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The flux of neutrino-induced muons has been measured with the MACRO detector. Different event topologies have been detected, due to neutrino interactions in the apparatus and in the rock below it. The upward-throughgoing muon sample is the…

High Energy Physics - Experiment · Physics 2007-05-23 Paolo Bernardini

The screening of magnetic Z(N)-monopoles and the associated screening length in SU(N) gauge theories are analyzed theoretically, and computed numerically in the 3d SU(2) theory. The nature of the screening excitations as well as their mass…

High Energy Physics - Phenomenology · Physics 2009-11-11 Ph. de Forcrand , C. Korthals-Altes , O. Philipsen

M-theory compactified on a $G_2$ manifold with resolved $E_8$ singularities realizes 4d $\mathcal{N} = 1$ supersymmetric gauge theories coupled to gravity with three families of Standard Model fermions. Beginning with one $E_8$ singularity,…

High Energy Physics - Theory · Physics 2021-07-28 Eric Gonzalez , Gordon Kane , Khoa Dang Nguyen , Malcolm J. Perry

Interactions with neutrons and protons play a crucial role for the neutrino opacity of matter in the supernova core. Their current implementation in many simulation codes, however, is rather schematic and ignores not only modifications for…

Solar and Stellar Astrophysics · Physics 2015-08-12 Tobias Melson , Hans-Thomas Janka , Robert Bollig , Florian Hanke , Andreas Marek , Bernhard Mueller

The Daya Bay, Double Chooz and RENO experiments recently observed a significant distortion in their detected reactor antineutrino spectra, being at odds with the current predictions. Although such a result suggests to revisit the current…

High Energy Physics - Experiment · Physics 2017-09-01 G. Mention , M. Vivier , J. Gaffiot , T. Lasserre , A. Letourneau , T. Materna

SU(N_c) Yang-Mills theory is investigated at finite densities of N_f heavy quark flavors. The calculation of the (continuum) quark determinant in the large-mass limit is performed by analytic methods and results in an effective gluonic…

High Energy Physics - Lattice · Physics 2009-10-31 Kurt Langfeld , Gwansoo Shin

We discuss the physics of four-dimensional compact U(1) lattice gauge theory from the point of view of softly broken N=2 supersymmetric SU(2) Yang-Mills theory. We provide arguments in favor of (pseudo-)critical mass exponents 1/3, 5/11 and…

High Energy Physics - Theory · Physics 2009-10-30 Jan Ambjorn , Domenec Espriu , Naoki Sasakura

I propose the first multiscalar singlet extension of the Standard Model (SM), that generates tree level top quark and exotic fermion masses as well as one and three loop level masses for charged fermions lighter than the top quark and for…

High Energy Physics - Phenomenology · Physics 2016-09-06 A. E. Cárcamo Hernández

Double- and single-differential cross sections for inclusive charged-current neutrino-nucleus scattering are reported for the kinematic domain 0 to 2 GeV/c in three-momentum transfer and 0 to 2 GeV in available energy, at a mean…

High Energy Physics - Experiment · Physics 2025-03-21 M. A. Acero , B. Acharya , P. Adamson , L. Aliaga , N. Anfimov , A. Antoshkin , E. Arrieta-Diaz , L. Asquith , A. Aurisano , A. Back , N. Balashov , P. Baldi , B. A. Bambah , E. Bannister , A. Barros , S. Bashar , A. Bat , K. Bays , R. Bernstein , T. J. C. Bezerra , V. Bhatnagar , D. Bhattarai , B. Bhuyan , J. Bian , A. C. Booth , R. Bowles , B. Brahma , C. Bromberg , N. Buchanan , A. Butkevich , S. Calvez , T. J. Carroll , E. Catano-Mur , J. P. Cesar , A. Chatla , R. Chirco , B. C. Choudhary , A. Christensen , M. F. Cicala , T. E. Coan , A. Cooleybeck , C. Cortes-Parra , D. Coveyou , L. Cremonesi , G. S. Davies , P. F. Derwent , P. Ding , Z. Djurcic , K. Dobbs , M. Dolce , D. Doyle , D. Duenas Tonguino , E. C. Dukes , A. Dye , R. Ehrlich , E. Ewart , P. Filip , M. J. Frank , H. R. Gallagher , F. Gao , A. Giri , R. A. Gomes , M. C. Goodman , M. Groh , R. Group , A. Habig , F. Hakl , J. Hartnell , R. Hatcher , M. He , K. Heller , V Hewes , A. Himmel , T. Horoho , Y. Ivaneev , A. Ivanova , B. Jargowsky , J. Jarosz , C. Johnson , M. Judah , I. Kakorin , D. M. Kaplan , A. Kalitkina , B. Kirezli-Ozdemir , J. Kleykamp , O. Klimov , L. W. Koerner , L. Kolupaeva , R. Kralik , A. Kumar , C. D. Kuruppu , V. Kus , T. Lackey , K. Lang , J. Lesmeister , A. Lister , J. Liu , J. A. Lock , M. Lokajicek , M. MacMahon , S. Magill , W. A. Mann , M. T. Manoharan , M. Manrique Plata , M. L. Marshak , M. Martinez-Casales , V. Matveev , B. Mehta , M. D. Messier , H. Meyer , T. Miao , W. H. Miller , S. Mishra , S. R. Mishra , R. Mohanta , A. Moren , A. Morozova , W. Mu , L. Mualem , M. Muether , K. Mulder , D. Myers , D. Naples , A. Nath , S. Nelleri , J. K. Nelson , R. Nichol , E. Niner , A. Norman , A. Norrick , T. Nosek , H. Oh , A. Olshevskiy , T. Olson , M. Ozkaynak , A. Pal , J. Paley , L. Panda , R. B. Patterson , G. Pawloski , R. Petti , R. K. Plunkett , L. R. Prais , M. Rabelhofer , A. Rafique , V. Raj , M. Rajaoalisoa , B. Ramson , B. Rebel , P. Roy , O. Samoylov , M. C. Sanchez , S. Sanchez Falero , P. Shanahan , P. Sharma , A. Sheshukov , Shivam , A. Shmakov , W. Shorrock , S. Shukla , D. K. Singha , I. Singh , P. Singh , V. Singh , E. Smith , J. Smolik , P. Snopok , N. Solomey , A. Sousa , K. Soustruznik , M. Strait , L. Suter , A. Sutton , K. Sutton , S. Swain , C. Sweeney , A. Sztuc , B. Tapia Oregui , P. Tas , T. Thakore , J. Thomas , E. Tiras , Y. Torun , D. Tran , J. Trokan-Tenorio , J. Urheim , P. Vahle , Z. Vallari , J. D. Villamil , K. J. Vockerodt , M. Wallbank , M. Wetstein , D. Whittington , D. A. Wickremasinghe , T. Wieber , J. Wolcott , M. Wrobel , S. Wu , W. Wu , Y. Xiao , B. Yaeggy , A. Yahaya , A. Yankelevich , K. Yonehara , Y. Yu , S. Zadorozhnyy , J. Zalesak , R. Zwaska

