1990
DOI: 10.1016/0550-3213(90)90600-i
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Bosonic realization of a universal W-algebra and Z∞ parafermions

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Cited by 101 publications
(124 citation statements)
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“…This limit has been studied previously in specific examples, in [38][39][40][41][42][43], in order to produce representations of the W ∞ algebra. In this limit c ≃ kN + O(1) (3.11) and in this sense it looks like the theory is reducing in this case to a vectorial large-N theory.…”
Section: The Simple Large-n Limitmentioning
confidence: 99%
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“…This limit has been studied previously in specific examples, in [38][39][40][41][42][43], in order to produce representations of the W ∞ algebra. In this limit c ≃ kN + O(1) (3.11) and in this sense it looks like the theory is reducing in this case to a vectorial large-N theory.…”
Section: The Simple Large-n Limitmentioning
confidence: 99%
“…In coset theories primary field dimensions can also be of the order of O 1 N as shown in [23,38,39]. Consider the coset…”
Section: Jhep04(2011)113mentioning
confidence: 99%
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“…For large value of k, c φ → 2 and the underlying W k algebra linearizes in the k → ∞ limit giving rise to the well known Z ∞ parafermionic realization of W ∞ [21].…”
Section: Explicit Realizationmentioning
confidence: 99%
“…For example, we saw above that in the ferromagnetic case, the Heisenberg chain goes to a scale invariant theory with dynamical critical exponent z = 2. On the other hand, the k → ∞ limit of the Z k parafermions is a c = 2 conformal (and Lorentz invariant) theory, Z ∞ , described in [44] (this theory is also W ∞ symmetric). Moreover, in the anti-ferromagnetic case, the Heisenberg theory is described by the su(2) 1 theory, but the k → ∞ limit of M(k + 2, k + 1) is an irrational CFT [45].…”
Section: The Su(2) Intmentioning
confidence: 99%