TWI529931B - Semiconductor device and method for fabricating the same - Google Patents
Semiconductor device and method for fabricating the same Download PDFInfo
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Description
本發明係有關於一種半導體裝置,特別係有關於一種具有高電壓場效電晶體與低接通電阻的半導體裝置及其製造方法。 The present invention relates to a semiconductor device, and more particularly to a semiconductor device having a high voltage field effect transistor and a low on resistance and a method of fabricating the same.
雙極-互補式金屬氧化物半導體-射頻橫向擴散金氧半場效電晶體(Bipolar-CMOS-LDMOS,BCD)廣泛地運用於電源管理積體電路(power management integrated circuit,PMIC)應用中。BCD技術係將雙極裝置、互補式金屬氧化物半導體(CMOS)與射頻橫向擴散金氧半場效電晶體(laterally diffused metal-oxide semiconductor,LDMOS)整合於單一晶片中。在一個BCD裝置中,雙極裝置係用來驅動高電流,CMOS可使降低數位電路的能耗(power consumption),而LDMOS具有高電壓處理能力。 Bipolar-complementary metal-oxide-semiconductor-transistor-emitting diodes (Bipolar-CMOS-LDMOS, BCD) are widely used in power management integrated circuit (PMIC) applications. The BCD technology integrates a bipolar device, a complementary metal oxide semiconductor (CMOS), and a laterally diffused metal-oxide semiconductor (LDMOS) into a single wafer. In a BCD device, the bipolar device is used to drive high current, the CMOS can reduce the power consumption of the digital circuit, and the LDMOS has high voltage processing capability.
LDMOS裝置廣泛地運用於日常應用中。而接通電阻是LDMOS裝置之能耗的一個重要因子,LDMOS裝置的接通電阻與能耗成正比。隨著省電與高效能的電子裝置之需求日益增加,製造商不斷地尋求降低LDMOS裝置的接通電阻與漏電的方法。然而,降低接通電阻與斷態崩潰電壓(off-state breakdown voltage)息息相關。具體而言,降低接通電阻會使斷 態崩潰電壓大幅地降低。因此,傳統的LDMOS裝置可傳遞高斷態崩潰電壓,卻不能使接通電阻降低。 LDMOS devices are widely used in everyday applications. The on-resistance is an important factor in the energy consumption of the LDMOS device, and the on-resistance of the LDMOS device is proportional to the energy consumption. As the demand for power-saving and high-performance electronic devices increases, manufacturers are continually seeking ways to reduce the on-resistance and leakage of LDMOS devices. However, reducing the on-resistance is closely related to the off-state breakdown voltage. Specifically, lowering the on-resistance will break The state collapse voltage is greatly reduced. Therefore, the conventional LDMOS device can transmit a high off-state breakdown voltage, but cannot lower the on-resistance.
LDMOS裝置包括漂移(drift)區與主體(body)區。經實驗發現,當漂移區的摻雜濃度提高,可使LDMOS裝置的接通電阻降低。然而,LDMOS裝置的斷態崩潰電壓亦隨著漂移區的摻雜濃度提高而降低。 The LDMOS device includes a drift region and a body region. It has been found through experiments that when the doping concentration of the drift region is increased, the on-resistance of the LDMOS device can be lowered. However, the off-state breakdown voltage of the LDMOS device also decreases as the doping concentration of the drift region increases.
因此,業界仍需一種改良的半導體裝置及其製造方法。 Therefore, there is still a need in the industry for an improved semiconductor device and method of fabricating the same.
本發明一實施例提供一種半導體裝置,包括:一基底,具有一第一導電型態,其包括:一主體區,具有第一導電型態;一源極區域,形成於主體區中;一漂移區,具有一第二導電型態;以及一汲極區域型,形成於漂移區中;一多重(multiple)表面電場降低(reduced surface field,RESURF)結構,埋植於基底之漂移區中;以及一閘介電層,形成於基底之上其中第一導電型態相反於第二導電型態。 An embodiment of the invention provides a semiconductor device comprising: a substrate having a first conductivity type, comprising: a body region having a first conductivity type; a source region formed in the body region; a drift a region having a second conductivity type; and a drain region type formed in the drift region; a multiple reduced surface field (RESURF) structure implanted in the drift region of the substrate; And a gate dielectric layer formed on the substrate, wherein the first conductivity type is opposite to the second conductivity type.
本發明另一實施例提供一種半導體裝置的製造方法,包括:提供具有一第一導電型態的一基底;植入帶有第一導電型態的一摻質於基底中,以定義一主體區;植入帶有一第二導電型態的一摻質於基底中,以定義一漂移區;形成一多重(multiple)表面電場降低(reduced surface field,RESURF)結構於漂移區中;形成一閘介電層於基底之上;形成一源極區域於主體區中;以及形成一汲極區域於漂移區中,其中第一導電型態相反於第二導電型態。 Another embodiment of the present invention provides a method of fabricating a semiconductor device, comprising: providing a substrate having a first conductivity type; implanting a dopant having a first conductivity type in the substrate to define a body region Implanting a dopant having a second conductivity type in the substrate to define a drift region; forming a multiple reduced surface field (RESURF) structure in the drift region; forming a gate The dielectric layer is over the substrate; a source region is formed in the body region; and a drain region is formed in the drift region, wherein the first conductivity type is opposite to the second conductivity pattern.
