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Ornella Palamara (WIN09 Chair)14/09/2009, 08:45
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Riccardo Barbieri14/09/2009, 09:00
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Roberto Tenchini14/09/2009, 09:45
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Gino Isidori14/09/2009, 11:00
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Tim Gershon14/09/2009, 11:45
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Sandhya Choubey14/09/2009, 15:30
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Art McDonald14/09/2009, 16:15
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Neal Weiner14/09/2009, 17:30
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Bruno Serfass14/09/2009, 18:15
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Pier Oddone15/09/2009, 09:00
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David Schmitz15/09/2009, 09:30
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Cristiano GALBIATI15/09/2009, 10:00
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Giulia Ricciardi15/09/2009, 11:00
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Andrei Nikiforov15/09/2009, 11:00
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Mu-Chun Chen15/09/2009, 11:00Neutrino PhysicsI will review recent developments in theoretical models for neutrino masses and mixing. Emphases are given to models based on finite group family symmetries in which Tri-bimaximal neutrino mixing pattern is generated. In particular, I will describe one recent model based on grand unification, in which both the Tri-bimaximal neutrino mixing and realistic CKM matrix are generated. The prediction...Go to contribution page
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Marcella Bona15/09/2009, 11:25Electro Weak Symmetry Breaking
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Georges Vasseur15/09/2009, 11:30Weak Decays, CP violation and CKM
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Martin HIRSCH15/09/2009, 11:30Neutrino PhysicsMajorana neutrino masses can be generated in a variety of ways. They could be due to some variant of the seesaw mechanism or be generated radiatively. Also within supersymmetric models neutrino masses can be non-zero if R-parity is broken. This talk discusses different signals of various neutrino mass models one can expect for the LHC experiments.Go to contribution page
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Ennio Salvioni15/09/2009, 11:50
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Chih-Hsiang Cheng15/09/2009, 12:00Weak Decays, CP violation and CKM
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PROBIR ROY15/09/2009, 12:00Neutrino PhysicsWithin the type-I seesaw framework with three heavy right chiral neutrinos and in the basis where the latter and the charged leptons are mass diagonal, we investigate the effects of mu-tau symmetry as well as trbimaximal mixing on the maximally allowed four zero neutrino Yukawa textures which had already led to a predicitve and highly constrained theoretical scheme. A drastic reduction of the...Go to contribution page
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Itaru Shimizu15/09/2009, 15:30Neutrino PhysicsThe KamLAND experiment searched for the oscillation of anti-neutrinos emitted from distant nuclear reactors. We observed the anti-neutrino spectral distortion, which was a piece of evidence of neutrino oscillations. Due to their clear spectral distortion, the neutrino mass difference was determined with 2.8% precision. In the near future, we will have a sensitivity also to the low energy solar...Go to contribution page
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Tagir Aushev15/09/2009, 15:30
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Sascha Mehlhase15/09/2009, 15:30Electro Weak Symmetry Breaking
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Alexandre Sousa15/09/2009, 15:50Neutrino PhysicsThe Main Injector Neutrino Oscillation Search (MINOS) long baseline experiment measures a muon neutrino beam in two locations: a Near detector at Fermilab, close to beam production, and a Far detector, 735 km downstream, in Northern Minnesota. Comparisons of the observed energy spectrum at the Far detector with the expectation derived from the Near detector measurement allow MINOS to study...Go to contribution page
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Seung Lee15/09/2009, 15:55
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Matthew Moulson15/09/2009, 16:00Weak Decays, CP violation and CKM
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Mayly Sanchez15/09/2009, 16:10Neutrino PhysicsMINOS is a long baseline neutrino oscillation experiment designed to make precision measurements of the neutrino mixing parameters associated with the atmospheric neutrino mass splitting. Using a neutrino beam from the Main Injector (NuMI) facility at Fermilab, it compares the neutrino energy spectrum for neutrino interactions observed in two large detectors located at Fermilab and in the...Go to contribution page
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Gilad Perez15/09/2009, 16:20Electro Weak Symmetry Breaking
