TWI584476B - High voltage metal-oxide-semiconductor transistor device and method of fabricating the same - Google Patents

High voltage metal-oxide-semiconductor transistor device and method of fabricating the same Download PDF

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TWI584476B
TWI584476B TW100130576A TW100130576A TWI584476B TW I584476 B TWI584476 B TW I584476B TW 100130576 A TW100130576 A TW 100130576A TW 100130576 A TW100130576 A TW 100130576A TW I584476 B TWI584476 B TW I584476B
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electric field
high voltage
deep well
doping
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TW201310642A (en
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王智充
徐尉倫
黃善禧
林克峰
吳德源
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聯華電子股份有限公司
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高壓金氧半導體電晶體元件及其製作方法High-voltage MOS semiconductor transistor component and manufacturing method thereof

本發明係關於一種高壓金氧半導體電晶體元件及其製作方法,尤指一種M形之高壓金氧半導體電晶體元件及其製作方法。The invention relates to a high voltage metal oxide semiconductor transistor component and a manufacturing method thereof, in particular to an M-shaped high voltage metal oxide semiconductor transistor component and a manufacturing method thereof.

高壓金氧半導體(high voltage metal-oxide-semiconductor,HV MOS)電晶體元件因可同時承受一般電力系統所提供之高電壓以及具有開關的特性,故已被廣地應用在中央處理器電源供應(CPU power supply)、電管理系統(power management system)、直流/交流轉換器(AC/DC converter)、LCD與電漿電視驅動器、車用電子、電腦週邊、小尺寸直流馬達控制器、以及消費性電子產品等領域。High voltage metal-oxide-semiconductor (HV MOS) transistor components have been widely used in central processor power supplies because they can withstand the high voltages provided by general power systems and have switching characteristics. CPU power supply), power management system, AC/DC converter, LCD and plasma TV drivers, automotive electronics, computer peripherals, small DC motor controllers, and consumer Electronic products and other fields.

習知HV MOS電晶體元件係為一圓形元件,亦即其汲極之上視圖案為圓形,而其源極之上視圖案則為圓環形狀,使源極以汲極之圓心為圓心,環繞汲極。並且,HV MOS電晶體元件之汲極一般電性連接至電源之高電壓端,例如800伏特或以上,因此汲極與源極之間設置有耐壓結構,以提高HV MOS電晶體元件之崩潰電壓,使HV MOS電晶體元件在高電壓環境下仍可正常運作。The conventional HV MOS transistor component is a circular component, that is, the top view of the drain is circular, and the top view of the source is a ring shape, so that the source is centered on the bottom of the bungee. Center of the circle, around the bungee. Moreover, the drain of the HV MOS transistor component is generally electrically connected to the high voltage terminal of the power source, for example, 800 volts or more, so that a withstand voltage structure is provided between the drain and the source to improve the collapse of the HV MOS transistor component. The voltage allows the HV MOS transistor components to operate normally in high voltage environments.

由於圓形HV MOS電晶體元件之通道寬度係由源極與汲極之間的圓環區域之圓周長來決定,因此若欲提高HV MOS電晶體元件之導通電流,則需加大圓形HV MOS電晶體元件之半徑,但亦大幅地增加了HV MOS電晶體元件之面積。為了同時增加HV MOS電晶體元件之導通電流且達到最小化HV MOS電晶體元件之面積,已發展出跑道形HV MOS電晶體元件與M形HV MOS電晶體元件。Since the channel width of the circular HV MOS transistor component is determined by the circumferential length of the annular region between the source and the drain, if the on-current of the HV MOS transistor component is to be increased, the circular HV needs to be increased. The radius of the MOS transistor component, but also greatly increases the area of the HV MOS transistor component. In order to simultaneously increase the on-current of the HV MOS transistor element and minimize the area of the HV MOS transistor element, a racetrack-shaped HV MOS transistor element and an M-shaped HV MOS transistor element have been developed.

然而,習知M形HV MOS電晶體元件之崩潰電壓係小於圓形HV MOS電晶體元件之崩潰電壓,因此當將圓形HV MOS電晶體元件、跑道形HV MOS電晶體元件以及M形HV MOS電晶體元件同時整合於同一積體電路晶片中時,會受限於M形HV MOS電晶體元件之崩潰電壓,而降低整體積體電路晶片之耐壓能力。However, the breakdown voltage of the conventional M-shaped HV MOS transistor element is smaller than the breakdown voltage of the circular HV MOS transistor element, so when a circular HV MOS transistor element, a racetrack HV MOS transistor element, and an M-shaped HV MOS are used When the transistor elements are simultaneously integrated into the same integrated circuit chip, the breakdown voltage of the M-shaped HV MOS transistor element is limited, and the withstand voltage capability of the whole bulk circuit chip is reduced.

有鑑於此,提升M形HV MOS電晶體元件之崩潰電壓且最佳化整合有M形HV MOS電晶體元件與圓形HV MOS電晶體元件之晶片的崩潰電壓實為業界極力達成之目標。In view of this, it is an industry-wide goal to increase the breakdown voltage of the M-shaped HV MOS transistor element and optimize the breakdown voltage of the chip in which the M-shaped HV MOS transistor element and the circular HV MOS transistor element are integrated.

本發明之目的之一在於提供一種高壓金氧半導體(high voltage metal-oxide-semiconductor,HV MOS)電晶體元件及其製作方法,以提升M形HV MOS電晶體元件之崩潰電壓,進而最佳化整合有M形HV MOS電晶體元件與圓形HV MOS電晶體元件之晶片的崩潰電壓。One of the objects of the present invention is to provide a high voltage metal-oxide-semiconductor (HV MOS) transistor component and a method for fabricating the same, which are to improve the breakdown voltage of the M-shaped HV MOS transistor component and optimize it. A breakdown voltage of a wafer integrated with an M-shaped HV MOS transistor element and a circular HV MOS transistor element.

為達上述之目的,本發明提供一種HV MOS電晶體元件,其包括一基底、一深井區、一第一摻雜區、一高壓井區、一第二摻雜區、一第三摻雜區、一閘極結構以及一第四摻雜區。基底具有一第一導電類型,且基底具有至少一電場集中區。深井區設於基底中,且具有不同於第一導電類型之一第二導電類型。第一摻雜區設於深井區中,其中位於電場集中區中之第一摻雜區之摻雜濃度與深井區之摻雜濃度具有一第一比值,位於電場集中區之外的第一摻雜區之摻雜濃度與深井區之摻雜濃度具有一第二比值,且第一比值大於第二比值。高壓井區設於基底中,且具有第一導電類型。第二摻雜區設於深井區中,且具有該第二導電類型,其中第一摻雜區位於第二摻雜區與高壓井區之間。第三摻雜區設於高壓井區中,且具有第二導電類型,其中電場集中區圍繞部份第三摻雜區。閘極結構設於第一摻雜區與第三摻雜區之間的高壓井區上。第四摻雜區設於高壓井區中,且具有第一導電類型。To achieve the above objective, the present invention provides a HV MOS transistor device including a substrate, a deep well region, a first doped region, a high voltage well region, a second doped region, and a third doped region. a gate structure and a fourth doped region. The substrate has a first conductivity type and the substrate has at least one electric field concentration region. The deep well region is disposed in the substrate and has a second conductivity type different from one of the first conductivity types. The first doping region is disposed in the deep well region, wherein the doping concentration of the first doping region in the electric field concentration region has a first ratio to the doping concentration of the deep well region, and the first doping outside the electric field concentration region The doping concentration of the impurity region has a second ratio to the doping concentration of the deep well region, and the first ratio is greater than the second ratio. The high voltage well region is disposed in the substrate and has a first conductivity type. The second doped region is disposed in the deep well region and has the second conductivity type, wherein the first doped region is located between the second doped region and the high voltage well region. The third doped region is disposed in the high voltage well region and has a second conductivity type, wherein the electric field concentration region surrounds a portion of the third doped region. The gate structure is disposed on the high voltage well region between the first doped region and the third doped region. The fourth doped region is disposed in the high voltage well region and has a first conductivity type.

