Abstract
Whispering Gallery Mode resonators made from optically nonlinear crystals have small mode volume and extremely high quality factor which makes them ideal for various nonlinear conversion process at low power, ultimately at single photon level.
Highlights
The ordinary and extraordinary thermorefractive coefficients in birefringent materials can significantly differ. This allows for the differential tuning of the TE and transverse magnetic filed (TM) whispering gallery modes (WGMs) spectra, a capability very important for some sensor applications [211, 212]10 and for achieving the phase matching in various nonlinear optics applications [213]
Analysis of nonlinear optical processes dynamics in phasematched WGM resonators has been reported for the second harmonic generation (SHG) [107, 213, 256, 317, 335] and optical parametric oscillator (OPO) [213, 253,254,255,256, 336], as well as for the sum-frequency generation (SFG) [320, 321, 337, 338] and difference-frequency generation (DFG) [339]
Generation of optical frequency sum [320] and difference [368] have been demonstrated. Some of these experiments [108, 110, 112, 158, 228, 255, 257, 318,319,320, 357, 360, 361, 366, 367] have been relying on the natural phase matching whereas Quasi-phase matching (QPM) with periodical domain inversion was harnessed in others [107, 157, 326, 363,364,365]
Summary
Light does not interact with light in everyday life. This interaction can only be induced by means of nonlinear physical systems and is only observable with strong enough electromagnetic fields. Methods involving optical fibers [1], plasmons [2], hollow-core photonic crystal fibers [3], as well as metameterials [4,5,6] allow reducing the light power requirement This reduction is still insufficient for many applications where it is desirable to achieve a strong nonlinear response with faint light, at a few- or single-photon level. Unlike other types of optical cavities, monolithic ones can be integrated on a chip and multiplexed, which makes them indispensable in creation of chipscale nonlinear optical devices able to generate optical harmonics, produce non-classical states of light, process quantum information and so on These resonators allow reducing the footprint of nonlinear optics experiments and moving them from the lab to industrial applications, and facilitate nonlinear interaction at the single-photon level, representing one of the major goals of optical science nowadays. In the rest of this section, we briefly review the history and distinctive properties of WGM resonators
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