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In [[theoretical physics]], a '''minimal model''' or '''Virasoro minimal model''' is a [[two-dimensional conformal field theory]] whose spectrum is built from finitely many irreducible representations of the [[Virasoro algebra]].
In [[theoretical physics]], a '''minimal model''' or '''Virasoro minimal model''' is a [[two-dimensional conformal field theory]] whose spectrum is built from finitely many irreducible representations of the [[Virasoro algebra]].
Minimal models have been classified and solved, and found to obey an [[ADE classification]]. <ref>A. Cappelli, J-B. Zuber, "A-D-E Classification of Conformal Field Theories", [http://www.scholarpedia.org/article/A-D-E_Classification_of_Conformal_Field_Theories Scholarpedia]</ref>
Minimal models have been classified and solved, and found to obey an [[ADE classification]]. <ref>A. Cappelli, J-B. Zuber, "A-D-E Classification of Conformal Field Theories", [http://www.scholarpedia.org/article/A-D-E_Classification_of_Conformal_Field_Theories Scholarpedia]</ref>
Minimal models can also be defined based on algebras that are larger than the Virasoro algebra, such as [[W-algebra|W-algebras]].
The term minimal model can also refer to rational CFTs based on algebras that are larger than the Virasoro algebra, such as [[W-algebra|W-algebras]].


==Classification==
==Classification==

Revision as of 21:03, 2 October 2017

In theoretical physics, a minimal model or Virasoro minimal model is a two-dimensional conformal field theory whose spectrum is built from finitely many irreducible representations of the Virasoro algebra. Minimal models have been classified and solved, and found to obey an ADE classification. [1] The term minimal model can also refer to rational CFTs based on algebras that are larger than the Virasoro algebra, such as W-algebras.

Classification

These conformal field theories have a finite set of conformal families which close under fusion. However, generally these will not be unitary. Unitarity imposes the further restriction that q and p are related by q=m and p=m+1.

for m = 2, 3, 4, .... and h is one of the values

for r = 1, 2, 3, ..., m−1 and s= 1, 2, 3, ..., r.

The first few minimal models correspond to central charges and dimensions:

  • m = 3: c = 1/2, h = 0, 1/16, 1/2. These 3 representations are related to the Ising model at criticality. The three operators correspond to the identity, spin and energy density respectively.
  • m = 4: c = 7/10. h = 0, 3/80, 1/10, 7/16, 3/5, 3/2. These 6 give the scaling fields of the tri critical Ising model.
  • m = 5: c = 4/5. These give the 10 fields of the 3-state Potts model.
  • m = 6: c = 6/7. These give the 15 fields of the tri critical 3-state Potts model.

References

  1. ^ A. Cappelli, J-B. Zuber, "A-D-E Classification of Conformal Field Theories", Scholarpedia
  • P. Di Francesco, P. Mathieu, and D. Sénéchal, Conformal Field Theory, Springer-Verlag, New York City, 1997. ISBN 0-387-94785-X.