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Georgia Karagiorgi15/09/2009, 16:30Neutrino PhysicsMiniBooNE is a short-baseline experiment located at Fermilab, sensitive to muon (anti)neutrino to electron (anti)neutrino appearance and muon (anti)neutrino disappearance oscillations at high $\Delta m^2~$ 1 eV$^2$. These oscillation searches have been motivated by the 3.8$\sigma$ excess of electron antineutrino events in a muon antineutrino beam observed by the LSND experiment in 1995. In...Go to contribution page
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Yasuhiro Nakajima15/09/2009, 17:30Neutrino PhysicsNeutrino oscillation is a probe for new physics not included in the Standard Model. We search for muon neutrino disappearance at \Delta m^2 ~ 1 eV^2 using the Fermilab Booster Neutrino beamline and two experiments, SciBooNE and MiniBooNE. The neutrino fluxes are measured at SciBooNE and MiniBooNE detectors, located at 100 m and 540 m downstream from the neutrino production target,...Go to contribution page
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Sandra Leone15/09/2009, 17:30Weak Decays, CP violation and CKM
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Akitaka Ariga15/09/2009, 17:50Neutrino PhysicsThe OPERA experiment is a long baseline neutrino experiment aiming at the first observation of the appearance of a new flavor signal predicted by the neutrino flavor-mixing oscillations hypothesis. The OPERA is designed to detect a tau neutrino appearance in the pure muon neutrino beam from CERN to Gran Sasso (CNGS beam). The target has a modular structure made of units based on Emulsion Cloud...Go to contribution page
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Anze Zupanc15/09/2009, 18:00Weak Decays, CP violation and CKM
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Mr Teppei Baba (Tokai university)15/09/2009, 18:10Neutrino PhysicsTo find hidden structure of flavor neutrino mass matrix, we study properties of flavor neutrino mass satisfying the strong scaling Ansatz (SSA) that predicts non maximal $\nu_2 - \nu_3$ mixing, vanishing $U_{e3}$ and inverted mass hierarchy. However, we find another possibility of SSA that tiny deviation from this Ansatz permits us to realize normal mass hierarchy and tiny value of...Go to contribution page
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MyeongJae Lee15/09/2009, 18:30Weak Decays, CP violation and CKM
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Kang Soon Park16/09/2009, 09:00Neutrino PhysicsRENO(Reactor Experiment for Neutrino Oscillation), is under construction to measure the smallest neutrino mixing angle theta_13 using antineutrinos emitted from the Yonggwang power plant in Korea with world-second largest thermal power output of 16.4 GW. A high precision measurement of reactor neutrino oscillation can be achieved by two identical detectors. Each detector consists 16-ton...Go to contribution page
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Massimo Casarsa16/09/2009, 09:00Electro Weak Symmetry BreakingSince the beginning of Run II the Fermilab Tevatron has delivered 6.9 fb-1 of proton-antiproton collisions at a center of mass energy of 1.96 TeV. Using the collected dataset the CDF and D0 experiments are pursuing extensive Physics programs which have as a main goal the search for a Standard Model Higgs boson. The contribution will review the CDF and D0 results on the direct Standard Model...Go to contribution page
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Damir Becirevic16/09/2009, 09:00Weak Decays, CP violation and CKM
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Steve kettell16/09/2009, 09:20Neutrino PhysicsThe Daya Bay experiment aims to measure the last unobserved neutrino mixing angle theta_13 with a sensitivity of sin^2 (2 theta_13) < 0.01 at 90% C.L. The experiment will measure the flux and energy spectrum of reactor antineutrinos through the inverse beta-decay reaction on protons in eight detectors in three underground sites at different distances from the reactor cores. An overview...Go to contribution page
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Gerhard Ecker16/09/2009, 09:30Weak Decays, CP violation and CKM
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Alberto Graziano16/09/2009, 09:35Electro Weak Symmetry Breaking
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Marcos Dracos16/09/2009, 09:40Neutrino PhysicsThe Double Chooz neutrino oscillation experiment will perform a highly sensitive measurement of the neutrino mixing angle ฮธ13. The Double Chooz project will utilize two detectors, a near one providing the unoscillated neutrino flux coming from the two reactor cores of the Chooz nuclear plant (France), and a far detector measuring the neutrino flux after oscillation. The signal comparison...Go to contribution page
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Giancarlo D'Ambrosio16/09/2009, 10:00Weak Decays, CP violation and CKM
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Hidekazu Kakuno16/09/2009, 10:00Neutrino PhysicsT2K (Tokai-to-Kamioka) is a second generation long baseline neutrino experiment utilizing a newly built neutrino source with a MW class high energy proton accelerator complex (J-PARC neutrino facility), a near neutrino detector (ND280) to characterize the neutrino beam 280 meters from the source, and Super-Kamiokande as the far detector at 295 km. The primary motivation for T2K is...Go to contribution page
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Bjoren Duling16/09/2009, 11:00Weak Decays, CP violation and CKM
