799 research outputs found

    Proceedings of the workshop "Standard Model at the LHC" University College London 30 March - 1 April 2009

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    Proceedings from a 3-day discussion on Standard Model discoveries with the first LHC dataComment: 9 contributions to the proceedings of the LHC Standard Model worksho

    Elastic and quasi-elastic pppp and γp\gamma^\star p scattering in the Dipole Model

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    We have in earlier papers presented an extension of Mueller's dipole cascade model, which includes sub-leading effects from energy conservation and running coupling as well as colour suppressed saturation effects from pomeron loops via a ``dipole swing''. The model was applied to describe the total and diffractive cross sections in pppp and γp\gamma^*p collisions, and also the elastic cross section in pppp scattering. In this paper we extend the model to describe the corresponding quasi-elastic cross sections in γp\gamma^*p, namely the exclusive production of vector mesons and deeply virtual compton scattering. Also for these reactions we find a good agrement with measured cross sections. In addition we obtain a reasonable description of the tt-dependence of the elastic pppp and quasi-elastic γp\gamma^\star p cross sections

    Deep inelastic scattering and "elastic" diffraction

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    We examine the total cross section of virtual photons on protons, σγp(W2,Q2)\sigma_{\gamma^* p}(W^2,Q^2), at low xQ2/W21x \cong Q^2/W^2 \ll 1 and its connection with ``elastic'' diffractive production γT,LpXT,LJ=1p\gamma^*_{T,L}p \to X^{J=1}_{T,L} p in the two-gluon exchange dynamics for the virtual forward Compton scattering amplitude. Solely based on the generic structure of two-gluon exchange, we establish that the cross section is described by the (imaginary part of the) amplitude for forward scattering of qqˉq \bar q vector states, (qqˉ)T,LJ=1p(qqˉ)T,LJ=1p(q \bar q)^{J=1}_{T,L} p \to (q \bar q)^ {J=1}_{T,L} p. The generalized vector dominance/color dipole picture (GVD/CDP) is accordingly established to only rest on the two-gluon-exchange generic structure. This is explicitly seen by the sum rules that allow one to directly relate the total cross section to the cross section for elastic diffractive forward production, γT,Lp(qqˉ)T,LJ=1p\gamma^*_{T,L} p\to (q \bar q)^{J=1}_{T,L} p, of vector states.Comment: 24 pages, latex file with three eps figures. BI-TP 2002/2

    Interference in Exclusive Vector Meson Production in Heavy Ion Collisions

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    Photons emitted from the electromagnetic fields of relativistic heavy ions can fluctuate into quark anti-quark pairs and scatter from a target nucleus, emerging as vector mesons. These coherent interactions are identifiable by final states consisting of the two nuclei and a vector meson with a small transverse momentum. The emitters and targets can switch roles, and the two possibilities are indistinguishable, so interference may occur. Vector mesons are negative parity so the amplitudes have opposite signs. When the meson transverse wavelength is larger than the impact parameter, the interference is large and destructive. The short-lived vector mesons decay before amplitudes from the two sources can overlap, and so cannot interfere directly. However, the decay products are emitted in an entangled state, and the interference depends on observing the complete final state. The non-local wave function is an example of the Einstein-Podolsky-Rosen paradox.Comment: 13 pages with 3 figures; submitted to Physical Review Letter

    Properties of Regge Trajectories

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    Early Chew-Frautschi plots show that meson and baryon Regge trajectoies are approximately linear and non-intersecting. In this paper, we reconstruct all Regge trajectories from the most recent data. Our plots show that meson trajectories are non-linear and intersecting. We also show that all current meson Regge trajectories models are ruled out by data.Comment: 30 pages, latex, 18 figures, to be published in Physical Review

    On the Energy Dependence of the Dipole-Proton Cross Section in Deep Inelastic Scattering

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    We study the dipole picture of high-energy virtual-photon-proton scattering. It is shown that different choices for the energy variable in the dipole cross section used in the literature are not related to each other by simple arguments equating the typical dipole size and the inverse photon virtuality, contrary to what is often stated. We argue that the good quality of fits to structure functions that use Bjorken-x as the energy variable - which is strictly speaking not justified in the dipole picture - can instead be understood as a consequence of the sign of scaling violations that occur for increasing Q^2 at fixed small x. We show that the dipole formula for massless quarks has the structure of a convolution. From this we obtain derivative relations between the structure function F_2 at large and small Q^2 and the dipole-proton cross section at small and large dipole size r, respectively.Comment: 27 page

    Diffractive production and the total cross section in deep inelastic scattering

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    We explore the consequences for diffractive production, gamma* p --> X p, in deep inelastic scattering at low values of x\sim Q^2/W^2 <<1 that follow from our recent representation of the total photoabsorption cross section, sigma_{gamma* p}, in the generalized vector dominance/ color dipole picture(GVD/CDP) that is based on the generic structure of the two-gluon-exchange from QCD. Sum rules are derived that relate the transverse and the longitudinal (virtual) photoabsorption cross section to diffractive forward production of q q-bar states that carry photon quantum numbers ("elastic diffraction"). Agreement with experiment in the W^2 and Q^2 dependence is found for M_X^2/Q^2<<1, where M_X is the mass of the produced system X. An additional component ("inelastic diffraction"), not actively contributing to the forward Compton amplitude, is needed for diffractive production at high values of M_X. Our previous theoretical representation of the total photoabsorption cross section sigma_{gamma* p}=sigma_{gamma* p}(eta), in terms of the scaling variable eta=(Q^2+m_0^2)/Lambda^2(W^2) is extended to include the entire kinematic domain, x==0, where scaling in eta holds experimentally.Comment: 19 pages with 4 figures,(eps and ps files), Late

    The description of F2 at small x incorporating angular ordering

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    We study the perturbative QCD description of the HERA measurements of F2(x,Q2)F_2 (x, Q^2) using a gluon distribution that is obtained from an evolution incorporating angular ordering of the gluon emissions, and which embodies both GLAP and BFKL dynamics. We compare the predictions with recent HERA data for F2F_2. We present estimates of the charm component F2c(x,Q2)F_2^c (x, Q^2) and of FL(x,Q2)F_L (x, Q^2).Comment: 8 LaTeX pages + 4 uuencoded figure

    Multiple Interactions in Two-Photon Collisions

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    We compute cross sections for events where two pairs of partons scatter off each other in the same γγ\gamma\gamma reaction, giving rise to at least 3 high--{\mbox{pTp_T^{}}} jets. Unlike in {\mbox{ppˉp \bar p}}\ collisions we find the signal to lie well above the background from higher order QCD processes. If the usual ``eikonaliztion" assumption is correct, the signal should be readily observable at LEP2, and might already be detectable in data taken at TRISTAN.Comment: 8 pages, plain LaTeX, 2 figures (not included). A compressed PS file of the entire paper, including figures, can be obtained via anonymous ftp from ftp://phenom.physics.wisc.edu/pub/preprints/1995/madph-95-921.ps.
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