3,922 research outputs found

    Quantum loops in radiative decays of the a1a_1 and b1b_1 axial-vector mesons

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    A previous model where the low-lying axial-vector mesons are dynamically generated, implementing unitarity in coupled channels in the vector-pseudoscalar (VPVP) meson interaction, is applied to evaluate the decay widths of the a_1(1260)and and b_1(1235)axialvectormesonsinto axial-vector mesons into \pi\gamma.Unlikethecaseofthe. Unlike the case of the a_1,the, the b_1radiativedecayissystematicallyunderestimatedattreelevel.Inthisworkweevaluateforthefirsttimetheloopcontributioncomingfromaninitial radiative decay is systematically underestimated at tree level. In this work we evaluate for the first time the loop contribution coming from an initial VPvertex.Despitethelargesuperficialdivergenceoftheloops,theconvergenceoftherelevantloopscanbeestablishedbyusingargumentsofgaugeinvariance.Thepartialdecaywidthsobtainedagreeverywellwiththeexperimentalvalueswithinuncertainties,andshowthattheloopcontributioniscrucialinthe vertex. Despite the large superficial divergence of the loops, the convergence of the relevant loops can be established by using arguments of gauge invariance. The partial decay widths obtained agree very well with the experimental values within uncertainties, and show that the loop contribution is crucial in the b_1caseandalsoimportantforthe case and also important for the a_1$ case.Comment: 16 pages, 4 figurs Added extra discussio

    Clues for the existence of two K1(1270)K_1(1270) resonances

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    The axial vector meson K1(1270)K_1(1270) was studied within the chiral unitary approach, where it was shown that it has a two-pole structure. We reanalyze the high-statistics WA3 experiment KpKπ+πpK^- p\to K^-\pi^+\pi^- p at 63 GeV, which established the existence of both K1(1270)K_1(1270) and K1(1400)K_1(1400), and we show that it clearly favors our two-pole interpretation. We also reanalyze the traditional K-matrix interpretation of the WA3 data and find that the good fit of the data obtained there comes from large cancellations of terms of unclear physical interpretation.Comment: published version in PRD; typos corrected; title changed to "Clues for the existence of two K1(1270)K_1(1270) resonances

    A description of the f2(1270), rho3(1690), f4(2050), rho5(2350) and f6(2510) resonances as multi-rho(770) states

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    In a previous work regarding the interaction of two ρ(770)\rho(770) resonances, the f2(1270)f_2(1270) (JPC=2++J^{PC}=2^{++}) resonance was obtained dynamically as a two-ρ\rho molecule with a very strong binding energy, 135~MeV per ρ\rho particle. In the present work we use the ρρ\rho\rho interaction in spin 2 and isospin 0 channel to show that the resonances ρ3(1690)\rho_3(1690) (33^{--}), f4(2050)f_4(2050) (4++4^{++}), ρ5(2350)\rho_5(2350) (55^{--}) and f6(2510)f_6(2510) (6++6^{++}) are basically molecules of increasing number of ρ(770)\rho(770) particles. We use the fixed center approximation of the Faddeev equations to write the multi-body interaction in terms of the two-body scattering amplitudes. We find the masses of the states very close to the experimental values and we get an increasing value of the binding energy per ρ\rho as the number of ρ\rho mesons is increased.Comment: 17 pages, 6 figure

    Recoverin Regulates Light-dependent Phosphodiesterase Activity in Retinal Rods

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    The Ca2+-binding protein recoverin may regulate visual transduction in retinal rods and cones, but its functional role and mechanism of action remain controversial. We compared the photoresponses of rods from control mice and from mice in which the recoverin gene was knocked out. Our analysis indicates that Ca2+-recoverin prolongs the dark-adapted flash response and increases the rod's sensitivity to dim steady light. Knockout rods had faster Ca2+ dynamics, indicating that recoverin is a significant Ca2+ buffer in the outer segment, but incorporation of exogenous buffer did not restore wild-type behavior. We infer that Ca2+-recoverin potentiates light-triggered phosphodiesterase activity, probably by effectively prolonging the catalytic activity of photoexcited rhodopsin

    How different Fermi surface maps emerge in photoemission from Bi2212

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    We report angle-resolved photoemission spectra (ARPES) from the Fermi energy (EFE_F) over a large area of the (kx,kyk_x,k_y) plane using 21.2 eV and 32 eV photons in two distinct polarizations from an optimally doped single crystal of Bi2_2Sr2_2CaCu2_2O8+δ_{8+\delta} (Bi2212), together with extensive first-principles simulations of the ARPES intensities. The results display a wide-ranging level of accord between theory and experiment and clarify how myriad Fermi surface (FS) maps emerge in ARPES under various experimental conditions. The energy and polarization dependences of the ARPES matrix element help disentangle primary contributions to the spectrum due to the pristine lattice from those arising from modulations of the underlying tetragonal symmetry and provide a route for separating closely placed FS sheets in low dimensional materials.Comment: submitted to PR

    Hidden gauge formalism for the radiative decays of axial-vector mesons

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    The radiative decay of the axial-vector resonances into a pseudoscalar meson and a photon is studied using the vector meson Lagrangian obtained from the hidden gauge symmetry (HGS) formalism. The formalism is well suited to study this problem since it deals with pseudoscalar and vector mesons in a unified way, respecting chiral invariance. We show explicitly the gauge invariance of the set of diagrams that appear in the approach and evaluate the radiative decay width of the a1(1260) and b1(1235) axial vector meson resonances into pi gamma. We also include the contribution of loops involving anomalous couplings and compare the results to those obtained previously within another formalism.Comment: 24 pages, 6 tables, 11 figure

    Selected topics on Hadrons in Nuclei

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    In this talk we report on selected topics on hadrons in nuclei. The first topic is the renormalization of the width of the Λ(1520)\Lambda(1520) in a nuclear medium. This is followed by a short update of the situation of the ω\omega in the medium. The investigation of the properties of Kˉ\bar{K} in the nuclear medium from the study of the (Kflight,p)(K_{flight},p) reaction is also addressed, as well as properties of X,Y,Z charmed and hidden charm resonances in a nuclear medium. Finally we address the novel issue of multimeson states.Comment: Talk at the International Nuclear Physics Conference, Vancouver, July 201
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