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Howard 1 , T. Weinhold 1 , F. Shahandeh 2 , J. Combes 1 , M. Vanner 3 , A. White 1 , and M. COVID has impacted many institutions and organizations around the world, disrupting the progress of research.
Through this difficult time APS and the Physical Review editorial office are fully equipped and actively working to support researchers by continuing to carry out all editorial and peer-review functions and publish research in the journals as well as minimizing disruption to journal access.
We appreciate your continued effort and commitment to helping advance science, and allowing us to publish the best physics journals in the world.
And we hope you, and your loved ones, are staying safe and healthy. Many researchers now find themselves working away from their institutions and, thus, may have trouble accessing the Physical Review journals.
To address this, we have been improving access via several different mechanisms. Petrie polygon orthographic projections of first four n cubes.
Red dots represent the projection of a single vertex onto a unique point in phase space, and orange dots the projection of two vertices onto the same point.
Density plots of the Wigner functions of the first four hypercube states. All axes are in terms of the ground state width.
The color bar on the bottom shows the value of the Wigner function where blue and green indicate areas of negative quasiprobability. Post these interactions, the optical fields in both arms are interfered, split into the polarization components, and detected in an avalanche photon detector APD.
Normalized probability densities of hypercube states; left to right columns correspond to second-, third- and fourth-order hypercube states.
Top row: Ideal densities, from Eq. Middle row: Densities predicted from a model that accounts for experimental drift, timing uncertainties, and counting statistics; see Supplemental Material [ 18 ].
Note the predicted variations in peak height, width, and shape. Bottom row: Measured probability densities, the Bhattacharyya coefficient a classical analogue of the fidelity between the middle row of density plots and the experimentally measured density plots are 0.
The uncertainties represent 1 standard deviation obtained from the statistical uncertainties in determining the values of X and P.
The signature of hypercube states in the thermal regime—the ring of outer-edge-vertices—is clearly visible in all plots. Learn about our response to COVID , including freely available research and expanded remote access support.
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