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Dr Cecilia Voena (INFN Roma)30/01/2015, 17:00Applications and InstrumentationsShort ContributionHadron therapy is a technique for cancer treatment that exploits ion beams (mostly protons and carbons). A critical issue is the monitoring accuracy of the dose released by the beam to the tumor and to the surrounding tissues. We present the design of a dual-tracking device capable of online dose monitor through the detection of prompt photons and charged particles produced by the...Go to contribution page
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Johannes Rauch30/01/2015, 17:20Short ContributionWe will present a summary of the activity of the TU Munich's Belle and Belle II groups concerning the decay of charm mesons D+ and D0 into multiple hadrons. A summary of analytical techniques for the amplitude analysis of three- and four-pion final states will be presented.Go to contribution page
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Ruediger Haake (University of Muenster)30/01/2015, 17:40Short ContributionHighly energetic jets are sensitive probes for the kinematics and the topology of nuclear collisions. Jets are collimated sprays of charged and neutral particles, which are produced in the fragmentation of hard scattered partons in an early stage of the collision. The measurement of jet spectra in p-Pb collisions provides an important way of quantifying the effects of cold nuclear matter in...Go to contribution page
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Mr Leonard Koch30/01/2015, 18:00Short ContributionThe Belle II experiment at KEK in Tsukuba, Japan will perform studies with B mesons with a factor $\times 40$ increased luminosity compared to the Belle experiment. One of the main goals of Belle II is the search for physics beyond the Standard Model, for example in rare B meson decays described by with loop diagrams. Detecting $B$ mesons frequently involves the detection of $K_{S}^{0}$...Go to contribution page
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30/01/2015, 18:20
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Prof. Luciano Moretto (UCB and LBNL)30/01/2015, 18:40Short ContributionThe log-lin dependence of the hadronic density of states with mass is known as the Hagedorn. A similar dependence is observed, at energies a factor of one thousand lower,in most atomic nuclei. The latter behavior is due to a 1st order phase transition from a superfluid to an ideal gas of quasi particles. This transition is consistent with the BCS Hamiltonian treated within a microcanonical...Go to contribution page
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