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Pierluigi Belli16/09/2009, 11:00The highly radiopure about 250 kg NaI(Tl) DAMA/LIBRA set-up is running at the Gran Sasso National Laboratory of the I.N.F.N.. Results exploiting the model independent annual modulation signature for Dark Matter particles in the galactic halo are presented (exposure of 0.53 ton x yr). The DAMA/LIBRA data confirm the evidence for the presence of Dark Matter particles in the galactic halo as...Go to contribution page
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Mayly Sanchez (Argonne National Laboratory)16/09/2009, 11:00Neutrino PhysicsNOvA is a next generation long baseline neutrino experiment. It has been designed to study electron neutrino appearance in a muon neutrino beam using a totally active, segmented, liquid scintillator detector located off the Fermilab NuMI beam axis. Construction of a prototype Near detector will commence this year and will be placed in the existing NuMI beam during 2010. The Far Detector will...Go to contribution page
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Takuya Hasegawa16/09/2009, 11:20Neutrino PhysicsAs the first phase experiment utilizes J-PARC(Japan Proton Accelerator Research Complex) neutrino facility, T2K(Tokai to Kamioka Long Baseline Neutrino Experiment) starts operation. T2K is supposed to give critical information, which guides the future direction of the neutrino physics. I will discuss possible future discovery experiment next to T2K. Talk will focus especially on describing...Go to contribution page
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Sebastian Arrenberg16/09/2009, 11:25The Cryogenic Dark Matter Search Experiment (CDMS) employs a total of 30 Germanium and Silicon Detectors at the Soudan Underground Laboratory to detect weakly interacting massive particles (WIMPs) via their elastic scattering from the target nuclei. Previous CDMS results, released in February 2008, yielded a world-leading limit for spin-independent WIMP-nucleon cross sections for WIMP masses...Go to contribution page
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Andre Rubbia16/09/2009, 11:40Neutrino PhysicsThe LAGUNA design study is presently assessing the feasibility of a new large underground infrastructure in Europe for next generation neutrino and proton decay search experiment I will describe the status of LAGUNA and discuss possible options for future long baseline experiments coupled to a potential future program at CERN.Go to contribution page
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Mitchell Soderberg16/09/2009, 12:00
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Terrence Hart16/09/2009, 15:30Neutrino PhysicsA Neutrino Factory producing intense neutrino beams from muon decays is an intriguing possibility for the next generation of neutrino experiments. Determination of the neutrino mass hierarchy, precision measurements of the neutrino mixing parameters, and observation of CP violation in the neutrino sector are among the many studies possible with a Neutrino Factory. A Neutrino Factory can also...Go to contribution page
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Antonio Limosani16/09/2009, 15:30Weak Decays, CP violation and CKM
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Dario Grasso16/09/2009, 15:30The Fermi Large Area Telescope (LAT) has recently provided the measurement of the high energy (20 GeV to 1 TeV) cosmic ray electrons plus positrons (CRE) spectrum with unprecedented accuracy. The spectrum shows no prominent features and it is significantly harder than that inferred from several previous experiments. While the reported Fermi-LAT data alone can be interpreted in terms of a...Go to contribution page
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Alain Blondel16/09/2009, 15:50Neutrino Physics"R&D and Design Studies towards novel neutrino beams are advancing well in Europe. International R&D experiments (HARP, MERIT, MICE, EMMA) have been and are succesfully being performed. Design studies of high power upgrades of existing (ISIS) or planned (SPL) proton machines, of detector concepts and sites (Laguna) and of high intensity beams (EUROnu) are in progress. EUROnu aims, in...Go to contribution page
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Paolo Papini16/09/2009, 15:55
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Silke Nelson16/09/2009, 16:00Weak Decays, CP violation and CKM
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Vittorio Palladino16/09/2009, 16:10Neutrino PhysicsMuon ionization cooling provides the only practical solution to prepare high brilliance beams necessary for a neutrino factory or muon colliders. The muon ionization cooling experiment (MICE)* is under development at the Rutherford Appleton Laboratory (UK). It comprises a dedicated beam line to generate a range of input emittance and momentum, with time-of-flight and Cherenkov detectors...Go to contribution page
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Matthew Reece16/09/2009, 16:20
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Shoichi Uchinami16/09/2009, 16:30Neutrino PhysicsIn neutrino oscillation with non-standard interactions (NSI) the system is enriched with CP violation caused by phases due to NSI in addition to the standard lepton Kobayashi-Maskawa phase $ยฅdelta$. In this paper we show that it is possible to disentangle the two CP violating effects by measurement of muon neutrino appearance by a near-far two detector setting in neutrino factory...Go to contribution page
