TWI815280B - Transistor structure - Google Patents
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- TWI815280B TWI815280B TW111102343A TW111102343A TWI815280B TW I815280 B TWI815280 B TW I815280B TW 111102343 A TW111102343 A TW 111102343A TW 111102343 A TW111102343 A TW 111102343A TW I815280 B TWI815280 B TW I815280B
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/60—Insulated-gate field-effect transistors [IGFET]
- H10D30/64—Double-diffused metal-oxide semiconductor [DMOS] FETs
- H10D30/65—Lateral DMOS [LDMOS] FETs
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/20—Electrodes characterised by their shapes, relative sizes or dispositions
- H10D64/27—Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
- H10D64/311—Gate electrodes for field-effect devices
- H10D64/411—Gate electrodes for field-effect devices for FETs
- H10D64/511—Gate electrodes for field-effect devices for FETs for IGFETs
- H10D64/517—Gate electrodes for field-effect devices for FETs for IGFETs characterised by the conducting layers
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/20—Electrodes characterised by their shapes, relative sizes or dispositions
- H10D64/27—Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
- H10D64/311—Gate electrodes for field-effect devices
- H10D64/411—Gate electrodes for field-effect devices for FETs
- H10D64/511—Gate electrodes for field-effect devices for FETs for IGFETs
- H10D64/517—Gate electrodes for field-effect devices for FETs for IGFETs characterised by the conducting layers
- H10D64/519—Gate electrodes for field-effect devices for FETs for IGFETs characterised by the conducting layers characterised by their top-view geometrical layouts
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Abstract
Description
本發明是有關於一種半導體結構,且特別是有關於一種電晶體結構。 The present invention relates to a semiconductor structure, and in particular to a transistor structure.
電晶體元件的品質因數(figure of merit,FOM)是由導通電阻(Ron)與閘極/汲極充電電荷量(Qgd)的乘積所決定。此外,閘極/汲極充電電荷量是由閘極與汲極之間的米勒電容(miller capacitance)(如,邊緣電容(fringe capacitance))所決定。目前,為了提高電晶體元件的能量轉換效率並抑制功率損耗,必須降低電晶體元件的品質因數。因此,如何有效地降低電晶體元件的品質因數為目前持續努力的目標。 The figure of merit (FOM) of a transistor element is determined by the product of the on-resistance (R on ) and the gate/drain charge (Q gd ). In addition, the amount of gate/drain charge is determined by the miller capacitance (eg, fringe capacitance) between the gate and drain. Currently, in order to improve the energy conversion efficiency of transistor elements and suppress power loss, it is necessary to reduce the quality factor of transistor elements. Therefore, how to effectively reduce the quality factor of transistor elements is the current goal of continuous efforts.
本發明提供一種電晶體結構,其可有效地降低電晶體元件的品質因數。 The present invention provides a transistor structure that can effectively reduce the quality factor of the transistor element.
本發明提出一種電晶體結構,包括基底、隔離結構、第一閘極、第二閘極、介電間隙壁與導電間隙壁。隔離結構設置在 基底中。第一閘極設置在基底上。第一閘極與基底彼此電性隔離。第二閘極設置在隔離結構上。第一閘極與第二閘極彼此分離且彼此電性隔離。介電間隙壁圍繞第一閘極的側壁與第二閘極的側壁。導電間隙壁設置在介電間隙壁上,且圍繞第一閘極的側壁與第二閘極的側壁。第二閘極與導電間隙壁彼此電性連接。 The invention proposes a transistor structure, which includes a substrate, an isolation structure, a first gate, a second gate, a dielectric spacer and a conductive spacer. The isolation structure is set at in the base. The first gate is disposed on the substrate. The first gate and the substrate are electrically isolated from each other. The second gate is disposed on the isolation structure. The first gate and the second gate are separated from each other and electrically isolated from each other. The dielectric spacer surrounds the sidewalls of the first gate and the sidewalls of the second gate. The conductive spacer is disposed on the dielectric spacer and surrounds the sidewall of the first gate and the sidewall of the second gate. The second gate electrode and the conductive gap wall are electrically connected to each other.