100‧‧‧LDMOS裝置 100‧‧‧LDMOS device
200‧‧‧半導體裝置 200‧‧‧Semiconductor device
110、210‧‧‧基底 110, 210‧‧‧ base
120、220‧‧‧磊晶層 120, 220‧‧‧ epitaxial layer
122、212、222‧‧‧主體區 122, 212, 222‧‧‧ main body area
124、214、224‧‧‧漂移區 124, 214, 224‧ ‧ drift zone
130‧‧‧淺溝隔離 130‧‧‧Shallow trench isolation
150、250‧‧‧源極區域 150, 250‧‧‧ source area
160、260‧‧‧汲極區域 160, 260‧‧ ‧ bungee area
20、30、40、50‧‧‧遮罩層 20, 30, 40, 50‧‧‧ mask layers
300、400、600‧‧‧摻雜製程 300, 400, 600‧‧‧ doping process
500‧‧‧離子佈植 500‧‧‧Ion implantation
700‧‧‧熱成長製程 700‧‧‧Hot growth process
230‧‧‧多重表面電場降低(RESURF)結構 230‧‧‧Multiple surface electric field reduction (RESURF) structure
230a‧‧‧第一離子區域 230a‧‧‧first ion zone
230b‧‧‧第二離子區域 230b‧‧‧Second ion zone
232‧‧‧第一離子層 232‧‧‧First ion layer
234‧‧‧第二離子層 234‧‧‧Second ion layer
x‧‧‧第一水平方向 X‧‧‧first horizontal direction
y‧‧‧第二水平方向 Y‧‧‧second horizontal direction
270‧‧‧第一閘介電層 270‧‧‧First gate dielectric layer
270a‧‧‧階形(step) 270a‧‧‧steps (step)
272‧‧‧第二閘介電層 272‧‧‧second gate dielectric layer
280‧‧‧階形閘介電層 280‧‧‧ step gate dielectric layer
252‧‧‧源極電極 252‧‧‧ source electrode
262‧‧‧汲極電極 262‧‧‧汲electrode
282‧‧‧閘電極 282‧‧‧ gate electrode
290‧‧‧層間介電層 290‧‧‧Interlayer dielectric layer
第1圖繪示出傳統的LDMOS裝置100;第2a~5h圖係根據本發明實施例繪示出半導體裝置200之製造方法的流程圖;第6a~6d圖根據一範例實施例繪示出階形閘介電結構280的形成方法;第7a~7d圖係根據另一範例實施例繪示出階形閘介電結構280的形成方法;第8圖係根據本發明實施例繪示出半導體裝置200的剖面示意圖。 1 is a flow chart showing a manufacturing method of a semiconductor device 200 according to an embodiment of the present invention; and FIGS. 6a to 6d are diagrams showing a step according to an exemplary embodiment. A method of forming a gate dielectric structure 280; a method of forming a step gate dielectric structure 280 according to another exemplary embodiment; and a drawing of a semiconductor device according to an embodiment of the invention; A schematic view of the section of 200.
以下說明本發明實施例之製作與使用。然而,可輕易了解本發明實施例提供許多合適的發明概念而可實施於廣泛的各種特定背景。所揭示的特定實施例僅僅用於說明以特定方法製作及使用本發明,並非用以侷限本發明的範圍。 The making and using of the embodiments of the present invention are described below. However, it will be readily understood that the embodiments of the present invention are susceptible to many specific embodiments of the invention and can The specific embodiments disclosed are merely illustrative of the invention, and are not intended to limit the scope of the invention.
以下配合圖式說明詳細的實施例。如果可能的話,圖式及說明中使用相同的標號來表示相同或相似的部件。在圖式中,為了清楚及方便性,而擴大形狀及厚度。以下說明將特別針對本發明實施例之裝置或是其中元件的形成部分。可以理解的是未特別繪示或說明的元件可具有各種不同的型式。可以理解的是以下的圖式並未依照比例繪示,而僅僅提供說明之用。 The detailed embodiments are described below in conjunction with the drawings. Wherever possible, the same reference numerals are used in the drawings In the drawings, the shape and thickness are enlarged for clarity and convenience. The following description will specifically address the device of the embodiment of the invention or the forming portion of the component therein. It will be understood that elements not specifically shown or described may be of various different types. It is to be understood that the following drawings are not to scale and are merely illustrative.
請參照第1圖,其繪示出傳統的LDMOS裝置100。 LDMOS裝置100包括基底110,基底110具有一主體區122以及一漂移區124形成於其中。基底110更包括多個淺溝隔絕(shallow trench isolation,STI)130形成於其中。在LDMOS裝置100中,因為STI 130的阻撓,使從源極150流至汲極160的電流須繞道而行(如第1圖之虛線所示)。這樣的電流路徑的偏差使LDMOS裝置100產升高接通電阻。 Referring to FIG. 1, a conventional LDMOS device 100 is illustrated. The LDMOS device 100 includes a substrate 110 having a body region 122 and a drift region 124 formed therein. The substrate 110 further includes a plurality of shallow trench isolation (STI) 130 formed therein. In the LDMOS device 100, the current flowing from the source 150 to the drain 160 has to be bypassed (as indicated by the dashed line in Fig. 1) due to the obstruction of the STI 130. Such a deviation of the current path causes the LDMOS device 100 to raise the on-resistance.
第2a~5e圖係根據本發明實施例繪示出半導體裝置200之製造方法的流程圖。 2a-5e are flowcharts illustrating a method of fabricating the semiconductor device 200 in accordance with an embodiment of the present invention.
第2a~2d圖係根據實施例繪示出半導體裝置200之主體區與漂移區的製造方法。請參考第2a圖,提供具有第一導電型態的基底210。基底210可為矽主體(bulk)基底、或矽覆絕緣體(silicon-on-insulator,SOI)基底等。一些實施例中,基底210可具有p型的第一導電型態,例如摻雜硼的基體。另一些實施例中,基底210可具有n型的第一導電型態,例如磷或砷基底。亦可使用其他合適的基底。 2a-2d illustrate a method of fabricating a body region and a drift region of the semiconductor device 200 according to an embodiment. Referring to Figure 2a, a substrate 210 having a first conductivity type is provided. The substrate 210 may be a bulk substrate, or a silicon-on-insulator (SOI) substrate or the like. In some embodiments, substrate 210 can have a p-type first conductivity type, such as a boron-doped matrix. In other embodiments, substrate 210 can have an n-type first conductivity type, such as a phosphorous or arsenic substrate. Other suitable substrates can also be used.
