TW425672B - Forming HV-CMOS with grading doping electrode - Google Patents
Forming HV-CMOS with grading doping electrode Download PDFInfo
- Publication number
- TW425672B TW425672B TW88107367A TW88107367A TW425672B TW 425672 B TW425672 B TW 425672B TW 88107367 A TW88107367 A TW 88107367A TW 88107367 A TW88107367 A TW 88107367A TW 425672 B TW425672 B TW 425672B
- Authority
- TW
- Taiwan
- Prior art keywords
- patent application
- scope
- trench
- region
- source
- Prior art date
Links
Landscapes
- Insulated Gate Type Field-Effect Transistor (AREA)
Abstract
Description
4256 7 2 五、發明說明(1) 5-1發明領域 本發明係有關於一種半導體元件的構造及製造方法, 特別疋有關於提尚電流驅動能力的元件及縮小元件所佔面 積的構造及製造方法。 5-2發明背景: .隨著時間發展,科技演變,積集電路(integrated circuits)逐漸朝向南密集度目標邁進。這也使得半導體 元件的體積及元件與元件間的距離亦有日漸縮小化的趨勢 ,因此,既使半導體元件小到以埃為測量單位,仍需維持 元件原來所擁有的最佳使用狀態是極重要的,特別是在高 電壓操作下仍可輕易達到高電流驅動能力。傳統的高壓 CMOS(HV-CMOS)元件結構’其通道(channel )及漂移區域 (dr 1 ft region)都在水平方向易佔據較大的晶片面積,且 在高電壓操作下不易達到高電流驅動能力。因此,更先進 的製造技術及更好的元件結構之需求顯得迫切。 第一 A圓為一傳統的CM〇s電晶體結構之剖面圖,其結 構包括一 p型導通型基板丨〇,一 N+源極丨丨,一 N+汲極丨2,一 漂移區域13 ’ 一場氧化層(F〇x)14,一閘極氧化層(gate oxide)15 ’ 及一閘極16。4256 7 2 V. Description of the invention (1) 5-1 Field of the invention The present invention relates to a structure and manufacturing method of a semiconductor device, and particularly to a structure and manufacturing of a device that improves current driving capability and reduces the area occupied by the device. method. 5-2 Background of the Invention: With the development of time and the evolution of technology, integrated circuits are gradually moving towards the goal of south density. This also makes the volume of semiconductor components and the distance between components also gradually shrink. Therefore, even if the semiconductor components are as small as Angstroms as the measurement unit, it still needs to maintain the best use of the components. Importantly, especially under high voltage operation, high current drive capability can still be easily achieved. The traditional high-voltage CMOS (HV-CMOS) element structure 'its channel and dr 1 ft region are easy to occupy a large chip area in the horizontal direction, and it is not easy to achieve high current driving capability under high voltage operation . Therefore, the need for more advanced manufacturing technologies and better component structures is urgent. The first circle A is a cross-sectional view of a conventional CMOS transistor structure, and its structure includes a p-type conduction substrate 丨 〇, an N + source 丨 丨, an N + drain 丨 2, and a drift region 13 ′ field An oxide layer (Fox) 14, a gate oxide layer 15 ', and a gate electrode 16.
