TWI572038B - High voltage metal-oxide-semiconductor field-effect transistor device - Google Patents
High voltage metal-oxide-semiconductor field-effect transistor device Download PDFInfo
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本發明是有關於一種高壓金氧半場效電晶體元件的結構,且特別是有關於一種可提升元件崩潰電壓之高壓金氧半場效電晶體元件的結構。 The present invention relates to a structure of a high voltage MOS field device, and more particularly to a structure of a high voltage MOSFET that can raise the breakdown voltage of a device.
習知之高壓金氧半場效電晶體(High Voltage Metal-Oxide-Semiconductor Field-Effect Transistor,以下簡稱HV MOSFET)元件布局通常設計成圓形,從圓形的HV MOSFET元件之上視剖面圖來看,圓心部分即為汲極(Drain),而環繞汲極之外環部分即為源極(Source)。此外,圓形HV MOSFET的通道寬度是由汲極與源極之間區域之圓周長來決定,因此,若欲提高HV MOSFET元件的導通電流,則需增加圓形HV MOSFET元件的半徑,但也相對的增加了HV MOSFET元件的面積。 The high voltage metal-Oxide-Semiconductor Field-Effect Transistor (HV MOSFET) component layout is usually designed to be circular, from the top view of the circular HV MOSFET component. The center of the circle is the drain (Drain), and the outer part of the ring around the drain is the source. In addition, the channel width of the circular HV MOSFET is determined by the circumference of the region between the drain and the source. Therefore, if the on-current of the HV MOSFET device is to be increased, the radius of the circular HV MOSFET component needs to be increased, but also The area of the HV MOSFET component is relatively increased.
而為了同時增加HV MOSFET元件的導通電流並且使HV MOSFET元件的面積達到最小化,目前已發展出跑道形HV MOSFET元件以及M形HV MOSFET元件。然而,若欲得到較大的導通電流,M形HV MOSFET元件是目前之較佳選擇。 In order to simultaneously increase the on-current of the HV MOSFET component and minimize the area of the HV MOSFET component, a racetrack-shaped HV MOSFET component and an M-shaped HV MOSFET component have been developed. However, for larger on-state currents, M-shaped HV MOSFET components are currently the preferred choice.
但是,習知製程所完成之M形HV MOSFET元件的崩潰電壓(Breakdown Voltage,簡稱BDV)分別小於圓形與跑道形之HV MOSFET元件之崩潰電壓,因此若同時整合此三種形狀之 HV MOSFET元件於同一積體電路晶片中時,則會受限於M形HV MOSFET元件的崩潰電壓,致使整體積體電路晶片之耐壓能力下降。 However, the breakdown voltage (Breakdown Voltage, BDV) of the M-shaped HV MOSFET component completed by the conventional process is smaller than the breakdown voltage of the circular and racetrack-shaped HV MOSFET components, respectively, so if the three shapes are integrated at the same time, When the HV MOSFET device is in the same integrated circuit chip, it is limited by the breakdown voltage of the M-shaped HV MOSFET device, resulting in a decrease in the withstand voltage capability of the entire bulk circuit chip.
但經發明人研究顯示,習知之M形HV MOSFET元件,因具有多彎角的特殊元件形狀,而使得元件之部分區域具有較高電場與較大的電流,相對的降低此區域的耐壓能力,進而影響整體M形HV MOSFET元件之崩潰電壓,因此發明人於先前提出之申請案號為100130576之”高壓金氧半導體電晶體元件及其製作方法”來改善此一缺失,但仍有未盡理想之處。 However, according to research by the inventors, the conventional M-shaped HV MOSFET component has a higher electric field and a larger current in a part of the component due to the shape of a special component having a plurality of corners, and relatively reduces the withstand voltage capability of the region. In order to improve the breakdown voltage of the overall M-shaped HV MOSFET device, the inventor has previously applied the "high-voltage MOS transistor device and its fabrication method" of the application number 100130576 to improve this deficiency, but still has not completed Ideal.
有鑑於此,如何進一步提升M形HV MOSFET元件之崩潰電壓,用以達成整合各形狀之HV MOSFET元件的目標,係為發展本案之主要目的。 In view of this, how to further improve the breakdown voltage of M-shaped HV MOSFET components to achieve the goal of integrating various shapes of HV MOSFET components is to develop the main purpose of the case.
