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TWI517295B - Semiconductor device having P top layer and N energy level and manufacturing method thereof - Google Patents

Semiconductor device having P top layer and N energy level and manufacturing method thereof Download PDF

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TWI517295B
TWI517295B TW102101839A TW102101839A TWI517295B TW I517295 B TWI517295 B TW I517295B TW 102101839 A TW102101839 A TW 102101839A TW 102101839 A TW102101839 A TW 102101839A TW I517295 B TWI517295 B TW I517295B
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doped
semiconductor
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TW201430999A (en
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詹景琳
林鎮元
林正基
連士進
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旺宏電子股份有限公司
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Description

具有P頂層與N能階的半導體裝置及其製造方法 Semiconductor device having P top layer and N energy level and manufacturing method thereof

本案之實施例係有關一種半導體裝置,特別是一種金屬氧化物半導體裝置以及一種製造此裝置的方法。 Embodiments of the present invention relate to a semiconductor device, and more particularly to a metal oxide semiconductor device and a method of fabricating the same.

擴散金屬氧化物半導體(DMOS)裝置的特徵是同時擴散的源極區及後閘極區。電晶體通道透過該兩種擴散的差異而形成且不是分開植入,其導致通道長度縮短。較短的通道允許低功率耗損以及高速的能力。 A diffused metal oxide semiconductor (DMOS) device is characterized by a source region and a rear gate region that are simultaneously diffused. The transistor channel is formed by the difference in the two diffusions and is not implanted separately, which results in a shortened channel length. Shorter channels allow for low power consumption and high speed capability.

橫向擴散金屬氧化物半導體(LDMOS)裝置在其晶圓表面有導致橫向電流的源極以及汲極。設計LDMOS裝置的兩個重要參數是崩潰電壓以及導通電阻(on-resistance)。較佳的,高崩潰電壓以及低導通電阻讓裝置在高電壓運行下有相對較低的電力消耗。此外,低導通電阻在裝置飽和時提供較高的汲極電流,其可改善裝置的運行速度。 A laterally diffused metal oxide semiconductor (LDMOS) device has a source and a drain that cause lateral current on its wafer surface. Two important parameters for designing an LDMOS device are the breakdown voltage and on-resistance. Preferably, the high breakdown voltage and low on-resistance allow the device to have relatively low power consumption at high voltage operation. In addition, the low on-resistance provides a higher drain current when the device is saturated, which improves the operating speed of the device.

第一圖係為習用LDMOS裝置之飄移區的俯視圖。第一圖的LDMOS裝置具有LDMOS區10,其為方框所標示。LDMOS裝置1包括源極側20以及汲極側30。 The first figure is a top view of the drift zone of a conventional LDMOS device. The LDMOS device of the first figure has an LDMOS region 10, which is indicated by a square. The LDMOS device 1 includes a source side 20 and a drain side 30.

第二圖係為第一圖中所標示之LDMOS區10的俯視 圖。LDMOS區10有許多P型擴散層或P頂區40從源極側20連續延伸至汲極側30,其中P頂區40設置於高電壓N型井(HVNW)中。因此,該習用LDMOS區10包括N型能階或N能階區50部分,其設置於P頂端區40之上,其中P頂區40被N能階區50分開且N能階區50沒有設置於任何P頂層(P-TOP)之上。 The second figure is a top view of the LDMOS region 10 indicated in the first figure. Figure. The LDMOS region 10 has a plurality of P-type diffusion layers or P-top regions 40 extending continuously from the source side 20 to the drain side 30, wherein the P-top region 40 is disposed in a high voltage N-type well (HVNW). Therefore, the conventional LDMOS region 10 includes an N-type energy level or N-energy level region 50 portion disposed above the P top end region 40, wherein the P top region 40 is separated by the N energy level region 50 and the N energy level region 50 is not disposed. Above any P top layer (P-TOP).

第3A圖是第二圖中沿著AA’區域線的剖面圖。這種表示法下的習用LDMOS在以設置的HVNW 70中有P基板60。第一P井80在P基板60中形成,而第二P井90在HVNW 70中形成,其中第一P井80有P+摻雜區100以及第二P井90有另一P+摻雜區110緊鄰於N+摻雜源極區120。N+摻雜汲極區130形成於HVNW 70中。LDMOS區域10的部分以N能階區50表示,其設置於其中之P頂區40之上。蝕刻場氧化隔離區140實質上分離摻雜區100、110、120以及130。 Fig. 3A is a cross-sectional view along the line AA' in the second figure. The conventional LDMOS in this representation has a P substrate 60 in the HVNW 70 provided. A first P well 80 is formed in the P substrate 60, and a second P well 90 is formed in the HVNW 70, wherein the first P well 80 has a P + doped region 100 and the second P well 90 has another P + doping Region 110 is adjacent to N + doped source region 120. The N + doped drain region 130 is formed in the HVNW 70. A portion of the LDMOS region 10 is represented by an N energy level region 50 disposed over the P top region 40 therein. The etch field oxide isolation region 140 substantially separates the doped regions 100, 110, 120, and 130.

任何習知的控制閘極結構150可用於LDMOS裝置中。例如,控制閘極結構150包括導電層設置於介電層上。控制閘極結構150更包括介電側壁間隙壁(sidewall spacer)。蝕刻的層間介電(ILD)層160設置於該結構上。第一蝕刻金屬層170具有透過該ILD層160接觸的網絡。第3A圖的習用LDMOS範例具有界金屬介電(IMD)層180,其設置於第二蝕刻金屬層190之上,第二蝕刻金屬層190提供透過該ILD層180接觸的網絡。 Any conventional control gate structure 150 can be used in an LDMOS device. For example, the control gate structure 150 includes a conductive layer disposed on the dielectric layer. The control gate structure 150 further includes a dielectric sidewall spacer. An etched interlayer dielectric (ILD) layer 160 is disposed over the structure. The first etched metal layer 170 has a network that is in contact through the ILD layer 160. The conventional LDMOS example of FIG. 3A has an interfacial metal dielectric (IMD) layer 180 disposed over a second etched metal layer 190 that provides a network that is in contact through the ILD layer 180.

第3B圖是第二圖中沿著BB’區域線的剖面圖。傳統LDMOS的剖面圖跟第3A圖有相同的結構,除了P頂層沒有設置於HVNW 70之中。 Fig. 3B is a cross-sectional view along the line BB' in the second figure. The cross-sectional view of the conventional LDMOS has the same structure as that of the third embodiment, except that the P top layer is not disposed in the HVNW 70.

高電壓LDMOS裝置在半導體中有不同種用途。例如, LDMOS裝置可用於把相對高的電壓轉換成相對低的電壓或是當成設置用於驅動負載的轉換功率電晶體。然而,因為N能階區及該P型全摻雜區之間互相影響,習用高電壓LDMOS的專用導通電阻依然太高。在本領域中,依然有改善LDMOS裝置的需求,尤其是具有較低專用導通電阻的高電壓LDMOS裝置。 High voltage LDMOS devices have different uses in semiconductors. E.g, The LDMOS device can be used to convert a relatively high voltage to a relatively low voltage or as a switching power transistor that is configured to drive a load. However, since the N-level region and the P-type fully doped region interact with each other, the dedicated on-resistance of the conventional high-voltage LDMOS is still too high. There is still a need in the art to improve LDMOS devices, especially high voltage LDMOS devices with lower dedicated on-resistance.

本發明之實施例提供半導體裝置,尤其是金屬氧化物半導體(MOS)裝置。 Embodiments of the present invention provide semiconductor devices, particularly metal oxide semiconductor (MOS) devices.

本發明之一面向包括半導體,例如,金屬氧化物半導體(MOS)裝置,其包含P基板、高電壓N井(HVNW)設置於P基板中、第一P井形成於有第一P+摻雜區的P基板中、第二P井形成於有第二P井其緊鄰於N+摻雜源極區的HVNW中、分離的N能階以及形成於HVNW中的分離的P頂區。分離N能階以及P頂區有至少一或多層,其中每一層包含多個P頂區,其散佈於多個N能階區段間。 One aspect of the present invention is directed to a semiconductor, such as a metal oxide semiconductor (MOS) device, comprising a P substrate, a high voltage N well (HVNW) disposed in a P substrate, and a first P well formed in a first P + doping In the P substrate of the region, the second P well is formed in the HVNW having the second P well adjacent to the N + doped source region, the separated N energy level, and the separated P top region formed in the HVNW. The separated N energy level and the P top region have at least one or more layers, wherein each layer includes a plurality of P top regions interspersed between the plurality of N energy level segments.

本發明之實施例中分離的N能階與P頂區包括兩層或兩層以上,而複數個P頂區段以及複數個N能階區段為崩潰交叉(criss-cross)調整。 In the embodiment of the present invention, the separated N-level and P-top regions comprise two or more layers, and the plurality of P-top segments and the plurality of N-energy segments are subjected to a criss-cross adjustment.

根據本發明之實施例,複數個分離的P頂區段在該HVNW具有深度以定義複數個深度;寬度以定義複數個寬度;選自垂直鄰接分開的N能機區段之間隔距離以定義複數個間隔距離。在本發明之某些實施例中,複數個深度可相同,在本發明之其他實施例中,複數個深度呈現遞增。 In accordance with an embodiment of the present invention, a plurality of separate P-top segments have a depth at the HVNW to define a plurality of depths; a width to define a plurality of widths; and a separation distance from a vertically adjacent N-energy segment to define a complex number Separation distance. In some embodiments of the invention, the plurality of depths may be the same, and in other embodiments of the invention, the plurality of depths are incremented.

根據本發明之實施例,半導體可是橫向擴散金屬氧 化物半導體(LDMOS)。在本發明之某些實施例中,相較於其他有連續P頂區設置於連續N能階區下的LDMOS裝置,P頂區段間的每一個深度、P頂區段的寬度以及間隔距離,其在汲極電壓1伏特時的導通電阻約減少11.6%。根據本發明之實施例,該LDMOS裝置的崩潰電壓與具有連續P頂區的LDMOS裝置的崩潰電壓相同。 According to an embodiment of the invention, the semiconductor may be laterally diffused metal oxygen Semiconductor semiconductor (LDMOS). In some embodiments of the present invention, each depth between the P top segments, the width of the P top segment, and the separation distance compared to other LDMOS devices having a continuous P top region disposed under the continuous N energy level region Its on-resistance at the drain voltage of 1 volt is reduced by approximately 11.6%. According to an embodiment of the invention, the breakdown voltage of the LDMOS device is the same as the breakdown voltage of an LDMOS device having a continuous P top region.

在本發明之某些實施例中,相較於其他有連續P頂區設置於連續N能階區下的LDMOS裝置,複數個分離的N能階區段在該HVNW具有深度以定義複數個深度;寬度以定義複數個寬度;選自垂直鄰接分離的N能階區段的間隔距離以定義複數個間隔距離,以致在汲極電壓1伏特時的導通電阻約減少11.6%。 In some embodiments of the present invention, a plurality of separate N energy level segments have depth at the HVNW to define a plurality of depths compared to other LDMOS devices having a continuous P top region disposed under a continuous N energy level region. Width to define a plurality of widths; a separation distance selected from vertically adjacent N-energy segments to define a plurality of separation distances such that the on-resistance at a drain voltage of 1 volt is reduced by about 11.6%.

在本發明之實施例中,MOS裝置為LDMOS裝置且HVNW有N+摻雜汲極區。 In an embodiment of the invention, the MOS device is an LDMOS device and the HVNW has an N + doped drain region.

MOS裝置更可包括場氧化隔離區以使第一P+摻雜區與第二P+摻雜區隔離,其中第二P+摻雜區鄰近於HVNW的N+摻雜源極區以及摻雜區。例如,場氧化隔離區LDMOS裝置將第一P+摻雜區與第二P+摻雜區隔離,其中第二P+摻雜區鄰近於HVNW的N+摻雜源極區以及N+摻雜汲極區。 The MOS device may further include a field oxide isolation region to isolate the first P + doped region from the second P + doped region, wherein the second P + doped region is adjacent to the N + doped source region of the HVNW and doped Area. For example, the field oxide isolation region LDMOS device isolates the first P + doped region from the second P + doped region, wherein the second P + doped region is adjacent to the N + doped source region of the HVNW and the N + doping Bungee area.

MOS結構更包括閘極結構,其設置於HVNW的N+摻雜源區域與摻雜區之間。例如,LDMOS裝置包括閘極結構,其設置於HVNW的N+摻雜源極區與N+摻雜汲極區之間。 The MOS structure further includes a gate structure disposed between the N + doped source region and the doped region of the HVNW. For example, the LDMOS device includes a gate structure disposed between the N + doped source region of the HVNW and the N + doped drain region.

在本發明之某些實施例中,MOS裝置可為絕緣閘極雙極電晶體,其中第三P+摻雜區設置於HVNW中。在本發明之某些實施例中,MOS裝置可為二極體,其中N+摻雜汲極區設置於HVNW中。 In some embodiments of the invention, the MOS device can be an insulated gate bipolar transistor with a third P + doped region disposed in the HVNW. In certain embodiments of the present invention, the MOS device may be a diode, wherein the N + doped drain region is disposed in the HVNW.

本發明之一面向係為製造MOS裝置的方法,其包含 以下步驟:提供P型基板;於P型基板中形成高電壓N型井(HVNW);於P型基板中形成第一P型井;於HVNW中形成第二P型井;於HVNW中形成分開的N能階與分開的P頂區,其中分開的N能階與分開的P頂區至少有一層,且每一層包括複數個分開的P頂區段分散於HVNW的複數個分開的N能階區段中。 One aspect of the present invention is directed to a method of fabricating a MOS device, comprising The following steps: providing a P-type substrate; forming a high-voltage N-type well (HVNW) in the P-type substrate; forming a first P-type well in the P-type substrate; forming a second P-type well in the HVNW; forming a separation in the HVNW N energy level and separate P top regions, wherein the separated N energy levels and the separated P top regions have at least one layer, and each layer includes a plurality of separate P top segments dispersed in a plurality of separate N energy levels of the HVNW In the section.

製造MOS裝置的方法更包括形成場氧化隔離區。場氧化隔離區具有第一場結構重疊於第一P型井及第二P型井,以及第二場氧化結構重疊於N能階區。 The method of fabricating a MOS device further includes forming a field oxide isolation region. The field oxide isolation region has a first field structure overlapping the first P-type well and the second P-type well, and the second field oxidation structure is overlapped with the N energy level region.

製造MOS裝置的方法更包括形成閘極結構。例如,閘極結構形成的方式有:使用閘極氧化方法、形成多晶矽層以及形成間隙壁(spacer)圍繞於閘極結構。 The method of fabricating a MOS device further includes forming a gate structure. For example, the gate structure is formed by using a gate oxidation method, forming a polysilicon layer, and forming a spacer surrounding the gate structure.

製造MOS裝置的方法更包括以下步驟:於鄰近閘極結構的第二P型井中形成N+摻雜源極區;於第一P型井中形成第一P+摻雜區;於第二P型井中形成第二P+摻雜區以及形成摻雜區鄰近於HVNW中的第二場氧化結構。 The method of fabricating a MOS device further comprises the steps of: forming an N + doped source region in a second P-type well adjacent to the gate structure; forming a first P + doped region in the first P-type well; and forming a first P + doped region in the first P-type well; Forming a second P + doped region in the well and forming a doped region adjacent to the second field oxide structure in the HVNW.

