Laser resonator cavities with wavelength tuning arrangements
AssigneeMassachusetts Institute of Technology
InventorAli Javan
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AssigneeMassachusetts Institute of Technology
InventorAli Javan
Estimating the term…
Novel laser resonator cavities and laser wavelength tuning arrangements are disclosed. A pair of similar spectral dispersion means achieve in the resonator both a colinear region for rays of different wavelengths and a region in which rays of different wavelengths coextend separated and substantially parallel. Amplifying medium in an optical cavity following at least a first dispersion means, preferably in the parallel region of a laser having paired dispersion means, enable amplification at the different wavelengths while limiting their coupling via the amplifying medium. One or a number of apertures disposed in a dispersed path within a laser cavity are positioned to transmit a selected ray or rays and to block rays of unwanted wavelength whereby laser oscillation wavelength is determined. The above features are variously combined to achieve colinear output beams of various wavelengths and injection-type control of laser oscillation. Variable reflecting optics, e.g., a rotary mirror in a dispersed path, preferably in the near-parallel region of a laser having paired dispersion means, select different dispersed rays for reflection, enabling, e.g., rapid frequency scanning in a colinear output beam.
In a laser comprising an optical cavity defined by first and second reflecting optics, a first amplifying medium within the cavity and means to excite said medium to produce lasing conditions, said laser including means to restrict the laser beam to a common path for all wavelengths in the region of said first reflecting optics, the improvement comprising means including spectral dispersion apparatus disposed within the optical cavity, positioned to receive a beam of restricted cross section in said common path from said first reflecting optics and to disperse said beam to a plurality of paths in which rays of different wavelength are laterally spaced apart, said paths passing through said first amplifying medium whereby rays differing in wavelength can be subjected to amplification in different spatially separated portions of said first amplifying medium, said second reflecting optics constructed to reflect regeneratively said rays back along said paths, in laterally spaced apart condition through said portions of said first amplifying medium for further amplification, thence from said spectral dispersion apparatus along said common path to said first reflecting optics, said laser including a second amplifying medium disposed in the common beam path between said first reflecting optics and said spectral dispersion apparatus, in which path said rays are in a non-resolved, overlapping relation, and means to excite both said first and said second amplifying medium whereby a given wavelength amplified in a portion of said first amplifying medium can be present in said common beam path to cause excitation of laser oscillation at said wavelength in said second amplifying medium.
In a laser comprising an optical cavity defined by first and second reflecting optics and amplifying medium within the cavity, said laser including means to restrict the laser beam to a common path for a band of wavelengths for the output of said laser, the improvement comprising means including spectral dispersion apparatus disposed within the optical cavity, positioned to receive a beam of restricted cross section in said common path and to disperse said beam, said first and second reflecting optics constructed to reflect regeneratively said rays back and forth in said cavity along a regenerative path for amplification by said amplifying medium, a second source of radiation separate from said amplifying medium for producing radiation at a selected frequency and disposed to transmit said radiation at a relatively weak intensity to follow the said regenerative path, and means to excite both said second source and said first mentioned amplifying medium whereby a given wavelengths originating in said second source can be present in said amplifying medium to determine the wavelength of radiation amplified by said amplifying medium, whereby radiation at the determined frequency and at a relatively high level of intensity can be produced at said output.
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