本發明的目的在於提供一種高壓金氧半場效電晶體元件,其包含:一基底,具有一第一導電類型;一深井區,設置於基底中,具有不同於第一導電類型之一第二導電類型,且深井區具有一邊緣部與一中間部,邊緣部位於中間部的周圍並包圍中間部;一源極/基體區,設置於深井區中,其中定義出一通道區;一汲極區,設置於深井區中;一閘極結構,設置於源極/基體區與汲極區之間,其中包含有一絕緣層;以及一第一摻雜區,設於該區中並位於絕緣層之下方,且第一摻雜區具有第一導電類型,而位於邊緣部範圍之第一摻雜區之摻雜濃度與深井區之邊緣部之摻雜濃度間具有一第一比值,位於中間部範圍之第一摻雜區之摻雜濃度與深井區之中間部之摻雜濃度間具有一第 二比值,且第一比值與第二比值之變異度小於或等於5%。 It is an object of the present invention to provide a high voltage gold oxide half field effect transistor device comprising: a substrate having a first conductivity type; a deep well region disposed in the substrate and having a second conductivity different from the first conductivity type Type, and the deep well zone has an edge portion and an intermediate portion, the edge portion is located around the intermediate portion and surrounds the intermediate portion; a source/base region is disposed in the deep well region, wherein a channel region is defined; a drain region Provided in the deep well region; a gate structure disposed between the source/base region and the drain region, comprising an insulating layer; and a first doped region disposed in the region and located in the insulating layer Bottom, and the first doped region has a first conductivity type, and the doping concentration of the first doped region in the edge portion has a first ratio between the doping concentration of the edge portion of the deep well region, and is located in the middle portion There is a first between the doping concentration of the first doping region and the doping concentration of the middle portion of the deep well region Two ratios, and the variability of the first ratio and the second ratio is less than or equal to 5%.
在本發明的較佳實施例中,上述基底為一矽基板。 In a preferred embodiment of the invention, the substrate is a germanium substrate.
在本發明的較佳實施例中,上述源極/基體區包含:一高壓井區,設置於上述深井區中,具有上述第一導電類型;一基體接觸區,設置於上述高壓井區中,具有上述第一導電類型,其摻質濃度較上述高壓井區為高;以及一源極接觸區,設置於上述高壓井區中,具有上述第二導電類型。 In a preferred embodiment of the present invention, the source/substrate region comprises: a high-voltage well region disposed in the deep well region and having the first conductivity type; a substrate contact region disposed in the high-voltage well region, The first conductivity type has a higher dopant concentration than the high voltage well region; and a source contact region is disposed in the high voltage well region and has the second conductivity type.
在本發明的較佳實施例中,上述汲極區包含:一漂移區(DRIFT),設置於上述深井區中,具有上述第二導電類型;以及一汲極接觸區,設置於上述漂移區中,具有上述第二導電類型,其摻質濃度較上述漂移區為高。 In a preferred embodiment of the present invention, the drain region includes: a drift region (DRIFT) disposed in the deep well region and having the second conductivity type; and a drain contact region disposed in the drift region And having the above second conductivity type, the dopant concentration being higher than the drift region.
在本發明的較佳實施例中,上述閘極結構更包含:一閘極介電層,設置於該通道區上方;一閘極導體層,設置於上述閘極介電層表面上;以及一場電極結構,設置於上述絕緣層表面上。 In a preferred embodiment of the present invention, the gate structure further includes: a gate dielectric layer disposed over the channel region; a gate conductor layer disposed on the surface of the gate dielectric layer; and a field The electrode structure is disposed on the surface of the insulating layer.
在本發明的較佳實施例中,上述第一摻雜區係為一降場層。 In a preferred embodiment of the invention, the first doped region is a falling field layer.
在本發明的較佳實施例中,上述高壓金氧半場效電晶體元件為一M型高壓金氧半場效電晶體元件。 In a preferred embodiment of the invention, the high voltage MOS field device is an M type high voltage MOSFET.
在本發明的較佳實施例中,上述第一導電類型為P型,上述第二導電類型為N型。 In a preferred embodiment of the invention, the first conductivity type is a P type, and the second conductivity type is an N type.