第4頁 425672 五、發明說明(2) 上述之傳統的CMOS電晶體結構,其通道及漂移區域都 在水平方向且只有源極及没極區位於半導體基板中,這樣 的結構使得CMOS的通道及漂移區域更顯得短。當CMOS的通 道長度縮短後’熱載子效應(Hot Carrier Effects)將越 嚴重’而解決短通道CMOS的熱載子效應的方法有很多。其 中最簡單的就是降低CMOS電晶體的操作電壓。譬如,從5V 降低為3. 3 V,或是2. 5 V,使通道的橫向電場強度減小以致 於無法形成熱載子。如此雖可以大大的減低"載子倍增"的 現象’但是卻無法使用於高電壓操作下,如要避免降低 CMOS電晶體的操作電壓且同樣能解決短通道CMOS的熱載子 效應’則需加長CMOS的通道。水平方向的結構及加長CMOS 的通道都會佔據較大的晶片面積,其將無法溶入半導體元 件體積縮小化的趨勢。 另一種現在廣泛的被採用的解決熱載子效應之方法, 就是在原來的CMOS的源極和没極接近通道的地方加一組摻 雜濃度較原來N+型的源極與汲極濃度為低的N-型區,此設 a十稱為輕微推雜的;及極(Lightly Doped Drain)",或簡 稱為LDD。LDD的使用並不是全然沒有缺點。首先,它將使 得CMOS的製作變得複雜;其次,因為LDD的摻雜程度較低 ’電阻也就比較高’使得汲極到源極的串聯電阻(S e r i e s Resistance )增加。這將導致元件的操作速度降低,且電 力的消耗(Power Dissipation)上升。Page 4 425672 V. Description of the invention (2) The above-mentioned traditional CMOS transistor structure has channels and drift regions in the horizontal direction and only the source and non-electrode regions are located in the semiconductor substrate. Such a structure makes the channels and The drift area is even shorter. When the channel length of CMOS is shortened, ‘Hot Carrier Effects will become more severe’, and there are many ways to solve the thermal carrier effects of short-channel CMOS. The simplest of these is to lower the operating voltage of the CMOS transistor. For example, reducing from 5V to 3.3 V, or 2.5 V, reduces the transverse electric field strength of the channel so that hot carriers cannot be formed. Although the phenomenon of "carrier multiplication" can be greatly reduced in this way, it cannot be used in high-voltage operation. If you want to avoid reducing the operating voltage of CMOS transistors and also solve the hot-carrier effect of short-channel CMOS, then Need to lengthen the CMOS channel. Both the horizontal structure and the lengthened CMOS channel will occupy a larger chip area, which will not be able to dissolve into the semiconductor device and shrink the volume. Another widely used method to solve the hot carrier effect is to add a set of doping concentration to the source and drain of the original CMOS that is lower than the original N + source and drain concentration. N-type region, this design a is called slightly doped; and pole (Lightly Doped Drain), or LDD for short. The use of LDD is not entirely without its drawbacks. First, it will complicate the fabrication of CMOS. Second, because the LDD has a lower doping level, the resistance is higher, which increases the series resistance from drain to source (S e r e e s Resistance). This will lead to a reduction in the operating speed of the components and an increase in power consumption.
第5頁 42567 2 五、發明說明(3) 再者,因場氧化層底下有較淡的 ^ ^ . 隨者提回並導致較弱的電流驅動能力 . „ , . . . (Current Drive ι由於源極和没極的結構是對稱的,兩邊都 有杈、的摻雜濃度’整體的電流驅動能力更加的弱。最後 ’此電晶體結構在高壓下容易產生寄生雙載子(parasitic bipolar)的效應。 5 - 3發明目的及概述: 鑒於上述之發明背景中,傳統的高壓元件結構所產生 的諸多缺點,本發明的主要目的是在提出一種高壓半導體 元件的構造及製造方法,以兩種不同摻雜濃度當作漂移區 域的梯度摻雜使提高元件之電流驅動能力,並提高崩潰高 壓(Breakdown Voltage)。另做氧化間隙壁“叩。^ 〇xide )山來作^為多晶矽閘極(P〇ly Gate)之邊緣的著力點,以避免 崩潰高壓提早發生。再者,改變其元件之通道及漂移區域 的位置,由傳統的水平方向改換為垂直方向,使其所佔據 的晶片面積大大的減少。 本發明是形成電晶體元件的方法,其特殊的結構至少 包括下列成份’在第一 B圖中,首先,提供一 p型矽半導體 基板1〇〇 ’其中已形成有第一溝槽14〇及第二溝槽17〇 第二溝槽之深度較第一溝槽深。接著,一對源極(2〇〇, 130,及120)和汲極(21〇,131,及121)區分別形成於第一Page 5 42567 2 V. Description of the invention (3) Furthermore, the lighter ^ ^ under the field oxide layer brings it back and results in a weaker current drive capability. „,... (Current Drive ι The source and non-polar structures are symmetrical, with doping concentrations on both sides. The overall current driving capability is weaker. Finally, this transistor structure is prone to parasitic bipolar under high voltage. 