為達上述之目的,本發明提供一種HV MOS電晶體元件之製作方法。首先,提供一基底,基底具有一第一導電類型,且基底具有至少一電場集中區。接著,於基底中形成一深井區,且深井區具有不同於第一導電類型之一第二導電類型。然後,於深井區中形成一第一摻雜區,且第一摻雜區具有第一導電類型,其中位於電場集中區中之第一摻雜區之摻雜濃度與深井區之摻雜濃度具有一第一比值,位於電場集中區之外的第一摻雜區之摻雜濃度與深井區之摻雜濃度具有一第二比值,且第一比值大於第二比值。隨後,於基底中形成一高壓井區,並分別於深井區與高壓井區中形成一第二摻雜區與一第三摻雜區,高壓井區具有第一導電類型,且第二摻雜區與第三摻雜區具有第二導電類型,其中第一摻雜區位於第二摻雜區與高壓井區之間,且電場集中區圍繞部份第三摻雜區。To achieve the above object, the present invention provides a method of fabricating a HV MOS transistor. First, a substrate is provided, the substrate having a first conductivity type, and the substrate having at least one electric field concentration region. Next, a deep well region is formed in the substrate, and the deep well region has a second conductivity type that is different from one of the first conductivity types. Then, a first doped region is formed in the deep well region, and the first doped region has a first conductivity type, wherein the doping concentration of the first doped region in the electric field concentration region and the doping concentration of the deep well region have A first ratio, the doping concentration of the first doping region outside the electric field concentration region has a second ratio to the doping concentration of the deep well region, and the first ratio is greater than the second ratio. Subsequently, a high-pressure well region is formed in the substrate, and a second doping region and a third doping region are formed in the deep well region and the high-voltage well region, respectively, the high-voltage well region has a first conductivity type, and the second doping The region and the third doped region have a second conductivity type, wherein the first doped region is between the second doped region and the high voltage well region, and the electric field concentration region surrounds a portion of the third doped region.

本發明之M形HV MOS電晶體元件的崩潰電壓藉由調整位於電場集中區中之第一摻雜區之摻雜濃度與深井區之摻雜濃度的第一比值至大於位於電場集中區之外的第一摻雜區之摻雜濃度與深井區之摻雜濃度的第二比值而可增加,因此同時整合有M形HV MOS電晶體元件與圓形HV MOS電晶體元件之晶片的崩潰電壓可被有效提升。The breakdown voltage of the M-shaped HV MOS transistor device of the present invention is adjusted by adjusting a first ratio of a doping concentration of the first doping region in the electric field concentration region to a doping concentration of the deep well region to be greater than being located outside the electric field concentration region The second ratio of the doping concentration of the first doping region to the doping concentration of the deep well region may be increased, so that the breakdown voltage of the wafer in which the M-shaped HV MOS transistor component and the circular HV MOS transistor component are integrated may be Was effectively improved.

為使熟習本發明所屬技術領域之一般技藝者能更進一步了解本發明,下文特列舉本發明之具體較佳實施例,並配合所附圖式,仔細說明本發明的構成內容及所欲達成之功效。The present invention will be further understood by the following detailed description of the preferred embodiments of the invention, efficacy.

請參考第1圖與第2圖,第1圖為本發明一較佳實施例之高壓金氧半導體(high voltage metal-oxide-semiconductor,HV MOS)電晶體元件之上視示意圖,且第2圖為沿著第1圖之剖面線AA’之剖面示意圖。如第1圖與第2圖所示,HV MOS電晶體元件100係製作於一基底102上,例如矽基底,且基底102具有一第一導電類型。HV MOS電晶體元件100包括一第一絕緣層104、一深井區106、一漂移區108、一第一摻雜區110、一高壓井區112、一第二摻雜區114、一第三摻雜區116、一閘極結構118以及一第四摻雜區120。深井區106、第二摻雜區114與第三摻雜區116具有不同於第一導電類型之一第二導電類型,且第一摻雜區110、高壓井區112以及第四摻雜區120具有第一導電類型。本實施例之第一導電類型與第二導電類型分別為P型與N型,但本發明不限於此,亦可互換。Please refer to FIG. 1 and FIG. 2 . FIG. 1 is a top view of a high voltage metal-oxide-semiconductor (HV MOS) transistor component according to a preferred embodiment of the present invention, and FIG. It is a schematic cross-sectional view along the section line AA' of Fig. 1. As shown in FIGS. 1 and 2, the HV MOS transistor device 100 is fabricated on a substrate 102, such as a germanium substrate, and the substrate 102 has a first conductivity type. The HV MOS transistor component 100 includes a first insulating layer 104, a deep well region 106, a drift region 108, a first doped region 110, a high voltage well region 112, a second doped region 114, and a third doped region. The impurity region 116, a gate structure 118, and a fourth doping region 120. The deep well region 106, the second doping region 114 and the third doping region 116 have a second conductivity type different from the first conductivity type, and the first doping region 110, the high voltage well region 112, and the fourth doping region 120 Has a first conductivity type. The first conductivity type and the second conductivity type of the embodiment are respectively P-type and N-type, but the invention is not limited thereto and may be interchanged.

