TW200814313A - Semiconductor device - Google Patents

Semiconductor device Download PDF

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Publication number
TW200814313A
TW200814313A TW96122236A TW96122236A TW200814313A TW 200814313 A TW200814313 A TW 200814313A TW 96122236 A TW96122236 A TW 96122236A TW 96122236 A TW96122236 A TW 96122236A TW 200814313 A TW200814313 A TW 200814313A
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Taiwan
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region
type
collector
base region
electrode
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TW96122236A
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Chinese (zh)
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TWI350001B (en
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Yoshinobu Kono
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Sanken Electric Co Ltd
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Abstract

The semiconductor device in accordance with the present invention is an IGBT which includes a first base area of a first conductive type; a second base area of a second conductive type, provided at one of main surfaces of the first semiconductor area; an emitter area of the first conductive type, which is formed in the second base area; a collector area of the second conductive type, which is formed at the other main surface of the first semiconductor area; and a collector short area of the first conductive type, which is formed at the other main surface of the first semiconductor area, in a manner such that the collector short area is inserted into the collector area, so as to divide the collector area. An external electrode forming part, where no second base area is formed, is provided at the periphery of one of the main surfaces of the first base area, and the second base area is formed in a cell forming area inside the external electrode forming part. The collector short area is formed only in the cell forming area.

Description

200814313 九、發明說明: 【發明所屬之技術領域】 縱型構造之絕 transistor)(以 本發明係關於一種具有用於積體電路之 緣閘極型雙極電晶體(insulated gate bip()lar 下稱為IGBT)之構造的半導體裝置。 【先前技術】 ^ IGBT係具有閘極,且藉由對該閘極施加電壓,可進 行電晶體之導通(0N)/不導通(〇FF)控制的雙極電晶體, 同時具有場效電晶體所具有之高輸入阻抗的特性、以及雙 極電晶體所具有之低輸出阻抗的特性的元件(device)。以 PNP型之lGBT之一例而言,有帛5圖所示之構造(例如參 照專利文獻1)。 弟5圖係頒示在集極區域侧使用了交替配置p型半導 體區域(集極區域)100與N型半導體區域(集極短路區 域之所谓況用基板(universal substrate)之IGBT之剖 I 面構造概念圖。 該IGBT係藉由磊晶成長法在上述汎用基板上依序形 成N型緩衝層1〇2、及n型基極區域1〇3。 此外’在N型基極區域1 〇 3的表面(圖示之上部側的 面)係藉由P型雜質擴散處理形成複數個P型基極區域 104 ’此外’在該p型基板區域1 内的表面係藉由n型 雜質擴散處理形成N型射極區域1〇5。 在各P型基極區域104間之N型基極區域103的表面 形成有閘極絕緣膜1 〇 6。 319357 5 200814313 在上述閘極絕緣膜106上形成有閘極電極1〇7,該閘 極電極107係由絕緣膜108所覆蓋。 P型基極區域104及N型射極區域1〇5係與射極電極 109電性連接。 • 此外,在汎用基板中之P型半導體區域1〇〇 型半 導體區域101的下面(圖示之下部側的面)形成有集極電極 no。藉此使p型半導體區域100&N型半導體區域ι〇ι 各個分別具有作為集極區域、集極短路區域的功能。 於上述腦T的構造中,亦會有在況用基板上未形成 N型緩衝層1〇2,而直接形成N型基極區域1〇3的情形。 在如上述之N型半導體區域1〇1所示具有作為集極短 路區域之作用的區域的励T中,係在半導體裝置内部形 成將N型基極區域103作為陰極,將p型基極區域ι〇4作 為陽極的PN接合面二極體(PN juncti〇n di〇de)。 第6圖係顯示第5圖之IGBT之等效電路概念圖,如 圖所示’ PN接合面二極體的陰極與IGBT之集極電極ιι〇 電性連接,PN接合面二極體的陽極與igbt之射極電極 1〇9電性連接。在此,PN接合面二極體係藉由N型半導體 區域1(Π、Ν型緩衝層1G2u型基極層(亦即心基極區 域’以下同)103構成陰極,陽極係由p型基極區域ι〇4所 構成。 藉由具有該集極短路區域的構造,可縮短由igbt之 導通(on)狀態移至不導通(〇ff)狀態的時間。 (專利文獻1)日本特開平05_〇32〇5號公報 319357 6 200814313 【發明内容】 (發明所欲解決之課題) 但是,上述PN接合面 以下所構成: 二極體的反向恢復時間 trr係由 ⑴上述PN接合面二極體的電流由順向電流值減少至「〇 為止,此外電流(以下稱為逆向電流)以逆向流通,該逆200814313 IX. Description of the invention: [Technical field of the invention] A permanent structure of a vertical structure (with the present invention relating to a gated bipolar transistor (insulated gate bip) under the edge of an integrated circuit A semiconductor device having a structure called IGBT. [Prior Art] ^ The IGBT has a gate, and by applying a voltage to the gate, it is possible to perform conduction (ON)/non-conduction (〇FF) control of the transistor. A polar transistor, which has both a high input impedance characteristic of a field effect transistor and a low output impedance characteristic of a bipolar transistor. In the case of a PNP type lGBT, there is a defect. 5 (see, for example, Patent Document 1). The second drawing shows that the p-type semiconductor region (collector region) 100 and the N-type semiconductor region (the collector short-circuit region) are alternately arranged on the collector region side. A schematic diagram of a cross-sectional structure of an IGBT of a universal substrate. The IGBT is formed by sequentially forming an N-type buffer layer 1 〇 2 and an n-type base region 1 on the above-mentioned general-purpose substrate by an epitaxial growth method. 〇 3. In addition' The surface of the N-type base region 1 〇3 (the surface on the upper side in the drawing) is formed by a P-type impurity diffusion process to form a plurality of P-type base regions 104' in addition to the surface in the p-type substrate region 1. The N-type emitter region 1〇5 is formed by the n-type impurity diffusion treatment. A gate insulating film 1〇6 is formed on the surface of the N-type base region 103 between the respective P-type base regions 104. 319357 5 200814313 A gate electrode 1〇7 is formed on the gate insulating film 106, and the gate electrode 107 is covered by an insulating film 108. The P-type base region 104 and the N-type emitter region 1〇5 are connected to the emitter electrode 109. In addition, a collector electrode no is formed on the lower surface (the surface on the lower side in the drawing) of the P-type semiconductor region 1 of the P-type semiconductor region in the general-purpose substrate. Thereby, the p-type semiconductor region 100 & Each of the N-type semiconductor regions ι〇ι has a function as a collector region and a collector short-circuit region. In the above-described structure of the brain T, an N-type buffer layer 1〇2 is not formed on the substrate for use, but directly The case where the N-type base region 1〇3 is formed. In the N-type semiconductor region 1〇1 as described above In the excitation T having the region functioning as the collector short-circuit region, a PN junction diode having the N-type base region 103 as a cathode and the p-type base region ι 4 as an anode is formed inside the semiconductor device. (PN juncti〇n di〇de). Fig. 6 shows the equivalent circuit concept diagram of the IGBT of Fig. 5, as shown in the figure 'The cathode of the PN junction diode and the collector electrode of the IGBT. Connected, the anode of the PN junction diode is electrically connected to the emitter electrode 1〇9 of the igbt. Here, the PN junction surface dipole system is formed by the N-type semiconductor region 1 (the Π, Ν type buffer layer 1G2u type base layer (that is, the core base region 'below the same) 103) constitutes a cathode, and the anode is composed of a p-type base. The structure of the region ι〇4. By the structure having the collector short-circuit region, the time from the on state of the igbt to the non-conduction state (〇ff) can be shortened. (Patent Document 1) Japanese Patent Laid-Open No. 05_ 〇32〇5号公告319357 6 200814313 [Problem to be Solved by the Invention] However, the PN junction surface is configured as follows: The reverse recovery time trr of the diode is based on (1) the PN junction surface diode The current is reduced from the forward current value to "〇, and the current (hereinafter referred to as reverse current) flows in the reverse direction.

