Fig. 1: Experimental setup for measuring the speed of particles. | Nature

Fig. 1: Experimental setup for measuring the speed of particles.

From: Energy–speed relationship of quantum particles challenges Bohmian mechanics

Fig. 1

a, Schematic of the experimental setup. The microcavity consists of two planar mirrors, one of which is nanostructured, with an optically active dye in between. The optical medium can be non-resonantly pumped to induce a lasing process, generating microcavity photons at the point of pumping. A small amount of the light circulating in the microcavity is transmitted through the mirrors and can be imaged onto a camera. b, Height map and cross-sections (see colour coding) of the nanostructured mirror. The height profile of the nanostructured mirror effectively induces a potential energy landscape that confines and guides the photons in the transverse plane of the resonator. Specifically, the light is guided in a waveguiding potential from x = −900 μm to the end of the structure at x = 500 μm. In the first section, from x = −900 μm to x = −600 μm, a linear ramp potential is superimposed on the waveguide potential. By changing the position of the non-resonant optical pumping along the ramp with a spatial light modulator (SLM), we can set the initial potential energy of photons. At x = 0, a step potential of height V0 = (0.538 ± 0.003) meV is superimposed on the waveguide that runs from x = 0 μm to x = 500 μm. Apart from the main waveguide described above (red cross-section), an auxiliary waveguide (green cross-section) is introduced at the start of the step potential at x = 0. This effectively creates a double-well potential in the direction orthogonal to the waveguide axis (grey cross-section), with a coupling between the respective ground states of the wells of J0 = 2π(6.34 ± 0.01) GHz. c, Camera images showing the photon populations in the coupled waveguides for three distinct energy regimes associated with three different dynamics: population oscillations in the classically allowed regime \((\varDelta > {\hbar }{J}_{0})\), long-range non-oscillatory propagation \((|\varDelta |\le {\hbar }{J}_{0})\) and evanescent decay \((\varDelta < -{\hbar }{J}_{0})\). Scale bar, 50 μm (b, height); 100  μm (b, length).

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