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Franco Giuliani16/09/2009, 17:30The large difference between the time constants of the two scintillation pulse com- ponents of a noble liquid like liquid Argon or Neon provide a very reliable correlation between pulse shape and type of event. This pulse shape discrimination already pro- vides the power of rejecting a background $10^{8}-10^{9}$ times larger than the signal. A 400 kg LAr detector, MiniCLEAN, is...Go to contribution page
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Olga Lalakulich16/09/2009, 17:30Neutrino PhysicsModern long-baseline neutrino experiments, aiming at precise measurements of the neutrino oscillation parameters require a thorough understanding of neutrino cross sections in medium-energy region. An overview of neutrino-nucleon and neutrino-nucleus cross sections in a few GeV region is presented. Cross section on a nucleon target is expressed as a sum of quasi-elastic, resonance and DIS...Go to contribution page
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Rainer Wanke16/09/2009, 17:30Weak Decays, CP violation and CKM
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Darren Grant16/09/2009, 17:55IceCube is a cubic kilometer neutrino telescope under construction at the South Pole, a successor to the first-generation AMANDA telescope designed to the search for astrophysical neutrino sources. IceCube is now three quarters complete with the full detector expected to be operating in early 2011. Data taken with the partially built detector already provides world-leading...Go to contribution page
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Mauro Piccini16/09/2009, 18:00Weak Decays, CP violation and CKM
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Yoshinari Hayato16/09/2009, 18:00Neutrino PhysicsRecent experimental studies of neutrino oscillation require more precise knowledge of the neutrino-nucleus scatterings. Therefore, several experiments to study neutrino nucleus-scattering experiments have been performed. In this presentation, I will report the recent results of neutrino scatterings from SciBooNE and MiniBooNE.Go to contribution page
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3. Hadro-production measurements for the T2K experiment with the NA61/SHINE detector at the CERN SPSClaudia Christina Strabel16/09/2009, 18:20Neutrino PhysicsIn this talk the NA61/SHINE detector will be presented, which is a large acceptance hadron spectrometer at the CERN SPS. It allows for a precise study of the particle production from the interactions of a 31 GeV/c proton beam on a Carbon target in order to predict the neutrino flux of the T2K experiment at J-PARC, Japan. Requirements for the T2K experiment will be discussed together with the...Go to contribution page
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Zurab Berezhiani16/09/2009, 18:20
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Steve Boyd16/09/2009, 18:40
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Angelo Nucciotti (Dip. Fisica, Univ. di Milano-Bicocca and INFN Sez. di Milano-Bicocca)17/09/2009, 09:00Neutrino PhysicsNeutrinoless double beta decay is a powerful tool to investigate the fundamental nature of neutrinos and to determine the absolute neutrino mass scale. To date, CUORE is the only fully approved next generation 1-ton size experiment with the goal of exploring the inverted hierarchy region for the neutrino masses. CUORE is an array of 988 TeO2 cryogenic detectors containing 200 kg of Te-130 -...Go to contribution page
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Jure Zupan17/09/2009, 09:00We consider the hypothesis that Dark Matter (DM) has tree-level interactions only with leptons. Such a framework, where DM recoils against electrons bound in atoms, has been proposed as an explanation for the annually modulated scintillation signal in DAMA/LIBRA versus the absence of a signal for nuclear recoils in experiments like CDMS or XENON10. However, even in such a leptophilic...Go to contribution page
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Alejandro Ibarra17/09/2009, 09:00Weak Decays, CP violation and CKM
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Luciano Pandola17/09/2009, 09:25Neutrino PhysicsNeutrinoless double-beta-decay could be the key to understanding the nature of the neutrino: if observed it would prove its Majorana-nature and the half-life of the decay would be a direct measure of the yet unknown absolute scale of the neutrino mass. The GErmanium Detector Array (GERDA) experiment at the INFN, Gran Sasso Laboratory, Italy, is designed to investigate the...Go to contribution page
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Alessandro Baldini17/09/2009, 09:40Weak Decays, CP violation and CKM
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Karol Lang17/09/2009, 09:50Neutrino PhysicsThe NEMO-3 experiment, located in the Modane Underground Laboratory, is searching for neutrinoless double beta decay since 2003. We will present the latest results for seven isotopes used on NEMO-3: 48Ca, 96Zr, 82Se, 100Mo, 116Cd, 130Te and 150Nd. We observe no evidence for neutrinoless double beta decay and based on 100Mo data set an upper limit on the effective Majorana neutrino...Go to contribution page
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Ettore Segreto17/09/2009, 09:50
