-
Notifications
You must be signed in to change notification settings - Fork 3
Description
Motivation
Add the mixed-state entanglement separability decision problem, a central problem in quantum information and a canonical NP-hard weak-membership problem over a convex set.
Definition
Name: MixedEntanglementSeparability
Reference:
- Gurvits, L. (2003). Classical deterministic complexity of Edmonds' problem and Quantum Entanglement.
- Gharibian, S. (2009/2018). Strong NP-Hardness of the Quantum Separability Problem.
Let rho be a bipartite density matrix on C^M ⊗ C^N (rho >= 0, Tr(rho)=1).
rho is separable iff it can be written as:
rho = sum_t p_t (|a_t><a_t| ⊗ |b_t><b_t|),
where p_t >= 0, sum_t p_t = 1.
Because exact boundary membership is numerically ill-posed, we use the weak-membership promise version:
- YES:
rhois at leastbetainside the separable set - NO:
rhois at leastbetaoutside the separable set
(beta > 0; points within the margin are promise-gap inputs.)
Variables
- Count: decomposition-size dependent, continuous (not fixed finite discrete variables)
- Per-variable domain: real probabilities and complex amplitudes (or equivalent real Bloch coordinates)
- Meaning: candidate separable decomposition parameters
(p_t, a_t, b_t)or equivalent convex-combination coordinates - Constraint: PSD/trace constraints for
rho, and convex-combination constraints for decomposition
Schema (data type)
Type name: MixedEntanglementSeparability
Variants: subsystem dimensions (M, N) and real/complex representation
| Field | Type | Description |
|---|---|---|
rho |
Vec<Vec<Complex64>> (or split real/imag parts as two Vec<Vec<f64>>) |
Input density matrix on C^M ⊗ C^N |
dim_a |
usize |
Subsystem dimension M |
dim_b |
usize |
Subsystem dimension N |
beta |
f64 |
Weak-membership promise margin |
Complexity
- Best known exact algorithm: no known polynomial-time exact algorithm for general instances
- Complexity class: NP-hard (weak membership formulation), strongly NP-hard for inverse-polynomial margin
- References:
- Gurvits (2003): NP-hardness of weak membership near boundary with inverse-exponential margin (
beta <= 1/exp(M,N)) - Gharibian (2009/2018): strong NP-hardness with inverse-polynomial promise margin (
beta <= 1/poly(M,N))
- Gurvits (2003): NP-hardness of weak membership near boundary with inverse-exponential margin (
Extra Remark
- This problem is a geometric convex-membership problem over the separable set
S_{M,N}. - RSDF is an important intermediate source problem in hardness chains leading to this model.
- Practical solvers often rely on relaxations/certificates (e.g., PPT criterion, entanglement witnesses, SDP hierarchies), which are incomplete in general.
How to solve
- It can be solved by (existing) bruteforce.
- Other, refer to convex relaxation / SDP hierarchies / entanglement-witness methods.
Example Instance
Instance 1: Separable (YES)
M = N = 2
rho = 0.5 * (|00><00| + |11><11|)
This is explicitly separable as a convex combination of product pure states.
Instance 2: Entangled (NO, for sufficiently small beta)
M = N = 2
|Phi+> = (|00> + |11>) / sqrt(2)
rho = |Phi+><Phi+|
rho is a Bell state (entangled), hence not separable.
Note: these two examples are sanity-check instances. The NP-hard regime is reached for highly mixed states near the separable-set boundary (e.g., parameterized Werner/isotropic families or bound-entangled constructions).
Validation Method
- Cross-check small-dimensional cases with known criteria (PPT is necessary and sufficient for
2x2and2x3) - Compare with SDP-based outer/inner approximations of the separable set
- Verify known benchmark states (Bell, isotropic, Werner families) at parameter values with known separability thresholds