2018
DOI: 10.1088/1367-2630/aab47f
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Quantum noise in bright soliton matterwave interferometry

Abstract: There has been considerable recent interest in matterwave interferometry with bright solitons in quantum gases with attractive interactions, for applications such as rotation sensing. We model the quantum dynamics of these systems and find that the attractive interactions required for the presence of bright solitons causes quantum phase-diffusion, which severely impairs the sensitivity. We propose a scheme that partially restores the sensitivity, but find that in the case of rotation sensing, it is still bette… Show more

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Cited by 28 publications
(18 citation statements)
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“…For many T = 0 non-equilibrium phenomena it is sufficient to treat this initial condition as a multimode coherent state that is sampled by seeding the initial mean-field condensate wavefunction with on average half an atom of vacuum noise per mode [48]. Zero temperature TW with this initial condition has successfully modelled BEC dynamics in regimes where nonclassical particle correlations become important [49][50][51][52][53][54][55][56][57][58]. For finite-temperature studies, the relevant c-field theory is the stochastic projected Gross-Pitaevskii equation (SPGPE), which describes interactions between degenerate modes of the quantum field with a static thermal reservoir [59].…”
Section: Classical Field Methodologymentioning
confidence: 99%
“…For many T = 0 non-equilibrium phenomena it is sufficient to treat this initial condition as a multimode coherent state that is sampled by seeding the initial mean-field condensate wavefunction with on average half an atom of vacuum noise per mode [48]. Zero temperature TW with this initial condition has successfully modelled BEC dynamics in regimes where nonclassical particle correlations become important [49][50][51][52][53][54][55][56][57][58]. For finite-temperature studies, the relevant c-field theory is the stochastic projected Gross-Pitaevskii equation (SPGPE), which describes interactions between degenerate modes of the quantum field with a static thermal reservoir [59].…”
Section: Classical Field Methodologymentioning
confidence: 99%
“…For many T = 0 non-equilibrium phenomena it is sufficient to treat this initial condition as a multimode coherent state that is sampled by seeding the initial mean-field condensate wavefunction with on average half an atom of vacuum noise per mode [47]. Zero temperature TW with this initial condition has successfully modelled BEC dynamics in regimes where nonclassical particle correlations become important [48][49][50][51][52][53][54][55][56][57]. For finite-temperature studies, the relevant c-field theory is the stochastic projected Gross-Pitaevskii equation (SPGPE), which describes interactions between degenerate modes of the quantum field with a static thermal reservoir [58].…”
Section: Classical Field Methodologymentioning
confidence: 99%
“…In this case, we have increased the interaction time for the read-out compared to the state preparation step. Moreover, We also include U 2 = U 1 , which may be applicable in the case when it is not easy to reverse the sign of the interaction constant χ, such as when one is working with bright-solitons [48], or enhanced nonlinear interactions due to state-dependent potentials [9]. Figure 4 shows F c as a function of detection noise for different choices of U 2 when χt 1 = 0.027 (when the metrological gain using the spin squeezing parameter is maximum) and 0.072 (when the QFI is maximum).…”
Section: Robustifying Entanglement Against Detection Noisementioning
confidence: 99%