2,267 research outputs found

    Description of self-synchronization effects in distributed Josephson junction arrays using harmonic analysis and power balance

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    Power generation and synchronisation in Josephson junction arrays have attracted attention for a long time. This stems from fundamental interest in nonlinear coupled systems as well as from potential in practical applications. In this paper we study the case of an array of junctions coupled to a distributed transmission line either driven by an external microwave or in a self-oscillating mode. We simplify the theoretical treatment in terms of harmonic analysis and power balance. We apply the model to explain the large operation margins of SNS- and SINIS-junction arrays. We show the validity of the approach by comparing with experiments and simulations with self-oscillating es-SIS junction arrays.Comment: 5 pages, 3 figure

    Selected topics in e^+e^- collisions

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    Content : 1) The leading twist pion wave function, 2) "Improved" QCD sum rules with non-local condensates, 3) Pion and kaon form factors and charmonium decays: theory vs experiment, 4) \gamma^{*}\gamma\pi^{o} - form factor, 5) The new non-local axial anomaly, 6) Cross sections \gamma\gamma --> \pi^+\pi^-, K^+K^-, K_S K_S .Comment: Talk given at the International Workshop "e^+e^- collisions from \phi to J/\psi", March 1, 2006, Novosibirsk, Russia; 20 pages, 7 figures; v2: sect.2 expanded to clarify the argumentation, a number of small improvements in the tex

    Two photon decay of the pseudoscalars, the chiral symmetry breaking corrections

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    The extrapolation of the decay amplitudes of the pseudoscalar mesons into two photons from the soft meson limit where it is obtained from the axial-anomaly to the mass shell involves the contribution of the 0^ - continuum. These chiral symmetry breaking corrections turn out to be large. The effects of these corrections on the calculated pi ^0 decay rate, on the values of the singlet-octet mixing angle and on the ratios f_8 / f_pi and f_0 / f_pi are discussed. The implications for the transition form factors gamma gamma* --> pseudoscalars are also evaluated and confronted with the available experimental data.Comment: Computational errors straightened and study of the implications on the form factors of the transitions gamma gamma* --> pseudoscalars adde

    QED radiative corrections to the decay pi^0 to e^+e^-

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    We reconsider QED radiative corrections (RC) to the π0e+e\pi^{0}\to e^{+}e^{-} decay width. One kind of RC investigated earlier has a renormalization group origin and can be associated with the final state interaction of electron and positron. It determines the distribution of lepton pair invariant masses in the whole kinematic region. The other type of RC has a double-logarithmic character and is related to almost on-mass-shell behavior of the lepton form factors. The total effect of RC for the π0e+e\pi^{0}\to e^{+}e^{-} decay is estimated to be 3.2% and for the decay ηe+e\eta \to e^{+}e^{-} is 4.3%.Comment: 12 pages, 3 figure

    Eddy current studies from the undulator-based positron source target wheel prototype

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    The ef­fi­cien­cy of fu­ture positron sources for the next gen­er­a­tion of high-en­er­gy par­ti­cle col­lid­ers (e.g. ILC, CLIC, LHeC) can be im­proved if the positron-pro­duc­tion tar­get is im­mersed in the mag­net­ic field of ad­ja­cent cap­ture op­tics. If the tar­get is also ro­tat­ing due to heat de­po­si­tion con­sid­er­a­tions then eddy cur­rents may be in­duced and lead to ad­di­tion­al heat­ing and stress­es. In this paper we pre­sent data from a ro­tat­ing tar­get wheel pro­to­type for the base­line ILC positron source. The wheel has been op­er­at­ed at rev­o­lu­tion rates up to 1800rpm in fields of the order of 1 Tesla. Com­par­isons are made be­tween torque data ob­tained from a trans­duc­er on the tar­get drive shaft and the re­sults of fi­nite-el­e­ment sim­u­la­tions. Ro­tor­dy­nam­ics is­sues are pre­sent­ed and fu­ture ex­per­i­ments on other as­pects of the positron source tar­get sta­tion are con­sid­ered

    Quark-hadron duality, axial anomaly and mixing

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    Interplay between axial anomaly and quark-hadron duality in the presence of strong mixing is considered. The anomaly sum rule for meson transition form factors based on the dispersive representation of axial anomaly and quark-hadron duality in octet channel is analyzed. The comparison of this sum rule to the experimental data on η\eta and η\eta' mesons transition form factors shows that the interval of duality in this channel is rather small, contradicting the usual understanding of quark-hadron duality. The same values of interval of duality are supported by considering the two-point correlator in the local duality limit. This contradiction may be resolved by introducing of some nonperturbative non-OPE correction to the relevant spectral density. The form and value of this correction are discussed.Comment: 9 pages, 1 figure, reference adde

    Detecting and Studying Higgs Bosons at a Photon-Photon Collider

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    We examine the potential for detecting and studying Higgs bosons at a photon-photon collider facility associated with a future linear collider. Our study incorporates realistic \gam\gam luminosity spectra based on the most probable available laser technology. Results include detector simulations. We study the cases of: a) a SM-like Higgs boson; b) the heavy MSSM Higgs bosons; c) a Higgs boson with no WW/ZZWW/ZZ couplings from a general two Higgs doublet model.Comment: 52 pages, 26 figures, revised version with new appendi

    Pion light cone wave function in the non-local NJL model

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    We use the simple instanton motivated NJL-type model to calculate the leading twist pion light cone wave function. The model consists in employing the momentum dependent quark mass in the quark loop entering the definition of the wave function. The result is analytical up to a solution of a certain algebraic equation. Various properties including the kT dependence of the pion wave function are discussed. The resulting kT integrated wave function is not asymptotic and is in agreement with recent analysis of the CLEO data.Comment: 9 pages, 12 figures, formulas (23-25) corrected, typos correcte

    ηη\eta-\eta^\prime mixing and the next-to-leading-order power correction

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    The next-to-leading-order O(1/Q4)O(1/Q^4) power correction for ηγ\eta\gamma and ηγ\eta^\prime\gamma form factors are evaluated and employed to explore the ηη\eta-\eta^\prime mixing. The parameters of the two mixing angle scheme are extracted from the data for form factors, two photon decay widths and radiative J/ψJ/\psi decays. The χ2\chi^2 analysis gives the result: fη1=(1.16±0.06)fπ,fη8=(1.33±0.23)fπ,θ1=9±3,θ8=21.3±2.3f_{\eta_1}=(1.16\pm0.06)f_\pi, f_{\eta_8}=(1.33\pm0.23)f_\pi, \theta_1=-9^\circ\pm 3^\circ, \theta_8=-21.3^\circ\pm 2.3^\circ, where fη1(8)f_{\eta_{1(8)}} and θ1(8)\theta_{1(8)} are the decay constants and the mixing angles for the singlet (octet) state. In addition, we arrive at a stringent range for fηc:10f_{\eta^\prime}^c:-10 MeVfηc4\le f_{\eta^\prime}^c\le -4 MeV.Comment: 23 pages, 9 figures, To be publshied in Phys. Rev.
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