於本實施例中,N型深井區106設於P型基底102中,且用以作為HV MOS電晶體元件100之汲極。第一絕緣層104設於P型基底102上,用以定義N型深井區106之位置。N型漂移區108設於N型深井區106中。N型第二摻雜區114設於N型漂移區108中,且N型第二摻雜區114具有複數個突出部121朝同一方向延伸且彼此平行,使任兩相鄰突出部121之間有一凹口122。藉此,N型第二摻雜區114係為一M形結構或梳子形結構,且可以將N型深井區106電性連接至一汲極金屬層,使電源所產生之高電壓可藉由汲極金屬層輸入至N型深井區106。P型高壓井區112設於N型深井區106中,且N型深井區106包圍P型高壓井區112。並且,P型高壓井區112沿著具有M形結構之N型第二摻雜區114的周圍環繞N型第二摻雜區114,而具有M形環狀結構,並用以作為HV MOS電晶體元件100之基極。N型第三摻雜區116設於P型高壓井區112中,且用以作為HV MOS電晶體元件100之源極。N型第三摻雜區116圍繞N型第二摻雜區114,並具有與P型高壓井區112相同之M形環狀結構。P型第四摻雜區120設於P型高壓井區112中,並圍繞N型第三摻雜區114,用以將作為HV MOS電晶體元件100之基極的P型高壓井區112電性連接至外界。閘極結構118設於P型第一摻雜區110與N型第三摻雜區116之間的P型高壓井區112上,用以作為HV MOS電晶體元件100之閘極。P型第一摻雜區110設於N型第二摻雜區114與P型高壓井區112之間的N型深井區106中,並圍繞N型第二摻雜區114,可提高介於N型第二摻雜區114與P型高壓井區112間之N型深井區106之耐壓能力,以避免N型深井區106因過高電壓而產生崩潰。由此可知,本實施例之HV MOS電晶體元件100係為具有複數個凹口122之M形元件或梳子形元件,但本發明之HV MOS電晶體元件100並不限具有複數個凹口122,而亦可具有至少一個凹口122。 In the present embodiment, the N-type deep well region 106 is disposed in the P-type substrate 102 and serves as the drain of the HV MOS transistor element 100. A first insulating layer 104 is disposed on the P-type substrate 102 to define the location of the N-type deep well region 106. The N-type drift region 108 is disposed in the N-type deep well region 106. The N-type second doping region 114 is disposed in the N-type drift region 108, and the N-type second doping region 114 has a plurality of protrusions 121 extending in the same direction and parallel to each other, so that between any two adjacent protrusions 121 There is a notch 122. Thereby, the N-type second doping region 114 is an M-shaped structure or a comb-shaped structure, and the N-type deep well region 106 can be electrically connected to a drain metal layer, so that the high voltage generated by the power source can be The drain metal layer is input to the N-type deep well region 106. The P-type high pressure well region 112 is disposed in the N-type deep well region 106, and the N-type deep well region 106 surrounds the P-type high pressure well region 112. Moreover, the P-type high-voltage well region 112 surrounds the N-type second doping region 114 along the N-type second doping region 114 having an M-shaped structure, and has an M-shaped annular structure and is used as an HV MOS transistor. The base of component 100. The N-type third doping region 116 is disposed in the P-type high voltage well region 112 and serves as a source of the HV MOS transistor element 100. The N-type third doped region 116 surrounds the N-type second doped region 114 and has the same M-shaped annular structure as the P-type high voltage well region 112. The P-type fourth doping region 120 is disposed in the P-type high voltage well region 112 and surrounds the N-type third doping region 114 for electrically charging the P-type high voltage well region 112 which is the base of the HV MOS transistor component 100. Sexual connection to the outside world. The gate structure 118 is disposed on the P-type high voltage well region 112 between the P-type first doping region 110 and the N-type third doping region 116 to serve as a gate of the HV MOS transistor component 100. The P-type first doping region 110 is disposed in the N-type deep well region 106 between the N-type second doping region 114 and the P-type high-voltage well region 112, and surrounds the N-type second doping region 114 to improve the The withstand voltage capability of the N-type deep well region 106 between the N-type second doped region 114 and the P-type high-pressure well region 112 prevents the N-type deep well region 106 from collapsing due to excessive voltage. It can be seen that the HV MOS transistor element 100 of the present embodiment is an M-shaped element or a comb-shaped element having a plurality of notches 122, but the HV MOS transistor element 100 of the present invention is not limited to having a plurality of notches 122. It is also possible to have at least one notch 122.

此外,基底102具有複數個電場集中區124定義於其上,其中各電場集中區124係位於N型第二摻雜區114與P型高壓井區112之間,且位於各凹口122之底部區域。電場集中區124係位於N型深井區106的一部分。並且,各電場集中區124係為一半圓弧形區域,並圍繞部份N型第三摻雜區116。本發明之電場集中區124之數量係依據凹口122之數量而定,因此基底102不限具有複數個電場集中區124,而可具有至少一個電場集中區124。於本實施例中,位於各電場集中區124中之P型第一摻雜區110之摻雜濃度與N型深井區106之摻雜濃度具有一第一比值,且位於各電場集中區124之外的P型第一摻雜區110之摻雜濃度與N型深井區106之摻雜濃度具有一第二比值。並且,位於各電場集中區124中之N型深井區106之摻雜濃度小於位於各電場集中區124之外之N型深井區106之摻 雜濃度,使第一比值大於第二比值。於本實施例中,位於各電場集中區124中之P型第一摻雜區110之摻雜濃度需搭配位於各電場集中區124中之N型深井區106之摻雜濃度來做相對應之調整,以具有適當之第一比值,使HV MOS電晶體元件100可達到所欲之操作功效。並且,本實施例位於各電場集中區124中之N型深井區106之摻雜濃度係隨著越接近P型第一摻雜區110之二側而越小。換言之,位於各電場集中區124中,鄰近各電場集中區124之內側與外側之N型深井區106之摻雜濃度係大於位於遠離各電場集中區124之內側與外側之N型深井區106之摻雜濃度,且越鄰近各電場集中區124之內側與外側,N型深井區106之摻雜濃度越小,但本發明不限於此。於本發明其他實施例中,位於各電場集中區124中之N型深井區106的摻雜濃度可僅隨著越鄰近各電場集中區124之內側而越小,或僅隨著越鄰近各電場集中區124之外側而越小。或者,位於各電場集中區124中之N型深井區106的摻雜濃度亦可不具有梯度變化。 In addition, the substrate 102 has a plurality of electric field concentration regions 124 defined therein, wherein each of the electric field concentration regions 124 is located between the N-type second doping region 114 and the P-type high-pressure well region 112, and is located at the bottom of each of the notches 122. region. The electric field concentration region 124 is located in a portion of the N-type deep well region 106. Moreover, each of the electric field concentration regions 124 is a semi-circular arc-shaped region and surrounds a portion of the N-type third doping region 116. The number of electric field concentration regions 124 of the present invention is determined by the number of recesses 122. Therefore, the substrate 102 is not limited to have a plurality of electric field concentration regions 124, but may have at least one electric field concentration region 124. In this embodiment, the doping concentration of the P-type first doping region 110 in each of the electric field concentration regions 124 has a first ratio with the doping concentration of the N-type deep well region 106, and is located in each electric field concentration region 124. The doping concentration of the outer P-type first doping region 110 has a second ratio to the doping concentration of the N-type deep well region 106. Moreover, the doping concentration of the N-type deep well region 106 located in each electric field concentration region 124 is smaller than that of the N-type deep well region 106 located outside each electric field concentration region 124. The impurity concentration is such that the first ratio is greater than the second ratio. In this embodiment, the doping concentration of the P-type first doping region 110 located in each of the electric field concentration regions 124 is matched with the doping concentration of the N-type deep well region 106 located in each of the electric field concentration regions 124. Adjusting to have a suitable first ratio allows the HV MOS transistor component 100 to achieve the desired operational efficiency. Moreover, the doping concentration of the N-type deep well region 106 in each of the electric field concentration regions 124 of the present embodiment is smaller as it approaches the two sides of the P-type first doping region 110. In other words, in each of the electric field concentration regions 124, the doping concentration of the N-type deep well region 106 adjacent to the inner side and the outer side of each electric field concentration region 124 is greater than that of the N-type deep well region 106 located far from the inner and outer sides of each electric field concentration region 124. The doping concentration, and the closer to the inner side and the outer side of each electric field concentration region 124, the smaller the doping concentration of the N-type deep well region 106, but the present invention is not limited thereto. In other embodiments of the present invention, the doping concentration of the N-type deep well region 106 located in each of the electric field concentration regions 124 may be smaller as it is closer to the inner side of each electric field concentration region 124, or only the more adjacent electric fields. The outer side of the concentration area 124 is smaller. Alternatively, the doping concentration of the N-type deep well region 106 located in each of the electric field concentration regions 124 may not have a gradient change.

