SUSY Quivers, Intersecting Branes and the Modest Hierarchy Problem
By D. Cremades, Luis E Ibáñez, F. Marchesano. 2002
147 citations recorded by the source corpus.
We present a class of chiral non-supersymmetric D = 4 field theories in which quadratic divergences appear only at two loops. They may be depicted as ``SUSY quivers'' in which the nodes represent a gauge group with extended e.g., N = 4 SUSY whereas links represent bifundamental matter fields which transform as chiral multiplets with respect to different N = 1 subgroups. One can obtain this type of field theories from simple D6-brane configurations on type IIA string theory compactified on a six-torus. We discuss the conditions under which this kind of structure is obtained from D6-brane intersections. We also discuss some aspects of the effective low-energy field theory. In particular we compute gauge couplings and Fayet-Iliopoulos terms from the Born-Infeld action and show how they match the field theory results. This class of theories may be of phenomenological interest in order to understand the modest hierarchy problem i.e., the stability of the hierarchy between the weak scale and a fundamental scale of order 10-100 TeV which appears e.g. in low string scale models. Specific D-brane models with the spectrum of the SUSY Standard Model and three generations are presented.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/52d784b68f7ce9ee1f3337ed54b9c3373bd6b6de
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Citations in the corpus
- Flux-induced soft supersymmetry breaking in chiral type IIB orientifolds with D3 / D7-branes (2004, background): “The piece VD represents D–term contributions to the scalar potential due to Fayet– Iliopolous terms. See Ref. [ 38 ] for further details.”
- Loop-corrected compactifications of the heterotic string with line bundles (2005, methodology): “A derivation of this equation via an FI term in an effective four-dimensional theory has been carried out in [51].”
- D‐branes in Standard Model building, gravity and cosmology (2003, background): “In addition, the issue of question (B), became acute: the theories are technically useless due to the instability induced by the hierarchy problem.”
- Chiral four-dimensional string compactifications with intersecting D-branes (2003, unknown): “compactifications of type IIA theory with D6-branes wrapped on intersecting 3-cycles, extensively studied in the last two years [1, 2, 3, 4, 5 , 7, 8, 9] 1 . The discussion is organized”
- Exact standard model structures from intersecting D5-branes (2002, background): “For additional non-SUSY constructions and recent developments in the context of intersecting branes, see [18, 19, 20, 21, 22, 23, 24, 25, 26, 27, 28].”
- TOWARD REALISTIC INTERSECTING D-BRANE MODELS (2005, methodology): “For a supersymmetric three-cycle, πa, the tree level gauge kinetic function is a holomorphic function of complex structure moduli fields and it is of the form [55, 41, 136]”
- Yukawa couplings in intersecting D-brane models (2003, background): “Consideration of such possibilities lead to the idea of Quasi-Supersymmetry in [11, 12] (see [45] for related work).”
- Chiral D-brane Models with Frozen Open String Moduli (2005, background): “Any deviation from these particular points in the Kähler moduli space will be seen, in the D-brane effective theory, as a non-vanishing FI-term [96,97].”
- Gauge threshold corrections in intersecting brane world models (2003, background): “In the presentpaperwe turn to the question ofcom puting one{loop gauge threshold corrections in intersecting brane world m odels, which is also very im portant from the phenom enologicalpointofview.”
- Intersecting Brane Models of Particle Physics and the Higgs Mechanism (2002, methodology): “This may be of interest when dealing with scenarios where the fundamental scale of physics is two or three orders of magnitude above the electroweak scale [15].”
- Computing Yukawa couplings from magnetized extra dimensions (2004, unknown): “Indeed, as seen in [22], it pairs with RR-field to form the complex scalar of an N = 1 chiral multiplet.”
- Getting just the supersymmetric standard model at intersecting branes on the Z(6) orientifold (2004, background): “ng rise to Pati-Salam-Models, and leading to non-flat and non-factorizable branes which give up the complete predictability of the worldsheet CFT approach. Another possibility are the constructions of [39,40], where only the sectors between certain branes are locally N= 1-supersymmetric (Q-SUSY theor”
- Building MSSM flux vacua (2004, background): “A small deviation from this condition can be understood as a non-vanishing FI-term in the D = 4 effective theory [40,49].”