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RADIATION ENHANCED DIFFUSION

机译:辐射增强扩散

摘要

1401276 Semi-conductor devices MULLARD Ltd 28 July 1972 [6 Sept 1971] 41462/71 Addition to 1307546 Heading H1K In a method of manufacturing a semiconductor device in which impurity diffusion from a high impurity concentration region 14 to a lower impurity concentration region 20 is enhanced by the effect of bombarding radiation 19 incident on the region 20 and causing lattice damage therein, the crystal axes and radiation energy are chosen so that the incident particles channel through the crystal lattice at least as far as, but not substantially beyond, the boundary between the regions 14 and 20. In this way the lateral extent of the region 20 is more precisely controlled than would be the case if no channelling occurred. The radiation 19 is preferably protons, but may also comprise electrons, helium ions or donor or acceptor ions, the latter providing simultaneous bombardment enhanced diffusion and ion inplantation. The higher and lower doped regions may be of the same or opposite conductivity types. Fig. 4, illustrates the manufacture of a Si junction-gate FET in which current between source and drain electrodes passes vertically through channel portions of a 11D-oriented P-doped N-type epitaxial layer 12 bounded, and optionally surrounded, by P-type regions formed by channelled-bombardment enhanced diffusion of B from PSP+/SP-type buried layers 14 in the N-type substrate 11. The regions 20 are made to extend right through the thickness of the layer 12 by commencing proton bombardment at an energy such that the channelling range just reaches the substrate 11 and subsequently reducing the proton energy so that the damaged region, and hence the diffused region 20, extends progressively further from the impurity-source region 14. A mask 17 of Mo or Nichrome (Registered Trade Mark) defines the lateral extent of the damaged regions. PSP+/SP-type surface diffusions may also be effected into the windows 18 to ensure that the gate junction terminates beneath oxide layer 16. Source, gate and drain electrodes of Au/Sb alloy are applied respectively to the substrate 11, the regions 20 and the remaining regions of the epitaxial layer 12. For a 111 oriented wafer the radiation 19 may alternatively be caused to impinge obliquely upon the surface at such an angle that channelling may occur along the 110 axis. A further junction-gate FET is described (see Figs. 7-9, not shown) in which channel current passes horizontally through portions (40) of an N-type epitaxial layer bounded by P-type gate walls (38) formed in the manner of the invention. The channel portions (40) are entirely bounded by P-type gate portions constituted by the walls (38), the PSP+/SP-type buried layer (35) from which the impurity for the walls (38) has been caused to diffuse, and a surface implanted region interconnecting the walls (38). The manufacture of a vertical bipolar transistor having a profiled collector impurity distribution beneath the emitter region, and of a lateral bipolar transistor the regions of which are formed by channelled-bombardment enhanced diffusion of impurities into an epitaxial layer from buried regions prediffused into the substrate, are also briefly mentioned.
机译:1401276半导体器件MULLARD Ltd 1972年7月28日[1971年9月6日] 41462/71附加到标题H1K在制造半导体器件的方法中,其中杂质从高杂质浓度区域14到低杂质浓度区域20的扩散是通过轰击入射在区域20上的辐射19并在其中引起晶格破坏的效果增强,选择晶轴和辐射能,以使入射粒子至少穿过但不超过边界而穿过晶格。在区域14和20之间的区域之间,通过这种方式,与不发生沟道的情况相比,可以更精确地控制区域20的横向范围。辐射19优选是质子,但也可以包含电子,氦离子或施主或受主离子,后者同时提供轰击增强的扩散和离子注入。较高和较低掺杂区可以是相同或相反的导电类型。图4示出了Si结栅FET的制造,其中,源电极和漏电极之间的电流垂直地流过<11D-取向的P-掺杂的N-型外延层12的沟道部分,该沟道部分被P包围,并任选地被P包围。通过沟道轰击增强B从N型衬底11中的P + 型掩埋层14扩散而形成的B型区域。使区域20直接延伸穿过层12的厚度。通过以这样的能量开始质子轰击,使得沟道范围刚好到达衬底11,并且随后减小质子能量,从而使受损区域以及因此扩散区域20从杂质源区域14逐渐进一步延伸。掩模17钼或镍铬合金的商标(注册商标)定义了受损区域的横向范围。 P + 型表面扩散也可以在窗口18中进行,以确保栅极结在氧化物层16下方终止。Au/ Sb合金的源极,栅极和漏极分别施加到衬底上在图11中,区域20和外延层12的其余区域。对于<111>取向的晶片,可以替代地使辐射19以一定角度倾斜地入射在表面上,使得沿着<110>轴可能发生沟道。描述了另一结型栅极FET(见图7-9,未示出),其中沟道电流水平地流过由形成在半导体器件中的P型栅极壁(38)界定的N型外延层的部分(40)。本发明的方式。沟道部分(40)完全由由壁(38),P + 型掩埋层(35)构成的P型栅极部分界定,其中P + 型掩埋层(35)从该掩埋层构成壁(38)使金属扩散,并与壁(38)互连的表面植入区域。制造在发射极区下方具有分布的集电极杂质分布的垂直双极晶体管,以及横向双极晶体管的制造,该横向双极晶体管的区域是通过沟道轰击增强了杂质从预扩散到衬底中的掩埋区到外延层中扩散而形成的,也简要提及。

著录项

  • 公开/公告号CA970078A

    专利类型

  • 公开/公告日1975-06-24

    原文格式PDF

  • 申请/专利权人 N.V. PHILIPSGLOEILAMPENFABRIEKEN;

    申请/专利号CA19720150882

  • 发明设计人 SHANNON JOHN M.;

    申请日0000-00-00

  • 分类号H01L29/808;H01L21/00;H01L21/22;

  • 国家 CA

  • 入库时间 2022-08-23 04:18:50

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