78 research outputs found

    1+1^{-+} exotic meson at light quark masses

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    The mass of the 1+1^{-+} exotic meson, created with hybrid interpolating fields, is explored at light quark masses approaching 25 MeV (mπ/mρ1/3m_\pi / m_\rho \simeq 1/3). Access to such light quark masses is facilitated by the use of the Fat-Link Irrelevant Clover (FLIC) fermion action. Additionally, we make use of large (203×4020^3 \times 40) lattices to obtain good control of statistical and finite volume errors. Our results indicate that the 1+1^{-+} exotic exhibits significant curvature close the chiral limit, indicating previous linear extrapolations, far from the chiral regime, have overestimated the mass of the 1+1^{-+}. We find for the first time in lattice studies a 1+1^{-+} mass in agreement with the π1(1600)\pi_1 (1600) candidate. We also find a strangeness ±\pm1 JP=1J^P = 1^- state with a mass close to 2 GeV.Comment: 8 pages, 11 figures, 3 tables, published versio

    Experimental Status of Exotic Mesons and the GlueX Experiment

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    One of the unanswered and most fundamental questions in physics regards the nature of the confinement mechanism of quarks and gluons in QCD. Exotic hybrid mesons manifest gluonic degrees of freedom and their spectroscopy will provide the data necessary to test assumptions in lattice QCD and the specific phenomenology leading to confinement. Within the past two decades a number of experiments have put forth tantalizing evidence for the existence of exotic hybrid mesons in the mass range below 2 GeV. This talk represents an overview of the available data and what has been learned. In looking toward the future, the GlueX experiment at Jefferson Laboratory represents a new initiative that will perform detailed spectroscopy of the light-quark meson spectrum. This experiment and its capabilities will be reviewed.Comment: 10 pages, 8 figures, 2nd Meeting of the APS Topical Group on Hadron Physics GHP06, Nashville, TN (10/22-10/24/06

    Radiative Decays of the Upsilon(1S) to a Pair of Charged Hadrons

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    Using data obtained with the CLEO~III detector, running at the Cornell Electron Storage Ring (CESR), we report on a new study of exclusive radiative Upsilon(1S) decays into the final states gamma pi^+ pi^-, gamma K^+ K^-, and gamma p pbar.. We present branching ratio measurements for the decay modes Upsilon(1S) to gamma f_2(1270), Upsilon(1S) to gamma f_2'(1525), and Upsilon(1S) to gamma K^+K^-; helicity production ratios for f_2(1270) and f_2'(1525); upper limits for the decay Upsilon(1S) to gamma f_J(2200), with f_J(2220) to pi^+ pi^-, K^+ K^-, p pbar; and an upper limit for the decay Upsilon(1S) to gamma X(1860), with X(1860) to gamma p pbar.Comment: 17 pages postscript,also available through http://www.lns.cornell.edu/public/CLNS/2005/, Submitted to PR

    Evidence for Exotic J^{PC}=1^{-+} Meson Production in the Reaction pi- p --> eta pi- p at 18 GeV/c

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    Details of the analysis of the eta pi- system studied in the reaction pi^{-} p --> eta pi^{-} p at 18 GeV/c are given. Separate analyses for the 2 gamma and pi+ pi- pi0 decay modes of the eta are presented. An amplitude analysis of the data indicates the presence of interference between the a(2)(1320)- and a J^{PC}=1^{-+} wave between 1.2 and 1.6 GeV/c^2. The phase difference between these waves shows phase motion not attributable solely to the a(2)(1320)-. The data can be fitted by interference between the a(2)(1320)- and an exotic 1^{-+} resonance with M = 1370 +-16 +50 -30} MeV/c^2 and Gamma = 385 +- 40 +65 -105 MeV/c^2. Our results are compared with those of other experiments.Comment: 50 pages of text and 34 figure

    Simulation of the thermally induced austenitic phase transition in NiTi nanoparticles

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    The reverse martensitic ("austenitic") transformation upon heating of equiatomic nickel-titanium nanoparticles with diameters between 4 and 17 nm is analyzed by means of molecular-dynamics simulations with a semi-empirical model potential. After constructing an appropriate order parameter to distinguish locally between the monoclinic B19' at low and the cubic B2 structure at high temperatures, the process of the phase transition is visualized. This shows a heterogeneous nucleation of austenite at the surface of the particles, which propagates to the interior by plane sliding, explaining a difference in austenite start and end temperatures. Their absolute values and dependence on particle diameter are obtained and related to calculations of the surface induced size dependence of the difference in free energy between austenite and martensite.Comment: 6 pages, 4 figures, accepted for publication in "The European Physical Journal B

    Observation of vertex factorisation breaking in central pp interactions

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    Central \pipi events produced in pp interactions are studied in terms of correlations between the outgoing protons. It is observed there is more ρ0\rho^{0}(770) and \fmeson production in reactions where the outgoing protons %fastest and slowest particles in the laboratory frame are on opposite sides of the beam. This effect is not attributable to the trigger or the experimental acceptance, and suggests that the vertices do not factorise

    A partial wave analysis of the centrally produced K+KK^{+}K^{-} and Ks0Ks0K^{0}_{s}K^{0}_{s} systems in pp interactions at 450 GeV/c and new information on the spin of the f1f_{1} (1710)

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    A partial wave analysis of the centrally produced K+K- and K0K0 channels has been performed in pp collisions using an incident beam momentum of 450 GeV/c. An unambiguous physical solution has been found in each channel. The striking feature is the observation of peaks in the S-wave corresponding to the f0(1500) and fJ(1710) with J = 0. The D-wave shows evidence for the f2(1270)/a2(1320), the f2(1525) and the f2(2150) but there is no evidence for a statistically significant contribution in the D-wave in the 1.7 GeV mass region

    Evidence for Exotic Meson Production in the Reaction πpηπp \pi^{-} p \to \eta \pi^{-} p at 18 GeV/c

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    The ηπ\eta \pi^{-} system has been studied in the reaction πpηπp\pi^{-} p \to \eta \pi^{-} p at 18 GeV/c. A large asymmetry in the angular distribution is observed indicating interference between L-even and L-odd partial waves. The a2(1320)a_{2}(1320) is observed in the JPCJ^{PC} = 2++2^{++} wave, as is a broad enhancement between 1.2 and 1.6 GeV/c^{2} in the JPC=1+J^{PC} = 1^{-+} wave. The observed phase difference between these waves shows that there is phase motion in addition to that due to a2(1320)a_{2}(1320) decay. The data can be fitted by interference between the a2(1320)a_{2}(1320) and an exotic 1+1^{-+} resonance with M=(1370±16+5030M = (1370 \pm 16 {+50}\atop{-30}) MeV/c^2 and Γ=(385±40+65105\Gamma =(385 \pm 40 {+65}\atop{-105}) MeV/c^2
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