States for phase estimation in quantum interferometry
arXiv:quant-ph/0412037 · doi:10.1088/1464-4266/7/1/004
Abstract
Ramsey interferometry allows the estimation of the phase of rotation of the pseudospin vector of an ensemble of two-state quantum systems. For small, the noise-to-signal ratio scales as the spin-squeezing parameter , with possible for an entangled ensemble. However states with minimum are not optimal for single-shot measurements of an arbitrary phase. We define a phase-squeezing parameter, , which is an appropriate figure-of-merit for this case. We show that (unlike the states that minimize ), the states that minimize can be created by evolving an unentangled state (coherent spin state) by the well-known 2-axis counter-twisting Hamiltonian. We analyse these and other states (for example the maximally entangled state, analogous to the optical "NOON" state ) using several different properties, including , , the coefficients in the pseudo angular momentum basis (in the three primary directions) and the angular Wigner function . Finally we discuss the experimental options for creating phase squeezed states and doing single-shot phase estimation.
8 pages and 5 figures
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- Maximum information gain in weak or continuous measurements of qudits: complementarity is not enough
- Speeding Up Squeezing with a Periodically Driven Dicke Model
- Phase Estimation with Non-Unitary Interferometers: Information as a Metric
- Quantum enhancement of N-photon phase sensitivity by interferometric addition of down-converted photon pairs to weak coherent light
- Optimal lossy quantum interferometry in phase space
- Dynamical generation of phase-squeezed states in a two-component Bose-Einstein condensates
- Spin coherence scale: operator-ordering sensitivity beyond the Heisenberg-Weyl group