=流成為,大值為止的時間,亦即pN接合面二極體 處於短路狀態的期間忭;以及 ⑺由逆向電流成為最大值的時間點至幾乎成為「 成為最大值之5%以下)為止的期間,亦即至州接合面 二極體發揮逆阻止(逆向電壓阻止)功能為止的期間 在此,當上述期严曰1 to豆於期ts時,一般而言可知 谷易對輸出產生振鈴(ringing),而容易產生因該振铃所引 起的雜訊(noise)。 為了減低該雜訊,必須具備使上述期間td比期間 長’亦即將td/ts形成為比習知例A的二極體特性(軟修復 (soft recovery)特性)。 另一方面,於上述之内建二極體之IGBT中,如第7 所示,當在射極電極,及集極電極m之間施加有 提高射極電極109侧之電位的電壓時(順偏壓狀態),使順 向電流流至將上述之N型基極區域1〇3設為陰極、p型基 極區域104設為陽極的PN接合面二極體(〇N狀態)。 隹接著,當在射極電極109及集極電極110之間施加使 集極電極110側的電位高於射極電極1〇9的電壓時(逆偏壓 319357 7 200814313 狀態),即藉由逆阻止功能而使?]^接合面二極體呈逆電犀 阻止狀態(OFF狀態)。 & 然而,於上述之習知之内建二極體之IGBt中,係於 與集極電極m相對向之一般基板的整面中,將集極區域 型半導體區域_與集極短路區域_半導體區域⑻ 交替連接於集極電極Π〇。 士為了+上述理纟,如第7_)所示,當形成逆偏麼狀態 w•,由於畜積在N型基極區域103等的電子會經由n型半 導體區域⑻(集極短路區域)而較早排出至集極電極㈣, 因此會有無法良好達成内建二極體之軟修復化的問題。 本發明係鑑於上述情形而研創者,與在风用基板整面 形成有集極短路區域的習知例相比較,係提供—種使上述 ㈣ω較期間ts長’亦即對PN接合面二極體實現軟修復 斗寸性,以減低雜訊之IGBT構造的半導體裝置。 (用以解決課題之手段) 本發明之半導體裝置係具有絕緣閘極型雙極電晶體構 造之半ΐ體裝置,其特徵為具有:第1導電型之第1基極 區或,第2 ‘電型之第2基極區域,設置在該第工基極區 域之一方之主面側;第1導電型之射極區域,形成在前述 弟2基極區域内;帛2導電型之集極區域,配置在前述第 土極區域之另一方之主面側;以及第工導電型之集極短 ^區域’在前述第i基極區域之另—方之主面側,以分割 :述ί極區域的方式’插介於集極區域間而形成,而且在 則述弟1基極區域之一方之主面側的外周部設置未形成有 319357 8 200814313 =第2基極區域的外部電極形成部’並將前述第2基極 區域形成在該外部電極形成部之内側的電晶體單元 (=nsistW)形成區域,將前述集極短路區域僅形成在前 述早元形成區域内。 較佳為前述集極短路區域係僅形成在以俯視觀之與前 处弟2基極區域相重疊的位置。 典型而言,在前述第1基極區域 在前述射極區域間設有間極電極/之—方主面側上部, 的溝=時’前述間極電極亦可設在形成在前述射極區域間 (發明之效果) 根據本發明,當集極短路區 極電晶體的單元形成區域^域配置在形成有縱型雙 極形成部未配置隼極:路巴=成有單元區域的外部電 部的第!其托「猎此形成有外部電極形成 合面二極體施加逆向錢層,當對叫接 修復特性。 王之PN接合面二極體的軟 亦即’根據本發明, 短路狀態的期間tS,將作為由逆向帝二極體處於 點至幾乎成為「 向包々,L成為隶大值的時間 阻止功能為的期間之PN接合面二極體發揮逆 刀月b為止的期間 奴知评延 例。 長,亦即使比例td/ts大於習知 319357 9 200814313 此外,根據本發明,於俯視中,由於在形成有縱型雙 極電晶體之單元形成區域形成有集極短路區域,亦即在存 在於形成有IGBT之下部的況用基板的區域形成有集極短 路區域’因此亦無損於可縮短IGBT< 〇FF動作時 項特性。 寸分 【實施方式】 實施形態之半導體裝置的 以下參知、圖不說明本發明一 IGBT 〇= the flow becomes a period until a large value, that is, a period in which the pN junction diode is in a short-circuit state; and (7) a time point from when the reverse current becomes the maximum value to almost "5% or less of the maximum value" During the period, that is, the period until the state of the junction electrode of the state exerts the reverse blocking (reverse voltage blocking) function, when the above period is strict to 1 to the bean ts, it is generally known that the valley is ringing the output ( Ringing), it is easy to generate noise caused by the ringing. In order to reduce the noise, it is necessary to have the period td longer than the period ', that is, td/ts is formed to be two poles than the conventional example A. On the other hand, in the IGBT of the built-in diode described above, as shown in Fig. 7, when the emitter electrode and the collector electrode m are applied, the improvement is performed. When the voltage of the potential on the side of the emitter electrode 109 (the forward bias state), the forward current flows to the PN junction in which the N-type base region 1〇3 is the cathode and the p-type base region 104 is the anode. Face diode (〇N state). 隹 Next, when in the emitter When the potential of the collector electrode 110 side is higher than the voltage of the emitter electrode 1〇9 between the pole 109 and the collector electrode 110 (reverse bias 319357 7 200814313 state), that is, by the reverse blocking function?]^ The junction surface diode is in an anti-electric rhinoceros blocking state (OFF state). However, in the above-described conventional built-in diode IGBt, it is in the entire surface of the general substrate opposite to the collector electrode m. , the collector region semiconductor region _ and the collector short region _ semiconductor region (8) are alternately connected to the collector electrode Π〇. For the above reason, as shown in the seventh _), when the reverse bias state w•, Since electrons accumulated in the N-type base region 103 and the like are discharged to the collector electrode (4) earlier through the n-type semiconductor region (8) (collector short-circuit region), soft repair of the built-in diode cannot be achieved well. The present invention has been made in view of the above circumstances, and compared with a conventional example in which a collector short-circuited region is formed on the entire surface of a wind substrate, the above-described (four) ω is longer than the period ts, that is, to the PN. The joint surface diode achieves a soft repairing fit to reduce A semiconductor device having an IGBT structure of noise. (Means for Solving the Problem) The semiconductor device of the present invention is a semiconductor device having an insulated gate type bipolar transistor structure, and is characterized in that: a base region or a second base region of the second 'electric type is disposed on one of the main surface sides of the first base region; and an emitter region of the first conductivity type is formed in the base region of the second base The collector region of the 帛2 conductivity type is disposed on the other main surface side of the first earth electrode region; and the collector short region of the work conductivity type is in the other side of the ith base region The main surface side is formed by the division: the method of describing the ф pole region is inserted between the collector regions, and the outer peripheral portion on the main surface side of one of the base regions of the first base is not formed with 319357 8 200814313 = The external electrode forming portion 'in the second base region> and the second base region are formed in a transistor unit (=nsistW) forming region inside the external electrode forming portion, and