2017
DOI: 10.1103/physreva.96.022327
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Optimal quantum operations at zero energy cost

Abstract: Quantum technologies are developing powerful tools to generate and manipulate coherent superpositions of different energy levels. Envisaging a new generation of energy-efficient quantum devices, here we explore how coherence can be manipulated without exchanging energy with the surrounding environment. We start from the task of converting a coherent superposition of energy eigenstates into another. We identify the optimal energy-preserving operations, both in the deterministic and in the probabilistic scenario… Show more

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Cited by 22 publications
(13 citation statements)
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References 107 publications
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“…There are some very interesting related ideas in the literature: in [24], general quantum operations costing zero energy are studied. Also, the energy cost of creating entanglement in specific many-body systems was calculated in [25].…”
Section: Introductionmentioning
confidence: 99%
“…There are some very interesting related ideas in the literature: in [24], general quantum operations costing zero energy are studied. Also, the energy cost of creating entanglement in specific many-body systems was calculated in [25].…”
Section: Introductionmentioning
confidence: 99%
“…Our results can help to investigate phenomena such as catalytic transformations [36][37][38][39][40], and act as a starting point for the investigation of mixed state transformations, transformations in the asymptotic limit [28] or approximate transformations [41]. Akin to developments in coherence theory, we can also incorporate further physical restrictions [11] such as conservation of energy [42], or restrictions for distributed scenarios such as local superposition-free operations and classical communication [43][44][45][46]. As in coherence theory [28,44], there are also connections to entanglement theory [12,13] to be further understood.…”
mentioning
confidence: 99%
“…For a continuous time evolution of a closed system, energy conservation throughout the process requires [H(t), U ] = 0 ∀t [50], where H(t) = H 0 +V (t) and V (t) is the interaction Hamiltonian. The unitary evolution from time t 1 to t 2 can be given by a unitary U (t) of the form…”
Section: Theoremmentioning
confidence: 99%