Abstract

We initiate the application of Hamiltonian Truncation methods to solve strongly coupled QFTs in $d=2+1$. By analysing perturbation theory with a Hamiltonian Truncation regulator, we pinpoint the challenges of such an approach and propose a way that these can be addressed. This enables us to formulate Hamiltonian Truncation theory for $\phi^4$ in $d=2+1$, and to study its spectrum at weak and strong coupling. The results obtained agree well with the predictions of a weak/strong self-duality possessed by the theory. The $\phi^4$ interaction is a strongly relevant UV divergent perturbation, and represents a case study of a more general scenario. Thus, the approach developed should be applicable to many other QFTs of interest.

Highlights

  • There is currently no known universal and efficient method to derive the phenomenological implications of strongly coupled quantum field theories (QFTs)

  • We initiate the application of Hamiltonian truncation methods to solve strongly coupled QFTs in d 1⁄4 2 þ 1

  • Disconnected vacuum diagrams cancel in an intricate manner in Hamiltonian perturbation theory; and we find that such cancelation is spoiled with the ET regularization, introducing new UV divergences

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Summary

INTRODUCTION

There is currently no known universal and efficient method to derive the phenomenological implications of strongly coupled quantum field theories (QFTs). A closely related version, coined conformal truncation, exploits light-cone quantization to truncate the wave-functions at infinite volume [3,4,5,6,7] Another guise of HT uses a massive Fock-Space basis to truncate the Hamiltonian. Many of the techniques that we will develop should be useful for formulating HT in any dimension for theories in which V is a strongly relevant perturbation. The results of Hamiltonian truncation at weak coupling must match those of perturbation theory. Disconnected vacuum diagrams cancel in an intricate manner in Hamiltonian perturbation theory; and we find that such cancelation is spoiled with the ET regularization, introducing new UV divergences.

Definitions
The approach
PERTURBATION THEORY
Examples
Analytic solution The free theory is given by the action
Perturbative solution
Vacuum
E2T ð4:12Þ
First excited state
Hamiltonian truncation solution
HAMILTONIAN TRUNCATION FOR A UV DIVERGENT PERTURBATION
Problems with naive perturbation theory
The general case
Two-point bubbles II
Further comments
Patching up perturbation theory with ET regularization
Patch I
Eiks ð5:41Þ
Hamiltonian truncation formulation
ET dependence
Comparison with perturbation theory
Theory
Numerical results
VIII. SUMMARY AND OUTLOOK
Principal equations
Cancellation of disconnected two-point bubbles
Sources of finite regulator dependence
Full Text
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