An optical pulse source, comprising: a first single mode DFB semiconductor laser having a first grating for generating light at a first frequency; a second single mode DFB semiconductor laser having a second grating for generating light at a second frequency; the lasers having a common active medium and shared optical path, the lasers providing mutual light injection imposed on each other resulting in generation of a beat signal at a difference frequency of two lasers; an optical compressor disposed for receiving the beat signal and compressing the pulse duration of the signal, thus forming a train of short optical pulses having a pre-determined duration and a repetition rate.
›2.↳ 1A source as defined in claim 1 further comprising a saturable absorber disposed to receive the beat signal before it is received by the compressor, th…d2+2
A source as defined in claim 1 further comprising a saturable absorber disposed to receive the beat signal before it is received by the compressor, the absorber providing an initial time compression of the signal, thus transforming the beat signal into an initial train of optical pulses.
›3.↳ 2A source as defined in claim 2 further comprising an optical amplifier for amplification the initial train of pulses.d3+1
A source as defined in claim 2 further comprising an optical amplifier for amplification the initial train of pulses.
›7.↳ 3A source as defined in claim 3 wherein the optical amplifier comprises an erbium doped fiber amplifier.d4
A source as defined in claim 3 wherein the optical amplifier comprises an erbium doped fiber amplifier.
›4.↳ 1A source as defined in claim 1 wherein the optical compressor comprises a dispersion decreasing fiber.d2
A source as defined in claim 1 wherein the optical compressor comprises a dispersion decreasing fiber.
›5.↳ 1A source as defined in claim 1 wherein the optical compressor comprises a dispersion shifted fiber.d2
A source as defined in claim 1 wherein the optical compressor comprises a dispersion shifted fiber.
›6.↳ 1A source as defined in claim 1 wherein the optical compressor comprises an erbium doped fiber amplifier.d2
A source as defined in claim 1 wherein the optical compressor comprises an erbium doped fiber amplifier.
›8.↳ 1A source as defined in claim 1 further comprising means for data encoding into the train of short pulses.d2+1
A source as defined in claim 1 further comprising means for data encoding into the train of short pulses.
›9.↳ 8A source as defined in claim 8 wherein the means for data encoding comprises an optical modulator operating at a speed determined by the repetition ra…d3
A source as defined in claim 8 wherein the means for data encoding comprises an optical modulator operating at a speed determined by the repetition rate.
›10.↳ 1A source as defined in claim 1 wherein the repetition rate of the pulse train is from approximately several tens GHz to approximately several hundred …d2
A source as defined in claim 1 wherein the repetition rate of the pulse train is from approximately several tens GHz to approximately several hundred GHz.
›11.↳ 1A source as defined in claim 1 wherein the repetition rate of the pulse train is from approximately 20 GHz to approximately 80 GHz.d2+1
A source as defined in claim 1 wherein the repetition rate of the pulse train is from approximately 20 GHz to approximately 80 GHz.
›18.↳ 11A source radiation as defined in claim 11 further comprising means for stabilizing the frequencies of both lasers.d3
A source radiation as defined in claim 11 further comprising means for stabilizing the frequencies of both lasers.
›12.↳ 1A source as defined in claim 1 wherein the duration of pulses in the pulse train is within a range from sub picoseconds to picoseconds.d2
A source as defined in claim 1 wherein the duration of pulses in the pulse train is within a range from sub picoseconds to picoseconds.
›13.↳ 1A source as defined in claim 1 wherein first and second DFB lasers comprise one of the gain coupled and loss coupled DFB lasers.d2+3
A source as defined in claim 1 wherein first and second DFB lasers comprise one of the gain coupled and loss coupled DFB lasers.
›14.↳ 13A source as defined in claim 13 wherein the active medium includes a multiple quantum well structure.d3+2
A source as defined in claim 13 wherein the active medium includes a multiple quantum well structure.
›15.↳ 14A source as defined in claim 14 wherein the first and second gratings are formed by etching grooves directly through the multiple quantum well structu…d4+1
A source as defined in claim 14 wherein the first and second gratings are formed by etching grooves directly through the multiple quantum well structure.
