2016
DOI: 10.1007/jhep10(2016)025
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Tunneling in axion monodromy

Abstract: The Coleman formula for vacuum decay and bubble nucleation has been used to estimate the tunneling rate in models of axion monodromy in recent literature. However, several of Coleman's original assumptions do not hold for such models. Here we derive a new estimate with this in mind using a similar Euclidean procedure. We find that there are significant regions of parameter space for which the tunneling rate in axion monodromy is not well approximated by the Coleman formula. However, there is also a regime rele… Show more

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Cited by 29 publications
(59 citation statements)
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“…This structre is also present in models of axion monodromy where it has been argued that tunneling between branches can compete with the perturbative evolution of the inflaton [40][41][42][43][44][45][46]. A rough estimate of the size of non-perturbative effects is given by the Coleman-De Luccia thin-wall approximation [47] of the tunneling rate:…”
Section: Jhep05(2018)075mentioning
confidence: 96%
“…This structre is also present in models of axion monodromy where it has been argued that tunneling between branches can compete with the perturbative evolution of the inflaton [40][41][42][43][44][45][46]. A rough estimate of the size of non-perturbative effects is given by the Coleman-De Luccia thin-wall approximation [47] of the tunneling rate:…”
Section: Jhep05(2018)075mentioning
confidence: 96%
“…So the viability of inflation requires that these membranes are not so light that their emission 'discharges' the initial field displacement too quickly, spoiling slow roll [4,5,51]. It appears reasonable to assume that the WGC places an upper bound on such charged membranes, though opinions differ as to how prohibitive this constraint is [54][55][56][57].…”
Section: The Weak Gravity Conjecture and Membranesmentioning
confidence: 99%
“…Tunneling between the different branches is mediated by nucleating a membrane electrically charged under the 3-form field, but the tunneling rate is not fast enough to constrain large field inflation significantly [24][25][26]. Invariance under the gauge symmetry of the 3-form field also constrains the form of the higher dimensional corrections, which should appear as functions of the field strength F 4 or ρ(φ ) over the cut-off scale [7,8,27].…”
Section: Description In Terms Of Minkowski 4-formsmentioning
confidence: 99%