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A holomorphic triple over a compact Riemann surface consists of two holomorphic vector bundles and a holomorphic map between them. After fixing the topological types of the bundles and a real parameter, there exist moduli spaces of stable…

Algebraic Geometry · Mathematics 2016-09-07 Steven B. Bradlow , Oscar Garcia-Prada , Peter B. Gothen

We construct five families of two-dimensional moduli spaces of parabolic Higgs bundles (respectively local systems) by taking the equivariant Hilbert scheme of a certain finite group acting on the cotangent bundle of an elliptic curve. We…

Algebraic Geometry · Mathematics 2012-06-26 Michael Groechenig

We report on a calculation of Higgs-boson contributions to the decays B_s -> l^+l^- and B -> K l^+l^- (l=e, mu) which are governed by the effective Hamiltonian describing b -> s l^+ l^-. Compact formulae for the Wilson coefficients are…

High Energy Physics - Phenomenology · Physics 2011-03-23 C. Bobeth , T. Ewerth , F. Krüger , J. Urban

The non-perturbative superpotential generated by a heterotic superstring wrapped once around a genus-zero holomorphic curve is proportional to the Pfaffian involving the determinant of a Dirac operator on this curve. We show that the space…

High Energy Physics - Theory · Physics 2014-11-18 Evgeny I. Buchbinder , Ron Donagi , Burt A. Ovrut

It is pointed out (not for the first time) that the minimal Standard Model, without additional gauge-singlet right-handed neutrinos or isotriplet Higgs fields, allows for nonvanishing neutrino masses and mixing. The required interaction…

High Energy Physics - Phenomenology · Physics 2013-02-01 F. R. Klinkhamer

Providing an Ultra-Violet completion valid up to the Planck scale is of paramount importance to validate the composite Higgs paradigm, at par with supersymmetry. We propose the first complete and feasible framework, based on partial…

High Energy Physics - Phenomenology · Physics 2019-11-14 Giacomo Cacciapaglia , Shahram Vatani , Chen Zhang

The electroweak symmetry is nonlinearly realized in an extension of the minimal supersymmetric standard model (MSSM) through an additional pair of constrained Higgs doublet superfields. The superpotential couplings of this constrained Higgs…

High Energy Physics - Phenomenology · Physics 2015-05-28 T. E. Clark , S. T. Love , T. ter Veldhuis

In this talk we discuss a few relevant aspects of heterotic M-theory. These are the stabilization of the two relevant moduli (the length of the eleventh segment (pi rho) and the volume of the internal six manifold (V)) in models where…

High Energy Physics - Phenomenology · Physics 2016-11-03 T. Barreiro , B. de Carlos

We study the sub-structure of the heterotic Kahler moduli space due to the presence of non-Abelian internal gauge fields from the perspective of the four-dimensional effective theory. Internal gauge fields can be supersymmetric in some…

High Energy Physics - Theory · Physics 2009-09-28 Lara B. Anderson , James Gray , Andre Lukas , Burt Ovrut

On a complex curve, we establish a correspondence between integrable connections with irregular singularities, and Higgs bundles such that the Higgs field is meromorphic with poles of any order. The moduli spaces of these objects are…

Differential Geometry · Mathematics 2007-05-23 Olivier Biquard , Philip Boalch

An explicit orbifold example of the non-zero correlation functions related to the additional contribution to the induced mass term for Higgs particles at low energies is given. We verify that they form finite dimensional representations of…

High Energy Physics - Theory · Physics 2015-06-26 D. Erdenebayar

A search for a standard model Higgs boson produced in association with a top-quark pair and decaying to bottom quarks is presented. Events with hadronic jets and one or two oppositely charged leptons are selected from a data sample…

High Energy Physics - Experiment · Physics 2015-06-16 CMS Collaboration

In these lectures we present a brief review of the Higgs boson sector in the ``Standard Model'', and its Minimal Supersymmetric Extension, with particular emphasis on the main mechanisms for Higgs production and decay at LEP2 and LHC, and…

High Energy Physics - Phenomenology · Physics 2016-09-06 M. Quiros

Heisenberg modules over noncommutative tori may also be viewed as Gabor frames. Building on this fact, we relate to deformations of noncommutative tori a bundle of Banach spaces induced by Heisenberg modules. The construction of this bundle…

Operator Algebras · Mathematics 2025-06-12 Malte Gerhold , Arvin Lamando , Franz Luef

The minimal supersymmetric standard model involves a rather restrictive Higgs potential with two Higgs fields. Recently, the full set of classes of symmetries allowed in the most general two Higgs doublet model was identified; these classes…

High Energy Physics - Phenomenology · Physics 2014-11-20 P. M. Ferreira , Howard E. Haber , Joao P. Silva

We propose a supersymmetric extension of the standard model which is a realistic alternative to the MSSM, and which has several advantages. No ``mu'' supersymmetric Higgs/Higgsino mass parameter is needed for sufficiently heavy charginos.…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ann E. Nelson , Nuria Rius , Veronica Sanz , Mithat Unsal

It is argued that the dual transformation of non-Abelian monopoles occurring in a system with gauge symmetry breaking G -> H is to be defined by setting the low-energy H system in Higgs phase, so that the dual system is in confinement…

High Energy Physics - Theory · Physics 2008-11-26 Minoru Eto , Luca Ferretti , Kenichi Konishi , Giacomo Marmorini , Muneto Nitta , Keisuke Ohashi , Walter Vinci , Naoto Yokoi

We present a new mechanism to generate large $A$-terms at tree-level in the MSSM through the use of superpotential operators. The mechanism trivially resolves the $A/m^2$ problem which plagues models with conventional, loop-induced…

High Energy Physics - Phenomenology · Physics 2015-01-07 Aria Basirnia , Daniel Egana-Ugrinovic , Simon Knapen , David Shih

The Hidden Abelian Higgs Model (HAHM) is an extension of the Standard Model based on the gauge group $G =SU(3)_{C} \times SU(2)_{L} \times U(1)_{Y} \times U(1)_{X}$ i.e. an extra $U(1)_{X}$ gauge group in addition to the SM gauge groups.In…

High Energy Physics - Phenomenology · Physics 2015-07-10 Nady Bakhet , Maxim Yu. Khlopov , Tarek Hussein

We explore the phenomenology of virtual spin-1 contributions to the h to gamma gamma and h to Z gamma decay rates in gauge extensions of the standard model. We consider generic lorentz and gauge invariant vector self-interactions, which can…

High Energy Physics - Phenomenology · Physics 2014-03-05 Don Bunk , Jay Hubisz , Bithika Jain