TW434900B - Insulated gate bipolar transistor with controllable latch - Google Patents
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Description
4349〇〇 五、發明說明⑴ — 發明領域 本發明係有關一種功率電子裝置,特別是關於一種可 控制閃鎖之絕緣閘雙載子半導體元件者。 發明背景 諸如馬達驅動電路及照明設備等高功率應用的半導體 裝置的發展始於雙載子接面電晶體(Bip〇lar junct i〇n Transistor; BJT)。雖然bjT能夠符合許多需求,卻也存 在許多基本的缺失使其難以滿足所有的高功率應用,例如 ’ B J T係一電流控制元件,其驅動電路較為複雜且昂貴, 並且輸入阻抗仍太低。功率金氧半場效電晶體(p〇wer 、 M0SFET)被提出來解決既有的困難,在一功率M〇SFET中, 一閘極電極偏壓被用來作為打開及關閉元件的控制。雖然 功率M0SFET具有許多優點,卻被其相當高的導通電阻所抵 消’此乃由於其欠缺少數載子(minority carrier)傳輸, 結果導致元件之操作順向電流密度受到侷限。基於功率 BJT與M0SFET的特點,結合雙載子電流傳導及M〇s控制電流 流通的混合式元件被發展出且提供超越β 或M0SFET的顯 著優點’絕緣閘極雙載子電晶體(Insulated Gate Bipolar Transistor; IGBT)及射極切換式閘流體 (Emitter Switching Thyristor; EST)乃是其中的二種。 」 一個典型的IGBT如第一圖所示’其包括p+集極區域1〇 ' N+缓衝層12、N-漂移層14、P型基極區域〗6及…射極區 -域1 8 ’基極區域1 6上方設有閘極2 0,二者之間形成有閑極 氧化層2 2,元件二側的金屬層2 4及2 6分別為射極與集極電4349〇 V. Description of the Invention ⑴-Field of the Invention The present invention relates to a power electronic device, and more particularly to an insulated gate bipolar semiconductor device capable of controlling a flash lock. BACKGROUND OF THE INVENTION The development of semiconductor devices for high-power applications such as motor drive circuits and lighting equipment began with bipolar junction transistors (BJT). Although bjT can meet many requirements, there are also many basic defects that make it difficult to meet all high-power applications. For example, ‘B J T is a current control element whose driving circuit is more complex and expensive, and the input impedance is still too low. Power metal-oxide-semiconductor field-effect transistors (POWER, MOSFET) have been proposed to solve the existing difficulties. In a power MOFET, a gate electrode bias is used to control the opening and closing elements. Although the power MOSFET has many advantages, it is canceled by its rather high on-resistance. This is due to its lack of a minimum carrier transmission, and as a result, the forward current density of the device is limited. Based on the characteristics of power BJT and M0SFET, a hybrid element combining bi-carrier current conduction and Mos control current flow has been developed and offers significant advantages over β or M0SFET 'Insulated Gate Bipolar Transistor (Insulated Gate Bipolar Transistor) Transistor (IGBT) and Emitter Switching Thyristor (EST) are two of them. '' A typical IGBT is shown in the first figure 'It includes p + collector region 10' N + buffer layer 12, N-drift layer 14, P-type base region 6 and ... emitter region-domain 1 8 ' A gate electrode 20 is provided above the base region 16 and a free oxide layer 22 is formed between the two. The metal layers 24 and 26 on the two sides of the element are the emitter and collector respectively.
第5頁 43 49 〇 〇Page 5 43 49 〇 〇
五、發明說明(2) 極區域。由於IGBT在開啟態下漂移區域的傳導調變 (conductivity modulation),其開啟態損失(⑽ 1〇33)遠 低於功率M0SFET。即使如此’更低的傳導損失仍被期待以 閘流體來達成’這是因為閘流體在打開時提供比IG β τ更高 程度的傳導調變及更低的順向壓降。V. Description of the invention (2) Polar region. Due to the conductivity modulation of the drift region of the IGBT in the on-state, its on-state loss (⑽103) is much lower than the power MOSFET. Even so, 'lower conduction losses are still expected to be achieved with gate fluids' because the gate fluids provide a higher degree of conduction modulation and lower forward pressure drop than IG β τ when opened.