the collector short-circuit region is formed only in the foregoing The yuan is formed within the area. Preferably, the collector short-circuit region is formed only at a position overlapping with the front base 2 base region in plan view. Typically, in the first base region, an upper portion of the interpole electrode/the main surface side is provided between the emitter regions, and the trench is formed in the emitter region. (Effect of the Invention) According to the present invention, when the unit formation region of the collector short-circuit region of the polar transistor is disposed in the vertical bipolar formation portion, the drain is not disposed: the roadbar = the external electric portion having the unit region First! It is said that the external electrode is formed with an external electrode to form a counter-polar diode to apply a reverse layer of money, and when it is called a repairing property, the softness of the PN junction surface diode of the king is, that is, according to the present invention, the period tS of the short-circuit state, In the period from the point of the reverse dynasty diode to the PN junction surface of the period in which the PN junction diode is in the period of time, the PN junction diode is a period of time. Long, even if the ratio td/ts is larger than the conventional 319357 9 200814313. Further, according to the present invention, in a plan view, since a collector short-circuit region is formed in a cell formation region in which a vertical bipolar transistor is formed, that is, in existence The collector short-circuit region is formed in the region where the condition substrate of the lower portion of the IGBT is formed. Therefore, the IGBT&; FF operation time characteristic can be shortened. [Invention] The following description and diagram of the semiconductor device of the embodiment are shown. Does not explain an IGBT of the present invention

弟1圖係顯示上述-實施形態之IGBT之平面構造的 俯視圖12圖係第!圖之線a_a中之mBT之剖面構迭 的線視剖視圖(為便於圖示,記載為使單元(cell)形成區域2 、欠乍(減少P型基極區域104的個數))。 該IGBT之各單元的構造雖與第5圖所示之習知構造 相同’但於半導體裝置中形成㈣半導體區域⑻(集極短 路區域)的位i(亦即區域),在本實施开》態及習知例中並不 相同。習知例係於半導體裳置之況用基板整面中形成有华 極短路區域。另一方面,於本實施形態中,集極短路區: 係僅形成在供形成IGBT之電晶體單元的單元形成區域2。 亦即,以俯視觀之,在N型基極區域103之下部方向 的面(另一方之主面側),於隔介N型緩衝層1〇2而相對向 、:"用基板中’僅在與單元开)成區域2相重疊之汎用基板 的範圍,以將P型半導體區域1〇〇(集極區域)分割的方式 插在1>型半導體區域1QQ間而形成有N型半導體區域 319357 10 200814313 、,於本m靶形怨中,所謂俯視係用在從垂直於汎用基板 平面的方向觀看基板面,而顯示各半導體之形成區域的平 面性重疊狀態的情形。 y於第1圖中,本實施形態中之半導體裝置1(縱型IGBT) f分割成:用以形成屬於焊墊㈣)料部拉出用電極之外 ^電極2A的外部電極形成部3、以及用以形成之電 曰曰體單το的單A形成區域2,N型半導體區域⑻(集極短 ^路區域)僅形成在單元形成區域2,更詳而言之,以俯視觀 之,N型半&體區域i i僅形成在與p型基極區域1⑽ 相重登的位置,以使載子不會由N型半導體區域101(集極 短路區域)急遽排出的方式,在外部電極形成部3不形成集 極短路區域1〇1。 ’、 ^藉此方式存在於外部電極形成部3的載子係如位於 單凡形成區域2的载子所示,不會急遽地由N型半導體區Fig. 1 shows a plan view of the planar structure of the IGBT according to the above-described embodiment. A cross-sectional view of the cross-section of the mBT in the line a_a of the figure (for convenience of illustration, it is described that the cell is formed in the region 2 and is under-reduced (the number of the P-type base regions 104 is reduced)). The structure of each unit of the IGBT is the same as the conventional structure shown in FIG. 5, but the position i (ie, the area) of the semiconductor region (8) (collector short-circuit region) is formed in the semiconductor device, and is implemented in the present embodiment. The state and the conventional examples are not the same. A conventional example is in which a semiconductor short-circuited region is formed on the entire surface of the substrate when the semiconductor is placed. On the other hand, in the present embodiment, the collector short-circuit region is formed only in the cell formation region 2 of the transistor unit for forming the IGBT. That is, in a plan view, the surface in the lower direction of the N-type base region 103 (the other main surface side) is opposed to the N-type buffer layer 1〇2, and the substrate is used in the substrate. The N-type semiconductor region is formed by interposing a P-type semiconductor region 1 〇〇 (collector region) between the 1 >-type semiconductor region 1QQ only in a range of the general-purpose substrate overlapping the region 2; 319357 10 200814313 In the present invention, the plan view is used to view the substrate surface from a direction perpendicular to the plane of the general-purpose substrate, and to display a planar overlapping state of the formation regions of the respective semiconductors. In the first embodiment, the semiconductor device 1 (vertical IGBT) f in the present embodiment is divided into: an external electrode forming portion 3 for forming an electrode 2A other than the electrode for pulling out the material of the pad (4). And a single A formation region 2 for forming the electric body body το, the N-type semiconductor region (8) (collector short circuit region) is formed only in the cell formation region 2, and more specifically, in a plan view, The N-type half & body region ii is formed only at a position opposite to the p-type base region 1 (10) so that the carrier is not suddenly discharged by the N-type semiconductor region 101 (collector short-circuit region), at the external electrode The formation portion 3 does not form the collector short-circuit region 1〇1. ', the carrier existing in the external electrode forming portion 3 by this means, as shown in the carrier of the single-form formation region 2, does not rush to the N-type semiconductor region.

