Laser tuning by spectrally dependent spatial filtering
Abstract
A laser tuning mechanism which embodies “spectrally dependent spatial filtering” (SDSF) and contemplates two key elements of the tuning mechanism. The first element of the SDSF tuning mechanism is a spectrally dependent beam distortion (i.e. alteration of the amplitude and/or phase profile of the beam) provided by an SDSF tuning element in a laser cavity. The second element of the SDSF tuning mechanism is an intracavity spatial filter which makes the round trip cavity loss a sensitive function of both beam distortion and cavity alignment. Such a laser can be aligned so that a specific beam distortion, which is provided by the SDSF tuning element at a tunable wavelength, is required to obtain minimum round trip cavity loss, thereby providing tunable laser emission. A preferred embodiment of the SDSF tuning mechanism is an external cavity semiconductor laser having a zeroth order acousto-optic tuning element.
Claims
exact text as granted — not AI-modified1 . A laser comprising an optical resonator, said optical resonator comprising:
a) a pumped gain medium; and b) a tuning element comprising a tunable optical spectral notch filter; wherein said optical resonator is aligned such that radiation is emitted from said optical resonator at substantially a single emission wavelength which is selected by said tuning element.
2 . The laser of claim 1 wherein said tuning element comprises a volume hologram.
3 . The laser of claim 1 wherein a three wave parametric interaction occurs within said tuning element.
4 . The laser of claim 3 wherein said three wave parametric interaction is an acousto-optic interaction and an optical beam circulating within said optical resonator passes through said tuning element as a zeroth order beam.
5 . The laser of claim 1 wherein said optical resonator further comprises a grid fixing etalon.
6 . The laser of claim 1 wherein a parasitic etalon within said optical resonator provides discrete tunability.
7 . The laser of claim 1 wherein the round trip path length of said optical resonator is selected so as to provide discrete tunability.
8 . The laser of claim 1 further comprising means for monitoring said single emission wavelength.
9 . The laser of claim 1 further comprising means for monitoring a wavelength difference between said single emission wavelength and a center wavelength of said tuning element.
10 . A method for generating a laser beam comprising:
a) pumping a gain medium positioned within an optical resonator, said optical resonator defining an intracavity beam path; and b) passing light traveling on said beam path through a tunable optical spectral notch filter provided by a tuning element; wherein said optical resonator is aligned such that radiation is emitted from said optical resonator at substantially a single emission wavelength which is selected by said tuning element.
11 . The method of claim 10 further comprising passing light traveling on said beam path through a spatial filter.
12 . The method of claim 10 wherein said tuning element comprises a volume hologram.
13 . The method of claim 10 wherein a three wave parametric interaction occurs within said tuning element.
14 . The method of claim 13 wherein said three wave parametric interaction is an acousto-optic interaction.
15 . The method of claim 10 further comprising passing light traveling on said beam path through a grid fixing etalon.
16 . The method of claim 10 wherein a parasitic etalon within said optical resonator provides discrete tunability.
17 . The method of claim 10 wherein the optical length of said beam path is selected so as to provide discrete tunability.
18 . The method of claim 10 wherein an acousto-optic interaction occurs within said tuning element, said method further comprising:
c) emitting a portion of a first order beam from said optical resonator to provide a first order signal; d) emitting a portion of a zeroth order beam from said optical resonator to provide a zeroth order signal; e) deriving a normalized first order signal from said first order signal and said zeroth order signal; and f) controlling the center wavelength of said tuning element to hold said normalized first order signal fixed to a predetermined value.
19 . A laser comprising an optical resonator, said optical resonator comprising:
a) a pumped gain medium; and b) means for selecting an emission wavelength; wherein said optical resonator is aligned such that radiation is emitted from said optical resonator at substantially said emission wavelength which is selected by said means in accordance with a spectrally dependent spatial filtering (SDSF) tuning mechanism.Cited by (0)
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