在本發明的較佳實施例中,上述第一導電類型為N型,上述第二導電類型為P型。 In a preferred embodiment of the invention, the first conductivity type is N-type and the second conductivity type is P-type.
請參見圖1,其係HV MOSFET元件之剖面示意圖,其中 包含有一基底1,其具有第一導電類型;而深井區11設置於該基底1中,具有不同於該第一導電類型之第二導電類型。而源極/基體區12與汲極區13皆設置於該深井區11中,而源極/基體區12中具有第一導電類型之高壓井區17,而高壓井區17中定義出一通道區14,閘極結構15係設置於該通道區14上方,而該通道區14與汲極區13間設有絕緣層19,可用例如場氧化層(field oxide)等結構來完成。至於第一摻雜區16係設於深井區11中並位於該場氧化層之下方,且該第一摻雜區16具有該第一導電類型。以下內容以第一導電類型為P型而第二導電類型為N型舉例說明,但實際應用並不限於此,也可以是第一導電類型為N型而第二導電類型為P型。 Please refer to FIG. 1 , which is a schematic cross-sectional view of an HV MOSFET device, wherein A substrate 1 is provided having a first conductivity type; and a deep well region 11 is disposed in the substrate 1 having a second conductivity type different from the first conductivity type. The source/base region 12 and the drain region 13 are both disposed in the deep well region 11, and the source/base region 12 has the high conductivity well region 17 of the first conductivity type, and the high voltage well region 17 defines a channel. The gate structure 15 is disposed above the channel region 14, and the insulating layer 19 is disposed between the channel region 14 and the drain region 13, and can be completed by a structure such as a field oxide. The first doped region 16 is disposed in the deep well region 11 and below the field oxide layer, and the first doped region 16 has the first conductivity type. The following is exemplified by the first conductivity type being P-type and the second conductivity type being N-type, but the practical application is not limited thereto, and the first conductivity type is N-type and the second conductivity type is P-type.
經發明人研究後發現,HV MOSFET元件在經歷較高溫度且較長時間之熱製程後,由於熱製程中高溫所造成的熱擴散效應,會導致M形HV MOSFET元件內部之摻質產生分佈上的變化,造成用以完成P型降場層(P-top)之第一摻雜區16中的P型摻質與深井區11中的N型摻質之濃度比值不均勻,導致部份區域中第一摻雜區16的P型摻質與深井區11的N型摻質之濃度比值已偏離預設值過遠而誘發崩潰電壓的下降。尤其是深井區11之邊緣部111中之N型摻質,因其易向深井區11外部擴散而濃度將大幅下降,導致深井區11之邊緣部111與中間部112中之N型摻質濃度將產生如圖2所示之不均勻現象,圖2中係表示出深井區11之上視圖,其係原本均勻分佈之N型摻質之濃度經過長時間熱製程造成的熱擴散效應後所形成之濃度分佈示意圖,造成深井區11之邊緣部111之N型摻質濃度比中間部112之N型摻質濃度為低。 According to the research by the inventors, it is found that the HV MOSFET component undergoes a high temperature and a long time after the thermal process, due to the thermal diffusion effect caused by the high temperature in the thermal process, the dopant in the M-shaped HV MOSFET component is distributed. The variation causes the concentration ratio of the P-type dopant in the first doped region 16 to complete the P-type p-top layer to the N-type dopant in the deep well region 11 to be uneven, resulting in a partial region. The concentration ratio of the P-type dopant in the first doped region 16 to the N-type dopant in the deep well region 11 has deviated too far from the preset value to induce a drop in the breakdown voltage. In particular, the N-type dopant in the edge portion 111 of the deep well region 11 is greatly reduced in concentration due to its easy diffusion to the outside of the deep well region 11, resulting in the N-type dopant concentration in the edge portion 111 and the intermediate portion 112 of the deep well region 11. The unevenness as shown in Fig. 2 will be produced. In Fig. 2, the upper view of the deep well region 11 is shown, which is formed by the concentration of the N-type dopant which is originally uniformly distributed after the thermal diffusion effect caused by the long-time thermal process. The concentration distribution diagram is such that the N-type dopant concentration of the edge portion 111 of the deep well region 11 is lower than the N-type dopant concentration of the intermediate portion 112.