第二圖提供一個EST的結構示意圖,其包括ρ+陽極區 域3 0、Ν+缓衝層32、Ν-漂移層34、Ρ型基極區域36、Ν+浮 動區域38及Ν+陰極區域40 ’閘極42位於浮動區域38及陰極 區域4 0之間的上方’且閘極氧化層4 4介於其間,金屬層4 6 及48分別為陰極與陽極,電極區域。很不幸地,由於存在寄 生閘流體,此元件可能發生閂鎖現象而造成無法關閉,進 而導致,燒毀。· 如第三圖所示的’ I GBT在使用壕溝閘極2 0 ’後可以抑 制閃鎖現象,不過其導通阻值調變的效應仍難以和EST相 比’並且其壕溝需承受較高的電壓。而EST由於結構本身 之特性使其無法以壕溝形成閘極,因此閂鎖效應不可避免 〇 針對IGBT或EST的缺失尚有其他許多努力加以改善。 Bauer等人在美國專利號碼4, 985, 74 ι中於IGBT中埋設復合 層(recombination layer)以避免閂鎖發生,Sakurai亦在 美國專利號碼5,0 8 9,8 6 4中抑制IG B T的閂鎖現象,The second figure provides a schematic diagram of the structure of EST, which includes p + anode region 30, N + buffer layer 32, N-drift layer 34, P-type base region 36, N + floating region 38, and N + cathode region 40. 'The gate 42 is located above the floating region 38 and the cathode region 40' and the gate oxide layer 44 is interposed therebetween, and the metal layers 46 and 48 are the cathode, anode, and electrode regions, respectively. Unfortunately, due to the presence of a parasitic fluid, this element may latch up and fail to close, resulting in burnout. · As shown in the third figure, 'I GBT can suppress the flash-lock phenomenon after using the trench gate 20', but its on-resistance modulation effect is still difficult to compare with EST 'and its trench needs to withstand higher Voltage. However, due to the characteristics of the EST, it is impossible to form a gate with a trench, so the latch-up effect is inevitable. There are many other efforts to improve the lack of IGBT or EST. Bauer et al. Embedded a recombination layer in the IGBT in U.S. Patent No. 4,985,74 to prevent latch-up. Sakurai also suppresses IG BT in U.S. Patent No. 5,0 8,9,8 6 4 Latch-up,
Fu j lhira等人在美國專利號碼5, 〇97, 3〇2中偵測負載電流 以避免IGBT燒毀’ Sakurai在美國專利號碼5, 200, 632中改 善的傳導調變,Hiraki等人及Iwamura分別在美國專Fu j lhira et al. Detected load current in U.S. Patent No. 5, 〇97,302 to avoid IGBT burnout 'Sakurai improved conduction modulation in U.S. Patent No. 5,200,632, Hiraki et al. And Iwamura respectively Specialized in the U.S.
第6頁 434c 五、發明說明(3) 利號碼5,2 8 2, 0 1 8及5, 6 5 9,1 8 5中藉增加壕溝深度及雙重閘 極降低IGBT的導通阻值,Ba 1 i ga在美國專利號碼 5,306,930中以及She kar等人在美國專利號碼5, 293, 〇54和 5,2 94, 8 1 6中所提出的EST利用各種不同的機制來抑制寄生 閘流體的閂鎖效應,Otsuki等人在美國專利號碼 5, 378, 90 3中整合IGBT及EST,Shekar等人亦在美國專利。虎 碼5, 471,075中利用雙通道壕溝型FET抑制EST的問鎖效應& ,Sakurai等人、Seki及Iwamura分別在美國專利號石 丨'、 5,459,339、5,349,212 及5,644,150 中利用雙閘拖 ^ 流體結構及I G B T狀態而降低元件的導通壓降,a j丨 ' 尸、 專利號碼5, 719, 41 1中消彌EST的寄生間流體的結^在^, 美國專利號碼5, 844, 258中控制電洞電流在流入主 在 前進入間流體的陰極以避免EST的寄生問流體被 '極之 而,這些習知技藝不能同時解決前述所有的問題,^ ,其他的缺失,因A,高輸入p且抗、低導 、=帶 塵、高導通電流密度且不受閃鎖侵害的雙載^電 被期待的。 电曰曰體仍是 發明目的與概述 針對上述種種缺失,本發明提供_ 控制閃鎖之絕緣閘雙載子電晶體,直 达應用的可 詳言之,此閘流體具有第一導雷二 卜 ㈤机體結構, 第一區域上之第二導電型態之第二 报出认―形成於 上之第一導電型態之第三區域,迓成於第二區域 區域接觸第三區域益形成卜N接弟一導電一型態之第四 弟一及弟二區域分別Page 6 434c V. Description of the invention (3) Profit numbers 5, 2 8 2, 0 1 8 and 5, 6 5 9, 1 8 5 Increase the trench depth and double gate to reduce the IGBT on-resistance, Ba 1 The ESTs proposed by iga in U.S. Patent No. 5,306,930 and She kar et al. in U.S. Patent Nos. 5,293,055 and 5,2 94,8 1 6 use a variety of different mechanisms to suppress the For the latch-up effect, Otsuki et al. Integrated IGBT and EST in US Patent No. 5, 378, 90 3, and Shekar et al. Also in US patent. Tiger code 5, 471,075 using a dual channel trench FET to suppress the interlocking effect of EST & Sakurai et al., Seki and Iwamura use double gates in U.S. Patent Nos. '5,459,339, 5,349,212 and 5,644,150 respectively Drag the fluid structure and the IGBT state to reduce the on-state voltage drop of the device. Aj 