請參照第2b圖,在基底210上形成一遮罩層20。遮罩層20可為經圖案化的光阻層或硬遮罩層(例如,氮化矽、或氮氧化矽等)。形成遮罩層20後,實施一摻雜製程300以選擇性地(selectively)將一第一導電型態的摻質摻入基底210中,進而定義出主體區212。一些範例實施例中,基底210的濃度可高於主體區212的濃度。舉例來說,當主體區為p型時,基底210可為高度摻雜的p型(p+)。接著,在形成主體區212後將遮罩層20移除。 Referring to FIG. 2b, a mask layer 20 is formed on the substrate 210. The mask layer 20 can be a patterned photoresist layer or a hard mask layer (eg, tantalum nitride, or hafnium oxynitride, etc.). After the mask layer 20 is formed, a doping process 300 is performed to selectively incorporate a first conductivity type dopant into the substrate 210 to define the body region 212. In some example embodiments, the concentration of the substrate 210 may be higher than the concentration of the body region 212. For example, when the body region is p-type, the substrate 210 can be highly doped p-type (p+). Next, the mask layer 20 is removed after the body region 212 is formed.
請參照第2c圖,在基底之上形成另一遮罩層30。 遮罩層30可為經圖案化的光阻層或硬遮罩層(例如,氮化矽、或氮氧化矽等)。形成遮罩層20後,實施一摻雜製程400以選擇性地(selectively)將一第二導電型態的摻質摻入基底210中,進而定義出漂移區214。第二導電型態相反於第一導電型態。 Referring to Figure 2c, another mask layer 30 is formed over the substrate. The mask layer 30 can be a patterned photoresist layer or a hard mask layer (eg, tantalum nitride, or hafnium oxynitride, etc.). After the mask layer 20 is formed, a doping process 400 is performed to selectively incorporate a second conductivity type dopant into the substrate 210 to define the drift region 214. The second conductivity type is opposite to the first conductivity type.
一些實施例中,漂移區214可為形成於主體區212之前一寬廣的區域。如第3a圖所示,藉由佈植製程而形成主體區212於漂移區域214中。 In some embodiments, the drift region 214 can be a wide region formed before the body region 212. As shown in FIG. 3a, body region 212 is formed in drift region 214 by a routing process.
另一些實施例中,可在基底210上視需要地(optionally)形成一磊晶層,且主體區與漂移區係形成於磊晶層中。請參照第3b圖,一具有第一導電型態的磊晶層220形成於基底210上。此外,基底210之摻雜濃度大於磊晶層220之摻雜濃度。舉例來說,當第一導電型態為n型時,半導體基底210可為高度摻雜的n型(N+)基底,而磊晶層220則為輕度摻雜n型(n-)磊晶層。可藉由磊晶生長(epitaxial growth)形成厚度為3~10um的磊晶層220。在這樣的實施例中,主體區222與漂移區224系形成於磊晶層220中。主體區222與漂移區224的形成方法相似於主體區212與漂移區214,故在此不再贅述以防重複。 In other embodiments, an epitaxial layer may be formed on the substrate 210 as desired, and the body region and the drift region are formed in the epitaxial layer. Referring to FIG. 3b, an epitaxial layer 220 having a first conductivity type is formed on the substrate 210. In addition, the doping concentration of the substrate 210 is greater than the doping concentration of the epitaxial layer 220. For example, when the first conductivity type is n-type, the semiconductor substrate 210 can be a highly doped n-type (N+) substrate, and the epitaxial layer 220 is a lightly doped n-type (n-) epitaxial layer. Floor. The epitaxial layer 220 having a thickness of 3 to 10 um can be formed by epitaxial growth. In such an embodiment, body region 222 and drift region 224 are formed in epitaxial layer 220. The method of forming the body region 222 and the drift region 224 is similar to the body region 212 and the drift region 214, and therefore will not be described herein to prevent repetition.
接著,在形成主體區212與漂移區214後,執行形成多重(multiple)表面電場降低(reduced surface field,RESURF)結構的步驟。 Next, after forming the body region 212 and the drift region 214, a step of forming a multiple reduced surface field (RESURF) structure is performed.
第4a~4b圖根據實施例繪示出多重(multiple)表面電場降低(reduced surface field,RESURF)結構的製造方法。請參照第3a圖,在半導體基底210(或磊晶層220)上形成一遮罩層40以露出定義為表面電場降低區域的範圍。遮罩層40可為經圖 案化的光阻層或硬遮罩層(例如,氮化矽、或氮氧化矽等)。形成遮罩層40後,進行多道離子佈植(ion implantation)製程500以形成多重RESURF結構230。多重RESURF結構230係形成於漂移區214(或224)中。請參照第4b圖,在形成多重RESURF結構230後,移除遮罩層40並執行一退火製程以活化被植入的離子。 4a-4b illustrate a method of fabricating a multiple reduced surface field (RESURF) structure in accordance with an embodiment. Referring to FIG. 3a, a mask layer 40 is formed on the semiconductor substrate 210 (or the epitaxial layer 220) to expose a range defined as a surface electric field reduction region. The mask layer 40 can be a map A photoresist layer or a hard mask layer (for example, tantalum nitride, or hafnium oxynitride, etc.). After the mask layer 40 is formed, a multi-ion ion implantation process 500 is performed to form a multiple RESURF structure 230. A multiple RESURF structure 230 is formed in the drift region 214 (or 224). Referring to FIG. 4b, after forming the multiple RESURF structure 230, the mask layer 40 is removed and an annealing process is performed to activate the implanted ions.
