What is the conjecture
This is problem #30 in Reinhard F. Werner's open-problems collection, later maintained by a community of quantum researchers.
Status: this problem is listed as solved on the Solved Quantum Problems page (solved negatively by Haagerup–Musat; first in 2011, with a stronger follow-up in 2015; see below).
Problem (Open Quantum Problem #30: “Asymptotic Version of Birkhoff's Theorem”).
A classical theorem of Birkhoff says that every doubly stochastic matrix is a convex combination of permutation matrices.
In the quantum setting, doubly stochastic matrices become doubly stochastic quantum channels, i.e. completely positive maps preserving both the trace and the identity. The direct quantum analogue is false, but perhaps it becomes true asymptotically under tensor powers.
Decide whether for every doubly stochastic quantum channel T, the tensor powers T^{⊗ n} become arbitrarily well approximable by convex combinations of unitarily implemented channels.
Concretely, let T : M_d(C) → M_d(C) be a doubly stochastic quantum channel, i.e. a completely positive, trace-preserving, and unital map. Let
Aut(M_d(C)) = { ad_U : x ↦ U x U^* | U ∈ U(d) }
be the unitarily implemented channels, and for a set A of channels write
d_cb(T, A) := inf_{R ∈ A} ||T - R||_cb.
The Birkhoff defect of T is then
d_B(T) := d_cb(T, conv(Aut(M_d(C)))),
the cb-norm distance from T to the convex hull of unitary channels.
The asymptotic quantum Birkhoff conjecture asks whether
d_B(T^{⊗ n}) → 0 as n → ∞
for every doubly stochastic channel T. Equivalently: can every doubly stochastic quantum channel become arbitrarily close, after taking enough tensor powers, to a convex combination of unitary conjugations on the large tensor-product system?
The OQP page also records a weaker Jamiołkowski-dualized variant: if a bipartite state on equal-dimensional systems has maximally mixed marginals, must large tensor powers of that state be approximable in trace norm by convex combinations of maximally entangled pure states?
Solved statement to formalize (Haagerup–Musat, 2011; strengthened in 2015):
The asymptotic quantum Birkhoff conjecture is false.
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In Commun. Math. Phys. 303 (2011), Haagerup–Musat proved that for every n ≥ 3 there exist τ_n-Markov maps on M_n(C) (equivalently, doubly stochastic / UCPT channels) that do not satisfy the asymptotic quantum Birkhoff property. In fact, any non-factorizable τ_n-Markov map T : M_n(C) → M_n(C) is a counterexample. Writing FM(M_n(C)) for the set of factorizable maps, they show
d_cb(T^{⊗ k}, FM(M_n(C)^{⊗ k})) ≥ d_cb(T, FM(M_n(C))) for all k ≥ 1.
Since conv(Aut(M_n(C)^{⊗ k})) ⊂ FM(M_n(C)^{⊗ k}), a non-factorizable channel can never become asymptotically mixed-unitary.
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In Commun. Math. Phys. 338 (2015), Haagerup–Musat strengthened the picture by giving even a factorizable counterexample: a factorizable UCPT Schur multiplier T_B on M_6(C) with T_B ∉ conv(Aut(M_6(C))), and hence T_B^{⊗ r} ∉ conv(Aut(M_{6^r}(C))) for every r ≥ 2. More generally, for UCPT Schur multipliers T : M_n(C) → M_n(C) and S : M_k(C) → M_k(C),
d_cb(T ⊗ S, conv(Aut(M_{nk}(C)))) ≥ (1/2) d_cb(T, conv(Aut(M_n(C)))).
So tensoring does not wash out the Birkhoff defect for these examples.
This means that the natural quantum analogue of Birkhoff's theorem fails not only exactly, but even asymptotically.
