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Sven Aerts

Publications and source records attributed to Sven Aerts.

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Experimental Evidence for Quantum Structure in Cognition

We proof a theorem that shows that a collection of experimental data of membership weights of items with respect to a pair of concepts and its conjunction cannot be modeled within a classical measure theoretic weight structure in case the experimental data contain the effect called overextension. Since the effect of overextension, analogue to the well-known guppy effect for concept combinations, is abundant in all experiments testing weights of items with respect to pairs of concepts and their conjunctions, our theorem constitutes a no-go theorem for classical measure structure for common data of membership weights of items with respect to concepts and their combinations. We put forward a simple geometric criterion that reveals the non classicality of the membership weight structure and use experimentally measured membership weights estimated by subjects in experiments to illustrate our geometrical criterion. The violation of the classical weight structure is similar to the violation of the well-known Bell inequalities studied in quantum mechanics, and hence suggests that the quantum formalism and hence the modeling by quantum membership weights can accomplish what classical membership weights cannot do.

math-ph

Bayes-optimal detection of TNT content by nuclear quadrupole resonance

We study the statistical performance and applicability of a simple quantum state discrimination technique for the analysis of data from nuclear quadrupole resonance experiments on a TNT sample. The target application is remote detection of anti-personnel landmines.We show that, even for data that allows the determination of only one time dependent component of the NQR subsystem, the use of the Bayes optimal detector leads to greatly improved ROC curves with respect to the popular demodulation technique, especially for spin echo signals with a low signal to noise ratio. The method can easily be extended to incorporate results from other sensing modalities and the incorporation of informationally complete measurements that estimate the full density matrix of the NQR subsystem.

cond-mat.other

Quantum and classical probability as Bayes-optimal observation

We propose a simple abstract formalisation of the act of observation, in which the system and the observer are assumed to be in a pure state and their interaction deterministically changes the states such that the outcome can be read from the state of the observer after the interaction. If the observer consistently realizes the outcome which maximizes the likelihood ratio that the outcome pertains to the system under study (and not to his own state), he will be called Bayes-optimal. We calculate the probability if for each trial of the experiment the observer is in a new state picked randomly from his set of states, and the system under investigation is taken from an ensemble of identical pure states. For classical statistical mixtures, the relative frequency resulting from the maximum likelihood principle is an unbiased estimator of the components of the mixture. For repeated Bayes-optimal observation in case the state space is complex Hilbert space, the relative frequency converges to the Born rule. Hence, the principle of Bayes-optimal observation can be regarded as an underlying mechanism for the Born rule. We show the outcome assignment of the Bayes-optimal observer is invariant under unitary transformations and contextual, but the probability that results from repeated application is non-contextual. The proposal gives a concise interpretation for the meaning of the occurrence of a single outcome in a quantum experiment as the unique outcome that, relative to the state of the system, is least dependent on the state of the observe at the instant of measurement.

quant-ph

Undecidable classical properties of observers

A property of a system is called actual, if the observation of the test that pertains to that property, yields an affirmation with certainty. We formalize the act of observation by assuming that the outcome correlates with the state of the observed system and is codified as an actual property of the state of the observer at the end of the measurement interaction. For an actual property, the observed outcome has to affirm that property with certainty, hence in this case the correlation needs to be perfect. A property is called classical if either the property or its negation is actual. It is shown by a diagonal argument that there exist classical properties of an observer that he cannot observe perfectly. Because states are identified with the collection of properties that are actual for that state, it follows that no observer can perfectly observe his own state. Implications for the quantum measurement problem are briefly discussed.

quant-ph

A realistic device that simulates the non-local PR box without communication

A black box with two input bits and two output bits is called a non-local PR box, if the XOR of the output bits equals the AND of the input bits. In a recent article, Cerf et al. show that Alice and Bob, using such a PR box, can effectively simulate entanglement without the need of communication. We show that an adaptation of a model due to Dirk Aerts, yields a realistic simulation of the non-local PR box without communication. Because the model is entirely realistic, it cannot violate relativistic constraints. Like a non-local box, it can be used to simulate the singlet state coincidence probabilities, but the time to complete the observation of the outcome will exceed the time it takes a photon to travel one arm in an EPRB setup. The model explicitly shows how to produce an outcome that is locally perfectly random, but nevertheless determines what happens in the other wing of the experiment, without communication taking place between the two wings. In this sense, it can serve as an accurate metaphor for the mechanism of entanglement. The model considerably strengthens the claim that no communication is necessary to simulate entanglement.

quant-ph

Necessity of Combining Mutually Incompatible Perspectives in the Construction of a Global View: Quantum Probability and Signal Analysis

The scientific fields of quantum mechanics and signal-analysis originated within different settings, aimed at different goals and started from different scientific paradigms. Yet the development of the two subjects has become increasingly intertwined. We argue that these similarities are rooted in the fact that both fields of scientific inquiry had to deal with finding a single description for a phenomenon that yields complete information about itself only when we consider mutually incompatible accounts of that phenomenon.

quant-ph

The Violation of Bell Inequalities in the Macroworld

We show that Bell inequalities can be violated in the macroscopic world. The macroworld violation is illustrated using an example involving connected vessels of water. We show that whether the violation of inequalities occurs in the microworld or in the macroworld, it is the identification of nonidentical events that plays a crucial role. Specifically, we prove that if nonidentical events are consistently differentiated, Bell-type Pitowsky inequalities are no longer violated, even for Bohm's example of two entangled spin 1/2 quantum particles. We show how Bell inequalities can be violated in cognition, specifically in the relationship between abstract concepts and specific instances of these concepts. This supports the hypothesis that genuine quantum structure exists in the mind. We introduce a model where the amount of nonlocality and the degree of quantum uncertainty are parameterized, and demonstrate that increasing nonlocality increases the degree of violation, while increasing quantum uncertainty decreases the degree of violation.

quant-ph

Two-photon Franson-type experiments and local realism

The two-photon interferometric experiment proposed by Franson [Phys. Rev. Lett. 62, 2205 (1989)] is often treated as a "Bell test of local realism". However, it has been suggested that this is incorrect due to the 50% postselection performed even in the ideal gedanken version of the experiment. Here we present a simple local hidden variable model of the experiment that successfully explains the results obtained in usual realizations of the experiment, even with perfect detectors. Furthermore, we also show that there is no such model if the switching of the local phase settings is done at a rate determined by the internal geometry of the interferometers.

quant-ph

Two-photon Franson-type interference experiments are not tests of local realism

We report a local hidden-variable model which reproduces quantum predictions for the two-photon interferometric experiment proposed by Franson [Phys. Rev. Lett. 62, 2205 (1989)]. The model works for the ideal case of full visibility and perfect detection efficiency. This result changes the interpretation of a series of experiments performed in the current decade.

quant-ph