Brillouin fiber laser spectrometer
An apparatus includes a spectrometer receiving an optical input signal that includes an input optical spectrum. The spectrometer includes a fiber laser cavity pumped by a first optical replica of the optical input signal that generates stimulated Brillouin scattering traveling in a direction opposite to a direction of the optical input signal. The first optical replica of the optical input signal excites at least one lasing mode in the fiber laser cavity. The at least one lasing mode respectively includes at least one lasing mode frequency. The at least one lasing mode frequency is offset by a respective Brillouin frequency shift from the respective at least one input frequency. The spectrometer also includes an optical heterodyne receiver. The optical heterodyne receiver generates the electrical output signal. The spectrometer outputs a measurement of the input optical spectrum based on the respective Brillouin frequency shift and the at least one input frequency.
1. An apparatus comprising:
a spectrometer receiving an optical input signal, the optical input signal comprising an input optical spectrum, said input optical spectrum comprising at least one input frequency, said spectrometer being free of a pump generator generating the optical input signal, said spectrometer outputting a measurement of the input optical spectrum, said spectrometer comprising:
a fiber laser cavity pumped by a first optical replica of the optical input signal, the first optical replica of the optical input signal generating stimulated Brillouin scattering traveling in a direction opposite to a direction of the optical input signal, the first optical replica of the optical input signal exciting at least one lasing mode in the fiber laser cavity, the at least one lasing mode respectively comprising at least one lasing mode frequency, the at least one lasing mode frequency being offset by a respective Brillouin frequency shift from the respective at least one input frequency, said fiber laser cavity outputting a portion of the at least one lasing mode;
an optical heterodyne receiver receiving a second optical replica of the optical input signal and, from said fiber laser cavity, the portion of at least one lasing mode, said optical heterodyne receiver generating an electrical output signal, the electrical output signal comprising an output electrical spectrum that includes a compressed, electrical replica of the input optical spectrum; and
a processor receiving the electrical output signal and outputting the measurement of the input optical spectrum based on a monotonic relationship between the respective Brillouin frequency shift and the at least one input frequency.
2. The apparatus according to claim 1 , wherein said fiber laser cavity comprises a round-trip time of flight and further comprises:
a first electro-optic modulator pulsing the at least one lasing mode at a repetition rate that approximately matches the round-trip time of flight so that stimulated Brillouin scattering amplifies the at least one pulsed lasing mode.
3. The apparatus according to claim 2 , wherein said fiber laser cavity comprises:
a first non-resonant pumping circulator receiving the first optical replica of the optical input signal.
4. The apparatus according to claim 3 , wherein said spectrometer further comprises:
a first optical amplifier outside of said fiber laser cavity and amplifying the optical input signal before said fiber laser cavity receives the first optical replica of the optical input signal,
wherein said fiber laser cavity comprises a lasing threshold and the first optical replica of the optical input signal comprises a power, said first optical amplifier amplifying the power so that the power exceeds the lasing threshold.
5. The apparatus according to claim 4 , wherein said first optical amplifier comprises one of a doped fiber amplifier, a semiconductor optical amplifier, and a fiber Raman amplifier.
6. The apparatus according to claim 4 , wherein said fiber laser cavity comprises at least one of:
a second non-resonant pumping circulator operably connected to said first non-resonant pumping circulator; and
a second optical amplifier operably connected to said electro-optic modulator and capable of spectral hole burning, thereby reducing gain-competition.
7. The apparatus according to claim 5 , wherein said spectrometer further comprises:
a splitter operably connecting to said first optical amplifier and to said optical heterodyne receiver; and
a first coupler operably connecting said first electro-optic modulator to said optical heterodyne receiver,
wherein said optical heterodyne receiver comprises:
a second coupler receiving the second optical replica of the optical input signal from the first coupler and receiving the portion of the at least one lasing mode from said fiber laser cavity via said first coupler; and
a photodetector operably connected to said second coupler.
8. The apparatus according to claim 7 , wherein said photodetector generates photodetector output,
wherein said spectrometer comprises:
an electrical downconverter operably connected to said photodetector and to said processor, said electrical downconverter electrically downshifting the photodetector output to generate the electrical output signal.
9. The apparatus according to claim 7 , wherein said optical heterodyne receiver comprises:
a second electro-optic modulator operably connecting said splitter and said second coupler, said second electro-optic modulator downshifting the second optical replica of the optical input signal, said second electro-optic modulator transmitting the downshifted second optical replica of the optical input signal to said second coupler.
10. The apparatus according to claim 1 , wherein said fiber laser cavity comprises a fiber ring cavity.
11. The apparatus according to claim 1 , wherein the output electrical spectrum comprises a radio frequency spectrum.