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Thomas Dinter

Publications and source records attributed to Thomas Dinter.

2 recordsLinked to original sources

Anti-resonant reflecting acoustic rib waveguides for strong opto-acoustic interaction

Few known material systems can simultaneously guide optical and elastic fields through total internal reflection. This natural limit has restricted the realization of strong optoacoustic effects to highly-specialised and purpose-built platforms which employ either exotic materials, or complex waveguide designs. Here we apply the concept of Anti-Resonant Reflecting Acoustic Waveguides (ARRAWs) as a potential solution to this issue. ARRAWs confine the elastic field to a high-elastic-velocity core via the anti-resonances of a cladding layer of lower elastic velocity. We numerically study the appearance and dispersion of ARRAW-guided modes in a conventional silicon-on-insulator rib waveguide geometry. Applying the technique to the problem of efficient backwards Stimulated Brillouin Scattering (SBS), we predict that ARRAW guidance, in conjunction with conventional optical confinement, can produce Brillouin gains comparable to those of more exotic geometries.

physics.optics

Three-Dimensional and Selective Displacement Sensing of a Levitated Nanoparticle via Spatial Mode Decomposition

We propose and experimentally demonstrate a novel detection method that significantly improves the precision of real-time measurement of the three-dimensional displacement of a levitated dipolar scatterer. Our technique relies on spatial mode sorting of the light scattered by the levitated object, allowing us to selectively extract the position information of all translational degrees of freedom with minimal losses. To this end, we collect all the light back-scattered from a levitated nanoparticle using a parabolic mirror and couple it into a spatial mode sorter. We measure displacement sensitivities ($\sqrt{S_{\mathrm{imp}, x}}, \sqrt{S_{\mathrm{imp}, y}}, \sqrt{S_{\mathrm{imp}, z}}$) $=$ (1.7, 2.4, 1.0) $\times$ $10^{-14}$ m/$\sqrt{\mathrm{Hz}}$ below the zero-point motion ($x_{\mathrm{zpm}}, y_{\mathrm{zpm}}, z_{\mathrm{zpm}}$) $=$ (2.2, 2.4, 1.6) $\times$ $10^{-12}$ m of the levitated particle considered here. In the regime where environmental decoherence is not limited by gas collision we estimate that our method can reach measurement efficiencies of $(\eta_{^{\mathrm{tot}}}^{_{x}}, \eta_{^{\mathrm{tot}}}^{_{y}}, \eta_{^{\mathrm{tot}}}^{_{z}}) = (0.13, 0.18, 0.33) > 1/9$, which would enable the 3D motional quantum ground state of a levitated optomechanical system.

physics.optics