Polarization and wavelength stable superfluorescent sources using Faraday rotator mirrors
First Claim
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1. A superfluorescent source, comprising:
- an optical pump;
a laser medium with a dopant therein, the medium being pumped by pump light from the optical pump, the medium producing amplified spontaneous emission (ASE) having first and second orthogonal polarization components, the pump light providing unequal gain to the ASE in the first and second polarization components to cause the ASE to have a spectrum that has a mean wavelength for the first orthogonal polarization component that is different than a mean wavelength for the second orthogonal polarization component, the ASE being emitted from the medium in first and second directions;
an optical coupler that optically couples the pump to the medium;
a Faraday rotator mirror that receives the ASE emitted from the medium in the first direction and that reflects the ASE back to the medium to propagate in the second direction through the medium and be emitted from the medium in the second direction, the Faraday rotator mirror rotating the polarization of each orthogonal component of the reflected ASE by 90 degrees to cause the ASE emitted from the medium in the first direction in the first polarization to propagate back through the medium in the second direction in the second polarization and to cause the ASE emitted from the medium in the first direction in the second polarization to propagate back through the medium in the second direction in the first polarization, the pump light providing unequal gains to the first and second orthogonal polarization components of the reflected ASE propagating through the medium in the second direction such that a net gain experienced by the first orthogonal polarization component of the reflected ASE emitted from medium in the second direction is approximately equal to a net gain experienced by the second orthogonal polarization component of the reflected ASE emitted from the medium in the second direction, thereby reducing the polarization dependence of the output of the source; and
an output port that couples ASE emitted in the second direction from the source.
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Abstract
The wavelength stability of superfluorescent sources is controlled with optical arrangements in which the polarization-dependent gain (PDG) induced by the polarized pump light is reduced. In one apparatus and method, a Faraday rotator mirror is used at the end of the waveguide in the superfluorescent source. In another apparatus and method, the birefringence of the waveguide is exploited in conjunction with a Faraday rotator mirror to further average out the effect of PDG on the mean wavelength difference between the spectral outputs of orthogonal polarization components.
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Citations
27 Claims
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1. A superfluorescent source, comprising:
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an optical pump;
a laser medium with a dopant therein, the medium being pumped by pump light from the optical pump, the medium producing amplified spontaneous emission (ASE) having first and second orthogonal polarization components, the pump light providing unequal gain to the ASE in the first and second polarization components to cause the ASE to have a spectrum that has a mean wavelength for the first orthogonal polarization component that is different than a mean wavelength for the second orthogonal polarization component, the ASE being emitted from the medium in first and second directions;
an optical coupler that optically couples the pump to the medium;
a Faraday rotator mirror that receives the ASE emitted from the medium in the first direction and that reflects the ASE back to the medium to propagate in the second direction through the medium and be emitted from the medium in the second direction, the Faraday rotator mirror rotating the polarization of each orthogonal component of the reflected ASE by 90 degrees to cause the ASE emitted from the medium in the first direction in the first polarization to propagate back through the medium in the second direction in the second polarization and to cause the ASE emitted from the medium in the first direction in the second polarization to propagate back through the medium in the second direction in the first polarization, the pump light providing unequal gains to the first and second orthogonal polarization components of the reflected ASE propagating through the medium in the second direction such that a net gain experienced by the first orthogonal polarization component of the reflected ASE emitted from medium in the second direction is approximately equal to a net gain experienced by the second orthogonal polarization component of the reflected ASE emitted from the medium in the second direction, thereby reducing the polarization dependence of the output of the source; and
an output port that couples ASE emitted in the second direction from the source. - View Dependent Claims (2, 3, 4, 5, 6, 9, 10, 11, 12, 13, 14, 15, 16)
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7. A superfluorescent source, comprising:
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a laser medium with a dopant therein that produces amplified spontaneous emission (ASE) whose spectrum has a mean wavelength that is different for different polarization components of the ASE, said medium being pumped by pump light from said optical pump, wherein said medium is polarization maintaining and the pump light is directed into said medium in such a way that equal powers of the pump light are launched along birefringence axes of said medium;
an optical coupler that optically couples said pump to said medium;
a Faraday rotator mirror that reduces the polarization dependence of the output of said source, said mirror reflecting ASE emitted from said medium back through said medium; and
an output port that couples ASE from said source. - View Dependent Claims (8, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26, 27)
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Specification
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Current AssigneeBoard of Trustees of the Leland Stanford Junior University (Stanford University)
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Original AssigneeBoard of Trustees of the Leland Stanford Junior University (Stanford University)
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InventorsFalquier, Dario G., Digonnet, Michel J. F.
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Primary Examiner(s)Hellner, Mark
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Application NumberUS09/429,044Time in Patent Office1,117 DaysField of Search359/333, 359/341.1, 372/6, 372/19US Class Current359/333CPC Class CodesH01S 3/06795 with superfluorescent emiss...
