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Physical Review A

Gleason-Busch theorem for sequential measurements

Kieran Flatt, Stephen Mark Barnett, Sarah Croke

Published Dec 20, 2017• 7 citations
Publisher

Abstract

Gleason's theorem is a statement that, given some reasonable assumptions, the Born rule used to calculate probabilities in quantum mechanics is essentially unique [A. M. Gleason, Indiana Univ. Math. J. 6, 885 (1957)]. We show that Gleason's theorem contains within it also the structure of sequential measurements, and along with this the state update rule. We give a small set of axioms, which are physically motivated and analogous to those in Busch's proof of Gleason's theorem [P. Busch, Phys. Rev. Lett. 91, 120403 (2003)], from which the familiar Kraus operator form follows. An axiomatic approach has practical relevance as well as fundamental interest, in making clear those assumptions which underlie the security of quantum communication protocols. Interestingly, the two-time formalism is seen to arise naturally in this approach.

DOI
10.1103/physreva.96.062125

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Gleason's theorem is a statement that, given some reasonable assumptions, the Born rule used to calculate probabilities in quantum mechanics is essentially unique [A. M. Gleason, Indiana Univ. Math. J. 6, 885 (1957)]. We show that Gleason's theorem contains within it also the structure of sequential measurements, and along with this the state update rule. We give a small set of axioms, which are physically motivated and analogous to those in Busch's proof of Gleason's theorem [P. Busch, Phys. Rev. Lett. 91, 120403 (2003)], from which the familiar Kraus operator form follows. An axiomatic approach has practical relevance as well as fundamental interest, in making clear those assumptions which underlie the security of quantum communication protocols. Interestingly, the two-time formalism is seen to arise naturally in this approach.
Probabilities enter quantum mechanics via Born's rule, the uniqueness of which was proven by Gleason. Busch subsequently relaxed the assumptions of this proof, expanding its domain of applicability in the process. Extending this work to sequential measurement processes is the aim of this paper. Given only a simple set of postulates, a probability measure is derived utilising the concept of Liouville space and the most general permissible quantum channel arises in the same manner. Super-Liouville space is constructed and a Bayesian interpretation of this object is provided. An important application of the new method is demonstrated, providing an axiomatic derivation of important results of the BB84 protocol in quantum cryptography.
Busch's theorem deriving the standard quantum probability rule can be regarded as a more general form of Gleason's theorem. Here we show that a further generalisation is possible by reducing the number of quantum postulates used by Busch. We do not assume that the positive measurement outcome operators are effects or that they form a probability operator measure. We derive a more general probability rule from which the standard rule can be obtained from the normal laws of probability when there is no measurement outcome information available, without the need for further quantum postulates. Our general probability rule has prediction-retrodiction symmetry and we show how it may be applied in quantum communications and in retrodictive quantum theory.
The postulates of quantum theory are rather abstract in comparison with those of other physical theories such as special relativity. This thesis considers two tools for investigating this discrepancy and makes a connection between them. The first of these tools, Gleason-type theorems, illustrates the interplay between postulates concerning observables, states and probabilities of measurement outcomes, demonstrating that they need not be entirely independent. Gleason’s original and remarkable result applied to observables described by projection-valued measures; however, the theorem does not hold in dimension two. Busch generalised the idea to observables described by positive operator measures, proving a result which holds for all separable Hilbert spaces. We show that Busch’s assumptions may be weakened without affecting the result. The manner in which we weaken the assumptions brings them closer to Gleason’s original treatment of projection-valued measures. We will then demonstrate the connection between Gleason-type theorems and Cauchy’s functional equation, a connection which yields an alternative proof of Busch’s result. The second tool we consider is the family of general probabilistic theories which offers a means of comparing quantum theory with reasonable alternatives. We identify a general probabilistic theory which reproduces the set of non-local correlations achievable in quantum theory, a property often thought to be particular to quantum theory. Finally, we connect these two tools by determining the class of general probabilistic theories which admit a Gleason-type theorem.
When a system is measured, its state is changed. A mathematical consequence of this statement is that scenarios in which a quantum system is measured repeatedly, or the same system is used to measure many others, require the use of Kraus’s formalism. Three projects which fall into this category are discussed in this thesis. One is of foundational interest and two are more oriented towards experiment. The first piece of work is an analysis of the uniqueness of each of Kraus's formulae for joint and conditional probabilities. Gleason, Busch and others were interested in whether the probability rules of quantum mechanics were constructed ad hoc or whether they had deeper significance. They showed that the Born rule was the only way of calculating quantum probabilities consistent with some basic assumptions about the nature of a physical theory. I extend this work to the sequential measurement case and show that no further assumptions are required for joint, over single, probabilities. A mathematical technique, the use of operator space, from that work is then developed, in my second reported piece of work, for use as a tool in quantum cryptanalysis. I show that calculations of the best eavesdropping strategies for quantum key distribution protocols can be done in a straightforward manner. I rediscover optimal strategies for BB84 and B92, two of the most commonly discussed protocols, and report a new attack for PBC00. Multiple-copy state discriminators look for methods of distinguishing states given a number of systems all in that state. An open question is whether a quantum memory, a device which interacts with other systems and does not decohere, aids this problem. In the third piece of work reported here, I compare the ability of two schemes, one which uses a quantum memory and one which does not, for performing multiple-copy state discrimination. One surprising result is that the scheme that uses quantum memory always performs worse than the one which does not. Another is that both schemes tend to the same limit in the case that the resource is an infinite number of copies. This suggests that a quantum memory may not be helpful.
In the context of generalized measurement theory, the Gleason-Busch theorem assures the unique form of the associated probability function. Recently, in Flatt et al. Phys. Rev. A 96, 062125 (2017), the case of subsequent measurements has been treated, with the derivation of the L\"uders rule and its generalization (Kraus update rule). Here we investigate the special case of subsequent measurements where an intermediate measurement is a composition of two measurements (a or b) and the case where the causal order is not defined (a and b or b and a). In both cases interference effects can arise. We show that the associated probability cannot be written univocally, and the distributive property on its arguments cannot be taken for granted. The two probability expressions correspond to the Born rule and the classical probability; they are related to the intrinsic possibility of obtaining definite results for the intermediate measurement. For indefinite causal order, a causal inequality is also deduced. The frontier between the two cases is investigated in the framework of generalized measurements with a toy model, a Mach-Zehnder interferometer with a movable beam splitter.
The Born rule — that the probability of obtaining outcome i in a measurement of a quantum system in state |ψ⟩ is given by P(i) = |⟨i|ψ⟩|² — is conventionally introduced as an axiom of quantum mechanics. We present a derivation of the Born rule based on a structural distinction within the substrate-field framework between F1, the unbounded equilibrium configuration of a fundamental scalar field that carries the unitary wave-function dynamics, and F2, the bounded observable configuration that records definite measurement outcomes. F1 → F2 sampling occurs at each Planck-scale time quantum and produces stochastic localization with a probability distribution that, by Gleason's theorem and the non-contextuality of the sampling mechanism, must be of the form Tr(ρ P_i). The squared-modulus form follows. We complement the Gleason argument with Zurek's environment-assisted invariance to address the equal-amplitude case explicitly and discuss the relationship to existing derivations including the decision-theoretic approach of Deutsch and Wallace, the QBist program of Caves, Fuchs, and Schack, and the Bohmian treatment of Dürr, Goldstein, and Zanghì. The contribution of the present argument is to provide a physical mechanism — F1/F2 sampling — that generates probabilities, eliminating the need to postulate them as primitive while retaining the mathematical structure already secured by Gleason's theorem.