Self-collimated unstable resonator semiconductor laser
AssigneeThe United States of America as represented by the United States National Aeronautics and Space Administration
InventorRobert J. Lang
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Abstract
Self-collimation of the output is achieved in an unstable resonator semiconductor laser by providing a large concave mirror M.sub.1 and a small convex mirror M.sub.2 on opposite surfaces of a semiconductor body of a material having an effective index of refraction denoted by n, where the respective mirror radii R.sub.1, R.sub.2 and beam radii r.sub.1, r.sub.2 are chosen to satisfy a condition ##EQU1## with a value of geometric magnification ##EQU2## where r.sub.1 and r.sub.2 are the radii of counterpropagating beams at respective mirrors of radii R.sub.1 and R.sub.2.
Claims7
A self-collimated unstable resonator semiconductor laser comprising a body of semiconductor material for emitting light in response to injected current, said semiconductor material having two opposing external surfaces shaped to form mirrors M.sub.1 and M.sub.2 of a resonant cavity, said mirror M.sub.1 being of a concave shape of radius R.sub.1 and the other surface mirror being of a convex shape of radius R.sub.2, said radius R.sub.2 being selected for said convex shape of mirror M.sub.2 for collimation of output rays passing through said mirror M.sub.2 by refraction as they exit said mirror M.sub.2.
A self-collimated unstable resonator semiconductor laser comprising a body of semiconductor material having an know index of refraction n, said semiconductor material emitting light in response to injected current and having two opposing external surfaces shaped to form mirrors M.sub.1 and M.sub.2 of a resonant cavity for said emitted light, said mirror M.sub.1 being of a concave shape of radius R.sub.1 for a counterpropagating beam of radius r.sub.1 ad said mirror M.sub.2 being of a concave shape of radius R.sub.2 for a counterpropagating beam of radius r.sub.2, said mirror radii R.sub.1 and R.sub.2 being chosen according to the following equations:
- ##EQU16## and said beam radii r.sub.1 and r.sub.2 being chosen according to the following equations:
- ##EQU17## where .alpha.=.beta./n, .beta..tbd.1-g.sub.2.sup.-1 and g.sub.2 .tbd.1-1/R.sub.2 with a value of geometric magnification 1.ltoreq.M.ltoreq.(n+1)/(n-1) to satisfy a condition ##EQU18##
A self-collimated unstable resonator semiconductor laser comprising a large concave mirror M.sub.1 and a small convex mirror M.sub.2 on opposite surfaces of a semiconductor body of a material having an effective index of refraction n, where the respective mirror radii R.sub.1, R.sub.2 are chosen according to the following equations:
- ##EQU19## and beam radii r.sub.1, r.sub.2 are chosen according to the following equations:
- ##EQU20## where .alpha.=.beta./n, .beta..tbd.1-g.sub.2.sup.-1 and g.sub.2 .tbd.1-1/R.sub.2 with a value of geometric magnification ##EQU21## to satisfy a condition:
- ##EQU22## where r.sub.1 and r.sub.2 are the radii of counterpropagating beams at respective mirrors of radii R.sub.1 and R.sub.2, for self-collimation of the output beam by refraction across discontinuity of the index of refraction at the exit of light rays from said convex mirror M.sub.2.
Dependencies are inferred from the claim text.