90 research outputs found

    X-wave mediated instability of plane waves in Kerr media

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    Plane waves in Kerr media spontaneously generate paraxial X-waves (i.e. non-dispersive and non-diffractive pulsed beams) that get amplified along propagation. This effect can be considered a form of conical emission (i.e. spatio-temporal modulational instability), and can be used as a key for the interpretation of the out of axis energy emission in the splitting process of focused pulses in normally dispersive materials. A new class of spatio-temporal localized wave patterns is identified. X-waves instability, and nonlinear X-waves, are also expected in periodical Bose condensed gases.Comment: 4 pages, 6 figure

    Charge exchange ρ0π+\rho^0 \pi^+ photoproduction and implications for searches of exotic meson

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    We analyze the process γ⃗+p→ρ0π+n\vec \gamma +p\to \rho^0 \pi^{+}n at low momentum transfer focusing on a possibility of production of an exotic JPC=1−+J^{PC}=1^{-+} meson state. In particular we discuss polarization observables and conclude that linear photon polarization is instrumental for separating of the exotic wave.Comment: 23 pages, 6 figure

    Exotic ρ±ρ0\rho^\pm\rho^0 state photoproduction

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    It is shown that the list of unusual mesons planned for a careful study in photoproduction can be extended by the exotic states X±(1600)X^\pm(1600) with IG(JPC)=2+(2++)I^G(J ^{PC})=2^+(2^{++}) which should be looked for in the ρ±ρ0\rho^\pm\rho^0 decay channels in the reactions ÎłN→ρ±ρ0N\gamma N\to\rho^\pm\rho^0N and ÎłN→ρ±ρ0Δ\gamma N\to\rho^\pm \rho^0\Delta. The full classification of the ρ±ρ0\rho^\pm\rho^0 states by their quantum numbers is presented. A simple model for the spin structure of the Îłp→f2(1270)p \gamma p\to f_2(1270)p, Îłp→a20(1320)p\gamma p\to a^0_2(1320)p, and ÎłN→X±(N,Δ)\gamma N\to X^\pm (N, \Delta) reaction amplitudes is formulated and the tentative estimates of the corresponding cross sections at the incident photon energy Eγ≈6E_\gamma\approx 6 GeV are obtained: σ(Îłp→f2(1270)p)≈0.12\sigma(\gamma p\to f_2(1270)p)\approx0.12 ÎŒ\mub, σ(Îłp→a20(1320)p)≈0.25 \sigma(\gamma p\to a^0_2(1320)p)\approx0.25 ÎŒ\mub, σ(ÎłN→X±N→ρ±ρ0N)≈0.018\sigma(\gamma N\to X^\pm N\to\rho^\pm\rho^0N)\approx0.018 ÎŒ\mub, and σ(Îłp→X−Δ++→ρ−ρ0Δ++)≈0.031\sigma(\gamma p\to X^-\Delta^{++ }\to\rho^-\rho^0\Delta^{++})\approx0.031 ÎŒ\mub. The problem of the X±X^\pm signal extraction from the natural background due to the other π±π0π+π−\pi^\pm\pi^0 \pi^+\pi^- production channels is discussed. In particular the estimates are presented for the Îłp→h1(1170)π+n\gamma p\to h_1(1170)\pi^+n, Îłp→ρâ€Č+n→π+π0π+π−n\gamma p\to\rho'^{+}n\to \pi^+\pi^0\pi^+\pi^-n, and Îłp→ωρ0p\gamma p\to\omega\rho^0p reaction cross sections. Our main conclusion is that the search for the exotic X±(2+(2++))X^\pm(2^+(2^{++})) states is quite feasible at JEFLAB facility. The expected yield of the ÎłN→X±N→ρ±ρ0N\gamma N\to X^\pm N\to\rho^\pm\rho^0N events in a 30-day run at the 100% detection efficiency approximates 2.8×1062.8\times10^6 events.Comment: 19 pages, revtex, 1 figure in postscipt, some comments and references added, a few minor typos corrected, to be published in Phys. Rev.

    ATLAS detector and physics performance: Technical Design Report, 1

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