Passive states as optimal inputs for single-jump lossy quantum channels

The passive states of a quantum system minimize the average energy among all the states with a given spectrum. We prove that passive states are the optimal inputs of single-jump lossy quantum channels. These channels arise from a weak interaction of the quantum system of interest with a large Markov...

Full description

Bibliographic Details
Main Authors: De Palma, Giacomo (Author), Mari, Andrea (Author), Lloyd, Seth (Contributor), Giovannetti, Vittorio (Author)
Other Authors: Massachusetts Institute of Technology. Department of Mechanical Engineering (Contributor), Massachusetts Institute of Technology. Research Laboratory of Electronics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2017-07-10T19:12:08Z.
Subjects:
Online Access:Get fulltext
LEADER 01849 am a22002173u 4500
001 110603
042 |a dc 
100 1 0 |a De Palma, Giacomo  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Mechanical Engineering  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Research Laboratory of Electronics  |e contributor 
100 1 0 |a Lloyd, Seth  |e contributor 
700 1 0 |a Mari, Andrea  |e author 
700 1 0 |a Lloyd, Seth  |e author 
700 1 0 |a Giovannetti, Vittorio  |e author 
245 0 0 |a Passive states as optimal inputs for single-jump lossy quantum channels 
260 |b American Physical Society,   |c 2017-07-10T19:12:08Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/110603 
520 |a The passive states of a quantum system minimize the average energy among all the states with a given spectrum. We prove that passive states are the optimal inputs of single-jump lossy quantum channels. These channels arise from a weak interaction of the quantum system of interest with a large Markovian bath in its ground state, such that the interaction Hamiltonian couples only consecutive energy eigenstates of the system. We prove that the output generated by any input state ρ majorizes the output generated by the passive input state ρ[subscript 0] with the same spectrum of ρ. Then, the output generated by ρ can be obtained applying a random unitary operation to the output generated by ρ[superscript 0]. This is an extension of De Palma et al. [IEEE Trans. Inf. Theory 62, 2895 (2016)], where the same result is proved for one-mode bosonic Gaussian channels. We also prove that for finite temperature this optimality property can fail already in a two-level system, where the best input is a coherent superposition of the two energy eigenstates. 
546 |a en 
655 7 |a Article 
773 |t Physical Review A