丨 'corpse, Patent No. 5, 719, 41 1 Eliminate the interstitial fluid of EST's parasitic fluid ^ In US Patent No. 5, 844, 258 In the control of the hole current flowing into the cathode of the main fluid before entering the main fluid to avoid the parasitics of the EST, the fluid cannot be eliminated. These techniques cannot solve all the problems mentioned above at the same time. Double-resistance, low-conductance, low-conductance, = dusting, high-conduction-current-density, and unaffected by flash-lock are expected. Electricity is still the purpose and summary of the invention. In view of the above-mentioned shortcomings, the present invention provides an insulated gate bipolar transistor for controlling flash locks. For direct applications, it can be said in detail that this gate fluid has a first lead and a second lead. Body structure, the second report of the second conductivity type on the first region-the third region of the first conductivity type formed on the first region, formed in the second region to contact the third region to form N Receiving one conductive one type of the fourth and first two areas respectively
43 4 五、發明說明(4) 接觸第一及第二電極區域;另二場效電晶體結構被用來控 制閘流體的開啟及關閉,其中,第一場效電晶體因應一開 啟偏壓信號而導通第四區域至第二區域,第二場效電晶體 介於第四區域與第二電極區域之間,因應一截斷偏壓信號 而關閉閘流體。 二場效電晶體皆可使用平面閘極或壕溝閘極。當二場 效電晶體被打開,第一至第四區域所構成的閘流體導通, 其上之壓降甚低;而藉由改變第二場效電晶體的閘極電壓 能夠截斷閘流體的電子流通路徑,強迫閘流體關閉,使得 此半導體元件具有可控制閂鎖的能力。因此,本發明能夠 達到高輸入阻抗、低導通壓降、耐高電壓、高導通電流密 度以及可控制閂鎖的目的。 圖式簡單說明 對於熟習本技藝之人士而言,從以下所作的詳細敘述 配合伴隨的圖式,本發明將能夠更清楚地被瞭解,其各種 目的及優點將會變得更明顯。 1. 圖式說明: 第一圖係一典型的IG B T之剖視圖。 第二圖係一習知的EST之剖視圖。 第三圖係一習知的壕溝型I G B T之剖視圖。 第四圖係本發明之較佳實施例之剖視圖。 第五圖係本發明另一實施例之剖視圖。 第六圖係本發明又一實施例之剖視圖。 2. 圖號說明:43 4 V. Description of the invention (4) Contacting the first and second electrode regions; the other two field effect transistor structures are used to control the opening and closing of the gate fluid. Among them, the first field effect transistor responds to an open bias signal. And the fourth region to the second region is turned on, and the second field effect transistor is interposed between the fourth region and the second electrode region, and the gate fluid is closed in response to a cutoff of the bias signal. Both field-effect transistors can use planar gates or trench gates. When the two field-effect transistors are turned on, the gate fluid formed by the first to fourth regions is turned on, and the voltage drop thereon is very low; and by changing the gate voltage of the second field-effect transistor, the electrons of the gate fluid can be cut off. The flow path forces the sluice fluid to close so that this semiconductor element has the ability to control the latch. Therefore, the present invention can achieve the objectives of high input impedance, low on-voltage drop, high voltage resistance, high on-current density, and controllable latch-up. Brief Description of the Drawings For those skilled in the art, the present invention will be more clearly understood from the detailed descriptions made with the accompanying drawings, and its various purposes and advantages will become more apparent. 1. Schematic description: The first diagram is a cross-sectional view of a typical IG B T. The second figure is a cross-sectional view of a conventional EST. The third figure is a cross-sectional view of a conventional trench type I G B T. The fourth figure is a sectional view of a preferred embodiment of the present invention. The fifth figure is a sectional view of another embodiment of the present invention. The sixth figure is a sectional view of another embodiment of the present invention. 2. Drawing number description:
