Dissipative soliton mode fiber based optical parametric oscillator
US-9140959-B2 · Sep 22, 2015 · US
US9684223B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9684223-B2 |
| Application number | US-201514616531-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 6, 2015 |
| Priority date | Feb 6, 2015 |
| Publication date | Jun 20, 2017 |
| Grant date | Jun 20, 2017 |
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An optical apparatus that includes an optical source that generates a first optical pulse with a first optical wavelength. The optical apparatus also includes an optical amplifier that outputs an amplified pulse. The optical apparatus also includes a first waveguide that is connected to the optical amplifier and a second waveguide. Wherein the second waveguide converts the energy of the amplified pulse into energy of a second pulse that has a second optical wavelength different from the first optical wavelength. Wherein, the following equation is satisfied: L_min≦L≦π/γP. In which a length of the first waveguide is L, a nonlinear coefficient of the first waveguide is γ, a peak power of the amplified pulse as it is received by the first waveguide is P, and a minimum length of the first waveguide is L_min or L is equal to zero.
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What is claimed is: 1. An optical apparatus comprising: an optical source that generates a first pulse with a first optical wavelength; an optical amplifier that amplifies the first pulse and outputs an amplified pulse with the first optical wavelength; a first waveguide that is connected to the optical amplifier which receives the amplified pulse; a second waveguide that is connected to the first waveguide and receives the amplified pulse, wherein the second waveguide converts the energy of the amplified pulse into energy of a second pulse while a relative center position of the second pulse for the amplified pulse is crossing a center position of the amplified pulse in a first direction, wherein the second pulse has a second optical wavelength different from the first optical wavelength; wherein the amplifier, the first waveguide, and the second waveguide form an optical loop which feeds the second pulse back to the amplifier, the first waveguide, and the second waveguide; an output coupler to output a portion of the second pulse outside of the optical loop; wherein the following equation is satisfied: L min ≦L≦π/γP, in which a length of the first waveguide is L, a nonlinear coefficient of the first waveguide is γ, a peak power of the amplified pulse as it is received by the first waveguide is P, and a minimum length of the first waveguide is L min . 2. The optical apparatus according to claim 1 , wherein the energy of the first pulse is converted to the energy of the second pulse by a parametric process. 3. The optical apparatus according to claim 2 , wherein the first pulse is used as a pump wave and the second pulse is an idler wave or a signal wave. 4. The optical apparatus according to claim 1 , wherein the second waveguide comprises a photonic crystal fiber. 5. The optical apparatus according to claim 1 , wherein the optical amplifier includes at least one fiber selected from the group of: double clad gain fiber, polarization maintaining double clad gain fiber, single mode gain fiber, and polarization maintaining gain fiber. 6. The optical apparatus according to claim 1 , further comprising a third waveguide after the optical coupler in the optical loop; wherein a length of the third waveguide is “I”, a pulse duration of the first pulse is “t”, and a dispersion parameter of the second pulse is “D” in the third waveguide which satisfy the following equation: I≧t/D. 7. The optical apparatus according to claim 1 , wherein L min is 10 mm.
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