What is the conjecture
This is problem #38 in the community-maintained Open Quantum Problems collection.
Problem (Open Quantum Problem #38: “The PPT-squared conjecture”).
Let ρ_AB and ρ_CD be quantum states with positive partial transpose (i.e. they are PPT states), and let M be a positive operator describing a yes/no measurement on the BC-system. Then consider the state on AD, conditional on the result of M being “yes”,
σ_AD = λ Tr_{BC}((ρ_AB ⊗ ρ_CD)(1_A ⊗ M ⊗ 1_D)),
where λ is a normalization factor.
The conjecture states that all such σ_AD are separable.
A standard formalization is as follows:
- Fix finite-dimensional Hilbert spaces
H_A, H_B, H_C, H_D.
ρ_AB and ρ_CD are density operators on H_A ⊗ H_B and H_C ⊗ H_D, respectively.
- A bipartite state
ω_XY is PPT iff its partial transpose is positive semidefinite:
(id_X ⊗ T_Y)(ω_XY) ≥ 0
(with respect to a fixed local basis on Y).
- A bipartite state
ω_XY is separable iff it can be written as a convex combination of product states:
ω_XY = ∑_i p_i (α_i ⊗ β_i),
where p_i ≥ 0, ∑_i p_i = 1, and α_i, β_i are local density operators.
- Let
M ≥ 0 be a positive operator / postselected effect on H_B ⊗ H_C with nonzero success probability
p = Tr[(ρ_AB ⊗ ρ_CD)(1_A ⊗ M ⊗ 1_D)] > 0.
Define the postselected entanglement-swapping output
σ_AD = p^{-1} Tr_{BC}[(ρ_AB ⊗ ρ_CD)(1_A ⊗ M ⊗ 1_D)].
Then the conjecture is:
- Main conjecture: whenever
ρ_AB and ρ_CD are PPT, the swapped state σ_AD is always separable across the bipartition A:D, for every positive operator M with nonzero success probability.
A standard equivalent reformulation is in terms of PPT maps and entanglement-breaking maps (via the Choi–Jamiołkowski correspondence):
- A completely positive map
Φ is PPT iff T ∘ Φ (equivalently Φ ∘ T) is completely positive, i.e. its Choi matrix is PPT.
- A completely positive map
Φ is entanglement breaking iff its Choi matrix is separable
(equivalently, in the trace-preserving case, iff (id ⊗ Φ)(τ) is separable for every bipartite state τ).
In that language, the conjecture can be written as:
- Equivalent map formulation: if
Φ and Ψ are PPT maps, then Ψ ∘ Φ is entanglement breaking.
The name “PPT-squared” comes from the especially natural special case Ψ = Φ, but the formulation commonly studied in the literature allows two a priori different PPT maps.
Known partial results / current open regime:
- The conjecture is known in several special cases (e.g. for maps on
M_2, for the n = 3 / two-qutrit case, for Gaussian channels, for all Choi-type maps, and in certain random/asymptotic regimes).
- The general finite-dimensional case remains open.
Where to find the details / references
Primary sources:
Key related references (from the OQP page and later core literature):
- K. Horodecki, M. Horodecki, P. Horodecki, and J. Oppenheim, “Secure key from bound entanglement” (Phys. Rev. Lett. 94, 160502 (2005); arXiv: quant-ph/0309110)
(motivation: PPT states can still carry secret key)
- S. Bäuml, M. Christandl, K. Horodecki, and A. Winter, “Limitations on quantum key repeaters” (Nature Communications 6, 6908 (2015); arXiv: 1402.5927)
(explains the repeater motivation behind the conjecture)
- M. Christandl and R. Ferrara, “Private states, quantum data hiding and the swapping of perfect secrecy” (Phys. Rev. Lett. 119, 220506 (2017); arXiv: 1609.04696)
(directly related entanglement-swapping / private-state background; cited on the OQP page)
- M. Kennedy, N. A. Manor, and V. I. Paulsen, “Compositions of PPT Maps” (Quantum Inf. Comput. 18, 472–480 (2018); arXiv: 1710.08475)
(records the state-vs-map formulation, proves asymptotic results, and discusses the 2×2 case)
- B. Collins, Z. Yin, and P. Zhong, “The PPT square conjecture holds generically for some classes of independent states” (J. Phys. A 51, 425301 (2018); arXiv: 1803.00143)
(random / asymptotic evidence)
- M. Christandl, A. Müller-Hermes, and M. M. Wolf, “When Do Composed Maps Become Entanglement Breaking?” (Ann. Henri Poincaré 20, 2295–2322 (2019); arXiv: 1807.01266)
(systematic treatment; proves important special cases including dimension 3 and Gaussian channels; gives equivalent conjectures)
- L. Chen, Y. Yang, and W.-S. Tang, “Positive-partial-transpose square conjecture for n = 3” (Phys. Rev. A 99, 012337 (2019); arXiv: 1807.03636)
(independent proof of the n = 3 / two-qutrit case; states that the case n ≥ 4 remains open)
- S. Singh and I. Nechita, “The PPT^2 conjecture holds for all Choi-type maps” (Ann. Henri Poincaré 23, 3311–3329 (2022); arXiv: 2011.03809)
(proves the conjecture for a large structured family of maps including Choi-type maps)
(If you want to include a brief “recent progress” pointer section, see also Sang-Jun Park, “k-Positivity and high-dimensional bound entanglement under symplectic group symmetry” (arXiv:2602.09860, 2026), which proves the conjecture for symplectic-covariant / conjugate-symplectic-covariant PPT maps. But the references above are already enough for writing the issue.)