在本發明之某些實施例中,摻雜區可為N+摻雜汲極區以及MOS裝置可為LDMOS裝置或二極體。在本發明之其他實施例中,摻雜區可為其他P+摻雜區以及MOS裝置可為絕緣閘極雙極電晶體(insulated gate bipolar transistor)。 In some embodiments of the invention, the doped region can be an N + doped drain region and the MOS device can be an LDMOS device or a diode. In other embodiments of the invention, the doped regions may be other P + doped regions and the MOS device may be insulated gate bipolar transistors.

在LDMOS裝置的案例中,P頂區段的數量、P頂區段的寬度、每一P頂區段到N能階區的距離以及P頂區段之間的間隔距離,與其他有連續P頂區的LDMOS裝置相比,在汲極電壓上至少減少15%,約1伏特。 In the case of the LDMOS device, the number of P top sections, the width of the P top section, the distance from each P top section to the N energy level zone, and the separation distance between the P top sections, and other continuous P Compared to the LDMOS device in the top region, the drain voltage is reduced by at least 15%, about 1 volt.

本發明之另一面向更包括製造於該發明方法的一產 品。 Another aspect of the invention further includes a product manufactured by the method of the invention Product.

本發明這些實施例與其它面向以及本發明實施例在下列描述與所附圖式結合檢閱時將成為明顯的,雖然本發明是經由所附申請專利範圍而指出其特殊性。 The embodiments of the present invention will be apparent from the following description, taken in conjunction with the appended claims,