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Monica Sisti17/09/2009, 11:00
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Riccardo Cenci17/09/2009, 11:00Weak Decays, CP violation and CKM
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Claudia Lazzaro17/09/2009, 11:00The goal of the ArDM experiment is a direct detection of weakly interacting massive particles (WIMP) in the universe using a double phase argon TPC. This detector has a fiducial volume of about 1 ton of liquid argon and the detection is done independently by collecting the scintillation light as also by the ionization charge. The Argon scintillation light has to be converted with...Go to contribution page
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Daniel McKinsey17/09/2009, 11:25Dark MatterThe LUX dark matter experiment is a 350 kg two-phase xenon time projection chamber. There are several advantages of liquid xenon for WIMP detection: high scintillation yield, high ionization yield, low intrinsic radioactivity, easy purification, effective gamma-ray self-shielding, and significant A^2 enhancement of the spin-independent WIMP cross-section. LUX is currently under construction...Go to contribution page
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Peter Fierlinger17/09/2009, 11:30Weak Decays, CP violation and CKM
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Steven Biller17/09/2009, 11:30
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Cristiano Galbiati17/09/2009, 11:50I will discuss progress on procurement of large quantities of depleted argon from underground sources in the US, and the how this could improve future dark matter searches with argon detector. I will also discuss results from R&D efforts on two-phase argon detectors in the US and future plans.Go to contribution page
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Itaru Shimizu17/09/2009, 12:00
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Andrzej Szelc17/09/2009, 12:15The use of liquid noble gas detectors in the search for Dark Matter is quickly becoming more widespread and they are already playing one of the major parts in the field. One of the possible signatures of the presence of Dark Matter is the so called annual modulation effect, possibly already observed by the DAMA collaboration. The liquid noble gas detectors are generally tailored to observe...Go to contribution page
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Aldo Ianni17/09/2009, 12:15
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Kamales Kar18/09/2009, 09:00Neutrino PhysicsThe effect of collective flavor oscillations of neutrinos driven by neutrino-neutrino interaction at the very high density region of core collapse supernovae controls the emitted flux of neutrinos of different flavors. In the process one or more swaps of the flavors for both neutrinos and antineutrinos take place depending on the initial neutrino flux and distributions, particularly for...Go to contribution page
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Jaap Panman18/09/2009, 09:00Weak Decays, CP violation and CKM
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Jan Schumacher18/09/2009, 09:00
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Giovanni Fiorentini18/09/2009, 09:20
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Phillip URQUIJO18/09/2009, 09:25
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Marcello GIORGI18/09/2009, 09:30Weak Decays, CP violation and CKM
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Robert McElrath18/09/2009, 09:50Electro Weak Symmetry BreakingTheories of natural Electroweak Symmetry Breaking can involve light higgses. These imply significant changes in search strategies at the Tevatron, LHC, and B-factories. I will review some non-standard Higgs scenarios which involve higgs-to-higgs decays, and the experimental signatures thereof.Go to contribution page
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Yasuo Takeuchi18/09/2009, 09:50Neutrino Physics
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Masanori Yamauchi18/09/2009, 10:00Weak Decays, CP violation and CKM
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Fanny DUFOUR18/09/2009, 10:10
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Steve kettell18/09/2009, 11:00Weak Decays, CP violation and CKMThe extremely rare decay K+ -> pi+ neutrino anti-neutrino has been studied for the last 20 years with the E787 and E949 experiments and the high-intensity proton beam of the AGS accelerator at Brookhaven National Laboratory. The E949 experiment previously reported results above the K+ -> pi+pi0 peak, in the pion momentum region [211,229] MeV/c {Phys.Rev.Lett.93:031801(2004);...Go to contribution page
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Elena Guardincerri18/09/2009, 11:00Neutrino PhysicsBorexino is a liquid scintillator, solar neutrino detector running underground at the Laboratori Nazionali del Gran Sasso, Italy. Thanks to the extreme radio-purity achieved throughout its whole set-up Borexino is capable of detecting solar neutrinos below 2 MeV. Among the main results obtained so far are the first measurement of the 7Be solar neutrinos flux, whose value is in agreement...Go to contribution page
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Emilio Migneco18/09/2009, 11:20
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Gino Isidori18/09/2009, 11:25
