Structural and dynamic origin of the boson peak in a Cu-Zr

Boson-fermion pairing in a boson-fermion environment A Storozhenko,1,2 P Schuck,1,3 T Suzuki,4 H Yabu,4 and J Dukelsky5 1Institut de Physique Nucléaire, IN2P3-CNRS, Université Paris-Sud, F-91406 Orsay Cédex, France

ElectroweakMonopole Productionat theLHC- a Snowmass WhitePaper

represents the Cho-Maison dyon, where Z = A − B and we have chosen f(0) = 1 and A(∞) = M W/2 but not the Dirac’s monopole It has the electric charge 4π/e, not 2π/e [2] Second, this monople naturally ad-mits a non-trivialdressing of weak bosons With the non-trivial dressing, the monopole becomes the Cho-Maison dyon

Finite Energy Electroweak Dyon - CERN

have the Cho-Maison monopole with A = B = 0 In general, with A0 6= 0, we nd the Cho-Maison dyon solution shown in Fig 1 [6] The solution looks very much like the well-known Prasad-Sommer eld solution of the Julia-Zee dyon But there is a crucial di erence The Cho-Maison dyon now has a non-trivial B − A, which represents the non-vanishing

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Structural and dynamic origin of the boson peak in a Cu-Zr

2Laboratoire de Physique et Modelisation des Milieux Condens´ ´es, UMR-CNRS 5493, Maison des Magist `eres, BP 166 CNRS, 38042 Grenoble-Cedex 09, France

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[PDF] Structural and dynamic origin of the boson peak in a Cu-Zr