MOS晶(jing)体管种(zhong)(zhong)类 mos管种(zhong)(zhong)类名(ming)称详解!
信(xin)息来源:本站(zhan) 日期(qi):2017-05-31
MOS晶体管种类.
按沟道区中载流子类型分
N沟MOS晶体管:衬底为P型,源漏为重掺杂的N+,沟道中载流子为电子
P沟MOS晶体管:衬底为(wei)N型,源漏为(wei)重掺杂(za)的P+,沟(gou)道中载流子为(wei)空(kong)穴
在(zai)正常青(qing)况下,只需一(yi)种(zhong)类型的(de)载流子(zi)在(zai)工作,因此也(ye)称其为单极晶体管。
按工作方式分增强型晶体管:若在零栅压下不存在漏源导电沟道,为了构成导电沟道,需求施加一定的栅压,也就是说沟道要经过、"增强"才干导通
耗尽型晶体管(guan):器(qi)(qi)件(jian)本身在漏源之间(jian)就存(cun)在导电沟道,即使(shi)在零(ling)栅压下器(qi)(qi),件(jian)也是(shi)导通的e 若(ruo)要(yao)使(shi)器(qi)(qi)件(jian)截(jie)止,就必需施加(jia)栅压使(shi)沟道耗尽型。
假(jia)定(ding)、漏端电(dian)(dian)(dian)压Vds为(wei)(wei)(wei)(wei)正(zheng)(zheng),当栅(zha)上施加一(yi)(yi)个小于(yu)开启电(dian)(dian)(dian)压的正(zheng)(zheng)栅(zha)压时,栅(zha)氧下面(mian)的P型(xing)(xing)表(biao)面(mian)区的空穴被(bei)耗(hao)尽,在(zai)硅(gui)表(biao)面(mian)构(gou)成(cheng)一(yi)(yi)层负电(dian)(dian)(dian)荷,这些电(dian)(dian)(dian)荷被(bei)称为(wei)(wei)(wei)(wei)耗(hao)尽层电(dian)(dian)(dian)荷Qb。这时的漏源(yuan)电(dian)(dian)(dian)流(liu)为(wei)(wei)(wei)(wei)透(tou)露电(dian)(dian)(dian)流(liu)。假(jia)定(ding)Vgs>Vth,在(zai)哩硅(gui)表(biao)面(mian)构(gou)成(cheng)可(ke)移动的负电(dian)(dian)(dian)蒲Qi层,即导电(dian)(dian)(dian)沟道(dao)。由于(yu)表(biao)面(mian)为(wei)(wei)(wei)(wei)N型(xing)(xing)的导电(dian)(dian)(dian)沟道(dao)与(yu)哩衬底(di)的导电(dian)(dian)(dian)类型(xing)(xing)相反,因(yin)此该表(biao)面(mian)导电(dian)(dian)(dian)沟道(dao)被(bei)称 为(wei)(wei)(wei)(wei)反型(xing)(xing)层。
在Vgs=Vth时,表面的少数载流子浓度(电子)等于休内的多数载流子(空穴)的浓度。栅压越高,表面少数载流子的电荷密度Qi越高。(可动电荷Qi也可称为反型电荷)此时,假定漏源之间存在电势差,由于载流子(NMOS中为电子)的(de)扩散,会构成电(dian)(dian)(dian)流Ids。这时PN结的(de)透露电(dian)(dian)(dian)流仍然(ran)存在,但它与(yu) 沟道电(dian)(dian)(dian)流相比非常小(xiao),普通可(ke)以忽略。由于反型电(dian)(dian)(dian)荷Qi猛(meng)烈(lie)地(di)依赖与(yu)栅压(ya),因(yin)此(ci)可(ke)以应用栅压(ya)控制沟道电(dian)(dian)(dian)流。
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