3,995 research outputs found

    Isolating CP-violating \gamma ZZ coupling in e+e- \to \gamma Z with transverse beam polarizations

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    We revisit the process e+eγZe^+e^- \to \gamma Z at the ILC with transverse beam polarization in the presence of anomalous CP-violating γZZ\gamma Z Z coupling λ1\lambda_1 and γγZ\gamma \gamma Z coupling λ2\lambda_2. We point out that if the final-state spins are resolved, then it becomes possible to fingerprint the anomalous coupling {\rm Re}λ1\lambda_1.90% confidence level limit on {\rm Re}λ1\lambda_1 achievable at ILC with center-of-mass energy of 500 GeV or 800 GeV with realistic initial beam polarization and integrated luminosity is of the order of few times of 10210^{-2} when the helicity of ZZ is used and 10310^{-3} when the helicity of γ\gamma is used. The resulting corrections at quadratic order to the cross section and its influence on these limits are also evaluated and are shown to be small. The benefits of such polarization programmes at the ILC are compared and contrasted for the process at hand. We also discuss possible methods by which one can isolate events with a definite helicity for one of the final-state particles.Comment: 13 pages, 9 figures, using RevTex; v2 is a significantly revised version of v1, and corresponds to the version that has been published in Physical Review

    F and D Values with Explicit Flavor Symmetry Breaking and \Delta s Contents of Nucleons

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    We propose a new model for describing baryon semi-leptonic decays for estimating FF and DD values with explicit breaking effects of both SU(3) and SU(2) flavor symmetry, where all possible SU(3) and SU(2) breaking effects are induced from an effective interaction. An overall fit including the weak magnetism form factor yields F=0.477±0.001F=0.477\pm 0.001 and D=0.835±0.001D=0.835\pm 0.001 with χ2=4.43/5\chi^2=4.43/5 d.o.f. with Vud=0.975±0.002V_{ud}=0.975\pm 0.002 and Vus=0.221±0.002V_{us}=0.221\pm 0.002. The spin content of strange quarks Δs\Delta s is estimated from the obtained values FF and DD, and the nucleon spin problem is re-examined. Furthermore, the unmeasured values of (g1/f1)(g_1/f_1) and (g1)(g_1) for other hyperon semi-leptonic decays are predicted from this new formula.Comment: 15 pages, 1 figure, final version to appear in PR

    Fitting Precision Electroweak Data with Exotic Heavy Quarks

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    The 1999 precision electroweak data from LEP and SLC persist in showing some slight discrepancies from the assumed standard model, mostly regarding bb and cc quarks. We show how their mixing with exotic heavy quarks could result in a more consistent fit of all the data, including two unconventional interpretations of the top quark.Comment: 7 pages, no figure, 2 typos corrected, 1 reference update

    HERA prospects on Compositeness and New Vector Bosons

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    The absence of deviations from the Standard Model for the differential cross section dσ/dQ2{d\sigma}/{dQ^2} at HERA is used to set limits on electron quark compositeness scale and on new vector bosons, especially the hadrophilic one recently introduced as a possible explanation for LEP/SLC and CDF anomalies.Comment: Latex file, 7 pages and 1 ps fig, few comments on others experiments are added, results are unchanged. To appear in Phys. Let.

    Neutrino Masses and Leptogenesis with Heavy Higgs Triplets

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    A simple and economical extension of the minimal standard electroweak gauge model (without right-handed neutrinos) by the addition of two heavy Higgs scalar triplets would have two significant advantages. \underline {Naturally} small Majorana neutrino masses would become possible, as well as leptogenesis in the early universe which gets converted at the electroweak phase transition into the present observed baryon asymmetry.Comment: 12 pages including one figur

    Solutions to the R_b, R_c and alpha_s puzzles by Vector Fermions

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    We propose two minimal extensions of Standard Model, both of which can easily accommodate the recent puzzling observations about the excess in RbR_b, the deficit in RcR_c and the discrepancy in the low energy and high energy determinations of αs\alpha_{s}. Each model requires three additional heavy vectorial fermions in order to resolve the puzzles. The current phenomenological constraints and the new potential phenomena are also discussed.Comment: 12 pages, in LaTeX, postscript file also appear http://www.uic.edu/~keung/pub/rbrc.p

    Precise bounds on the Higgs boson mass

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    We study the renormalization group evolution of the Higgs quartic coupling λH\lambda_{H} and the Higgs mass mHm_{H} in the Standard Model. The one loop equation for λH\lambda_{H} is non linear and it is of the Riccati type which we numerically and analytically solve in the energy range [mt,EGU][m_{t},E_{GU}] where mtm_{t} is the mass of the top quark and EGU=1014E_{GU}=10^{14} GeV. We find that depending on the value of λH(mt)\lambda_{H}(m_{t}) the solution for λH(E)\lambda_{H}(E) may have singularities or zeros and become negative in the former energy range so the ultra violet cut off of the standard model should be below the energy where the zero or singularity of λH\lambda_{H} occurs. We find that for 0.369λH(mt)0.6130.369\leq\lambda_{H}(m_{t})\leq0.613 the Standard Model is valid in the whole range [mt,EGU][m_{t},E_{GU}]. We consider two cases of the Higgs mass relation to the parameters of the standard model: (a) the effective potential method and (b) the tree level mass relations. The limits for λH(mt)\lambda_{H}(m_{t}) correspond to the following Higgs mass relation 150mH193150\leq m_{H}\lessapprox 193 GeV. We also plot the dependence of the ultra violet cut off on the value of the Higgs mass. We analyze the evolution of the vacuum expectation value of the Higgs field and show that it depends on the value of the Higgs mass. The pattern of the energy behavior of the VEV is different for the cases (a) and (b). The behavior of λH(E)\lambda_{H}(E), mH(E)m_{H}(E) and v(E)v(E) indicates the existence of a phase transition in the standard model. For the effective potential this phase transition occurs at the mass range mH180m_{H}\approx 180 GeV and for the tree level mass relations at mH168m_{H}\approx 168 GeV.Comment: 14 pages, 7 figures. Expanded the discussion of the Higgs mass relation between the parameters of the Standard Model. Included the method of the Higgs effective potentia

    A study of the nuclear medium influence on transverse momentum of hadrons produced in deep inelastic neutrino scattering

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    The influence of nuclear effects on the transverse momentum (pT)(p_T) distributions of neutrinoproduced hadrons is investigated using the data obtained with SKAT propane-freon bubble chamber irradiated in the neutrino beam (with EνE_{\nu} = 3-30 GeV) at Serpukhov accelerator. Dependences of onthekinematicalvariablesofinclusivedeepinelasticscatteringandoftheproducedhadronsaremeasured.Ithasbeenobserved,thatthenucleareffectscauseanenhancementof on the kinematical variables of inclusive deep-inelastic scattering and of the produced hadrons are measured. It has been observed, that the nuclear effects cause an enhancement of of hadrons (more pronounced for the positively charged ones) produced in the target fragmentation region at low invariant mass of the hadronic system (2 <W<< W < 4 GeV) or at low energies transferred to the current quark (2 <ν<9< \nu < 9 GeV). At higher WW or ν\nu, no influence of nuclear effects on is observed. Measurement results are compared with predictions of a simple model, incorporating secondary intranuclear interactions of hadrons (with a formation length extracted from the Lund fragmentation model), which qualitatively reproduces the main features of the data.Comment: 23 pages, 7 figure
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