值得一提的是,當HV MOS電晶體元件100導通時,電性連接至高電壓之N型第二摻雜區114與作為源極之N型第三摻雜區116之間會產生高電場,且電場方向從N型第二摻雜區114指向N型第三摻雜區116。由於各電場集中區124為半圓弧形區域,因此各電場集中區124之外側長度係大於各電場集中區124之內側長度,使各電場集中區124中之電場會從各電場集中區124之外側向各電場集中區124之內側聚集,如第1圖之箭頭所示。由此可知,位於各 電場集中區124中之P型第一摻雜區110與N型深井區106較位於各電場集中區124之外之P型第一摻雜區110與N型深井區106承受較高電壓密度。本實施例之HV MOS電晶體元件100係藉由調整第一比值大於第二比值提升於各電場集中區124中之P型第一摻雜區110與N型深井區106之耐壓能力,以避免各電場集中區124中之P型第一摻雜區110與N型深井區106因HV MOS電晶體元件100通以過高之電壓而先產生崩潰,並且可同時提升HV MOS電晶體元件100之崩潰電壓。於本實施例中,位於各電場集中區124中之N型深井區106之摻雜濃度亦可隨著越接近P型高壓井區112越小,以藉由於各電場集中區124中電場聚集越密集之N型深井區106中摻雜濃度較淡之濃度來提升崩潰電壓。 It is worth mentioning that when the HV MOS transistor element 100 is turned on, a high electric field is generated between the N-type second doping region 114 electrically connected to the high voltage and the N-type third doping region 116 as the source. And the electric field direction is directed from the N-type second doping region 114 to the N-type third doping region 116. Since each of the electric field concentration regions 124 is a semi-circular arc-shaped region, the length of the outer side of each electric field concentration region 124 is greater than the inner length of each electric field concentration region 124, so that the electric field in each electric field concentration region 124 is from the outer side of each electric field concentration region 124. The inner side of each electric field concentration area 124 is gathered as shown by the arrow in Fig. 1. It can be seen that each is located The P-type first doped region 110 and the N-type deep well region 106 in the electric field concentration region 124 are subjected to a higher voltage density than the P-type first doped region 110 and the N-type deep well region 106 located outside the respective electric field concentration regions 124. The HV MOS transistor element 100 of the present embodiment is improved in the withstand voltage capability of the P-type first doping region 110 and the N-type deep well region 106 in each of the electric field concentration regions 124 by adjusting the first ratio to be greater than the second ratio. It is avoided that the P-type first doping region 110 and the N-type deep well region 106 in each of the electric field concentration regions 124 first collapse due to the excessive voltage of the HV MOS transistor element 100, and the HV MOS transistor element 100 can be simultaneously lifted. The breakdown voltage. In this embodiment, the doping concentration of the N-type deep well region 106 located in each of the electric field concentration regions 124 may also be smaller as it is closer to the P-type high-pressure well region 112, so that the electric field is concentrated in each of the electric field concentration regions 124. The dense N-type deep well region 106 has a lighter doping concentration to increase the breakdown voltage.

另外,HV MOS電晶體元件100另包括一第二絕緣層126以及複數個場電極128。第二絕緣層126設於P型第一摻雜區110上,用於避免N型第二摻雜區116之高電壓破壞閘極結構118。場電極128設於第二絕緣層126上,且為浮接狀態,使場電極128可用於提升HV MOS電晶體元件110之崩潰電壓。 In addition, the HV MOS transistor component 100 further includes a second insulating layer 126 and a plurality of field electrodes 128. The second insulating layer 126 is disposed on the P-type first doping region 110 for preventing the high voltage of the N-type second doping region 116 from damaging the gate structure 118. The field electrode 128 is disposed on the second insulating layer 126 and is in a floating state, so that the field electrode 128 can be used to raise the breakdown voltage of the HV MOS transistor element 110.

請參考第3圖,第3圖為不同HV MOS電晶體元件位於電場集中區之外的P型第一摻雜區之摻雜濃度與N型深井區之摻雜濃度的第二比值與崩潰電壓之關係示意圖。如第3圖所示,第一關係曲線130係代表圓形HV MOS電晶體元件之第二比值與崩潰電壓之關係。第二關係曲線132代表在位於各電場集中區中之P型第一摻雜 區之摻雜濃度與N型深井區之摻雜濃度的第一比值與第二比值相同之情況下M形HV MOS電晶體元件之第二比值與崩潰電壓之關係。第三關係曲線134代表本實施例之M形HV MOS電晶體元件在第一比值大於第二比值之情況下第二比值與崩潰電壓之關係。比較第二關係曲線132與第三關係曲線134,於相同第二比值時,第三關係曲線134之崩潰電壓係大於第二關係曲線132之崩潰電壓。換句話說,當M形HV MOS電晶體元件之第一比值調整至大於第二比值時,第二關係曲線132會向上偏移,而成為第三關係曲線134。並且,值得注意的是,圓形HV MOS電晶體元件之第一關係曲線130之崩潰電壓會隨著第二比值增加而降低,但M形HV MOS電晶體元件之第二關係曲線132與第三關係曲線134之崩潰電壓會隨著第二比值增加而增加。因此,本實施例之M形HV MOS電晶體元件藉由調整第一比值至大於第二比值使崩潰電壓在相同的第二比值的情況下可被提升,並使第一關係曲線130與第三關係曲線134之交點的崩潰電壓大於第一關係曲線130與第二關係曲線134之交點的崩潰電壓。並且,第一關係曲線130與第三關係曲線134之交點的第二比值較第一關係曲線130與第二關係曲線132之交點的第二比值接近一基準值BL,藉此可避免因第二比值偏離基準值BL過大而造成HV MOS電晶體元件產生不正常運作。因此,同時整合有M形HV MOS電晶體元件與圓形HV MOS電晶體元件之晶片的崩潰電壓可被有效提升。 Please refer to FIG. 3, which is the second ratio and the breakdown voltage of the doping concentration of the P-type first doping region and the doping concentration of the N-type deep well region of different HV MOS transistor components outside the electric field concentration region. Schematic diagram of the relationship. As shown in FIG. 3, the first relationship curve 130 represents the relationship between the second ratio of the circular HV MOS transistor element and the breakdown voltage. The second relationship curve 132 represents a P-type first doping in each of the electric field concentration regions. The relationship between the second ratio of the M-shaped HV MOS transistor element and the breakdown voltage in the case where the first ratio of the doping concentration of the region to the doping concentration of the N-type deep well region is the same as the second ratio. The third relationship curve 134 represents the relationship between the second ratio and the breakdown voltage in the case where the first ratio is greater than the second ratio of the M-shaped HV MOS transistor element of the present embodiment. Comparing the second relationship curve 132 with the third relationship curve 134, when the same second ratio is used, the breakdown voltage of the third relationship curve 134 is greater than the breakdown voltage of the second relationship curve 132. In other words, when the first ratio of the M-shaped HV MOS transistor element is adjusted to be greater than the second ratio, the second relationship curve 132 is shifted upward to become the third relationship curve 134. Moreover, it is worth noting that the breakdown voltage of the first relationship curve 130 of the circular HV MOS transistor element decreases as the second ratio increases, but the second relationship curve 132 and the third of the M-shaped HV MOS transistor element The breakdown voltage of the relationship curve 134 will increase as the second ratio increases. Therefore, the M-shaped HV MOS transistor component of the embodiment can be raised by adjusting the first ratio to be greater than the second ratio so that the breakdown voltage is at the same second ratio, and the first relationship curve 130 and the third relationship are The collapse voltage at the intersection of the relationship curve 134 is greater than the collapse voltage at the intersection of the first relationship curve 130 and the second relationship curve 134. Moreover, the second ratio of the intersection of the first relationship curve 130 and the third relationship curve 134 is closer to a reference value BL than the second ratio of the intersection of the first relationship curve 130 and the second relationship curve 132, thereby avoiding the second ratio The ratio deviates too much from the reference value BL to cause the HV MOS transistor element to malfunction. Therefore, the breakdown voltage of the wafer in which the M-shaped HV MOS transistor element and the circular HV MOS transistor element are integrated can be effectively improved.