有鑑於此,本案於圖3A至圖3C中提出一種技術方案來 解決此類問題,首先,圖3A中表示出於一P型基底3中形成一N型深井區31,且控制該N型深井區31中邊緣部311之N型摻質濃度與中間部312之N型摻質濃度於摻雜完成時呈現不同,主要是邊緣部311之N型摻質濃度大於中間部312之N型摻質濃度。然後,如圖3B所示,於該N型深井區31中形成源極/基體(body)區32與汲極區33以及第一摻雜區36,然後再完成閘極結構35等其它結構而形成如圖3C所示之高壓金氧半電晶體元件剖面圖。其中該P型基底3可為P型矽基板,而源極/基體(body)區32包含有P型高壓井區320、摻質濃度較P型高壓井區320為高之P+基體接觸區321以及N+源極接觸區322。至於汲極區33包含有N型漂移區(N-DRIFT)330以及摻質濃度較N型漂移區330為高之N+汲極接觸區331。至於閘極結構35則包含有設置於通道34、N型深井區31與第一摻雜區36上方之閘極介電層(gate dielectric layer)350以及絕緣層(insulator layer)352,以及設置於該閘極介電層(gate dielectric layer)350以及絕緣層352表面上之閘極導體層351以及場電極結構353。 In view of this, the present invention proposes a technical solution in FIGS. 3A to 3C. To solve such a problem, first, FIG. 3A shows that an N-type deep well region 31 is formed in a P-type substrate 3, and the N-type dopant concentration and the intermediate portion 312 of the edge portion 311 in the N-type deep well region 31 are controlled. The N-type dopant concentration is different when the doping is completed, mainly because the N-type dopant concentration of the edge portion 311 is greater than the N-type dopant concentration of the intermediate portion 312. Then, as shown in FIG. 3B, a source/body region 32 and a drain region 33 and a first doping region 36 are formed in the N-type deep well region 31, and then other structures such as the gate structure 35 are completed. A cross-sectional view of the high voltage MOS semi-transistor element as shown in Fig. 3C is formed. The P-type substrate 3 may be a P-type germanium substrate, and the source/body region 32 includes a P-type high-pressure well region 320 and a P+ substrate contact region 321 having a higher dopant concentration than the P-type high-pressure well region 320. And an N+ source contact region 322. The drain region 33 includes an N-type drift region (N-DRIFT) 330 and an N+ drain contact region 331 having a higher dopant concentration than the N-type drift region 330. The gate structure 35 includes a gate dielectric layer 350 disposed above the channel 34, the N-type deep well region 31 and the first doped region 36, and an insulator layer 352, and is disposed on the gate layer The gate dielectric layer 350 and the gate conductor layer 351 on the surface of the insulating layer 352 and the field electrode structure 353.
如此一來,由於在摻雜完成時,N型深井區31中邊緣部311之N型摻質濃度被控制在大於中間部312之N型摻質濃度濃度,因此,在經過長時間熱製程造成的熱擴散效應後,深井區31之邊緣部311之N型摻質濃度將可因擴散而降低至與中間部312之N型摻質濃度的水準,最好是讓第一摻雜區36的P型摻質與深井區31的N型摻質之濃度比值在邊緣部311與中間部312間之相對百分偏差(percentage difference)變異度小於或等於5%。如此一來,便可有效改善習用手段缺失,達到提昇崩潰電壓的功效增進,而且還可以搭配申請案號為 100130576之”高壓金氧半導體電晶體元件及其製作方法”的技術手段一起使用,如此將可達到更好的效果。 As a result, since the N-type dopant concentration of the edge portion 311 in the N-type deep well region 31 is controlled to be greater than the N-type dopant concentration concentration of the intermediate portion 312 at the completion of doping, it is caused by a long heat process. After the thermal diffusion effect, the N-type dopant concentration of the edge portion 311 of the deep well region 31 may be lowered by diffusion to a level corresponding to the N-type dopant concentration of the intermediate portion 312, preferably the first doped region 36 The concentration ratio of the P-type dopant to the N-type dopant of the deep well region 31 is less than or equal to 5% of the relative difference between the edge portion 311 and the intermediate portion 312. In this way, the lack of conventional means can be effectively improved, and the effect of improving the breakdown voltage can be improved, and the application number can also be matched. The technical means of the "high-voltage MOS transistor crystal element and its manufacturing method" of 100130576 are used together, so that a better effect can be achieved.
