2005
DOI: 10.1016/j.nuclphysb.2005.01.021
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Continuum limit of the integrable superspin chain

Abstract: By a combination of analytical and numerical techniques, we analyze the continuum limit of the integrable 3 ⊗3 ⊗ 3 ⊗3 . . . sl(2/1) superspin chain. We discover profoundly new features, including a continuous spectrum of conformal weights, whose numerical evidence is infinite degeneracies of the scaled gaps in the thermodynamic limit. This indicates that the corresponding conformal field theory has a non compact target space (even though our lattice model involves only finite dimensional representations). We a… Show more

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Cited by 60 publications
(140 citation statements)
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“…(2.11) seems to be overcome if one uses the approach of [50]. 7 The attribute "projective" is used here in the sense of category theory and should not be confused with the notion of projective representations that is used when algebraic relations are only respected up to some multipliers (cocycles). 8 It should be stressed that this property is not true for type II Lie superalgebras.…”
Section: Projective Modulesmentioning
confidence: 99%
“…(2.11) seems to be overcome if one uses the approach of [50]. 7 The attribute "projective" is used here in the sense of category theory and should not be confused with the notion of projective representations that is used when algebraic relations are only respected up to some multipliers (cocycles). 8 It should be stressed that this property is not true for type II Lie superalgebras.…”
Section: Projective Modulesmentioning
confidence: 99%
“…For further string motivated research in this direction see e.g. [15,16,17], and for more condensed matter oriented work see [19,20,21,22]). …”
Section: Introductionmentioning
confidence: 99%
“…As a way out, one can try to 'discretize' the sigma model and construct a lattice spin chain of length N that would flow into the former in the continuum limit N → ∞. It has been proposed [10,11] to look for such models among integrable graded spin chains with the Hilbert space of the type (V ⊗V) ⊗N/2 with V andV being conjugated infinite-dimensional representations of supergroups. However, the tensor product V⊗V contains in general irreducible components which have neither the highest, nor the lowest weight vectors and, as a consequence, the nested Bethe ansatz is not applicable.…”
Section: Introductionmentioning
confidence: 99%