依照本發明的一實施例所述,在上述電晶體結構中,第二閘極不位在任何主動區上。 According to an embodiment of the invention, in the above transistor structure, the second gate is not located on any active region.
依照本發明的一實施例所述,在上述電晶體結構中,第一閘極與第二閘極可在第一閘極的閘極寬度方向上排列。 According to an embodiment of the invention, in the above transistor structure, the first gate and the second gate may be arranged in the gate width direction of the first gate.
依照本發明的一實施例所述,在上述電晶體結構中,部分介電間隙壁可位在第一閘極與第二閘極之間。部分導電間隙壁可位在第一閘極與第二閘極之間。 According to an embodiment of the present invention, in the above transistor structure, part of the dielectric spacer may be located between the first gate and the second gate. A portion of the conductive spacer may be located between the first gate and the second gate.
依照本發明的一實施例所述,在上述電晶體結構中,導電間隙壁與第一閘極可電性連接至不同的電壓源。 According to an embodiment of the invention, in the above transistor structure, the conductive spacer and the first gate are electrically connected to different voltage sources.
依照本發明的一實施例所述,在上述電晶體結構中,更可包括共用接觸窗(share contact)。共用接觸窗電性連接至第二閘極與導電間隙壁。 According to an embodiment of the present invention, the above-mentioned transistor structure may further include a shared contact. The common contact window is electrically connected to the second gate and the conductive gap wall.
依照本發明的一實施例所述,在上述電晶體結構中,更可包括第三閘極。第三閘極設置在隔離結構上。第二閘極位在第一閘極與第三閘極之間。第一閘極與第三閘極彼此分離且彼此電性隔離。介電間隙壁與導電間隙壁分別圍繞第三閘極的側壁。第二閘極、第三閘極與導電間隙壁彼此電性連接。 According to an embodiment of the present invention, the above transistor structure may further include a third gate. The third gate is arranged on the isolation structure. The second gate is located between the first gate and the third gate. The first gate and the third gate are separated from each other and electrically isolated from each other. The dielectric spacer and the conductive spacer respectively surround the sidewalls of the third gate. The second gate electrode, the third gate electrode and the conductive gap wall are electrically connected to each other.
依照本發明的一實施例所述,在上述電晶體結構中,部分介電間隙壁可位在第一閘極與第二閘極之間以及第二閘極與第三閘極之間。部分導電間隙壁可位在第一閘極與第二閘極之間以及第二閘極與第三閘極之間。 According to an embodiment of the present invention, in the above transistor structure, part of the dielectric spacer may be located between the first gate and the second gate and between the second gate and the third gate. A portion of the conductive spacer may be located between the first gate and the second gate and between the second gate and the third gate.
依照本發明的一實施例所述,在上述電晶體結構中,可包括彼此分離的多個第一閘極與彼此分離的多個第二閘極。第三閘極可位在多個第二閘極的同一側。 According to an embodiment of the present invention, the transistor structure may include a plurality of first gates separated from each other and a plurality of second gates separated from each other. The third gate can be located on the same side of the plurality of second gates.
依照本發明的一實施例所述,在上述電晶體結構中,可包括彼此分離的多個第一閘極。第二閘極可位在多個第一閘極的同一側。 According to an embodiment of the present invention, the above transistor structure may include a plurality of first gates separated from each other. The second gate can be located on the same side of the plurality of first gates.
基於上述,在本發明所提出的電晶體結構中,第一閘極與第二閘極彼此電性隔離,導電間隙壁圍繞第一閘極的側壁與第二閘極的側壁,且第二閘極與導電間隙壁彼此電性連接。因此,可藉由對導電間隙壁施加電壓(如,接地電壓)來抑制邊緣電容,藉此可降低整體米勒電容。如此一來,可有效地降低電晶體元件的品質因數,進而提高電晶體元件的能量轉換效率並抑制功率損耗。 Based on the above, in the transistor structure proposed by the present invention, the first gate and the second gate are electrically isolated from each other, the conductive gap wall surrounds the side walls of the first gate and the second gate, and the second gate The pole and the conductive gap wall are electrically connected to each other. Therefore, the fringing capacitance can be suppressed by applying a voltage (eg, ground voltage) to the conductive spacer wall, thereby reducing the overall Miller capacitance. In this way, the quality factor of the transistor element can be effectively reduced, thereby improving the energy conversion efficiency of the transistor element and suppressing power loss.
