2017 IEEE International Symposium on Information Theory (ISIT) 2017
DOI: 10.1109/isit.2017.8006874
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Compression for quantum population coding

Abstract: Abstract-We study the compression of n quantum systems, each prepared in the same state belonging to a given parametric family of quantum states. For a family of states with f independent parameters, we devise an asymptotically faithful protocol that requires a hybrid memory of size (f /2) log n, including both quantum and classical bits. Our construction uses a quantum version of local asymptotic normality and, as an intermediate step, solves the problem of compressing displaced thermal states of n identicall… Show more

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Cited by 5 publications
(7 citation statements)
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“…The memory cost is (1/2) log n qubits in the leading order, with the same amount of ancillary classical bits if the purity of the clock state is undetermined. The cost matches the general statement in [15], which says that (1/2) logn (qu)bits are needed per degree of freedom. Compared to [15], the protocols here are constructed using a completely different approach from the protocols, tailor-made for qubit clock states: The second order term of its memory cost is O(log log n) in contrast to x log n (for any positive x) as in [15].…”
Section: Introductionsupporting
confidence: 76%
See 1 more Smart Citation
“…The memory cost is (1/2) log n qubits in the leading order, with the same amount of ancillary classical bits if the purity of the clock state is undetermined. The cost matches the general statement in [15], which says that (1/2) logn (qu)bits are needed per degree of freedom. Compared to [15], the protocols here are constructed using a completely different approach from the protocols, tailor-made for qubit clock states: The second order term of its memory cost is O(log log n) in contrast to x log n (for any positive x) as in [15].…”
Section: Introductionsupporting
confidence: 76%
“…The cost matches the general statement in [15], which says that (1/2) logn (qu)bits are needed per degree of freedom. Compared to [15], the protocols here are constructed using a completely different approach from the protocols, tailor-made for qubit clock states: The second order term of its memory cost is O(log log n) in contrast to x log n (for any positive x) as in [15]. The error of the protocols here also vanishes faster than that of the protocols in [15] as n grows large.…”
Section: Introductionsupporting
confidence: 76%
“…This task is very similar to the simulation task considered in this paper, except that the parameter t is now invisible. The counterpart of this task for states is the task of compressing multicopy states, recently studied both theoretically [53], [54], [55], [56], [46] and experimentally [57]. The task of channel compression is more involved since the input of the channel is not necessary in the many-copy form, and these compression protocols for states cannot be applied directly.…”
Section: Discussionmentioning
confidence: 99%
“…The calculations can be found in Appendix F. The quantum version of local asymptotic normality has been derived in several different forms [17,16,39] with applications in quantum statistics [40,12], benchmarks [41] and data compression [42]. Here we use the version of [17], which states that n identical copies of a qudit state can be locally approximated by a c-q Gaussian state in the large n limit.…”
Section: 1mentioning
confidence: 99%
“…(35) RLD quantum Fisher information at t 0 J t 0 Eq. (42) general method is illustrated through examples. The conclusions are drawn in Section 11.…”
Section: Introductionmentioning
confidence: 99%