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Augusto Ceccucci18/09/2009, 11:30Weak Decays, CP violation and CKM
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Robert CIESIELSKI18/09/2009, 11:50Electro Weak Symmetry Breaking
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Annarita Margiotta18/09/2009, 11:50Neutrino PhysicsANTARES is an underwater neutrino telescope, located about 2500 m under the sea, 40 km off the coast of Toulon/France. Consisting of about 900 optical modules it is currently the largest neutrino detector in the northern hemisphere and has been taking data in its final configuration since May 2008. In this talk the physics potential and the detection technique are described and first results...Go to contribution page
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Taku Yamanaka18/09/2009, 12:00The purpose of the J-PARC E14 KOTO experiment is to search for new physics beyond the standard model that enhances the branching ratio of the \(K_L \to \pi^0 \nu \bar{\nu}\) decay. The experiment looks for two and only two photons from the decay that have a finite transverse momentum. The detector consists of a pure CsI calorimeter and hermetic photon veto counters placed in a vacuum...Go to contribution page
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Adam Falkowski18/09/2009, 14:00DG1 - Summary and PerspectivesGo to contribution page
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Yves Sirois18/09/2009, 14:45DG1 - Summary and perspectivesGo to contribution page
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Gerhard Buchalla18/09/2009, 15:30
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Marco Sozzi18/09/2009, 16:15
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Hiroshi Nunokawa18/09/2009, 17:30DG3 - Summary and perspectivesGo to contribution page
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Bonnie Fleming18/09/2009, 18:00
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Oliviero Cremonesi18/09/2009, 18:30DG3 - Summary and perspectivesGo to contribution page
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Adam Falkowski19/09/2009, 09:00
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Daniel McKinsey19/09/2009, 09:45
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Herbert PIETSCHMANN19/09/2009, 10:30
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Ornella Palamara19/09/2009, 10:40
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Dr Rukmani Mohanta (University of Hyderabad)Weak Decays, CP violation and CKMThe recent observation of the mass difference in B_s system seems to be not in complete agreement with the corresponding standard model value. We consider the model with an extra vector like down quark to explain this discrepancy and obtain the constraints on the new physics parameters. Thereafter, we show that with these new constraints, this model can successfully explain other observed...Go to contribution page
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Andrew SonnenscheinDark Matter
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Dr Anjan Giri (National Institute of Technology, Rourkela, India)We study the effect of non-universal Z' boson in the decay modes B -> K pi. In the standard model these modes receive dominant contributions from b -> s QCD penguins. Therefore, in this limit one expects $S_{\pi^0 K^0} \approx \sin 2 \beta $, $A_{\pi^0 K^0} \approx 0$ and $A_{\pi^0 K^-} \approx A_{\pi^+ K^-}$. The corrections due to the presence of small non-penguin contributions is found to...Go to contribution page
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Weak Decays, CP violation and CKM
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Dr Mitchell Soderberg (Yale University)Neutrino PhysicsLiquid Argon Time Projection Chamber (LAr TPC) detectors are well suited to study neutrino interactions, and are an intriguing option for future massive detectors capable of measuring the parameters that characterize neutrino oscillations. These detectors combine fine-grained tracking with calorimetry, allowing for excellent imaging and particle identification ability. The ability of liquid...Go to contribution page
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Massimiliano GrazziniElectro Weak Symmetry Breaking
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Christina HagemannNeutrino PhysicsThe EXO collaboration aims to measure the regular double beta of 136Xe and carry out a sensitive search for neutrinoless double beta decay. Discovery of the neutrinoless decay would provide information on the neutrino mass scale and provide the first measurement of a lepton number violating process. The status of the EXO efforts will be provided including the latest update for the 200 kg...Go to contribution page
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Blair EdwardsThe results from the first science run of ZEPLIN-III will be presented which have resulted in an upper limit to the WIMP-nucleon spin-independent elastic scattering cross-section of 8.1x10(-8)pb. The instrument performance charateristics and behaviour will be reviewed. The status of preparations for the second science run will be givenGo to contribution page
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Lucia Votano (LNGS Director)
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Pier Oddone (Fermilab Director)
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