第5a~5h圖根據本發明實施例繪示出不同排列組合的多重RESURF結構230。請參照第5a圖,其根據一範例實施例繪示出多重RESURF結構230的剖面示意圖。此實施例中,多重RESURF結構230為一多層結構,其包括多個第一離子區域230a與多個第二離子區域230b。多重RESURF結構230係由該些第一離子區域230a與第二離子區域230b於垂直方向交錯排列而成。第一與二離子區域230a、230b具有不同的導電型態。一些實施例中,該些第一離子區域230a的導電型態為相同於主體區212的第一導電型態,而該些第二離子區域230b的導電型態為相同於漂移區214的第二導電型態。另一些實施例中,該些第一離子區域230a的導電型態為第二導電型態,而該些第二離子區域230b的導電型態為第一導電型態。 Figures 5a-5h illustrate multiple RESURF structures 230 of different permutations combined in accordance with an embodiment of the present invention. Please refer to FIG. 5a, which illustrates a cross-sectional view of a multiple RESURF structure 230 according to an exemplary embodiment. In this embodiment, the multiple RESURF structure 230 is a multilayer structure including a plurality of first ion regions 230a and a plurality of second ion regions 230b. The multiple RESURF structure 230 is formed by staggering the first ion regions 230a and the second ion regions 230b in the vertical direction. The first and second ion regions 230a, 230b have different conductivity types. In some embodiments, the conductivity patterns of the first ion regions 230a are the same as the first conductivity patterns of the body regions 212, and the conductivity patterns of the second ion regions 230b are the same as the second regions of the drift regions 214. Conductive type. In other embodiments, the conductivity patterns of the first ion regions 230a are the second conductivity type, and the conductivity patterns of the second ion regions 230b are the first conductivity patterns.
第5b圖係根據另一範例實施例繪示出多重RESURF結構230的剖面示意圖。請參照第5b圖,多重RESURF結構230為一多層結構,其包括多個第一導電型態的第一離子區域230a與多個第二導電型態的第二離子區域230b。在此實施例中,係由該些第一離子區域230a與第二離子區域230b於一第一水平方向x交錯排列而成。第一與二離子區域230a、230b具有不同的導電型態。一些實施例中,該些第一離子區域230a的 導電型態為相同於主體區212的第一導電型態,而該些第二離子區域230b的導電型態為相同於漂移區214的第二導電型態。另一些實施例中,該些第一離子區域230a的導電型態為第二導電型態,而該些第二離子區域230b的導電型態為第一導電型態。 Figure 5b depicts a cross-sectional view of a multiple RESURF structure 230 in accordance with another exemplary embodiment. Referring to FIG. 5b, the multiple RESURF structure 230 is a multi-layer structure including a plurality of first ion regions 230a of a first conductivity type and a second ion region 230b of a plurality of second conductivity patterns. In this embodiment, the first ion regions 230a and the second ion regions 230b are staggered in a first horizontal direction x. The first and second ion regions 230a, 230b have different conductivity types. In some embodiments, the first ion regions 230a The conductivity type is the same as the first conductivity type of the body region 212, and the conductivity patterns of the second ion regions 230b are the same as the second conductivity pattern of the drift region 214. In other embodiments, the conductivity patterns of the first ion regions 230a are the second conductivity type, and the conductivity patterns of the second ion regions 230b are the first conductivity patterns.
請參照第5c圖,其係根據又一範例實施例繪示出多重RESURF結構230的三維透視圖。多重RESURF結構230為一多層結構,其包括多個第一導電型態的第一離子區域230a與多個第二導電型態的第二離子區域230b。在此實施例中,係由該些第一離子區域230a與第二離子區域230b於一第二水平方向y交錯排列而成。第一與二離子區域230a、230b具有不同的導電型態。一些實施例中,該些第一離子區域230a的導電型態為相同於主體區212的第一導電型態,而該些第二離子區域230b的導電型態為相同於漂移區214的第二導電型態。另一些實施例中,該些第一離子區域230a的導電型態為第二導電型態,而該些第二離子區域230b的導電型態為第一導電型態。 Referring to Figure 5c, a three-dimensional perspective view of the multiple RESURF structure 230 is depicted in accordance with yet another example embodiment. The multiple RESURF structure 230 is a multilayer structure including a plurality of first ion regions 230a of a first conductivity type and a second ion region 230b of a plurality of second conductivity types. In this embodiment, the first ion regions 230a and the second ion regions 230b are staggered in a second horizontal direction y. The first and second ion regions 230a, 230b have different conductivity types. In some embodiments, the conductivity patterns of the first ion regions 230a are the same as the first conductivity patterns of the body regions 212, and the conductivity patterns of the second ion regions 230b are the same as the second regions of the drift regions 214. Conductive type. In other embodiments, the conductivity patterns of the first ion regions 230a are the second conductivity type, and the conductivity patterns of the second ion regions 230b are the first conductivity patterns.
