Abstract:We present a novel source of dark energy, which is motivated by the prevalence of hidden sectors in string theory models and is consistent with all of the proposed swampland conjectures. Thermal effects hold a light hidden sector scalar at a point in field space that is not a minimum of its zero temperature potential. This leads to an effective 'cosmological constant', with an equation of state w = −1, despite the scalar's zero temperature potential having only a 4D Minkowski or AdS vacuum. For scalar masses µ… Show more
“…It appears that one needs further SUSY breaking and the F -term problem re-emerges. An interesting alternative to quintessence has been introduced in [104]: The zero-temperature scalar potential is assumed to satisfy the de Sitter conjecture, but a thermally excited hidden sector stabilizes a scalar field at a positive-energy hilltop. The authors illustrate this idea using a simple Higgs-like potential V = −m 2 φ φ 2 /2 + λφ 4 + C. Since the hidden sector must not introduce too much dark radiation, the temperature and hence also m φ are bounded from above by today's CMB temperature, which is roughly 0.24 meV.…”
Section: Loopholes and Alternative Approachesmentioning
We attempt a systematic analysis of string-theoretic quintessence models as an alternative to metastable de Sitter vacua. It appears that, within the boundaries of what is known, largevolume type-IIB flux compactifications are preferred. Here the quintessence scalar is the ratio of certain 4-cycle volumes. It has already been noticed that the volume modulus, which must be stabilized, tends to remain too light. One may call this the "light volume problem". In addition, we identify an "F -term problem": The positive energy density of standard-model SUSY breaking is higher than the depth of all known negative contributions. We discuss what it would take to resolve these issues and comment on partially related challenges for axionic quintessence. In particular, large cancellations between positive and negative potential terms appear unavoidable in general. As a further challenge, one should then explain why a small de-tuning cannot be used to uplift into a deep slow-roll regime, violating de Sitter swampland conjectures.
“…It appears that one needs further SUSY breaking and the F -term problem re-emerges. An interesting alternative to quintessence has been introduced in [104]: The zero-temperature scalar potential is assumed to satisfy the de Sitter conjecture, but a thermally excited hidden sector stabilizes a scalar field at a positive-energy hilltop. The authors illustrate this idea using a simple Higgs-like potential V = −m 2 φ φ 2 /2 + λφ 4 + C. Since the hidden sector must not introduce too much dark radiation, the temperature and hence also m φ are bounded from above by today's CMB temperature, which is roughly 0.24 meV.…”
Section: Loopholes and Alternative Approachesmentioning
We attempt a systematic analysis of string-theoretic quintessence models as an alternative to metastable de Sitter vacua. It appears that, within the boundaries of what is known, largevolume type-IIB flux compactifications are preferred. Here the quintessence scalar is the ratio of certain 4-cycle volumes. It has already been noticed that the volume modulus, which must be stabilized, tends to remain too light. One may call this the "light volume problem". In addition, we identify an "F -term problem": The positive energy density of standard-model SUSY breaking is higher than the depth of all known negative contributions. We discuss what it would take to resolve these issues and comment on partially related challenges for axionic quintessence. In particular, large cancellations between positive and negative potential terms appear unavoidable in general. As a further challenge, one should then explain why a small de-tuning cannot be used to uplift into a deep slow-roll regime, violating de Sitter swampland conjectures.
“…The Dine-Seiberg runaway argument and several no-go theorems then indicate that moduli stabilisation in a de Sitter vacuum will be at the limits of theoretical control, requiring a delicate interplay between diverse string theoretic ingredients. We have focussed, therefore, on two alternative scenarios for Dark Energy: runaway quintessence (reviewing [30] and presenting some further results) and Thermal Dark Energy [31].…”
Section: Discussionmentioning
confidence: 99%
“…We will then discuss quintessence models in string theory, focusing on the runaway potentials that are ubiquitous in string compactifications, summarising [30] and including some further results using supergravity. Finally we will review Thermal Dark Energy [31].…”
Section: Pos(corfu2019)123mentioning
confidence: 99%
“…Given the difficulties encountered in building de Sitter vacua and quintessence in string theory, and the several upcoming observational probes into Dark Energy, it is extremely interesting to consider well-motivated alternative Dark Energy scenarios in string theory. In the remainder of this talk we will review the proposal [31].…”
Section: Thermal Dark Energymentioning
confidence: 99%
“…The lack of any compelling model of de Sitter or quintessence from string theory thus far, drives the search for completely novel string theory origins for Dark Energy. In Thermal Dark Energy [31], high temperature effects in a light hidden sector hold a string theory modulus away from its zero temperature minimum. This sources a positive potential energy density that mimics a cosmological constant, until, as the temperature falls, a phase transition to the true minimum takes place.…”
We consider various candidates for Dark Energy, motivated by string theory. Several no-go theorems push de Sitter string vacua, with w = −1, to the limits of theoretical control, and all known examples depend on a delicate interplay between different string theoretic ingredients. On the other hand, runaway moduli directions are ubiquitous in string theory, and could plausibly source slow-roll quintessence. We consider various candidate supergravity potentials, motivated by string theory, including single-field Kähler potentials for bulk and local moduli, and leading superpotentials of the form W = W 0 +Ae −aΦ or W = W 0 +AΦ p. Conditions on the scalar potential imposed by supergravity are very restrictive, ruling out e.g. quintessence with K = −n ln(Φ +Φ) and W = W 0 + AΦ p. Out of the examples considered, one can simultaneously satisfy V > 0 and * Includes work done in collaborations with Ed Hardy, Yessenia Olguin-Trejo, and Gianmassimo Tasinato. † Speaker.
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