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2-out-of-n CHSH Game: Generalized Nonlocality

Updated 12 July 2026
  • 2-out-of-n CHSH game is a generalization of the classic CHSH game where a pair is chosen from n indices to perform a CHSH-type XOR test.
  • The optimal quantum strategy achieves a bias of 1/√2 with winning probability 1/2 + 1/(2√2), characterized by Clifford-algebra structures and pairwise anti-commutation relations.
  • Variants include graph-based, multiplayer, parallel, sequential, and iterated settings, each highlighting distinct combinatorial and algebraic aspects in nonlocality tests.

The expression “2-out-of-nn CHSH game” does not denote a single universally standardized object in the arXiv literature. In the most explicit usage represented here, it refers to the family denoted CHSH(n)\mathrm{CHSH}(n), in which the referee first chooses a pair of distinct indices i<ji<j out of {1,…,n}\{1,\dots,n\} and then asks questions derived from that chosen pair; in that precise sense, CHSH(n)\mathrm{CHSH}(n) is a “choose 2 out of nn” CHSH-type XOR game (Ostrev, 2015). Other papers use closely related but inequivalent constructions, including graph-based pair-selection CHSH extensions (Cui et al., 2024), the nn-player binary-output instance of CHSHn-d\mathrm{CHSH}_n\text{-}d (Murta et al., 2015), parallel or sequential repetitions of ordinary CHSH (Coladangelo, 2016, Reichardt et al., 2012), and the iterated CHSH game arising from entanglement swapping on a repeater chain (Dmello et al., 2024). The topic is therefore best understood as a family of non-equivalent CHSH generalizations whose common feature is the embedding of ordinary CHSH structure into a larger nn-indexed setting.

1. Terminological scope and competing formalizations

The literature distinguishes several objects that are easy to conflate. One is the explicit “choose-2-from-nn” XOR game CHSH(n)\mathrm{CHSH}(n)0, where two indices are selected from CHSH(n)\mathrm{CHSH}(n)1 and the resulting pair defines a CHSH-type test (Ostrev, 2015). A second is the graph-based extension CHSH(n)\mathrm{CHSH}(n)2, where CHSH(n)\mathrm{CHSH}(n)3 players sit on the vertices of a graph CHSH(n)\mathrm{CHSH}(n)4, an edge is sampled uniformly, and the original two-player CHSH game is played only on that selected pair (Cui et al., 2024). A third is the multiplayer linear game CHSH(n)\mathrm{CHSH}(n)5, whose binary-output winning condition is an CHSH(n)\mathrm{CHSH}(n)6-player XOR constraint rather than a pair-selection rule (Murta et al., 2015). A fourth is the iterated CHSH game, in which a line of repeater nodes performs successive entanglement swaps and the final CHSH test is applied only to the two surviving endpoints (Dmello et al., 2024).

Formal object Core definition Relation to “2-out-of-CHSH(n)\mathrm{CHSH}(n)7”
CHSH(n)\mathrm{CHSH}(n)8 Choose CHSH(n)\mathrm{CHSH}(n)9, then play a CHSH-type XOR test on that pair Exact choose-2-of-i<ji<j0 interpretation
i<ji<j1 Choose an edge of a graph and play CHSH on that pair Pair-selection on prescribed pairs
i<ji<j2 i<ji<j3-player XOR game with parity constraint “2 outcomes for i<ji<j4 players,” not choose-2
Iterated CHSH i<ji<j5-round entanglement-swapping chain, final CHSH on endpoints Two endpoints after an i<ji<j6-stage process

This terminological divergence matters. Some papers explicitly state that they do not study a “2-out-of-i<ji<j7” object even when their scenario has two distinguished endpoints or two outputs. The most precise encyclopedia usage therefore treats i<ji<j8 as the canonical choose-2-of-i<ji<j9 CHSH game, and then places alternative usages around it as related but distinct constructions (Ostrev, 2015, Dmello et al., 2024).

