Fiber-laser-based gigahertz sources through difference frequency generation (DFG) by nonlinear optical (NLO) materials
A fiber-laser-based implementation of a Gigahertz source through difference frequency generation (DFG) by nonlinear optical (NLO) materials is compact, tunable and scalable. A pair of pulsed fiber lasers, preferably single-frequency, generate output pulses at frequencies ω 1 and ω 2 that overlap temporally. A beam combiner combines the laser outputs and routes the combined output to a GHz generator head where a nonlinear interaction process in the NLO material generates GHz radiation.
1. A Gigahertz (GHz) source, comprising:
a GHz generator head including a nonlinear optic (NLO) material;
a first Q-switched fiber laser configured to generate a first pulsed laser output at a frequency ω 1 ;
a second Q-switched fiber laser configured to generate a second pulsed laser output at a frequency ω 2 that at least partially temporally overlaps said first pulsed laser output; and
a beam combiner configured to combine the first and second laser outputs and routes the combined output to the GHz generator head where a nonlinear interaction process in the NLO material generates GHz radiation between 30 and 300 GHz that is output from the head,
where each said first and second Q-switched fiber laser comprises a polarization-dependent resonant cavity including a fiber chain having a gain medium between narrowband and broadband fiber gratings, a pump source that couples energy into the fiber chain to pump the gain medium and a modulator that applies stress to the fiber chain to induce birefringence and switch the cavity Q-factor to alternately store energy in the gain medium and then release the energy of the laser output in a laser pulse.
2. The GHz source of claim 1 , wherein the beam combiner is spliced between the first and second fiber lasers and the GHz generator head.
3. The GHz source of claim 1 , wherein at least a portion of the fiber chain comprises a polarization-dependent fiber.
4. The GHz source of claim 1 , wherein the narrowband fiber grating is formed in a polarization maintaining (PM) fiber creating a pair of reflection bands that correspond to different polarization modes, said broadband grating having a reflection band that is aligned to one of the narrowband grating's reflection bands.
5. The GHz source of claim 1 , wherein the modulator is a piezoelectric transducer (PZT).
6. The GHz source of claim 1 , wherein the first and second lasers emit single-transverse and single-longitudinal mode light.
7. The GHz source of claim 6 , wherein the GHz radiation is single-transverse and single-longitudinal mode.
8. A Gigahertz (GHz) source, comprising:
a GHz generator head including a nonlinear optic (NLO) material;
a first Q-switched fiber laser configured to generate a sequence of first laser single-transverse, single-longitudinal mode pulses at a frequency ω 1 ;
a second Q-switched fiber laser configured to generate a sequence of second single-transverse, single-longitudinal mode laser pulses at a frequency ω 2 , the Q-switching of said lasers being timed so that their laser pulses overlap temporally; and
a beam combiner configured to combine the first and second laser pulses and route the combined output to the GHz generator head where a nonlinear interaction process in the NLO material generates single-transverse, single-longitudinal mode GHz radiation between 30 and 300 GHz that is output from the head,
where each said first and second Q-switched fiber laser comprises a polarization-dependent resonant cavity including a fiber chain having a gain medium between narrowband and broadband fiber gratings, a pump source that couples energy into the fiber chain to pump the gain medium and a modulator that applies stress to the fiber chain to induce birefringence and switch the cavity Q-factor to alternately store energy in the gain medium and then release the energy of the laser output in a laser pulse.