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    • 1. 发明授权
    • Method of manufacturing a transistor
    • 制造晶体管的方法
    • US06706615B2
    • 2004-03-16
    • US10401672
    • 2003-03-31
    • Mizue KitadaToshiyuki TakemoriShinji Kunori
    • Mizue KitadaToshiyuki TakemoriShinji Kunori
    • H01L2176
    • H01L29/7813H01L29/04H01L29/0634H01L29/0696H01L29/402H01L29/407H01L29/66348H01L29/7397
    • A technique for reducing an on-resistance of a transistor is provided. A power MOSFET of the present invention has a semiconductor material which is disposed under a polysilicon gate and composed of polysilicon into which impurities are doped at low concentration. Therefore, a depletion layer is expanded to the inside of the semiconductor material under the polysilicon gate. Since the electric field strengths are uniform from the surface of a drain layer to a depth of the bottom surface of the semiconductor material and a high electric field is not generated at one site, the avalanche breakdown voltage of the transistor is increased. Therefore, the concentration of impurities in drain layer can be made higher than that in a conventional transistor and thereby the on-resistance of the transistor 1 can be reduced.
    • 提供了降低晶体管的导通电阻的技术。 本发明的功率MOSFET具有半导体材料,该半导体材料设置在多晶硅栅极下方,并以低浓度杂质杂质的多晶硅构成。 因此,耗尽层在多晶硅栅极下扩展到半导体材料的内部。 由于电场强度从漏极层的表面到半导体材料的底面的深度均匀,并且在一个部位不产生高电场,所以晶体管的雪崩击穿电压增加。 因此,可以使漏层中的杂质浓度高于常规晶体管中的杂质浓度,从而可以降低晶体管1的导通电阻。
    • 8. 发明授权
    • Transistor and method of manufacturing the same
    • 晶体管及其制造方法
    • US06573559B2
    • 2003-06-03
    • US09793964
    • 2001-02-28
    • Mizue KitadaToshiyuki TakemoriShinji Kunori
    • Mizue KitadaToshiyuki TakemoriShinji Kunori
    • H01L2976
    • H01L29/7813H01L29/04H01L29/0634H01L29/0696H01L29/402H01L29/407H01L29/66348H01L29/7397
    • A technique for reducing an on-resistance of a transistor is provided. A power MOSFET of the present invention has a semiconductor material which is disposed under a polysilicon gate and composed of polysilicon into which impurities are doped at low concentration. Therefore, a depletion layer is expanded to the inside of the semiconductor material under the polysilicon gate. Since the electric field strengths are uniform from the surface of a drain layer to a depth of the bottom surface of the semiconductor material and a high electric field is not generated at one site, the avalanche breakdown voltage of the transistor is increased. Therefore, the concentration of impurities in drain layer can be made higher than that in a conventional transistor and thereby the on-resistance of the transistor 1 can be reduced.
    • 提供了降低晶体管的导通电阻的技术。 本发明的功率MOSFET具有半导体材料,该半导体材料设置在多晶硅栅极下方,并以低浓度杂质杂质的多晶硅构成。 因此,耗尽层在多晶硅栅极下扩展到半导体材料的内部。 由于电场强度从漏极层的表面到半导体材料的底面的深度均匀,并且在一个部位不产生高电场,所以晶体管的雪崩击穿电压增加。 因此,可以使漏层中的杂质浓度高于常规晶体管中的杂质浓度,从而可以降低晶体管1的导通电阻。
    • 9. 发明授权
    • Semiconductor device
    • 半导体器件
    • US06404032B1
    • 2002-06-11
    • US09820837
    • 2001-03-30
    • Mizue KitadaShinji Kunori
    • Mizue KitadaShinji Kunori
    • H01L2947
    • H01L29/66143H01L29/0634H01L29/872
    • Trenches are formed in the surface of a second semiconductor layer of a first conductivity type. A semiconductor filled material of a second conductivity type is filled in the trench. A Schottky metal electrode is formed on the surface of the second semiconductor layer and the surface of the semiconductor filled material. A Schottky junction is formed between the Schottky metal electrode and the second semiconductor layer. An ohmic contact is formed between the Schottky metal electrode and the semiconductor filled material. An avalanche breakdown voltage is increased when the impurity concentration of the second semiconductor layer and the semiconductor filled material and the interval between the trenches are set such that both the second semiconductor layer interposed between the semiconductor filled materials and the semiconductor filled material are completely depleted when the Schottky junction is reverse biased.
    • 沟槽形成在第一导电类型的第二半导体层的表面中。 在沟槽中填充第二导电类型的半导体填充材料。 在第二半导体层的表面和半导体填充材料的表面上形成肖特金属电极。 在肖特基金属电极和第二半导体层之间形成肖特基结。 在肖特基金属电极和半导体填充材料之间形成欧姆接触。 当第二半导体层和半导体填充材料的杂质浓度和沟槽之间的间隔被设定为使得介于半导体填充材料和半导体填充材料之间的第二半导体层两者都完全耗尽时,雪崩击穿电压增加, 肖特基结是反向偏置的。