The confinement problem has been solved in the anisotropic (2+1)-dimensional SU(N) Yang-Mills theory at weak coupling. In this paper, we find the low-lying spectrum for N=2. The lightest excitations are pairs of fundamental particles of the…

High Energy Physics - Theory · Physics 2008-11-26 Peter Orland

We consider the neutrino physics of models with a sequentially broken U(2) flavor symmetry. Such theories yield the observed pattern of quark and lepton masses, while maintaining sufficient degeneracies between superparticles of the first…

High Energy Physics - Phenomenology · Physics 2014-11-17 Christopher D. Carone , Lawrence J. Hall

The high-temperature phase of SU(2) Yang-Mills theory is addressed by means of dimensional reduction with a special emphasis on the properties of center vortices. For this purpose, the vortex vacuum which arises from center projection is…

High Energy Physics - Lattice · Physics 2009-10-31 J. Gattnar , K. Langfeld , A. Schafke , H. Reinhardt

We have identified low-energy magnetic excitations in a doped quantum critical system by means of polarized neutron scattering experiments. The presence of these excitations could explain why Ce(Fe$_{0.76}$Ru$_{0.24}$)$_2$Ge$_2$ displays…

Strongly Correlated Electrons · Physics 2016-10-06 Tom Heitmann , Jagat Lamsal , Shannon Watson , Ross Erwin , Wangchun Chen , Yang Zhao , Wouter Montfrooij

In the present work we analyse $\mathcal{N}=(2,2)$ supersymmetric Yang-Mills (SYM) theory in two dimensions by means of lattice simulations. The theory arises as dimensional reduction of $\mathcal{N}=1$ SYM theory in four dimensions. As in…

High Energy Physics - Lattice · Physics 2019-03-19 D. August , M. Steinhauser , B. H. Wellegehausen , A. Wipf

If there exist only three light neutrinos below the weak scale, the neutrino masses can arise by breaking the lepton number L. One example is the Zee mechanism for the neutrino masses. We study phenomenological implications of neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jihn E. Kim , Jae Sik Lee

Intermediate valence compounds containing rare earth or actinide ions are archetypal systems for the investigation of strong electron correlations. Their effective electron masses of 10 to 50 times the free electron mass result from a…

We consider the possibility that the quark condensate formed by QCD confinement generates Majorana neutrino masses m_\nu via dimension seven operators. No degrees of freedom beyond the Standard Model are necessary, below the electroweak…

High Energy Physics - Phenomenology · Physics 2011-02-01 Hooman Davoudiasl , Lisa L. Everett

We conjecture that neutrino physics might correspond to the spontaneous magnetisation phase of an Ising-like spin model interaction coupled to neutrino chirality which operates at scales close to the Planck mass. We argue that this scenario…

High Energy Physics - Phenomenology · Physics 2007-05-23 Steven D. Bass

This final article about the CHOOZ experiment presents a complete description of the electron antineutrino source and detector, the calibration methods and stability checks, the event reconstruction procedures and the Monte Carlo…

In this work we propose a renormalizable model based on the $SU(5)$ gauge group where neutrino mass originates at the two-loop level without extending the fermionic content of the Standard Model (SM). Unlike the conventional $SU(5)$ models,…

High Energy Physics - Phenomenology · Physics 2019-06-19 Shaikh Saad