井區域13之矽基板,在此矽基板形成源極區域20或汲極區域30亦可。For example, as the semiconductor substrate 10, a germanium substrate in which the epitaxial layer 12 and the well region 13 are not formed is used, and the source region 20 or the drain region 30 may be formed on the germanium substrate.
如上述,本發明當然包含此處未記載之各種實施形態等。是以,本發明之技術範圍係根據上述說明僅由妥當之申請專利範圍之發明特定事項決定。As described above, the present invention naturally includes various embodiments and the like not described herein. Therefore, the technical scope of the present invention is determined by the above-described description only by the specific matters of the invention of the scope of the patent application.
1...半導體裝置1. . . Semiconductor device
10...半導體基板10. . . Semiconductor substrate
11...矽基板11. . .矽 substrate
12...磊晶層12. . . Epitaxial layer
13...井區域13. . . Well area
20...源極區域20. . . Source area
21...低濃度源極區域twenty one. . . Low concentration source region
22...高濃度源極區域twenty two. . . High concentration source region
30...汲極區域30. . . Bungee area
31...低濃度汲極區域31. . . Low concentration bungee region
32...高濃度汲極區域32. . . High concentration bungee area
40...閘極絕緣膜40. . . Gate insulating film
50...閘極電極50. . . Gate electrode
51...側壁51. . . Side wall
60...LOCOS絕緣膜60. . . LOCOS insulation film
圖1係顯示本發明第1實施形態之半導體裝置之構造之示意剖面圖。1 is a schematic cross-sectional view showing the structure of a semiconductor device according to a first embodiment of the present invention.
圖2係顯示本發明第1實施形態之半導體裝置之構造之示意俯視圖。Fig. 2 is a schematic plan view showing a structure of a semiconductor device according to a first embodiment of the present invention.
圖3係沿著圖2之III-III方向之剖面圖。Figure 3 is a cross-sectional view taken along line III-III of Figure 2;
圖4係顯示本發明第1實施形態之半導體裝置與比較例之電流電壓特性之圖表。Fig. 4 is a graph showing current-voltage characteristics of a semiconductor device and a comparative example according to the first embodiment of the present invention.
圖5(a)、(b)係用以說明本發明第1實施形態之半導體裝置之製造方法之步驟剖面圖(其1)。5 (a) and (b) are cross-sectional views (1) of the steps of the method of manufacturing the semiconductor device according to the first embodiment of the present invention.
圖6(a)、(b)係用以說明本發明第1實施形態之半導體裝置之製造方法之步驟剖面圖(其2)。6 (a) and (b) are cross-sectional views (2) of the steps of the method of manufacturing the semiconductor device according to the first embodiment of the present invention.
圖7(a)、(b)係用以說明本發明第1實施形態之半導體裝置之製造方法之步驟剖面圖(其3)。7 (a) and (b) are cross-sectional views (3) of the steps of the method of manufacturing the semiconductor device according to the first embodiment of the present invention.
圖8(a)、(b)係用以說明本發明第1實施形態之半導體裝置之製造方法之步驟剖面圖(其4)。8 (a) and (b) are cross-sectional views (4) of the steps of the method of manufacturing the semiconductor device according to the first embodiment of the present invention.
圖9(a)、(b)係用以說明本發明第1實施形態之半導體裝置之製造方法之步驟剖面圖(其5)。9 (a) and (b) are cross-sectional views (5) of the steps of the method of manufacturing the semiconductor device according to the first embodiment of the present invention.
圖10(a)、(b)係用以說明本發明第1實施形態之半導體裝置之製造方法之步驟剖面圖(其6)。10 (a) and (b) are cross-sectional views (6) of the steps of the method of manufacturing the semiconductor device according to the first embodiment of the present invention.
圖11(a)、(b)係用以說明本發明第1實施形態之半導體裝置之製造方法之步驟剖面圖(其7)。11 (a) and (b) are cross-sectional views (7) of a method of manufacturing a semiconductor device according to a first embodiment of the present invention.
圖12(a)、(b)係用以說明本發明第1實施形態之半導體裝置之製造方法之步驟剖面圖(其8)。12 (a) and (b) are cross-sectional views (8) of the steps of the method of manufacturing the semiconductor device according to the first embodiment of the present invention.
圖13係顯示本發明第2實施形態之半導體裝置之構造之示意剖面圖。Fig. 13 is a schematic cross-sectional view showing the structure of a semiconductor device according to a second embodiment of the present invention.
圖14係顯示本發明第2實施形態之半導體裝置之構造之示意俯視圖。Fig. 14 is a schematic plan view showing the structure of a semiconductor device according to a second embodiment of the present invention.
圖15係沿著圖14之XV-XV方向之剖面圖。Figure 15 is a cross-sectional view taken along line XV-XV of Figure 14.
圖16係顯示本發明第2實施形態之變形例之半導體裝置之構造之示意俯視圖。Fig. 16 is a schematic plan view showing a structure of a semiconductor device according to a modification of the second embodiment of the present invention.
圖17係用以說明本發明第2實施形態之半導體裝置之製造方法之步驟剖面圖(其1)。Fig. 17 is a cross-sectional view (1) showing a step of a method of manufacturing a semiconductor device according to a second embodiment of the present invention.
圖18係用以說明本發明第2實施形態之半導體裝置之製造方法之步驟剖面圖(其2)。Fig. 18 is a cross-sectional view (2) showing a step of a method of manufacturing a semiconductor device according to a second embodiment of the present invention.
圖19係用以說明本發明第2實施形態之半導體裝置之製造方法之步驟剖面圖(其3)。19 is a cross-sectional view (3) of a step for explaining a method of manufacturing a semiconductor device according to a second embodiment of the present invention.
10...半導體基板10. . . Semiconductor substrate
11...矽基板11. . .矽 substrate
12...磊晶層12. . . Epitaxial layer
13...井區域13. . . Well area
40...閘極絕緣膜40. . . Gate insulating film
50...閘極電極50. . . Gate electrode
51...側壁51. . . Side wall
60...LOCOS絕緣膜60. . . LOCOS insulation film
S...周邊區域S. . . Surrounding area
T...邊界T. . . boundary
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