BARYON STRUCTURE IN AdS/QCD V.E. Lyubovitskij 1,2† , T. Gutsche 1 , I. Schmidt 3 , A. Vega 3 (1) Institut für Theoretische Physik, Universität Tübingen, Kepler Center <strong>for</strong> Astro and Particle Physics, Auf der Morgenstelle 14, D-72076 Tübingen, Germany (2) Department <strong>of</strong> Physics, Tomsk State University, 634050 Tomsk, Russia (3) Departamento de Física y Centro Científico Tecnológico de Valparaíso (CCTVal), Universidad Técnica Federico Santa María, Casilla 110-V, Valparaíso, Chile † E-mail: valeri.lyubovitskij@uni-tuebingen.de We develop the s<strong>of</strong>t-wall model (bottom-down AdS/QCD approach) <strong>for</strong> description <strong>of</strong> baryons [1]-[4]. As application we present a detailed analysis <strong>of</strong> nucleon electromagnetic and axial <strong>for</strong>m factors in a holographic s<strong>of</strong>t-wall model [2]. This approach is based on an action which describes hadrons with broken con<strong>for</strong>mal invariance and incorporates confinement through the presence <strong>of</strong> a background dilaton field [1]-[6]. For N c = 3 we describe the nucleon structure in a superposition <strong>of</strong> a three valence quark state with high Fock states including an adjustable number <strong>of</strong> partons (quarks, antiquarks and gluons) via studying the dynamics <strong>of</strong> 5D fermion fields <strong>of</strong> different scaling dimension in antide Sitter (ADS) space. According to the gauge/gravity duality the 5D fermion fields <strong>of</strong> different scaling dimension correspond to the Fock state components with a specific number <strong>of</strong> partons. In the present application we restrict to the contribution <strong>of</strong> 3, 4 and 5 parton components in the nucleon Fock state. With a minimal number <strong>of</strong> free parameters (dilaton scale parameter, mixing parameters <strong>of</strong> partial contributions <strong>of</strong> Fock states, coupling constants in the effective Lagrangian) we achieve a reasonable agreement with data <strong>for</strong> the nucleon <strong>for</strong>m factors. References [1] T. Gutsche, V.E. Lyubovitskij, I. Schmidt, A. Vega, Phys. Rev. D85, 076003 (2012) [2] T. Gutsche, V.E. Lyubovitskij, I. Schmidt, A. Vega, arXiv:1204.6612 [hep-ph], Phys. Rev. D86, (2012) [in print] [3] A. Vega, I. Schmidt, T. Gutsche, V.E. Lyubovitskij, Phys. Rev. D83, 036001 (2011) [4] A. Vega, I. Schmidt, T. Gutsche, V.E. Lyubovitskij, Phys. Rev. D85, 076003 (2012) [5] T. Branz, T. Gutsche, V.E. Lyubovitskij, I. Schmidt, A. Vega, Phys. Rev. D82, 074022 (2010) [6] A. Vega, I. Schmidt, T. Branz, T. Gutsche, V.E. Lyubovitskij, Phys. Rev. D80, 055014 (2009) 90
START AND TRIGGER DETECTOR T0 OF THE ALICE EXPERIMENT A.I. Maevskaya, T.L. Karavicheva, A.B. Kurepin, A.N. Kurepin <strong>Institute</strong> <strong>for</strong> <strong>Nuclear</strong> <strong>Research</strong> Russian Academy <strong>of</strong> Science, Moscow, Russia One <strong>of</strong> the most important part <strong>of</strong> the ALICE installation is the T0 detector <strong>for</strong> the trigger and start system <strong>for</strong> time <strong>of</strong> flight. The short description and per<strong>for</strong>mance <strong>of</strong> this detector will be presented. High time resolution was obtained <strong>for</strong> <strong>for</strong> pp interactions about 40 ps and 20ps <strong>for</strong> heavy ions. The detector is used <strong>for</strong> online luminosity monitoring with fast feedback to accelerator team. T0 detector supplies five different trigger signals <strong>for</strong> background rejection and physics selections. The detector shows very good per<strong>for</strong>mance and stable work at high interaction rate up to 400 KHz. 91