為讓本發明的上述特徵和優點能更明顯易懂,下文特舉實施例,並配合所附圖式作詳細說明如下。 In order to make the above-mentioned features and advantages of the present invention more obvious and easy to understand, embodiments are given below and described in detail with reference to the accompanying drawings.
10,20,30,40:電晶體結構 10,20,30,40:Transistor structure
100:基底 100:Base
102:隔離結構 102:Isolation structure
104,106:閘極 104,106: Gate
108:介電間隙壁 108: Dielectric spacer
110:導電間隙壁 110: Conductive gap wall
112,114:摻雜區 112,114: Doped area
116:井區 116:Well area
118:深井區 118:Sham Tseng District
120:閘介電層 120: Gate dielectric layer
122:共用接觸窗 122: Shared contact window
124:接觸窗 124:Contact window
126:介電層 126:Dielectric layer
AA:主動區 AA: active area
D1:閘極寬度方向 D1: Gate width direction
D2:通道長度方向 D2: channel length direction
R:凹槽 R: Groove
圖1A為根據本發明的一些實施例電晶體結構的上視圖。 Figure 1A is a top view of a transistor structure according to some embodiments of the present invention.
圖1B為沿著圖1A中的I-I’剖面線的剖面圖。 Fig. 1B is a cross-sectional view along the line I-I' in Fig. 1A.
圖1C為沿著圖1A中的II-II’剖面線的剖面圖。 Figure 1C is a cross-sectional view along the II-II' section line in Figure 1A.
圖2為根據本發明的另一些實施例電晶體結構的上視圖。 FIG. 2 is a top view of a transistor structure according to other embodiments of the present invention.
圖3為根據本發明的另一些實施例電晶體結構的上視圖。 FIG. 3 is a top view of a transistor structure according to other embodiments of the present invention.
圖4為根據本發明的另一些實施例電晶體結構的上視圖。 FIG. 4 is a top view of a transistor structure according to other embodiments of the present invention.
下文列舉實施例並配合附圖來進行詳細地說明,但所提供的實施例並非用以限制本發明所涵蓋的範圍。為了方便理解,在下述說明中相同的構件將以相同的符號標示來說明。此外,附圖僅以說明為目的,並未依照原尺寸作圖。另外,上視圖中的特徵與剖面圖中的特徵並非按相同比例繪製。事實上,為論述清晰起見,可任意增大或減小各種特徵的尺寸。 Examples are listed below and described in detail with reference to the drawings. However, the provided examples are not intended to limit the scope of the present invention. To facilitate understanding, the same components will be identified with the same symbols in the following description. In addition, the drawings are for illustrative purposes only and are not drawn to original size. Also, the features in the upper view are not drawn to the same scale as those in the section view. In fact, the dimensions of the various features may be arbitrarily increased or reduced for clarity of discussion.
圖1A為根據本發明的一些實施例電晶體結構的上視圖。圖1B為沿著圖1A中的I-I’剖面線的剖面圖。圖1C為沿著圖1A中的II-II’剖面線的剖面圖。 Figure 1A is a top view of a transistor structure according to some embodiments of the present invention. Fig. 1B is a cross-sectional view along the line I-I' in Fig. 1A. Figure 1C is a cross-sectional view along the II-II' section line in Figure 1A.