5-3 Purpose and Summary of the Invention: In view of the many shortcomings of the traditional high-voltage component structure in the above background of the invention, the main purpose of the present invention is to propose a structure and manufacturing method for high-voltage semiconductor components, with two different The doping concentration is used as the gradient doping of the drift region to improve the current driving capability of the device and increase the Breakdown Voltage. Another oxide spacer “氧化. ^ × ide” is used as the polycrystalline silicon gate (P 〇ly Gate) at the edge of the force to avoid the collapse of high voltage early. Furthermore, by changing the position of the channel and drift region of its components, the traditional horizontal direction is changed to the vertical direction, so that the area occupied by the chip is greatly reduced. The invention is a method for forming a transistor element. Its special structure includes at least the following components. In the first diagram B, first, a p-type silicon semiconductor substrate 100 is provided, in which a first trench 14o has been formed, and The second trench 170 is deeper than the first trench. Next, a pair of source (200, 130, and 120) and drain (21, 131, and 121) regions are formed on the first
第6頁 4 2567 2·. 五'發明說明(4) 溝槽及第二溝槽 槽的深度相當。 兩側的半導體基板中,其深度約與第二溝 在 ,其内 .導通型 上,也 之導通 度大於 成是在 及在第 面,第 一及第 之濃度 該對 之第 已 同 型係 源極和 一摻雜 樣是在 成一第 相同於 第一摻雜區 形成一第三 二摻雜區上 三摻雜區内 -—推雜區之 〉 及極區中已形成一 質之導通型係相反 该對源極和汲極區 二摻雜區130及1 31 上述第一摻雜區之 之濃度。最後,整 推雜區200及210在 方之後,其表面就 之第三摻雜質之導 導通型’且其摻雜 第一摻雜區120及121 於上述半導體基板之 中且在第一摻雜區之 ’其内之第二摻雜質 導通型,且其摻雜濃 個源極和汲極區的完 該對源極和汲極區中 是源極/汲極區之表 通型係相同於上述第 濃度大於第二摻雜區 此外’元件之結構更包 溝槽的側壁上,其用來作問 緣層。再者,一閘極氧化層 及底部表面上,並且有—多 間氧化層之上並填滿第—溝 源極和汲極區的表面相等。 括一氧化矽間隙壁i 6 〇在第一 極電極之邊緣的著力點及一絕 1 8 0形成在該第二溝槽的側壁 晶石夕埋層閘極電極19〇形成於 槽及第二溝槽,其表面約與該 上述之特殊結構至少 槽的方式來放置閘極和間 包括下列幾點優勢,首先,以溝 隙壁及改變通道和漂移區域的位Page 6 4 2567 2 ·. Description of the Five 'Invention (4) The grooves and the second grooves have the same depth. In the semiconductor substrates on both sides, the depth is about the same as that of the second trench, and the continuity of the conduction type is greater than that on and on the first, first, and first concentrations of the pair. A pole and a doping pattern are formed in a first and the same as the first doped region to form a third and second doped region. The three doped region—the doped region—and the polar region have formed a qualitative conduction system. Conversely, the concentration of the first and second doped regions 130 and 1 31 of the pair of source and drain regions. Finally, after the impurity regions 200 and 210 are completely pushed, the surface of the third dopant is on-conducting type and its first doped regions 120 and 121 are doped in the semiconductor substrate and in the first doped region. The second dopant on-type in the hetero-region, and its doped source and drain regions are complete. The pair of source and drain regions is a source / drain surface-type system. The structure of the element, which is the same as the above-mentioned first concentration is greater than the second doped region, further includes a sidewall of the trench, which is used as an interlayer. Furthermore, a gate oxide layer and the bottom surface, and there are a plurality of oxide layers and fill the first trench with the same source and drain surfaces. Including the silicon oxide barrier wall i 6 〇 at the edge of the first electrode electrode and an insulation 180 formed in the side wall of the second trench spar burial gate electrode 19 formed in the groove and the second Grooves, the surface of which is about the same as the above-mentioned special structure, at least the way to place the gate electrode, and the following include the following advantages. First, the groove wall and the position of the channel and drift region are changed.
