All

What are you looking for?

All
Projects
Results
Organizations

Quick search

  • Projects supported by TA ČR
  • Excellent projects
  • Projects with the highest public support
  • Current projects

Smart search

  • That is how I find a specific +word
  • That is how I leave the -word out of the results
  • “That is how I can find the whole phrase”

Functional integrals and inequivalent representations in Quantum Field Theory

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F68407700%3A21340%2F17%3A00312895" target="_blank" >RIV/68407700:21340/17:00312895 - isvavai.cz</a>

  • Result on the web

    <a href="http://dx.doi.org/10.1016/j.aop.2017.05.022" target="_blank" >http://dx.doi.org/10.1016/j.aop.2017.05.022</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1016/j.aop.2017.05.022" target="_blank" >10.1016/j.aop.2017.05.022</a>

Alternative languages

  • Result language

    angličtina

  • Original language name

    Functional integrals and inequivalent representations in Quantum Field Theory

  • Original language description

    We discuss canonical transformations in Quantum Field Theory in the framework of the functional-integral approach. In contrast with ordinary Quantum Mechanics, canonical transformations in Quantum Field Theory are mathematically more subtle due to the existence of unitarily inequivalent representations of canonical commutation relations. When one works with functional integrals, it is not immediately clear how this algebraic feature manifests itself in the formalism. Here we attack this issue by considering the canonical transformations in the context of coherent-state functional integrals. Specifically, in the case of linear canonical transformations, we derive the general functional-integral representations for both transition amplitude and partition function phrased in terms of new canonical variables. By means of this, we show how in the infinite-volume limit the canonical transformations induce a transition from one representation of canonical commutation relations to another one and under what conditions the representations are unitarily inequivalent. We also consider the partition function and derive the energy gap between statistical systems described in two different representations which, among others, allows to establish a connection with continuous phase transitions. We illustrate the inner workings of the outlined mechanism by discussing two prototypical systems: the van Hove model and the Bogoliubov model of weakly interacting Bose gas. (C) 2017 Elsevier Inc. All rights reserved.

  • Czech name

  • Czech description

Classification

  • Type

    J<sub>imp</sub> - Article in a specialist periodical, which is included in the Web of Science database

  • CEP classification

  • OECD FORD branch

    10303 - Particles and field physics

Result continuities

  • Project

    <a href="/en/project/GF17-33812L" target="_blank" >GF17-33812L: An information-theoretical perspective on complex systems</a><br>

  • Continuities

    P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)

Others

  • Publication year

    2017

  • Confidentiality

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Data specific for result type

  • Name of the periodical

    Annals of Physics

  • ISSN

    0003-4916

  • e-ISSN

    1096-035X

  • Volume of the periodical

    383

  • Issue of the periodical within the volume

    Aug

  • Country of publishing house

    US - UNITED STATES

  • Number of pages

    32

  • Pages from-to

    207-238

  • UT code for WoS article

    000407667300013

  • EID of the result in the Scopus database

    2-s2.0-85033451161