域1〇1(木極短路區域)排出,而朝位於單元形成區域2的N (型半導體區域1G1移動,且依序排出至集極電極ιι〇。 接著於第2圖中,在具有igBT構造之半導體裝置 的木極區域側(圖不之下部方向的側),於外部單元形成區 域2中’交替形成p型半導體區域(集極區域)⑽及n型 半導體區域(集極短路區域)1〇1❿予以配置,於外部電極形 成部3中僅形成有P型半導體區域(集極區域)1〇〇的況用 基板上,形成有由N型基極區域1〇3成為構成之 IGBT。 該1咖係在具有N型半導體區域101及!>型半導體 319357 11 200814313 區域100的上述汎用基板上,與習知例相同地,藉由磊晶 成長法依序形成N型緩衝層102及N型基極區域1〇3。 此外,在N型基極區域103的表面(圖示之上部侧的 面,另一方之主面侧)係藉由P型雜質擴散處理形成有複數 個P型基極區域104,此外,在該P型基極區域1〇4内的 表面,係藉由N型雜質擴散處理而形成有N型射極區域 105。亦即,N型射極區域105係於俯視中,形成在p型基 極區域104所包含的位置,而且深度亦形成為比p型基極 區域104淺,以完全由p型基極區域1〇4所包含的構造而 5,亦即,與除了(上側)表面以外的其他半導體區域相接 的外周面係利用與P型基極區域104相接的構造所形成。 在各P型基極區域104間之N型基極區域1〇3的表面 係形成有閘極絕緣膜1 〇 6。 在上述閘極絕緣膜106上係以導電體形成有閘極電極 107 ’該閘極電極1 〇7係由絕緣膜1 所覆蓋。 在P型基極區域104及N型射極區域1〇5的表面係與 射極電極1〇9電性連接而構成,換言之,p型基極區域ι〇4 及N型射極區域1〇5係透過射極電極1〇9而電性連接。 此外,在汎用基板中之P型半導體區域100與N型半 導體區域101的下面(圖示之下部側的面,另一方主面側) 係形成有集極電極110。藉此方式,使p型半導體區域100 及N型半導體區域101各個分別具有作為集極區域、集極 短路區域的功能。 。 般基板表面之方向的表 於俯視中,亦即當由垂直於一 319357 12 200814313 =上錢看N型基極區域!Q3時,p型基極區域1〇4係如 第1圖所示,以帶狀(條紋狀)延伸形成。 接著,於與P型基極區域1〇4之上述延伸方向呈正交 =方向(第1圖# A_A線)中,當觀看半導體裝置i之剖面 才如第2圖所不,在半導體裝置i的中央側,彼此間離 配置複數個P型基極區域104。在該彼此間離配置之" 基極區域1G4的内部分別形成有N型射極區域ι〇5。The field 1〇1 (the wood pole short-circuited region) is discharged, and moves toward the N (the semiconductor region 1G1 located in the cell formation region 2, and sequentially discharges to the collector electrode ιι. Next, in Fig. 2, the igBT structure is present. On the side of the wood pole region of the semiconductor device (the side in the lower direction of the drawing), the p-type semiconductor region (collector region) (10) and the n-type semiconductor region (collector short-circuit region) are alternately formed in the external cell formation region 2 In the case where only the P-type semiconductor region (collector region) is formed in the external electrode forming portion 3, an IGBT having an N-type base region 1〇3 is formed. 1 is applied to the above-mentioned general-purpose substrate having the N-type semiconductor region 101 and the ?> semiconductor 319357 11 200814313 region 100, and the N-type buffer layers 102 and N are sequentially formed by the epitaxial growth method as in the conventional example. In the surface of the N-type base region 103 (the surface on the upper side and the other main surface side), a plurality of P-type groups are formed by P-type impurity diffusion treatment. Polar region 104, in addition, in the P-type base region The surface in 1〇4 is formed by N-type impurity diffusion treatment to form an N-type emitter region 105. That is, the N-type emitter region 105 is formed in the plan view and is formed in the p-type base region 104. Position, and depth is also formed shallower than the p-type base region 104, completely in the configuration included by the p-type base region 1〇4, that is, connected to other semiconductor regions other than the (upper) surface The outer peripheral surface is formed by a structure in contact with the P-type base region 104. A gate insulating film 1 〇6 is formed on the surface of the N-type base region 1〇3 between the respective P-type base regions 104. A gate electrode 107' is formed on the gate insulating film 106 by a conductor. The gate electrode 1 〇7 is covered by the insulating film 1. In the P-type base region 104 and the N-type emitter region 1〇5 The surface is electrically connected to the emitter electrode 1〇9, in other words, the p-type base region ι4 and the N-type emitter region 1〇5 are electrically connected through the emitter electrode 1〇9. The P-type semiconductor region 100 in the general-purpose substrate and the lower surface of the N-type semiconductor region 101 (the lower side surface of the illustration, the other main On the surface side, the collector electrode 110 is formed. In this manner, each of the p-type semiconductor region 100 and the N-type semiconductor region 101 has a function as a collector region and a collector short-circuit region. In the plan view, that is, when the N-type base region!Q3 is viewed perpendicular to a 319357 12 200814313 = the money, the p-type base region 1〇4 is as shown in Fig. 1 in a strip shape (striped shape). Then, in the direction orthogonal to the extending direction of the P-type base region 1〇4 (the first FIG. #A_A line), when the cross section of the semiconductor device i is viewed as shown in FIG. 2, On the center side of the semiconductor device i, a plurality of P-type base regions 104 are disposed apart from each other. An N-type emitter region ι 5 is formed inside each of the base regions 1G4 disposed apart from each other.