以下將進一步說明本實施例之HV MOS電晶體元件之製作方 法。請參考第4圖至第9圖,並一併參考第2圖。第4圖至第9圖為本發明較佳實施例之HV MOS電晶體元件之製作方法示意圖。如第4圖所示,首先提供P型基底102。然後,於P型基底102上形成一第一遮罩135以及複數個第二遮罩136,例如光阻遮罩。第一遮罩135定義出N型深井區106之位置,且第二遮罩136位於各電場集中區124中。隨後,對P型基底102全面性進行一第一離子佈植製程,於P型基底102中佈植N型離子。如第5圖所示,本實施例之各第二遮罩136係為一圓弧狀遮罩,且各第二遮罩136圍繞各電場集中區124之內側,並從各電場集中區124之內側依序排列至各電場集中區124之外側。值得注意的是,越接近各電場集中區124之內側與外側,任二相鄰之第二遮罩136之間距越小,使後續於各電場集中區124中所形成之N型深井區106之摻雜濃度隨著越接近所形成之P型第一摻雜區110之二側而越小,以藉由於各電場集中區124中電場聚集越密集之N型深井區106中,亦即鄰近P型第一摻雜區110之二側之N型深井區106,摻雜較淡之濃度來提升崩潰電壓。本發明之第二遮罩136並不限為圓弧狀遮罩,且各第二遮罩136亦可為一條狀圖案,且各第二遮罩136指向各電場集中區124之內側,如第6圖所示。藉此,後續於各電場集中區124中所形成之N型深井區106之摻雜濃度隨著越接近所形成之P型第一摻雜區110之內側而越小。本發明之第二遮罩136不限於上述,亦可根據所需之耐壓條件來調整任二相鄰之第二遮罩136間之間距或各第二遮罩之寬度與形狀,使位於各電場集中區124中之N型深井區106之摻雜濃度可具有梯度變化或不具有梯度變化。 The manufacturer of the HV MOS transistor component of the present embodiment will be further described below. law. Please refer to Figures 4 to 9, and refer to Figure 2 together. 4 to 9 are schematic views showing a method of fabricating a HV MOS transistor component according to a preferred embodiment of the present invention. As shown in Fig. 4, a P-type substrate 102 is first provided. Then, a first mask 135 and a plurality of second masks 136, such as a photoresist mask, are formed on the P-type substrate 102. The first mask 135 defines the location of the N-type deep well region 106, and the second mask 136 is located in each of the electric field concentration regions 124. Subsequently, a first ion implantation process is performed on the P-type substrate 102 in a comprehensive manner, and N-type ions are implanted in the P-type substrate 102. As shown in FIG. 5, each of the second masks 136 of the present embodiment is an arc-shaped mask, and each of the second masks 136 surrounds the inner side of each of the electric field concentration regions 124 and is separated from each of the electric field concentration regions 124. The inner side is sequentially arranged to the outer side of each electric field concentration area 124. It should be noted that the closer to the inner side and the outer side of each electric field concentration area 124, the smaller the distance between any two adjacent second masks 136, so that the N-type deep well area 106 formed in each electric field concentration area 124 is subsequently The doping concentration is smaller as it is closer to the two sides of the formed P-type first doping region 110, so that the denser electric field in the electric field concentration region 124 is denser in the N-type deep well region 106, that is, adjacent to P. The N-type deep well region 106 on both sides of the first doped region 110 is doped with a lighter concentration to increase the breakdown voltage. The second mask 136 of the present invention is not limited to an arc-shaped mask, and each of the second masks 136 may also have a strip pattern, and each of the second masks 136 is directed to the inner side of each electric field concentration area 124, such as Figure 6 shows. Thereby, the doping concentration of the N-type deep well region 106 formed in each of the electric field concentration regions 124 is smaller as it approaches the inner side of the formed P-type first doping region 110. The second mask 136 of the present invention is not limited to the above, and the distance between any two adjacent second masks 136 or the width and shape of each second mask may be adjusted according to the required withstand voltage conditions. The doping concentration of the N-type deep well region 106 in the electric field concentration region 124 may or may not have a gradient change.

如第7圖所示,接著移除第一遮罩135與第二遮罩136,並進行一熱驅入製程,以形成N型深井區106。由於第二遮罩136遮蔽各電場集中區124之部份P型基底102,因此摻雜於各電場集中區124中之N型離子濃度係低於摻雜於各電場集中區124之外的N型離子濃度。藉此,位於各電場集中區124中之N型深井區106之摻雜濃度可小於位於各電場集中區124之外之N型深井區106之摻雜濃度。 As shown in FIG. 7, the first mask 135 and the second mask 136 are then removed and a thermal drive process is performed to form an N-type deep well region 106. Since the second mask 136 shields part of the P-type substrate 102 of each of the electric field concentration regions 124, the N-type ion concentration doped in each of the electric field concentration regions 124 is lower than that of the N-doped regions 124. Type ion concentration. Thereby, the doping concentration of the N-type deep well region 106 located in each of the electric field concentration regions 124 may be smaller than the doping concentration of the N-type deep well region 106 located outside the respective electric field concentration regions 124.

