2018
DOI: 10.1088/1367-2630/aae738
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All phase-space linear bosonic channels are approximately Gaussian dilatable

Abstract: We compare two sets of multimode quantum channels acting on a finite collection of harmonic oscillators: (a) the set of linear bosonic channels, whose action is described as a linear transformation at the phase space level; and (b) Gaussian dilatable channels, that admit a Stinespring dilation involving a Gaussian unitary. Our main result is that the set (a) coincides with the closure of (b) with respect to the strong operator topology. We also present an example of a channel in (a) which is not in (b), implyi… Show more

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Cited by 18 publications
(13 citation statements)
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“…which implies that the sequence { D η, α √ 1−η } η∈[0,1) converges to D α in the strong sense [LSW18,Lemma 8].…”
Section: Appendix B: Convergence Of the Experimental Implementation Omentioning
confidence: 94%
See 1 more Smart Citation
“…which implies that the sequence { D η, α √ 1−η } η∈[0,1) converges to D α in the strong sense [LSW18,Lemma 8].…”
Section: Appendix B: Convergence Of the Experimental Implementation Omentioning
confidence: 94%
“…A connection between the notion of strong convergence and the notion of uniform convergence over energy-bounded states was established in [Shi18a]. Later, these different topologies of convergence were studied in the context of linear bosonic channels and Gaussian dilatable channels in [LSW18]. Furthermore, topologies of convergence in the context of teleportation simulation of physically relevant phaseinsensitive bosonic Gaussian channels have been investigated in [Wil18].…”
Section: (A10)mentioning
confidence: 99%
“…Let us consider for instance the case λ = 0. Since χ σ,0 achieves it maximum modulus at 0 (see [96,Proposition 14] and [97,Lemma 10]), if it is a Gaussian it must be centred, i.e. [44,Eq.…”
Section: E Relative Entropy Of Non-gaussianitymentioning
confidence: 99%
“…( 21) corresponds to a pure loss channel of parameter 1 N [43]. Varying the environment state one obtains instead a general attenuator [44][45][46][47][48][49]. The reduced map Λ j : D(A) → D(B j ) is given by Λ j = Tr B\B j • Λ and has the same form for all j, as shown in Appendix B.1.…”
Section: Testing Optimality Of the Objectivity Bound With An N-splittermentioning
confidence: 99%