Prerequisites needed
- Finite-dimensional quantum mechanics: density matrices, tensor products, partial trace, postselected measurements / POVM effects
- Separability vs entanglement; convex decompositions into product states
- Partial transpose and the PPT criterion
- Quantum channels / completely positive maps and the Choi–Jamiołkowski correspondence
- Linear algebra / matrix analysis: positive semidefinite operators, transpose, tensor products, traces
- (Optional) Positive maps, decomposable maps, entanglement-breaking maps, and Schmidt number methods
- ams-81 (Quantum theory)
- ams-15 (Linear and multilinear algebra; matrix theory)
- ams-47 (Operator theory)
- ams-94 (Information and communication theory)
Choose either option
What is the conjecture
This is problem #38 in the community-maintained Open Quantum Problems collection.
A standard formalization is as follows:
H_A, H_B, H_C, H_D.ρ_ABandρ_CDare density operators onH_A ⊗ H_BandH_C ⊗ H_D, respectively.ω_XYis PPT iff its partial transpose is positive semidefinite:(id_X ⊗ T_Y)(ω_XY) ≥ 0(with respect to a fixed local basis on
Y).ω_XYis separable iff it can be written as a convex combination of product states:ω_XY = ∑_i p_i (α_i ⊗ β_i),where
p_i ≥ 0,∑_i p_i = 1, andα_i, β_iare local density operators.M ≥ 0be a positive operator / postselected effect onH_B ⊗ H_Cwith nonzero success probabilityp = Tr[(ρ_AB ⊗ ρ_CD)(1_A ⊗ M ⊗ 1_D)] > 0.Define the postselected entanglement-swapping output
σ_AD = p^{-1} Tr_{BC}[(ρ_AB ⊗ ρ_CD)(1_A ⊗ M ⊗ 1_D)].Then the conjecture is:
ρ_ABandρ_CDare PPT, the swapped stateσ_ADis always separable across the bipartitionA:D, for every positive operatorMwith nonzero success probability.A standard equivalent reformulation is in terms of PPT maps and entanglement-breaking maps (via the Choi–Jamiołkowski correspondence):
Φis PPT iffT ∘ Φ(equivalentlyΦ ∘ T) is completely positive, i.e. its Choi matrix is PPT.Φis entanglement breaking iff its Choi matrix is separable(equivalently, in the trace-preserving case, iff
(id ⊗ Φ)(τ)is separable for every bipartite stateτ).In that language, the conjecture can be written as:
ΦandΨare PPT maps, thenΨ ∘ Φis entanglement breaking.The name “PPT-squared” comes from the especially natural special case
Ψ = Φ, but the formulation commonly studied in the literature allows two a priori different PPT maps.Known partial results / current open regime:
M_2, for then = 3/ two-qutrit case, for Gaussian channels, for all Choi-type maps, and in certain random/asymptotic regimes).Where to find the details / references
Primary sources:
https://www.birs.ca/workshops/2012/12w5084/report12w5084.pdf
Key related references (from the OQP page and later core literature):
(motivation: PPT states can still carry secret key)
(explains the repeater motivation behind the conjecture)
(directly related entanglement-swapping / private-state background; cited on the OQP page)
(records the state-vs-map formulation, proves asymptotic results, and discusses the
2×2case)(random / asymptotic evidence)
(systematic treatment; proves important special cases including dimension
3and Gaussian channels; gives equivalent conjectures)(independent proof of the
n = 3/ two-qutrit case; states that the casen ≥ 4remains open)(proves the conjecture for a large structured family of maps including Choi-type maps)
(If you want to include a brief “recent progress” pointer section, see also Sang-Jun Park, “
k-Positivity and high-dimensional bound entanglement under symplectic group symmetry” (arXiv:2602.09860, 2026), which proves the conjecture for symplectic-covariant / conjugate-symplectic-covariant PPT maps. But the references above are already enough for writing the issue.)Prerequisites needed
AMS categories
Choose either option