而如何於摻雜完成時將N型深井區31中邊緣部311之N型摻質濃度控制在大於中間部312之N型摻質濃度之狀況,本案提出下列幾種作法:第一種作法,就是可利用兩道遮罩來進行N型摻質之植入,其中第一遮罩係具有一開口來進行出N型摻質植入而定義出深井區31,然後再利用第二遮罩之開口來露出邊緣部311而進行第二次的N型摻質植入,如此將可使得邊緣部311之N型摻質濃度大於中間部312之N型摻質濃度。第二種作法,就是利用如圖4中所示之遮罩40來進行一次N型摻質之植入,其中遮罩之開口41係完全露出邊緣部311但於中間部312則設置有柵欄狀條狀物42,如此一來,在進行完N型摻質植入後,中間部312中將有部份區域未能植入N型摻質,如此也可以使得邊緣部311之N型摻質濃度大於中間部312之N型摻質濃度。至於第三種作法,就是將以漸層式遮罩(gradient mask)來進行一次N型摻質之植入,其中漸層式遮罩邊緣之網點密度較低,越往中間之網點密度較高,如此一來,在進行完N型摻質植入後,也可以使得邊緣部311之N型摻質濃度大於中間部312之N型摻質濃度。 How to control the N-type dopant concentration of the edge portion 311 in the N-type deep well region 31 to be greater than the N-type dopant concentration in the intermediate portion 312 when the doping is completed, the following several methods are proposed in the present case: the first method, That is, the implantation of the N-type dopant can be performed by using two masks, wherein the first mask has an opening for N-type dopant implantation to define the deep well region 31, and then the second mask is used. The opening is exposed to expose the edge portion 311 for the second N-type dopant implantation, such that the N-type dopant concentration of the edge portion 311 is greater than the N-type dopant concentration of the intermediate portion 312. The second method is to perform an N-type dopant implantation using the mask 40 as shown in FIG. 4, wherein the opening 41 of the mask completely exposes the edge portion 311 but the intermediate portion 312 is provided with a fence shape. The strip 42 is such that after the N-type dopant implantation is completed, a portion of the intermediate portion 312 is not implanted with the N-type dopant, so that the N-type dopant of the edge portion 311 can also be made. The concentration is greater than the N-type dopant concentration of the intermediate portion 312. As for the third method, an N-type dopant implantation is performed with a gradient mask, wherein the density of the dots of the gradient mask edge is lower, and the density of the dots toward the middle is higher. In this way, after the N-type dopant implantation is performed, the N-type dopant concentration of the edge portion 311 can be made larger than the N-type dopant concentration of the intermediate portion 312.
另外,將第一摻雜區36的P型摻質與深井區31的N型摻質之濃度比值在邊緣部311與中間部312間之變異度控制在小於或等於5%之方式還有下列方法。主要是在不對N型深井區31中邊緣部311之N型摻質進行濃度調整的狀況下,改對第一摻雜區36中的P型摻質濃度來進行調整,也就是將屬於邊緣部311範圍內第一摻雜區36的P型摻質濃度調低,而將屬於中間部312範圍內第一摻雜區36的P型摻質濃度調高。 其作法也有下列幾種變化:第一種作法,就是可利用兩道遮罩來進行第一摻雜區36的P型摻質之植入,其中第一遮罩係具有一開口來露出所有的第一摻雜區36並進行出P型摻質植入,然後再利用第二遮罩之開口來露出中間部312而進行第二次的P型摻質植入,如此將可使得中間部312範圍內之第一摻雜區36的P型摻質濃度大於邊緣部311範圍內之第一摻雜區36的P型摻質濃度。第二種作法,就是利用如圖5中所示之遮罩50來進行一次P型摻質之植入,遮罩中屬於中間部312範圍內之開口51係完全露出第一摻雜區36,但屬於邊緣部311範圍內之開口52則為柵欄狀,如此也可使得中間部312範圍內之第一摻雜區36的P型摻質濃度大於邊緣部311範圍內之第一摻雜區36的P型摻質濃度。至於第三種作法,也就是將以漸層式遮罩(gradient mask)來進行一次P型摻質之植入,其中漸層式遮罩中間部開口中之網點密度較低,越往邊緣之開口中網點密度較高,如此一來,在進行完P型摻質植入後,也可以使得中間部312範圍內之第一摻雜區36的P型摻質濃度大於邊緣部311範圍內之第一摻雜區36的P型摻質濃度。而由於摻雜完成之第一摻雜區36並不會像深井區31中N型摻質會因熱製程而較易擴散逸失,因此在經過長時間熱製程造成的熱擴散效應後,深井區31之邊緣部311之N型摻質濃度將可因擴散而降低,剛好與讓邊緣部311範圍中第一摻雜區36中濃度較低的P型摻質匹配,因此濃度比值在邊緣部311與中間部312間之變異度仍可控制在小於或等於5%。 