Semiconductor devices by laser enhanced diffusion
AssigneeMotorola, Inc.
InventorsJames N. Smith, Arthur D. Thompson, III
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Abstract
A process is described for the doping of semiconductors utilizing laser beam melting of the semiconductor surface in the presence of a dopant source. By selecting the laser wavelength to satisfy one of several criteria relating the semiconductor absorption coefficient and wafer thickness, or the dopant thickness and doping depth, the heating and melting are constrained to occur in a small local region near the surface where the laser beam impinges. Use of this invention to produce Zener diodes having abrupt doping profiles, as well as other device structures, is also discussed.
Claims11
A process utilizing a laser beam of wavelength .lambda. for doping a region of area A and depth d, wherein d is measured perpendicular to A, in a semiconductor body while the average temperature T of said semiconductor body during doping remains within a small range T-T.sub.A of initial ambient temperature T.sub.A of said semiconductor body, comprising the steps of:
- forming a dopant source of thickness t on said semiconductor body, wherein t.ltoreq.d and said dopant source and semiconductor body form a combination;
- choosing said wavelength .lambda. so that at said ambient temperature T.sub.A, more than 90% of the energy of said laser beam is absorbed within said combination in a depth D.ltoreq.n (t+d) where n.ltoreq.10, and D is measured perpendicular to A from an exterior surface of said dopant source means;
- placing said combination in a path of said laser beam;
- energizing said laser beam to an energy density Q which exceeds a melting threshold Q.sub.m but is less than a boiling threshold Q.sub.B so as to melt a small local surface region of said combination substantially immediately beneath a spot within area A where said laser beam impinges on said combination so that the depth of melting in said semiconductor body corresponds substantially to d;
- moving said combination and said laser beam relative to each other so that other small local surface regions newly illuminated by said laser beam are successively melted, and local surface regions no longer illuminated successively refreeze;
- continuing until substantially the entire area A has been melted and refrozen.
A process utilizing a laser beam of wavelength .lambda. for doping a region of area A and depth d, wherein d is measured perpendicular to A, in a semiconductor body while the average temperature T of said semiconductor body during doping remains within a small range T-T.sub.A of initial ambient temperature T.sub.A of said semiconductor body, comprising the steps of:
- forming a dopant source of thickness t on said semiconductor body, wherein t.ltoreq.d, and said dopant source and semiconductor body form a combination;
- choosing said wavelength .lambda. so that .alpha.L>5 wherein .alpha. is the absorption coefficient at said initial ambient temperature T.sub.A and L is the thickness of said semiconductor body, L being measured in the direction traversed by said laser beam;
- placing said combination in a path of said laser beam;
- energizing said laser beam to an energy density Q which exceeds a melting threshold Q.sub.m but is less than a boiling threshold Q.sub.B so as to melt a small local surface region of said combination substantially immediately beneath a spot within area A where said laser beam impinges on said combination so that the depth of melting in said semiconductor body corresponds substantially to d;
- moving said combination and said laser beam relative to each other so that other small local surface regions newly illuminated by said laser beam are successively melted;
- and local surface regions no longer illuminated successively refreeze;
- continuing until substantially the entire area A has been melted and refrozen.
A process utilizing a laser beam of wavelength .lambda. for doping a region of area A and depth d, wherein d is measured perpendicular to A, in a semiconductor body while the average temperature T of said semiconductor body during doping remains within a small range T-T.sub.A of initial ambient temperature T.sub.A of said semiconductor body, comprising the steps of:
- forming a dopant source of thickness t on said semiconductor body, wherein t.ltoreq.d, and said dopant source and semiconductor body form a combination;
- choosing said wavelength .lambda. so that .alpha..sub.1 L>5+1n (.alpha..sub.2 /.alpha..sub.1) for .alpha..sub.2 >.alpha..sub.1 and .alpha..sub.1 L>5 for .alpha..sub.2 .ltoreq..alpha..sub.1, wherein .alpha..sub.1 is the absorption coefficient at said initial ambient temperature T.sub.A of a first region of said semiconductor body of first conductivity, first encountered by said laser beam, and .alpha..sub.2 is the absorption coefficient at said initial ambient temperature T.sub.A of a second region of said semiconductor body of second conductivity, next encountered by said laser beam on passing through said first region, and L is the thickness of said semiconductor body measured in the direction traversed by said laser beam;
- placing said combination in a path of said laser beam;
- energizing said laser beam to an energy density Q which exceeds a melting threshold Q.sub.m but is less than a boiling threshold Q.sub.B so as to melt a small local surface region of said combination substantially immediately beneath a spot within area A where said laser beam impinges on said combination so that the depth of melting in said semiconductor body corresponds substantially to d;
- moving said combination and said laser beam relative to each other so that other small local surface regions newly illuminated by said laser beam are successively melted;
- and local surface regions no longer illuminated successively refreeze;
- continuing until substantially the entire area A has been melted and refrozen.
Dependencies are inferred from the claim text.