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- From: marty@amaterasu.physics.uiuc.edu (Marty Gelfand)
- Subject: Re: Link invariants and gauge theory
- References: <BzMAyM.Du2@news.cso.uiuc.edu> <1992Dec22.051055.13451@nuscc.nus.sg>
- Message-ID: <Bzo6Hx.L43@news.cso.uiuc.edu>
- Sender: usenet@news.cso.uiuc.edu (Net Noise owner)
- Organization: Department of Physics, University of Illinois at Urbana-Champaign
- Date: Tue, 22 Dec 1992 16:44:19 GMT
- Lines: 30
-
- In article <1992Dec22.051055.13451@nuscc.nus.sg> matmcinn@nuscc.nus.sg (Brett McInnes) writes:
- >marty@amaterasu.physics.uiuc.edu (Marty Gelfand) writes:
- >: Hey, who says conformal field theory is of no real use??? Down here
- >: in low-energy physics it has been fruitful in problems such as
- > ^^^^^^^^^
- > : quantum spin chains, multichannel Kondo systems,
- >and 2D finite-temperature : critical phenomena (including random systems).
- >:
- >Can you be a little more specific? I must admit that I am sceptical, but
- >maybe I just attended some bad talks. However, I am willing to have my
- >prejudices dispelled.
-
- For 2D critical phenomena, conformal invariance provides a variety
- of unexpected relationships among properties of critical points,
- in particular, between critical exponents, finite-size scaling amplitudes,
- and (this was harder) critical amplitude ratios, because they are all
- related to the "central charge" c of the critical model. Conformal field
- theory provides a classification scheme for 2D critical points
- (due to Belavin, Polyakov, and Z.m.l.chikov): if c is in a certain range,
- it must take on one of a sequence of discrete values, and if it does,
- then all the critical exponents of the model are determined.
- John Cardy has a review in vol 11 of Phase Transitions and Critical Phenomena
- (Domb and Lebowitz, eds).
-
- For applications to 1D quantum systems see, for example, I. Affleck et al,
- J Phys A 22, 511 (1989) and references therein. For other applications
- take a look at anything done by Andreas Ludwig.
-
- Sorry I can't give a brilliant exposition of this stuff, it's way
- beyond me. --Marty Gelfand marty@amaterasu.physics.uiuc.edu
-