2018
DOI: 10.1103/physreva.98.032113
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Quantum-limited Euler angle measurements using anticoherent states

Abstract: Many protocols require precise rotation measurement. Here we present a general class of states that surpass the shot noise limit for measuring rotation around arbitrary axes. We then derive a quantum Cramér-Rao bound for simultaneously estimating all three parameters of a rotation (e.g., the Euler angles), and discuss states that achieve Heisenberg-limited sensitivities for all parameters; the bound is saturated by "anticoherent" states [Zimba, Electron. J. Theor. Phys. 3, 143 (2006)] (we are reluctant to use … Show more

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Cited by 51 publications
(53 citation statements)
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“…This problem involves estimating rotations about unknown axes. It has been shown in [13] that spin states with vanishing spin expectation value and isotropic variances of the spin components are valuable for estimating such rotations, as they saturate the quantum Cramér-Rao bound for any axis. Also, recently, the problem of characterizing a rotation about an unknown direction encoded into a spin-j state has been considered in [14].…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
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“…This problem involves estimating rotations about unknown axes. It has been shown in [13] that spin states with vanishing spin expectation value and isotropic variances of the spin components are valuable for estimating such rotations, as they saturate the quantum Cramér-Rao bound for any axis. Also, recently, the problem of characterizing a rotation about an unknown direction encoded into a spin-j state has been considered in [14].…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…For small rotation angles η, the average fidelity is minimized by anticoherent states, which are characterized by the fact that they do not manifest any privileged direction; in this respect, they are as distinct as possible from coherent states [17]. The role of anticoherent states for optimal detection of rotations has also been observed and was subsequently quantified in terms of quantum Fisher information in [13]. Between these two extreme cases of η ∼ 0 and η ∼ π, optimal states are neither coherent nor anticoherent in general.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
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“…To investigate this point it is advantageous to use the Majorana stellar representation [343], which allows us to uniquely depict a spin state state living in H by 2 points on the unit sphere [344]. Several decades after its conception, this representation has recently attracted a great deal of attention in several fields [345][346][347][348][349][350][351][352][353][354][355][356][357][358].…”
Section: Majorana Representationmentioning
confidence: 99%
“…However, this focus on the single-parameter case is neither necessary nor advisable. Recent suggestions advise adopting a multiple parameter approach [15,16], thus making quantumenhanced multiparameter estimation [17][18][19][20][21][22][23][24][25][26][27][28] an important component of the next quantum revolution.…”
Section: Introductionmentioning
confidence: 99%