第8頁 434900 五、發明說明(5) 10 集 極 1¾ 域 14 漂 移 層 18 射 極 區 域 22 閘 極 氧 化 層 26 集 極 電 極 區域 32 緩 衝層 36 基 極 區 域 40 陰 極 區 域 44 閘 極 氧 化 層 48 陽 極 電 極 區域 52 P + 基 底 12 緩衝層 16 基極區域 2 0/ 20*閘極 24 射極電極區域 30 陽極區域 34 漂移層 38 浮動區域 42 閘極 46 陰極電極區域 50 漂移層 54 緩衝層 58 N型井 62 N +區域 66 絕緣層 70 絕緣層 74 第二電極區域 78 平面閘極Page 8 434900 V. Description of the invention (5) 10 Collector 1¾ Domain 14 Drift layer 18 Emitter region 22 Gate oxide layer 26 Collector electrode region 32 Buffer layer 36 Base region 40 Cathode region 44 Gate oxide layer 48 Anode Electrode region 52 P + substrate 12 Buffer layer 16 Base region 2 0/20 * Gate 24 Emitter electrode region 30 Anode region 34 Drift layer 38 Float region 42 Gate 46 Cathode electrode region 50 Drift layer 54 Buffer layer 58 N-type Well 62 N + region 66 Insulating layer 70 Insulating layer 74 Second electrode region 78 Planar gate
56 P型井 6〇 P型基極區域 6 4 平面閘極 6 8壕溝閘極 72第一電極區域 76 N+區域 8 0壤溝閘極 詳細說明 第四圖提供本發明一較佳實施例之剖視圖。此元件之 形成係沉積一N-漂移層50於一P+基底52上,並且如同—般 的IGBT或EST的構造一樣,在漂移層5〇與基底52之間更形& 成一N+緩衝層54,漂移層50的另一面形成p型井56,然後 於?型井56内依序形成二相反導電型態的井58及?型基極區56 P-type well 60-P-type base region 6 4 Planar gate 6 8 Trench gate 72 First electrode region 76 N + region 8 0 Trench gate Detailed description The fourth figure provides a cross-sectional view of a preferred embodiment of the present invention . The formation of this element is to deposit an N-drift layer 50 on a P + substrate 52, and to form an N + buffer layer 54 between the drift layer 50 and the substrate 52 as in the general IGBT or EST structure. A p-type well 56 is formed on the other side of the drift layer 50, and then? Wells 58 of two opposite conductivity types are sequentially formed in the well 56? Base region
第9頁 4349 Ο ο 五、發明說明(6) 域60,Ρ型基極區域6 0之表面再形成Ν+區域62 型井56與 漂移層50鄰接區域之表面上方形成一平面閘極64,一絕緣 層66介於閘極64與Ρ型井56表面之間,Ρ型井56表面接近閘 極64之區域即形成一受控於閘極64之通道。 此元件之另一控制功能手段係藉壕溝閘極68,壕溝係 從Ν+區域62的表面向下貫穿Ν+區域62及Ρ型基極區域60, 並且進入Ν型井58中,壕溝具有底面及側壁,其與閘極68 之間形成有絕緣層7 0,使得壕溝之側壁外形成一受控於閘 極6 8之通道。如同圖中所示,在此實施例中,閘極6 4及6 8 係連接至同一電極信號,這可以利用一導電層(圖中未示 出)連接閘極64及68來達成,此係一般熟知積體電路技術 者應當瞭解的,不另詳細敘述。而在不同的實施例中,閘 極64及68亦可利用二不同的電極G1及G2分別控制,以便獲 得不同的電晶體特性。 最後’於此元件的上、下分別形成金屬層72及74作為 此元件的電極區域,其中,第一電極區域72接觸Ρ型井5 6 、Ρ型基極區域60及Ν+區域62的上表面,而第二電極區域 74則接觸Ρ+基底52。 現在說明此元件的操作原理及過程。當閘極電極 G1/G2被施予一適當的電壓,使得閘極64及68所控制的通 道被打開,電子從Ν+區域62經由閘極68所控制的通道注入 Ν型井58 ’再經由閘極64所控制的通道注入漂移層50。另 —方面’電洞則循著電子路徑之相反方向,從漂移層5〇注 入Ρ型井56 ’再由ρ型井56的金屬接觸流出,因而引發ρ型Page 9 4349 Ο ο V. Description of the invention (6) The surface 60, the P-type base region 60 and the N + region 62 are formed on the surface of the type well 56 and the surface adjacent to the drift layer 50 to form a planar gate 64. An insulation layer 66 is interposed between the gate electrode 64 and the surface of the P-type well 56, and the area near the gate electrode 64 on the surface of the P-type well 56 forms a channel controlled by the gate electrode 64. Another control function of this element is through the trench gate 68. The trench passes through the N + region 62 and the P-type base region 60 from the surface of the N + region 62 and enters the N-type well 58. The trench has a bottom surface. And a side wall, an insulating layer 70 is formed between the gate 68 and the gate 68, so that a channel controlled by the gate 68 is formed outside the side wall of the trench. As shown in the figure, in this embodiment, the gate electrodes 6 4 and 6 8 