1‧‧‧LDMOS裝置 1‧‧‧LDMOS device

10‧‧‧LDMOS區 10‧‧‧LDMOS area

20‧‧‧源極側 20‧‧‧Source side

30‧‧‧汲極側 30‧‧‧汲polar side

40‧‧‧P頂區 40‧‧‧P top area

50‧‧‧N能階區 50‧‧‧N energy level zone

60‧‧‧P基板 60‧‧‧P substrate

70‧‧‧HVNW 70‧‧‧HVNW

80‧‧‧第一P井 80‧‧‧First P well

90‧‧‧第二P井 90‧‧‧Second P well

100‧‧‧P+摻雜區 100‧‧‧P + doped area

110‧‧‧P+摻雜區 110‧‧‧P + doped area

120‧‧‧N+摻雜源極區 120‧‧‧N + doped source region

130‧‧‧N+摻雜汲極區 130‧‧‧N + doped bungee zone

140‧‧‧場氧化隔離區 140‧‧ ‧ field oxidation isolation zone

150‧‧‧控制閘極結構 150‧‧‧Control gate structure

160‧‧‧層間介電(ILD)層 160‧‧‧Interlayer dielectric (ILD) layer

170‧‧‧第一蝕刻金屬層 170‧‧‧First etched metal layer

180‧‧‧界金屬介電(IMD)層 180‧‧‧Interfacial Metal Dielectric (IMD) layer

190‧‧‧第二蝕刻金屬層 190‧‧‧Second etched metal layer

210‧‧‧LDMOS區域 210‧‧‧LDMOS area

220‧‧‧源極端 220‧‧‧ source extreme

230‧‧‧汲極端 230‧‧‧汲 extreme

240‧‧‧分離的N能階及分離的P頂區 240‧‧‧Separated N-level and separated P-top

255‧‧‧N能階區 255‧‧‧N energy level zone

245‧‧‧分離的P頂區段 245‧‧‧Separated P-top section

260‧‧‧P基板 260‧‧‧P substrate

270‧‧‧HVNW 270‧‧‧HVNW

280‧‧‧第一P井 280‧‧‧First P well

290‧‧‧第二P井 290‧‧‧Second P well

300‧‧‧P+摻雜區 300‧‧‧P + doped area

310‧‧‧P+摻雜區 310‧‧‧P + doped area

320‧‧‧N+摻雜源極區 320‧‧‧N + doped source region

330‧‧‧N+摻雜汲極區 330‧‧‧N + doped bungee zone

340‧‧‧場氧化隔離區 340‧‧‧Field Oxidation Isolation Area

350‧‧‧控制閘極結構 350‧‧‧Control gate structure

345‧‧‧閘極氧化層 345‧‧ ‧ gate oxide layer

355‧‧‧間隙壁 355‧‧‧ spacer

360‧‧‧層間介電(ILD)層 360‧‧‧Interlayer dielectric (ILD) layer

370‧‧‧第一金屬層 370‧‧‧First metal layer

365‧‧‧第一核心區 365‧‧‧First core area

375‧‧‧絕緣區 375‧‧‧Insulated area

380‧‧‧內金屬介電(IMD)層 380‧‧•Metal dielectric (IMD) layer

390‧‧‧第二金屬層 390‧‧‧Second metal layer

400‧‧‧介電層 400‧‧‧ dielectric layer

410‧‧‧第18A圖區塊 410‧‧‧第18A图块

420‧‧‧第18B圖展示之點 420‧‧‧The point shown in Figure 18B

430‧‧‧第19A圖區塊 430‧‧‧第19A图块

440‧‧‧第19B圖展示之點 440‧‧‧The point shown in Figure 19B

450‧‧‧第20A圖區塊 450‧‧‧第20A图块

460‧‧‧第20B圖展示之線 460‧‧‧Fig. 20B shows the line

470‧‧‧第21A圖區塊 470‧‧‧第21A图块

480‧‧‧第21B圖展示之線 480‧‧‧The line shown in Figure 21B

490‧‧‧第22A圖區塊 490‧‧‧第22A图块

500‧‧‧第22B圖展示之點 500‧‧‧The point shown in Figure 22B

510‧‧‧第23A圖區塊 510‧‧‧第23A图块

520‧‧‧第23B圖展示之點 520‧‧‧The point shown in Figure 23B

530‧‧‧習用LDMOS裝置 530‧‧‧Using LDMOS devices

540‧‧‧LDMOS裝置 540‧‧‧LDMOS device

550‧‧‧最大崩潰電壓 550‧‧‧Maximum breakdown voltage

560‧‧‧習用LDMOS裝置 560‧‧‧Using LDMOS devices

570‧‧‧LDMOS裝置 570‧‧‧LDMOS device

580‧‧‧導通電阻 580‧‧‧ On-resistance

600‧‧‧LDMOS裝置 600‧‧‧LDMOS device

610‧‧‧600的框線部分 Framed part of 610‧‧600

620‧‧‧分離的P頂區段 620‧‧‧Separated P top section

630‧‧‧分離的N能階區段 630‧‧‧Separated N-level segments

700‧‧‧P基板 700‧‧‧P substrate

710‧‧‧HVNW 710‧‧‧HVNW

720‧‧‧第一P井 720‧‧‧First P well

725‧‧‧第二P井 725‧‧‧Second P well

730‧‧‧第一P+摻雜區 730‧‧‧First P + doped area

735‧‧‧第二P+摻雜區 735‧‧‧Second P + doped area

740‧‧‧N+摻雜源極區 740‧‧‧N + doped source region

745‧‧‧N+摻雜汲極區 745‧‧‧N + doped bungee zone

760‧‧‧分離的N能階及分離的P頂區 760‧‧‧Separated N-level and separated P-top

770‧‧‧場氧化隔離區 770‧‧ Field Oxidation Isolation Area

780‧‧‧控制閘極結構 780‧‧‧Control gate structure

785‧‧‧層間介電層 785‧‧‧Interlayer dielectric layer

790‧‧‧導電層 790‧‧‧ Conductive layer

800‧‧‧P基板 800‧‧‧P substrate

810‧‧‧HVNW 810‧‧‧HVNW

820‧‧‧第一P井 820‧‧‧First P well

825‧‧‧第二P井 825‧‧‧Second P well

830‧‧‧第一P+摻雜區 830‧‧‧First P + doped area

835‧‧‧第二P+摻雜區 835‧‧‧Second P + doped area

840‧‧‧N+摻雜區 840‧‧‧N + doped area

845‧‧‧第三P+摻雜區 845‧‧‧ Third P + doped area

860‧‧‧分離的N能階及分離 的P頂區 860‧‧‧Separated N-level and separation P top area

870‧‧‧場氧化隔離區 870‧‧ ‧ field oxidation isolation zone

880‧‧‧控制閘極結構 880‧‧‧Control gate structure

885‧‧‧層間介電層 885‧‧‧Interlayer dielectric layer

890‧‧‧導電層 890‧‧‧ Conductive layer

900‧‧‧P基板 900‧‧‧P substrate

910‧‧‧HVNW 910‧‧‧HVNW

920‧‧‧第一P井 920‧‧‧First P well

925‧‧‧第二P井 925‧‧‧Second P well

930‧‧‧第一P+摻雜區 930‧‧‧First P + doped area

935‧‧‧第二P+摻雜區 935‧‧‧Second P + doped area

940‧‧‧N+摻雜源極區 940‧‧‧N + doped source region

945‧‧‧N+摻雜汲極區 945‧‧‧N + doped bungee zone

960‧‧‧分離的N能階及分離的P頂區 960‧‧‧Separated N-level and separated P-top

970‧‧‧場氧化隔離區 970‧‧ ‧ field oxidation isolation zone

980‧‧‧控制閘極結構 980‧‧‧Control gate structure

985‧‧‧層間介電層 985‧‧‧Interlayer dielectric layer

990‧‧‧導電層 990‧‧‧ Conductive layer

1000‧‧‧LDMOS裝置 1000‧‧‧LDMOS device

1050‧‧‧HVNW 1050‧‧‧HVNW

1060‧‧‧場氧化隔離區 1060‧‧‧Field Oxidation Isolation Zone

1070‧‧‧閘極氧化 1070‧‧‧gate oxidation

1080‧‧‧多晶矽層 1080‧‧‧Polysilicon layer

1090‧‧‧間隙壁 1090‧‧‧ spacer

1100‧‧‧第二P井及HVNW 1100‧‧‧Second P well and HVNW

1110‧‧‧第一P井及第二P井 1110‧‧‧First P well and second P well

1120‧‧‧層間介電層 1120‧‧‧Interlayer dielectric layer

1130‧‧‧層間介電層 1130‧‧‧Interlayer dielectric layer

因此本發明已經以通常用語描述,現在將參照所附圖式,其不須要按比例描繪,以及其中:第1圖係揭示LDMOS裝置的俯視圖;第2圖係揭示LDMOS區域的俯視圖;第3A圖係揭示第2圖中沿著AA’區段線之LDMOS區域的剖面圖;第3B圖係揭示第2圖中沿著BB’區段線之LDMOS區域的剖面圖;第4圖係揭示依照本發明實施例的LDMOS區域的俯視圖;第5A圖係揭示依照本發明實施例的第4圖中沿著AA’區段線之LDMOS區域的剖面圖;第5B圖係揭示依照本發明實施例的第4圖中沿著BB’區段線之LDMOS區域的剖面圖;第6A及6B圖係揭示依照本發明實施例,在高電壓N井被形成於P基板中後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第7A及7B圖係揭示依照本發明實施例,在第一P井被形成於P基板中以及第二P井被形成於HVNW中後,第4圖中 沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第8A及8B圖係揭示依照本發明實施例,在HVNW中形成第一分離N井區以及第一分離P頂區後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第9A圖係揭示依照本發明實施例,在HVNW中設置第二分離P頂區以及第二分離N井區後,第4圖中沿著AA’區段線之LDMOS區域的剖面圖;第9B圖係揭示依照本發明實施例,在HVNW中設置N能階區後,第4圖中沿著BB’區段線之LDMOS區域的剖面圖;第10A及10B圖係揭示依照本發明實施例,在形成場氧化隔離區後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第11A及11B圖係揭示依照本發明實施例,在實施閘極氧化方法後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第12A及12B圖係揭示依照本發明實施例,在形成控制閘極結構的多晶矽層後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第13A及13B圖係揭示依照本發明實施例,在形成包圍控制閘極結構的間隙壁後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第14A及14B圖係揭示依照本發明實施例,在N+摻雜源極區形成於第二P井中以及N+摻雜汲極區形成於HVNW中後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖; 第15A及15B圖係揭示依照本發明實施例,在P+摻雜區形成於第一P井中以及另一P+摻雜區形成於第二P井中後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第16A及16B圖係揭示依照本發明實施例,在形成層間介電層後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第17A及17B圖係揭示依照本發明實施例,在形成第一金屬層後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖;第18A及18B圖係TCAD模擬圖示,其展示習用LDMOS裝置在崩潰時的衝擊產生率(impact generation rate);第19A及19B圖係依照本發明實施例之TCAD模擬圖示,其揭示LDMOS裝置在崩潰時的衝擊產生率;第20A及20B圖係TCAD模擬圖示,其揭示習用LDMOS裝置在崩潰時的潛在電位(potential profile);第21A及21B圖係依照本發明實施例之TCAD模擬圖示,其揭示LDMOS裝置在崩潰時的潛在電位;第22A及22B圖係TCAD模擬圖示,其揭示習用LDMOS裝置在崩潰時的電場(electric field);第23A及23B圖係依照本發明實施例之TCAD模擬圖示,其揭示LDMOS裝置在崩潰時的電場(electric field);第24A圖係依照本發明實施例之習用LDMOS裝置以及本發明之LDMOS裝置的汲極電壓對比汲極電流的圖示;第24B圖係依照本發明實施例之習用LDMOS裝置以 及本發明之LDMOS裝置的汲極電壓對比汲極電流的另一圖示;第25圖係依照本發明實施例之LDMOS裝置的的剖面圖;第26圖係揭示依照本發明實施例之第25圖LDMOS裝置中框線部分的剖面圖,其揭示第一分離P頂區及第二分離P頂區之分離元件的寬度變化;第27圖係揭示依照本發明實施例之第25圖LDMOS裝置中框線部分的剖面圖,其揭示第一分離P頂區、第二分離P頂區、第一分離N能階區以及第二分離N能階區之分離元件之間的間隔變化;第28圖係揭示依照本發明實施例之第25圖LDMOS裝置中框線部分的剖面圖,其揭示第一分離N能階區及第二分離N能階區之分離元件的寬度變化;第29圖係揭示依照本發明實施例之第25圖LDMOS裝置中框線部分的剖面圖,其揭示第一分離N能階區、第二分離N能階區、第一分離P頂區以及第二分離P頂區之分離元件之間的間隔變化;第30圖係揭示依照本發明實施例之第25圖LDMOS裝置中框線部分的剖面圖,其揭示第一分離P頂區以及第二分離P頂區之分離元件之間的深度變化;第31圖係揭示依照本發明實施例之第25圖LDMOS裝置中框線部分的剖面圖,其揭示第一分離N能階區以及第二分離N能階區之分離元件之間的深度變化;第32A圖係揭示依照本發明實施例之N通道金屬氧 化物半導體裝置(N-channel metal oxide semiconductor device)的剖面圖,其具有複數個分離N能階區段以及複數個分離P頂區段;第32B圖係揭示依照本發明實施例之沒有分離N能階區段以及分離N能階P頂區段的N通道金屬氧化物半導體裝置的N能階區段的剖面圖;第33A圖係揭示依照本發明實施例之絕緣閘極雙極電晶體的剖面圖,其具有複數個分離N能階區段以及複數個分離P頂區段;第33B圖係揭示依照本發明實施例之沒有分離N能階區段以及分離N能階P頂區段的絕緣閘極雙極電晶體的N能階區段的剖面圖;第34A圖係揭示依照本發明實施例之二極體的剖面圖,其具有複數個分離N能階區段以及複數個分離P頂區段;第34B圖係揭示依照本發明實施例之沒有分離N能階區段以及分離N能階P頂區段的二極體的N能階區段的剖面圖;以及第34B圖係揭示依照本發明實施例之沒有分離N能階區段以及分離N能階P頂區段的二極體的N能階區段的剖面圖。 The present invention has been described with reference to the accompanying drawings, which are not necessarily to scale, and wherein: FIG. 1 is a top view of the LDMOS device; FIG. 2 is a top view of the LDMOS region; A cross-sectional view of the LDMOS region along the AA' segment line in FIG. 2 is disclosed; FIG. 3B is a cross-sectional view showing the LDMOS region along the BB' segment line in FIG. 2; A top view of an LDMOS region of an embodiment of the invention; FIG. 5A is a cross-sectional view of the LDMOS region along the AA' segment line in FIG. 4 in accordance with an embodiment of the present invention; and FIG. 5B discloses a first embodiment of the present invention. 4 is a cross-sectional view of the LDMOS region along the BB' segment line; FIGS. 6A and 6B are diagrams showing a high voltage N well formed in the P substrate, along the AA in FIG. 4, in accordance with an embodiment of the present invention. A cross-sectional view of the respective LDMOS regions of the 'and BB' segment lines; and FIGS. 7A and 7B are diagrams showing that after the first P well is formed in the P substrate and the second P well is formed in the HVNW, in accordance with an embodiment of the present invention Figure 4 is a cross-sectional view of the LDMOS region along the AA' and BB' segment lines; Figures 8A and 8B are revealed According to an embodiment of the present invention, after forming the first separated N well region and the first separated P top region in the HVNW, the cross-sectional views of the respective LDMOS regions along the AA' and BB' segment lines in FIG. 4; FIG. 9A A cross-sectional view of the LDMOS region along the AA' segment line in FIG. 4 after the second separated P top region and the second separated N well region are disposed in the HVNW according to an embodiment of the present invention; FIG. 9B reveals In accordance with an embodiment of the present invention, a cross-sectional view of the LDMOS region along the BB' segment line in FIG. 4 after the N energy level region is disposed in the HVNW; FIGS. 10A and 10B are diagrams showing the formation of the field in accordance with an embodiment of the present invention. After oxidizing the isolation region, a cross-sectional view of each of the LDMOS regions along the AA' and BB' segment lines in FIG. 4; and FIGS. 11A and 11B are diagrams showing the fourth embodiment after performing the gate oxidation method according to an embodiment of the present invention. A cross-sectional view of each of the LDMOS regions along the AA' and BB' segment lines; FIGS. 12A and 12B are diagrams showing the formation of a polysilicon layer under the control gate structure, in FIG. 4, in accordance with an embodiment of the present invention. Cross-sectional views of respective LDMOS regions of the AA' and BB' segment lines; Figures 13A and 13B show the formation of packages in accordance with an embodiment of the present invention A cross-sectional view of each of the LDMOS regions along the AA' and BB' segment lines in FIG. 4 after controlling the spacers of the gate structure; FIGS. 14A and 14B are diagrams showing N + doping in accordance with an embodiment of the present invention. After the source region is formed in the second P well and the N + -doped drain region is formed in the HVNW, the cross-sectional views of the respective LDMOS regions along the AA' and BB' segment lines in FIG. 4; FIGS. 15A and 15B It is disclosed that along the AA' and BB' section lines in FIG. 4, after the P + doped region is formed in the first P well and the other P + doped region is formed in the second P well, in accordance with an embodiment of the present invention. Cross-sectional views of respective LDMOS regions; FIGS. 16A and 16B are cross-sectional views showing respective LDMOS regions along the AA' and BB' segment lines in FIG. 4 after forming an interlayer dielectric layer in accordance with an embodiment of the present invention. 17A and 17B are cross-sectional views showing respective LDMOS regions along the AA' and BB' segment lines in FIG. 4 after forming the first metal layer; FIGS. 18A and 18B are diagrams. TCAD simulation diagram showing the impact generation rate of a conventional LDMOS device at the time of collapse; 19A and 19B are TCAD modes according to an embodiment of the present invention The figure shows the rate of impact generation of the LDMOS device at the time of collapse; the 20A and 20B diagrams are TCAD simulation diagrams, which reveal the potential profile of the conventional LDMOS device at the time of collapse; the 21A and 21B diagrams are in accordance with this TCAD simulation diagram of an embodiment of the invention, which reveals the potential potential of the LDMOS device at the time of collapse; 22A and 22B are TCAD simulation diagrams showing the electric field of the conventional LDMOS device at the time of collapse; 23A and 23B The figure is a TCAD simulation diagram according to an embodiment of the present invention, which discloses an electric field of an LDMOS device at the time of collapse; FIG. 24A is a diagram showing a drain voltage of a conventional LDMOS device according to an embodiment of the present invention and the LDMOS device of the present invention. FIG. 24B is another illustration of a threshold voltage versus a drain current of a conventional LDMOS device and an LDMOS device of the present invention; FIG. 25 is an embodiment of the present invention. Sectional view of the LDMOS device; Fig. 26 is a cross-sectional view showing the portion of the frame line in the LDMOS device of the 25th embodiment of the present invention, which discloses the division of the first separated P top region and the second separated P top region. FIG. 27 is a cross-sectional view showing a portion of a frame line in an LDMOS device according to a 25th embodiment of the present invention, which discloses a first separated P top region, a second separated P top region, and a first separated N energy. a variation of the spacing between the separation elements of the step region and the second separated N energy level region; and FIG. 28 is a cross-sectional view showing the portion of the frame line of the LDMOS device of FIG. 25 according to an embodiment of the present invention, which discloses the first separation N energy The width variation of the separation element of the step region and the second separated N energy level region; FIG. 29 is a cross-sectional view showing the frame line portion of the LDMOS device according to the 25th embodiment of the present invention, which discloses the first separated N energy level region. a variation between the separation elements of the second separated N energy level region, the first separated P top region, and the second separated P top region; and FIG. 30 illustrates a frame line of the LDMOS device according to the 25th embodiment of the present invention. a partial cross-sectional view showing a change in depth between the first separated P top region and the separated elements of the second separated P top region; and FIG. 31 is a view showing a portion of the frame line in the LDMOS device according to the 25th embodiment of the present invention. a cross-sectional view showing the first separated N energy level region and the second Depth variation between discrete elements from the N energy level region; FIG. 32A is a cross-sectional view showing an N-channel metal oxide semiconductor device having multiple separations in accordance with an embodiment of the present invention An N-level segment and a plurality of separate P-top segments; FIG. 32B discloses an N-channel MOS device having no separated N-level segments and separated N-level P-top segments in accordance with an embodiment of the present invention A cross-sectional view of an N-energy step; FIG. 33A is a cross-sectional view showing an insulated gate bipolar transistor having a plurality of discrete N-level segments and a plurality of discrete P-top segments in accordance with an embodiment of the present invention; Figure 33B is a cross-sectional view showing an N-energy step of an insulated gate bipolar transistor having no separated N-level segments and separated N-level P-top segments in accordance with an embodiment of the present invention; A cross-sectional view of a diode according to an embodiment of the present invention having a plurality of discrete N-energy segments and a plurality of separate P-top segments; and FIG. 34B discloses a non-separating N-energy segment in accordance with an embodiment of the present invention And separating the N-level P top section A cross-sectional view of a N-energy step of the body; and a 34B-throw showing an N-energy step of the dipole without separating the N-energy segment and separating the N-level P-top segment in accordance with an embodiment of the present invention Sectional view.

第35圖係為依照本發明之實施例之製造LDMOS裝置之方法的流程圖。 Figure 35 is a flow chart of a method of fabricating an LDMOS device in accordance with an embodiment of the present invention.

本發明某些實施例現在將參照所附圖式充分地在下文描述,但不是本發明的所有實施例都會展示,本發明的各種實 施例可以用很多不同形式實施,且不應該被詮釋為對實施例之侷限,反而,提供這些實施例將使本揭露滿足適用的法律規範。 Some embodiments of the present invention will now be described fully below with reference to the accompanying drawings, but not all embodiments of the invention The embodiments may be embodied in many different forms and should not be construed as being limited to the embodiments. Instead, these embodiments are provided so that this disclosure will satisfy the applicable legal.

除非上下文清楚地另外指出,本案說明書以及所附請求項中所使用的單數形式“一”以及“該”應涵蓋複數的指涉,例如,對“一P頂區段”的指涉包括複數如此的P頂區段。 The singular forms "a", "the", "the" and "the" are used in the <Desc/Clms Page number> P top section.

在本揭露中所使用的某些特定用語,它們只使用在上位與描述性概念且不為了限制之目的,所有的用語,包括技術與科學用語,除非上下文清楚地另外定義,皆具有如本發明所屬領域中的普通技藝者所普遍瞭解的相同意義;再者,如在普遍使用之字典中所定義者,應該被解釋為具有如本發明所屬領域中具有普通技藝之人所普遍瞭解的意義,以及,如在普遍使用之字典中所定義者,應該解釋為具有與在相關領域以及本揭露的上下文中它們的意義一致的意義,這些普遍地使用之用語將不會解釋成過度理想或者刻板的概念,除非上下文清楚地另外定義。 Certain terms used in the present disclosure are used in the generic and descriptive concepts only and not for the purpose of limitation, all terms, including technical and scientific terms, unless the context clearly The same meanings are generally understood by those of ordinary skill in the art; further, as defined in commonly used dictionaries, should be interpreted as having a meaning as commonly understood by those of ordinary skill in the art to which the invention pertains. And, as defined in commonly used dictionaries, should be interpreted as having meaning consistent with their meaning in the relevant art and the context of the disclosure, such commonly used terms will not be interpreted as excessively ideal or rigid. Concept, unless the context clearly defines otherwise.

本揭露所使用的“MOS裝置”意指金屬氧化半導體裝置,例如橫向擴散金屬氧化物半導體(LDMOS)、N通道金屬氧化半導體(NMOS)、絕緣閘極雙極電晶體(IGBT)以及二極體。其裝置可設置以適用於相對於其他半導體裝置的高電壓或甚至超高電壓。 As used herein, "MOS device" means a metal oxide semiconductor device such as a laterally diffused metal oxide semiconductor (LDMOS), an N-channel metal oxide semiconductor (NMOS), an insulated gate bipolar transistor (IGBT), and a diode. . The device can be arranged to be suitable for high voltages or even ultra-high voltages relative to other semiconductor devices.

本揭露所使用的“LDMOS裝置”意指具有平行源極及汲極區的金屬氧化物半導體場效電晶體(MOSFET)。根據本發明之某些實施例,本發明之LDMOS裝置的特性為高崩潰電壓以及低導通電阻。本發明之LDMOS裝置及其製造方法可使LDMOS裝置具有相對高的崩潰電壓。此外,本發明之LDMOS裝置及其製造方法 可使LDMOS裝置相對於其他習知的LDMOS裝置具有較低的導通電阻。 As used herein, "LDMOS device" means a metal oxide semiconductor field effect transistor (MOSFET) having parallel source and drain regions. In accordance with certain embodiments of the present invention, the LDMOS device of the present invention is characterized by a high breakdown voltage and a low on-resistance. The LDMOS device of the present invention and the method of fabricating the same can cause the LDMOS device to have a relatively high breakdown voltage. Further, the LDMOS device of the present invention and the method of manufacturing the same The LDMOS device can be made to have a lower on-resistance than other conventional LDMOS devices.

第4圖係揭示依照本發明實施例的LDMOS區域210的俯視圖。LDMOS區域210具有一層複數個分離設置的N能階擴散區段,其插入於複數個分離設置的P型擴散區段,其亦為分離N能階及分離P頂區240。分離N能階以及分離P頂區240從LDMOS區域210的源極端220延伸至汲極端230。分離N能階以及分離P頂區240設置於高電壓N型井(HVNW)中。故依照本發明實施例,LDMOS區域210定義為多重且分離的N能階以及分離的P頂區240,其中每一區被無分離且設置的N能階區255所分離,而其不包括複數個分離且設置的N能階區段或任何分離設置的P頂區段。 Figure 4 is a top plan view of an LDMOS region 210 in accordance with an embodiment of the present invention. The LDMOS region 210 has a plurality of discretely disposed N-level diffusion segments interposed in a plurality of separate P-type diffusion segments, which are also separated N-levels and separated P-top regions 240. The split N level and the split P top region 240 extend from the source terminal 220 of the LDMOS region 210 to the drain terminal 230. The separated N energy level and the separated P top region 240 are disposed in a high voltage N-type well (HVNW). Therefore, in accordance with an embodiment of the present invention, LDMOS region 210 is defined as a multiplexed and separated N level and a separate P top region 240, wherein each region is separated by a non-separated and set N energy level region 255, which does not include a complex number Separate and set N-level segments or any separate P-top segments.

第5A圖係揭示依照本發明實施例的第4圖中沿著AA’區段線之LDMOS區域的剖面圖。依照本發明實施例之LDMOS裝置的實施展示具有P型半導體基板或P基板260,其可以全部或部分的方式形成P型層,像是P型磊晶層,其中已設置HVNW 270。第一P井280形成於P基板260中而第二P井290形成於HVNW 270中,其中第一P井280有P+摻雜區300以及第二P井290有另一P+摻雜區310鄰近於N+摻雜源極區320。N+摻雜汲極區330已被形成於HVNW 270中。這塊LDMOS區域210包括分離的N能階及分離的P頂區240,其具有複數個分離的N能階區段250插入於複數個分離的P頂區段245。場氧化隔離區340將摻雜區300、310、320以及330分開。 Figure 5A is a cross-sectional view showing the LDMOS region along the AA' segment line in Figure 4 in accordance with an embodiment of the present invention. Implementations of LDMOS devices in accordance with embodiments of the present invention have a P-type semiconductor substrate or P-substrate 260 that may form a P-type layer, such as a P-type epitaxial layer, in all or part of the manner in which HVNW 270 has been disposed. A first P well 280 is formed in the P substrate 260 and a second P well 290 is formed in the HVNW 270, wherein the first P well 280 has a P + doped region 300 and the second P well 290 has another P + doped region. 310 is adjacent to the N + doped source region 320. The N + doped drain region 330 has been formed in the HVNW 270. The LDMOS region 210 includes a separate N-level and a separate P-top region 240 having a plurality of discrete N-level segments 250 interposed in a plurality of separate P-top segments 245. Field oxide isolation region 340 separates doped regions 300, 310, 320, and 330.

任何習用的控制閘極結構350均可用於LDMOS裝置。例如,控制閘極結構350可包括配至於介電層上的導電層。 控制閘極結構350更包括介電側壁間隙壁。層間介電(ILD)層360設置於所述之結構上。第一金屬層370包括透過ILD層360的接觸網路(network of contacts)。本實施例中第4圖的LDMOS裝置展示內金屬介電(IMD)層380設置於第二蝕刻的金屬層390上以提供透過IMD層380的接觸網路。 Any conventional control gate structure 350 can be used for the LDMOS device. For example, the control gate structure 350 can include a conductive layer that is disposed on the dielectric layer. The control gate structure 350 further includes a dielectric sidewall spacer. An interlayer dielectric (ILD) layer 360 is disposed on the structure. The first metal layer 370 includes a network of contacts that pass through the ILD layer 360. The LDMOS device of FIG. 4 in this embodiment shows an inner metal dielectric (IMD) layer 380 disposed on the second etched metal layer 390 to provide a contact network through the IMD layer 380.