請參照第5d圖,其係根據又另一範例實施例繪示出多重RESURF結構230的剖面示意圖。在此實施例中,多重RESURF結構230係由多個第一離子層232與第二離子層234交錯排列而形成。該些第一離子層232係由第一離子區域230a所形成。一些實施例中,該些第一離子層232可由第二離子區域230b所形成。該些第二離子層234為由多個第一離子區域230a與多個第二離子區域230b於第一水平方向x交錯排列而組成的複合區域。第一與二離子區域230a、230b具有不同的導電型 態。一些實施例中,該些第一離子區域230a的導電型態為相同於主體區212的第一導電型態,而該些第二離子區域230b的導電型態為相同於漂移區214的第二導電型態。另一些實施例中,該些第一離子區域230a的導電型態為第二導電型態,而該些第二離子區域230b的導電型態為第一導電型態。 Referring to FIG. 5d, a cross-sectional view of a multiple RESURF structure 230 is illustrated in accordance with yet another exemplary embodiment. In this embodiment, the multiple RESURF structure 230 is formed by staggering a plurality of first ion layers 232 and second ion layers 234. The first ion layers 232 are formed by the first ion regions 230a. In some embodiments, the first ion layer 232 can be formed by the second ion region 230b. The second ion layers 234 are composite regions composed of a plurality of first ion regions 230a and a plurality of second ion regions 230b staggered in the first horizontal direction x. The first and second ion regions 230a, 230b have different conductivity types state. In some embodiments, the conductivity patterns of the first ion regions 230a are the same as the first conductivity patterns of the body regions 212, and the conductivity patterns of the second ion regions 230b are the same as the second regions of the drift regions 214. Conductive type. In other embodiments, the conductivity patterns of the first ion regions 230a are the second conductivity type, and the conductivity patterns of the second ion regions 230b are the first conductivity patterns.
一些實施例中,如第5e圖所示,多重RESURF結構230係由多個第一離子區域230a與多個第二離子區域230b於第一水平方向x與一垂直方向交錯排列而組成的多層結構。第一與二離子區域230a、230b具有不同的導電型態。一些實施例中,該些第一離子區域230a的導電型態為相同於主體區212的第一導電型態,而該些第二離子區域230b的導電型態為相同於漂移區214的第二導電型態。另一些實施例中,該些第一離子區域230a的導電型態為第二導電型態,而該些第二離子區域230b的導電型態為第一導電型態。 In some embodiments, as shown in FIG. 5e, the multiple RESURF structure 230 is a multilayer structure composed of a plurality of first ion regions 230a and a plurality of second ion regions 230b staggered in a first horizontal direction x and a vertical direction. . The first and second ion regions 230a, 230b have different conductivity types. In some embodiments, the conductivity patterns of the first ion regions 230a are the same as the first conductivity patterns of the body regions 212, and the conductivity patterns of the second ion regions 230b are the same as the second regions of the drift regions 214. Conductive type. In other embodiments, the conductivity patterns of the first ion regions 230a are the second conductivity type, and the conductivity patterns of the second ion regions 230b are the first conductivity patterns.
請參照第5f圖,其係根據一範例實施例繪示出多重RESURF結構230的三維透視圖。多重RESURF結構230多重RESURF結構230係由多個第一離子層232與多個第二離子層234於第一水平方向x交錯排列而組成的多層結構。該些第一離子層232為多個第一離子區域230a與多個第二離子區域230b於第二水平方向y交錯排列而組成的複合區域。第一與二離子區域230a、230b具有不同的導電型態。一些實施例中,該些第一離子區域230a的導電型態為相同於主體區212的第一導電型態,而該些第二離子區域230b的導電型態為相同於漂移區214的第二導電型態。另一些實施例中,該些第一離子區域230a的 導電型態為第二導電型態,而該些第二離子區域230b的導電型態為第一導電型態。 Referring to Figure 5f, a three-dimensional perspective view of the multiple RESURF structure 230 is depicted in accordance with an exemplary embodiment. Multiple RESURF Structure 230 The multiple RESURF structure 230 is a multilayer structure composed of a plurality of first ion layers 232 and a plurality of second ion layers 234 staggered in a first horizontal direction x. The first ion layer 232 is a composite region composed of a plurality of first ion regions 230a and a plurality of second ion regions 230b staggered in the second horizontal direction y. The first and second ion regions 230a, 230b have different conductivity types. In some embodiments, the conductivity patterns of the first ion regions 230a are the same as the first conductivity patterns of the body regions 212, and the conductivity patterns of the second ion regions 230b are the same as the second regions of the drift regions 214. Conductive type. In other embodiments, the first ion regions 230a The conductive type is the second conductive type, and the conductive patterns of the second ion regions 230b are the first conductive type.
請參照第5g圖,其係根據一範例實施例繪示出多重RESURF結構230的三維透視圖。多重RESURF結構230多重RESURF結構230係由多個第一離子層232與多個第二離子層234於第一水平方向y交錯排列而組成的多層結構。該些第一離子層232為多個第一離子區域230a與多個第二離子區域230b於第二水平方向x交錯排列而組成的複合區域。該些第二離子層234係由多個第一離子區域230a所形成。一些實施例中,該些第二離子層234係由多個第二離子區域230b所形成。第一與二離子區域230a、230b具有不同的導電型態。一些實施例中,該些第一離子區域230a的導電型態為相同於主體區212的第一導電型態,而該些第二離子區域230b的導電型態為相同於漂移區214的第二導電型態。另一些實施例中,該些第一離子區域230a的導電型態為第二導電型態,而該些第二離子區域230b的導電型態為第一導電型態。 Referring to Figure 5g, a three-dimensional perspective view of the multiple RESURF structure 230 is depicted in accordance with an exemplary embodiment. Multiple RESURF Structure 230 The multiple RESURF structure 230 is a multilayer structure composed of a plurality of first ion layers 232 and a plurality of second ion layers 234 staggered in a first horizontal direction y. The first ion layers 232 are composite regions in which a plurality of first ion regions 230a and a plurality of second ion regions 230b are staggered in the second horizontal direction x. The second ion layers 234 are formed by a plurality of first ion regions 230a. In some embodiments, the second ion layers 234 are formed by a plurality of second ion regions 230b. The first and second ion regions 230a, 230b have different conductivity types. In some embodiments, the conductivity patterns of the first ion regions 230a are the same as the first conductivity patterns of the body regions 212, and the conductivity patterns of the second ion regions 230b are the same as the second regions of the drift regions 214. Conductive type. In other embodiments, the conductivity patterns of the first ion regions 230a are the second conductivity type, and the conductivity patterns of the second ion regions 230b are the first conductivity patterns.
