Abstract:We study the production of charginos e + e − →χ + iχ − j , (i, j = 1, 2) with polarized beams and the subsequent decaysχ. . , 4), including the complete spin correlations between production and decay. Analytical formulae are presented for the joint spin-density matrix of the charginos, for the chargino decay matrix and for the differential cross section of the combined processes of production and decays. We present numerical results for pair production of the lighter chargino with unpolarized beams and the lep… Show more
“…. 4, at a linear collider with polarised beams with subsequent leptonic tree-body decaysχ [31]. Since observables like decay angular distributions and T-odd triple product correlations depend on the polarisation of the decaying neutralinos [32] the full spin correlations between production and decay are included.…”
Section: Supersymmetrymentioning
confidence: 99%
“…Since observables like decay angular distributions and T-odd triple product correlations depend on the polarisation of the decaying neutralinos [32] the full spin correlations between production and decay are included. In [31] the complete analytical formulae for longitudinal polarised beams are given, including complex couplings to allow the study of CP violating phenomena. In figure 5 in the scenario SPS1a [33] for unpolarised beams (solid) and beam polarisations P e − = −0.8, P e + = +0.6 (dashed), P e − = +0.8, P e + = −0.6 (dotted).…”
Abstract. We review some recent studies about the parameter determination of top quarks, W bosons, Higgs bosons, supersymmetric particles and in the ADD model of extra dimensions at a linear collider.
“…. 4, at a linear collider with polarised beams with subsequent leptonic tree-body decaysχ [31]. Since observables like decay angular distributions and T-odd triple product correlations depend on the polarisation of the decaying neutralinos [32] the full spin correlations between production and decay are included.…”
Section: Supersymmetrymentioning
confidence: 99%
“…Since observables like decay angular distributions and T-odd triple product correlations depend on the polarisation of the decaying neutralinos [32] the full spin correlations between production and decay are included. In [31] the complete analytical formulae for longitudinal polarised beams are given, including complex couplings to allow the study of CP violating phenomena. In figure 5 in the scenario SPS1a [33] for unpolarised beams (solid) and beam polarisations P e − = −0.8, P e + = +0.6 (dashed), P e − = +0.8, P e + = −0.6 (dotted).…”
Abstract. We review some recent studies about the parameter determination of top quarks, W bosons, Higgs bosons, supersymmetric particles and in the ADD model of extra dimensions at a linear collider.
“…with complete spin correlations are calculated using the same formalism as in [3] for e + e − -annihilation.…”
Section: Definitions and Formalismmentioning
confidence: 99%
“…2) are given in [3,4]. They depend on the gaugino mass parameters M 1 , M 2 , the higgsino mass parameter µ, the ratio tan β of the vacuum expectation values of the neutral Higgs fields and the left selectron and the sneutrino mass.…”
Section: Helicity Amplitudes and Cross Sectionsmentioning
confidence: 99%
“…The analytical formulae for the quantities P αβ , Σ a P,αβ , Σ ′b P,αβ and Σ ab P,αβ are given in the next section. Analytical expressions for the decay matrices for the leptonic decays (2) and (3) can be found in [3,4].…”
Section: Helicity Amplitudes and Cross Sectionsmentioning
We discuss the pair production of charginos in collisions of polarized photons γγ →χ + νe including the complete spin correlations. Analytical formulae are given for the polarization and the spin-spin correlations of the charginos. Since the production is a pure QED process the decay dynamics can be studied separately. For high energy photons from Compton backscattering of polarized laser pulses off polarized electron beams numerical results are presented for the cross section, the angular distribution and the forward-backward asymmetry of the decay positron. Finally we study the dependence on the gaugino mass parameter M1 and on the sneutrino mass for a gaugino-like MSSM scenario.
The physics potential is briefly summarized for an e + e − linear collider operating at center-of-mass energies up to √ s = 1 TeV and delivering integrated luminosities up to L = 0.5 ab −1 in one to two years. This machine will allow us to perform precision studies of the top quark and the electroweak gauge bosons at the per-mille level. It will be an ideal instrument to investigate the properties of the Higgs boson and to establish essential elements of the Higgs mechanism as the fundamental mechanism for breaking the electroweak symmetries. In the area beyond the Standard Model, new particles and their interactions can be discovered and explored comprehensively. In supersymmetric theories, the mechanism of the symmetry breaking can be investigated experimentally and the underlying unified theory can be reconstructed. The high precision allows stable extrapolations up to scales near the Planck mass.
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