All-optically triggerable organic/inorganic photonic devices

Optical resonant cavities form the foundation for a wide range of integrated optical components. While a high performance laser requires a high quality factor (Q) cavity, other types of devices, like modulators, rely on the cavity resonant wavelength being tunable. Numerous mechanisms based on the thermo-optic and electro-optic effects have been leveraged to create switchable or tunable devices; however, these are very power hungry and/or require complex control machinery. In the present work, we graft an air-stable, optically triggerable functional group to the surface of an ultra-high-Q optical cavity. The Aazobenzene functional group switches from trans to cis upon exposure to blue light, and it can be thermally triggered to revert to the initial trans state. Using a single tapered optical fiber waveguide, blue and near-IR light can be coupled into the device simultaneously. When the blue light interacts with the Aazo group, the resonant wavelength blue shifts. Upon exposure to a CO2 laser, the resonant wavelength returns to its initial position. Several different aspects of the device operation were investigated, including the kinetics of the switching, the effect of switching via a resonant or non-resonant optical field, and sterics of the switching. Notably, by tuning the surface density of the Aazo groups using a multi-material surface chemistry, it is possible to control the magnitude of the shift.

[1]  Shun Fujii,et al.  Transition between Kerr comb and stimulated Raman comb in a silica whispering gallery mode microcavity , 2017, 1712.04601.

[2]  A. Matsko,et al.  Optical resonators with whispering-gallery modes-part I: basics , 2006, IEEE Journal of Selected Topics in Quantum Electronics.

[3]  A. Armani,et al.  Low threshold anti-Stokes Raman laser on-chip , 2019, Photonics Research.

[4]  A. Matsko,et al.  Kerr frequency comb generation in overmoded resonators. , 2012, Optics express.

[5]  M. Gorodetsky,et al.  Raman-Kerr frequency combs in microresonators with normal dispersion. , 2017, Optics express.

[6]  Andrea M. Armani,et al.  Bioconjugation Strategies for Microtoroidal Optical Resonators , 2010, Sensors.

[7]  Guilu Long,et al.  Optothermal control of the Raman gain enhanced ringing in microresonators , 2018, EPL (Europhysics Letters).

[8]  Y. Hao,et al.  Multiple-layer black phosphorus phototransistor with Si microdisk resonator based on whispering gallery modes. , 2019, Applied optics.

[9]  A. Leinse,et al.  High-Q tellurium-oxide-coated silicon nitride microring resonators. , 2019, Optics letters.

[10]  T. Carmon,et al.  Stimulated Brillouin Cavity Optomechanics in Liquid Droplets. , 2018, Physical review letters.

[11]  Alan E. Willner,et al.  Nonlinear conversion efficiency in Kerr frequency comb generation. , 2014, Optics letters.

[12]  K. Vahala,et al.  Ultralow-threshold Raman laser using a spherical dielectric microcavity , 2002, Nature.

[13]  Xinliang Zhang,et al.  Tunable Brillouin and Raman microlasers using hybrid microbottle resonators , 2019, Nanophotonics.

[14]  T. Carmon,et al.  Acoustic whispering-gallery modes in optomechanical shells , 2012 .

[15]  T. J. Kippenberg,et al.  Cavity optomechanics with ultrahigh-Q crystalline microresonators , 2009, 0911.1178.

[16]  Hailin Wang,et al.  Resolved-sideband and cryogenic cooling of an optomechanical resonator , 2009 .

[17]  A. Armani,et al.  All-optical reversible controls of integrated photonics by self-assembled azobenzene. , 2020, 2001.01114.

[18]  A. Universal relations for coupling of optical power between microresonators and dielectric waveguides , 2004 .

[19]  A. Matsko,et al.  Quartic dissipative solitons in optical Kerr cavities. , 2019, Optics letters.

[20]  Nan Yu,et al.  Spatiotemporal dynamics of Kerr-Raman optical frequency combs , 2015 .