亦即,於俯視中,在長條形狀(帶狀)的p型基極區域 内幵/成有相似形狀之長條形狀的N型射極區域⑻。 尘射極區域105係沿著p型基極區域1〇4的外周 緣’而朝向長條方向以帶狀延伸。 心上述P型基極區域104的帶狀區域係隔介閘極絕緣膜 106而與閘極電極1G7相對向,且具有作為周知之通道形 ί區域的功能。亦即,藉由對閘極雜H)7施加⑴的電 s’而在”閘極电極j 〇7相對向之p型基極區域1 的表 :形成通道而呈導通狀態,且使N型基極區域1〇5及_ 二二區域1〇3成為導通狀態。因此’於俯視中,相對於閘 2極:〇7iN型射極區域1〇5、p型基極區域⑽及以 土極區4 1G3的排列順序,使各個表面隔介閘極 1〇6而相對向形成。 眠 报J此’藉由該以帶狀延伸的1個P型基極區域104、 ΜίΓ P型基極區域1〇4内部的N型射極區域105、以 目對應形成的閘極電極1〇7,形成IGBT的單一元 件區域(單元區域)。 J平凡 319357 13 200814313 如上所述’於苐1圖中,在丰導 -^ ^ ^ ^ „ 在牛置1的中央側係 叹有.相互間離配置?型基極區域1〇4的區域,亦即 有複數個單元區域的單4成區域2。 另一方面,在半導體裝置1的外周側係設有未形成有 早凡區域的外部電極形成部3。該未形成有單元區域的外 部電極形成部3係以環狀或包圍的形狀包圍形成有IGBT 之單元的單元形成區域2。That is, in a plan view, a long-shaped N-type emitter region (8) having a similar shape is formed in a strip-shaped base region of a strip shape (band shape). The dust emitter region 105 extends in a strip shape toward the strip direction along the outer peripheral edge ' of the p-type base region 1〇4. The strip-shaped region of the P-type base region 104 is opposed to the gate electrode 1G7 by the gate insulating film 106, and has a function as a well-known channel region. That is, by applying the electric s' of (1) to the gate impurity H)7, the surface of the p-type base region 1 opposite to the gate electrode j 〇7 is formed to be in a conducting state, and N is made The type base region 1〇5 and the _2nd region 1〇3 are in an on state. Therefore, in the plan view, the gate 2: 〇7iN type emitter region 1〇5, p-type base region (10) and soil The order of the polar regions 4 1G3 is such that the respective surfaces are formed opposite to each other by the gates 1 〇 6 . The P-type base region 104 and the Γ Γ P-type base are extended by the band. The N-type emitter region 105 inside the region 1〇4 and the gate electrode 1〇7 formed in the corresponding direction form a single element region (cell region) of the IGBT. J P. 319357 13 200814313 As described above, in the diagram of '苐1 In the Feng guide -^ ^ ^ ^ „ in the central side of the cattle set 1 sigh. The region of the type base region 1〇4, that is, the single quadruple region 2 having a plurality of unit regions. On the other hand, an external electrode forming portion 3 in which an early region is not formed is provided on the outer peripheral side of the semiconductor device 1. The external electrode forming portion 3 in which the unit region is not formed surrounds the unit forming region 2 in which the unit of the IGBT is formed in a ring shape or a surrounding shape.

^在此,在未形成有單元區域的上述外部電極形成部3 係配置有周知之連接電極(接合焊塾)或閘極匯流排線等外 部電極2A。 於本實施形態中,為了設置用以形成接合焊墊的外部 電極形成部3,單元形成區域2形成為局部性凹向内側的 ^狀,結果,如第1圖所示,中央侧之單元區域(P型基極 區域104)的延伸長度係比其他單元區域的延伸長度短。 ^如上所述,於本實施形態之IGBT中,形成有將集極 私極110及N型緩衝層i 02電性連接的N型半導體區域 1〇1(集極短路區域)。 然而’該所形成的區域與習知的IGBT不同,集極短 路區域ιοί係僅配置在形成有IGBT之單元的單元形成區 域2 ’在未形成有單元區域的外部電極形成部3並未配置 N型半導體區域1〇1(集極短路區域)。 此外’如第1圖所示,N型半導體區域1〇1係於俯視 中’形成為相互間離的擴散層,與N型基極區域1〇4相重 田 ® ’而且在外周包含在N型基極區域104的位置,排列於 14 319357 200814313 N型基極區域1()4的長條方向而設置複數個。 措由如上所述的構成,如第3圖⑷之半導體裝置!之 也力逆向偏£的狀您之後,載子(電子)由集極短路區域⑻ 附近’亦即單兀形成區域2中之N型緩衝層⑽及N型美 極層H)3移動至N料導體區域1〇1(集極短路區域),= 由集極電極110作為電流而流通。 然而,在未形成有N型半導體區域1〇1(集極短路區域) 之外部,極形成部3中的N型緩衝層1()2及N型基極層 斤田年貝的载子係忮慢移動,且經由N型半導體區域 1〇1(集極短路區域)而作為電流流通至集極電極11〇而排Here, the external electrode 2A such as a known connection electrode (joint bonding pad) or a gate bus bar is disposed in the external electrode forming portion 3 in which the cell region is not formed. In the present embodiment, in order to provide the external electrode forming portion 3 for forming the bonding pad, the unit forming region 2 is formed in a partially concave inner shape, and as a result, as shown in Fig. 1, the central side unit region The extension length of the (P-type base region 104) is shorter than the extension length of the other unit regions. As described above, in the IGBT of the present embodiment, the N-type semiconductor region 1〇1 (collector short-circuit region) electrically connecting the collector private electrode 110 and the N-type buffer layer i 02 is formed. However, the region formed by this is different from the conventional IGBT, and the collector short-circuit region ιοί is disposed only in the cell formation region 2 ′ where the IGBT is formed. The external electrode formation portion 3 in which the cell region is not formed is not disposed. Type semiconductor region 1〇1 (collector short-circuit region). Further, as shown in Fig. 1, the N-type semiconductor region 1〇1 is formed as a diffusion layer which is formed to be separated from each other in plan view, and is N-type base region 1〇4 phased in the field 'and is included in the outer periphery in the N-type The position of the base region 104 is arranged in a plurality of directions in the strip direction of the N-type base region 1 () 4 of 14 319 357 200814313. The configuration is as described above, such as the semiconductor device of Fig. 3 (4)! After that, the carrier (electron) is moved from the vicinity of the collector short-circuit region (8), that is, the N-type buffer layer (10) and the N-type US layer H in the single-turn formation region 2 to N. The material conductor region 1〇1 (collector short-circuit region) = is distributed by the collector electrode 110 as a current. However, in the case where the N-type semiconductor region 1〇1 (collector short-circuit region) is not formed, the N-type buffer layer 1 () 2 and the N-type base layer in the pole forming portion 3 are carrier systems of the N-type base layer Slowly moving, and flowing through the N-type semiconductor region 1〇1 (collector short-circuit region) as current flows to the collector electrode 11〇

