Chip-integrated mode-locked lasers based on thin-film nonlinear waveguides
A chip-scale mode-locked laser including a cavity including a gain medium for amplifying signal electromagnetic radiation (signal) through stimulated emission, the signal comprising a signal wavelength; and a passive or active mode-locking device to enforce pulse formation in the laser. The mode-locking device includes a thin-film waveguide having a thickness on the order of the signal wavelength so as to confine and guide the signal along the thin-film waveguide, and a material comprising a second-order nonlinear susceptibility to enable active or passive mode-locking of the signal. The mode-locking device leads to generation of pulses of the signal outputted from the mode-locked laser.
1. A chip-scale mode-locked laser, comprising:
a cavity comprising:
a gain medium for amplifying signal electromagnetic radiation (signal) through stimulated emission, the signal comprising a signal wavelength; and
a passive mode-locking device that provides an intensity-dependent transmission or reflection for the signal to enforce pulse formation in the laser, the passive mode-locking device comprising:
a thin-film waveguide having a thickness on the order of the signal wavelength so as to confine and guide the signal along the thin-film waveguide,
a material comprising a second-order nonlinear susceptibility enabling at least one of second harmonic generation or optical parametric amplification of the signal along the waveguide, and
an output directional coupler providing different coupling ratios for the signal and a second harmonic of the signal (second harmonic), wherein the mode-locking device leads to generation of pulses of the signal outputted from the mode-locked laser.
2. The mode-locked laser of claim 1 , wherein the gain medium comprises a second material deposited on or integrated with the thin-film waveguide, providing the stimulated emission of the signal in a presence of a pump electromagnetic radiation (pump) pumping the second material.
3. The mode-locked laser of claim 2 , wherein the gain medium comprises a rare-earth ion-doped oxide.
4. The mode-locked laser of claim 2 , wherein the second material comprises a rare-earth ion-doped oxide gain grown on top of the waveguide by atomic layer deposition (ALD) process or rare-earth ions diffused into the waveguide at a high temperature.
5. The mode-locked laser of claim 1 , wherein the thin-film waveguide comprises a ridge having a width and the thickness guiding a mode associated with the signal, or a pump electromagnetic radiation optically pumping the gain medium to form the signal, with most of the mode's energy confined in a transverse cross-sectional area of the waveguide smaller than 3 micrometers by 3 micrometers.
6. The mode-locked laser of claim 1 , wherein:
the signal is formed in response to an input pump electromagnetic radiation pumping the gain medium,
the input pump is continuous wave, and
the pulses each have a pulse width of less than 100 picoseconds.
7. The mode-locked laser of claim 1 , wherein:
the gain medium comprises a semiconductor material that can be pumped either by pump electromagnetic radiation or electric current, and
the gain medium is integrated with the thin-film waveguide either through evanescent coupling or butt coupling.
8. The mode-locked laser of claim 7 , wherein the thin-film waveguide is butt-coupled to the gain medium and an input port of the thin-film waveguide is adiabatically tapered in width in order to match one or more mode sizes of the pump electromagnetic radiation in the thin-film waveguide and in the gain medium.
9. The mode-locked laser of claim 7 , wherein the thin-film waveguide is heterogeneously integrated with the gain medium through wafer bonding or micro-transfer-printing process and so that a transfer of the signal between the thin-film waveguide and the gain medium is through evanescent coupling.
10. The mode-locked laser of claim 1 , wherein:
the mode-locking device is configured as a nonlinear mirror to enforce the pulse formation and passive mode-locking of the signal electromagnetic radiation;
the nonlinear mirror further comprises metal electrodes next to the thin-film waveguide; and
a relative phase between the signal and the second harmonic of the signal can be adjusted by applying a voltage on the electrodes according to an electro-optical effect.
11. The mode-locked laser of claim 10 , wherein an output facet of the nonlinear mirror is mechanically polished and coated with a dielectric coating, and the dielectric coating ensures partial reflection of the signal and unity reflection of the second harmonic of the signal.
