Abstract:
Microwaves are generated by heterodyning the outputs of two or more optical lasers which have differing central frequencies to produce beat frequencies in the microwave range. One of the beat frequencies is used to modulate the output of at least one of the lasers so as to produce sidebands which differ from the central frequency by an integral number of the sideband frequency. Each laser is connected to one of the other lasers by a weak optical link to optically injection lock the laser to the sideband of the other laser.
Abstract:
A tunable semiconductor laser comprises a gain section having an MQW active region, a uniform pitch grating DFB region, and first waveguide. A composite reflector, including a second MQW region and a second waveguide, forms a cavity resonator with the DFB region. A tuning voltage applied to the composite reflector induces refractive index changes, thereby allowing the center wavelength to be altered. A dither signal applied the composite reflector broadens the spectrum of the laser output, thereby reducing SBS in fiber optic systems
Abstract:
The invention concerns the generation of synthetic light wavelengths in which light from a first light source (D.sub.1) is coupled into a common light path section (L.sub.G1) and its average frequency value (.nu..sub.1) is locked with a resonant frequency (.nu..sub.1) of the Fabry-Perot resonator (R). The light from a second light source (D.sub.2) is coupled into the common light path section (L.sub.G1) and its average frequency value (.nu..sub.2) is set in order to reach a subsequent resonant frequency (.nu..sub.2) of the Fabry-Perot resonator (R) and be locked therewith. A beat frequency (.DELTA..nu..sub.12), which is measured by electronic counters whilst a corresponding measured frequency value (f.sub.12) is prepared, is formed between the frequencies (.nu..sub.1, .nu..sub.2) of the light from the two light sources (D.sub.1, D.sub.2). The light from at least one further light source (D.sub.i) is coupled into the common light path section (L.sub.G1) and its average frequency value (.nu..sub.i) is first adapted to the average frequency value (.nu..sub.1 or .nu..sub.2) of one of the above light sources (D.sub.1, D.sub.2) and then altered until it reaches a pre-determined resonance of the Fabry-Perot resonator (R) and is locked therewith, the number (k.sub.1) of resonances passed through being counted. The beat frequency (.DELTA..nu..sub.1i or .DELTA..nu..sub.2i) between the frequency (.nu..sub.1 or .nu..sub.2) of the light from the selected light source (D.sub.1 or D.sub.2) and from the further light source (D.sub.i) is calculated as the product (k.sub.1 .times..DELTA..nu..sub.12 or k.sub.1 +1.times..DELTA..nu..sub.12) of the beat frequency (.DELTA..nu..sub.12) between the frequencies (.nu..sub.1, .nu..sub.2) of the light from the first and second light sources (D.sub.1, D.sub.2) and the number (k.sub.i or k.sub.1 +1) of resonances passed through.
Abstract:
Two independent laser oscillators are injection-locked to different optical modes of a mode-locked laser, then combined and detected to produce the heterodyne output signal in the microwave to submillimeter wave frequency band. Since the phase fluctuations of the mode-locked laser modes are highly correlated, the phase fluctuations of the heterodyne output signal are greatly reduced, providing a low phase-noise oscillator signal. Since the modes of the mode-locked laser can span hundreds of GigaHertz, the oscillator can be employed to generate microwave, millimeter wave or submillimeter wave frequencies.
Abstract:
A method for physical random number generation includes the steps of: modulating the gain of a vertical-cavity surface-emitting laser periodically from the lower threshold to the upper threshold and back; maintaining the gain per round trip positive for a longer period than the round trip time of the cavity; maintaining the net gain per round trip negative for a longer period than the round trip time of the cavity, in order to create optical pulses of random amplitude; detecting the optical pulses; converting the optical pulses into electrical analog pulses; and digitising the electrical analog pulses into random numbers.
Abstract:
Period-one nonlinear dynamics of semiconductor lasers are utilized to provide an apparatus for photonic microwave power amplification in radio-over-fiber links through optical modulation depth improvement. The microwave power amplification apparatus includes a microwave-modulated optical signal generation module and a microwave power amplification module. The amplification capability of the present microwave power amplification apparatus covers a broad microwave range, from less than 25 GHz to more than 60 GHz, and a wide gain range, from less than 10 dB to more than 30 dB. The microwave phase quality is mainly preserved while the microwave power is largely amplified, improving the signal-to-noise ratio up to at least 25 dB. The bit-error ratio at 1.25 Gb/s is better than 10−9 and a sensitivity improvement of up to at least 15 dB is feasible.
Abstract:
The invention relates to a beat signal generating device for use in a Terahertz system, comprising a first monomode laser for generating radiation of a first wavelength; a second monomode laser for generating radiation of a second wavelength different from the first wavelength; a first and a second output port; a phase modulating unit for modifying both the phase of radiation generated by the first laser and the phase of radiation generated the second laser, wherein the beat signal generating device is configured in such a way that the radiation generated by the first laser is transmitted through the second laser and superposed with the radiation generated by the second laser at the second output port, and the radiation generated by the second laser is transmitted through the first laser and superposed with the radiation generated by the first laser at the first output port, such that a first beat signal will be emitted at the first output port and a second beat signal will be emitted at the second output port, wherein the phase between the first and the second beat signal can be adjusted by means of the phase modulating unit. The invention also relates to a Terahertz system and the use of a beat signal generating device.
Abstract:
Provided is a terahertz wave apparatus. The terahertz wave apparatus includes: a wavelength-fixed laser emitting a first laser light having a fixed first wavelength; a wavelength-swept laser emitting a second laser light having a tunable second wavelength; a coupler coupling the first laser light with the second laser light; and a generator converting a mixed light emitted from the coupler into a terahertz wave, wherein a frequency of the terahertz wave is continuously tunable.
Abstract:
Provided is a multiple distributed feedback laser device. The laser device includes an active layer, a first diffraction grating, and a second diffraction grating. The substrate includes a first distributed feedback region, a modulation region, and a second distributed feedback region. The first diffraction grating is coupled to the active layer in the first distributed feedback region. The second diffraction grating is coupled to the active layer in the second distributed feedback region. In addition, the laser device includes a first micro heater and a second micro heater. The first micro heater supplies heat to the first diffraction grating. The second micro heater supplies heat to the second diffraction grating. The first micro heater and the second micro heater are controlled independently from each other.
Abstract:
The present invention provides a pulse train generator comprising: a dual-frequency signal light source for generating a dual-frequency signal; a soliton shaper for soliton-shaping output light from the dual-frequency signal light source; and an adiabatic soliton compressor for performing adiabatic soliton compression on output light from the soliton shaper, and also provides a waveform shaper used in this pulse train generator, including a plurality of highly nonlinear optical transmission lines and a plurality of low-nonlinearity optical transmission lines which has a nonlinearity coefficient lower than that of the plurality of highly nonlinear optical transmission lines and which has a second-order dispersion value of which an absolute value is different from that of the plurality of highly nonlinear optical transmission lines. Further, the present invention provides a light source comprising a plurality of continuous light sources of which at least one oscillates in a multimode; a multiplexer for multiplexing output light from the continuous light sources; and a nonlinear phenomenon producer for producing a nonlinear phenomenon on output light from the multiplexer so as to suppress SBS (Stimulated Brillouin Scattering).