請參照圖1A至圖1C,電晶體結構10包括基底100、隔離結構102、閘極104、閘極106、介電間隙壁108與導電間隙壁110。在一些實施例中,電晶體結構10可為功率金屬氧化物半導體電晶體(power metal oxide semiconductor(MOS)transistor),如橫向擴散金屬氧化物半導體電晶體(lateral diffused metal oxide semiconductor(LDMOS)transistor)。基底100可為半導體基底,
如矽基底。隔離結構102設置在基底100中。隔離結構102可在基底100中定義出主動區AA。隔離結構102例如是淺溝渠隔離結構(shallow trench isolation,STI)。隔離結構102的材料可為例如是氧化矽、氮化矽或其組合。
Referring to FIGS. 1A to 1C , the
此外,電晶體結構10更可包括摻雜區112、摻雜區114、井區116與深井區118中的至少一者。摻雜區112與摻雜區114位在閘極104的兩側的基底100中。摻雜區112與摻雜區114分別可作為源極區與汲極區中的一者與另一者。此外,摻雜區112與摻雜區114可位在主動區AA中。摻雜區112與摻雜區114可具有第一導電型(如,N型)。以下,第一導電型與第二導電型可分別為N型導電型與P型導電型中的一者與另一者。在本實施例中,第一導電型是以N型導電型為例,且第二導電型是以P型導電型為例,但本發明並不以此為限。在另一些實施例中,第一導電型可為P型導電型,且第二導電型可為N型導電型。
In addition, the
井區116位在基底100中。井區116可具有第二導電型(如,P型)。摻雜區112與摻雜區114可位在井區116中。深井區118位在基底100中。深井區118可具有第一導電型(如,N型)。井區116可位在深井區118中。
Well
閘極104設置在基底100上。在一些實施例中,部分閘極104可位在主動區AA上,且部分閘極104可位在隔離結構102上。閘極104的材料例如是摻雜多晶矽。閘極104與基底100彼此電性隔離。舉例來說,電晶體結構10更可包括閘介電層120。
閘介電層120位在閘極104與基底100之間,藉此閘極104與基底100可彼此電性隔離。閘介電層120的材料例如是氧化矽。
The
閘極106設置在隔離結構102上。閘極104與閘極106彼此分離且彼此電性隔離。閘極104與閘極106可在閘極104的閘極寬度方向D1上排列。在一些實施例中,閘極寬度方向D1可垂直於通道長度方向D2。在本實施例中,將「通道長度方向」定義為延伸通過摻雜區112與摻雜區114的方向。在一些實施例中,閘極106不位在任何主動區上。閘極106的材料例如是摻雜多晶矽。
介電間隙壁108圍繞閘極104的側壁與閘極106的側壁。在一些實施例中,介電間隙壁108可為圍繞閘極104的側壁與閘極106的側壁的連續結構。在一些實施例中,部分介電間隙壁108可位在閘極104與閘極106之間。在一些實施例中,介電間隙壁108可設置在閘極104的側壁、閘極106的側壁、隔離結構102與閘介電層120上。介電間隙壁108的材料例如是氮化矽。
導電間隙壁110設置在介電間隙壁108上,且圍繞閘極104的側壁與閘極106的側壁。在一些實施例中,導電間隙壁110可為圍繞閘極104的側壁與閘極106的側壁的連續結構。導電間隙壁110可位在介電間隙壁108的凹槽R中。在一些實施例中,部分導電間隙壁110可位在閘極104與閘極106之間。導電間隙壁110的材料例如是摻雜多晶矽。
The
閘極106與導電間隙壁110彼此電性連接。舉例來說,
電晶體結構10更可包括共用接觸窗122。共用接觸窗122電性連接至閘極106與導電間隙壁110,藉此閘極106與導電間隙壁110可彼此電性連接。此外,共用接觸窗122的設置位置並不限於圖中的位置,且共用接觸窗122的數量並不限於圖中的數量。只要共用接觸窗122的設置位置與數量可使得共用接觸窗122電性連接至閘極106與導電間隙壁110,即屬於本發明所涵蓋的範圍。共用接觸窗122的材料例如是鎢。
The
電晶體結構10更可包括接觸窗124與介電層126中的至少一者。接觸窗124電性連接至閘極104。共用接觸窗122與接觸窗124可電性連接至不同的電壓源,藉此導電間隙壁110與閘極104可電性連接至不同的電壓源。接觸窗124的材料例如是鎢。介電層126可覆蓋基底100、隔離結構102、閘極104、閘極106、介電間隙壁108與導電間隙壁110。共用接觸窗122與接觸窗124可位在介電層126中。介電層126的材料例如是氧化矽。
The
基於上述實施例可知,在電晶體結構10中,閘極104與閘極106彼此電性隔離,導電間隙壁110圍繞閘極104的側壁與閘極106的側壁,且閘極106與導電間隙壁110彼此電性連接。因此,可藉由對導電間隙壁110施加電壓(如,接地電壓)來抑制邊緣電容,藉此可降低整體米勒電容。如此一來,可有效地降低電晶體元件的品質因數,進而提高電晶體元件的能量轉換效率並抑制功率損耗。
Based on the above embodiments, it can be seen that in the
圖2為根據本發明的另一些實施例電晶體結構的上視圖。 FIG. 2 is a top view of a transistor structure according to other embodiments of the present invention.
