2011
DOI: 10.1103/physrevlett.107.171301
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Populating the Whole Landscape

Abstract: Every de Sitter vacuum can transition to every other de Sitter vacuum despite any obstacle, despite intervening anti-de Sitter sinks, despite not being connected by an instanton. Eternal inflation populates the whole landscape.

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Cited by 36 publications
(44 citation statements)
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“…This would erase all memory of the initial conditions. Furthermore Brown and Dahlen (2011) have argued that despite some potential problems -vacua not connected by instantons, or only connected through sinks (Clifton et al, 2007) -all dS vacua are reachable with non-zero transition rates. This result holds for minima of the same potential, but arguments were given for parts of the landscape with different topologies as well.…”
Section: The Dominant Vacuummentioning
confidence: 99%
“…This would erase all memory of the initial conditions. Furthermore Brown and Dahlen (2011) have argued that despite some potential problems -vacua not connected by instantons, or only connected through sinks (Clifton et al, 2007) -all dS vacua are reachable with non-zero transition rates. This result holds for minima of the same potential, but arguments were given for parts of the landscape with different topologies as well.…”
Section: The Dominant Vacuummentioning
confidence: 99%
“…After emerging, the field will roll down the potential until the next minimum. This process allows to connect minima for which a CDL instanton does not exist, and has been argued to be essential to populate the landscape [48], since up-tunneling from AdS cannot proceed through usual CDL instantons. The decay rate of this stochastic diffusion process is equivalent to that of an homogeneous tunneling of the whole universe in which the bubble radius is R b ∼ l 4 .…”
Section: Jhep11(2017)066mentioning
confidence: 99%
“…[44][45][46][47][48] and references therein). A HM instanton describes the quantum transition of a field starting at the minimum and emerging at the top of the barrier due to quantum fluctuations in a sort of Brownian motion [46][47][48]. After emerging, the field will roll down the potential until the next minimum.…”
Section: Jhep11(2017)066mentioning
confidence: 99%
“…Domain walls between stable de Sitter vacua trigger an instability towards nonpositive vacuum energy [18][19][20][21][22][23].…”
Section: Jhep12(2016)155mentioning
confidence: 99%
“…Therefore, the presence of a domain wall between metastable vacua will generically de-stabilize some moduli, as illustrated in figure 1. The instability towards a runaway phase leads to the collapse of the interior de Sitter vacuum and naively poses an obstacle to populating the landscape [19][20][21][22][23].…”
Section: Jhep12(2016)155mentioning
confidence: 99%