12. The mode-locked laser of claim 1 , wherein the mode-locking device further comprises an electro-optic modulator comprising metal electrodes next to the thin-film waveguide, wherein a radio-frequency voltage source applied on the electrodes applies an electric field across the thin-film waveguide so as to periodically modulate a refractive index of the thin-film according to an electro-optical effect.
13. The mode-locked laser of claim 1 , wherein the output directional coupler comprises a loop mirror.
14. The mode-locked laser of claim 1 , wherein the material of the thin-film waveguide comprises lithium niobate, lithium tantalate, Potassium Titanyl Phosphate (KTP), aluminum nitride, gallium arsenide, indium phosphide, or aluminum gallium arsenide.
15. The mode-locked laser of claim 1 , wherein:
the waveguide comprises a plurality of quasi-phase-matched regions through spatially varying nonlinear susceptibility, for instance through ferroelectric poling or orientation patterning, that ensures phase-matched second-order nonlinear interactions:
in a first region of the waveguide, wherein the mode locking device generates the second harmonic electromagnetic radiation comprising the second harmonic of the signal wavelength through the non-linear interaction comprising second harmonic generation,
in a second region, wherein the device down-converts at least a portion of the second harmonic electromagnetic radiation into the signal wavelength through the non-linear interaction comprising the optical parametric amplification;
the device further comprising the output directional coupler that preferentially couples the signal out of the laser cavity, as compared to the second harmonic, so as to selectively enhance resonance of higher intensity signal modes of the signal while suppressing resonance of lower-intensity signal modes in the cavity due to the stronger second harmonic generation processes in the first region of the waveguide and the stronger optical parametric amplification process in the second region of the waveguide for the higher intensity modes as compared to the lower intensity signal modes,
and the electromagnetic radiation coupled out of the cavity through the output directional coupler comprises a train of the mode-locked pulses each having a pulse duration of less than 100 picoseconds.
16. The mode-locked laser of claim 1 , wherein the waveguide comprises:
a first quasi-phase-matched region wherein a phase-matched nonlinear process is the second harmonic generation of signal,
a second quasi-phase-matched region wherein the signal is parametrically amplified by the second harmonic,
a third region between the first region and the second region to provide an approximately 180 phase shift in the relative phase of the signal and the second harmonic.
17. A method of making a chip-scale mode-locked laser, comprising:
providing a cavity comprising:
a gain medium for amplifying signal electromagnetic radiation (signal) through stimulated emission, the signal comprising a signal wavelength; and
a passive mode-locking device that provides an intensity-dependent transmission or reflection for the signal to enforce pulse formation in the laser, the mode-locking device comprising:
a thin-film waveguide having a thickness on the order of the signal wavelength so as to confine and guide the signal along the thin-film waveguide,
a material comprising a second-order nonlinear susceptibility enabling at least one of second harmonic generation or optical parametric amplification of the signal along the waveguide, and
an output directional coupler providing different coupling ratios for the signal and a second harmonic of the signal (second harmonic), wherein the mode-locking device leads to generation of pulses of the signal outputted from the mode-locked laser.
18. A method of operating a chip-scale mode-locked laser, comprising:
coupling a gain medium and a passive mode-locking device in a cavity;
amplifying signal electromagnetic radiation (signal) through stimulated emission in the gain medium, the signal comprising a signal wavelength; and
passively mode-locking the signal using the passive mode-locking device that provides an intensity-dependent transmission or reflection for the signal so as to enforce pulse formation in the laser, wherein the passive mode-locking device comprises:
a thin-film waveguide having a thickness on the order of the signal wavelength so as to confine and guide the signal along the thin-film waveguide,
a material comprising a second-order nonlinear susceptibility enabling at least one of second harmonic generation or optical parametric amplification of the signal along the waveguide, and
an output directional coupler providing different coupling ratios for the signal and a second harmonic of the signal (second harmonic), wherein operation of the mode-locking device leads to generation of pulses of the signal outputted from the mode-locked laser.