[PDF] Top 20 Estudio de la prevalencia del agujero macular

... The NA61/SHINE experiment [1] is a multi-purpose fixed target experiment at the Super Proton Synchrotron (SPS) of the European Organization for Nuclear Research ...The strong ... See full document

... The NA61/SHINE experiment at the CERN SPS [1] pursues a two-fold physics programme: (1) measurements of hadron spectra in hadron-nucleus collisions for neutrino and cosmic rays ... See full document

... summarized results from the multi- purpose experiment NA61 / SHINE at the CERN ...by NA61 / SHINE are valuable for the tuning of hadronic interaction models ... See full document

... the NA61/SHINE experiment at the CERN Super Proton ...spectrometer, SHINE aims to accomplish a number of physics goals: measuring spec- tra of identified hadrons in hadron-nucleus ... See full document

... The SPS Heavy Ion and Neutrino Experiment (NA61 / SHINE) [1] is a fixed-target experi- ment located at the CERN Super Proton Synchrotron ...The NA61 / SHINE detector is ... See full document

... the NA61 / SHINE fixed target experiment is to uncover properties of the onset of deconfinement by systematic study of collision energy and nuclear mass dependence of hadron production in the region of ... See full document

... / SHINE is a multi-purpose experimental facility to study hadron production in hadron-proton, hadron-nucleus and nucleus-nucleus collisions at the CERN Super Proton ...of strong interactions, ... See full document

... the strong interaction programme of the experiment is to discover the Critical Point (CP) [2] of strongly interacting matter and study the properties of the onset of deconfinement (OD) [3, ...studying ... See full document

... / SHINE [1] is a fixed target experiment at the CERN SPS accelerator ...Its strong in- teractions programme is a continuation and extension of the NA49 experiment [2], following ... See full document

... The NA61 / SHINE experiment [1] is a multi-purpose fixed target experiment at the Super Proton Synchrotron (SPS) of the European Organization for Nuclear Research ...The strong ... See full document

... The NA61/SHINE apparatus is a wide-acceptance hadron spectrometer at the CERN ...published results. Since 2007 pilot run the experiment has been updated with a new forward ... See full document

... Abstract. NA61/SHINE is a fixed target experiment designed to study hadron-proton, hadron-nucleus and nucleus-nucleus interactions at the CERN ...the results from pion-carbon ... See full document

... The NA61/SHINE experiment studies hadron production in hadron+hadron, hadron+nucleus and nucleus+nucleus ...The strong interactions program has two main purposes: study the properties ... See full document

... All results have been fully corrected with the Monte ...The results are presented in the form of differential multiplicities as required for the T2K ...the results with various MC model predictions ... See full document

... with a momentum bite of ∼ 1%. Only 6% of the hadrons are charged kaons (unseparated beam). It is crucial to make a positive identification of the minority particles of interest, kaons, in the high rate beam environment ... See full document

... Independently, an individual thick MIMOSA-26 sensor was operated directly in the heavy ion beam. This test aimed to observe the response of the sensor to heavy ions and to spot the probability of latch-ups and ... See full document

... background from the decays K + → μ + ν μ (on the left), K + → πππ (on the right) and K + → π + π 0 (a peak from this decay splits the signal region into 2 ... See full document

... The results confirm the feasibility of using CMOS sensor based vertex detectors in a fixed target heavy ion environment and can also be considered as a success- ful test of the building blocks ... See full document

... photoemission from various GaAs-based semiconductor photo-cathodes, using circu- larly polarized laser light ...violating experiment from 20 µA to 100 ... See full document

... We have also extract an improved direct limit on the CKM matrix element 0 . 81 < |V tb | ≤ 1 at 95% C.L. and a limit of |V tb | < 0 . 59 for a high mass fourth generation bottom quark assuming unitarity of the ... See full document