此如第3圖(b)所示,與亦形成在外部電極形成部 ^之N型半導體區域1G1(集極短路區域),亦即在況用基板 小面:成有N型半導體區域101之習知例相比較,關於微 ^電机I流動的時間,期間td比期間ts長(圖中td,),且 td/ts的比例變大,藉此可實現軟修復特性。 ^ P於第3圖(b)中,實線表示本實施形態中之電流 ^的机動狀態,錢表示習知例中之電流工的流動狀態。由 ::圖(b)可知’與習知例相比較,接合面二極體處於短路 期間ts係、較沒有變化,但可使由逆向電麈成為最大 =日守間點起具有接合面二極體之逆阻止功能的期間td, 中的朗td|,形成⑽/阶⑼/⑻的關係, /、白"例相比較,可改善接合面二極體的軟修復特性。 319357 15 200814313 的丨^丁外。’以其他實施形態而言,可對應第4圖所示構造 ‘能之夺以半導體’:置1之平面構造而言,亦與-實施形 :弟圖相同,本實施形態中之半導體裝置1(縱型IGBT) 係分割成:用以形成屬於焊墊等外部拉出用電極之外部電 的外部電極形成部3、以及用以形成之電晶體 f元的單元形成區域2, N型半導體區域⑻(集極短= ί 域)僅形成在單元形成區域2,更詳而言之,以俯視觀之, 將N型半導體區域101(集極短路區域)僅形成在與P型基 極區域104A相重豐的位置,而未形成在外部電極形成部 3 〇 ( 接著’於第4圖中,在半導體袭置^構造的集極區 域側⑽示之下部方向的側),與上述之一實施形態相同 地’於早凡形成區域2中,交替配置p型半導體區域(集極 區或)100及N型半導體區域(集極短路區域),在於外 部電極形成部3中僅於配置有p型半導體區域1〇〇之所謂 沉用基板上形成有IGBT。 ”該IGBT係與—實施形態相同,在上述況用基板上, ”白知例相同地’藉由蠢晶成長法依序形成N ^緩衝層 1〇2以及N型基極區域1〇3。 此外,在N型基極區域103的表面(第4圖之上部侧 ^面)係以長條狀形成溝200,與該溝細的側壁相鄰接, 藉由p㈣質擴散處理形成複數個p型基極區域i〇4a, 此外藉型雜質擴散處理在該P型基極區域104A内 319357 16 200814313 的表面形成有N型射極區域i〇5A。 在此’ N型射極區域1 〇5a亦與溝2〇〇的侧壁相鄰接 而形成。亦即,N型射極區域105A係於俯視中,形成在p 型基極區域104A所包含的位置,而且深度亦形成為比p 型基極區域104A淺,作為完全由P型基極區域1〇4A所包 含的構造而形成。 此外,形成在各P型基極區域i 〇4A間的溝2〇〇係將 閘極電極、P型基極區域1〇4入及N型射極區域i〇5a之間 電性絕緣,因此在内面形成有閘極絕緣膜1G6A。 在上述閘極絕緣膜106A内面係形成有閘極電極 107A,、該閘極電極1〇7八係由未圖示之絕緣膜所覆蓋。亦 即’在溝200内係在該溝2〇〇的内面隔介閘極絕緣膜1⑽a 而形成有閘極電極1 〇7A。 p型基極區域H)4A&N型射極區域1Q5A_過射極 電極109A而電性連接,亦即,在p型基極區域i〇4a及n 型射極區域1G5A的表面係形成有射極電極1Q9a,而將p 型基極區域i〇4a&n型射極區域1G5Af性連接。 此外’於況用基板中之p型半導體區域⑽及㈣ 導體區域1〇1的下面(圖示之下部側的面)係形成有集極電 f 110。糟此使P型半導體區域⑽及心半導體區域⑻ 各個分別具有作為集極區域、集極短路區域的功能。 /型基極區域1G4A係與上述之—實施形態相同,由平 ’亦即虽由N型基極區域103的上面側觀看時,如 弟圖所不’係以帶狀延伸而(以條紋狀)形成複數個。 319357 17 200814313 仅著,於與p型基極區域i 〇4A之上述延伸方向呈正 交的方向(第1圖的A-A線)中,當觀看半導體裝置1之剖 面守如圖所示,在半導體裝置1的中央側,彼此間離配 置複數個P型基極區域104A。在該彼此分離配置之p型 基極區域104A的内部分別成有N型射極區域i〇5a。此 外,在單元形成區域之溝200之間係以帶狀形成有p型基 極區域104A,於該p型基極區域1〇4内表面中與n型射 極區域105A相對向而形成。 N型射極區域105A係沿著p型基極區域i〇4a的外周 緣’而朝向長條方向以帶狀延伸。 冬上述p型基極區域ι〇4Α的帶狀區域係透過閘極絕緣 膜106A而與閘極電極1〇7A的側壁相對向,且具有作為周 知之通道形成區域的功能。亦即,藉由對閘極電極 施加(+)的電壓,而在與閘極電極1〇7入相對向之p型基極 區域104A的侧面,亦即與溝2〇〇之側壁相接的區域形成 通道而呈導通狀態,且使N型射極區域1〇5人及n型基極 區域103成為電性導通狀態。 、口此如第4圖之線視剖視圖所示,藉由N型射極區 域1〇5Α、Ρ型基極區域1〇4A&N型基極區域1〇3的排列 順序,使各個的侧面透過閘極絕緣膜1〇6A而與閘極電極 107A的側面相對向而形成。亦即,以n型射極區域1〇5八、 P型基極區域104A及N型基極區域1〇3的順序形成階層 構造。 藉由該以帶狀延伸的1個p型基極區域104A、形成在 319357 18 200814313 该P型基極區域104A内部的N型射極區域1〇5A、以及與 其相對應形成的閘極電極1〇7A,形成在溝2〇〇的側壁形成 通道之IGBT的單一元件區域(單元區域)。 如上所述,於第!圖中,在半導體裝置1的中央側, 係設有彼此間離配置P型基極區域1〇4A的區域,亦即配 置有複數個單it區域的單元形成區域2。關於其他動作因As shown in FIG. 3(b), the N-type semiconductor region 1G1 (collector short-circuit region) also formed in the external electrode forming portion, that is, the surface of the substrate for the case: the N-type semiconductor region 101 is formed. In comparison with the conventional example, the period td is longer than the period ts (td in the figure), and the ratio of td/ts becomes large, whereby the soft repair characteristic can be realized. ^ P In Fig. 3(b), the solid line indicates the maneuver state of the current ^ in the present embodiment, and the money indicates the flow state of the current worker in the conventional example. It can be seen from: (b) that compared with the conventional example, the junction surface diode is in the short-circuit period ts system, and there is no change, but it can be made from the reverse power to the maximum = day-to-day point with the joint surface In the period td of the reverse body blocking function, the relationship between (10)/order (9)/(8) is formed, and the soft repair characteristics of the joint surface diode can be improved. 319357 15 200814313 丨^丁外. In other embodiments, the semiconductor device 1 of the present embodiment can be used in the same manner as the embodiment of the first embodiment. (Vertical IGBT) is divided into: an external electrode forming portion 3 for forming external electric power belonging to an external drawing electrode such as a pad, and a cell forming region 2 for forming a transistor f element, an N-type semiconductor region (8) (collective short = ί domain) is formed only in the cell formation region 2, and more specifically, in a plan view, the N-type semiconductor region 101 (collector short-circuit region) is formed only in the P-type base region 104A The position of the phase is not formed in the external electrode forming portion 3 〇 (following in the fourth figure, on the side of the collector region side of the semiconductor layer structure (10) showing the lower direction), and one of the above is implemented In the same manner, in the early formation region 2, the p-type semiconductor region (collector region) 100 and the N-type semiconductor region (collector short-circuit region) are alternately arranged, and only the p-type is disposed in the external electrode forming portion 3. On the so-called sink substrate of the semiconductor region To have IGBT. The IGBT system is formed in the same manner as in the embodiment, and the N ^ buffer layer 1 〇 2 and the N-type base region 1 〇 3 are sequentially formed by the stray crystal growth method on the above-mentioned condition substrate. Further, on the surface of the N-type base region 103 (the upper side surface of Fig. 