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Erschienen in: Quantum Information Processing 7/2015

01.07.2015

Geometry of contextuality from Grothendieck’s coset space

verfasst von: Michel Planat

Erschienen in: Quantum Information Processing | Ausgabe 7/2015

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Abstract

The geometry of cosets in the subgroups \(H\) of the two-generator free group \(G=\langle a,b\rangle \) nicely fits, via Grothendieck’s dessins d’enfants, the geometry of commutation for quantum observables. In previous work, it was established that dessins stabilize point-line geometries whose incidence structure reflects the commutation of (generalized) Pauli operators. Now we find that the nonexistence of a dessin for which the commutator \((a,b)=a^{-1}b^{-1}ab\) precisely corresponds to the commutator of quantum observables \([\mathcal {A},\mathcal {B}] = \mathcal {A}\mathcal {B}-\mathcal {B}\mathcal {A}\) on all lines of the geometry is a signature of quantum contextuality. This occurs first at index \(|G\):\(H|=9\) in Mermin’s square and at index \(10\) in Mermin’s pentagram, as expected. Commuting sets of \(n\)-qubit observables with \(n>3\) are found to be contextual as well as most generalized polygons. A geometrical contextuality measure is introduced.

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Fußnoten
1
For another mathematical approach of quantum contextuality based on sheaf theory, the reader should look at [12] and the references therein.
 
2
A Tits generalized polygon (or generalized \(n\)-gon) is a point-line incidence structure whose incidence graph has diameter \(n\) and girth \(2n\). A generalized polygon of order \((s,t)\) is such that every line contains \(s+1\) points and every point lies on \(t+1\) lines. According to Feit-Higman theorem, the finite generalized \(n\)-gons, \(s,t \ge 2\), exist for \(n=2,3,4,6\) or \(8\). One uses the notation \(GQ\) (for a generalized quadrangle), \(GH\) (for a generalized hexagon) and \(GO\) (for a generalized octagon) corresponding to \(n=4,6\) and \(8\), respectively.
 
3
A geometric hyperplane of a generalized polygon is a proper subspace meeting each line at a unique point or containing the whole line. The set of hyperplanes can be constructed in an efficient way by using an addition law for the hyperplanes: The ‘sum’ of two hyperplanes is just the complement of the symmetric difference in the relevant \(G\)-set of indices labelling the vertices of the geometry [22, 23].
 
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Metadaten
Titel
Geometry of contextuality from Grothendieck’s coset space
verfasst von
Michel Planat
Publikationsdatum
01.07.2015
Verlag
Springer US
Erschienen in
Quantum Information Processing / Ausgabe 7/2015
Print ISSN: 1570-0755
Elektronische ISSN: 1573-1332
DOI
https://doi.org/10.1007/s11128-015-1004-2

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