3,824,696 research outputs found

    Semiclassical Calculation of Photon-Stimulated Schwinger Pair Creation

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    We consider the electron-positron pair creation by a photon in an external constant electric field. The presented treatment is based on a purely quasiclassical calculation of the imaginary part of the on-shell photon polarization operator. By using this approach we find the pair production rate for photons with polarization parallel as well as orthogonal to the external electric field in the leading order in the parameter eE/m2eE / m ^ 2, which has been recently found by other methods. For the orthogonal polarization we also find a new contribution to the rate, which is leading in the ratio of the photon energy to the electron mass ω/m\omega/m. We also reproduce by a purely geometrical calculation the exponential factor in the probability of the stimulated pair creation at arbitrary energy of the photon.Comment: 16 pages, 4 figure

    Heavy quark spin symmetry breaking in near-threshold JPC=1J^{PC}=1^{--} quarkonium-like resonances

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    A mixing of near-threshold quarkonium-like resonances with heavy meson-antimeson pairs results in an enhancement of heavy quark spin symmetry breaking, since the meson pairs are not eigenstates of the heavy quark spin. The decomposition of PP-wave states of meson pairs in terms of the heavy-quark-pair spin states is considered in the channel with JPC=1J^{PC}=1^{--}, which is directly produced in e+ee^+e^- annihilation. Specific processes are suggested for experimental study of the effects of the mixing with heavy meson pairs and of the internal spin structure of bottomonium and charmonium resonances.Comment: 15 page

    The cˉc{\bar c} c purity of ψ(3770)\psi(3770) and ψ\psi' challenged

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    It is suggested that the resonance ψ(3770)\psi(3770) may contain a sizeable (O(10O(10%) in terms of the probability weight factor) four-quark component with the up- and down- quarks and antiquarks in addition to the ccˉc {\bar c} pair, which component in itself has a substantial part with the isospin I=1. Furthermore such four-quark part of the wave function should also affect the properties of the ψ\psi' charmonium resonance through the ψ(3770)ψ\psi(3770) - \psi' mixing previously considered in the literature. It is argued that an admixture of extra light quark pairs can explain a possible discrepancy between the theoretical expectations and the recent data on the non-DDˉD {\bar D} decay width of the ψ(3770)\psi(3770) and the ratio of the yield of charged and neutral DD meson pairs in its decays, as well as on the extra rate of the ψ\psi' direct decay into light hadrons and the rate of the decay ψπ0J/ψ\psi' \to \pi^0 J/\psi. It is further argued that the suggested four-quark component of the wave function of the ψ(3770)\psi(3770) should give rise to a measurable rate of the decays ψ(3770)ηJ/ψ\psi(3770) \to \eta J/\psi and ψ(3770)π0J/ψ\psi(3770) \to \pi^0 J/\psi.Comment: 13 page

    On domain shapes and processes in supersymmetric theories

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    A supersymmetric theory with several scalar superfields generically has several domain wall type classical configurations which interpolate between various supersymmetric vacua of the scalar fields. Depending on the couplings, some of these configurations develop instability and decay into multiple domain walls, others can form intersections in space. These phenomena are considered here in a simplest, yet non-trivial, model with two scalar superfields.Comment: 10 pages, LaTeX, 5 figures in LaTe

    Comment on "Summing One-Loop Graphs at Multi-Particle Threshold"

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    The propagator of a virtual ϕ\phi-field with emission of nn on-mass-shell particles all being exactly at rest is calculated at the tree-level in λϕ4\lambda \phi^4 theory by directly solving recursion equations for the sum of Feynman graphs. It is shown that the generating function for these propagators is equivalent to a Fourier transform of the recently found Green's function within the background-field technique for summing graphs at threshold suggested by Lowell Brown. Also the derivation of the result that the tree-level on-mass-shell scattering amplitudes of the processes 2n2 \to n are exactly vanishing at threshold for n>4n > 4 is thus given in the more conventional Feynman diagram technique.Comment: 7 pages, LaTeX, TPI-MINN-92/46-