第7頁 —425672 五、發明說明(5) 置,由水平方向換為 。通道的長度也隨著 字型轉換為本發明的 的長度的增長而大大 部份,如果第一摻雜 很淡,元件可持高壓 雜區及第二摻雜區的 電壓但其電流驅動能 摻雜濃度,由淺到濃 。最後’本發明之間 ’上層不至於比下層 垂直方向 溝槽式之 11凹”字型 的減低^ 區及第二 但其電流 摻雜濃度 力會較強 ,來互補 隙壁的位 早崩潰。 ,都可 閘極而 ’熱載 在源極 摻雜區 驅動能 都相當 。因此 上述之 置可避 減少佔 増長, 子效應 /汲極 的摻雜 力較弱 但很濃 ’本發 缺陷以 /¾. 山 、也 免朋潰 據之晶 由傳統 產生會 區摻雜 濃度都 ,如果 ,元件 明採用 提高崩 電壓提 片面積 的"一” 因通道 濃度的 相當且 第一摻 持不多 不同的 潰電壓 早發生 5-4圖式簡單說明 第一 A圖顯示一典型CMOS源極/汲極的剖面結構圓形 〇 第一 B圖顯示本發明其中一實施例之高壓元件剖面結 構圓形。 弟一 A圖顯示一半導體基板。 第二B圖顯示一選擇性添加蟲晶石夕(epitaxial S1 Hcon)之半導體基板。 第二C圖顯示形成一氧化層於半導體基板之表面上。 第二D圖顯示趨入η塑摻雜質於半導體基板中之第一 摻雜區。Page 7 —425672 V. Description of the invention (5) Change from horizontal to. The length of the channel is also greatly increased as the length of the font is converted to the length of the present invention. If the first doping is light, the device can hold the voltage of the high-voltage doped region and the second doped region but its current can drive the doping. Miscellaneous concentration, from shallow to thick. Finally, the upper layer of the "between the invention" is not lower than the 11-concave groove-shaped reduced region of the vertical direction of the lower layer and the second, but its current doping concentration force will be stronger to compensate for the early collapse of the gap wall. Both can be gated and the driving energy of the hot-loaded source-doped region is equivalent. Therefore, the above-mentioned arrangement can avoid reducing the occupation length, and the sub-effect / drain doping force is weak but very strong. ¾. Also, the crystals do not have the same doping concentration as traditionally produced. If the element is used, the "to increase the chipping area of the chip" is "one" because the channel concentration is the same and the first doping is not much different. Figure 5-4 shows the breakdown voltage early. The first diagram A shows a typical CMOS source / drain cross-section structure. The first diagram B shows the cross-sectional structure of a high-voltage element in one embodiment of the present invention. Brother A Figure A shows a semiconductor substrate. FIG. 2B shows a semiconductor substrate with epitaxial S1 Hcon selectively added. FIG. 2C shows that an oxide layer is formed on the surface of the semiconductor substrate. The second D diagram shows a first doped region in the semiconductor substrate that is doped with n-type dopants.
