2017
DOI: 10.1007/s00601-017-1275-5
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Light-Front Versus Equal-Time Quantization in $$\varvec{\phi ^4}$$ ϕ 4 Theory

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Cited by 2 publications
(3 citation statements)
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“…For this simple case where all operators are scalars, we can evaluate the integral over w to obtain the final Hamiltonian matrix element 14) where in evaluating this integral we've assumed (without loss of generality) that µ 2 > µ 2 . This expression agrees with eqs.…”
Section: Jhep10(2020)095mentioning
confidence: 99%
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“…For this simple case where all operators are scalars, we can evaluate the integral over w to obtain the final Hamiltonian matrix element 14) where in evaluating this integral we've assumed (without loss of generality) that µ 2 > µ 2 . This expression agrees with eqs.…”
Section: Jhep10(2020)095mentioning
confidence: 99%
“…In this section, we will work out matrix elements of 14) i.e., the mass term in the lightcone Hamiltonian (6.2). An important feature and simplification of lightcone quantization is that the vacuum is trivial [8][9][10].…”
Section: Jhep10(2020)095mentioning
confidence: 99%
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