4,122 research outputs found

    CP Violating Observables in e−e+→W−W+e^-e^+ \to W^-W^+

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    We consider various integrated lepton charge-energy asymmetries and azimuthal asymmetries as tests of CP violation in the process e−e+→W−W+e^-e^+ \to W^-W^+. These asymmetries are sensitive to different linear combinations of the CP violating form factors in the three gauge boson W−W+W^-W^+ production vertex, and can distinguish dispersive and absorptive parts of the form factors. It makes use of purely hadronic and purely leptonic modes of WW's decays as well as the mixed modes. The techniques of using the kinematics of jets or missing momentum to construct CP--odd observables are also employed. These CP violating observables are illustrated in the generalized Left-Right Model and the Charged Higgs Model.Comment: 23 pages, plus 11 postscript graphs not posted befor

    CP violation in top pair production at an e^+e^- collider

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    We investigate a possible CP violating effect in e+e−e^+e^- annihilation into ttˉt\bar t top quark pairs. As an illustrative example, we assume the source of the CP nonconservation is in the Yukawa couplings of a neutral Higgs boson which contain both scalar and pseudoscalar pieces. One of the interesting observable effects is the difference in production rates between the two CP conjugate polarized ttˉt\bar t states.Comment: 9 pages, 3 postscript figures not included but availabel upon request, CERN-TH.6658/9

    Dispersion relations for stationary light in one-dimensional atomic ensembles

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    We investigate the dispersion relations for light coupled to one-dimensional ensembles of atoms with different level schemes. The unifying feature of all the considered setups is that the forward and backward propagating quantum fields are coupled by the applied classical drives such that the group velocity can vanish in an effect known as "stationary light". We derive the dispersion relations for all the considered schemes, highlighting the important differences between them. Furthermore, we show that additional control of stationary light can be obtained by treating atoms as discrete scatterers and placing them at well defined positions. For the latter purpose, a multi-mode transfer matrix theory for light is developed
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