Spekkens ’ toy model in all dimensions and its relationship with stabiliser quantum mechanics

Spekkens’ toymodel is a non-contextual hidden variablemodel with an epistemic restriction, a constraint onwhat an observer can know about reality. The aimof themodel, developed for continuous and discrete prime degrees of freedom, is to advocate the epistemic view of quantum theory, where quantum states are states of incomplete knowledge about a deeper underlying reality. Many aspects of quantummechanics and protocols fromquantum information can be reproduced in themodel. In spite of its significance, a number of aspects of Spekkens’model remained incomplete. Formal rules for the update of states aftermeasurement had not beenwritten down, and the theory had only been constructed for prime-dimensional and infinite dimensional systems. In this work, we remedy this, by derivingmeasurement update rules and extending the framework to derivemodels in all dimensions, both prime and non-prime. Stabiliser quantummechanics (SQM) is a sub-theory of quantummechanics with restricted states, transformations andmeasurements. First derived for the purpose of constructing error correcting codes, it nowplays a role inmany areas of quantum information theory. Previously, it had been shown that Spekkens’model was operationally equivalent to SQM in the case of odd prime dimensions. Here, exploiting known results onWigner functions, we extend this to show that Spekkens’model is equivalent to SQM in all odd dimensions, prime and nonprime. This equivalence provides new technical tools for the study of technically difficult compounddimensional SQM.

[1]  Nicolas Delfosse,et al.  Contextuality as a resource for qubit quantum computation , 2015 .

[2]  Stephen D. Bartlett,et al.  Non-negative subtheories and quasiprobability representations of qubits , 2012, 1203.2652.

[3]  Victor Veitch,et al.  Contextuality Supplies the Magic for Quantum Computation , 2015, 2015 IEEE International Symposium on Multiple-Valued Logic.

[4]  Bill Edwards,et al.  Phase Groups and the Origin of Non-locality for Qubits , 2010, QPL@MFPS.

[5]  A. Kitaev,et al.  Universal quantum computation with ideal Clifford gates and noisy ancillas (14 pages) , 2004, quant-ph/0403025.

[6]  Jan-AAke Larsson A contextual extension of Spekkens' toy model , 2012 .

[7]  Necessity of negativity in quantum theory , 2009, 0910.3198.

[8]  J. Emerson,et al.  Corrigendum: Negative quasi-probability as a resource for quantum computation , 2012, 1201.1256.

[9]  R. Raussendorf,et al.  Wigner Function Negativity and Contextuality in Quantum Computation on Rebits , 2014, 1409.5170.

[10]  Nathan Wiebe,et al.  Efficient simulation scheme for a class of quantum optics experiments with non-negative Wigner representation , 2012, 1210.1783.

[11]  Victor Veitch,et al.  The resource theory of stabilizer quantum computation , 2013, 1307.7171.

[12]  N. Bohr II - Can Quantum-Mechanical Description of Physical Reality be Considered Complete? , 1935 .

[14]  Scott Aaronson,et al.  Improved Simulation of Stabilizer Circuits , 2004, ArXiv.

[15]  R. Raussendorf Quantum computation, discreteness, and contextuality , 2009 .

[16]  R. Spekkens Evidence for the epistemic view of quantum states: A toy theory , 2004, quant-ph/0401052.