4), the groove 200 is formed in a strip shape, adjacent to the thin side wall of the groove, and a plurality of p are formed by p (tetra) diffusion treatment. The base region i 〇 4a is further formed with an N-type emitter region i 〇 5A on the surface of the 319357 16 200814313 in the P-type base region 104A. Here, the 'N-type emitter region 1' 5a is also formed adjacent to the sidewall of the trench 2''. That is, the N-type emitter region 105A is formed in a plan view, is formed at a position included in the p-type base region 104A, and is formed to be shallower than the p-type base region 104A as a completely P-type base region 1 The structure included in 〇4A is formed. Further, the trench 2 formed between the respective P-type base regions i 〇 4A electrically insulates the gate electrode, the P-type base region 1〇4, and the N-type emitter region i〇5a. A gate insulating film 1G6A is formed on the inner surface. A gate electrode 107A is formed on the surface of the gate insulating film 106A, and the gate electrode 1 is covered with an insulating film (not shown). That is, the gate electrode 1 〇 7A is formed by interposing the gate insulating film 1 (10) a on the inner surface of the trench 2 in the trench 200. The p-type base region H) 4A & N-type emitter region 1Q5A_ the emitter electrode 109A is electrically connected, that is, the surface of the p-type base region i〇4a and the n-type emitter region 1G5A is formed. The emitter electrode 1Q9a is connected to the p-type base region i〇4a & n-type emitter region 1G5Af. Further, the collector electric power f 110 is formed on the lower surface (the surface on the lower side in the drawing) of the p-type semiconductor region (10) and the (four) conductor region 1〇1 in the case substrate. The P-type semiconductor region (10) and the core semiconductor region (8) each have a function as a collector region and a collector short-circuit region. The /type base region 1G4A is the same as the above-described embodiment, and when viewed from the upper side of the N-type base region 103, it is stretched in a strip shape (in a stripe shape) ) form a plurality of. 319357 17 200814313 In the direction orthogonal to the above-described extending direction of the p-type base region i 〇 4A (the AA line in FIG. 1), when the semiconductor device 1 is viewed as shown in the figure, in the semiconductor On the center side of the device 1, a plurality of P-type base regions 104A are disposed apart from each other. An N-type emitter region i〇5a is formed inside each of the p-type base regions 104A which are disposed apart from each other. Further, a p-type base region 104A is formed in a strip shape between the trenches 200 in the cell formation region, and is formed to face the n-type emitter region 105A on the inner surface of the p-type base region 1A4. The N-type emitter region 105A extends in a strip shape along the outer peripheral edge ' of the p-type base region i〇4a toward the strip direction. In the winter, the strip region of the p-type base region ι〇4Α is opposed to the sidewall of the gate electrode 1A7A through the gate insulating film 106A, and has a function as a well-known channel formation region. That is, by applying a (+) voltage to the gate electrode, it is in contact with the side surface of the p-type base region 104A opposite to the gate electrode 1〇7, that is, the side wall of the trench 2〇〇. The region forms a channel and is in an on state, and the N-type emitter region 1〇5 person and the n-type base region 103 are electrically connected. The mouth is as shown in the cross-sectional view of Fig. 4, and the sides are arranged by the arrangement order of the N-type emitter region 1〇5Α, the Ρ-type base region 1〇4A&N-type base region 1〇3. The gate insulating film 1A6A is formed to face the side surface of the gate electrode 107A. That is, the hierarchical structure is formed in the order of the n-type emitter region 1〇5, the P-type base region 104A, and the N-type base region 1〇3. The gate electrode 1 is formed by a p-type base region 104A extending in a strip shape, an N-type emitter region 1〇5A formed inside the P-type base region 104A at 319357 18 200814313, and a gate electrode 1 formed corresponding thereto 〇7A, a single element region (cell region) of the IGBT forming a channel on the sidewall of the trench 2〇〇. As mentioned above, in the first! In the figure, on the center side of the semiconductor device 1, a region in which the P-type base regions 1A and 4A are disposed apart from each other, that is, a cell formation region 2 in which a plurality of single-it regions are disposed is disposed. About other actions