第5B圖係揭示第4圖中沿著BB’區段線之LDMOS區域的剖面圖。依照本發明實施例之LDMOS裝置的剖面圖具有如第5圖相同之結構,惟分離的N能階區段及分離的P頂區段沒有設置在HVNW 270中。更確切地說,N能階區255設置於HVNW 270中。故依照本發明的實施例,第3B圖所顯示之習用結構的剖面以及第5B圖所顯示之發明的LDMOS裝置之剖面可實質地相似。第3A圖所顯示之習用結構的剖面以及第5A圖所顯示之發明的LDMOS裝置之剖面不同 Fig. 5B is a cross-sectional view showing the LDMOS region along the BB' segment line in Fig. 4. A cross-sectional view of an LDMOS device in accordance with an embodiment of the present invention has the same structure as in FIG. 5 except that separate N-energy segments and separate P-top segments are not disposed in HVNW 270. More specifically, the N energy level region 255 is disposed in the HVNW 270. Thus, in accordance with an embodiment of the present invention, the cross-section of the conventional structure shown in FIG. 3B and the cross-section of the LDMOS device of the invention shown in FIG. 5B may be substantially similar. The cross section of the conventional structure shown in Fig. 3A and the cross section of the LDMOS device shown in Fig. 5A are different.

第6A圖至第17B圖係本發明用以製造LDMOS裝置所描述之完整步驟的LDMOS裝置的剖面圖。圖編號以A結尾係沿著AA’區段線之LDMOS裝置之剖面的說明,以第4圖為例,展示分離的N能階及分離的P頂區240,而圖編號以B結尾係沿著BB’區段線之LDMOS裝置之剖面的說明,以第4圖為例,只展示N能階區255。 6A through 17B are cross-sectional views of the LDMOS device of the present invention for fabricating the complete steps described for the LDMOS device. The figure number ends with a description of the section of the LDMOS device along the AA' segment line. Taking Figure 4 as an example, the separated N level and the separated P top area 240 are shown, and the figure number ends with B. For the description of the cross section of the LDMOS device of the BB' segment line, taking the fourth figure as an example, only the N energy level region 255 is shown.

第6A及6B圖係揭示依照本發明實施例,在高電壓N井(HVNW)270被形成於P基板260中後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。HVNW 270從P基板260的上端部分開始往下延伸。形成HVNW 270的方法典型地包括沈積光阻以定義區域,其中HVNW 270會被形成於P基板260之中,接 著微影及顯影HVNW 270所需的圖案及位置。例如,植入法可透過微影的、光罩顯影的P基板260之磊晶層實施。在本發明之某些實施例中,植入法跟隨著N井驅入步驟(drive-in step)。驅入步驟典型地在升溫的某些時期發生。在本發明之某些實施例中,任何地方都有驅入步驟的升溫且於一1,000℃至1,150℃的範圍中持續一段從20分鐘至2小時的範圍。在本發明之某些實施例中,驅入步驟方法在1,150℃持續1小時。任何殘留光阻典型地可以同量地(commensurately)在處理HVNW 270的同時移除或在處理HVNW 270完成之候接續移除。 6A and 6B are diagrams showing the LDMOS regions along the AA' and BB' segment lines in FIG. 4 after the high voltage N well (HVNW) 270 is formed in the P substrate 260, in accordance with an embodiment of the present invention. Sectional view. The HVNW 270 extends downward from the upper end portion of the P substrate 260. The method of forming HVNW 270 typically includes depositing a photoresist to define a region, wherein HVNW 270 is formed in P substrate 260, The lithography and the pattern and position required to develop the HVNW 270. For example, the implantation method can be performed by a lithographic, epitaxial layer of a reticle-developed P substrate 260. In some embodiments of the invention, the implantation method follows a N-drive-in step. The drive-in step typically occurs during certain periods of warming up. In certain embodiments of the invention, there is a temperature rise anywhere in the drive-in step and a range from 20 minutes to 2 hours in the range of from 1,000 ° C to 1,150 ° C. In certain embodiments of the invention, the drive-in step method is continued at 1,150 ° C for 1 hour. Any residual photoresist can typically be removed in the same manner as the HVNW 270 is processed or removed while the HVNW 270 is being processed.

第7A及7B圖係揭示依照本發明實施例,在第一P井280被形成於P基板260中以及第二P井290被形成於HVNW 270中後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。P井可透過使用微影技術及採用P型雜質離子植入法於所需的層。在本發明之某些實施例中,離子植入法可跟隨著P井驅入步驟,如同前述之驅入步驟之狀況。程序也包括移除任何殘留光阻。第一P井280及第二P井290可實質且同時地形成或用不同步驟形成,後者較佳,如果分開類型(separate types)的離子分別要植入P基板260及HVNW 270中。 7A and 7B show that after the first P well 280 is formed in the P substrate 260 and the second P well 290 is formed in the HVNW 270, in FIG. 4 along AA' and BB, in accordance with an embodiment of the present invention. 'A cross-sectional view of the respective LDMOS regions of the segment lines. The P well can be applied to the desired layer by using lithography and P-type impurity ion implantation. In certain embodiments of the invention, the ion implantation method can follow the P-well drive step, as in the case of the aforementioned drive-in step. The program also includes removing any residual photoresist. The first P well 280 and the second P well 290 may be formed substantially and simultaneously or in different steps, preferably the same if separate ions of the separate types are implanted into the P substrate 260 and the HVNW 270, respectively.

第8A及8B圖係揭示依照本發明實施例,在HVNW 270中形成複數個分離的P頂區段245以及複數個分離的N能階區段250後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖視圖。複數個分離的P頂區段245及複數個分離的N能階區段250展示分離的N能階及分離的P頂區240。分離的P頂區段定義為P型擴散區,而分離的N能階區段定義為N型擴散區。 8A and 8B are diagrams showing the formation of a plurality of separate P top sections 245 and a plurality of separate N energy level sections 250 in HVNW 270, along AA' and BB in Fig. 4, in accordance with an embodiment of the present invention. A cross-sectional view of the respective LDMOS regions of the segment lines. A plurality of separate P top sections 245 and a plurality of separate N energy level sections 250 exhibit separate N energy levels and separate P top areas 240. The separated P top section is defined as a P type diffusion zone, and the separated N energy level section is defined as an N type diffusion zone.

例如,第一光阻可佈置以定義要將P頂區段245形成於HVNW 270之中的區域,接續以微影方法及顯影第一需要的圖案以確認在分離的N能階及分離的P頂區240中P頂區段245的位置。植入P型離子之實施可透過以第一圖案化的且顯影的光罩將複數個P頂區段沉積入HVNW 270。植入複數個分離的P頂區段245之方法可結束於去除裝置上多餘光阻。第一光罩可移除且第二光阻可沉積以定義要將N能階區段250形成於HVNW 270之中的區域,接續以微影方法及顯影需要的圖案以確認在分離的N能階及分離的P頂區240中N能階區段250的位置。植入N型離子之實施可透過以第二圖案化的且顯影的光罩將複數個N能階區段沉積入HVNW 270。對本領域習之技藝者而言,植入方法中一或多個所述步驟及/或條件,例如,HVNW 270中每個P頂區段245及每個N能階區段250達到較佳位置的植入能量可不同。 For example, the first photoresist may be arranged to define an area in which the P top section 245 is to be formed in the HVNW 270, followed by a lithography method and development of the first desired pattern to confirm the separated N level and the separated P The location of the P top section 245 in the top zone 240. Implantation of P-type ions can deposit a plurality of P-top sections into HVNW 270 through a first patterned and developed reticle. The method of implanting a plurality of separate P top sections 245 may end with removing excess photoresist on the device. The first mask is removable and the second photoresist can be deposited to define a region in which the N level segment 250 is to be formed in the HVNW 270, followed by a lithography method and a desired pattern for development to confirm the separated N energy. The position of the N-level segment 250 in the P-top region 240 of the step and separation. The implantation of the N-type ions can deposit a plurality of N-energy segments into the HVNW 270 through the second patterned and developed photomask. One or more of the steps and/or conditions in the implantation method, for example, each P top segment 245 and each N energy segment 250 in HVNW 270 achieves a preferred position for those skilled in the art. The implant energy can vary.

第9A圖係揭示依照本發明實施例,在HVNW 270的分離的N能階及分離的P頂區240中設置額外的N能階區段250及P頂區段245後,第4圖中沿著AA’區段線之LDMOS區域的剖面圖。如之前所述,光罩可用於LDMOS裝置,例如利用微影技術以及N型載體可植入HVNW 270以定義額外的N能階區段250,而N能階區段250定義分離的N能階及分離的P頂區240。光罩可移除且另一光罩可用於LDMOS裝置以及P型載體可植入HVNW 270以定義額外的P頂區段250,而P頂區段250定義分離的N能階及分離的P頂區240。如第9B圖所示之N能階區255,其可實質地為任何分離的P頂區段及複數個分離的N能階區段。 FIG. 9A is a diagram showing an additional N-energy step 250 and a P-top segment 245 in the separated N-level and separated P-top regions 240 of the HVNW 270, in accordance with an embodiment of the present invention, in FIG. A cross-sectional view of the LDMOS region of the AA' segment line. As previously described, the reticle can be used in LDMOS devices, for example, lithography and N-type carriers can be implanted into HVNW 270 to define additional N energy level segments 250, while N energy level segments 250 define separate N energy levels. And a separate P top region 240. The reticle is removable and another reticle is available for the LDMOS device and the P-type carrier is implantable with the HVNW 270 to define an additional P-top section 250, while the P-top section 250 defines a separate N-level and separate P-top Area 240. The N energy level region 255, as shown in FIG. 9B, may be substantially any separate P top segment and a plurality of separate N energy segment segments.

分離的N能階及分離的P頂區240的每一個複數個P 頂區段245以及複數個M能階區段250可同步形成或甚至在形成分離的P頂區240中以兩或多個微影及植入步驟形成。第8A及9A圖的實施例展示兩步驟(two-step)方法以將複數個分離的P頂區段245以及複數個N能階區段植入分離的N能階及分離的P頂區240。舉例來說,當形成具有在HVNW 270中數量易變的N能階區段250及P頂區段245及所述區段之變化深度、在P頂區段245有易變的P型離子濃度、在N能階區段250中有易變的N型離子濃度及/或將部分或全部的P頂區段疊層於N能階區段上,反之亦然以及在分離的N能階及分離的P頂區240中所述區段能連接或分開的分離的N能階及分離的P頂區240時,兩個以上之步驟特別有用。 Separate N energy levels and each P of the separated P top region 240 The top section 245 and the plurality of M energy level sections 250 may be formed simultaneously or even in the formation of separate P top regions 240 in two or more lithography and implantation steps. The embodiments of Figures 8A and 9A show a two-step method for implanting a plurality of separate P top segments 245 and a plurality of N energy segments into separate N energy levels and separate P top regions 240 . For example, when forming a N-energy step 250 and a P-top section 245 that are variable in the HVNW 270 and the depth of change of the section, there is a variable P-type ion concentration in the P-top section 245. Having a variable N-type ion concentration in the N-energy step 250 and/or laminating some or all of the P-top segments on the N-energy step, and vice versa, and in the separated N-level Two or more steps are particularly useful when the separate P-top regions 240 of the separated P top region 240 are capable of connecting or separating separate N energy levels and separate P top regions 240.

在本發明之其他實施例中,可實施任何一個步驟以完成在分離N能階及分離P頂區240中複數個分離P頂區段245以及複數個N能階區段250所需要的定位。在本發明之實施例中,第9A圖之說明步驟可不實施。例如,第8A圖的說明步驟以足夠提供在分離N能階及分離P頂區240中複數個分離P頂區段245以及複數個N能階區段250所需要的定位。 In other embodiments of the invention, any of the steps may be performed to accomplish the positioning required for separating the plurality of P-top segments 245 and the plurality of N-energy segments 250 in the separated N-level and separated P-top regions 240. In an embodiment of the invention, the steps illustrated in Figure 9A may not be implemented. For example, the illustrative step of FIG. 8A is sufficient to provide the positioning required for separating the plurality of P-top segments 245 and the plurality of N-energy segments 250 in the separated N-level and separated P-top regions 240.

根據本發明之某些實施例,舉例來說,N型載體可選自元素週期表5A族中任一個或多個元素,例如,根據本發明之某些實施例可為磷。在本發明之某些實施例中,需要的N型離子可由具有至少一元素選自5A族及至少一元素選自4A族的化合物形成,例如,矽磷化合物。 According to some embodiments of the invention, for example, the N-type carrier may be selected from any one or more of the elements of Group 5A of the Periodic Table of the Elements, for example, may be phosphorus according to certain embodiments of the invention. In certain embodiments of the invention, the desired N-type ion may be formed from a compound having at least one element selected from Group 5A and at least one element selected from Group 4A, for example, a phosphonium phosphorus compound.

根據本發明之某些實施例,P型載體可選自元素週期表3A族中任一個或多個元素,例如,根據本發明之某些實施例, 經常選自硼。在本發明之某些實施例中,需要的P型離子可由具有至少一元素選自3A族及至少一元素選自4A族的化合物形成,例如,P型離子可為矽硼化合物。 According to some embodiments of the invention, the P-type carrier may be selected from any one or more of the elements of Group 3A of the Periodic Table of the Elements, for example, in accordance with certain embodiments of the present invention, Often selected from boron. In certain embodiments of the invention, the desired P-type ions may be formed from a compound having at least one element selected from Group 3A and at least one element selected from Group 4A, for example, the P-type ion may be a bismuth boron compound.

在本發明之某些實施例中,分離的N能階及分離的P頂區240包括二個、三個、四個、五個、六個、七個、八個、九個、十個或更多個分離的P頂區段245以及包括二個、三個、四個、五個、六個、七個、八個、九個、十個或更多個分離的N能階區段250。 In some embodiments of the invention, the separated N-level and separated P-top regions 240 comprise two, three, four, five, six, seven, eight, nine, ten or More separate P-top sections 245 and including two, three, four, five, six, seven, eight, nine, ten or more separate N-level sections 250 .

試圖不被理論侷限,儘管分離的P頂區段245及分離的N能階區段250的數量變化以及分離的P頂區段中P型載體的濃度可由分離的N能階區段中N型載體的濃度所平衡。更試圖不被理論侷限,分離的N能階及分離的P頂區240可設置用於改善電荷平衡以及降低LDMOS裝置的特定導通電阻。依然試圖不被理論侷限,分離的N能階及分離的P頂區240被設置用於允許在HVNW 270的延伸汲極區有向下空乏結合從P基板260的向上空乏,其不被材料所影響且提供習用LDMOS裝置實質相近的崩潰電壓。對HVNW 270摻雜可達到較低的特定導通電阻。 Attempts are not limited by theory, although the number of separated P top sections 245 and the separated N energy level sections 250 and the concentration of P-type carriers in the separated P-top sections may be N-type in the separated N-energy stage sections. The concentration of the carrier is balanced. More attempted not to be limited by theory, separate N-level and separate P-top regions 240 can be provided to improve charge balance and reduce the specific on-resistance of the LDMOS device. Still attempting not to be limited by theory, the separated N-level and separated P-top regions 240 are configured to allow upward depletion in the extended drain region of HVNW 270 to combine upward depletion from P substrate 260, which is not materialized. Affects and provides a breakdown voltage that is similar to that of a conventional LDMOS device. The HVNW 270 doping can achieve a lower specific on-resistance.