如第8圖所示,接下來於P型基底102上同時形成一第三遮罩138與複數個第四遮罩140,例如光阻遮罩。第三遮罩138定義出P型第一摻雜區110之位置,且第四遮罩140係位於各電場集中區124中。然後,對P型基底102全面性進行一第二離子佈植製程,以於N型深井區106中佈植P型離子。如第9圖所示,接著移除第三遮罩138與第四遮罩140,並進行一熱驅入製程,以形成P型第一摻雜區110。由於第四遮罩140遮蔽各電場集中區124之部份N型深井區106,因此摻雜於各電場集中區124中之P型離子濃度係低於摻雜於各電場集中區124之外的P型離子濃度,以搭配位於各電場集中區124中之N型深井區106之摻雜濃度,來調整出適當之第一比值,使HV MOS電晶體元件100可達到所欲之操作功效,且位於各電場集中區124中之P型第一摻雜區110之摻雜濃度與N型深井區106之摻雜濃度的第一比值可大於位於各電場集中區124之外的P型第一摻雜區110之摻雜濃度與N型深井區106之摻雜濃度的第二比值。由於各電場集中區124中之P型離子濃度不限需低於各電 場集中區124之外的P型離子濃度才可達到適當之第一比值,因此本發明之方法並不限於P型基底102上形成第四遮罩140,亦可未形成第四遮罩140,使位於各電場集中區124中之P型第一摻雜區110之摻雜濃度與位於各電場集中區124之外之P型第一摻雜區110之摻雜濃度相同,亦可使第一比值大於第二比值。但本發明不以此為限。 As shown in FIG. 8, a third mask 138 and a plurality of fourth masks 140, such as photoresist masks, are simultaneously formed on the P-type substrate 102. The third mask 138 defines the location of the P-type first doped region 110, and the fourth mask 140 is located in each of the electric field concentration regions 124. Then, a second ion implantation process is performed on the P-type substrate 102 in a comprehensive manner to implant P-type ions in the N-type deep well region 106. As shown in FIG. 9, the third mask 138 and the fourth mask 140 are then removed, and a thermal drive process is performed to form a P-type first doped region 110. Since the fourth mask 140 shields a portion of the N-type deep well region 106 of each of the electric field concentration regions 124, the P-type ion concentration doped in each of the electric field concentration regions 124 is lower than that doped outside the respective electric field concentration regions 124. The P-type ion concentration is adjusted to the appropriate first ratio by the doping concentration of the N-type deep well region 106 located in each of the electric field concentration regions 124, so that the HV MOS transistor component 100 can achieve the desired operational efficiency, and The first ratio of the doping concentration of the P-type first doping region 110 located in each of the electric field concentration regions 124 to the doping concentration of the N-type deep well region 106 may be greater than the P-type first doping outside the respective electric field concentration regions 124. A second ratio of the doping concentration of the hetero region 110 to the doping concentration of the N-type deep well region 106. Since the concentration of P-type ions in each electric field concentration region 124 is not lower than each electric power The P-type ion concentration outside the field concentration area 124 can reach a suitable first ratio. Therefore, the method of the present invention is not limited to forming the fourth mask 140 on the P-type substrate 102, and the fourth mask 140 may not be formed. The doping concentration of the P-type first doping region 110 located in each of the electric field concentration regions 124 is the same as the doping concentration of the P-type first doping region 110 located outside the respective electric field concentration regions 124, and may also be made first. The ratio is greater than the second ratio. However, the invention is not limited thereto.

如第2圖所示,然後於N型深井區106中依序形成P型高壓井區112與N型漂移區108。隨後,於P型第一摻雜區110上形成第二絕緣層126,例如場氧化層。接著,於P型高壓井區112、N型深井區106以及第二絕緣層126上形成閘極結構118與場電極128,其中閘極結構118從部份P型高壓井區112延伸至部份第二絕緣層126上。然後於N型漂移區108中形成N型第二摻雜區114,且同時於P型高壓井區112中形成N型第三摻雜區116。P型第一摻雜區110係位於N型第二摻雜區114與P型高壓井區112之間,且各電場集中區124圍繞部份N型第三摻雜區116。接著於P型高壓井區112中形成P型第四摻雜區120。 As shown in FIG. 2, a P-type high pressure well region 112 and an N-type drift region 108 are then sequentially formed in the N-type deep well region 106. Subsequently, a second insulating layer 126, such as a field oxide layer, is formed over the P-type first doped region 110. Next, a gate structure 118 and a field electrode 128 are formed on the P-type high-voltage well region 112, the N-type deep well region 106, and the second insulating layer 126, wherein the gate structure 118 extends from the portion of the P-type high-voltage well region 112 to a portion On the second insulating layer 126. An N-type second doped region 114 is then formed in the N-type drift region 108 while an N-type third doped region 116 is formed in the P-type high voltage well region 112. The P-type first doped region 110 is between the N-type second doped region 114 and the P-type high-voltage well region 112, and each of the electric field concentration regions 124 surrounds a portion of the N-type third doped region 116. A P-type fourth doped region 120 is then formed in the P-type high voltage well region 112.

本發明形成具有不同摻雜濃度之N型深井區之方法不限利用光阻遮罩。請參考第10圖,第10圖為本發明另一較佳實施例之HV MOS電晶體元件之製作方法示意圖。如第10圖所示,相較於上述實施例,本實施例形成N型深井區之步驟係利用一半色調遮罩142進行第一離子佈植製程,且半色調遮罩142係對應於各電場集中區 124以外之區域,使摻雜於各電場集中區124中之N型離子濃度係低於摻雜於各電場集中區124之外的N型離子濃度。藉此,位於各電場集中區124中之N型深井區106之摻雜濃度可小於位於各電場集中區124之外之N型深井區106之摻雜濃度。此外,於本發明之其他實施例中,形成具有不同摻雜濃度之P型第一摻雜區110亦可使用半色調遮罩142,但不以此為限。 The method of the present invention for forming an N-type deep well region having different doping concentrations is not limited to the use of a photoresist mask. Please refer to FIG. 10, which is a schematic diagram of a method for fabricating a HV MOS transistor component according to another preferred embodiment of the present invention. As shown in FIG. 10, in comparison with the above embodiment, the step of forming the N-type deep well region in the present embodiment uses the halftone mask 142 to perform the first ion implantation process, and the halftone mask 142 corresponds to each electric field. Concentrated area The region other than 124 causes the N-type ion concentration doped in each of the electric field concentration regions 124 to be lower than the N-type ion concentration doped outside the respective electric field concentration regions 124. Thereby, the doping concentration of the N-type deep well region 106 located in each of the electric field concentration regions 124 may be smaller than the doping concentration of the N-type deep well region 106 located outside the respective electric field concentration regions 124. In addition, in other embodiments of the present invention, the P-type first doping region 110 having different doping concentrations may be used, but the halftone mask 142 may be used, but not limited thereto.

綜上所述,本發明利用圓弧狀或條狀遮罩或半色調遮罩遮蔽電場集中區中之部份P型基底,以形成具有不同摻雜濃度之N型深井區,且位於各電場集中區中之N型深井區之摻雜濃度小於各電場集中區之外的N型深井區之摻雜濃度。藉此,位於電場集中區中之P型第一摻雜區之摻雜濃度與N型深井區之摻雜濃度的第一比值可大於位於電場集中區之外的P型第一摻雜區之摻雜濃度與N型深井區之摻雜濃度的第二比值。並且,本發明之M形HV MOS電晶體元件的崩潰電壓可藉由調整第一比值至大於第二比值而增加,因此同時整合有M形HV MOS電晶體元件與圓形HV MOS電晶體元件之晶片的崩潰電壓可被有效提升。 In summary, the present invention utilizes an arc-shaped or strip-shaped mask or a halftone mask to shield a portion of the P-type substrate in the electric field concentration region to form an N-type deep well region having different doping concentrations, and is located at each electric field. The doping concentration of the N-type deep well region in the concentration zone is smaller than the doping concentration of the N-type deep well region outside the electric field concentration region. Thereby, the first ratio of the doping concentration of the P-type first doping region in the electric field concentration region to the doping concentration of the N-type deep well region may be greater than the P-type first doping region outside the electric field concentration region. The second ratio of the doping concentration to the doping concentration of the N-type deep well region. Moreover, the breakdown voltage of the M-shaped HV MOS transistor device of the present invention can be increased by adjusting the first ratio to be larger than the second ratio, thereby integrating the M-shaped HV MOS transistor element and the circular HV MOS transistor element at the same time. The chip's breakdown voltage can be effectively boosted.

