792 research outputs found

    Summary of Spin Physics Parallel Sessions

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    We summarize the activities in the spin physics parallel sessions of the 8th8^{\rm th} conference on intersections between particle and nuclear physics.Comment: Latex, 5 pages, to appear in the Proceedings of the 8th Conference on Intersections between Particle and Nuclear Physics (CIPANP 2003

    Spin dependent fragmentation function at Belle

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    The measurement of the so far unknown chiral-odd quark transverse spin distribution in either semi-inclusive DIS (SIDIS) or inclusive measurements in pp collisions at RHIC has an additional chiral-odd fragmentation function appearing in the cross section. These chiral-odd fragmentation functions (FF) can for example be the so-called Collins FF or the Interference FF. HERMES has given a first hint that these FFs are nonzero, however in order to measure the transversity one needs these FFs to be precisely known. We have used 29.0 fb1^{-1} of data collected by the Belle experiment at the KEKB e+ee^+e^- collider to measure azimuthal asymmetries for different charge combinations of pion pairs and thus access the Collins FF.Comment: Results presented at the DIS 2006 conference in Tsukuba, Japa

    Spin dependent fragmentation functions at Belle

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    The Belle detector at the KEKB e+e− collider provides large amounts of statistics to study the fragmentation of light quarks into final state hadrons. In addition to unpolarized fragmentation functions also spin dependent fragmentation can be studied. Belle has successfully extracted asymmetries related to the Collins and interference fagmentation functions for charged pions

    Sivers effect in Drell Yan at RHIC

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    On the basis of a fit to the Sivers effect in deep-inelastic scattering, we make predictions for single-spin asymmetries in the Drell-Yan process at RHIC.Comment: 10 pages, 7 figures, 1 table. v2: References and comments added, minor correction

    Three loop anomalous dimension of the second moment of the transversity operator in the MSbar and RI' schemes

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    We compute the anomalous dimension of the second moment of the transversity operator, \bar{\psi} \sigma^{\mu\nu} D^\rho \psi, at three loops in both the MSbar and RI' schemes. As a check on the result we also determine the O(1/N_f) critical exponent of the n-th moment of the transversity operator in d-dimensions in the large N_f expansion and determine leading order information on the n dependence of the anomalous dimension at three and four loops in MSbar. In addition the RI' anomalous dimension of the non-singlet twist-2 operator, \bar{\psi} \gamma^\mu D^\nu \psi, is also determined.Comment: 18 latex pages; additional reference include

    Test of CPT and Lorentz invariance from muonium spectroscopy

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    Following a suggestion of Kostelecky et al. we have evaluated a test of CPT and Lorentz invariance from the microwave spectroscopy of muonium. Hamiltonian terms beyond the standard model violating CPT and Lorentz invariance would contribute frequency shifts δν12\delta\nu_{12} and δν34\delta\nu_{34} to ν12\nu_{12} and ν34\nu_{34}, the two transitions involving muon spin flip, which were precisely measured in ground state muonium in a strong magnetic field of 1.7 T. The shifts would be indicated by anti-correlated oscillations in ν12\nu_{12} and ν34\nu_{34} at the earth's sidereal frequency. No time dependence was found in ν12\nu_{12} or ν34\nu_{34} at the level of 20 Hz, limiting the size of some CPT and Lorentz violating parameters at the level of 2×10232\times10^{-23} GeV, representing Planck scale sensitivity and an order of magnitude improvement in sensitivity over previous limits for the muon.Comment: 4 pages, 4 figures, uses REVTeX and epsf, submitted to Phys. Rev. Let

    A Hadron Blind Detector for the PHENIX Experiment

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    A novel Hadron Blind Detector (HBD) has been developed for an upgrade of the PHENIX experiment at RHIC. The HBD will allow a precise measurement of electron-positron pairs from the decay of the light vector mesons and the low-mass pair continuum in heavy-ion collisions. The detector consists of a 50 cm long radiator filled with pure CF4 and directly coupled in a windowless configuration to a triple Gas Electron Multiplier (GEM) detector with a CsI photocathode evaporated on the top face of the first GEM foil.Comment: 4 pages, 3 figures, Quark Matter 2005 conference proceeding
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