English

Critical behavior in $c=1$ matrix model with branching interactions

High Energy Physics - Theory 2009-10-28 v3

Abstract

Motivated by understanding the phase structure of d>1d >1 strings we investigate the c=1c=1 matrix model with g(\trM(t)2)2g' (\tr M(t)^{2})^{2} interaction which is the simplest approximation of the model expected to describe the critical phenomena of the large-NN reduced model of odd-dimensional matrix field theory. We find three distinct phases: (i) an ordinary c=1c=1 gravity phase, (ii) a branched polymer phase and (iii) an intermediate phase. Further we can also analyse the one with slightly generalized g(2)(1N\trM(t)2)2+g(3)(1N\trM(t)2)3++g(n)(1N\trM(t)2)n g^{(2)} (\frac{1}{N}\tr M(t)^{2})^{2} +g^{(3)} (\frac{1}{N}\tr M(t)^{2})^{3} + \cdots + g^{(n)} (\frac{1}{N}\tr M(t)^{2})^{n} interaction. As a result the multi-critical versions of the phase (ii) are found.

Keywords

Cite

@article{arxiv.hep-th/9403089,
  title  = {Critical behavior in $c=1$ matrix model with branching interactions},
  author = {Fumihiko Sugino and Osamu Tsuchiya},
  journal= {arXiv preprint arXiv:hep-th/9403089},
  year   = {2009}
}

Comments

11pages. latex (The arguments in Discussions are corrected and more clarified! Several grammatical errors are corrected. And some preprints in references are replaced with the published versions.)

R2 v1 2026-07-22T15:49:20.414Z