一些實施例中,如第5h圖所示,多重RESURF結構230係由多個第一離子區域230a與多個第二離子區域230b於第一水平方向y與一垂直方向交錯排列而組成的多層結構。第一與二離子區域230a、230b具有不同的導電型態。一些實施例中,該些第一離子區域230a的導電型態為相同於主體區212的第一導電型態,而該些第二離子區域230b的導電型態為相同於漂移區214的第二導電型態。另一些實施例中,該些第一離子區域230a的導電型態為第二導電型態,而該些第二離子區域 230b的導電型態為第一導電型態。 In some embodiments, as shown in FIG. 5h, the multiple RESURF structure 230 is a multilayer structure composed of a plurality of first ion regions 230a and a plurality of second ion regions 230b staggered in a first horizontal direction y and a vertical direction. . The first and second ion regions 230a, 230b have different conductivity types. In some embodiments, the conductivity patterns of the first ion regions 230a are the same as the first conductivity patterns of the body regions 212, and the conductivity patterns of the second ion regions 230b are the same as the second regions of the drift regions 214. Conductive type. In other embodiments, the conductive patterns of the first ion regions 230a are the second conductivity type, and the second ion regions The conductivity type of 230b is the first conductivity type.
應理解的是,雖然上述實施例係有關於特定排列的多重RESURF結構230,然而,本發明並不限於第5a~5h圖所示的排列組合。相反地,本發明涵蓋各種修改與排列組合。舉例來說,只要能縮短源極區域到汲極區域的電流路徑,多重RESURF結構的離子區域或離子層的數量可多漁獲少於第5a~5h圖所示的多重RESURF結構230,且多重RESURF結構的各個離子區域或離子層可具有不同的厚度或尺寸。此外,第5a~5h圖所示的多重RESURF結構亦可形成於如第3b圖的磊晶層之漂移區224中。 It should be understood that while the above embodiments are directed to a plurality of RESURF structures 230 for a particular arrangement, the invention is not limited to the permutations and combinations shown in Figures 5a-5h. Rather, the invention encompasses various modifications and permutations. For example, as long as the current path from the source region to the drain region can be shortened, the number of ion regions or ion layers of the multiple RESURF structure can be captured more than the multiple RESURF structure 230 shown in the 5a-5h diagram, and the multiple RESURF Each ionic region or ionic layer of the structure can have a different thickness or size. Further, the multiple RESURF structure shown in Figs. 5a to 5h may also be formed in the drift region 224 of the epitaxial layer as in Fig. 3b.
接著,具有一階形(step)形成於其邊緣的閘介電結構將根據一實施例在以下作敘述。 Next, a gate dielectric structure having a step formed on its edge will be described below in accordance with an embodiment.
第6a~6d圖根據一範例實施例繪示出階形閘介電結構280的形成方法。 6a-6d illustrate a method of forming a step gate dielectric structure 280 in accordance with an exemplary embodiment.
請參照第6a圖,在形成多重RESURF結構230後,在半導體基底210上(或磊晶層220)形成一第一閘介電層270。第一閘介電層270可包括氧化矽、氮化矽、氮氧化矽、高介電常數材料(high-k dielectrics)、其他合適的介電材料、或前述之組合。其中,高介電常數材料可包括金屬氧化物,例如,Li、Be、Mg、Ca、Sr、Sc、Y、Zr、Hf、Al、La、Ce、Pr、Nd、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb、Lu、或前述之組合等金屬的氧化物。第一金屬介電層270可由此領域習知技術而形成,例如原子層沉積(atomic layer deposition,ALD)、化學氣相沉積(chemical vapor deposition,CVD)、物理氣相沉積(physical vapor deposition,PVD)、熱氧化(thermal oxidation)、紫外光-臭氧氧化(UV-ozone oxidation)、或前述之組合。第一閘介電層270之厚度可為約400~5000埃。第一閘介電層270可同時覆蓋主體區212與漂移區214(或222與224)。 Referring to FIG. 6a, after forming the multiple RESURF structure 230, a first gate dielectric layer 270 is formed on the semiconductor substrate 210 (or the epitaxial layer 220). The first gate dielectric layer 270 can include hafnium oxide, tantalum nitride, hafnium oxynitride, high-k dielectrics, other suitable dielectric materials, or combinations of the foregoing. Wherein, the high dielectric constant material may include a metal oxide, for example, Li, Be, Mg, Ca, Sr, Sc, Y, Zr, Hf, Al, La, Ce, Pr, Nd, Sm, Eu, Gd, Tb An oxide of a metal such as Dy, Ho, Er, Tm, Yb, Lu, or a combination thereof. The first metal dielectric layer 270 can be formed by conventional techniques in the art, such as atomic layer deposition (ALD), chemical vapor deposition (CVD), physical vapor deposition (physical vapor deposition). Vapor deposition (PVD), thermal oxidation, UV-ozone oxidation, or a combination of the foregoing. The first gate dielectric layer 270 can have a thickness of about 400 to 5000 angstroms. The first gate dielectric layer 270 can cover both the body region 212 and the drift region 214 (or 222 and 224).
請參照第6b圖,利用一遮罩層50進行一蝕刻製程600以移除一部份的第一閘介電層270,進而在第一閘介電層270至少一邊緣上形成一階形270a(如第6c圖所示)。遮罩層50可為經圖案化的光阻層或硬遮罩層(例如,氮化矽、或氮氧化矽等)。蝕刻製程600可為乾蝕刻或濕蝕刻。應理解的是,雖然第6c圖所示的階形270a為一崖形,階形270a亦可為圓形或其他適合的形狀。在形成階形270a於第一閘介電層270之邊緣上後,將遮罩層50移除。 Referring to FIG. 6b, an etch process 600 is performed using a mask layer 50 to remove a portion of the first thyristor layer 270, thereby forming a step 270a on at least one edge of the first thyristor layer 270. (as shown in Figure 6c). The mask layer 50 can be a patterned photoresist layer or a hard mask layer (eg, tantalum nitride, or hafnium oxynitride, etc.). The etch process 600 can be dry etch or wet etch. It should be understood that although the step 270a shown in Fig. 6c is a cliff shape, the step 270a may also be circular or other suitable shape. After forming the step 270a on the edge of the first gate dielectric layer 270, the mask layer 50 is removed.
