dc.contributor.author | Lostaglio, Matteo | |
dc.contributor.author | Alhambra, Alvaro M. | |
dc.contributor.author | Perry, Christopher | |
dc.date.accessioned | 2018-05-11T09:29:22Z | |
dc.date.available | 2018-05-11T09:29:22Z | |
dc.date.issued | 2018-02 | |
dc.identifier.citation | Quantum 2, 52 (2018) | en_US |
dc.identifier.issn | 2521-327X | |
dc.identifier.uri | doi.org/10.22331/q-2018-02-08-52 | |
dc.identifier.uri | http://hdl.handle.net/123456789/1314 | |
dc.description.abstract | To what extent do thermodynamic resource
theories capture physically relevant constraints?
Inspired by quantum computation, we define
a set of elementary thermodynamic gates that
only act on 2 energy levels of a system at a
time. We show that this theory is well reproduced
by a Jaynes-Cummings interaction in
rotating wave approximation and draw a connection
to standard descriptions of thermalisation.
We then prove that elementary thermal
operations present tighter constraints on the allowed
transformations than thermal operations.
Mathematically, this illustrates the failure at finite
temperature of fundamental theorems by
Birkhoff and Muirhead-Hardy-Littlewood-Polya
concerning stochastic maps. Physically, this implies
that stronger constraints than those imposed
by single-shot quantities can be given if we
tailor a thermodynamic resource theory to the
relevant experimental scenario. We provide new
tools to do so, including necessary and sufficient
conditions for a given change of the population
to be possible. As an example, we describe the
resource theory of the Jaynes-Cummings model.
Finally, we initiate an investigation into how our
resource theories can be applied to Heat Bath
Algorithmic Cooling protocols | en_US |
dc.language.iso | en | en_US |
dc.relation.ispartofseries | 2018-02-08, volume 2, page 52; | |
dc.subject | Thermal | en_US |
dc.subject | Quantum | en_US |
dc.title | Elementary Thermal Operations | en_US |
dc.type | Article | en_US |