2. The explicit choose-2-of-{1,…,n}\{1,\dots,n\}0 game: {1,…,n}\{1,\dots,n\}1

For {1,…,n}\{1,\dots,n\}2, Alice’s question set is

{1,…,n}\{1,\dots,n\}3

and Bob’s question set is the set of ordered pairs

{1,…,n}\{1,\dots,n\}4

The referee first chooses a pair {1,…,n}\{1,\dots,n\}5 uniformly among all {1,…,n}\{1,\dots,n\}6 pairs with {1,…,n}\{1,\dots,n\}7, and then chooses uniformly one of the four question pairs

{1,…,n}\{1,\dots,n\}8

Each of these four pairs therefore occurs with probability

{1,…,n}\{1,\dots,n\}9

The winning predicate is CHSH-like: for the chosen pair CHSH(n)\mathrm{CHSH}(n)0, the players must give matching answers on

CHSH(n)\mathrm{CHSH}(n)1

and opposite answers on

CHSH(n)\mathrm{CHSH}(n)2

Equivalently,

CHSH(n)\mathrm{CHSH}(n)3

This is the formal sense in which the game first chooses “2 out of CHSH(n)\mathrm{CHSH}(n)4” and then imposes a CHSH-type XOR condition on the chosen pair (Ostrev, 2015).

The corresponding game matrix is

CHSH(n)\mathrm{CHSH}(n)5

For a quantum strategy with state CHSH(n)\mathrm{CHSH}(n)6 and CHSH(n)\mathrm{CHSH}(n)7 observables CHSH(n)\mathrm{CHSH}(n)8 for Alice and CHSH(n)\mathrm{CHSH}(n)9 for Bob, the bias is

nn0

The optimal quantum bias is

nn1

so the optimal winning probability is

nn2

The first member of the family, nn3, is the usual CHSH game after relabeling Bob’s two observables (Ostrev, 2015).

3. Algebraic structure of optimal and nearly optimal strategies

The exact optimality conditions for nn4 take an unusually rigid form. For every optimal strategy and every nn5,

nn6

Equivalently,

nn7

From these relations one derives, on the support of the state, the anti-commutation relations

nn8

The optimal-strategy analysis is therefore controlled by the Clifford-algebra structure generated by nn9 pairwise anti-commuting reflections (Ostrev, 2015).

This algebraic structure yields a full classification of exact optimal strategies. The irreducible block size is

nn0

On the support of nn1, Alice’s observables are block diagonal, with each block equal to a canonical family of pairwise anti-commuting observables nn2 built from tensor products of Pauli matrices. If nn3 is even, each block is

nn4

If nn5 is odd, then for nn6,

nn7

while for nn8, each block is either

nn9

Bob’s optimal observables are fixed blockwise by

CHSHn-d\mathrm{CHSH}_n\text{-}d0

The Schmidt support rank is a multiple of CHSHn-d\mathrm{CHSH}_n\text{-}d1, and unused orthogonal sectors may carry arbitrary CHSHn-d\mathrm{CHSH}_n\text{-}d2 observables without affecting optimality (Ostrev, 2015).

Near-optimal strategies satisfy robust analogues of the same state-dependent identities. If a strategy is CHSHn-d\mathrm{CHSH}_n\text{-}d3-optimal, then

CHSHn-d\mathrm{CHSH}_n\text{-}d4

A key caveat is that ordinary support-based rigidity fails: tiny Schmidt blocks can be modified arbitrarily while preserving near-optimality. The robust substitute is an approximate intertwining operator

CHSHn-d\mathrm{CHSH}_n\text{-}d5

where CHSHn-d\mathrm{CHSH}_n\text{-}d6 and CHSHn-d\mathrm{CHSH}_n\text{-}d7 form a canonical ideal strategy. This CHSHn-d\mathrm{CHSH}_n\text{-}d8 satisfies

CHSHn-d\mathrm{CHSH}_n\text{-}d9

and

nn0

A plausible implication is that nn1 supplies a rigidity theory whose natural invariant is an approximately embedded Clifford representation rather than full-support operator closeness (Ostrev, 2015).