In addition, the ratio of the concentration ratio of the P-type dopant of the first doping region 36 to the N-type dopant of the deep well region 31 between the edge portion 311 and the intermediate portion 312 is controlled to be less than or equal to 5%. method. The adjustment is mainly performed on the P-type dopant concentration in the first doping region 36 without adjusting the concentration of the N-type dopant in the edge portion 311 of the N-type deep well region 31, that is, it belongs to the edge portion. The P-type dopant concentration of the first doped region 36 in the range of 311 is lowered, and the P-type dopant concentration of the first doped region 36 belonging to the intermediate portion 312 is increased. The method also has the following changes: In the first method, the implantation of the P-type dopant of the first doping region 36 can be performed by using two masks, wherein the first mask has an opening to expose all of the The first doped region 36 is implanted with a P-type dopant, and then the opening of the second mask is used to expose the intermediate portion 312 for a second P-type dopant implantation, such that the intermediate portion 312 can be made The P-type dopant concentration of the first doped region 36 within the range is greater than the P-type dopant concentration of the first doped region 36 within the range of the edge portion 311. In the second method, a P-type dopant is implanted by using the mask 50 as shown in FIG. 5, and the opening 51 in the mask belonging to the middle portion 312 completely exposes the first doping region 36. However, the opening 52 in the range of the edge portion 311 is a fence shape, so that the P-type dopant concentration of the first doping region 36 in the range of the intermediate portion 312 is greater than the first doping region 36 in the range of the edge portion 311. P-type dopant concentration. As for the third method, a P-type dopant implantation is performed with a gradient mask, wherein the density of the dots in the opening of the intermediate layer of the gradient mask is lower, and the edge is higher. The dot density in the opening is relatively high, so that the P-type dopant concentration of the first doping region 36 in the range of the intermediate portion 312 can be made larger than the edge portion 311 after the P-type dopant implantation is performed. The P-type dopant concentration of the first doped region 36. However, since the first doping region 36 which is doped is not like the N-type dopant in the deep well region 31, it is more likely to diffuse and escape due to the thermal process, so after the thermal diffusion effect caused by the long-time thermal process, the deep well region The N-type dopant concentration of the edge portion 311 of 31 will be lowered by diffusion, just matching the P-type dopant having a lower concentration in the first doping region 36 in the range of the edge portion 311, and thus the concentration ratio is at the edge portion 311. The degree of variability with the intermediate portion 312 can still be controlled to be less than or equal to 5%.
綜上所述,本發明利用對摻雜濃度之調整而減少了元件完成後之濃度比值的不均勻,進而改善習用手段中M形HV MOSFET元件之崩潰電壓不足的現象。 In summary, the present invention utilizes the adjustment of the doping concentration to reduce the unevenness of the concentration ratio after the completion of the component, thereby improving the phenomenon of insufficient breakdown voltage of the M-shaped HV MOSFET device in the conventional device.
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,任何熟習此技藝者,在不脫離本發明之精神和範圍內,當可作些許之更動與潤飾,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。 While the present invention has been described in its preferred embodiments, the present invention is not intended to limit the invention, and the present invention may be modified and modified without departing from the spirit and scope of the invention. The scope of protection is subject to the definition of the scope of the patent application.
