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    • 3. 发明授权
    • Insulated gate semiconductor device
    • 绝缘栅半导体器件
    • US06342709B1
    • 2002-01-29
    • US09117997
    • 1998-08-11
    • Yoshitaka SugawaraKatsunori Asano
    • Yoshitaka SugawaraKatsunori Asano
    • H01L3300
    • H01L29/7811H01L29/0619H01L29/1095H01L29/1608H01L29/42368H01L29/7397H01L29/7809H01L29/7813
    • In a semiconductor device having a trench type insulated gate structure, in the case where a drift layer 2 of an n− conduction type has a high carrier density, when a high voltage is applied between a drain and a source in such a manner that a channel is not formed, the electric field strength of an insulator layer 9 below the trench type insulated gate is increased, thus causing breakdown. The withstand voltage of the semiconductor device is limited by the breakdown of the insulator layer 9, and it is difficult to realize high withstand voltage. In the characteristic of the present invention, a field relaxation semiconductor region 1 of a conduction type opposite to the conduction type of the drift layer 2 is formed within the drift layer 2 below the insulator layer 9 in the trench of the trench type insulated gate semiconductor device. Also, the thickness of a bottom portion of the insulator layer 9 provided in the trench of the trench type insulated gate semiconductor device is made significantly greater than the thickness of a lateral portion thereof.
    • 在具有沟槽型绝缘栅极结构的半导体器件中,在n型导电型漂移层2具有高载流子密度的情况下,当在漏极和源极之间施加高电压时, 通道不形成,沟槽型绝缘栅下方的绝缘体层9的电场强度增加,从而导致击穿。 半导体器件的耐电压受绝缘体层9击穿的限制,难以实现高耐压。在本发明的特征中,与导通相反的导电类型的场弛豫半导体区域1 在沟槽型绝缘栅半导体器件的沟槽中的绝缘体层9下方的漂移层2内形成漂移层2的类型。 此外,设置在沟槽型绝缘栅极半导体器件的沟槽中的绝缘体层9的底部的厚度显着大于其侧面部分的厚度。
    • 7. 发明申请
    • Voltage-controlled semiconductor device
    • 压控半导体器件
    • US20070200150A1
    • 2007-08-30
    • US10593878
    • 2005-03-17
    • Katsunori Asano
    • Katsunori Asano
    • H01L29/80
    • H01L29/1095H01L29/0623H01L29/7391H01L29/7395
    • SiC-IGBTs, which have an inversion-type channel with high channel resistance and have high on-voltage due to an influence from the surface state of the interface between a gate insulating film and a base layer, are required to decrease the on-voltage. An embedded collector region is partially formed in a base layer which is formed on an emitter layer of a SiC semiconductor. A channel layer is formed on the base layer and the embedded collector region to constitute an accumulation-type channel. Consequently, at on time, holes are accumulated in the upper layer portion of the channel layer so that a low-resistant channel is formed. Current by the holes flows to the emitter layer through a channel from the collector region and becomes a base current for an npn transistor composed of the embedded collector region, the base region and the emitter region.
    • 需要具有高通道电阻的反型通道和由于栅极绝缘膜和基极层之间的界面的表面状态的影响而具有高导通电压的SiC-IGBT,以降低导通电压 。 嵌入式集电极区域部分地形成在形成在SiC半导体的发射极层上的基极层中。 沟道层形成在基极层和嵌入的集电极区域上,构成积聚型沟道。 因此,在时间上,在沟道层的上层部分积聚有孔,从而形成低阻抗沟道。 这些空穴的电流通过来自集电极区域的沟道流到发射极层,成为由嵌入集电极区域,基极区域和发射极区域构成的npn晶体管的基极电流。
    • 8. 发明申请
    • Gate turn-off thyristor
    • 门极关断晶闸管
    • US20070120145A1
    • 2007-05-31
    • US10552268
    • 2004-04-07
    • Katsunori AsanoYoshitaka Sugawara
    • Katsunori AsanoYoshitaka Sugawara
    • H01L31/111
    • H01L29/1016H01L29/0615H01L29/0834H01L29/744
    • A mesa-type wide-gap semiconductor gate turn-off thyristor has a low gate withstand voltage and a large leakage current. Since the ionization rate of P-type impurities greatly increases at high temperatures when compared with that at room temperature, the hole implantation amount increases and the minority carrier lifetime becomes longer. Consequently, the maximum controllable current is significantly lowered when compared with that at room temperature. To solve these problems, a p-type base layer is formed on an n-type SiC cathode emitter layer which has a cathode electrode on one surface, and a thin n-type base layer is formed on the p-type base layer. A mesa-shaped p-type anode emitter layer is formed in the central region of the n-type base layer. An n-type gate contact region is formed sufficiently apart from the junction between the p-type anode emitter layer and the n-type base layer, and an n-type low-resistance gate region is so formed in the n-type base layer that it surrounds the anode emitter layer.
    • 台式宽间隙半导体栅极截止晶闸管具有低栅极耐受电压和较大的漏电流。 由于与高温下相比,P型杂质的电离率大大增加,所以空穴注入量增加,少数载流子寿命变长。 因此,与室温相比,最大可控电流显着降低。 为了解决这些问题,在单面表面具有阴极的n型SiC阴极发射极层上形成p型基极层,在p型基极层上形成薄的n型基极层。 在n型基极层的中心区域形成台状p型阳极发射极层。 与p型阳极发射极层和n型基极层之间的接合部充分地形成n型栅极接触区域,在n型基极层上形成n型低电阻栅极区域 它围绕阳极发射极层。