第8頁 4 256 7 2 五、發明說明(6) 第二E圖顯示趨入η型摻雜質於半導體基板中之第二 摻雜區。 第二F圖顯示形成一第一溝槽於半導體基板中。 第二G圖顯示用保角覆蓋(conformal)的方式沉積一 氧化層。 第二Η圖顯示形成一間隙壁及一第二溝槽。 第二I圖顯示形成一閘極氧化層於第二溝槽底部的表 面及側壁上。 第二J圖顯示沉積一多晶矽層並填滿第一溝槽及第二 溝槽。 第二Κ圖顯示趨入η型摻雜質於半導體基板中之第三 摻雜區,既本發明另一實施例之高壓元件剖面結構圖形。 第二L圖形同第一 Β圖形。 主要部分之代表符號: 10 ρ型半導體基板 11 源極 12 汲極 13 漂移區域(Drift Region) 14 場氧化層(FOX) 1 5 閘極氧化層(gate oxide) 16 閘極 100 ρ型半導體基板 101 p~epi型半導體基板Page 8 4 256 7 2 V. Description of the invention (6) The second E diagram shows the second doped region in the semiconductor substrate that is approaching the n-type dopant. FIG. 2F shows that a first trench is formed in the semiconductor substrate. Figure G shows a conformal deposition of an oxide layer. The second figure shows the formation of a spacer wall and a second trench. FIG. 2I shows that a gate oxide layer is formed on the surface and the sidewall of the bottom of the second trench. The second J figure shows that a polycrystalline silicon layer is deposited and fills the first trench and the second trench. The second K diagram shows a third doped region in the semiconductor substrate, which is an n-type dopant, which is a cross-sectional structure pattern of a high-voltage device according to another embodiment of the present invention. The second L pattern is the same as the first B pattern. Representative symbols of main parts: 10 ρ-type semiconductor substrate 11 source 12 drain 13 drift region 14 field oxide layer (FOX) 1 5 gate oxide 16 gate 100 ρ type semiconductor substrate 101 p ~ epi type semiconductor substrate
425672 五、發明說明(7) 110 氧化石夕層(silicon oxide) 1 2 0源極第一摻雜區(n井1 ) 1 2 1汲極第一摻雜區(N井】) 130源極第二摻雜區(N井2) 131汲極第二摻雜區(N井2) 140 第一溝槽(first trench) 1 5 0氧化矽層 1 6 0 間隙壁(s p a c e r) 1 7 0第二溝槽 1 8 0閘極氧化層 190 多晶矽閘極電極(p〇lysilic〇n gate electr〇de) 2 0 0源極第三摻雜區 2 1 0汲極第三摻雜區 5-5發明詳細說明: 、在本發,的—實施例令,提供一種梯度摻雜式源極/ 汲,=形成尚壓互補式金屬氧化半導體(HV-CM0S)的構造 及製造方法,其特殊結構之製程詳述於第二A圖至第圖 中1首先,提供—ρ型導通型半導體基板ι〇〇 ’如第二Α圖 ::。第二B圖顯示本實施例一可選擇性之添加磊晶矽之 乂 、基板1 01其功此疋預防閉鎖(fatch up)發生於互 補式金屬氧化半導體元件中,為了使該發明結構簡單化, 以下之元件結構將不包括磊晶矽半導體基板(p-epi425672 V. Description of the invention (7) 110 silicon oxide layer (silicon oxide) 1 2 0 source first doped region (n-well 1) 1 2 1 drain first doped region (N-well) 130 source Second doped region (N-well 2) 131 Drain second doped region (N-well 2) 140 first trench 1 5 0 silicon oxide layer 1 6 0 spacer 1 7 0 Two trenches 1 8 0 gate oxide layer 190 polysilicon gate electrode 2 0 0 source third doped region 2 1 0 drain third doped region 5-5 invention Detailed description: In the present invention, an embodiment order provides a gradient doped source / sink, = structure and manufacturing method for forming a still-complementary complementary metal oxide semiconductor (HV-CM0S), and a process for its special structure Detailed descriptions in the second A to the first FIG. 1 First, a p-type semiconductor substrate ι ′ is provided, such as the second A ::. FIG. 2B shows the first embodiment of the present invention, which can selectively add epitaxial silicon and the substrate 101 to prevent latch-up from occurring in the complementary metal oxide semiconductor device. In order to simplify the structure of the invention The following device structures will not include epitaxial silicon semiconductor substrates (p-epi
I !1I! 1
