Non-linear optical device
A non-linear optical device includes a frequency-conversion waveguide and first and second input waveguides. The longitudinal axes of the input waveguides are inclined to that of the frequency-conversion waveguide such a first transverse mode is excited in the latter at the input frequency in operation of the device. The frequency-conversion waveguide supports a second transverse mode at an output frequency of the device, such that the phase velocity of the second transverse mode at the output frequency is substantially equal to that of the first transverse mode at the input frequency, thus providing phase-matching by balancing the effects of chromatic and modal dispersion.
1. A non-linear optical device for converting optical radiation of a first frequency into optical radiation of a second frequency, the non-linear optical device comprising:
a first optical waveguide having a waveguide core comprising optically non-linear material,
the first optical waveguide supporting, at the first frequency, a first transverse mode that is excited by a first excitation source, and
the first optical waveguide supporting, at the second frequency, a second transverse mode so as to provide phase velocities of the first and second transverse modes at the first and second frequencies respectively, that are substantially equal; and
a second optical waveguide coupled to the first optical waveguide, the second optical waveguide supporting, at the first frequency, a fundamental mode that is excited by a second excitation source, wherein
the longitudinal axes of the first and second optical waveguides lie in the same plane and intersect at an angle that provides for fundamental mode radiation at the first frequency in the second optical waveguide to excite the first transverse mode supported by the first optical waveguide.
2. The non-linear optical device according to claim 1 , further comprising:
a third optical waveguide coupled to the first optical waveguide, the third optical waveguide supporting, at the first frequency, a fundamental mode that is excited by a third excitation source, wherein
the longitudinal axes of the first and third optical waveguides lie in the same plane and intersect at an angle that provides for fundamental mode radiation at the first frequency in the third optical waveguide to excite the first transverse mode supported by the first optical waveguide.
3. The non-linear optical device according to claim 2 , further comprising a multimode interference device arranged to divide input radiation at the first frequency into first and second output portions, wherein
the first and second portions are applied to the second and third optical waveguides, respectively, to excite the fundamental modes thereof.
4. The non-linear optical device according to claim 1 , wherein the device is arranged to provide parametric down-conversion of optical radiation of the first frequency.
5. The non-linear optical device according to claim 1 , wherein the device is arranged to provide optical parametric amplification.
6. A source of entangled photon pairs comprising the non-linear optical device according to claim 5 .
7. The non-linear optical device according to claim 1 , wherein the device is arranged to provide parametric up-conversion of optical radiation of the first frequency.
8. A source of entangled photon pairs comprising the non-linear optical device according to claim 7 .
9. The non-linear optical device according to claim 1 , wherein the device is arranged to provide second harmonic generation.
10. The non-linear optical device according to claim 1 , wherein the first optical waveguide is a semiconductor optical waveguide.
11. The non-linear optical device according to claim 10 , wherein the first optical waveguide has a GaAs or AlGaAs core and AlGaAs cladding layers.