2017
DOI: 10.1103/physreva.96.032316
|View full text |Cite
|
Sign up to set email alerts
|

Operational one-to-one mapping between coherence and entanglement measures

Abstract: We establish a general operational one-to-one mapping between coherence measures and entanglement measures: Any entanglement measure of bipartite pure states is the minimum of a suitable coherence measure over product bases. Any coherence measure of pure states, with extension to mixed states by convex roof, is the maximum entanglement generated by incoherent operations acting on the system and an incoherent ancilla. Remarkably, the generalized CNOT gate is the universal optimal incoherent operation. In this w… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

5
170
0

Year Published

2017
2017
2024
2024

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 145 publications
(175 citation statements)
references
References 81 publications
(243 reference statements)
5
170
0
Order By: Relevance
“…Alternatively, the form of the achievable region can be proven using results in [18][19][20]. We also note that for pure states the conversion problem has been completely solved for SIO [7] and IO [45].…”
Section: Summary Of Resultsmentioning
confidence: 98%
See 1 more Smart Citation
“…Alternatively, the form of the achievable region can be proven using results in [18][19][20]. We also note that for pure states the conversion problem has been completely solved for SIO [7] and IO [45].…”
Section: Summary Of Resultsmentioning
confidence: 98%
“…This extension has found several applications in remote quantum protocols, including the tasks of quantum state merging [42,43] and assisted coherence distillation [38,41], which has also been demonstrated experimentally very recently [44]. Coherence in multipartite systems has also been studied with respect to other types of nonclassicality such as entanglement [21,23,30,45] and quantum discord [46,47].…”
mentioning
confidence: 91%
“…Note that these two classes, incoherent operations and strictly incoherent operations, are distinct as sets of CPTP maps, although it is known that they induce the same possible state transformations of a given state into a target state for qubits [27] and for pure states in arbitrary dimension [28] (correcting the earlier erroneous proof of the claim by [19]; the SIO part of the pure state transformations is due to [17]). However, for the distillation of pure coherence at rate C r (ρ) [17], IO are needed and it remains unknown whether SIO can attain the same rate.…”
Section: Proposition 3 (Chitambar/hsieh [25])mentioning
confidence: 91%
“…It may still be the case that there is in general a difference between MIO-simulation cost and MIO-coherence generating capacity, but deciding this possibility is beyond the scope of the present investigation. We only note that Theorem 1 gives us a singleletter formula for the MIO-coherence generating capacity, namely C MIO gen (T ) = P r (T ) = sup ρ on A⊗C C r (T ⊗id)ρ −C r (ρ), (28) the complete relative entropy coherence power of T . The supremum is over all auxiliary systems C and mixed states ρ on A ⊗ C. Indeed, the upper bound of Eq.…”
Section: Discussionmentioning
confidence: 99%
“…However, for SIO and IO, while K GIO n is mainly responsible for coherence-destruction, the permutation operator P n and relabeling operator R n enable the transfers between different incoherent basis states. In fact, the above analysis implies the reason why GIO or SIO is equally powerful as other seemingly more powerful operations (such as IO or MIO) on many occasions, a phenomenon emerged in many recent relevant works [20,69,70].…”
Section: Observation 3 the Kraus Operators Of Sio And Io Can Be Obtamentioning
confidence: 96%