Fetching the paper…
Reading the bibliography…
Even though entanglement is very vulnerable to interactions with the environment, it can be created by purely dissipative processes.
C. H. Bennett et al, Phys. Rev. Lett. 70, 1895 (1993)
1993
Earlier work this paper cites.
J. F. Poyatos, J. I. Cirac, and P. Zoller, Phys. Rev. Lett. 77
1996
Earlier work this paper cites.
C. H. Bennett et al. Phys. Rev. Lett. 76
1996
Earlier work this paper cites.
C. H. Bennett, D. P. DiVincenzo, J. A. Smolin, and W. K. Wootters, Phys. Rev. A 54
1996
Earlier work this paper cites.
C. H. Bennett, H. J. Bernstein, S. Popescu, and B. Schumacher, Phys. Rev. A 53
1996
Earlier work this paper cites.
Joseph Kerckhoff, Hendra I. Nurdin, Dmitri S. Pavlichin, Hideo Mabuchi, Phys. Rev. Lett. 105, 040502 (2010); J. P. Paz and W. H. Zurek, Proc. of the Royal Soc. of London. Series A 454, 355 (Jan. 1998)
1998
Earlier work this paper cites.
H.-J. Briegel, W. Dür, J. I. Cirac, and P. Zoller, Phys. Rev. Lett. 81
1998
Cited alongside, same era.
M. Żukowski, A. Zeillinger, M. A. Horne, and A. K. Ekert, Phys. Rev. Lett. 71
1998
Cited alongside, same era.
R. F. Werner, Phys. Rev. A 40
1999
Cited alongside, same era.
M. Horodecki, P. W. Shor, and M. B. Ruskai, Rev. Math. Phys. 15
2003
Cited alongside, same era.
J. Dehaene, M. Van den Nest, B. De Moor and F. Verstraete, Phys. Rev. A 67
2003
Cited alongside, same era.
2006
Cited alongside, same era.
S. Diehl et al. Nature Phys. 4
2008
Later among the works it cites.
F. Verstraete, M. M. Wolf, and J. I. Cirac, Nature Phys. 5
2009
Later among the works it cites.
H. Krauter et al. arXiv:1006.4344 (2010)
2010
Closest in time.
M. B. Plenio and S. F. Huelga, Phys. Rev. Lett. 88
2011
Closest in time.
F. Pastawski, L. Clemente, and J. I. Cirac, Phys. Rev. A 83
2011
Closest in time.
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…
LOCC channels are completely positive trace preserving maps that can be realized by means of Local Operations and Classical Communication
Cited in the paper.
We assume, that the time scales for classical communication Γ − 1 \Gamma^{-1} (see appendix) are sufficiently long such that retardation effects can be ignored
Cited in the paper.
Supplemental Material
Cited in the paper.
The variant of scheme I without communication is fundamentally different from scheme II, presented in Sec. 4 and cannot not be formulated in terms master equations of the form ρ ˙ ∝ ( T ( ρ ) − ρ ) \dot{\rho}\propto\left(T(\rho)-\rho\right) , where T ( ρ ) T(\rho) is a LOCC channel
Cited in the paper.
The slowest term converges as 𝒪 ( t 3 δ Γ 3 ( Γ + δ ) e − t ( Γ + δ ) ) \mathcal{O}\left(\frac{t^{3}\delta\Gamma^{3}}{(\Gamma+\delta)}e^{-t(\Gamma+\delta)}\right) . After an initial waiting time of the order of 1 δ \frac{1}{\delta} the steady state is reached up to an error of the order 𝒪 ( α − 2 e − α − 1 ) \mathcal{O}\left(\alpha^{-2}e^{-\alpha^{-1}}\right)
Cited in the paper.
It can be shown that this back-action has only a small effect on the steady state of the source system, and not accumulate if many source systems are coupled to 𝒯 {\cal T} . If the parameter δ \delta is small, the back-action can be bounded several source system can be combined as described above. The strict avoidance of a state depended back-action is enforced only for the sake of clarity
Cited in the paper.