4. Pair-selection networks and multiplayer CHSH variants

A different formalization of “2-out-of-nn2” arises in graph-based multiplayer extensions. For a simple connected graph nn3 on nn4 vertices, the game nn5 is defined by sampling an edge uniformly and playing the original two-player game only on that pair. Formally,

nn6

For CHSH, this is the natural “pair-selection on a prescribed set of pairs” extension. The main conclusion is exceptionally restrictive: nn7 Equivalently, in this graph model, quantum players can outperform the classical CHSH value only in the original two-player case and on the four-player line nn8 (Cui et al., 2024).

The obstruction is Bell monogamy. On the three-party path nn9,

nn0

so the average CHSH winning probability over the two edges cannot exceed nn1. On the four-party path nn2,

nn3

which gives

nn4

For six-party graphs, the paper reports numerical monogamy relations such as

nn5

again excluding any quantum advantage. Thus, under edge-based pair selection, almost all network topologies destroy CHSH nonlocality (Cui et al., 2024).

A different multiplayer generalization replaces pair selection by an nn6-player linear constraint. The game denoted nn7 has winning condition

nn8

over nn9. In the binary-output case CHSH(n)\mathrm{CHSH}(n)00,

CHSH(n)\mathrm{CHSH}(n)01

which is an CHSH(n)\mathrm{CHSH}(n)02-player XOR game. Its quantum value is bounded by

CHSH(n)\mathrm{CHSH}(n)03

and therefore

CHSH(n)\mathrm{CHSH}(n)04

independent of CHSH(n)\mathrm{CHSH}(n)05. This construction matches the phrase “2 outcomes for CHSH(n)\mathrm{CHSH}(n)06 players,” but it is not a choose-2-of-CHSH(n)\mathrm{CHSH}(n)07 game (Murta et al., 2015).

5. Parallel, sequential, and iterated CHSH constructions

Parallel repetition of ordinary CHSH leads to a different kind of CHSH(n)\mathrm{CHSH}(n)08-indexed generalization. In the parallel self-testing framework, Alice and Bob receive CHSH(n)\mathrm{CHSH}(n)09-bit questions and return CHSH(n)\mathrm{CHSH}(n)10-bit answers, with one nominal CHSH subtest per coordinate. If each subtest CHSH(n)\mathrm{CHSH}(n)11 satisfies

CHSH(n)\mathrm{CHSH}(n)12

then there exists a local isometry extracting

CHSH(n)\mathrm{CHSH}(n)13

In the robust version, if every subtest is at least CHSH(n)\mathrm{CHSH}(n)14, the extracted state is CHSH(n)\mathrm{CHSH}(n)15-close to CHSH(n)\mathrm{CHSH}(n)16 EPR pairs. The proof isolates each coordinate by conditioning on the other CHSH(n)\mathrm{CHSH}(n)17 question bits, constructs large sets of “good” conditional subtests, and then uses pairwise commutation to glue the coordinatewise CHSH rigidities into a tensor-product structure (Coladangelo, 2016).

Sequential repetition addresses memoryful, transcript-dependent devices rather than simultaneous copies. In the sequential rigidity theorem for CHSH(n)\mathrm{CHSH}(n)18 CHSH games, there exists a constant CHSH(n)\mathrm{CHSH}(n)19 such that any CHSH(n)\mathrm{CHSH}(n)20-structured strategy is CHSH(n)\mathrm{CHSH}(n)21-simulated by an ideal strategy. Up to local isometries,

CHSH(n)\mathrm{CHSH}(n)22

is embedded in the devices, and round CHSH(n)\mathrm{CHSH}(n)23 uses the ideal CHSH observables on the CHSH(n)\mathrm{CHSH}(n)24-th qubit. This is not a choose-2-of-CHSH(n)\mathrm{CHSH}(n)25 game either, but it shows that repeated near-optimal CHSH performance forces a fixed tensor-product register of EPR pairs (Reichardt et al., 2012).

