Generating a 4-photon Tetrahedron State: Towards Simultaneous Super-sensitivity to Non-commuting Rotations
It is often thought that the super-sensitivity of a quantum state to an observable comes at the cost of a decreased sensitivity to other non-commuting observables. For example, a squeezed state squeezed in position quadrature is super-sensitive to position displacements, but very insensitive to mome...
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Zusammenfassung: | It is often thought that the super-sensitivity of a quantum state to an
observable comes at the cost of a decreased sensitivity to other non-commuting
observables. For example, a squeezed state squeezed in position quadrature is
super-sensitive to position displacements, but very insensitive to momentum
displacements. This misconception was cleared with the introduction of the
compass state, a quantum state equally super-sensitive to displacements in
position and momentum. When looking at quantum states used to measure spin
rotations, N00N states are known to be more advantageous than classical methods
as long as they are aligned to the rotation axis. When considering the
estimation of a rotation with unknown direction and amplitude, a certain class
of states stands out with interesting properties. These states are equally
sensitive to rotations around any axis, are second-order unpolarized, and can
possess the rotational properties of platonic solids in particular dimensions.
Importantly, these states are optimal for simultaneously estimating the three
parameters describing a rotation. In the asymptotic limit, estimating all d
parameters describing a transformation simultaneously rather than sequentially
can lead to a reduction of the appropriately-weighted sum of the measured
parameters' variances by a factor of d. We report the experimental creation and
characterization of the lowest-dimensional such state, which we call the
"tetrahedron state" due to its tetrahedral symmetry. This tetrahedron state is
created in the symmetric subspace of four optical photons' polarization in a
single spatial and temporal mode, which behaves as a spin-2 particle. While
imperfections due to the hardware limit the performance of our method, we argue
that better technology can improve our method to the point of outperforming any
other existing strategy in per-photon comparisons. |
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DOI: | 10.48550/arxiv.2310.17150 |