IH 第〗0頁 425672 五、發明說明(8) substrate)101 ° 在第二c圖中,採用電漿化學氣相沉積(p]asma Enhanced CVD)法形成一氧化矽層11〇於半導體基板ι〇〇之 表面上,該氧化矽層的厚度約界於9〇〇埃和35〇〇埃之間。 其中上述之氧化石夕層可採用任何一種化學氣相沉積法( Chenucal Vapor Depositi〇n)形成,如Ap 單只限於PECVD。此氧化石夕層11〇係用“作為二植IH No. 0 page 425672 V. Description of the invention (8) substrate) 101 ° In figure 2c, a silicon oxide layer 11 is formed on the semiconductor substrate by a plasma chemical vapor deposition (p) asma Enhanced CVD method. On the surface, the thickness of the silicon oxide layer is between about 900 and 3500 angstroms. The oxidized stone layer mentioned above can be formed by any of the chemical vapor deposition methods (Chenucal Vapor Deposition). For example, Ap is limited to PECVD. This oxidized stone layer 11 series uses "as a second plant"
Im = V日或Λ熱擴散製程me·1…㈣-)的幕軍 減少離子植入時之破壞的犧牲層( bacriiiciai Layer) 〇 極之圖巾’乃使用著名的微影技術來決定源極/沒 熱擴散製程趨入第一摻雜質,該第 1用 質之導通型係相反於上述半導體基板之= 第二摻二示,係採用相同步驟形成該源極"及極之 :相同=(,Γ)130及131 ’其内之第二摻雜質之導通型 第-摻雜區之導通型’ 1其摻雜漠度大於該 t雊&之摻雜濃度。 刻出中,幕罩層產生’採用渠溝隔離法圖案餘 溝槽U0,其深度相當於^^井〗之深度但不超越。 第11頁 44s72 五、發明說明(9) 在第二G圖中’係利用保角覆蓋(conf ormai)式的沉積 法沿邊形成一氧化矽層1 5 0 ’此層也可採用氮化矽為材質 ’遠氧化矽層覆蓋在第一溝槽1 4 0之底部表面和側壁上及 源極/汲極之頂部表面。此氧化矽層丨5〇不能使用化學氣相 沉積法形成,否則整個第一溝槽】4〇將會被填滿,其會影 響往後閘極的接觸面積。因此,應使用黏置性較高的結構 ’其流動性較低。 在第二}{圖中,回蝕刻源極/汲極頂部表面之氧化矽層 1_5 0至氧化矽層11〇之高度。隨後,產生幕罩層及採用渠溝 隔離法圖案蝕刻出第二溝槽丨7 〇,其深度超越該第一溝槽 1 4〇之深度,且其寬度較第一溝槽窄。第二溝槽1 70之側壁 加底部的長度相當於閘極之長度。當第二溝槽1 7〇產生後 ,一間隙壁160也隨即形成於該第一溝槽丨4〇之側壁及部份 底。卩表面上,此間隙壁是一絕緣層,其用來作閘極電極之 邊緣的著力點。 1 8 0於第二溝槽 在第二I圖中,沿邊形成一閘氧化層 1 7 0底部的表面及側壁上。 ί 1 η Ϊ 圖令,回蝕刻源極/汲極頂部表面之氧化矽層 Ϊ頂部表面。其後,採用低壓化學氣相沉積法 替個亓型摻雜多晶矽U〇Ped P〇lysilicon)層於 面上及填滿第一溝槽和第二溝槽,之後,回蝕Im = V day or Λ thermal diffusion process me · 1 ... ㈣-) The sacrifice layer (bacriiiciai Layer) that reduces the damage during ion implantation 〇 The map of the pole 'uses the famous lithography technology to determine the source / No thermal diffusion process goes to the first dopant, the first type of conductive type is opposite to the above semiconductor substrate = the second doping is shown, the source electrode is formed using the same steps " and the pole: the same = (, Γ) 130 and 131 'The conduction type of the second dopant within the conduction type of the first-doped region'1 has a doping degree greater than the doping concentration of t 雊 &. During the engraving, the curtain cover layer is formed with a trench trench isolation pattern U0, the depth of which is equal to the depth of ^^ well but does not exceed. Page 11 44s72 V. Explanation of the invention (9) In the second G chart, 'a silicon oxide layer 1 50 is formed along the edge using a conformal covering (conf ormai) type deposition method.' This layer can also be made of silicon nitride. The material 'far silicon oxide layer covers the bottom surface and sidewalls of the first trench 140 and the top surface of the source / drain. This silicon oxide layer 50 cannot be formed by chemical vapor deposition, otherwise the entire first trench] 40 will be filled, which will affect the contact area of the gate in the rear. Therefore, a structure with higher adhesion should be used because its fluidity is lower. In the second} {figure, the silicon oxide layer 1-50 on the top surface of the source / drain is etched back to a height of 110. Subsequently, a mask layer is generated and a second trench 171 is etched with a trench isolation method pattern, the depth of which exceeds the depth of the first trench 140, and its width is narrower than that of the first trench. The length of the side wall and the bottom of the second trench 1 70 is equivalent to the length of the gate. When the second trench 170 is generated, a spacer 160 is also formed on the side wall and a part of the bottom of the first trench 400. On the surface, the spacer is an insulating layer, which is used as the point of force for the edge of the gate electrode. 