請參照圖1A與圖2,圖2的電晶體結構20與圖1A的電晶體結構10的差異如下。如圖2所示,電晶體結構20更可包括閘極202。閘極202設置在隔離結構102上。閘極106位在閘極104與閘極202之間。閘極104與閘極202彼此分離且彼此電性隔離。閘極104、閘極106與閘極202可在閘極104的閘極寬度方向D1上排列。在一些實施例中,閘極202不位在任何主動區上。閘極202的材料例如是摻雜多晶矽。
Please refer to FIG. 1A and FIG. 2 . The differences between the
介電間隙壁108與導電間隙壁110分別圍繞閘極202的側壁。在一些實施例中,介電間隙壁108與導電間隙壁110可分別為圍繞閘極104的側壁、閘極106的側壁與閘極202的側壁的連續結構。部分介電間隙壁108可位在閘極104與閘極106之間以及閘極106與閘極202之間。部分導電間隙壁110可位在閘極104與閘極106之間以及閘極106與閘極202之間。閘極106、閘極202與導電間隙壁110彼此電性連接。舉例來說,閘極106、閘極202與導電間隙壁110可藉由共用接觸窗122而彼此電性連接。在本實施例中,共用接觸窗122可設置在閘極106與閘極202之間,但共用接觸窗122的設置位置並不限於圖中的位置。只要共用接觸窗122的設置位置可使得共用接觸窗122電性連接至閘極106、閘極202與導電間隙壁110,即屬於本發明所涵蓋的範圍。
The
此外,電晶體結構20與電晶體結構10中相同的構件使用相同的符號表示,且電晶體結構20與電晶體結構10中相同或相似的內容,可參考上述實施例對電晶體結構10的說明,於此不
再說明。
In addition, the same components in the
圖3為根據本發明的另一些實施例電晶體結構的上視圖。 FIG. 3 is a top view of a transistor structure according to other embodiments of the present invention.
請參照圖1A與圖3,圖3的電晶體結構30與圖1A的電晶體結構10的差異如下。如圖3所示,電晶體結構30可包括彼此分離的多個閘極104。多個閘極104可分別位在對應的主動區AA上。閘極106可位在多個閘極104的同一側。此外,閘極104的數量並不限於圖中的數量。只要閘極104的數量為多個,即屬於本發明所涵蓋的範圍。
Please refer to FIG. 1A and FIG. 3 . The differences between the
另外,電晶體結構30與電晶體結構10中相同的構件使用相同的符號表示,且電晶體結構30與電晶體結構10中相同或相似的內容,可參考上述實施例對電晶體結構10的說明,於此不再說明。
In addition, the same components in the
圖4為根據本發明的另一些實施例電晶體結構的上視圖。 FIG. 4 is a top view of a transistor structure according to other embodiments of the present invention.