1‧‧‧基底 1‧‧‧Base
11‧‧‧深井區 11‧‧‧Shenjing District
111‧‧‧深井區之邊緣部 111‧‧‧The edge of the deep well area
112‧‧‧深井區之中間部 112‧‧‧The middle part of the deep well area
12‧‧‧源極/基體區 12‧‧‧Source/base area
13‧‧‧汲極區 13‧‧‧Bungee Area
14‧‧‧通道區 14‧‧‧Channel area
15‧‧‧閘極結構 15‧‧‧ gate structure
16‧‧‧第一摻雜區 16‧‧‧First doped area
17‧‧‧高壓井區 17‧‧‧High-pressure well area
19‧‧‧絕緣層 19‧‧‧Insulation
3‧‧‧基底 3‧‧‧Base
31‧‧‧深井區 31‧‧‧Shenjing District
311‧‧‧深井區之邊緣部 311‧‧‧The edge of the deep well area
312‧‧‧深井區之中間部 312‧‧‧The middle part of the Sham Tseng District
32‧‧‧源極/基體區 32‧‧‧Source/base area
320‧‧‧高壓井區 320‧‧‧High-pressure well area
321‧‧‧基體接觸區 321‧‧‧Body contact area
322‧‧‧源極接觸區 322‧‧‧Source contact area
33‧‧‧汲極區 33‧‧‧Bungee Area
330‧‧‧漂移區 330‧‧‧Drift area
331‧‧‧汲極接觸區 331‧‧‧汲polar contact area
34‧‧‧通道區 34‧‧‧Channel area
35‧‧‧閘極結構 35‧‧‧ gate structure
350‧‧‧閘極介電層 350‧‧ ‧ gate dielectric layer
351‧‧‧閘極導體層 351‧‧‧ gate conductor layer
352‧‧‧絕緣層 352‧‧‧Insulation
353‧‧‧場電極結構 353‧‧‧Field electrode structure
36‧‧‧第一摻雜區 36‧‧‧First doped area
40‧‧‧遮罩 40‧‧‧ mask
41‧‧‧開口 41‧‧‧ openings
42‧‧‧柵欄狀條狀物 42‧‧‧Fence bars
50‧‧‧遮罩 50‧‧‧ mask
51‧‧‧開口 51‧‧‧ openings
52‧‧‧柵欄狀開口 52‧‧‧Fenced opening
圖1:其係HV MOSFET元件之剖面示意圖。 Figure 1: Schematic diagram of a HV MOSFET component.
圖2:其係顯示深井區原本均勻分佈之N型摻質之濃度經過長時間熱製程造成的熱擴散效應後所形成之濃度分佈示意圖。 Figure 2: It is a schematic diagram showing the concentration distribution formed by the concentration of the N-type dopant in the deep well area after a long-term thermal process.
圖3A至圖3C:顯示本案所發展出來之一種形成HV MOSFET元件的方法之示意圖。 3A to 3C are schematic views showing a method of forming an HV MOSFET device developed in the present invention.
圖4顯示一種應用於本案之遮罩的示意圖。 Figure 4 shows a schematic view of a mask applied to the present case.
圖5顯示另一種應用於本案之遮罩的示意圖。 Figure 5 shows a schematic view of another mask applied to the present case.
3‧‧‧基底 3‧‧‧Base
31‧‧‧深井區 31‧‧‧Shenjing District
32‧‧‧源極/基體區 32‧‧‧Source/base area
320‧‧‧高壓井區 320‧‧‧High-pressure well area
321‧‧‧源極接觸區 321‧‧‧Source contact area
322‧‧‧基體接觸區 322‧‧‧Body contact area
33‧‧‧汲極區 33‧‧‧Bungee Area
330‧‧‧漂移區 330‧‧‧Drift area
331‧‧‧汲極接觸區 331‧‧‧汲polar contact area
34‧‧‧通道區 34‧‧‧Channel area
35‧‧‧閘極結構 35‧‧‧ gate structure
350‧‧‧閘極介電層 350‧‧ ‧ gate dielectric layer
351‧‧‧閘極導體層 351‧‧‧ gate conductor layer
352‧‧‧絕緣層 352‧‧‧Insulation
353‧‧‧場電極結構 353‧‧‧Field electrode structure
36‧‧‧第一摻雜區 36‧‧‧First doped area
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