TY - JOUR
T1 - Phase variance of squeezed vacuum states
AU - Bagan, E.
AU - Monras, A.
AU - Munoz-Tapia, R.
PY - 2008/10/31
Y1 - 2008/10/31
N2 - We consider the problem of estimating the phase of squeezed vacuum states within a Bayesian framework. We derive bounds on the average Holevo variance for an arbitrary number N of uncorrelated copies. We find that it scales with the mean photon number n, as dictated by the Heisenberg limit, i.e., as n-2, only for N>4. For N≤4 this fundamental scaling breaks down and it becomes n-N/2. Thus, a single squeezed vacuum state performs worse than a single coherent state with the same energy. We find the optimal splitting of a fixed given energy among various copies. We also compute the variance for repeated individual measurements (without classical communication or adaptivity) and find that the standard Heisenberg-limited scaling n-2 is recovered for large samples. © 2008 The American Physical Society.
AB - We consider the problem of estimating the phase of squeezed vacuum states within a Bayesian framework. We derive bounds on the average Holevo variance for an arbitrary number N of uncorrelated copies. We find that it scales with the mean photon number n, as dictated by the Heisenberg limit, i.e., as n-2, only for N>4. For N≤4 this fundamental scaling breaks down and it becomes n-N/2. Thus, a single squeezed vacuum state performs worse than a single coherent state with the same energy. We find the optimal splitting of a fixed given energy among various copies. We also compute the variance for repeated individual measurements (without classical communication or adaptivity) and find that the standard Heisenberg-limited scaling n-2 is recovered for large samples. © 2008 The American Physical Society.
UR - https://www.scopus.com/pages/publications/55749107289
U2 - 10.1103/PhysRevA.78.043829
DO - 10.1103/PhysRevA.78.043829
M3 - Article
SN - 1050-2947
VL - 78
JO - Physical Review A - Atomic, Molecular, and Optical Physics
JF - Physical Review A - Atomic, Molecular, and Optical Physics
M1 - 043829
ER -