are connected to the same electrode signal. This can be achieved by connecting the gate electrodes 64 and 68 with a conductive layer (not shown in the figure). Those who are generally familiar with integrated circuit technology should understand that it will not be described in detail. In different embodiments, the gates 64 and 68 can also be controlled by two different electrodes G1 and G2, respectively, so as to obtain different transistor characteristics. Finally, metal layers 72 and 74 are formed above and below the element as electrode regions of the element, respectively, wherein the first electrode region 72 contacts the P-type well 5 6, the P-type base region 60 and the N + region 62 above. Surface, and the second electrode region 74 contacts the P + substrate 52. The operating principle and process of this element will now be explained. When a suitable voltage is applied to the gate electrodes G1 / G2, the channels controlled by the gates 64 and 68 are opened, and electrons are injected from the N + region 62 through the channel controlled by the gate 68 into the N-well 58 'and then The channel controlled by the gate electrode 64 is injected into the drift layer 50. On the other hand, the “hole” follows the opposite direction of the electron path, and is injected into the P-type well 56 from the drift layer 50 and then flows out from the metal contact of the ρ-type well 56, thereby initiating the ρ-type
第10頁 五、發明說明C7) 井56及N型井58之接面順向偏壓,進而造成基底52、漂移 層50、P型井56及N型井58所形成的閘流體導通,此閘流體 一旦導通即發生閂鎖現象’其上之壓降將非常地低。另一 方面,此閘流體可以利甩閘極68截斷其電子流通路徑,而 將此元件關閉’換言之,此絕緣閘雙載子電晶體具有可控 制閂鎖的能力。 與壕溝型I GBT相比較,本發明所提供的電晶體不需耐 南電壓之壕溝,並且具有更低的導通壓降d與£3了相比較 ’本發明所提供的電晶體不但具有更低的導通壓降,而且 不會發生不可控制之閂鎖而使元件燒毀。 第四圖所示實施例係以P型基板為基礎形成此半導體 元件’在其他實施例中,可以使用N型基板來製造此元件 ’此時係將N型基板當作漂移層,於其背侧依序形成N+緩 衝層及P+層,N型基板的另一側則形成如前一實施例的構 造。 h第四圖所示裝置的說明可以發現本發明的特點,在 一可控制閂鎖之絕緣閘雙載子電晶體中,包括有一閘流體 f構及至少二場效電晶體結構,閘極64因應—開啟偏壓信 號而使N型井58經由通道電性連接至漂移層5〇,另一場效 電晶體則介於電極區域72與N型井58之間,其閘極68能夠 因應一截斷偏壓信號而阻隔閘流體的電子流通路徑,強迫 閘流體關閉,從而避免不可控制的閂鎖現象發生。 為截斷閘流體的電子流通路徑,第二場效電晶體亦可 使用平面閘極,第五圖顯示—實施例之剖視圖。在此元件Page 10 V. Description of the invention C7) The junctions of the well 56 and the N-type well 58 are forward biased, which in turn causes the sluice fluid formed by the base 52, the drift layer 50, the P-type well 56 and the N-type well 58 to conduct. Once the brake fluid is turned on, a latch-up phenomenon occurs, and the pressure drop thereon will be very low. On the other hand, the gate fluid can use the gate 68 to intercept its electronic flow path and close the element. In other words, the insulated gate bipolar transistor has the ability to control the latch. Compared with trench type I GBT, the transistor provided by the present invention does not need a trench withstand south voltage, and has a lower on-state voltage drop d. Compared with £ 3, the transistor provided by the present invention not only has a lower The on-state voltage drop, and the uncontrollable latch-up will not cause the component to burn out. The embodiment shown in the fourth figure is based on a P-type substrate to form this semiconductor element. In other embodiments, an N-type substrate can be used to manufacture this element. At this time, the N-type substrate is used as a drift layer. An N + buffer layer and a P + layer are sequentially formed on one side, and the structure on the other side of the N-type substrate is formed as in the previous embodiment. h The description of the device shown in the fourth figure can find the