接著,請參照第6d圖,在半導體基底210(或磊晶層220)上形成一第二閘介電層272,第二閘介電層272之厚度小於第一閘介電層270。第一閘介電層270與第二閘介電層272組成階形閘介電結構280。第二閘介電層272鄰接於第一閘介電層270。第二閘介電層272之厚度為約30~1000埃。可由相同於形成第一閘介電層270的方法而形成第二閘介電層272,例如,原子層沉積(atomic layer deposition,ALD)、化學氣相沉積(chemical vapor deposition,CVD)、物理氣相沉積(physical vapor deposition,PVD)、熱氧化(thermal oxidation)、紫外光-臭氧氧化(UV-ozone oxidation)、或前述之組合。第二閘介電層272的材料可相同於第一閘介電層270,例如,氧化矽、氮化矽、氮氧化矽、高介電常數材料(high-k dielectrics)、其他合適的介 電材料、或前述之組合。 Next, referring to FIG. 6d, a second gate dielectric layer 272 is formed on the semiconductor substrate 210 (or the epitaxial layer 220). The thickness of the second gate dielectric layer 272 is smaller than the first gate dielectric layer 270. The first gate dielectric layer 270 and the second gate dielectric layer 272 form a step gate dielectric structure 280. The second gate dielectric layer 272 is adjacent to the first gate dielectric layer 270. The second gate dielectric layer 272 has a thickness of about 30 to 1000 angstroms. The second gate dielectric layer 272 can be formed by the same method as the first gate dielectric layer 270, for example, atomic layer deposition (ALD), chemical vapor deposition (CVD), physical gas. Physical vapor deposition (PVD), thermal oxidation, UV-ozone oxidation, or a combination thereof. The material of the second gate dielectric layer 272 may be the same as the first gate dielectric layer 270, for example, hafnium oxide, tantalum nitride, hafnium oxynitride, high-k dielectrics, other suitable dielectric layers. Electrical material, or a combination of the foregoing.
第7a~7d圖係根據另一範例實施例繪示出階形閘介電結構280的形成方法。 7a-7d illustrate a method of forming a step gate dielectric structure 280 according to another exemplary embodiment.
請參照第7a圖,在半導體基底210上(或磊晶層220)形成一第一閘介電層270。第一閘介電層270可包括氧化矽、氮化矽、氮氧化矽、高介電常數材料(high-k dielectrics)、其他合適的介電材料、或前述之組合。其中,高介電常數材料可包括金屬氧化物,例如,Li、Be、Mg、Ca、Sr、Sc、Y、Zr、Hf、Al、La、Ce、Pr、Nd、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb、Lu、或前述之組合等金屬的氧化物。第一金屬介電層270可由此領域習知技術而形成,例如原子層沉積(atomic layer deposition,ALD)、化學氣相沉積(chemical vapor deposition,CVD)、物理氣相沉積(physical vapor deposition,PVD)、熱氧化(thermal oxidation)、紫外光-臭氧氧化(UV-ozone oxidation)、或前述之組合。第一閘介電層270之厚度可為約400~5000埃。第一閘介電層270可同時覆蓋主體區212與漂移區214(或222與224)。 Referring to FIG. 7a, a first gate dielectric layer 270 is formed on the semiconductor substrate 210 (or the epitaxial layer 220). The first gate dielectric layer 270 can include hafnium oxide, tantalum nitride, hafnium oxynitride, high-k dielectrics, other suitable dielectric materials, or combinations of the foregoing. Wherein, the high dielectric constant material may include a metal oxide, for example, Li, Be, Mg, Ca, Sr, Sc, Y, Zr, Hf, Al, La, Ce, Pr, Nd, Sm, Eu, Gd, Tb An oxide of a metal such as Dy, Ho, Er, Tm, Yb, Lu, or a combination thereof. The first metal dielectric layer 270 can be formed by conventional techniques in the art, such as atomic layer deposition (ALD), chemical vapor deposition (CVD), physical vapor deposition (PVD). ), thermal oxidation, UV-ozone oxidation, or a combination of the foregoing. The first gate dielectric layer 270 can have a thickness of about 400 to 5000 angstroms. The first gate dielectric layer 270 can cover both the body region 212 and the drift region 214 (or 222 and 224).
請參照第7b圖,在第一閘介電層270上形成遮罩層60,罩層60具有至少一開口60a以選擇性(selectively)暴露出一部份的第一閘介電層270。開口60a可由一蝕刻製程形成。 Referring to FIG. 7b, a mask layer 60 is formed on the first gate dielectric layer 270. The cap layer 60 has at least one opening 60a for selectively exposing a portion of the first gate dielectric layer 270. The opening 60a can be formed by an etching process.