180 in the second trench In the second I picture, a gate oxide layer 170 is formed along the edge on the bottom surface and on the sidewall. ί 1 η Ϊ Command, etch back the silicon oxide layer Ϊ top surface of the source / drain top surface. After that, a low-pressure chemical vapor deposition method was used to replace a 亓 -type doped polycrystalline silicon (UoPed Polysilicon) layer on the surface and fill the first trench and the second trench.
第12頁 425672 五、發明說明(ίο) _____ 刻該多晶砍層:形成1層 ;^— 與N井2之頂部表面等高。 兮扣 其裸露之表面 矽化合物或金屬類的材質形成。i閘極電極也可採用多晶 最後如第—K圖所示, 雜濃度之離子以形成—筮=边& 壤散表程趨入第三推 形成N+型源極2〇。及N+型汲極2 Η &其於表原面極就和二極區中,既 極區之表面,該第三摻雜區内之摻雜質之導疋通該型1極/没 上述第-及第二摻雜區,且其摻雜濃度大 1同於 其不單可減少佔據之= :例卜 並且能提高崩潰電壓及避免崩潰電壓提早發生:動犯力’ J發:另二實施例描述於第二L圖中,其結 和上述之第一《施非常相似,唯一不同之處是第—溝% 挖掘至N井2之底部的深度,及第二溝槽未超越N井1層,只 也使得該結構擁有較小的間隙壁但較長的通道。然而j, 構上有異但擁有相同的功能及優勢。 結 以上所述僅為本發明之較佳實施例而已,並非用以 定本發明之申請專利範圍;凡其它未脫離本發明所揭示限 精神下所元成之等效改變或修飾,均應包含在下述之申^ 專利範圍内。 sfPage 12 425672 V. Description of the invention (ίο) _____ Carved the polycrystalline cutting layer: to form 1 layer; ^ — the same height as the top surface of N well 2. The exposed surface is made of silicon compounds or metal materials. The i-gate electrode can also be polycrystalline. Finally, as shown in Fig. -K, ions with heteroconcentrations are formed to form-筮 = edge & And N + -type drain electrode 2 Η & it is on the surface of the original electrode and in the diode region, that is, the surface of the pole region, the conductivity of the dopant in the third doped region leads to the type 1 pole / not mentioned above The first and second doped regions, and their doping concentration is greater than 1 can not only reduce the occupation = = Example and can increase the breakdown voltage and prevent the breakdown voltage from occurring earlier: violent force 'J hair: another implementation The example is described in the second L diagram, and its knot is very similar to the first one described above. The only difference is that the depth of the first trench is excavated to the bottom of N well 2 and the second trench does not exceed N well 1. The layer only makes the structure have smaller partition walls but longer passages. However, j is structurally different but has the same functions and advantages. The above description is only a preferred embodiment of the present invention, and is not intended to determine the scope of the patent application of the present invention; all other equivalent changes or modifications made without departing from the spirit of the limits disclosed by the present invention should be included below Said within the scope of the patent. sf
第13頁Page 13
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW88107367A TW425672B (en) | 1999-05-06 | 1999-05-06 | Forming HV-CMOS with grading doping electrode |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW88107367A TW425672B (en) | 1999-05-06 | 1999-05-06 | Forming HV-CMOS with grading doping electrode |
Publications (1)
