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Related papers: $U(1)$ gauge vector field on a codimension-2 brane

200 papers

We discuss possible actions for the d=2, N=(2,2) large vector multiplet that gauges isometries of generalized Kahler geometries. We explore two scenarios that allow us to write kinetic and superpotential terms for the scalar…

High Energy Physics - Theory · Physics 2008-08-12 Itai Ryb

We study fluctuations about axisymmetric warped brane solutions in 6D minimal gauged supergravity. Much of our analysis is general and could be applied to other scenarios. We focus on bulk sectors that could give rise to Standard Model…

High Energy Physics - Theory · Physics 2008-11-26 S. L. Parameswaran , S. Randjbar-Daemi , A. Salvio

We study scenarios where a scalar field has a spatially varying vacuum expectation value such that the total field variation is super-Planckian. We focus on the case where the scalar field controls the coupling of a U(1) gauge field, which…

High Energy Physics - Theory · Physics 2017-03-16 Daniel Klaewer , Eran Palti

We study the effect of spatially dependent mass functions over the solution of the Klein-Gordon equation in the (3+1)-dimensions for spinless bosonic particles where the mixed scalar-vector Coulomb-like field potentials and masses are…

Mathematical Physics · Physics 2009-06-09 Sameer M. Ikhdair

A three-parameter (positive odd integer $s$, thickness factor $\lambda$, and asymmetry factor $a$) family of asymmetric thick brane solutions in five dimensions were constructed from a two-parameter ($s$ and $\lambda$) family of symmetric…

High Energy Physics - Theory · Physics 2009-09-24 Yu-Xiao Liu , Chun-E Fu , Li Zhao , Yi-Shi Duan

The model of a domain wall ("thick" brane) in noncompact five-dimensional space-time is considered with geometries of $AdS_5$ type generated by self-interacting scalar matter. The scalar matter is composed of two fields with O(2) symmetric…

High Energy Physics - Theory · Physics 2015-06-11 Alexander A. Andrianov , Vladimir A. Andrianov , Oleg O. Novikov

It was shown recently that the lagrangian of the Grosse-Wulkenhaar model can be written as lagrangian of the scalar field propagating in a curved noncommutative space. In this interpretation, renormalizability of the model is related to the…

High Energy Physics - Theory · Physics 2014-11-20 Maja Buric , Harald Grosse , John Madore

In this paper we investigate the localization and mass spectra of matter fields with spin 0, 1 and 1/2 on a geometric thick brane generated by pure 4D and 5D positive cosmological constants without bulk scalar fields. This model possesses a…

High Energy Physics - Theory · Physics 2015-03-19 Heng Guo , Alfredo Herrera-Aguilar , Yu-Xiao Liu , Dagoberto Malagon-Morejon , Refugio Rigel Mora-Luna

In this paper, based on the theory of parametric resonance, we propose a cosmological criterion on ways of compactification: we rule out such a model of compactification that there exists a Kaluza-Klein mode satisfying $2m_{KK}=\omega_b$,…

General Relativity and Quantum Cosmology · Physics 2009-10-31 Yoshiyuki Morisawa , Kunihito Uzawa , Shinji Mukohyama

We have studied the U(1) gauge field theory with Villain (periodic Gaussian) action on spherelike lattices. The effective size of the systems studied ranges from 6 to 16. We do not observe any 2-state signal in the distribution function of…

High Energy Physics - Lattice · Physics 2009-10-28 C. B. Lang , P. Petreczky

A Randall-Sundrum-like braneworld scenario is constructed in a 5D extension of the Lorentz-violating massive gravity. The gauge hierarchy problem is solved in current model. The linear perturbations are calculated, and it is found that the…

High Energy Physics - Theory · Physics 2023-10-09 Ke Yang , Shi-Fa Guo , Bao-Min Gu

We discuss the phenomenology of $(1,1)$-mode adjoint scalars in the framework of two Universal Extra Dimensions. The Kaluza-Klein (KK) towers of these adjoint scalars arise in the 4-dimensional effective theory from the 6th component of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kirtiman Ghosh , Anindya Datta

The electroweak model is formulated on the nonlinearly realized gauge group SU(2) X U(1). This implies that in perturbation theory no Higgs field is present. The paper provides the effective action at the tree level, the Slavnov Taylor…

High Energy Physics - Phenomenology · Physics 2010-11-22 Daniele Bettinelli , Ruggero Ferrari , Andrea Quadri

Gauging the M-2-brane effective action with respect to an Abelian isometry in such a way that the invariance under gauge transformations of the 3-form potential is maintained (slightly modified) we obtain a fully covariant action with…

High Energy Physics - Theory · Physics 2009-10-30 Tomas Ortin

A Randall-Sundrum type brane-cosmological model in which slow-roll inflation on the brane is driven solely by a bulk scalar field was recently proposed by Himemoto and Sasaki. We analyze their model in detail and calculate the quantum…

General Relativity and Quantum Cosmology · Physics 2009-10-09 Norichika Sago , Yoshiaki Himemoto , Misao Sasaki

Recently bulk Randall-Sundrum theories with the gauge group $SU(2)_L \times SU(2)_R \times U(1)_{B-L}$ have drawn a lot of interest as an alternative to electroweak symmetry breaking mechanism. These models are in better agreement with…

High Energy Physics - Phenomenology · Physics 2009-11-11 Sanghyeon Chang , Seong Chan Park , Jeonghyeon Song

We develop the necessary ingredients for the construction of realistic models with warped universal extra dimensions. Our investigations are based on the seven dimensional (7D) spacetime AdS_5 x T^2 and we derive the Kaluza-Klein (KK)…

High Energy Physics - Phenomenology · Physics 2009-08-13 Kristian L. McDonald

We derive various solutions for the gauge field and the gaugino when there are both 5D bulk kinetic terms and 4D brane kinetic terms. Below the compactification scale $1/y_c$, gauge interaction by the massless mode is universal, independent…

High Energy Physics - Theory · Physics 2007-05-23 Bumseok Kyae

Covariant forms are given to a gauge theory of massive tensor field. This is accomplished by introducing another auxiliary field of scalar type to the system composed of a symmetric tensor field and an auxiliary field of vector type. The…

High Energy Physics - Theory · Physics 2009-10-30 Shinji Hamamoto

We derive a local, gauge invariant action for the SU(N) non-linear sigma-model in 2+1 dimensions. In this setting, the model is defined in terms of a self-interacting pseudo vector-field \theta_\mu, with values in the Lie algebra of the…

High Energy Physics - Theory · Physics 2010-12-01 C. D. Fosco , C. P. Constantinidis