以上所述僅為本發明之較佳實施例,凡依本發明申請專利範圍所做之均等變化與修飾,皆應屬本發明之涵蓋範圍。 The above are only the preferred embodiments of the present invention, and all changes and modifications made to the scope of the present invention should be within the scope of the present invention.

100‧‧‧高壓金氧半導體電晶體元件 100‧‧‧High voltage MOS transistor components

102‧‧‧基底 102‧‧‧Base

104‧‧‧第一絕緣層 104‧‧‧First insulation

106‧‧‧深井區 106‧‧‧Shenjing District

108‧‧‧漂移區 108‧‧‧Drift area

110‧‧‧第一摻雜區 110‧‧‧First doped area

112‧‧‧高壓井區 112‧‧‧High-pressure well area

114‧‧‧第二摻雜區 114‧‧‧Second doped area

116‧‧‧第三摻雜區 116‧‧‧ Third doped area

118‧‧‧閘極結構 118‧‧‧ gate structure

120‧‧‧第四摻雜區 120‧‧‧fourth doping zone

121‧‧‧突出部 121‧‧‧Protruding

122‧‧‧凹口 122‧‧‧ Notch

124‧‧‧電場集中區 124‧‧‧Electrical field concentration area

126‧‧‧第二絕緣層 126‧‧‧Second insulation

128‧‧‧場電極 128‧‧ ‧ field electrode

130‧‧‧第一關係曲線 130‧‧‧first relationship curve

132‧‧‧第二關係曲線 132‧‧‧second relationship curve

134‧‧‧第三關係曲線 134‧‧‧ third relationship curve

135‧‧‧第一遮罩 135‧‧‧ first mask

136‧‧‧第二遮罩 136‧‧‧second mask

138‧‧‧第三遮罩 138‧‧‧ third mask

140‧‧‧第四遮罩 140‧‧‧Fourth mask

142‧‧‧半色調遮罩 142‧‧‧ halftone mask

BL‧‧‧基準值 BL‧‧‧ benchmark value

第1圖為本發明一較佳實施例之高壓金氧半導體電晶體元件之上視 示意圖。 1 is a top view of a high voltage MOS transistor component according to a preferred embodiment of the present invention. schematic diagram.

第2圖為沿著第1圖之剖面線AA’之剖面示意圖。 Fig. 2 is a schematic cross-sectional view taken along line AA' of Fig. 1.

第3圖為不同HV MOS電晶體元件位於電場集中區之外的P型第一摻雜區之摻雜濃度與N型深井區之摻雜濃度的第二比值與崩潰電壓之關係示意圖。 Fig. 3 is a graph showing the relationship between the doping concentration of the P-type first doped region and the doping concentration of the N-type deep well region and the breakdown voltage of the different HV MOS transistor elements outside the electric field concentration region.

第4圖至第9圖為本發明較佳實施例之HV MOS電晶體元件之製作方法示意圖。 4 to 9 are schematic views showing a method of fabricating a HV MOS transistor component according to a preferred embodiment of the present invention.

第10圖為本發明另一較佳實施例之HV MOS電晶體元件之製作方法示意圖。 FIG. 10 is a schematic view showing a manufacturing method of a HV MOS transistor component according to another preferred embodiment of the present invention.

100...高壓金氧半導體電晶體元件100. . . High voltage MOS transistor

102...基底102. . . Base

104...第一絕緣層104. . . First insulating layer

106...深井區106. . . Deep well area

108...漂移區108. . . Drift zone

110...第一摻雜區110. . . First doped region

112...高壓井區112. . . High pressure well area

114...第二摻雜區114. . . Second doped region

116...第三摻雜區116. . . Third doped region

118...閘極結構118. . . Gate structure

120...第四摻雜區120. . . Fourth doped region

124...電場集中區124. . . Electric field concentration area

126...第二絕緣層126. . . Second insulating layer

128...場電極128. . . Field electrode

Claims (19)

