2,663 research outputs found

    The Inverse Amplitude Method and Adler Zeros

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    The Inverse Amplitude Method is a powerful unitarization technique to enlarge the energy applicability region of Effective Lagrangians. It has been widely used to describe resonances from Chiral Perturbation Theory as well as for the Strongly Interacting Symmetry Breaking Sector. In this work we show how it can be slightly modified to account also for the sub-threshold region, incorporating correctly the Adler zeros required by chiral symmetry and eliminating spurious poles. These improvements produce negligible effects on the physical region.Comment: 17 pages, 4 figure

    A Study in Depth of f0(1370)

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    Claims have been made that f0(1370) does not exist. The five primary sets of data requiring its existence are refitted. Major dispersive effects due to the opening of the 4pi threshold are included for the first time; the sigma -> 4pi amplitude plays a strong role. Crystal Barrel data on pbar-p -> 3pizero at rest require f0(1370) signals of at least 32 and 33 standard deviations in 1S0 and 3P1 annihilation respectively. Furthermore, they agree within 5 MeV for mass and width. Data on pbar-p -> eta-eta-pizero agree and require at least a 19 standard deviation contribution. This alone is sufficient to demonstrate the existence of f0(1370). BES II data for J/Psi -> phi-pi-pi contain a visible f0(1370) signal > 8 standard devations. In all cases, a resonant phase variation is required. The possibility of a second pole in the sigma amplitude due to the opening of the 4pi channel is excluded. Cern-Munich data for pi-pi elastic scattering are fitted well with the inclusion of some mixing between sigma, f0(1370) and f0(1500). The pi-pi widths for f2(1565), rho3(1690), rho3(1990) and f4(2040) are determined.Comment: 25 pages, 22 figures. Typos corrected in Eqs 2 and 7. Introduction rewritten. Conclusions unchange

    Gender-related biases in admission decisions

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    Journal ArticleThe competitive admission process for educational programs in health sciences usually begins with a screening phase. Raters, who are often the same people who later interview the applicants, screen candidates based on information on their application forms. Only the applicants who survive the screening phase progress to the interview phase

    Nature of the f_0(600) from its N_c dependence at two loops in unitarized Chiral Perturbation Theory

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    By using unitarized two-loop Chiral Perturbation Theory partial waves to describe pion-pion scattering we find that the dominant component of the lightest scalar meson does not follow the q-qbar dependence on the number of colors that, in contrast, is obeyed by the lightest vectors. The method suggests that a subdominant q-qbar component of the f_0(600) possibly originates around 1 GeV.Comment: 4 pages, 1 Figure. To appear in Phys. Rev. Let

    Comment on Neutron-Proton Spin-Correlation Parameter A_{ZZ} at 68 Mev

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    We present two arguments indicating that the large value for the ϵ1\epsilon_1 mixing parameter at 50 MeV, which the Basel group extracted from their recent AzzA_{zz} measurement, may be incorrect. First, there are nucleon-nucleon (NN) potentials which predict the ϵ1\epsilon_1 at 50 MeV substantially below the Basel value and reproduce the Basel AzzA_{zz} data accurately. Second, the large value for ϵ1\epsilon_1 at 50 MeV proposed by the Basel group can only be explained by a model for the NN interaction which is very unrealistic (no ρ\rho-meson and essentially a point-like πNN\pi NN vertex) and overpredicts the ϵ1\epsilon_1 in the energy range where it is well determined (150--500 MeV) by a factor of two.Comment: 6 pages text (LaTex) and 2 figures (paper, will be faxed upon request), UI-NTH-930

    The nature of σ\sigma, κ\kappa, a0(980)a_0(980) and f0(980)f_0(980)

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    Masses and widths of the four light scalar mesons σ\sigma, κ\kappa, a0a_0(980) and f0f_0(980) may be reproduced in a model where mesons scatter via a qqˉq\bar{q} loop. A transition potential is used to couple mesons to qqˉq\bar{q} at a radius of 0.57\sim 0.57 fm. Inside this radius, there is an infinite bare spectrum of confined qqˉq\bar{q} states, for which a harmonic oscillator is chosen here. The coupled-channel system approximately reproduces the features of both light and heavy meson spectroscopy. The generation of σ\sigma, κ\kappa, a0(980)a_0(980) and f0(980)f_0(980) is a balance between attraction due to the qqˉq\bar q loop and suppression of the amplitudes at the Adler zeros. Phase shifts increase more rapidly as the coupling constant to the mesons increases. This leads to resonant widths which decrease with increasing coupling constant - a characteristically non-perturbative effect.Comment: Plain LaTeX, 10 pages, 3 EPS figures; v2: 11 pages, better-quality figures, extra references, version accepted for publication in Phys. Lett.

    Flatte-like distributions and the a_0(980)/f_0(980) mesons

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    We explore the features of Flatte-like parametrizations. In particular, we demonstrate that the large variation in the absolute values of the coupling constants to the pi-eta (or pi-pi) and KKbar channels for the a_0(980) and f_0(980) mesons that one can find in the literature can be explained by a specific scaling behaviour of the Flatte amplitude for energies near the KKbar threshold. We argue that the ratio of the coupling constants can be much better determined from a fit to experimental data.Comment: 12 pages, 12 figure

    CHIRAL SYMMETRY CONSTRAINTS ON THE K+K^+ INTERACTION WITH THE NUCLEAR PION CLOUD

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    The real part of the K+K^{+} selfenergy for the interaction of the K+K^{+} with the pion nuclear cloud is evaluated in lowest order of chiral perturbation theory and is found to be exactly zero in symmetric nuclear matter. This removes uncertainties in that quantity found in former phenomenological analyses and is supported by present experimental data on K+K^{+} nucleus scattering.Comment: 11 pp, LaTeX file, 4 figures (appended as compressed tar files, uses epsf.sty

    The preliminary lattice QCD calculation of κ\kappa meson decay width

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    We present a direct lattice QCD calculation of the κ\kappa meson decay width with the s-wave scattering phase shift for the isospin I=1/2I=1/2 pion-kaon (πK\pi K) system. We employ a special finite size formula, which is the extension of the Rummukainen-Gottlieb formula for the πK\pi K system in the moving frame, to calculate the scattering phase, which indicates a resonance around κ\kappa meson mass. Through the effective range formula, we extract the effective κπK\kappa \to \pi K coupling constant gκπK=4.54(76)g_{\kappa \pi K} = 4.54(76) GeV and decay width Γ=293±101\Gamma = 293 \pm 101 MeV. Our simulations are done with the MILC gauge configurations with Nf=2+1N_f=2+1 flavors of the "Asqtad" improved staggered dynamical sea quarks on a 163×4816^3\times48 lattice at (mπ+mK)/mκ0.8(m_\pi + m_K) / m_\kappa \approx 0.8 and lattice spacing a0.15a \approx 0.15 fm.Comment: To make it concise. arXiv admin note: text overlap with arXiv:1110.1422, but much of v1 text overlap with articles by same and other authors remove
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