2012
DOI: 10.1007/s11005-012-0582-5
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Multilocal Fermionization

Abstract: Abstract. We present a simple isomorphism between the algebra of one real chiral Fermi field and the algebra of n real chiral Fermi fields. The isomorphism preserves the vacuum state. This is possible by a "change of localization", and gives rise to new multilocal symmetries generated by the corresponding multilocal current and stress-energy tensor. The result gives a common underlying explanation of several remarkable recent results on the representation of the free Bose field in terms of free Fermi fields (A… Show more

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Cited by 21 publications
(34 citation statements)
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“…For the fermion field and any number of intervals, or the current field in the single interval case, this same phase factor determines completely the dependence of all eigenvectors in s. In this case the modular flow has a simple geometrical picture as a translation in the variable ω, ω → ω + 2πτ [22]. Perhaps a reason for the fermion to be special is the multilocal symmetries described by Rehren and Tedesco [46].…”
Section: Final Remarksmentioning
confidence: 99%
“…For the fermion field and any number of intervals, or the current field in the single interval case, this same phase factor determines completely the dependence of all eigenvectors in s. In this case the modular flow has a simple geometrical picture as a translation in the variable ω, ω → ω + 2πτ [22]. Perhaps a reason for the fermion to be special is the multilocal symmetries described by Rehren and Tedesco [46].…”
Section: Final Remarksmentioning
confidence: 99%
“…We will find that the multi-interval modular flow can be obtained by gluing together single interval modular flows. In the operator algebra language, this gluing is implemented by a non-local isomorphism between the single interval algebra of n free fermions, and the n-interval algebra of a single fermion, as was first observed in [1]. Our work provides a path integral interpretation of this isomorphism.…”
Section: Introductionmentioning
confidence: 80%
“…Undoing the diagonalization then expresses this coupling in terms of an antisymmetric matrix gauge field [1]:…”
Section: Generalization To Many Intervals and Finite Sizementioning
confidence: 99%
“…Now let K = L 2 (I 1 ) ⊕ L 2 (−I 1 ). Our goal is to have an explicit formula forĵ K : this is based on the formula for the modular operator for disjoint intervals in the free fermion case in [22], [29] and [7].…”
Section: Explicit Formula In a Special Casementioning
confidence: 99%
“…We will start with the following linear isomorphism from H ⊕ H to H which is inspired by Prop. 3 in [29] …”
Section: Explicit Formula In a Special Casementioning
confidence: 99%