[21]  T. J. Kippenberg,et al.  Ultra-high-Q toroid microcavity on a chip , 2003, Nature.

[22]  Lei Xu,et al.  Kerr parametric oscillations and frequency comb generation from dispersion compensated silica micro-bubble resonators. , 2013, Optics express.

[23]  Xiaoshun Jiang,et al.  Visible Kerr comb generation in a high-Q silica microdisk resonator with a large wedge angle , 2019, Photonics Research.

[24]  R. G. Pinnick,et al.  Lasing and stimulated Raman scattering in spherical liquid droplets: time, irradiance, and wavelength dependence. , 1990, Applied optics.

[25]  K. Vahala,et al.  Kerr-nonlinearity optical parametric oscillation in an ultrahigh-Q toroid microcavity. , 2004, Physical review letters.

[26]  A. Armani,et al.  Raman-Kerr frequency combs in Zr-doped silica hybrid microresonators. , 2018, Optics letters.

[27]  Raman laser from an optical resonator with a grafted single-molecule monolayer , 2019, 1911.07777.

[28]  S. Yegnanarayanan,et al.  Ultra-high Q planar silicon microdisk resonators for chip-scale silicon photonics. , 2007, Optics express.

[29]  Soheil Soltani,et al.  Low-threshold parametric oscillation in organically modified microcavities , 2018, Science Advances.

[30]  Andrea M Armani,et al.  Cascaded Raman microlaser in air and buffer. , 2012, Optics letters.

[31]  Jonathan M. Silver,et al.  Sub-milliwatt-level microresonator solitons with extended access range using an auxiliary laser , 2018, Optica.

[32]  Optically tunable microresonator using photoswitchable azobenzene monolayer , 2020, 2002.04644.

[33]  M. Gorodetsky,et al.  Ultimate Q of optical microsphere resonators. , 1996, Optics letters.

[34]  Marko Loncar,et al.  Monolithic lithium niobate photonic circuits for Kerr frequency comb generation and modulation , 2018, Nature Communications.

[35]  A. Matsko,et al.  Optical resonators with whispering-gallery modes-part II: applications , 2006, IEEE Journal of Selected Topics in Quantum Electronics.

[36]  H. Tang,et al.  Soliton microcomb generation at 2  μm in z-cut lithium niobate microring resonators. , 2019, Optics letters.

[37]  A. Matsko,et al.  Normal group-velocity dispersion Kerr frequency comb. , 2012, Optics letters.

[38]  Ashley J. Maker,et al.  Titanium-enhanced Raman microcavity laser. , 2014, Optics letters.

[39]  R. J. Weiblen,et al.  Bichromatic pumping in mid-infrared microresonator frequency combs with higher-order dispersion. , 2019, Optics express.

[40]  A. Armani,et al.  Stimulated Anti-Stokes Raman Emission Generated by Gold Nanorod Coated Optical Resonators , 2018, ACS Photonics.

[41]  S. C. Hill,et al.  Frequency splitting of degenerate spherical cavity modes: stimulated Raman scattering spectrum of deformed droplets. , 1991, Optics letters.

[42]  S. Bose,et al.  Enabling entanglement distillation via optomechanics , 2019, Physical Review A.

[43]  Soheil Soltani,et al.  On-chip asymmetric microcavity optomechanics. , 2016, Optics express.

[44]  Hyungwoo Choi,et al.  Emerging material systems for integrated optical Kerr frequency combs , 2020, Advances in Optics and Photonics.

[45]  G. Guo,et al.  Tunable Raman laser in a hollow bottle-like microresonator. , 2017, Optics express.

[46]  Thermo-optomechanical oscillations in high-Q ZBLAN microspheres , 2013, 2013 IEEE Photonics Conference.

[47]  A. Armani,et al.  Normal dispersion silicon oxynitride microresonator Kerr frequency combs , 2019, Applied Physics Letters.