一種高壓金氧半導體電晶體元件,包含有:一基底,具有一第一導電類型,該基底具有至少一電場集中區;一深井區,設於該基底中,且具有不同於該第一導電類型之一第二導電類型,且該電場集中區係位於該深井區的一部分;一第一摻雜區,設於該深井區中,其中位於該電場集中區中之該第一摻雜區之摻雜濃度與該深井區之摻雜濃度具有一第一比值,位於該電場集中區之外的該第一摻雜區之摻雜濃度與該深井區之摻雜濃度具有一第二比值,且該第一比值大於該第二比值;一高壓井區,設於該深井區中,且具有該第一導電類型;一第二摻雜區,設於該深井區中,且具有該第二導電類型,其中該第一摻雜區位於該第二摻雜區與該高壓井區之間,該電場集中區係位於該第二摻雜區與該高壓井區之間,且該第二摻雜區具有至少一凹口;一第三摻雜區,設於該高壓井區中,且具有該第二導電類型,其中該電場集中區圍繞部份該第三摻雜區;一閘極結構,設於該第一摻雜區與該第三摻雜區之間的該高壓井區上;以及一第四摻雜區,設於該高壓井區中,且具有該第一導電類型。 A high voltage MOS semiconductor transistor device comprising: a substrate having a first conductivity type, the substrate having at least one electric field concentration region; and a deep well region disposed in the substrate and having a different conductivity type a second conductivity type, wherein the electric field concentration region is located in a portion of the deep well region; a first doped region is disposed in the deep well region, wherein the first doped region is mixed in the electric field concentration region The doping concentration has a first ratio with the doping concentration of the deep well region, and the doping concentration of the first doping region outside the electric field concentration region has a second ratio to the doping concentration of the deep well region, and the The first ratio is greater than the second ratio; a high pressure well region is disposed in the deep well region and has the first conductivity type; a second doped region is disposed in the deep well region and has the second conductivity type The first doped region is located between the second doped region and the high voltage well region, and the electric field concentration region is located between the second doped region and the high voltage well region, and the second doped region Having at least one notch; a third doped region, In the high-voltage well region, and having the second conductivity type, wherein the electric field concentration region surrounds a portion of the third doped region; a gate structure is disposed in the first doped region and the third doped region And the fourth doped region is disposed in the high voltage well region and has the first conductivity type. 如請求項1所述之高壓金氧半導體電晶體元件,其中位於該電場集中區中之該深井區之摻雜濃度小於位於該電場集中區之外之該 深井區之摻雜濃度。 The high voltage MOS transistor device of claim 1, wherein a doping concentration of the deep well region located in the electric field concentration region is smaller than the concentration outside the electric field concentration region Doping concentration in the deep well area. 如請求項1所述之高壓金氧半導體電晶體元件,其中位於該電場集中區中之該第一摻雜區之摻雜濃度與位於該電場集中區之外之該第一摻雜區之摻雜濃度相同。 The high voltage MOS transistor device of claim 1, wherein a doping concentration of the first doping region in the electric field concentration region is mixed with the first doping region outside the electric field concentration region. The impurity concentration is the same. 如請求項1所述之高壓金氧半導體電晶體元件,其中位於該電場集中區中之該深井區之摻雜濃度越接近該第一摻雜區之二側越小。 The high voltage MOS transistor device of claim 1, wherein a doping concentration of the deep well region located in the electric field concentration region is smaller as a closer to two sides of the first doping region. 如請求項1所述之高壓金氧半導體電晶體元件,另包括一絕緣層,設於該第一摻雜區上。 The high voltage MOS transistor device of claim 1, further comprising an insulating layer disposed on the first doped region. 如請求項5所述之高壓金氧半導體電晶體元件,另包括複數個場電極,設於該絕緣層上。 The high voltage MOS transistor device of claim 5, further comprising a plurality of field electrodes disposed on the insulating layer. 如請求項1所述之高壓金氧半導體電晶體元件,其中該電場集中區係為一半圓弧形區域。 The high voltage MOS transistor device of claim 1, wherein the electric field concentration region is a semicircular arc region. 如請求項1所述之高壓金氧半導體電晶體元件,其中該高壓金氧半導體電晶體元件係為一M形元件。 The high voltage MOS transistor device of claim 1, wherein the high voltage MOS transistor device is an M-shaped device. 如請求項1所述之高壓金氧半導體電晶體元件,另包括一漂移 區,設於該深井區,且該第二摻雜區設於該漂移區中。 A high voltage MOS transistor device as claimed in claim 1, further comprising a drift a region is disposed in the deep well region, and the second doped region is disposed in the drift region. 一種高壓金氧半導體電晶體元件之製作方法,包括:提供一基底,其中該基底具有一第一導電類型,且該基底具有至少一電場集中區;於該基底中形成一深井區,且該深井區具有不同於該第一導電類型之一第二導電類型,其中該電場集中區係位於該深井區的一部分;於該深井區中形成一第一摻雜區,且該第一摻雜區具有該第一導電類型,其中位於該電場集中區中之該第一摻雜區之摻雜濃度與該深井區之摻雜濃度具有一第一比值,位於該電場集中區之外的該第一摻雜區之摻雜濃度與該深井區之摻雜濃度具有一第二比值,且該第一比值大於該第二比值;以及於該基底中形成一高壓井區,並分別於該深井區與該高壓井區中形成一第二摻雜區與一第三摻雜區,該高壓井區具有該第一導電類型,且該第二摻雜區與該第三摻雜區具有該第二導電類型,其中該第一摻雜區位於該第二摻雜區與該高壓井區之間,且該電場集中區圍繞部份該第三摻雜區,且其中該電場集中區係位於該第二摻雜區與該高壓井區之間,且該第二摻雜區具有至少一凹口。 A method of fabricating a high voltage MOS transistor device, comprising: providing a substrate, wherein the substrate has a first conductivity type, and the substrate has at least one electric field concentration region; forming a deep well region in the substrate, and the deep well The region has a second conductivity type different from the first conductivity type, wherein the electric field concentration region is located in a portion of the deep well region; a first doped region is formed in the deep well region, and the first doped region has The first conductivity type, wherein a doping concentration of the first doping region in the electric field concentration region has a first ratio with a doping concentration of the deep well region, and the first doping outside the electric field concentration region The doping concentration of the impurity region has a second ratio to the doping concentration of the deep well region, and the first ratio is greater than the second ratio; and forming a high pressure well region in the substrate, and respectively in the deep well region Forming a second doped region and a third doped region in the high voltage well region, the high voltage well region having the first conductivity type, and the second doped region and the third doped region having the second conductivity type Which of the a doped region is located between the second doped region and the high voltage well region, and the electric field concentration region surrounds a portion of the third doped region, and wherein the electric field concentration region is located in the second doped region and the high voltage region Between the well regions, and the second doped region has at least one recess. 如請求項10所述之高壓金氧半導體電晶體元件之製作方法,其中形成該深井區之步驟包括: 於該基底上形成一第一遮罩與複數個第二遮罩,其中該等第二遮罩位於該電場集中區中;以及對該基底全面性進行一第一離子佈植製程,以形成該深井區,使位於該電場集中區中之該深井區之摻雜濃度小於位於該電場集中區之外之該深井區之摻雜濃度。 The method of fabricating a high voltage MOS transistor according to claim 10, wherein the step of forming the deep well region comprises: Forming a first mask and a plurality of second masks on the substrate, wherein the second masks are located in the electric field concentration region; and performing a first ion implantation process on the substrate comprehensively to form the In the deep well region, the doping concentration of the deep well region located in the electric field concentration region is smaller than the doping concentration of the deep well region outside the electric field concentration region. 如請求項11所述之高壓金氧半導體電晶體元件之製作方法,其中各該第二遮罩係為一圓弧狀遮罩,且各該第二遮罩圍繞該電場集中區之一內側。 The method of fabricating a high voltage MOS transistor according to claim 11, wherein each of the second masks is an arc-shaped mask, and each of the second masks surrounds one of the inner sides of the electric field concentration region. 如請求項12所述之高壓金氧半導體電晶體元件之製作方法,其中任二相鄰之該等第二遮罩間之間距越接近該電場集中區之該內側與一外側越小。 The method of fabricating a high voltage MOS transistor according to claim 12, wherein the distance between any two adjacent second masks is closer to the inner side and the outer side of the electric field concentration region. 如請求項11所述之高壓金氧半導體電晶體元件之製作方法,其中各該第二遮罩係為一條狀遮罩,且各該第二遮罩指向該電場集中區之一內側。 The method of fabricating a high voltage MOS transistor according to claim 11, wherein each of the second masks is a strip mask, and each of the second masks is directed to an inner side of the electric field concentration region. 如請求項10所述之高壓金氧半導體電晶體元件之製作方法,其中形成該深井區之步驟包括利用一半色調遮罩進行一第一離子佈植製程,使位於該電場集中區中之該深井區之摻雜濃度小於位於該電場集中區之外之該深井區之摻雜濃度。 The method of fabricating a high voltage MOS transistor according to claim 10, wherein the step of forming the deep well region comprises performing a first ion implantation process using a halftone mask to cause the deep well located in the electric field concentration region The doping concentration of the region is less than the doping concentration of the deep well region outside the concentration region of the electric field. 如請求項10所述之高壓金氧半導體電晶體元件之製作方法,其中形成該第一摻雜區之步驟包括:於該基底上形成一第三遮罩與複數個第四遮罩,其中該等第四遮罩位於該電場集中區中;以及對該基底全面性進行一第二離子佈植製程,以形成該第一摻雜區。 The method of fabricating the high voltage MOS transistor device of claim 10, wherein the forming the first doped region comprises: forming a third mask and a plurality of fourth masks on the substrate, wherein the And waiting for the fourth mask to be located in the electric field concentration region; and performing a second ion implantation process on the substrate comprehensively to form the first doping region. 如請求項10所述之高壓金氧半導體電晶體元件之製作方法,另包括於該高壓井區中形成一第四摻雜區,且該第四摻雜區具有該第一導電類型。 The method of fabricating the high voltage MOS transistor device of claim 10, further comprising forming a fourth doped region in the high voltage well region, and the fourth doped region has the first conductivity type. 如請求項10所述之高壓金氧半導體電晶體元件之製作方法,另包括於該第一摻雜區上形成一絕緣層。 The method of fabricating the high voltage MOS transistor device of claim 10, further comprising forming an insulating layer on the first doped region. 如請求項18所述之高壓金氧半導體電晶體元件之製作方法,另包括於該絕緣層上形成一閘極結構與複數個場電極。 The method for fabricating a high voltage MOS transistor according to claim 18, further comprising forming a gate structure and a plurality of field electrodes on the insulating layer.
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