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      The renormalized Hamiltonian truncation method in the large \(E_T\) expansion

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          Abstract

          Hamiltonian Truncation Methods are a useful numerical tool to study strongly coupled QFTs. In this work we present a new method to compute the exact corrections, at any order, in the Hamiltonian Truncation approach presented by Rychkov et al. in Refs. [1-3]. The method is general but as an example we calculate the exact \(g^2\) and some of the \(g^3\) contributions for the \(\phi^4\) theory in two dimensions. The coefficients of the local expansion calculated in Ref. [1] are shown to be given by phase space integrals. In addition we find new approximations to speed up the numerical calculations and implement them to compute the lowest energy levels at strong coupling. A simple diagrammatic representation of the corrections and various tests are also introduced.

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          Author and article information

          Journal
          2015-12-17
          2016-04-21
          Article
          1512.05746
          5ad3966e-6b88-4a38-8209-8a3ba75b5cc6

          http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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          Custom metadata
          JHEP version, typos fixed in Appendix and eq. (23)
          hep-th cond-mat.stat-mech cond-mat.str-el hep-lat

          Condensed matter,High energy & Particle physics
          Condensed matter, High energy & Particle physics

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