CHSH inequality
In physics, the CHSH inequality can be used in the proof of Bell's theorem, which states that certain consequences of entanglement in quantum mechanics cannot be reproduced by local hidden variable theories. Experimental verification of violation of the inequalities is seen as experimental confirmation that nature cannot be described by local hidden variables theories. CHSH stands for John Clauser, Michael Horne, Abner Shimony, and Richard Holt, who described it in a much-cited paper published in 1969. They derived the CHSH inequality, which, as with John Bell's original inequality, is a constraint on the statistics of "coincidences" in a Bell test experiment which is necessarily true if there exist underlying local hidden variables. This constraint can, on the other hand, be infringed by quantum mechanics.
Statement
The usual form of the CHSH inequality iswhere
a and a′ are detector settings on side A, b and b′ on side B, the four combinations being tested in separate subexperiments. The terms E etc. are the quantum correlations of the particle pairs, where the quantum correlation is defined to be the expectation value of the product of the "outcomes" of the experiment, i.e. the statistical average of A·B, where A and B are the separate outcomes, using the coding +1 for the '+' channel and −1 for the '−' channel. Clauser et al.'s 1969 derivation was oriented towards the use of "two-channel" detectors, and indeed it is for these that it is generally used, but under their method the only possible outcomes were +1 and −1. In order to adapt to real situations, which at the time meant the use of polarised light and single-channel polarisers, they had to interpret '−' as meaning "non-detection in the '+' channel", i.e. either '−' or nothing. They did not in the original article discuss how the two-channel inequality could be applied in real experiments with real imperfect detectors, though it was later proved that the inequality itself was equally valid. The occurrence of zero outcomes, though, means it is no longer so obvious how the values of E are to be estimated from the experimental data.
The mathematical formalism of quantum mechanics predicts a maximum value for S of 2, which is greater than 2, and CHSH violations are therefore predicted by the theory of quantum mechanics.
A typical CHSH experiment
In practice most actual experiments have used light rather than the electrons that Bell originally had in mind. The property of interest is, in the best known experiments, the polarisation direction, though other properties can be used. The diagram shows a typical optical experiment. Coincidences are recorded, the results being categorised as '++', '+−', '−+' or '−−' and corresponding counts accumulated.Four separate subexperiments are conducted, corresponding to the four terms in the test statistic S. The settings a, a′, b and b′ are generally in practice chosen to be 0, 45°, 22.5° and 67.5° respectively — the "Bell test angles" — these being the ones for which the QM formula gives the greatest violation of the inequality.
For each selected value of a and b, the numbers of coincidences in each category are recorded. The experimental estimate for is then calculated as:
Once all the 's have been estimated, an experimental estimate of S can be found. If it is numerically greater than 2 it has infringed the CHSH inequality and the experiment is declared to have supported the QM prediction and ruled out all local hidden variable theories.
The CHSH paper lists many preconditions to derive the simplified theorem and formula. For example, for the method to be valid, it has to be assumed that the detected pairs are a fair sample of those emitted. In actual experiments, detectors are never 100% efficient, so that only a sample of the emitted pairs are detected. A subtle, related requirement is that the hidden variables do not influence or determine detection probability in a way that would lead to different samples at each arm of the experiment.
Derivation
The original 1969 derivation will not be given here since it is not easy to follow and involves the assumption that the outcomes are all +1 or −1, never zero. Bell's 1971 derivation is more general. He effectively assumes the "Objective Local Theory" later used by Clauser and Horne. It is assumed that any hidden variables associated with the detectors themselves are independent on the two sides and can be averaged out from the start. Another derivation of interest is given in Clauser and Horne's 1974 paper, in which they start from the CH74 inequality.It would appear from both these later derivations that the only assumptions really needed for the inequality itself are that the distribution of the possible states of the source remains constant and the detectors on the two sides act independently.
Bell's 1971 derivation
The following is based on page 37 of Bell's Speakable and Unspeakable, the main change being to use the symbol ‘E’ instead of ‘P’ for the expected value of the quantum correlation. This avoids any implication that the quantum correlation is itself a probability.We start with the standard assumption of independence of the two sides, enabling us to obtain the joint probabilities of pairs of outcomes by multiplying the separate probabilities, for any selected value of the "hidden variable" λ. λ is assumed to be drawn from a fixed distribution of possible states of the source, the probability of the source being in the state λ for any particular trial being given by the density function ρ, the integral of which over the complete hidden variable space is 1. We thus assume we can write:
where A and B are the average values of the outcomes. Since the possible values of A and B are −1, 0 and +1, it follows that:
Then, if a, a′, b and b′ are alternative settings for the detectors,
Taking absolute values of both sides, and applying the triangle inequality to the right-hand side, we obtain
We use the fact that and are both non-negative to rewrite the right-hand side of this as
By, this must be less than or equal to
which, using the fact that the integral of ρ is 1, is equal to
which is equal to.
Putting this together with the left-hand side, we have:
which means that the left-hand side is less than or equal to both and. That is:
from which we obtain
, which is the CHSH inequality.
Derivation from Clauser and Horne's 1974 inequality
In their 1974 paper, Clauser and Horne show that the CHSH inequality can be derived from the CH74 one. As they tell us, in a two-channel experiment the CH74 single-channel test is still applicable and provides four sets of inequalities governing the probabilities p of coincidences.Working from the inhomogeneous version of the inequality, we can write:
where j and k are each '+' or '−', indicating which detectors are being considered.
To obtain the CHSH test statistic S, all that is needed is to multiply the inequalities for which j is different from k by −1 and add these to the inequalities for which j and k are the same.