›16.↳ 15A source as defined in claim 15 wherein each grating has a period comprising a first section and a second section with substantially all quantum wells…d5
A source as defined in claim 15 wherein each grating has a period comprising a first section and a second section with substantially all quantum wells being etched away from the second section, thus providing no substantial photon emission in the second section and ensuring no substantial interaction between the lasers.
›17.↳ 1A source as defined in claim 1 further comprising means for stabilizing the frequency of one of the first and second lasers.d2
A source as defined in claim 1 further comprising means for stabilizing the frequency of one of the first and second lasers.
›19.↳ 1A source as defined in claim 1 further comprising means for tuning frequencies of the first and second lasers.d2
A source as defined in claim 1 further comprising means for tuning frequencies of the first and second lasers.
›20.↳ 1A source as defined in claim 1 further comprising means for modulating light generated by one of the first and second lasers.d2+1
A source as defined in claim 1 further comprising means for modulating light generated by one of the first and second lasers.
›21.↳ 20A source as defined in claim 20 wherein the modulation is provided at a frequency which is subharmonic to the beat frequency.d3
A source as defined in claim 20 wherein the modulation is provided at a frequency which is subharmonic to the beat frequency.
›22.↳ 1A source as defined in claim 1 further comprising means for modulating light generated by the lasers simultaneously.d2
A source as defined in claim 1 further comprising means for modulating light generated by the lasers simultaneously.
›23.↳ 1A source defined in claim 1 wherein pumping of the active medium is provided by current injection into the active medium.d2
A source defined in claim 1 wherein pumping of the active medium is provided by current injection into the active medium.
›24.↳ 1A source defined in claim 1 wherein pumping of the active medium is provided by an external optical pumping source.d2
A source defined in claim 1 wherein pumping of the active medium is provided by an external optical pumping source.
›25.↳ 1A source as defined in claim 1 wherein the first and second gratings have same periods.d2+5
A source as defined in claim 1 wherein the first and second gratings have same periods.
›26.↳ 25A source as defined in claim 25 wherein the first and second lasers generate light at the same side of stopband.d3+3
A source as defined in claim 25 wherein the first and second lasers generate light at the same side of stopband.
›27.↳ 26A source as defined in claim 26 wherein the difference between the first and second frequencies is provided by different current injection into the fi…d4
A source as defined in claim 26 wherein the difference between the first and second frequencies is provided by different current injection into the first and second lasers.
›28.↳ 26A source as defined in claim 26 wherein the difference between the first and second frequencies is provided by different width of the active medium in…d4
A source as defined in claim 26 wherein the difference between the first and second frequencies is provided by different width of the active medium in the first and second lasers.
›29.↳ 26A source as defined in claim 26 wherein the difference between the first and second frequencies is provided by difference in temperatures at which the…d4
A source as defined in claim 26 wherein the difference between the first and second frequencies is provided by difference in temperatures at which the first and second lasers are maintained.
›30.↳ 25A source as defined in claim 25 wherein the first and second lasers generate light at different sides of stopband.d3
A source as defined in claim 25 wherein the first and second lasers generate light at different sides of stopband.
›31.↳ 1A source as defined in claim 1 wherein the first and second gratings have different periods.d2+1
A source as defined in claim 1 wherein the first and second gratings have different periods.
›32.↳ 31A source as defined in claim 31 wherein the frequency of one of the lasers which is remote from an output facet does not fall within a stopband of the…d3
A source as defined in claim 31 wherein the frequency of one of the lasers which is remote from an output facet does not fall within a stopband of the other laser which is closer to the output facet so that light emitted by the remote laser can pass through the shared optical path to the output facet.
›33.↳ 1A source as defined in claim 1 wherein the first and second gratings comprise one of the uniform and chirped gratings.d2
A source as defined in claim 1 wherein the first and second gratings comprise one of the uniform and chirped gratings.
›34.↳ 1A source as defined in claim 1 wherein the first and second gratings are first order gratings.d2
A source as defined in claim 1 wherein the first and second gratings are first order gratings.
›35.↳ 1A source as defined in claim 1 wherein the first and second gratings are formed by one of the holographic writing and electron beam writing onto the a…d2
A source as defined in claim 1 wherein the first and second gratings are formed by one of the holographic writing and electron beam writing onto the active medium.