What is the conjecture
This is problem #25 in Reinhard F. Werner’s collection, later collected by a community of quantum researchers.
Problem (Open Quantum Problem #25: “Lockable entanglement measures”).
Are two-way distillible entanglement and secret key rate lockable?
A standard formalization is in terms of single-qubit AB-locking (loss of one local qubit by Alice or Bob):
- Fix a bipartite state
ρ_AB, and consider an extension ρ_Aa:B (or ρ_A:Bb) where the extra subsystem a (or b) is a qubit, i.e. dim(a)=2 (or dim(b)=2).
- For any bipartite resource measure
E, compare the value of E before and after the qubit is lost:
E(ρ_Aa:B) versus E(Tr_a ρ_Aa:B).
E is lockable (more precisely, AB-lockable) iff the loss of a single local qubit can reduce E by an arbitrarily large amount, i.e. iff
sup_{ρ_Aa:B, dim(a)=2} [ E(ρ_Aa:B) - E(Tr_a ρ_Aa:B) ] = +∞,
and similarly with the extra qubit on Bob’s side.
Equivalent formulations sometimes replace “trace out the qubit” by “measure/dephase one local qubit”; the OQP wording is specifically about loss of a qubit.
The two operational quantities in the problem are:
D_↔(ρ_AB) (also written E_D^↔): the two-way distillable entanglement, i.e. the optimal asymptotic rate at which Alice and Bob can distill maximally entangled pairs from many copies of ρ_AB using LOCC with two-way classical communication.
K_D(ρ_AB): the distillable secret key / secret key rate, i.e. the optimal asymptotic rate at which Alice and Bob can distill secret bits (equivalently, private states / private bits) from many copies of ρ_AB, secure against an adversary holding a purification.
So the open problem can be stated as two concrete questions:
- Two-way distillable entanglement: do there exist states
ρ_Aa:B with dim(a)=2 for which
D_↔(ρ_Aa:B) - D_↔(Tr_a ρ_Aa:B)
is arbitrarily large?
- Secret key rate: do there exist states
ρ_Aa:B with dim(a)=2 for which
K_D(ρ_Aa:B) - K_D(Tr_a ρ_Aa:B)
is arbitrarily large?
Equivalently, if the answer is “no”, one would like a non-lockability theorem giving a universal upper bound (or at least an O(1) bound) on the loss of D_↔ and/or K_D caused by discarding one local qubit.
Known surrounding facts that make this a particularly natural formalization target:
- Many entanglement/correlation measures are known to be lockable under single-qubit loss, including entanglement of formation, entanglement cost, logarithmic negativity, one-way distillable entanglement, and squashed entanglement.
- By contrast, the relative entropy of entanglement is non-lockable: losing one qubit can reduce it by at most
2.
- For secret key there is an important distinction between:
- E-locking, where extra information is given to Eve, and
- AB-locking, where one of the honest parties loses a local qubit.
The OQP problem is about the second notion. In fact, later work showed that distillable key is not E-lockable, while the AB-lockability question remains the relevant open one.
Where to find the details / references
Primary sources:
Key related references:
- K. Horodecki, M. Horodecki, P. Horodecki, and J. Oppenheim, “Locking entanglement measures with a single qubit” (Phys. Rev. Lett. 94, 200501 (2005); arXiv: quant-ph/0404096)
(introduces the locking phenomenon for entanglement measures; proves lockability of E_F, E_C, logarithmic negativity, and one-way distillable entanglement; shows relative entropy of entanglement is non-lockable)
- M. Christandl and A. Winter, “Uncertainty, Monogamy, and Locking of Quantum Correlations” (IEEE Trans. Inf. Theory 51, 3159–3165 (2005); arXiv: quant-ph/0501090)
(shows squashed entanglement is lockable; also discusses the distinction between lockability questions for entanglement and key)
- C. H. Bennett, G. Brassard, S. Popescu, B. Schumacher, J. A. Smolin, and W. K. Wootters, “Purification of Noisy Entanglement and Faithful Teleportation via Noisy Channels” (Phys. Rev. Lett. 76, 722–725 (1996); arXiv: quant-ph/9511027)
(standard starting point for entanglement distillation / two-way distillable entanglement)
- I. Devetak and A. Winter, “Distillation of secret key and entanglement from quantum states” (Proc. R. Soc. A 461, 207–235 (2005); arXiv: quant-ph/0306078)
(standard operational reference for distillable entanglement / secret key rates in the one-way setting)
- K. Horodecki, M. Horodecki, P. Horodecki, and J. Oppenheim, “General paradigm for distilling classical key from quantum states” (IEEE Trans. Inf. Theory 55, 1898–1929 (2009); arXiv: quant-ph/0506189)
(standard reference for private states and the formalism of distillable key)
- M. Christandl, A. Ekert, M. Horodecki, P. Horodecki, J. Oppenheim, and R. Renner, “Unifying classical and quantum key distillation” (TCC 2007; arXiv: quant-ph/0608199)