在本發明之某些實施例中,分離的N能階及分離的P頂區240可設置在接近第二P井290之處。例如,分離的P頂區段數量、HVNW 270中每一個P頂區段的位置、HVNW 270中每一個P頂區段之間以及相對於其他N能區段的位置以及其他所述之參數將會影響LDMOS裝置特定導通電阻降低的程度。此外,分離的N能階區段數量、HVNW 270中每一個N能階區段的位置、每一個N能階區段之間以及相對於其他P頂區段的位置以及其他所述之參 數將會影響LDMOS裝置特定導通電阻降低的程度。 In certain embodiments of the invention, separate N energy levels and separate P top regions 240 may be disposed proximate to the second P well 290. For example, the number of separate P-top segments, the location of each P-top segment in HVNW 270, the position between each P-top segment in HVNW 270, and relative to other N-energy segments, and other described parameters will It will affect the extent to which the specific on-resistance of the LDMOS device is reduced. In addition, the number of separated N-level segments, the position of each N-energy segment of HVNW 270, the position between each N-energy segment and relative to other P-top segments, and other such parameters The number will affect the extent to which the specific on-resistance of the LDMOS device is reduced.

最後,第9B圖所示之N能階區255係實質地為任何分離的P頂區段及複數個分離的N能階區段。 Finally, the N energy level region 255 shown in FIG. 9B is substantially any separated P top portion and a plurality of separate N energy level segments.

第10A及10B圖係揭示依照本發明實施例,在形成場氧化隔離區340後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。根據本發明之實施例,場氧化隔離區340可包括複數個將LDMOS裝置分離成不同區域的場氧化隔離結構。例如,在第10A及10B圖的實施例中,場氧化隔離區340包括分離成不同摻雜區域的場氧化隔離結構,其最後會形成第一P井280、第二P井290以及HVNW 270。 10A and 10B are cross-sectional views showing respective LDMOS regions along the AA' and BB' segment lines in Fig. 4 after forming the field oxide isolation region 340, in accordance with an embodiment of the present invention. In accordance with an embodiment of the present invention, field oxide isolation region 340 can include a plurality of field oxide isolation structures that separate LDMOS devices into different regions. For example, in the embodiment of FIGS. 10A and 10B, field oxide isolation region 340 includes field oxide isolation structures that are separated into different doped regions, which will eventually form first P well 280, second P well 290, and HVNW 270.

根據本發明之實施例,場氧化隔離區340可由使用相對厚的場氧化層而形成,例如,根據本發明之某些實施例,如第10A及10B圖所示,沿著LDMOS的上表面長出1微米或更大的尺度,接續施以光罩以及蝕刻以定義上表面的某些部分。 In accordance with an embodiment of the present invention, field oxide isolation region 340 may be formed using a relatively thick field oxide layer, for example, along the upper surface of LDMOS, as shown in Figures 10A and 10B, in accordance with certain embodiments of the present invention. On a scale of 1 micron or larger, a mask and etching are applied to define certain portions of the upper surface.

在本發明之某些實施例中,場氧化隔離區340可在成長後蝕刻以隔離LDMOS裝置的某些區域。例如,實質統一的場氧化層可應用於場氧化擴散。光阻可應用於成長場氧化層及接續進行微影及顯影以識別場氧化隔離層中要以蝕刻去除某些部分之區域。接續於蝕刻程序,任何殘留光阻可被移除,而複數個場氧化結構留存以定義場氧化隔離區340。在本發明之某些實施例中,前導材料像是墊氧化層(pad oxide)及/或矽氮化物可同樣被應用以及場氧化物氧化方法建立以蝕刻定義的結構中的場氧化物。 In some embodiments of the invention, the field oxide isolation regions 340 may be etched after growth to isolate certain regions of the LDMOS device. For example, a substantially uniform field oxide layer can be applied to field oxide diffusion. The photoresist can be applied to the growth field oxide layer and successively subjected to lithography and development to identify areas of the field oxide isolation layer that are to be etched to remove portions. Following the etch process, any residual photoresist can be removed and a plurality of field oxide structures remain to define the field oxide isolation region 340. In some embodiments of the invention, a precursor material such as a pad oxide and/or a germanium nitride may be applied as well as a field oxide oxidation process to etch the field oxide in the defined structure.

第11A及11B圖係揭示依照本發明實施例,在以實施閘極氧化方法形成閘極氧化層345後,第4圖中沿著AA’及BB’ 區段線各自之LDMOS區域的剖面圖。閘極氧化方法可包括犧牲氧化步驟,其透過將矽表面暴露於氧氣中一段時間,使氧化物成長進入矽表面。典型地,犧牲氧化方法在升高的溫度中實施,例如,從約800℃至約1,000℃或是更高的溫度範圍。在本發明之某些實施例中,升高的溫度可在從約850℃至約950℃的溫度範圍之間。依然在本發明之其他實施例中,升高的溫度可為約900℃。 11A and 11B are diagrams showing AA' and BB' in FIG. 4 after forming a gate oxide layer 345 by performing a gate oxidation method according to an embodiment of the present invention. A cross-sectional view of the respective LDMOS regions of the segment lines. The gate oxidation process can include a sacrificial oxidation step that causes the oxide to grow into the surface of the crucible by exposing the surface of the crucible to oxygen for a period of time. Typically, the sacrificial oxidation process is carried out at elevated temperatures, for example, from about 800 ° C to about 1,000 ° C or higher. In certain embodiments of the invention, the elevated temperature may be between a temperature range from about 850 °C to about 950 °C. In still other embodiments of the invention, the elevated temperature can be about 900 °C.

犧牲氧化方法可接續於閘極清理方法或更適當地,預先閘極清理方法(pre-gate clean process)以去除表面上要應用控制閘極處的本質氧化物。任何習用預先閘極清理方法均可使用。例如,預先閘極清理方法使用HF、HCL或臭氧以清潔要形成閘極氧化物處所需要的區域。最後,閘極氧化步驟可被使用來形成閘極氧化層345。 The sacrificial oxidation process can be followed by a gate cleaning process or, more suitably, a pre-gate clean process to remove the essential oxides on the surface where the control gate is to be applied. Any conventional pre-gate cleaning method can be used. For example, the pre-gate cleaning method uses HF, HCL, or ozone to clean the area needed to form the gate oxide. Finally, a gate oxidation step can be used to form the gate oxide layer 345.

第12A及12B圖係揭示依照本發明實施例,在形成控制閘極結構350的多晶矽層後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。形成多晶矽層的程序包括沈積多晶矽於閘極氧化層345,沈積方法常用化學氣相沈積法。多晶矽之沈積可接續沈積鎢矽化物(WSix),其結合於多晶矽層,常稱之為金屬矽化物(polycide)。微影方法步驟可用於定義金屬矽化物層將在蝕刻後殘留的區域。完成蝕刻後,定義控制閘極結構350多晶矽層存留。 12A and 12B are cross-sectional views showing respective LDMOS regions along the AA' and BB' segment lines in Fig. 4 after forming the polysilicon layer of the control gate structure 350 in accordance with an embodiment of the present invention. The procedure for forming the polysilicon layer includes depositing polysilicon in the gate oxide layer 345, which is commonly performed by chemical vapor deposition. The deposition of polycrystalline germanium can continue to deposit tungsten germanide (WSix), which is bonded to the polycrystalline germanium layer, often referred to as a metal cyanide (polycide). The lithography method step can be used to define the area where the metal telluride layer will remain after etching. After the etching is completed, the polysilicon layer of the control gate structure 350 is defined to remain.

第13A及13B圖係揭示依照本發明實施例,在形成包圍控制閘極結構350的多晶矽層的間隙壁(spacer)355後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。在本發明之實施例中。四乙氧基矽烷(TESO)的共形層可設置於LDMOS 裝置的表面。微影方法可用於定義包圍控制閘極結構350的殘留間隙壁355。已上光罩的表面可被蝕刻來形成包圍控制閘極結構350的殘留間隙壁355。較佳地,間隙壁355也可被視為控制閘極結構350的一部份。 13A and 13B are diagrams showing the respective LDMOS along the AA' and BB' segment lines in FIG. 4 after forming a spacer 355 surrounding the polysilicon layer of the control gate structure 350, in accordance with an embodiment of the present invention. A section view of the area. In an embodiment of the invention. The conformal layer of tetraethoxy decane (TESO) can be placed in LDMOS The surface of the device. The lithography method can be used to define a residual spacer 355 that surrounds the control gate structure 350. The surface of the reticle can be etched to form a residual spacer 355 that surrounds the control gate structure 350. Preferably, the spacer 355 can also be considered as part of the control gate structure 350.

第14A及14B圖係揭示依照本發明實施例,在N+摻雜源極區320形成於第二P井290中以及N+摻雜汲極區330形成於HVNW 270中後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。每一個N+摻雜區320及330可被植入各自之區域,方法為沈積光阻以定義N+摻雜區320及330要形成之處,接續以微影及顯影需要的圖案以識別N+摻雜區320及330的位置。N+離子可被植入或注入由光罩定義的區域以將N+摻雜源極區320形成於第二P井290中以及將N+摻雜汲極區330形成於HVNW 270中。在本發明之某些實施例中,每一個N+摻雜區320及330可由類似前述但分開的程序形成。 14A and 14B show that after the N + doped source region 320 is formed in the second P well 290 and the N + doped drain region 330 is formed in the HVNW 270, in FIG. 4, in accordance with an embodiment of the present invention, A cross-sectional view of the respective LDMOS regions along the AA' and BB' segment lines. Each of the N + doped regions 320 and 330 can be implanted in a respective region by depositing a photoresist to define where the N + doped regions 320 and 330 are to be formed, followed by lithography and development of the desired pattern to identify N + Doped regions 320 and 330 locations. The N + ions can be implanted or implanted into the region defined by the reticle to form the N + doped source region 320 in the second P well 290 and the N + doped drain region 330 in the HVNW 270. In some embodiments of the invention, each of the N + doped regions 320 and 330 may be formed by a process similar to that described above but separate.

第15A及15B圖係揭示依照本發明實施例,在P+摻雜區300形成於第一P井280中以及另一P+摻雜區310形成於第二P井290中後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。在本發明之某些實施例中,第二P井290的P+摻雜區310鄰近於第二P井290的N+摻雜源極區320。 15A and 15B show that after the P + doping region 300 is formed in the first P well 280 and the other P + doping region 310 is formed in the second P well 290, in accordance with an embodiment of the present invention, FIG. 4 A cross-sectional view of the respective LDMOS regions along the AA' and BB' segment lines. In some embodiments of the invention, the P + doped region 310 of the second P well 290 is adjacent to the N + doped source region 320 of the second P well 290.

每一個P+摻雜區330及310可被植入各自之區域,方法為沈積光阻以定義P+摻雜區300及310要形成之處,接續以微影及顯影需要的圖案以識別N+摻雜區300及310的位置。P+離子可被植入或注入由光罩定義的區域以將P+摻雜源極區300形成於第一P井280中以及將P+摻雜汲極區310形成於第二P井290中。 在本發明之某些實施例中,每一個P+摻雜區300及310可由類似前述但分開的程序形成。 Each of the P + doped regions 330 and 310 can be implanted in a respective region by depositing a photoresist to define where the P + doped regions 300 and 310 are to be formed, followed by a pattern required for lithography and development to identify N + Doped regions 300 and 310 locations. P + ions may be implanted or implanted into regions defined by the reticle to form P + doped source regions 300 in the first P well 280 and P + doped drain regions 310 in the second P well 290 in. In some embodiments of the invention, each P + doped region 300 and 310 may be formed by a process similar to that described above but separate.

第16A及16B圖係揭示依照本發明實施例,在形成層間介電(ILD)層360後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。ILD層360可由第一沈積層間介電材料於LDMOS裝置而形成。微影方法可接續用於建立圖案化的光阻以定義將有導電材料形成之處的第一核心區365。最後,第一核心區365將會被蝕刻以決定ILD層360的結構。 16A and 16B are cross-sectional views showing respective LDMOS regions along the AA' and BB' segment lines in Fig. 4 after forming the interlayer dielectric (ILD) layer 360, in accordance with an embodiment of the present invention. The ILD layer 360 can be formed from a first deposited interlayer dielectric material to the LDMOS device. The lithography method can then be used to create a patterned photoresist to define a first core region 365 where the conductive material will be formed. Finally, the first core region 365 will be etched to determine the structure of the ILD layer 360.

第17A及17B圖係揭示依照本發明實施例,在形成第一金屬層370後,第4圖中沿著AA’及BB’區段線各自之LDMOS區域的剖面圖。第一金屬層370的第一金屬可沿著ILD層360設置以實質地填充定義於ILD層360中的第一核心區360。微影方法可接續用於建立圖案化的光阻以定義將有界金屬介電(IMD)層380的介電材料形成之處的絕緣區375。最後,絕緣區375將會被蝕刻以決定第一金屬層370的結構。 17A and 17B are cross-sectional views showing respective LDMOS regions along the AA' and BB' segment lines in Fig. 4 after forming the first metal layer 370, in accordance with an embodiment of the present invention. The first metal of the first metal layer 370 can be disposed along the ILD layer 360 to substantially fill the first core region 360 defined in the ILD layer 360. The lithography method can then be used to create a patterned photoresist to define an insulating region 375 where the dielectric material of the bounded metal dielectric (IMD) layer 380 is formed. Finally, the insulating region 375 will be etched to determine the structure of the first metal layer 370.

接續層可相同地被應用。例如,如第5A及5B圖所示之實施例,IMD層380可應用於第一金屬層370。具有第二絕緣區的第二金屬層390可應用於IMD層380。另一介電層400,例如,可應用於第二金屬層390。 The splicing layers can be applied identically. For example, as in the embodiment illustrated in FIGS. 5A and 5B, the IMD layer 380 can be applied to the first metal layer 370. A second metal layer 390 having a second insulating region can be applied to the IMD layer 380. Another dielectric layer 400, for example, can be applied to the second metal layer 390.

第18A及18B圖係TCAD模擬圖示,其展示習用LDMOS裝置在崩潰時的衝擊產生率(impact generation rate)。第18B圖係為第18A圖區塊410更詳細的展示。第18B圖展示之點420為裝置中最大衝擊產生率發生處。第19A圖係依照本發明實施例之TCAD模擬圖示,其展示本發明之LDMOS裝置在崩潰時的衝擊產 生率。第19B圖係為第19A圖區塊430更詳細的展示。第19B圖展示之點440為裝置中最大衝擊產生率發生處。第18A至19B圖係為相對於崩潰時習用LDMOS裝置的衝擊產生率,本發明之LDMOS在崩潰時的衝擊產生率不會被的分離的N能階及分離的P頂區之材料所影響。故本發明之LDMOS裝置展示相似於習用裝置的衰退能力(depression capability)以及最大崩潰電壓不會被材料影響。 Figures 18A and 18B are TCAD simulation diagrams showing the impact generation rate of a conventional LDMOS device at the time of collapse. Figure 18B is a more detailed representation of block 110A block 410. Point 420, shown in Fig. 18B, is where the maximum impact rate in the device occurs. 19A is a TCAD simulation diagram showing the impact of the LDMOS device of the present invention in a crash according to an embodiment of the present invention. Birth rate. Figure 19B is a more detailed display of block 19A of block 19A. Point 440, shown in Figure 19B, is where the maximum impact rate occurs in the device. Figs. 18A to 19B are diagrams showing the rate of impact generation of the LDMOS of the present invention at the time of collapse, and the impact generation rate of the LDMOS of the present invention at the time of collapse is not affected by the material of the separated N level and the separated P top region. Therefore, the LDMOS device of the present invention exhibits a depression capability similar to that of the conventional device and the maximum breakdown voltage is not affected by the material.

