PPT-Muon Neutrino Charged Current Quasi Elastic Scattering in the

MINERvA Experiment Tammy Walton New Perspectives Meeting Hampton University June 1011 2013 1 Outline Motivation Overview of the Analysis Conclusions 2 3 n m n m JA Formaggio and GP Zeller Rev Mod Phys 84 13071341 2012. Particle Detection:. Part 2. Overview. Lecture 1:. Concepts of particle detection: what can we detect?. Basic design of particle detectors. Energy loss of charged particles in matter: Bethe Bloch formula. 2. Polarized Measurement of the Electric Form Factor of the Neutron – E02-013. Presented by. Jonathan Miller. For the Hall A E02-013 Collaboration. 6/14/2008. Outline. Collaboration. Electric Form Factor of the Neutron. MINERvA. Kevin McFarland. University of Rochester. NuINT11, Dehradun. 8 March 2011. ν. Goddess′. μ. To India . via. Indiana. Thank you to the organizers . for their efforts to allow me to attend . of Neutrinos. ニュートリノのヘリシティ. M.. . Goldhaber. , L. . Grodzins. and A. W. . Sunyar. Brookhaven National Laboratory. Phys. Rev. . . 109 (1958) 1015.. Contents. 1. Introduction. MINERvA is studying neutrino interactions in unprecedented detail on a variety of different nuclei. Low . Energy (LE) . Beam Goals: . S. tudy . both signal and background reactions relevant . to oscillation experiments (current and future). Alan Bross. N u F a c t 0 9. From . SuperBeams. to Neutrino Factories. Pre-Ramble. Neutrino Factory means different things to different people. Not so much for . SuperBeams. I will be talking about a muon-based Neutrino Factory as opposed to a . MINERvA is studying neutrino interactions in unprecedented detail on a variety of different nuclei. Low . Energy (LE) . Beam Goals: . S. tudy . both signal and background reactions relevant . to oscillation experiments (current and future). Ken Herwig. Instrument and Source Division. Neutron Sciences Directorate. Oak Ridge National Laboratory. August 13, 2016. OUTLINE. Background – the incoherent scattering cross section of H. Neutrons and QENS. Neutron Scattering. Ken Herwig. Instrument . and Source Division. Neutron . Sciences . Directorate. Oak Ridge . National Laboratory. June 22, 2015. OUTLINE. Background – the incoherent scattering cross section of H. Simulation Study of Muon Scattering For Tomography Reconstruction D. Mitra, A. Banerjee, S. White, S. Waweru, R. Hoch K. Gnanvo M. Hohlmann Florida Institute of Technology 10/27/2009 1 IEEE NSS-MIC 2009, Orlando, FL 1. The basis of the potential of . muon. beams. Muon. mass:. 200. . m. e. ~ . m. m. ~ 0.1. . m. p. Muon. decay:. n. e. , . n. m. Precisely known energy spectrum. Energy frontier:. No . brem. -/beam-. Neutron Scattering. Ken Herwig. Instrument . and Source Division. Neutron . Sciences . Directorate. Oak Ridge . National Laboratory. June 22, 2015. OUTLINE. Background – the incoherent scattering cross section of H. LHC, MAP, and LEMC. David . Neuffer. July 2018. 2. Outline. Next Heavy Lepton Collider . up to ~14 . TeV. in LHC tunnel. Needs muon source. PS or new MW proton . Linac. /storage ring. cooling …. or LEMC??. a+. 208. Pb Elastic Scattering. M . Nure. . Alam. Abdullah. , M Zahid Hasan, . Sinthia. . Binte. . Kholil. and Dipika Rani . Sarker. Department of Physics, Jagannath University, Dhaka-1100 Bangladesh.