(proves that distillable key is not E-lockable and explicitly leaves open whether it is AB-lockable)
- G. Gour, “How many ebits can be unlocked with one classical bit?” (Phys. Rev. A 75, 054301 (2007); arXiv: quant-ph/0703246)
(related “unlocking” viewpoint; gives bounds for pure-state ensembles and discusses the connection to distillable-entanglement lockability)
- K. Horodecki, M. Studziński, R. P. Kostecki, O. Sakarya, and D. Yang, “Upper bounds on the leakage of private data and an operational approach to Markovianity” (Phys. Rev. A 104, 052422 (2021); arXiv: 2107.10737)
(partial progress on the key side: proves non-lockability results for certain private-state classes, while the general K_D question remains open)
Prerequisites needed
- Finite-dimensional quantum mechanics: density matrices, purifications, tensor products, partial trace
- Entanglement theory: LOCC, maximally entangled states, entanglement distillation, one-way vs two-way classical communication
- Quantum cryptography / private states: distillable secret key, adversarial purification, public discussion / LOPC viewpoint
- Entropic quantities and continuity ideas: von Neumann entropy, mutual information, conditional mutual information
- (Helpful) Monogamy / no-cloning intuition, and basic examples of locking / data hiding
- ams-81 (Quantum theory)
- ams-94 (Information and communication theory)
- ams-47 (Operator theory)
- ams-15 (Linear and multilinear algebra; matrix theory)
Choose either option
What is the conjecture
This is problem #25 in Reinhard F. Werner’s collection, later collected by a community of quantum researchers.
A standard formalization is in terms of single-qubit AB-locking (loss of one local qubit by Alice or Bob):
ρ_AB, and consider an extensionρ_Aa:B(orρ_A:Bb) where the extra subsystema(orb) is a qubit, i.e.dim(a)=2(ordim(b)=2).E, compare the value ofEbefore and after the qubit is lost:E(ρ_Aa:B)versusE(Tr_a ρ_Aa:B).Eis lockable (more precisely, AB-lockable) iff the loss of a single local qubit can reduceEby an arbitrarily large amount, i.e. iffsup_{ρ_Aa:B, dim(a)=2} [ E(ρ_Aa:B) - E(Tr_a ρ_Aa:B) ] = +∞,and similarly with the extra qubit on Bob’s side.
Equivalent formulations sometimes replace “trace out the qubit” by “measure/dephase one local qubit”; the OQP wording is specifically about loss of a qubit.
The two operational quantities in the problem are:
D_↔(ρ_AB)(also writtenE_D^↔): the two-way distillable entanglement, i.e. the optimal asymptotic rate at which Alice and Bob can distill maximally entangled pairs from many copies ofρ_ABusing LOCC with two-way classical communication.K_D(ρ_AB): the distillable secret key / secret key rate, i.e. the optimal asymptotic rate at which Alice and Bob can distill secret bits (equivalently, private states / private bits) from many copies ofρ_AB, secure against an adversary holding a purification.So the open problem can be stated as two concrete questions:
ρ_Aa:Bwithdim(a)=2for whichD_↔(ρ_Aa:B) - D_↔(Tr_a ρ_Aa:B)is arbitrarily large?
ρ_Aa:Bwithdim(a)=2for whichK_D(ρ_Aa:B) - K_D(Tr_a ρ_Aa:B)is arbitrarily large?
Equivalently, if the answer is “no”, one would like a non-lockability theorem giving a universal upper bound (or at least an
O(1)bound) on the loss ofD_↔and/orK_Dcaused by discarding one local qubit.Known surrounding facts that make this a particularly natural formalization target:
2.The OQP problem is about the second notion. In fact, later work showed that distillable key is not E-lockable, while the AB-lockability question remains the relevant open one.
Where to find the details / references
Primary sources:
https://arxiv.org/abs/quant-ph/0504166
https://arxiv.org/pdf/quant-ph/0504166
Key related references:
(introduces the locking phenomenon for entanglement measures; proves lockability of
E_F,E_C, logarithmic negativity, and one-way distillable entanglement; shows relative entropy of entanglement is non-lockable)(shows squashed entanglement is lockable; also discusses the distinction between lockability questions for entanglement and key)
(standard starting point for entanglement distillation / two-way distillable entanglement)
(standard operational reference for distillable entanglement / secret key rates in the one-way setting)
(standard reference for private states and the formalism of distillable key)
(proves that distillable key is not E-lockable and explicitly leaves open whether it is AB-lockable)
(related “unlocking” viewpoint; gives bounds for pure-state ensembles and discusses the connection to distillable-entanglement lockability)
(partial progress on the key side: proves non-lockability results for certain private-state classes, while the general
K_Dquestion remains open)Prerequisites needed
AMS categories
Choose either option