第20A圖係TCAD模擬圖示,其展示習用LDMOS裝置在崩潰時的潛在電位(potential profile)。第20B圖係為第20A圖區塊450更詳細的展示。第20B圖展示之線450為裝置中最大潛在電位發生處。第21A圖係TCAD模擬圖示,其展示本發明之LDMOS裝置在崩潰時的潛在電位。第21B圖係為第21A圖區塊470更詳細的展示。第21B圖展示之線480為裝置中最大潛在電位發生處。第20A至21B圖係為在習用LDMOS裝置與本發明之LDMOS裝置之間,崩潰時的潛在電位分佈不會因材料而不同。故本發明之LDMOS裝置展示相似於習用裝置的潛在電位以及最大崩潰電壓不會被材料影響。 Figure 20A is a TCAD simulation diagram showing the potential profile of a conventional LDMOS device at the time of collapse. Figure 20B is a more detailed representation of block 450 of block 20A. Line 450, shown in Figure 20B, is where the maximum potential potential occurs in the device. Figure 21A is a TCAD simulation diagram showing the potential potential of the LDMOS device of the present invention in the event of a crash. Figure 21B is a more detailed representation of block 21A of block 21A. Line 480, shown in Figure 21B, is where the maximum potential potential occurs in the device. 20A to 21B are diagrams showing the potential potential distribution at the time of collapse between the conventional LDMOS device and the LDMOS device of the present invention, which does not differ depending on the material. Therefore, the LDMOS device of the present invention exhibits a potential potential similar to that of the conventional device and the maximum breakdown voltage is not affected by the material.

第22A圖係TCAD模擬圖示,其展示習用LDMOS裝置在崩潰時的電場(electric field)。第22B圖係為第22A圖區塊490更詳細的展示。第22B圖展示之點500為裝置中最大電場發生處。第23A圖係依照本發明實施例之TCAD模擬圖示,其展示本發明之LDMOS裝置在崩潰時的電場。第23B圖係為第23A圖區塊510更詳細的展示。第23B圖展示之點520為裝置中最大電場發生處。第22A至23B圖係為在習用LDMOS裝置與本發明之LDMOS裝置之 間,崩潰時的電場不會因材料而不同。故本發明之LDMOS裝置展示相似於習用裝置的電場以及最大崩潰電壓不會被材料影響。 Figure 22A is a TCAD simulation diagram showing the electric field of a conventional LDMOS device at the time of collapse. Figure 22B is a more detailed representation of block 22A of block 22A. The point 500 shown in Figure 22B is where the maximum electric field occurs in the device. Figure 23A is a diagram of a TCAD simulation in accordance with an embodiment of the present invention showing the electric field of the LDMOS device of the present invention in the event of a crash. Figure 23B is a more detailed representation of block 23A of block 23A. Point 520, shown in Figure 23B, is where the maximum electric field occurs in the device. 22A to 23B are diagrams of a conventional LDMOS device and an LDMOS device of the present invention. The electric field at the time of collapse does not vary from material to material. Therefore, the LDMOS device of the present invention exhibits an electric field similar to that of the conventional device and the maximum breakdown voltage is not affected by the material.

第24A圖係依照本發明實施例之習用LDMOS裝置530以及本發明之LDMOS裝置540的汲極電壓對比汲極電流的圖示。第24A圖係為在習用LDMOS裝置與本發明之LDMOS裝置之間,最大崩潰電壓550相同。然而,對比於在高汲極電壓的習用LDMOS裝置,本發明之LDMOS裝置汲極電流可能會增加的是因為本發明之裝置在電壓靠近崩電壓時具有較低的電阻。 Figure 24A is a graphical representation of the gate voltage vs. gate current of a conventional LDMOS device 530 and an LDMOS device 540 of the present invention in accordance with an embodiment of the present invention. Fig. 24A shows the maximum breakdown voltage 550 between the conventional LDMOS device and the LDMOS device of the present invention. However, in contrast to conventional LDMOS devices with high drain voltages, the LDMOS device of the present invention may increase the drain current because the device of the present invention has a lower resistance when the voltage is close to the collapse voltage.

第24B圖係依照本發明實施例之習用LDMOS裝置560以及本發明之LDMOS裝置570的汲極電壓對比汲極電流的另一圖示。第24B圖係為對於有連續P頂區的習用LDMOS裝置導通電阻,本發明之LDMOS裝置在汲極電壓為1伏特時,導通電阻580有11.6%的改善幅度。 Figure 24B is another illustration of the gate voltage versus the drain current of the conventional LDMOS device 560 and the LDMOS device 570 of the present invention in accordance with an embodiment of the present invention. Figure 24B shows the on-resistance of a conventional LDMOS device having a continuous P top region. The LDMOS device of the present invention has an improvement in the on-resistance 580 of 11.6% when the drain voltage is 1 volt.

第25圖係依照第5A圖的本發明實施例之LDMOS裝置600的的剖面圖。依照本發明實施例,LDMOS裝置600的框線部分610展示複數個分離的P頂區段620以及複數個分離的N能階區段630。 Figure 25 is a cross-sectional view of an LDMOS device 600 in accordance with an embodiment of the present invention in accordance with Figure 5A. In accordance with an embodiment of the invention, the frame portion 610 of the LDMOS device 600 exhibits a plurality of separate P top segments 620 and a plurality of separate N energy segments 630.

第26圖係揭示第25圖LDMOS裝置600中框線部分610的剖面圖細節,其揭示五個分別有WP1、WP2、WP3、WP4及WP5寬度的分離的P頂區段620。如前所述,在分離的N能階及分離的P頂區中可有任何數量的分離的P頂區段620,但了清楚顯示,第26圖展示之實施例有五個分離的P頂區段620。更詳細地說明,第26圖之實施例展示分離的N能階及分離的P頂區具有第一複數個P頂區段散佈於第一複數個分離的N能階區段之間的底層以及 第二複數個N能階段散佈於第二複數個分離的N能階區段之間的頂層。在第26圖的實施例中,底層之展示為第一底部區段,其為分離的P頂區段,接續為第二底部區段,其為分離的N能階區段,接續為第三底部區段,其為另一分離的P頂區段,接續為第四底部區段,其為另一分離的N能階區段,接續為第五底部區段,其為另一分離的P頂區段。在第26圖的實施例中,頂層之展示為實質地對準於第一底部區段的第一頂部區段,其為分離的N能階區段,接續為實質地對準於第二底部區段的第二頂部區段,其為分離的P頂區段,接續為實質地對準於第三底部區段的第三頂部區段,其為另一分離的N能階區段,接續為實質地對準於第四底部區段的第四頂部區段,其為另一分離的P頂區段,接續為實質地對準於第五底部區段的第五頂部區段,其為另一分離的N能階區段。依照本發明之實施例,第26圖所示的頂層與底層結構展示一種調整(arrangement),其為前述分離的P頂區段及分離的N能階區段的崩潰交叉調整(criss-cross arrangement)。 Figure 26 is a cross-sectional view detailing the frame portion 610 of the LDMOS device 600 of Figure 25, showing five separate P-top segments 620 having W P1 , W P2 , W P3 , W P4 and W P5 widths, respectively. . As previously mentioned, there may be any number of separate P-top segments 620 in the separated N-level and separated P-top regions, but it is clear that the embodiment shown in Figure 26 has five separate P-tops. Section 620. In more detail, the embodiment of Figure 26 shows that the separated N-level and separated P-top regions have a first plurality of P-top segments interspersed between the first plurality of discrete N-level segments and A second plurality of N energy stages are interspersed between the second plurality of discrete N energy level segments. In the embodiment of Figure 26, the bottom layer is shown as a first bottom section, which is a separate P-top section, followed by a second bottom section, which is a separate N-energy section, followed by a third a bottom section, which is another separate P-top section, continuing as a fourth bottom section, which is another separate N-energy section, followed by a fifth bottom section, which is another separate P Top section. In the embodiment of Figure 26, the top layer is shown as being substantially aligned with the first top section of the first bottom section, which is a separate N energy level section, which is subsequently substantially aligned with the second bottom a second top section of the section, which is a separate P top section, followed by a third top section substantially aligned with the third bottom section, which is another separate N energy level section, followed by To be substantially aligned with the fourth top section of the fourth bottom section, which is another separate P top section, followed by a fifth top section substantially aligned with the fifth bottom section, which is Another separate N energy level segment. In accordance with an embodiment of the present invention, the top and bottom structures illustrated in FIG. 26 exhibit an arrangement that is a crash-cross arrangement of the aforementioned separate P-top segments and separate N-energy segments. ).

在本發明之實施例中,分離的P頂區段620的寬度WP1、WP2、WP3、WP4及WP5可實質地相同。在其他某些實施例中,分離的P頂區段620的寬度WP1、WP2、WP3、WP4及WP5可不相同以在不實質地影響最大崩潰電壓下,於導通電阻中達到需要的削減。在本發明之某些實施例中,分離的P頂區段620中的P型離子植入濃度可不相同,使得縱使分離的P頂區段620之寬度不同,亦可達到完整耗盡的條件。在本發明之某些實施例中,沿著間隙壁距離SP1、SP2、SP3及SP4以及深度DP1、DP2、DP3、DP4及DP5對分離的P頂區段620的植入濃度及深度的同步調整可提供改善的導通電阻,而依然實 質地且同時地保持高崩潰電壓。 In an embodiment of the invention, the widths W P1 , W P2 , W P3 , W P4 , and W P5 of the separated P top sections 620 may be substantially the same. In other embodiments, the widths W P1 , W P2 , W P3 , W P4 , and W P5 of the separated P top sections 620 may be different to achieve the need in the on-resistance without substantially affecting the maximum breakdown voltage. The cut. In certain embodiments of the invention, the P-type ion implantation concentrations in the separate P-top sections 620 may be different such that even though the widths of the separated P-top sections 620 are different, complete depletion conditions may be achieved. In some embodiments of the invention, the separated P-top segments 620 are separated along the gap walls S P1 , S P2 , S P3 , and S P4 and the depths D P1 , D P2 , D P3 , D P4 , and D P5 . Synchronous adjustment of implant concentration and depth provides improved on-resistance while still maintaining a high breakdown voltage substantially and simultaneously.

第27圖係揭示第25圖LDMOS裝置600中框線部分610的剖面圖細節,其展示五個分離的P頂區段620及五個分離的N能階區段630,其中在上部區域的分離的N能階區段與在下部區域的分離的N能階區段由間隙壁距離SP1、SP2、SP3及SP4各自設置於上端與下端。分離的P頂區但及分離的N能階區段可為任何數量,但為第27圖之顯示目的,其展示之實施例各有五個。在本發明之實施例中,距離SP1、SP2、SP3及SP4可實質地相同。在本發明之其他實施例中,距離SP1、SP2、SP3及SP4可不相同以在不實質地影響最大崩潰電壓下,於導通電阻中達到需要的削減。在本發明之某些實施例中,分離的P頂區段620以及包括P頂區段寬度的分離的N能階區段630中的N型離子植入濃度中的P型離子植入濃度可不相同,使得縱使間隙壁距離SP1、SP2、SP3及SP4不同,亦可達到完整耗盡的條件。在本發明之某些實施例中,對分離的P頂區段620的植入濃度及寬度以及有一前一後的間隙壁距離SP1、SP2、SP3及SP4之分離的N能階區段630的植入濃度同步調整可提供改善的導通電阻,而依然實質地且同時地保持高崩潰電壓。 Figure 27 is a cross-sectional view detailing the frame line portion 610 of the LDMOS device 600 of Figure 25, showing five separate P top segments 620 and five separate N energy segments 630, wherein the separation in the upper region The N energy level section and the separated N energy level section in the lower area are respectively disposed at the upper end and the lower end by the spacer distances S P1 , S P2 , S P3 , and S P4 . The separate P top regions but separate N energy segments can be any number, but for the purposes of Figure 27, there are five embodiments shown. In an embodiment of the invention, the distances S P1 , S P2 , S P3 and S P4 may be substantially the same. In other embodiments of the invention, the distances S P1 , S P2 , S P3 , and S P4 may be different to achieve the desired reduction in on-resistance without substantially affecting the maximum breakdown voltage. In certain embodiments of the present invention, the P-type ion implantation concentration in the N-type ion implantation concentration in the separated P top section 620 and the separated N energy level section 630 including the P top section width may not The same, even if the gap walls are different from S P1 , S P2 , S P3 and S P4 , the condition of complete depletion can be achieved. In some embodiments of the invention, the implant concentration and width of the separated P top section 620 and the separated N energy levels of the gaps S P1 , S P2 , S P3 , and S P4 . Synchronous adjustment of the implant concentration of segment 630 can provide improved on-resistance while still maintaining a high breakdown voltage substantially and simultaneously.

第28圖係揭示第25圖LDMOS裝置600中框線部分610的剖面圖細節,其展示五個各自具有WN1、WN2、WN3、WN4及WN5的分離的N能階區段630。分離的N能階及分離的P頂區中分離的N能階區段630可為任何數量,但為第28圖之顯示目的,其展示之實施例有五個分離的N能階區段630。在本發明之實施例中,分離的N能階區段630的寬度WN1、WN2、WN3、WN4及WN5可實質地相同。在本發明之其他實施例中,分離的N能階區段630的寬度WN1、WN2、 WN3、WN4及WN5可不相同以在不實質地影響最大崩潰電壓下,於導通電阻中達到需要的削減。在本發明之某些實施例中,分離的N能階區段630的N型離子植入濃度可不相同,使得縱使分離的N能階區段630不同,亦可達到完整耗盡的條件。在本發明之某些實施例中,沿著間隙壁距離SN1、SN2、SN3、SN4及SN5以及DN1、DN2、DN3、DN4及DN5對分離的N能階區段630的植入濃度及寬度同步調整可提供改善的導通電阻,而依然實質地且同時地保持高崩潰電壓。 Figure 28 is a cross-sectional view detailing the frame portion 610 of the LDMOS device 600 of Figure 25, showing five separate N-level segments 630 each having W N1 , W N2 , W N3 , W N4 , and W N5 . . The separated N energy levels and the separated N energy level segments 630 in the separated P top regions can be any number, but for the purposes of the display of FIG. 28, the embodiment shown therein has five separate N energy level segments 630. . In an embodiment of the invention, the widths W N1 , W N2 , W N3 , W N4 , and W N5 of the separated N energy level segments 630 may be substantially the same. In other embodiments of the present invention, the widths W N1 , W N2 , W N3 , W N4 , and W N5 of the separated N-level segments 630 may be different to be in the on-resistance without substantially affecting the maximum breakdown voltage. Reach the required cuts. In some embodiments of the invention, the N-type ion implantation concentrations of the separated N-energy segments 630 may be different such that even if the separated N-energy segments 630 are different, complete depletion conditions may be achieved. In some embodiments of the invention, the separated N energy levels are along the gap walls S N1 , S N2 , S N3 , S N4 and S N5 and D N1 , D N2 , D N3 , D N4 and D N5 . Synchronous adjustment of the implant concentration and width of segment 630 can provide improved on-resistance while still maintaining a high breakdown voltage substantially and simultaneously.

