2022
DOI: 10.1007/jhep08(2022)138
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Tunneling potentials for the tunneling action: gauge invariance

Abstract: We formulate a procedure to obtain a gauge-invariant tunneling rate at zero temperature using the recently developed tunneling potential approach. This procedure relies on a consistent power counting in gauge coupling and a derivative expansion. The tunneling potential approach, while numerically more efficient than the standard bounce solution method, inherits the gauge-dependence of the latter when naïvely implemented. Using the Abelian Higgs model, we show how to obtain a tunneling rate whose residual gauge… Show more

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Cited by 10 publications
(5 citation statements)
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“…Instead of a bounce one has to find a "tunneling potential" function, V t (φ), that interpolates between the false vacuum and (the basin of) the true vacuum and minimizes an action functional, an integral in field space of a simple action density. The resulting action reproduces the Euclidean result and the approach has a number of good properties: it allows a fast and precise numerical calculation of the action [3]; it can be adapted to the study of vacuum decay by thermal fluctuations [3]; it can be used to get solvable potentials (that permit the analytical solution of the tunneling problem) [3][4][5]; it is very useful for vacuum decay in multi-field potentials as one searches for a minimum of the action functional (instead of a saddle-point, as in the Euclidean method) [6]; it can be generalized quite simply to include gravitational corrections offering a quite direct route to the derivation of key results [4,7]; it can deal with issues of gauge invariance [8]; etc.…”
Section: Jcap02(2023)023mentioning
confidence: 99%
See 1 more Smart Citation
“…Instead of a bounce one has to find a "tunneling potential" function, V t (φ), that interpolates between the false vacuum and (the basin of) the true vacuum and minimizes an action functional, an integral in field space of a simple action density. The resulting action reproduces the Euclidean result and the approach has a number of good properties: it allows a fast and precise numerical calculation of the action [3]; it can be adapted to the study of vacuum decay by thermal fluctuations [3]; it can be used to get solvable potentials (that permit the analytical solution of the tunneling problem) [3][4][5]; it is very useful for vacuum decay in multi-field potentials as one searches for a minimum of the action functional (instead of a saddle-point, as in the Euclidean method) [6]; it can be generalized quite simply to include gravitational corrections offering a quite direct route to the derivation of key results [4,7]; it can deal with issues of gauge invariance [8]; etc.…”
Section: Jcap02(2023)023mentioning
confidence: 99%
“…where am(u|m) is the Jacobi amplitude function and ξ e ≡ (d − 2)(d − 1) 2κ sin θ K(sin 2 (θ/2)) , (6.10) 8 Without gravity, we get V (φ) = Vt(φ)…”
Section: Jcap02(2023)023mentioning
confidence: 99%
“…Note that the total one-loop effective potential (equation (2.35)) carries explicit gauge dependence. Since, the important quantities of the study of phase transitions such as the locations of the extrema of V eff (T ), as well as the ratio φ c (T c )/T c , both are gauge-dependent [68,[73][74][75][76][77][78][79][80][81][82]. 1 In addition, the one-loop effective potential of equation (2.35) explicitly depends on the choice of the renormalization scale (Q), which might have a more significant impact than the gauge uncertainty [83].…”
Section: Jhep10(2023)057mentioning
confidence: 99%
“…The gauge dependence, thus, appears through the loop-induced contributions. Gauge invariant treatment of V T and quantities related to it, however, are also possible and are already advocated in the literature [29,150,[153][154][155][156][157][158][159][160][161][162][163][164]. One should also note that V 1−loop CW (see Eq.…”
Section: Contributions From Non-zero Temperaturementioning
confidence: 99%