Where to find the details / references
Primary sources:
Key solution references (as cited on the OQP page):
- U. Haagerup and M. Musat, “Factorization and dilation problems for completely positive maps on von Neumann algebras”, Commun. Math. Phys. 303, 555–594 (2011); arXiv: 1009.0778
- U. Haagerup and M. Musat, “An asymptotic property of factorizable completely positive maps and the Connes embedding problem”, Commun. Math. Phys. 338, 721–752 (2015); arXiv: 1408.6476
Related / background references mentioned on the OQP page (useful for a formalization roadmap):
- L. J. Landau and R. F. Streater, “On Birkhoff’s theorem for doubly stochastic completely positive maps of matrix algebras”, Linear Algebra Appl. 193, 107–127 (1993)
- M. Gregoratti and R. F. Werner, “Quantum Lost and Found”, J. Mod. Opt. 50, 915–933 (2003); arXiv: quant-ph/0209025
- A. Winter, “On environment-assisted capacities of quantum channels”, arXiv: quant-ph/0507045
- J. A. Smolin, F. Verstraete, and A. Winter, “Entanglement of assistance and multipartite state distillation”, Phys. Rev. A 72, 052317 (2005); arXiv: quant-ph/0505038
Prerequisites needed
- Finite-dimensional matrix algebras
M_n(C); completely positive maps; trace-preserving and unital channels (UCPT / doubly stochastic channels)
- Completely bounded norm / cb-distance; convex hulls; tensor products and tensor powers of channels
- Unitarily implemented channels
ad_U; mixed-unitary channels; Choi/Jamiołkowski correspondence
- Factorizable maps / exact factorizations through
M_n(C) ⊗ N for a finite tracial von Neumann algebra
- Depending on the route one formalizes:
- the 2011 route uses non-factorizable maps and operator-algebraic arguments,
- the 2015 route uses Schur multipliers and an explicit lower bound preventing asymptotic mixed-unitarity
- ams-81 (Quantum theory)
- ams-46 (Functional analysis)
- ams-47 (Operator theory)
Choose either option
What is the conjecture
This is problem #30 in Reinhard F. Werner's open-problems collection, later maintained by a community of quantum researchers.
Status: this problem is listed as solved on the Solved Quantum Problems page (solved negatively by Haagerup–Musat; first in 2011, with a stronger follow-up in 2015; see below).
Concretely, let
T : M_d(C) → M_d(C)be a doubly stochastic quantum channel, i.e. a completely positive, trace-preserving, and unital map. LetAut(M_d(C)) = { ad_U : x ↦ U x U^* | U ∈ U(d) }be the unitarily implemented channels, and for a set
Aof channels writed_cb(T, A) := inf_{R ∈ A} ||T - R||_cb.The Birkhoff defect of
Tis thend_B(T) := d_cb(T, conv(Aut(M_d(C)))),the cb-norm distance from
Tto the convex hull of unitary channels.The asymptotic quantum Birkhoff conjecture asks whether
d_B(T^{⊗ n}) → 0asn → ∞for every doubly stochastic channel
T. Equivalently: can every doubly stochastic quantum channel become arbitrarily close, after taking enough tensor powers, to a convex combination of unitary conjugations on the large tensor-product system?The OQP page also records a weaker Jamiołkowski-dualized variant: if a bipartite state on equal-dimensional systems has maximally mixed marginals, must large tensor powers of that state be approximable in trace norm by convex combinations of maximally entangled pure states?
Solved statement to formalize (Haagerup–Musat, 2011; strengthened in 2015):
The asymptotic quantum Birkhoff conjecture is false.
In
Commun. Math. Phys. 303 (2011), Haagerup–Musat proved that for everyn ≥ 3there existτ_n-Markov maps onM_n(C)(equivalently, doubly stochastic / UCPT channels) that do not satisfy the asymptotic quantum Birkhoff property. In fact, any non-factorizableτ_n-Markov mapT : M_n(C) → M_n(C)is a counterexample. WritingFM(M_n(C))for the set of factorizable maps, they showd_cb(T^{⊗ k}, FM(M_n(C)^{⊗ k})) ≥ d_cb(T, FM(M_n(C)))for allk ≥ 1.Since
conv(Aut(M_n(C)^{⊗ k})) ⊂ FM(M_n(C)^{⊗ k}), a non-factorizable channel can never become asymptotically mixed-unitary.In
Commun. Math. Phys. 338 (2015), Haagerup–Musat strengthened the picture by giving even a factorizable counterexample: a factorizable UCPT Schur multiplierT_BonM_6(C)withT_B ∉ conv(Aut(M_6(C))), and henceT_B^{⊗ r} ∉ conv(Aut(M_{6^r}(C)))for everyr ≥ 2. More generally, for UCPT Schur multipliersT : M_n(C) → M_n(C)andS : M_k(C) → M_k(C),d_cb(T ⊗ S, conv(Aut(M_{nk}(C)))) ≥ (1/2) d_cb(T, conv(Aut(M_n(C)))).So tensoring does not wash out the Birkhoff defect for these examples.
This means that the natural quantum analogue of Birkhoff's theorem fails not only exactly, but even asymptotically.
Where to find the details / references
Primary sources:
Key solution references (as cited on the OQP page):
Related / background references mentioned on the OQP page (useful for a formalization roadmap):
Prerequisites needed
M_n(C); completely positive maps; trace-preserving and unital channels (UCPT/ doubly stochastic channels)ad_U; mixed-unitary channels; Choi/Jamiołkowski correspondenceM_n(C) ⊗ Nfor a finite tracial von Neumann algebraAMS categories
Choose either option