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{{quote|coherence is basis dependent, so wherever we talk about coherence we must be clear which basis is presupposed.|{{xu16b}}}} | {{quote|coherence is basis dependent, so wherever we talk about coherence we must be clear which basis is presupposed.|{{xu16b}}}} | ||
The most important paper is by Baumgratz{{etal}}{{cite|baumgratz14a}} who study it in finite-dimensional Hilbert spaces, measuring coherence through the distance between the state and its closest incoherent state. The first work in that direction, however, is an unpublished [[arXiv]] preprint by [[Johan Aberg]] with a better terminology than "coherence" (namely, "superpositions").{{cite|aberg_arXiv06a}} Streltsov{{etal}}{{cite|streltsov15a}} used entanglement | The most important paper is by Baumgratz{{etal}}{{cite|baumgratz14a}} who study it in finite-dimensional Hilbert spaces, measuring coherence through the distance between the state and its closest incoherent state. The first work in that direction, however, is an unpublished [[arXiv]] preprint by [[Johan Aberg]] with a better terminology than "coherence" (namely, "superpositions").{{cite|aberg_arXiv06a}} Streltsov{{etal}}{{cite|streltsov15a}} used entanglement. | ||
[[Marc Aßmann]]{{etal}} brought those concepts within the problem of [[polariton condensation]].{{cite|luders21a}}{{cite|luders23a}}{{cite|luders23b}}{{cite|brune25a}} | |||
== A crime in terminology == | == A crime in terminology == | ||
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== Interesting papers == | == Interesting papers == | ||
* {{chitambar19a}} (review) | * {{chitambar19a}} (review) | ||
* {{baumgratz14a}} | * {{baumgratz14a}} | ||
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* {{streltsov18a}} links quantum coherence to purity. | * {{streltsov18a}} links quantum coherence to purity. | ||
* {{killoran16a}} | * {{killoran16a}} | ||
* {{hazra24a}} | |||
== Continuous variables == | == Continuous variables == | ||
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* {{tan17a}} | * {{tan17a}} | ||
* {{gianfelici21a}} | * {{gianfelici21a}} | ||
As a variation, or precursor, to that lies the problem of the phase of [[coherent states]]. Chief papers on that question include: | |||
* {{javanainen96a}} | |||
* {{molmer97a}} | |||
* {{molmer97b}} | |||
* {{molmer98a}} | |||
* {{nienhuis01a}} | |||
* {{bartlett06a}} | |||
* {{nha05a}} | |||
* {{noh08a}} | |||
* {{carmichael10a}} | |||
* {{milburn12a}} | |||
== References == | == References == | ||
<references /> | <references /> | ||
More accurately, the resource theory of quantum coherence, aims to describe the phenomenon of quantum superposition, and clarify its connections with other sui generis quantum effects such as (in the case of several particles) entanglement. It is a particular (but possibly the most illustrative, along with entanglement) case of quantum resource theory:
A quantum resource theory is based on two main ingredients, the free states and the free operations. [...] The free states — states which do not possess any resource and are cheap to prepare — are the incoherent states, that is, quantum states which are diagonal in a fixed reference basis.
coherence is basis dependent, so wherever we talk about coherence we must be clear which basis is presupposed.
The most important paper is by Baumgratz et al.[1] who study it in finite-dimensional Hilbert spaces, measuring coherence through the distance between the state and its closest incoherent state. The first work in that direction, however, is an unpublished arXiv preprint by Johan Aberg with a better terminology than "coherence" (namely, "superpositions").[2] Streltsov et al.[3] used entanglement.
Marc Aßmann et al. brought those concepts within the problem of polariton condensation.[4][5][6][7]
From Streltsov et al.[8]
From Wu et al.[9]
From Killoran et al.[10]
The original theory[1] was developped for finite-dimensional Hilbert spaces. There has been several attempts at extending it to infinite spaces:
As a variation, or precursor, to that lies the problem of the phase of coherent states. Chief papers on that question include: