Monogamy of non- signalling correlations Aram Harrow (MIT) Simons Institute, 27 Feb 2014 based on joint work with Fernando Brandão (UCL) arXiv:1210.6367.

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Presentation transcript:

monogamy of non- signalling correlations Aram Harrow (MIT) Simons Institute, 27 Feb 2014 based on joint work with Fernando Brandão (UCL) arXiv: εunpublished

“correlations” (multipartite conditional probability distributions) localp(x,y|a,b) = q A (x|a) q B (y|b) LHV (local hidden variable)p(x,y|a,b) = ∑ r π(r) q A (x|a,r) q B (y|b,r) quantum p(x,y|a,b) = hÃ| A a x ⊗ B b y |Ãi with ∑ x A a x = ∑ y B b y = I non-signalling∑ y p(x,y|a,b) = ∑ y p(x,y|a,b’) ∑ x p(x,y|a,b) = ∑ x p(x,y|a’,b) a x b y

why study boxes? Foundational: considering theories more general than quantum mechanics (e.g. Bell’s Theorem) Operational: behavior of quantum states under local measurement (e.g. this work) Computational: corresponds to constraint-satisfaction problems and multi-prover proof systems.

why non-signalling? Foundational: minimal assumption for plausible theory Operational: yields well-defined “partial trace” p(x|a) := ∑ y p(x,y|a,b) for any choice of b Computational: yields efficient linear program

the dual picture: games Complexity: classical (local or LHV) value is NP-hard quantum value has unknown complexity non-signalling value in P due to linear programming Non-local games: Inputs chosen according to µ(a,b) Payoff function is V(x,y|a,b) The value of a game using strategy p is ∑ x,y,a,b p(x,y|a,b) µ(a,b) V(x,y|a,b).

monogamy LHV correlations can be infinitely shared. This is an alternate definition. Applications 1.Non-shareability  secrecy can be certified by Bell tests 2.Gives a hierarchy of approximations for LHV correlations running in time poly(|X| |Y| k |A| |B| k ) 3.de Finetti theorems (i.e. k-extendable states ≈ separable) p(x,y|a,b) is k-extendable if there exists a NS box q(x,y 1,…,y k |a,b 1,…,b k ) with q(x,y i |a,b i ) = p(x,y i |a,b i ) for each i

results Theorem 1: If p is k-extendable and µ is a distribution on A, then there exists q ∈ LHV such that Theorem 2: If p(x 1,…,x k |a 1,…,a k ) is symmetric, 0<n<k, and µ = µ 1 ⊗ … ⊗ µ k then ∃ νsuch that cf. Christandl-Toner with q independent of µ cf. Terhal-Doherty-Schwab quant-ph/ If k≥|B| then p ∈ LHV.

proof idea of thm 1 consider extension p(x,y 1,…,y k |a,b 1,…,b k ) case 1 p(x,y 1 |a,b 1 ) ≈ p(x|a) ⋅ p(y 1 |b 1 ) case 2 p(x,y 2 |y 1,a,b 1,b 2 ) has less mutual information

proof sketch of thm 1 ∴ for some j we have Y 1, …, Y j-1 constitute a “hidden variable” which we can condition on to leave X,Y j nearly decoupled. Trace norm bound follows from Pinsker’s inequality.

what about the inputs? Apply Pinsker here to show that this is & || p(X,Y k | A,b k ) – LHV || 1 2 then repeat for Y k-1, …, Y 1

interlude: Nash equilibria Non-cooperative games: Players choose strategies p A ∈ Δ m, p B ∈ Δ n. Receive values V A, p A ⊗ p B and V B, p A ⊗ p B. Nash equilibrium: neither player can improve own value ε-approximate Nash: cannot improve value by > ε Correlated equilibria: Players follow joint strategy p AB ∈ Δ mn. Receive values V A, p AB and V B, p AB. Cannot improve value by unilateral change. Can find in poly(m,n) time with linear programming (LP). Nash equilibrium = correlated equilibrum with p = p A ⊗ p B