Publication Number | Publication Date |
---|---|
TW425672B true TW425672B (en) | 2001-03-11 |
Family
ID=21640567
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
TW88107367A TW425672B (en) | 1999-05-06 | 1999-05-06 | Forming HV-CMOS with grading doping electrode |
Country Status (1)
Country | Link |
---|---|
TW (1) | TW425672B (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2016070844A1 (en) * | 2014-11-07 | 2016-05-12 | Lighthouse Technologies Limited | Indoor smd led equipped for outdoor usage |
CN111668293A (en) * | 2019-03-07 | 2020-09-15 | 英飞凌科技股份有限公司 | Semiconductor device including trench structure and method of manufacturing |
-
1999
- 1999-05-06 TW TW88107367A patent/TW425672B/en not_active IP Right Cessation
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2016070844A1 (en) * | 2014-11-07 | 2016-05-12 | Lighthouse Technologies Limited | Indoor smd led equipped for outdoor usage |
CN111668293A (en) * | 2019-03-07 | 2020-09-15 | 英飞凌科技股份有限公司 | Semiconductor device including trench structure and method of manufacturing |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US6174773B1 (en) | Method of manufacturing vertical trench misfet | |
KR100305978B1 (en) | Field-effect trench transistors with lightly doped epitaxial regions on the surface of transistors | |
US8362552B2 (en) | MOSFET device with reduced breakdown voltage | |
TWI353025B (en) | Semiconductor structure with improved on resistanc | |
US8940606B2 (en) | Method for fabricating trench type power transistor device | |
US8969953B2 (en) | Method of forming a self-aligned charge balanced power DMOS | |
TWI475614B (en) | Trench device structure and fabrication | |
CN101375402B (en) | Transverse SOI semiconductor devices and manufacturing method thereof | |
JP2011512677A (en) | Semiconductor device structure and related processes | |
US20210273091A1 (en) | Split trench gate super junction power device | |
US8587061B2 (en) | Power MOSFET device with self-aligned integrated Schottky diode | |
US6777745B2 (en) | Symmetric trench MOSFET device and method of making same | |
CN101043053B (en) | Power semiconductor device having improved performance and method | |
TW201023361A (en) | Structures and methods for forming high density trench field effect transistors | |
CN109119461B (en) | Super-junction MOS type power semiconductor device and preparation method thereof | |
JP2009520365A (en) | Super junction power MOSFET | |
CN212676274U (en) | Charge balance power device | |
US20070034895A1 (en) | Folded-gate MOS transistor | |
JP4990458B2 (en) | Self-aligned silicon carbide LMOSFET | |
JPH11274313A (en) | Semiconductor device and its manufacture | |
CN103545356A (en) | Novel metal/polysilicon gate trench power MOSFET | |
CN105826360B (en) | Groove-shaped half super junction power device and preparation method thereof | |
US7572703B2 (en) | Method for manufacturing a vertical-gate MOS transistor with countersunk trench-gate | |
CN116936611B (en) | Low-loss bidirectional conduction IGBT structure and preparation method | |
US6133606A (en) | High voltage complementary semiconductor device (HV-CMOS) with gradient doping electrodes |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
GD4A | Issue of patent certificate for granted invention patent | ||
MK4A | Expiration of patent term of an invention patent |