第29圖係揭示第25圖LDMOS裝置600中框線部分610的剖面圖細節,其展示五個分離的P頂區段620以及五個分離的N能階區段630。分離的N能階及分離的P頂區中分離的N能階區段630可為任何數量,但為第28圖之顯示目的,其展示之實施例有五個分離的N能階區段630,其中在上部區域的分離的P頂區段與在下部區域的分離的P頂區段由間隙壁距離SN1、SN2、SN3及SN4各自設置於上端與下端。分離的P頂區但及分離的N能階區段可為任何數量,但為第29圖之顯示目的,其展示之實施例各有五個。在本發明之實施例中,距離SN1、SN2、SN3及SN4可實質地相同。在本發明之其他實施例中,距離SN1、SN2、SN3及SN4可不相同以在不實質地影響最大崩潰電壓下,於導通電阻中達到需要的削減。在本發明之某些實施例中,分離的P頂區段620中的P型離子植入濃度以及包括N能階區段之寬度的分離的N能階區段630中的N型離子植入濃度可不相同,使得縱使間隙壁距離SN1、SN2、SN3及SN4不同,亦可達到完整耗盡的條件。在本發明之某些實施例中,對分離的N能階區段630的植入濃度及寬度以及有一前一後的間隙壁距離SN1、SN2、SN3及SN4之分離的P頂區段620的植入濃度同步調整可提 供改善的導通電阻,而依然實質地且同時地保持高崩潰電壓。 Figure 29 is a cross-sectional detail view of the frame line portion 610 of the LDMOS device 600 of Figure 25 showing five separate P top segments 620 and five separate N energy segments 630. The separated N energy levels and the separated N energy level segments 630 in the separated P top regions can be any number, but for the purposes of the display of FIG. 28, the embodiment shown therein has five separate N energy level segments 630. The separated P top section in the upper region and the separated P top section in the lower region are respectively disposed at the upper end and the lower end by the spacer distances S N1 , S N2 , S N3 , and S N4 . The separated P top regions, but separate N energy segments, can be any number, but for the purposes of Figure 29, there are five embodiments shown. In an embodiment of the invention, the distances S N1 , S N2 , S N3 and S N4 may be substantially the same. In other embodiments of the invention, the distances S N1 , S N2 , S N3 , and S N4 may be different to achieve the desired reduction in on-resistance without substantially affecting the maximum breakdown voltage. In certain embodiments of the invention, the P-type ion implantation concentration in the separated P top section 620 and the N-type ion implantation in the separated N energy level section 630 including the width of the N energy level section The concentrations may be different, such that even if the spacers are different in distances S N1 , S N2 , S N3 and S N4 , complete depletion conditions can be achieved. In some embodiments of the invention, the implant concentration and width of the separated N-level segment 630 and the P top of the separated gap distances S N1 , S N2 , S N3 , and S N4 Synchronous adjustment of the implant concentration of segment 620 can provide improved on-resistance while still maintaining a high breakdown voltage substantially and simultaneously.

第30圖係揭示第25圖LDMOS裝置600中框線部分610的剖面圖細節,其展示五個分離的P頂區段620以及五個分離的N能階區段630,其中分離的P頂區段620各自有不同的植入深度DP1、DP2、DP3、DP4以及DP5。不同的植入深度可由改變植入方法所控制,例如植入能量。分離的P頂區段及分離的N能階區段可為任何數量,但為第30圖之顯示目的,其展示之實施例各有五個。在本發明之實施例中,深度DP1、DP2、DP3、DP4及DP5可實質地相同。在本發明之其他實施例中,深度DP1、DP2、DP3、DP4及DP5可不相同以在不實質地影響最大崩潰電壓下,於導通電阻中達到需要的削減。在本發明之某些實施例中,分離的P頂區段620中的P型離子植入濃度以及包括P頂區段寬度及間隙壁距離SP1、SP2、SP3及SP4的分離的N能階區段630中的N型離子植入濃度可不相同,使得縱使深度DP1、DP2、DP3、DP4及DP5不同,亦可達到完整耗盡的條件。在本發明之某些實施例中,對分離的P頂區段620的植入濃度及寬度、間隙壁距離SP1、SP2、SP3及SP4以及有一前一後的深度DP1、DP2、DP3及DP4之分離的N能階區段630的植入濃度同步調整可提供改善的導通電阻,而依然實質地且同時地保持高崩潰電壓。 Figure 30 is a cross-sectional view detailing the frame line portion 610 of the LDMOS device 600 of Figure 25, showing five separate P-top segments 620 and five separate N-energy segments 630 with separate P-top regions Segments 620 each have different implant depths D P1 , D P2 , D P3 , D P4 , and D P5 . Different implant depths can be controlled by changing the implantation method, such as implanting energy. The separated P-top section and the separated N-energy section can be any number, but for the purpose of display of Figure 30, there are five embodiments shown. In an embodiment of the invention, the depths D P1 , D P2 , D P3 , D P4 and D P5 may be substantially the same. In other embodiments of the invention, the depths D P1 , D P2 , D P3 , D P4 , and D P5 may be different to achieve the desired reduction in on-resistance without substantially affecting the maximum breakdown voltage. In certain embodiments of the invention, the P-type ion implantation concentration in the separated P top section 620 and the separation including the P top section width and the spacer distances S P1 , S P2 , S P3 , and S P4 The N-type ion implantation concentration in the N-energy step 630 may be different, so that even if the depths D P1 , D P2 , D P3 , D P4 , and D P5 are different, a complete depletion condition can be achieved. In some embodiments of the invention, the implant concentration and width of the separated P top section 620, the spacer distances S P1 , S P2 , S P3 , and S P4 , and the depths D P1 , D before and after The simultaneous adjustment of the implant concentration of the separate N-level segments 630 of P2 , D P3, and D P4 provides improved on-resistance while still maintaining a high breakdown voltage substantially and simultaneously.

第31圖係揭示第25圖LDMOS裝置600中框線部分610的剖面圖細節,其展示分離的N能階區段630各自有不同的植入深度DN1、DN2、DN3、DN4以及DN5。不同的植入深度可由改變植入方法所控制,例如植入能量。分離的P頂區段及分離的P頂區段可為任何數量,但為第31圖之顯示目的,其展示之實施例各有五個。在本發明之實施例中,深度DN1、DN2、DN3、DN4及DN5可實質地相同。 在本發明之其他實施例中,深度DN1、DN2、DN3、DN4及DN5可不相同以在不實質地影響最大崩潰電壓下,於導通電阻中達到需要的削減。在本發明之某些實施例中,分離的N能階區段630中的N型離子植入濃度以及包括N能階區段寬度及間隙壁距離SN1、SN2、SN3及SN4的分離的P頂區段620中的P型離子植入濃度可不相同,使得縱使深度DN1、DN2、DN3、DN4及DN5不同,亦可達到完整耗盡的條件。在本發明之某些實施例中,對分離的N能階區段630的植入濃度及寬度、間隙壁距離SN1、SN2、SN3及SN4以及有一前一後的深度DN1、DN2、DN3、DN4及DN5之分離的P頂區段620的植入濃度同步調整可提供改善的導通電阻,而依然實質地且同時地保持高崩潰電壓。 Figure 31 is a cross-sectional view detailing the frame portion 610 of the LDMOS device 600 of Figure 25, showing that the separated N-level segments 630 each have different implant depths D N1 , D N2 , D N3 , D N4 and D N5 . Different implant depths can be controlled by changing the implantation method, such as implanting energy. The separate P top section and the separated P top section can be any number, but for the purposes of Figure 31, there are five embodiments shown. In an embodiment of the invention, the depths D N1 , D N2 , D N3 , D N4 and D N5 may be substantially the same. In other embodiments of the invention, the depths D N1 , D N2 , D N3 , D N4 , and D N5 may be different to achieve the desired reduction in on-resistance without substantially affecting the maximum breakdown voltage. In some embodiments of the invention, the N-type ion implantation concentration in the separated N-level segment 630 and the N-energy segment width and the spacer distances S N1 , S N2 , S N3 , and S N4 The P-type ion implantation concentration in the separated P top section 620 can be different, so that even if the depths D N1 , D N2 , D N3 , D N4 , and D N5 are different, the condition of complete depletion can be achieved. In some embodiments of the invention, the implant concentration and width, the spacer distances S N1 , S N2 , S N3 , and S N4 of the separated N energy level segments 630 and the depth D N1 , Synchronous adjustment of the implant concentration of the separate P top sections 620 of D N2 , D N3 , D N4 , and D N5 can provide improved on-resistance while still maintaining a high breakdown voltage substantially and simultaneously.

更確切地,任何展示的常用變數,如分離的P頂區段及N能階區段的Wi、Si、Di,相對於有實質地且連續設置的P頂區的習用LDMOS裝置,分離的N能階及分離的P頂區的分離的P頂區段及分離的N能階區段中任一、組合或甚至全部均可設置用於對導通電阻提供至少5%的改善、至少10%的改善、至少15%的改善、至少20%的改善或至少25%的改善。 Rather, any of the commonly used variables shown, such as the separate P top and N energy segments, Wi, Si, Di, relative to a conventional LDMOS device with a substantially and continuously disposed P top region, separate N Any, a combination, or even all of the separate P-top segments and separate N-energy segments of the energy-producing and separated P-top regions may be provided to provide at least 5% improvement in on-resistance, at least 10% Improved, at least 15% improvement, at least 20% improvement or at least 25% improvement.

第32A圖係揭示依照本發明之實施例的N通道金屬氧化半導體(NMOS)裝置的剖面圖,特別是超高電壓NMOS裝置,其具有複數個分離的N能階區段以及複數個分離的P頂區段。第32圖之實施例係展示P基板700,其可以全部或部分的方式形成P型磊晶層,其中已設置HVNW 710。第一P井720形成於P基板700中而第二P井725形成於HVNW 710中,第一P井720有第一P+摻雜區730以及第二P井725有第二P+摻雜區735鄰近於N+摻雜源極區740。N+摻雜汲極區745形成於HVNW 710中。這塊NMOS裝 置由分離的N能階及分離的P頂區760所展示,其具有複數個分離的N能階區段以及複數個分離的P頂區段(沒有明確的框出)。場氧化隔離區770實質地將摻雜區730、735及740、745分開。NMOS也具有控制閘極結構780、層間介電層785以及導電層790。 32A is a cross-sectional view showing an N-channel metal oxide semiconductor (NMOS) device, particularly an ultra-high voltage NMOS device having a plurality of separate N-level segments and a plurality of separate Ps in accordance with an embodiment of the present invention. Top section. The embodiment of Fig. 32 shows a P substrate 700 which may form a P-type epitaxial layer in whole or in part, wherein HVNW 710 has been provided. The first P well 720 is formed in the P substrate 700 and the second P well 725 is formed in the HVNW 710, the first P well 720 has a first P + doped region 730 and the second P well 725 has a second P + doping Region 735 is adjacent to N + doped source region 740. An N + doped drain region 745 is formed in the HVNW 710. The NMOS device is shown by a separate N-level and separated P-top region 760 having a plurality of separate N-level segments and a plurality of separate P-top segments (not explicitly framed). Field oxide isolation region 770 substantially separates doped regions 730, 735 and 740, 745. The NMOS also has a control gate structure 780, an interlayer dielectric layer 785, and a conductive layer 790.

第32B圖係揭示第32A圖之NMOS裝置之沒有分離的N能階區段及分離的P頂區段的N能階區塊的剖面圖。 Figure 32B is a cross-sectional view showing the N-energy block of the NMOS device of Figure 32A without the separated N-level segment and the separated P-top segment.

第33A圖係揭示依照本發明之實施例的絕緣閘極雙極電晶體(IGBT)裝置的剖面圖,特別是超高電壓IGBT裝置,其具有複數個分離的N能階區段以及複數個分離的P頂區段。第33A圖之實施例係展示P基板800,其可以全部或部分的方式形成P型磊晶層,其中已設置HVNW 810。第一P井820形成於P基板800中而第二P井825形成於HVNW 810中,第一P井820有第一P+摻雜區830以及第二P井825有第二P+摻雜區835鄰近於N+摻雜區840。第三P+摻雜區845形成於HVNW 810中。這塊NMOS裝置由分離的N能階及分離的P頂區860所展示,其具有複數個分離的N能階區段以及複數個分離的P頂區段(沒有明確的框出)。場氧化隔離區870實質地將摻雜區830、835及840、845分開。IGBT裝置也具有控制閘極結構880、層間介電層885以及導電層890。 Figure 33A is a cross-sectional view showing an insulated gate bipolar transistor (IGBT) device in accordance with an embodiment of the present invention, particularly an ultrahigh voltage IGBT device having a plurality of discrete N-level segments and a plurality of separations P top section. The embodiment of Fig. 33A shows a P substrate 800 which may form a P-type epitaxial layer in whole or in part, wherein HVNW 810 has been provided. The first P well 820 is formed in the P substrate 800 and the second P well 825 is formed in the HVNW 810, the first P well 820 has a first P + doped region 830 and the second P well 825 has a second P + doped Region 835 is adjacent to N + doped region 840. A third P + doped region 845 is formed in the HVNW 810. The NMOS device is shown by a separate N-level and separated P-top region 860 having a plurality of separate N-level segments and a plurality of separate P-top segments (not explicitly framed). Field oxide isolation region 870 substantially separates doped regions 830, 835 and 840, 845. The IGBT device also has a control gate structure 880, an interlayer dielectric layer 885, and a conductive layer 890.

第33B圖係揭示第32A圖之IGBT裝置之沒有分離的N能階區段及分離的P頂區段的N能階區塊的剖面圖。 Figure 33B is a cross-sectional view showing the N-energy block of the IGBT device of Figure 32A without the separated N-level segment and the separated P-top segment.

第34A圖係揭示依照本發明之實施例的二極體的剖面圖,特別是超高電壓二極體,其具有複數個分離的N能階區段以及複數個分離的P頂區段。第34A圖之實施例係展示P基板900,其可以全部或部分的方式形成P型磊晶層,其中已設置HVNW 910。第一P井920形成於P基板900中而第二P井825形成於HVNW 810中,第一P井920有第一P+摻雜區930以及第二P井925有第二P+摻雜區935鄰近於N+源極摻雜區940。N+摻雜汲極區945形成於HVNW 910中。這塊NMOS裝置由分離的N能階及分離的P頂區960所展示,其具有複數個分離的N能階區段以及複數個分離的P頂區段(沒有明確的框出)。場氧化隔離區870實質地將摻雜區930、935及940、945分開。IGBT裝置也具有控制閘極結構980、層間介電層985以及導電層990。 Figure 34A is a cross-sectional view of a diode in accordance with an embodiment of the present invention, particularly an ultra high voltage diode having a plurality of discrete N energy segments and a plurality of separate P top segments. The embodiment of Fig. 34A shows a P substrate 900 which may form a P-type epitaxial layer in whole or in part, wherein HVNW 910 has been provided. The first P well 920 is formed in the P substrate 900 and the second P well 825 is formed in the HVNW 810, the first P well 920 has a first P + doped region 930 and the second P well 925 has a second P + doping Region 935 is adjacent to N + source doped region 940. An N + doped drain region 945 is formed in the HVNW 910. The NMOS device is shown by a separate N-level and separated P-top region 960 having a plurality of separate N-level segments and a plurality of separate P-top segments (not explicitly framed). Field oxide isolation region 870 substantially separates doped regions 930, 935 and 940, 945. The IGBT device also has a control gate structure 980, an interlayer dielectric layer 985, and a conductive layer 990.