finding (approximate) Nash eq Known complexity: Finding exact Nash eq. is PPAD complete. Optimizing over exact Nash eq is NP-complete. Algorithm for ε-approx Nash in time exp(log(m)log(n)/ε 2 ) based on enumerating over nets for Δ m, Δ n. Planted clique reduces to optimizing over ε-approx Nash. New result: Another algorithm for finding ε-approximate Nash with the same run-time. (uses k-extendable distributions)

algorithm for approx Nash Search over such that the A:B i marginal is a correlated equilibrium conditioned on any values for B 1, …, B i-1. LP, so runs in time poly(mn k ) Claim: Most conditional distributions are ≈ product. Proof: i I(A:B i |B <i ) ≤ log(m)/k. ∴ k = log(m)/ε 2 suffices.

application: free games free games: µ = µ A ⊗ µ B Corollary: From known hardness results for free games, implies that estimating the value of entangled games with √n players and answer alphabets of size exp(√n) is at least as hard as 3-SAT instances of length n. Corollary: The classical value of a free game can be approximated by optimizing over k-extendable non-signaling strategies. run-time is polynomial in (independently proved by Aaronson, Impagliazzo, Moshkovitz)

application: de Finetti theorems for local measurements Theorem 1’: If ρ AB is k-extendable and µ is a distribution over quantum operations mapping A to A’, then there exists a separable state σ such that Theorem 2’: If ρ is a symmetric state on A 1 …A k then there exists a measure ν on single-particle states such that improvements on Brandão-Christandl-Yard ) A’ dependence. 2) multipartite. 3) explicit. 4) simpler proof

ε-nets vs. info theory Problemε-netsinfo theory approx Nash max p ∈ Δ p T Ap LMM ‘03H. ‘14 free gamesAIM ‘14Brandão-H ‘13 max ρ ∈ Sep tr[Mρ] QMA(2) Shi-Wu ‘11 Brandão ‘14 BCY ‘10 Brandão-H ’12 BKS ‘13

general games? Theorem 1: If p is k-extendable and µ is a distribution on A, then there exists q ∈ LHV such that Can we remove the dependence of q on µ? Conjecture?: p ∈ k-ext  ∃ q ∈ LHV such that would imply that non-signalling games (in P) can be used to approximate the classical value of games (NP-hard) (probably) FALSE

general quantum games Conjecture: If ρ AB is k-extendable, then there exists a separable state σ such that Would yield alternate proofs of recent results of Vidick: NP-hardness of entangled quantum games with 4 playersNP-hardness of entangled quantum games with 4 players NEXP ⊆ MIP *NEXP ⊆ MIP * Proof would require strategies that work for quantum states but not general non-signalling distributions.

application: BellQMA(m) 3-SAT on n variables is believed to require a proof of size Ω(n) bits or qubits according to the ETH (Exp. Time Hypothesis) Chen-Drucker (building on Aaronson et al ) gave a 3-SAT proof using m = n 1/2 polylog(n) states each with O(log(n)) qubits (promised to be not entangled with each other). Verifier uses local measurements and classical post-processing. Our Theorem 2’ can simulate this with a m 2 log(n)-qubit proof. Implies m ≥ (n/log(n)) 1/2 or else ETH is false.

other applications tomography Can do “pretty good tomography” on symmetric states instead of on product states. polynomial optimization using SDP hierarchies Can optimize certain polynomials over n-dim hypersphere using O(log n) rounds. Suggests route to algorithms for unique games and small- set expansion. multi-partite separability testing can efficiently estimate 1-LOCC distance to Sep

open questions 1.Switch quantifiers and find a separable approximation (a) independent of the distribution on measurements (b) with error depending on the size of the output. 2.We know the non-signalling version of this is false. Can we find a simple counter-example? 3.Can one proof of size O(m 2 ) simulate two proofs of size m? i.e. is QMA = QMA(2)? 4.Better de Finetti theorems, perhaps combining with the exponential de Finetti theorems or the post-selection principle. 5. Unify ε-nets and information theory approaches.