String Theory and Particle Physics: An Introduction to String Phenomenology

By Luis E Ibáñez, A. Uranga. 2011

457 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/f17afb274dd7225ae9792b9f1ec240dfb8e5b7dd

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Citations in the corpus

F-term axion monodromy inflation (2014, background): “to achieve a Minkowski and/or supersymmetric vacua, see [55, 56] for examples).”
The Weak Gravity Conjecture in three dimensions (2016, background): “Modular invariance is a strong constraint on a theory: it forces a GSO projection, the equality of the left and right-moving central charges (modulo an integer), and for theories with extended chiral algebras in which the U(1) sector is modular invariant by itself it forces the charge lattice (the n”
De Sitter vs Quintessence in String Theory (2018, background): “ence29 4 Conclusions34 A Checking the swampland conjecture for model 237 1 Introduction Ever since the rst superstring revolution, there has been constant progress in the area of string phenomenology [1,2]. Based on our current understanding of string theory, the picture of the string landscape with”
Transplanckian axions!? (2015, background): “For instance, in realizations of natural or aligned inflation, similar effects can arise from euclidean D-brane instantons beyond those corresponding to gauge instantons (dubbed exotic or stringy [23–25], see [26,27] for a review).”
Relaxion monodromy and the Weak Gravity Conjecture (2015, methodology): “(8)This can arise from non-perturbative gauge dynamics on D-branes to which the axion couples, or from euclidean D-brane instanton effects, see [67] for background.”
Explicit de Sitter flux vacua for global string models with chiral matter (2013, background): “Moreover, over the past decade various successful mechanisms, in particular in the context of type IIB string theory, have been established which allow to address moduli stabilisation and realistic D-brane model building [2].”
Double field theory: a pedagogical review (2013, unknown): “We refer the reader to the string theory books [3] and references therein for a more detailed and complete discussion of this issue.”
D-branes at del Pezzo singularities: global embedding and moduli stabilisation (2012, background): “ . . . . . . . . . . . . . 49 B.2 Results for the ﬁve moduli case . . . . . . . . . . . . . . . . . . . . . . . . . 50 C RG details 56 1 1 Introduction Realistic string model building is a major task [1] not that much because there is a very large number of string compactiﬁcations, but mostly becaus”
Non-Abelian discrete gauge symmetries in 4d string models (2012, background): “6 Magnetized branes and discrete flavour symmetries In this section we discuss the appearance of non-Abelian discrete symmetries in magnetized toroidal compactifications, focusing on magnetized D-brane systems, although similar conclusions hold for analogous heterotic models and T-dual intersecting ”