第34B圖係揭示第34A圖之二極體之沒有分離的N能階區段及分離的P頂區段的N能階區塊的剖面圖。 Figure 34B is a cross-sectional view showing the N-energy block of the undivided N-energy segment and the separated P-top segment of the dipole of Figure 34A.

第35圖係為依照本發明之實施例之製造LDMOS裝置之方法的流程圖。製造LDMOS裝置1000的方法包括提供P基板1010;形成高電壓N井於P基板之中1020;形成P井於P基板及HVNW中1030;以及形成分離的P頂區於HVNW中1040,其中分離的P頂區包括複數個分離的P頂區段。在本發明之實施例中,分離的P頂區段散佈於一個或多個分離的N能階區段之間。 Figure 35 is a flow chart of a method of fabricating an LDMOS device in accordance with an embodiment of the present invention. The method of fabricating the LDMOS device 1000 includes providing a P substrate 1010; forming a high voltage N well 10 in the P substrate; forming a P well in the P substrate and the HVNW 1030; and forming a separated P top region in the HVNW 1040, wherein the separated The P top region includes a plurality of separate P top segments. In an embodiment of the invention, the separated P top sections are interspersed between one or more separate N energy level sections.

製造LDMOS裝置1000的方法更包括形成分離的N能階區於HVNW中1050,其中分離的N能階區包括一個或多個分離的M能階區段散佈於一個或多個分離的P頂區段之間。 The method of fabricating LDMOS device 1000 further includes forming a separate N energy level region in HVNW 1050, wherein the separated N energy level region includes one or more separate M energy level segments interspersed in one or more separate P top regions Between segments.

製造LDMOS裝置1000的方法更包括形成場氧化隔離區1060;形成控制閘極結構。形成控制閘極結構的步驟包括實施閘極氧化1070;形成控制閘極結構的多晶矽層1080;以及形成包圍控制閘極結構的多晶矽層的間隙壁1090。 The method of fabricating the LDMOS device 1000 further includes forming a field oxide isolation region 1060; forming a control gate structure. The step of forming the control gate structure includes performing gate oxidation 1070; forming a polysilicon layer 1080 that controls the gate structure; and forming a spacer 1090 surrounding the polysilicon layer of the control gate structure.

製造LDMOS裝置1000的方法更包括形成N+摻雜區於 第二P井及HVNW中1100;形成P+摻雜區於第一P井及第二P井中1110;以及沉積層間介電層1120;以及沉積第一金屬層於沉積層間介電層上1130。製造LDMOS裝置1000的方法更包括,例如,形成IMD層及/或第二金屬層。 The method for manufacturing the LDMOS device 1000 further includes: forming an N + doped region in the second P well and HVNW 1100; forming a P + doped region in the first P well and the second P well 1110; and depositing the interlayer dielectric layer 1120; And depositing a first metal layer on the inter-layer dielectric layer 1130. The method of fabricating the LDMOS device 1000 further includes, for example, forming an IMD layer and/or a second metal layer.

本發明的一個面向係將本發明用於由形成半導體閘極結構的製程或方法所形成的半導體結構之中,在某些實施例中,MOS裝置可以使用本發明所描述的任何方法形成。在進一步的實施例中,LDMOS裝置可以使用本發明所描述的任何方法形成。 One aspect of the present invention is directed to the use of the present invention in a semiconductor structure formed by a process or method of forming a semiconductor gate structure. In some embodiments, the MOS device can be formed using any of the methods described herein. In a further embodiment, the LDMOS device can be formed using any of the methods described herein.

在此所提出的多個有關本發明之變型與其它實施例,將會促使本發明所屬領域技藝者,想到有關於前述描述及其相關圖式所呈現的益處,因此,本發明並不受限於所揭露之特定實施例與變型,其它實施例亦擬被包括在所附請求項之保護範圍內,再者,雖然前述描述及其相關圖式在元件及/或功能之某些示範性組合的上下文中描述了實施例,但是元件及/或功能之不同組合可在不違背所附請求項之範圍的替代實施例的狀況下而提供,就此而言,除前述明白地描述以外的元件及/或功能之不同組合,也被預期可以在某些所附請求項中提出;在本揭露中所使用的某些特定用語,它們只使用在上位與描述性概念且不為了限制之目的。 The various modifications and other embodiments of the present invention described herein will be apparent to those skilled in the art of the present invention. Other embodiments are also intended to be included within the scope of the appended claims, and the foregoing description and related drawings are in some exemplary combinations of elements and/or functions. Embodiments are described in the context of the present invention, but different combinations of elements and/or functions may be provided without departing from the scope of the alternative embodiments of the appended claims. Different combinations of functions are also contemplated as being set forth in certain appended claims; certain specific terms used in the present disclosure are only used in the generic and descriptive concepts and not for the purpose of limitation.

240‧‧‧分離的N能階及分離的P頂區 240‧‧‧Separated N-level and separated P-top

255‧‧‧N能階區 255‧‧‧N energy level zone

245‧‧‧分離的P頂區段 245‧‧‧Separated P-top section

260‧‧‧P基板 260‧‧‧P substrate

270‧‧‧HVNW 270‧‧‧HVNW

280‧‧‧第一P井 280‧‧‧First P well

290‧‧‧第二P井 290‧‧‧Second P well

300‧‧‧P+摻雜區 300‧‧‧P + doped area

310‧‧‧P+摻雜區 310‧‧‧P + doped area

320‧‧‧N+摻雜源極區 320‧‧‧N + doped source region

330‧‧‧N+摻雜汲極區 330‧‧‧N + doped bungee zone

340‧‧‧場氧化隔離區 340‧‧‧Field Oxidation Isolation Area

350‧‧‧控制閘極結構 350‧‧‧Control gate structure

345‧‧‧閘極氧化層 345‧‧ ‧ gate oxide layer

355‧‧‧間隙壁 355‧‧‧ spacer

360‧‧‧層間介電(ILD)層 360‧‧‧Interlayer dielectric (ILD) layer

370‧‧‧第一金屬層 370‧‧‧First metal layer

365‧‧‧第一核心區 365‧‧‧First core area

375‧‧‧絕緣區 375‧‧‧Insulated area

380‧‧‧內金屬介電(IMD)層 380‧‧•Metal dielectric (IMD) layer

390‧‧‧第二金屬層 390‧‧‧Second metal layer

400‧‧‧介電層 400‧‧‧ dielectric layer

Claims (21)

一種半導體,包括:一P基板;一高電壓N井(HVNW),其設置於該P基板中;一第一P井,其形成於具有一第一P+摻雜區的該P基板中;一第二P井,其形成於具有一第二P+摻雜區的該HVNW中,其中該第二P+摻雜區鄰近於一N+摻雜源極區;以及一分離的N能階及P頂區,其設置於該HVNW中,其中該分離的N能階及P頂區具有由複數個N能階區段與複數個P頂區段交替排列所定義之一層或交叉排列所定義之多層。 A semiconductor comprising: a P substrate; a high voltage N well (HVNW) disposed in the P substrate; a first P well formed in the P substrate having a first P + doped region; a second P well formed in the HVNW having a second P + doped region, wherein the second P + doped region is adjacent to an N + doped source region; and a separate N energy level And a P top region disposed in the HVNW, wherein the separated N energy level and P top region have a layer or a cross arrangement defined by a plurality of N energy level segments and a plurality of P top segments alternately arranged Multiple layers. 如申請專利範圍第1項所述的半導體,其中該分離的N能階及P頂區包括二或多層以及該複數個P頂區段及複數個N能階區段在一崩潰交叉調整中。 The semiconductor of claim 1, wherein the separated N and P top regions comprise two or more layers and the plurality of P top segments and the plurality of N energy segments are in a collapse cross adjustment. 如申請專利範圍第1項所述的半導體,其中該半導體為一橫向擴散金屬氧化物半導體(LDMOS)以及該HVNW具有一N+摻雜汲極區。 The semiconductor of claim 1, wherein the semiconductor is a laterally diffused metal oxide semiconductor (LDMOS) and the HVNW has an N + doped drain region. 如申請專利範圍第3項所述的半導體,其中在該HVNW的該複數個P頂區段中每一區段具有一深度以定義複數個深度、一寬度以定義複數個寬度以及一間隔距離以定義複數個間隔距離。 The semiconductor of claim 3, wherein each of the plurality of P top sections of the HVNW has a depth to define a plurality of depths, a width to define a plurality of widths, and a separation distance to Define a number of separation distances. 如申請專利範圍第4項所述的半導體,其中該複數個深度中每一個深度係相同。 The semiconductor of claim 4, wherein each of the plurality of depths is the same depth. 如申請專利範圍第4項所述的半導體,其中該複數個深度的深度係遞增。 The semiconductor of claim 4, wherein the depth of the plurality of depths is increasing. 如申請專利範圍第4項所述的半導體,相較於其他有一連續P 頂區設置於一連續N能階區下的LDMOS裝置,其中該複數個深度、複數個寬度以及複數個間隔距離,其在一汲極電壓的一導通電阻中至少減少11.6%,約1伏特。 The semiconductor described in claim 4, having a continuous P compared to the other The top region is disposed in an LDMOS device under a continuous N energy level region, wherein the plurality of depths, the plurality of widths, and the plurality of spacer distances are reduced by at least 11.6%, about 1 volt, in an on-resistance of a drain voltage. 如申請專利範圍第7項所述的半導體,其中該LDMOS裝置的一崩潰電壓與該其他LDMOS裝置的一崩潰電壓相同。 The semiconductor of claim 7, wherein a breakdown voltage of the LDMOS device is the same as a breakdown voltage of the other LDMOS device. 如申請專利範圍第3項所述的半導體,其中在該HVNW中的該複數個N能階區段具有一深度以定義複數個深度、一寬度以定義複數個寬度以及選自垂直鄰近P頂區段的一間隔距離以定義複數個間隔距離。 The semiconductor of claim 3, wherein the plurality of N energy level segments in the HVNW have a depth to define a plurality of depths, a width to define a plurality of widths, and a vertical adjacent P top region A spacing distance of the segments to define a plurality of spacing distances. 如申請專利範圍第9項所述的半導體,相較於其他有一連續P頂區設置於一連續N能階區下的LDMOS裝置,其中該複數個深度、複數個寬度以及複數個間隔距離,其在一汲極電壓的一導通電阻中至少減少11.6%,約1伏特。 The semiconductor of claim 9, wherein the plurality of LDMOS devices having a continuous P top region are disposed under a continuous N energy level region, wherein the plurality of depths, a plurality of widths, and a plurality of spaced distances are At least 11.6%, approximately 1 volt, is reduced in an on-resistance of a drain voltage. 如申請專利範圍第3項所述的半導體,更包括一場氧化隔離區設置於使一第一P+摻雜區與一第二P+摻雜區隔離,其中該第二P+摻雜區鄰近於該N+摻雜源極區以及該N+摻雜汲極區。 The semiconductor of claim 3, further comprising an oxidation isolation region disposed to isolate a first P + doped region from a second P + doped region, wherein the second P + doped region is adjacent to And the N + doped source region and the N + doped drain region. 如申請專利範圍第11項所述的半導體,更包括一閘極結構設置於該N+摻雜源區域與該N+摻雜汲極區之間。 The semiconductor of claim 11, further comprising a gate structure disposed between the N + doped source region and the N + doped drain region. 如申請專利範圍第1項所述的半導體,其中該半導體為一絕緣閘極雙極電晶體以及該HVNW具有一第三P+摻雜區。 The semiconductor of claim 1, wherein the semiconductor is an insulated gate bipolar transistor and the HVNW has a third P + doped region. 如申請專利範圍第1項所述的半導體,其中該半導體為一二極體以及該HVNW具有一N+摻雜汲極區。 The semiconductor of claim 1, wherein the semiconductor is a diode and the HVNW has an N + doped drain region. 一種製造一半導體的方法,包括:提供一P基板層; 於該P基板層中形成一高電壓N井(HVNW);於該P基板中形成一第一P井;於該HVNW中形成一第二P井;以及於該HVNW中形成一分離的N能階及P頂區,其中該分離的N能階及P頂區具有由複數個N能階區段與複數個P頂區段交替排列所定義之一層或交叉排列所定義之多層。 A method of fabricating a semiconductor, comprising: providing a P substrate layer; Forming a high voltage N well (HVNW) in the P substrate layer; forming a first P well in the P substrate; forming a second P well in the HVNW; and forming a separate N energy in the HVNW And a P top region, wherein the separated N energy level and P top region have a plurality of layers defined by a layer or a cross arrangement defined by a plurality of N energy level segments and a plurality of P top segments alternately arranged. 如申請專利範圍第15項所述的方法,更包括形成一場氧化隔離區,其中該場氧化隔離區由一第一場結構重疊於該第一P型井及該第二P型井以及一第二場氧化結構重疊於該N能階區所定義。 The method of claim 15, further comprising forming an oxidation isolation region, wherein the field oxidation isolation region is overlapped by the first P-well and the second P-well and a first The two field oxidation structure is overlapped by the N energy level region. 如申請專利範圍第16項所述的方法,更包括形成一閘極結構。 The method of claim 16, further comprising forming a gate structure. 如申請專利範圍第17項所述的方法,其中該形成一閘極結構的步驟包括:實施一閘極氧化方法;形成一多晶矽層;以及形成圍繞於該閘極結構的一間隙壁。 The method of claim 17, wherein the step of forming a gate structure comprises: performing a gate oxidation method; forming a polysilicon layer; and forming a spacer surrounding the gate structure. 如申請專利範圍第17項所述的方法,更包括於該第二P型井中形成鄰近於該閘極結構的一N+摻雜源極區;於該第一P型井中形成一第一P+摻雜區;於該第二P型井中形成一第二P+摻雜區;以及於該HVNW中形成鄰近於該第二場氧化結構的一摻雜區。 The method of claim 17, further comprising forming an N + doped source region adjacent to the gate structure in the second P-type well; forming a first P in the first P-type well a doped region; a second P + doped region is formed in the second P-type well; and a doped region adjacent to the second field oxide structure is formed in the HVNW. 如申請專利範圍第19項所述的方法,其中該半導體為一橫向擴散金屬氧化物半導體以及該摻雜區為一N+摻雜汲極區。 The method of claim 19, wherein the semiconductor is a laterally diffused metal oxide semiconductor and the doped region is an N + doped drain region. 如申請專利範圍第19項所述的方法,其中該半導體為一絕緣閘極雙極電晶體以及該該摻雜區為一第三P+摻雜區。 The method of claim 19, wherein the semiconductor is an insulated gate bipolar transistor and the doped region is a third P + doped region.
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