characteristics of the present invention. An insulated gate bipolar transistor with a controllable latch includes a gate fluid f structure and at least two field effect transistor structures. The gate electrode 64 Correspondence—The N-well 58 is electrically connected to the drift layer 50 through the channel by turning on the bias signal, and another field-effect transistor is located between the electrode region 72 and the N-well 58, and its gate 68 can be cut off according to a The bias signal blocks the electronic flow path of the gate fluid, forcing the gate fluid to close, thereby preventing uncontrollable latch-up. In order to cut off the electronic flow path of the gate fluid, the second field-effect transistor can also use a planar gate. The fifth figure shows a cross-sectional view of the embodiment. In this component
第11頁 4 3 49^0 五、發明說明(8) ~ ' — 中,閘流體及第一場致電晶體之構造與第四圖所示 同,但第二場效電晶體改用平面閘極78,其係位於ρ型基 極區域60表面上方,控制從…區域76至1^型井58之間的二 道。二場效電晶體的閘極64及78可以使用同一層多晶矽形 成,如此一來簡化製程《雖然前述實施例使用了平面閘極 6 4,但熟白此項技藝之人士當知,實施例中的平面閘極6 4 可以壕溝閘極取代’第六圖顯示這個情況,在此電晶體 中,二場效電晶體的閘極6 8及8 0皆使用壕溝閘極。 以上對於本發明之較佳實施例所作的敘述係為闡明之 目的,而無意限定本發明精確地為所揭露的形式,基於以 上的教導或從本發明的實施例學習而作修改或變化是可能 的,實施例係為解說本發明的原理以及讓熟習該項技術者 以各種實施例利用本發明在實際應用上而選擇及敘述,本 發明的技術思想企圖由下列的申請專利範圍及其均等來決 定。Page 11 4 3 49 ^ 0 V. Description of the invention (8) ~ '— In the structure of the gate fluid and the first field-transmitting crystal is the same as that shown in the fourth figure, but the second field-effect transistor is replaced by a planar gate. 78, which is located above the surface of the p-type base region 60 and controls two paths from ... region 76 to 1 ^ -type well 58. The gates 64 and 78 of the two field-effect transistors can be formed using the same layer of polycrystalline silicon. This simplifies the manufacturing process. "Although the previous embodiment uses a planar gate 64, those skilled in the art know that in the embodiment, The planar gate 6 4 can be replaced by a trench gate. The sixth figure shows this situation. In this transistor, the gates 68 and 80 of the two field-effect transistors use trench gates. The above description of the preferred embodiment of the present invention is for the purpose of clarification, and is not intended to limit the present invention to exactly the disclosed form. Modifications or changes are possible based on the above teaching or learning from the embodiments of the present invention. The embodiments are selected and described in order to explain the principles of the present invention and allow those skilled in the art to utilize the present invention in practical applications in various embodiments. The technical idea of the present invention is intended to be covered by the following patent applications and their equivalents. Decide.
第12頁Page 12
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US7745906B2 (en) | 2006-07-07 | 2010-06-29 | Mitsubishi Electric Corporation | Semiconductor device having spaced unit regions and heavily doped semiconductor layer |
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US7745906B2 (en) | 2006-07-07 | 2010-06-29 | Mitsubishi Electric Corporation | Semiconductor device having spaced unit regions and heavily doped semiconductor layer |
US7902634B2 (en) | 2006-07-07 | 2011-03-08 | Mitsubishi Electric Corporation | Semiconductor device |
US8008746B2 (en) | 2006-07-07 | 2011-08-30 | Mitsubishi Electric Corporation | Semiconductor device |
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