The iterated CHSH game is different again. It is defined on a repeater chain

CHSH(n)\mathrm{CHSH}(n)26

where nearest-neighbor pairs share bipartite resources, each Bob performs a bipartite measurement, the Bob outcomes are broadcast, Alice and Charlie may apply local corrections, and a final CHSH test is performed on the effective endpoint state. If CHSH(n)\mathrm{CHSH}(n)27 is the Bob outcome string, with branch probabilities CHSH(n)\mathrm{CHSH}(n)28 and endpoint CHSH values CHSH(n)\mathrm{CHSH}(n)29, the game value is

CHSH(n)\mathrm{CHSH}(n)30

The paper emphasizes that this is not a combinatorial “pick any 2 out of CHSH(n)\mathrm{CHSH}(n)31” Bell game. Its main theorem is that oblate stabilizer theory reaches

CHSH(n)\mathrm{CHSH}(n)32

for arbitrary CHSH(n)\mathrm{CHSH}(n)33, while quantum theory reaches CHSH(n)\mathrm{CHSH}(n)34 for all CHSH(n)\mathrm{CHSH}(n)35 using Bell states, Bell measurements, and local Pauli corrections (Dmello et al., 2024).

6. Other generalized CHSH families and the boundaries of the concept

The finite-field game CHSH(n)\mathrm{CHSH}(n)36 is another generalized CHSH family often confused with “2-out-of-CHSH(n)\mathrm{CHSH}(n)37” terminology. Here Alice and Bob receive uniformly random inputs

CHSH(n)\mathrm{CHSH}(n)38

produce outputs

CHSH(n)\mathrm{CHSH}(n)39

and win iff

CHSH(n)\mathrm{CHSH}(n)40

For prime CHSH(n)\mathrm{CHSH}(n)41, the paper gives an explicit deterministic classical strategy with winning probability

CHSH(n)\mathrm{CHSH}(n)42

This is a multi-input, multi-output finite-field generalization of CHSH, not a choose-2-of-CHSH(n)\mathrm{CHSH}(n)43 Bell game (Pivoluska et al., 2015).

A second nearby family is the CHSH(n)\mathrm{CHSH}(n)44-outcome CHSH-type SATWAP inequality. It is a two-input, CHSH(n)\mathrm{CHSH}(n)45-output scenario with generalized observables

CHSH(n)\mathrm{CHSH}(n)46

and generalized correlators

CHSH(n)\mathrm{CHSH}(n)47

The SATWAP Bell expression has classical bound

CHSH(n)\mathrm{CHSH}(n)48

and quantum bound

CHSH(n)\mathrm{CHSH}(n)49

Again, this is “2 inputs and CHSH(n)\mathrm{CHSH}(n)50 outcomes,” not “choose 2 out of CHSH(n)\mathrm{CHSH}(n)51” (Baroni et al., 2024).

An LCS-based alternative generalization is the family CHSH(n)\mathrm{CHSH}(n)52, built from the inconsistent equations

CHSH(n)\mathrm{CHSH}(n)53

with answer alphabet CHSH(n)\mathrm{CHSH}(n)54. Its verifier predicate is

CHSH(n)\mathrm{CHSH}(n)55

CHSH(n)\mathrm{CHSH}(n)56

This family satisfies CHSH(n)\mathrm{CHSH}(n)57, has classical value CHSH(n)\mathrm{CHSH}(n)58, and admits the explicit quantum strategy value

CHSH(n)\mathrm{CHSH}(n)59

It is a CHSH(n)\mathrm{CHSH}(n)60-valued CHSH generalization with two questions per player and CHSH(n)\mathrm{CHSH}(n)61-ary outputs, not the standard choose-2-of-CHSH(n)\mathrm{CHSH}(n)62 game (Cui et al., 2019).

Taken together, these variants show that “2-out-of-CHSH(n)\mathrm{CHSH}(n)63 CHSH game” has a narrow exact meaning only in the CHSH(n)\mathrm{CHSH}(n)64 family, and a broader heuristic meaning in several adjacent constructions. The exact choose-2-of-CHSH(n)\mathrm{CHSH}(n)65 object is the XOR game CHSH(n)\mathrm{CHSH}(n)66; graph-based pair selection supplies a network version; multiplayer, finite-field, repeater-chain, and CHSH(n)\mathrm{CHSH}(n)67-outcome models instead generalize other aspects of CHSH—number of parties, algebraic alphabet, causal structure, or outcome cardinality—rather than the combinatorics of choosing two indices from CHSH(n)\mathrm{CHSH}(n)68.

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