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Starting from the previously constructed effective supergravity theory below the scale of U(1) breaking in orbifold compactifications of the weakly coupled heterotic string, we study the effective theory below the scale of supersymmetry…

High Energy Physics - Theory · Physics 2014-11-18 Mary K. Gaillard , Joel Giedt , Aleksey L. Mints

Type II string compactifications to 4d generically contain massless Ramond-Ramond U(1) gauge symmetries. However there is no massless matter charged under these U(1)'s, which makes a priori difficult to measure any physical consequences of…

High Energy Physics - Theory · Physics 2015-05-28 Pablo G. Camara , Luis E. Ibañez , Fernando Marchesano

We investigate orbifold compactifications of the heterotic string, addressing in detail their construction, classification and phenomenological potential. We present a strategy to search for models resembling the minimal supersymmetric…

High Energy Physics - Theory · Physics 2010-04-30 Saul Ramos-Sanchez

Flavor physics may help us understand theories beyond the standard model. In the context of supersymmetry, if we can measure the masses and mixings of sleptons and squarks, we may learn something about supersymmetry and supersymmetry…

High Energy Physics - Phenomenology · Physics 2014-11-20 Jonathan L. Feng , Sky T. French , Iftah Galon , Christopher G. Lester , Yosef Nir , Yael Shadmi , David Sanford , Felix Yu

The detection of pairs of sleptons, charginos and charged higgs bosons produced via photon-photon fusion at the LHC is studied, assuming a couple of benchmark points of the MSSM model. Due to low cross sections, it requires large integrated…

High Energy Physics - Phenomenology · Physics 2008-12-18 N. Schul , K. Piotrzkowski

In recent years it has been realized that in string/$M$ theories compactified to four dimensions which satisfy cosmological constraints, it is possible to make some generic predictions for particle physics and dark matter: a non-thermal…

High Energy Physics - Phenomenology · Physics 2012-05-25 Bobby Samir Acharya , Gordon Kane , Piyush Kumar

By including the effects of superstring thresholds, we reconsider minimal string unification together with the requirement of producing a supersymmetry-breaking gluino condensate in the hidden sector. This gives, for examples of…

High Energy Physics - Phenomenology · Physics 2008-02-03 Paul H. Frampton , Bettina Keszthelyi , Brian D. Wright , Thomas W. Kephart

If nature is described by string theory, and if the compactification radius is large (as suggested by the unification of couplings), then the theory is in a regime best described by the low energy limit of $M$-theory. We discuss some…

High Energy Physics - Theory · Physics 2009-10-30 Tom Banks , Michael Dine

Non-linearly realized supersymmetry, combined with the Standard Model field content and SU(3)XSU(2)XU(1) gauge invariance, permits local dimension-six operators involving a goldstino, a lepton doublet and a Higgs doublet. These interactions…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ignatios Antoniadis , Marc Tuckmantel , Fabio Zwirner

A bubble of nothing is a spacetime instability where a compact dimension collapses. After nucleation, it expands at the speed of light, leaving "nothing" behind. We argue that the topological and dynamical mechanisms which could protect a…

High Energy Physics - Theory · Physics 2020-05-15 Iñaki García Etxebarria , Miguel Montero , Kepa Sousa , Irene Valenzuela

In this thesis we discuss non-perturbative phenomena emerging in gauge and in string/supergravity theories. We compute the partition function of 5D minimal supersymmetric U(1) gauge theory with extra adjoint matter in general…

High Energy Physics - Theory · Physics 2011-02-08 Marine Samsonyan

In extended supersymmetric models with a hidden sector the lightest $R$-parity odd particle can reside in the hidden sector and act as dark matter. We consider the case when the hidden sector has ultraweak interactions with the visible…

High Energy Physics - Phenomenology · Physics 2020-02-25 Amin Aboubrahim , Wan-Zhe Feng , Pran Nath

We examine supersymmetric theories with approximately conformal sectors. Without an IR cutoff the theory has a continuum of modes, which are often referred to as "unparticles." Making use of the AdS/CFT correspondence we find that in the…

High Energy Physics - Phenomenology · Physics 2009-12-31 Haiying Cai , Hsin-Chia Cheng , Anibal D. Medina , John Terning

If $R$-parity is not conserved, the lightest supersymmetric particle (LSP) could decay via lepton number violating or baryon number violating interactions. The latter case is particularly insidious since it leads to a reduction of the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Howard Baer , Chih-hao Chen , Xerxes Tata

Strongly coupled heterotic $E_8\times E_8$ string theory, compactified to four dimensions on a large Calabi-Yau manifold ${\bf X}$, may represent a viable candidate for the description of low-energy particle phenomenology. In this regime,…

High Energy Physics - Theory · Physics 2009-10-30 Petr Horava

The presence of a hidden sector with very weak interactions with the standard model has significant implications on LHC signatures. In this work we discuss LHC phenomenology with the inclusion of a hidden sector by a $U(1)$ extension of…

High Energy Physics - Phenomenology · Physics 2019-09-20 Amin Aboubrahim , Pran Nath

We show that quantum systems of extended objects naturally give rise to a large class of exotic phases - namely topological phases. These phases occur when the extended objects, called ``string-nets'', become highly fluctuating and…

Strongly Correlated Electrons · Physics 2009-11-10 Michael A. Levin , Xiao-Gang Wen

Supersymmetric collider phenomenology depends crucially on whether the lightest observable-sector supersymmetric particle (LOSP) decays, and if so, what the LOSP decay products are. For instance, in SUSY models where the gravitino is…

High Energy Physics - Phenomenology · Physics 2022-09-09 Jesse Thaler , Zoe Thomas

We investigate supersymmetric models where neither R-parity nor lepton number nor baryon number is imposed. The full high energy theory has an exact horizontal U(1) symmetry that is spontaneously broken. Quarks and Higgs fields carry…

High Energy Physics - Phenomenology · Physics 2014-11-17 Galit Eyal , Yosef Nir

The first part of this talk presents the general complexion of baryon and lepton number non-conservation that may arise in the context of quark-lepton unification. The second part presents the status of grand unification with and without…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jogesh C. Pati