請參照第7c圖,在暴露於該口中的部份第一閘介電層270上進行一熱成長(thermal growth)製程700。該部份的第一閘介電層270(進行熱成長製程700的部份)膨脹至一較大的厚度。一些實施例中,可視情況地進行一第二熱成長製程,以使 該部份的第一閘介電層270更進一步地膨脹。膨脹的部份第一閘介電層270之厚度為約2000~6000埃。在一些實施例中,嚅地7圖所示,一部份的第一閘介電層270延伸至基底210(或壘晶層220)中。 Referring to FIG. 7c, a thermal growth process 700 is performed on a portion of the first gate dielectric layer 270 exposed to the port. The portion of the first gate dielectric layer 270 (the portion of the thermal growth process 700) is expanded to a greater thickness. In some embodiments, a second thermal growth process can be performed as appropriate to enable The portion of the first gate dielectric layer 270 is further expanded. The expanded portion of the first gate dielectric layer 270 has a thickness of about 2000 to 6000 angstroms. In some embodiments, a portion of the first gate dielectric layer 270 extends into the substrate 210 (or the via layer 220) as shown in FIG.
請參照第7d圖,移除遮罩層60及一部份的第一閘介電層270以形成階形閘介電結構280。 Referring to FIG. 7d, the mask layer 60 and a portion of the first gate dielectric layer 270 are removed to form the step gate dielectric structure 280.
在形成階形閘介電結構280後,進行一製程以形成源極與汲極區域。請參照第8圖,在主體區212(或222)中形成一源極區域250,以及在漂移區214(或224)中形成一汲極區域260。源極與汲極區域250、260可由此技藝習知的摻雜製程而形成,例如離子佈植製程。 After forming the step gate dielectric structure 280, a process is performed to form the source and drain regions. Referring to FIG. 8, a source region 250 is formed in the body region 212 (or 222), and a drain region 260 is formed in the drift region 214 (or 224). The source and drain regions 250, 260 can be formed by a doping process as is known in the art, such as an ion implantation process.
接著,形成一個傳統半導體裝置中常見的元件已完成半導體裝置200的製造,例如,層間介電(inter-layer dielectric,ILD)層290、源極/汲極電極252與262、以及閘電極282。請參照第8圖,層間介電層290可覆蓋於半導體基底210上並具有接觸孔(contact holes)以露出源極/汲極區域250、260。應注意的是,根據裝置的設計,接觸孔的數量可為二或更多。閘電極282可包括一單層或多層結構形成於階形閘介電結構280上。形成閘電極282的材料可包括金屬、摻雜的多晶矽、或前述之組合。形成閘電極282的製程可包括低壓化學氣相沉積(low-pressure chemical vapor deposition,LPCVD)、電漿增強化學氣相沉積(plasma enhaced chemical vapor deposition,PECVD)、其他合適的製程、或前述之組合。源極電極252係形成於源極區域250上,而汲極電極262係形成於汲極區域260上。 Next, fabrication of a semiconductor device 200 is completed by forming a component conventional in a conventional semiconductor device, for example, an inter-layer dielectric (ILD) layer 290, source/drain electrodes 252 and 262, and a gate electrode 282. Referring to FIG. 8, an interlayer dielectric layer 290 may be overlying the semiconductor substrate 210 and have contact holes to expose the source/drain regions 250, 260. It should be noted that the number of contact holes may be two or more depending on the design of the device. The gate electrode 282 can include a single or multi-layer structure formed on the step gate dielectric structure 280. The material forming the gate electrode 282 may include a metal, a doped polysilicon, or a combination of the foregoing. The process of forming the gate electrode 282 may include low-pressure chemical vapor deposition (LPCVD), plasma-enhanced chemical vapor deposition (PECVD), other suitable processes, or a combination thereof. . The source electrode 252 is formed on the source region 250, and the drain electrode 262 is formed on the drain region 260.
相較於傳統LDMOS裝置,本發明實施例至少提供以下優點。首先,多重RESURF結構230提供一個從源極區域250到汲極區域260的一個較短的電流路徑(如第8圖之虛線所示),這降低了半導體裝置200的接通電阻。再者,當接通電阻降低時,閘介電結構280的階形設計,能有效地維持崩潰電壓值。 Embodiments of the present invention provide at least the following advantages over conventional LDMOS devices. First, the multiple RESURF structure 230 provides a shorter current path from the source region 250 to the drain region 260 (as indicated by the dashed line in FIG. 8), which reduces the on-resistance of the semiconductor device 200. Moreover, when the on-resistance is lowered, the stepped design of the gate dielectric structure 280 can effectively maintain the breakdown voltage value.
雖然本發明已以較佳實施例揭露如上,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,在不脫離本發明之精神和範圍內,當可作更動、替代與潤飾。舉例來說,任何所屬技術領域中具有通常知識者可輕易理解此處所述的許多特徵、功能、製程及材料可在本發明的範圍內作更動。 Although the present invention has been disclosed in the above preferred embodiments, it is not intended to limit the invention, and any one of ordinary skill in the art can be modified, replaced and retouched without departing from the spirit and scope of the invention. . For example, those skilled in the art can readily appreciate that many of the features, functions, processes, and materials described herein can be modified within the scope of the invention.
200‧‧‧半導體裝置 200‧‧‧Semiconductor device
210‧‧‧基底 210‧‧‧Base
212‧‧‧主體區 212‧‧‧ main body area
214‧‧‧漂移區 214‧‧‧ drift zone
250‧‧‧源極區域 250‧‧‧ source area
260‧‧‧汲極區域 260‧‧‧Bungee area
230‧‧‧多重表面電場降低(RESURF)結構 230‧‧‧Multiple surface electric field reduction (RESURF) structure
270‧‧‧第一閘介電層 270‧‧‧First gate dielectric layer
270a‧‧‧階形(step) 270a‧‧‧steps (step)
272‧‧‧第二閘介電層 272‧‧‧second gate dielectric layer
280‧‧‧階形閘介電層 280‧‧‧ step gate dielectric layer
252‧‧‧源極電極 252‧‧‧ source electrode
262‧‧‧汲極電極 262‧‧‧汲electrode
282‧‧‧閘電極 282‧‧‧ gate electrode
290‧‧‧層間介電層 290‧‧‧Interlayer dielectric layer
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