與-實施形態相同,故省略說明。與一實施形態相同,N 型半導體區域101係僅形成在以俯視觀之與單元形成區域 2相重疊的部分。 、 此外 Λ細形態及其他實施形態均可將IGBT變形 為以下所示之構造而形成。 (1)可作成在未形成Ν型緩衝層1〇2,而形成有ρ型半導體 區域100及Ν型半導體區域1〇1的〉凡用基板上,直接 形成Ν型基極層1 〇3的構造。 ⑺Ν型半導體區域1G1(集極短㈣域)雖設在ρ型基極區 域1〇4(或104A)的下部,但亦可於俯視中形成在長條上 之P型基極區域104之間(當然形成在單元形成區域的 内部)。 ()雖將P型基極區域1G4(或論)形成為長條形狀的條紋 狀,但亦可形成為長條形狀之ρ型基極區域呈正交的 格子狀或者分割成預定寬度之區域的島狀⑽响。 【圖式簡單說明】 第1圖係顯示本發明—實施形態之半導體裝置^ 現中之平面構造的俯視圖 319357 19 200814313 A A中之半導體裝置1的線視剖 第2圖係第1圖之線 視圖。 第3圖(a)及⑻係用以說明本實施形態中載子(電子)由 N型緩衝層1 〇2及N型基極 的概念圖。 層1G3㈣至集極短路區域⑻ 之線 第4圖係本發明其他實施形態之半導體裝置 Α·Α、第1圖)中之半導體裝置1的線視剖視圖: =5圖係顯示IGBT之電晶體構造之剖視圖。 >第6圖係顯示咖了之等效電路之概念圖。 第7圖⑷及⑻係用以說明於施加順向電屢時及施加 =電壓時載子由集極短路區域1〇1排出之排出動作的概 怎圖。 【主要元件符號說明】 2A 100 101 102 104、 106、 108 110 半導體裝置 外部電極 P型半導體區域(集極區域) N型半導體區域(集極短路區域) 單元形成區域 外部電極形成部 N型緩衝層 104A P型基極層 106A 閘極絕緣膜 絕緣膜 集極電極 103 N型基極層 105、105A N型射極區域 107、107A閘極電極 109、109A射極電極 200 溝 319357 20The description is the same as that of the embodiment, and thus the description thereof is omitted. As in the first embodiment, the N-type semiconductor region 101 is formed only in a portion overlapping the cell formation region 2 in plan view. Further, the IGBT and the other embodiments can be formed by deforming the IGBT into the structure shown below. (1) It is possible to form the Ν-type base layer 1 〇 3 directly on the substrate on which the p-type semiconductor region 100 and the Ν-type semiconductor region 1 〇 1 are formed without forming the 缓冲-type buffer layer 1 〇 2 structure. (7) The Ν-type semiconductor region 1G1 (collector short (four) domain) is provided in the lower portion of the p-type base region 1〇4 (or 104A), but may be formed between the P-type base regions 104 on the strip in plan view. (Of course formed inside the cell formation region). () Although the P-type base region 1G4 (or the theory) is formed into a stripe shape of a long shape, the p-type base region of the elongated shape may be formed in an orthogonal lattice shape or divided into regions of a predetermined width. The island shape (10) rings. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a plan view showing a planar structure of a semiconductor device according to an embodiment of the present invention. 319357 19 200814313 A line cross-sectional view of a semiconductor device 1 in AA is a line view of FIG. . Fig. 3 (a) and (8) are diagrams for explaining the concept of the carrier (electron) in the present embodiment from the N-type buffer layer 1 〇 2 and the N-type base. Line 1G3 (4) to the collector short-circuit region (8). FIG. 4 is a cross-sectional view of the semiconductor device 1 in the semiconductor device according to another embodiment of the present invention, and FIG. 1 is a cross-sectional view showing the transistor structure of the IGBT. Cutaway view. > Figure 6 is a conceptual diagram showing the equivalent circuit of the coffee. Fig. 7 (4) and (8) are diagrams for explaining the discharge operation of the carrier discharged from the collector short-circuit region 1〇1 when the forward electric power is applied and the voltage is applied. [Description of main component symbols] 2A 100 101 102 104, 106, 108 110 Semiconductor device external electrode P-type semiconductor region (collector region) N-type semiconductor region (collector short-circuit region) Cell formation region External electrode formation portion N-type buffer layer 104A P-type base layer 106A gate insulating film insulating film collector electrode 103 N-type base layer 105, 105A N-type emitter region 107, 107A gate electrode 109, 109A emitter electrode 200 groove 319357 20

Claims (1)

200814313 十、申請專利範圍: 1. 一種半導體裝置,係具有絕緣閘極型雙極電晶體構造之 半導體裝置,其特徵為具有: 第1導電型之第1基極區域; 第2導電型之第2基極區域,設置在該第丨基極區 域之一方之主面侧; 第1導電型之射極區域,形成在前述第2基極區域 内; / 第2導電型之集極區域,配置在前述第丨基極區域 之另一方之主面側;以及 第1導電型之集極短路區域,在前述第〗基極區域 之另一方主面側,以分割前述集極區域的方式,插介於 集極區域間而形成, 、 Μ而且在前述第i基極區域之—方之主面側的外周部 °又=未=成有前述帛2基極區域的外部電極形成部,並 ^述,2基極區域形成在該外部電極形成部之内侧的 電^體單元形成區域,將前述集極短路區域僅形成在前 述單元形成區域内。 2·如申請專利範圍第1 短路區域係僅形成在 重疊的位置。 項之半導體裝置,其中,前述集極 以俯視觀之與前述第2基極區域相 3·如申請專利範圍第1 在成述第1基極區域 ^域間没有間極電極 項或第2項之半導體裝置,其中, 之一方之主面側上部,在前述射極 319357 21 200814313 ’前述閘極 4.如申請專利範圍第3項之半導體裝置,其中 電極係設在形成在前述射極區域間的溝内。 22 319357200814313 X. Patent application scope: 1. A semiconductor device comprising a semiconductor device having an insulated gate bipolar transistor structure, characterized by having: a first base region of a first conductivity type; and a second conductivity type 2 base region is provided on one of the main surface sides of the second base region; the first conductivity type emitter region is formed in the second base region; / the second conductivity type collector region is disposed On the other main surface side of the second base region; and the collector short-circuit region of the first conductivity type, the other main surface side of the first base region is inserted so as to divide the collector region Formed between the collector regions, and the outer peripheral portion of the main surface side of the ith base region is further = the outer electrode forming portion of the 帛2 base region is not formed, and The 2 base region is formed in the electrode unit forming region inside the external electrode forming portion, and the collector short-circuit region is formed only in the cell forming region. 2. If the patent application area 1st short-circuit area is formed only in the overlapping position. The semiconductor device of the present invention, wherein the collector is in a plan view and the second base region. 3. As claimed in the patent application, there is no interpole electrode term or second term between the first base region and the first base region. The semiconductor device of the semiconductor device of the present invention, wherein the electrode is disposed between the emitter regions of the semiconductor device of claim 3, wherein the electrode is provided in the emitter region. Inside the ditch. 22 319357
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