2021
DOI: 10.1063/5.0053154
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Toward transformable photonics: Reversible deforming soft cavities, controlling their resonance split and directional emission

Abstract: We report on reversible and continuously deformable soft micro-resonators and the control of their resonance split and directional emission. Assisted by computerized holographic-tweezers, functioning as an optical deformer of our device, we gradually deform the shape and change the functionality of a droplet whispering-gallery cavity. For example, we continuously deform hexagonal cavities to rectangular ones and demonstrate switching to directionally emitting mode-of-operation, or splitting a resonant mode to … Show more

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Cited by 4 publications
(3 citation statements)
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“…Early work by Ashkin and Dziedzic ( 52 ) used radiation pressure from a focussed laser beam to deform an air-liquid interface, using the direction of the deflection (outward) to answer open questions about the momentum of photons in a dielectric. The malleability of liquid-liquid and liquid-air interfaces has also been leveraged in optofluidic devices such as adaptive lenses and “lab-on-chip” applications ( 53 ), as well as for fluidic optomechanical resonators ( 54 56 ), the generation of giant optical nonlinearities ( 57 ), and transformable optical cavities ( 30 )—which have been proposed to reach the single-photon nonlinear regime ( 31 ). With the thick ( d = 24 nm) film considered here, the van der Waals pressure PvdW=normalρnormalαvdwd3, which opposes surface deformation and plays the role of the Young’s modulus in a solid, is two billion times softer than the underlying silica sphere ( 40 ).…”
Section: Discussionmentioning
confidence: 99%
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“…Early work by Ashkin and Dziedzic ( 52 ) used radiation pressure from a focussed laser beam to deform an air-liquid interface, using the direction of the deflection (outward) to answer open questions about the momentum of photons in a dielectric. The malleability of liquid-liquid and liquid-air interfaces has also been leveraged in optofluidic devices such as adaptive lenses and “lab-on-chip” applications ( 53 ), as well as for fluidic optomechanical resonators ( 54 56 ), the generation of giant optical nonlinearities ( 57 ), and transformable optical cavities ( 30 )—which have been proposed to reach the single-photon nonlinear regime ( 31 ). With the thick ( d = 24 nm) film considered here, the van der Waals pressure PvdW=normalρnormalαvdwd3, which opposes surface deformation and plays the role of the Young’s modulus in a solid, is two billion times softer than the underlying silica sphere ( 40 ).…”
Section: Discussionmentioning
confidence: 99%
“…We note however that the fountain pressure per absorbed photon is of similar magnitude to the thermoelastic stress which would occur in a crystalline material (see the Supplementary Materials). It is thus primarily the engineered ability to collect the thermal energy and operate with near optimally time-delayed forcing, combined with the much higher compliance of liquids compared to solids (29)(30)(31) which is responsible for the ultralow threshold observed here and not a fundamentally stronger nature of the fountain pressure force in superfluid helium. This makes these results broadly applicable to photothermally and electrothermally driven systems and different fluids.…”
Section: Introductionmentioning
confidence: 92%
“…When the cavity size of lasers tends to be micrometers or even sub-micrometers, microcavity lasers have emerged, in which the compact internal environment will produce rich light-matter interactions [12][13][14]. By confining the complex disordered medium inside the microcavity, the output of the microcavity laser will exhibit a variety of complex characteristics as the disorder degree of the cavity boundary and the internal medium changes [15][16][17][18].…”
Section: Introductionmentioning
confidence: 99%