    Bottomonium dipion transitions

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    Dipion transitions of the subthreshold bottomonium levels Υ(nS)Υ(nS)ππ\Upsilon (nS)\to \Upsilon (n'S) \pi\pi with n>n,n=2,3,4,n=1,2n>n', n=2,3,4, n'=1,2 are studied in the framework of the chiral decay Lagrangian, derived earlier. The channels BBˉ,BBˉ+c.c,BBˉB\bar B, B\bar B^*+ c.c, B^* \bar B^* are considered in the intermediate state and realistic wave functions of Υ(nS),B\Upsilon (n S),B and BB^* are used in the overlap matrix elements. Imposing the Adler zero requirement on the transition matrix element, one obtains 2d and 1d dipion spectra in reasonable agreement with experiment.Comment: 34 pages, 18 figure

    Properties of perturbative multi-particle amplitudes in ϕk\phi^k and O(N)O(N) theories

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    Threshold amplitudes are considered for multi-particle production in ϕk\phi^k and O(N) ϕ4O(N) ~\phi^4 theories. It is found that the disappearance of tree-level threshold amplitudes of 22 on-shell particles producing a large number of particles occurs in ϕk\phi^k theory only for k=3k=3 and k=4k=4. The one-loop correction to the threshold amplitude for a highly virtual scalar particle decaying into nn particles in an O(N)O(N) model is derived.Comment: 7 pages, LaTex, TPI-MINN-92/60-

    The Orbifold-String Theories of Permutation-Type: III. Lorentzian and Euclidean Space-Times in a Large Example

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    To illustrate the general results of the previous paper, we discuss here a large concrete example of the orbifold-string theories of permutation-type. For each of the many subexamples, we focus on evaluation of the \emph{target space-time dimension} D^j(σ)\hat{D}_j(\sigma), the \emph{target space-time signature} and the \emph{target space-time symmetry} of each cycle jj in each twisted sector σ\sigma. We find in particular a gratifying \emph{space-time symmetry enhancement} which naturally matches the space-time symmetry of each cycle to its space-time dimension. Although the orbifolds of Z2\Z_{2}-permutation-type are naturally Lorentzian, we find that the target space-times associated to larger permutation groups can be Lorentzian, Euclidean and even null (\hat{D}_{j}(\sigma)=0), with varying space-time dimensions, signature and symmetry in a single orbifold.Comment: 36 page

    Spin-spin Correlation in Some Excited States of Transverse Ising Model

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    We consider the transverse Ising model in one dimension with nearest-neighbour interaction and calculate exactly the longitudinal spin-spin correlation for a class of excited states. These states are known to play an important role in the perturbative treatment of one-dimensional transverse Ising model with frustrated second-neighbour interaction. To calculate the correlation, we follow the earlier procedure of Wu, use Szego's theorem and also use Fisher-Hartwig conjecture. The result is that the correlation decays algebraically with distance (nn) as 1/n1/\surd n and is oscillatory or non-oscillatory depending on the magnitude of the transverse field.Comment: 5 pages, 1 figur

    Becoming eco-responsible, active citizens through participation in the Eco Ambassadors project - a reflective analysis

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    This article offers a reflective analysis of the Eco Ambassadors Project as an example of the some of the ways in which learning about environmental issues and active citizenship can be encouraged and enabled through collaboration and negotiated participation. Some policy background to the project is given, followed by a critical consideration of the theoretical framework of situated learning and participation in a community of practice in relation to the project alongside theories of citizenship. Three activities undertaken during the project are highlighted and these are critically examined in relation to the theories under consideration. The paper argues that the theoretical framework of learning by participation can usefully augment and help better explain how learners develop their identities as citizens, and that through participation people can become active members of communities that are environmentally and politically aware
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