請參照圖2與圖4,圖4的電晶體結構40與圖2的電晶體結構20的差異如下。如圖4所示,電晶體結構40可包括彼此分離的多個閘極104與彼此分離的多個閘極106。多個閘極104可分別位在對應的主動區AA上。閘極202可位在多個閘極106的同一側。此外,電晶體結構40可包括多個共用接觸窗122。多個共用接觸窗122分別電性連接至閘極202、導電間隙壁110與對應的閘極106。此外,閘極104的數量、閘極106的數量與共用接觸窗122的數量並不限於圖中的數量。只要閘極104的數量、閘極106的數量與共用接觸窗122的數量分別為多個,即屬於本發
明所涵蓋的範圍。
Please refer to FIGS. 2 and 4 . The differences between the
另外,電晶體結構40與電晶體結構20中相同的構件使用相同的符號表示,且電晶體結構40與電晶體結構20中相同或相似的內容,可參考上述實施例對電晶體結構20的說明,於此不再說明。
In addition, the same components in the
綜上所述,在上述實施例的電晶體結構中,可藉由對導電間隙壁施加電壓(如,接地電壓)來抑制邊緣電容,藉此可降低整體米勒電容。如此一來,可有效地降低電晶體元件的品質因數,進而提高電晶體元件的能量轉換效率並抑制功率損耗。 In summary, in the transistor structure of the above embodiments, the fringe capacitance can be suppressed by applying a voltage (eg, ground voltage) to the conductive spacer wall, thereby reducing the overall Miller capacitance. In this way, the quality factor of the transistor element can be effectively reduced, thereby improving the energy conversion efficiency of the transistor element and suppressing power loss.
雖然本發明已以實施例揭露如上,然其並非用以限定本發明,任何所屬技術領域中具有通常知識者,在不脫離本發明的精神和範圍內,當可作些許的更動與潤飾,故本發明的保護範圍當視後附的申請專利範圍所界定者為準。 Although the present invention has been disclosed above through embodiments, they are not intended to limit the present invention. Anyone with ordinary knowledge in the technical field may make some modifications and modifications without departing from the spirit and scope of the present invention. Therefore, The protection scope of the present invention shall be determined by the appended patent application scope.
10: 電晶體結構
102: 隔離結構
104, 106: 閘極
108: 介電間隙壁
110: 導電間隙壁
112, 114: 摻雜區
122: 共用接觸窗
124: 接觸窗
AA: 主動區
D1: 閘極寬度方向
D2: 通道長度方向
10: Transistor structure
102:
Claims (10)
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| TW111102343A TWI815280B (en) | 2022-01-20 | 2022-01-20 | Transistor structure |
| CN202210115713.7A CN116525673A (en) | 2022-01-20 | 2022-02-07 | Transistor structure |
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Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TW466690B (en) * | 1999-12-15 | 2001-12-01 | United Microelectronics Corp | Manufacturing method of self-aligned contact hole |
| US20080102612A1 (en) * | 2006-10-25 | 2008-05-01 | International Business Machines Corporation | Silicided polysilicon spacer for enhanced contact area |
| US20170194491A1 (en) * | 2015-12-31 | 2017-07-06 | Globalfoundries Singapore Pte. Ltd. | High voltage device with low rdson |
| US20170330947A1 (en) * | 2015-10-14 | 2017-11-16 | United Microelectronics Corp. | Metal-oxide-semiconductor transistor and method of forming gate layout |
| US20210234042A1 (en) * | 2020-01-28 | 2021-07-29 | Shuming Xu | Metal-oxide semiconductor for field-effect transistor having enhanced high-frequency performance |
-
2022
- 2022-01-20 TW TW111102343A patent/TWI815280B/en active
- 2022-02-07 CN CN202210115713.7A patent/CN116525673A/en active Pending
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TW466690B (en) * | 1999-12-15 | 2001-12-01 | United Microelectronics Corp | Manufacturing method of self-aligned contact hole |
| US20080102612A1 (en) * | 2006-10-25 | 2008-05-01 | International Business Machines Corporation | Silicided polysilicon spacer for enhanced contact area |
| US20170330947A1 (en) * | 2015-10-14 | 2017-11-16 | United Microelectronics Corp. | Metal-oxide-semiconductor transistor and method of forming gate layout |
| US20170194491A1 (en) * | 2015-12-31 | 2017-07-06 | Globalfoundries Singapore Pte. Ltd. | High voltage device with low rdson |
| US20210234042A1 (en) * | 2020-01-28 | 2021-07-29 | Shuming Xu | Metal-oxide semiconductor for field-effect transistor having enhanced high-frequency performance |
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| TW202331850A (en) | 2023-08-01 |
| CN116525673A (en) | 2023-08-01 |
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