2007
DOI: 10.1103/physrevlett.98.131301
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Measures on Transitions for Cosmology from Eternal Inflation

Abstract: We argue that, in the context of eternal inflation in the landscape, making predictions for cosmological--and possibly particle physics--observables requires a measure on the possible cosmological histories as opposed to one on the vacua themselves. If significant slow-roll inflation occurs, the observables are generally determined by the history after the last transition between metastable vacua. Hence, we start from several existing measures for counting vacua and develop measures for counting the transition… Show more

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Cited by 32 publications
(36 citation statements)
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“…Since an eternally inflating multiverse contains an infinite number of each type of vacuum allowed in the landscape, it is necessary to use some regularization procedure to compute the prior probability distribution. Many such regularization procedures, or probability measures, have been proposed [21,22,23,24,25]. For a more complete and up to date account see Ref.…”
Section: Introductionmentioning
confidence: 99%
“…Since an eternally inflating multiverse contains an infinite number of each type of vacuum allowed in the landscape, it is necessary to use some regularization procedure to compute the prior probability distribution. Many such regularization procedures, or probability measures, have been proposed [21,22,23,24,25]. For a more complete and up to date account see Ref.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, we observe Q to lie comfortably in the middle of the anthropic range [45], indicating that no such strong selection effect is at work. 5 Note that a similar story applies to the magnitude of the gravitational constant G [35].…”
Section: A Global Time Cutoffsmentioning
confidence: 95%
“…Instead, the particle will orbit the HM point until the trajectory becomes singular due to the evolution of the scale factor. Therefore, we conclude that the instanton must lie along a line of symmetry (passing through the HM point), where the angular momentum can remain zero, and the problem becomes effectively one-dimensional 10 . Slicing the potential along one of the discrete lines of symmetry, we can determine the condition for the existence of a single-pass CDL instanton as…”
Section: Single and Multiple Pass Instantonsmentioning
confidence: 99%
“…In general, τ is not altered much between minima on adjacent sheets of the potential (see Table I). Given a particular value of z, the potential on the τ −plane has a global minimum as 10 It makes little sense to interpret instantons in directions associated with a continuous symmetry as tunneling solutions since there will be a classically allowed path between the instanton endpoints. Discrete lines of symmetry associate d with positive eigenvalues of the mass matrix should be ignored as well.…”
Section: A Euclidean Pathsmentioning
confidence: 99%
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