Monte Carlo Simulation of Two-Electron Spin Correlations

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This Demonstration simulates the results of spin measurements on two-electron spins, using rotatable analyzers along directions and that can be selected by the user. The two electrons remain in an eigenstate of total spin squared.

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The applied Monte Carlo method is designed to simulate the probabilistic predictions of quantum mechanics. A continuously updated diagram lets you observe how the correlation coefficients of the simulated events move toward the predicted quantum-mechanical values. Since the events are determined by an algorithm, the Demonstration is a deterministic version of quantum mechanics in which the phase of the wavefunction plays the role of a hidden variable.

The program runs freely upon activating the "run" checkbox. It will react to all available controls; in particular, it can be stopped by the "reset" checkbox.

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Contributed by: Ulrich Mutze (April 2015)
Open content licensed under CC BY-NC-SA


Snapshots


Details

Snapshot 1: measuring along the same direction results in perfect anticorrelation

Snapshot 2: 10° deviation of the measuring directions allows parallel alignment in rare cases

Snapshot 3: 10° deviation from orthogonality makes a small correlation coefficient

Snapshot 4: orthogonal directions make the correlation coefficient vanish

Snapshot 5: constructive addition of spins is the usual case in triplet states

This Demonstration considers the simplest nontrivial quantum system composed of two subsystems, allowing us to study the phenomenon of entanglement. This system was employed by D. Bohm in his discussion of the EPR "paradox" and is referred to in most discussions of Bell's inequality (see e.g. the Scholarpedia article "Bell's Theorem"). It is an idealized system in which the spacial dependence of the electron wavefunctions is ignored, and thus no (anti-)symmetry restrictions from Pauli's principle are imposed. Nevertheless, it turns out that the "groundstate" (i.e. the state with the lowest eigenvalue, 0 in this case) of the operator , the so-called singlet state, is necessarily antisymmetric with respect to an exchange of the electrons. This state has the property that the spins, if both measured along the same direction (i.e. ), are always found to be antiparallel.



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