PPT-Muon Neutrino Charged Current Quasi Elastic Scattering in the

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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

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Muon Neutrino Charged Current Quasi Elastic Scattering in the: Transcript

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. Atoms in magnetic field. orbiting electron behaves like current loop . .  magnetic moment . μ. = current x area . interaction energy = . μ. ·B. (both vectors!) = . μ. ·B. . loop current = -. Miguel A. Gonzalez. Institut. Laue-. Langevin. (Grenoble, France). gonzalezm@ill.eu. Outline. General remarks and reminders. The main equations and their physical meaning. QENS models for translational diffusion and localized motions. 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 . MathematicsSubjectClassication.54C08.Keywordsandphrases.m-structure,(;s)-continuous,-quasi-irresolute,weakly-irresolute,-quasi-irresolute,m-compact,S-closed,m-quasi-closedgraph.c\r2005MathematicaM electron, and electron-neutrino have =+1; their anti-particles have =-1; muon, and muon-neutrino have =+1; their anti-particles have THUS, there should be two types of neutrinos: electron-kind and muo . True Experiments. Characteristics. Threats to validity controlled by experiments. Threats not controlled by experiments. Obstacles to true experiments in the field. . Quasi-experiments. The logic of quasi-experiments . Yong Ma. Sparse model space for projected Hessian. Quasi-Newton FWI. Eigenvector (largest . eigenvalue. ). Eigenvector (smallest . eigenvalue. ). 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 . Research Objective. Show direct cause & effect. Study relationships among variables for existing groups. Explain outcomes after the fact. Type of Design. True Experiment. Quasi-Experiment. Cross-Sectional. Cioli Barazandeh, Angel . Gutarra-leon. and Walerian Majewski. Mentor: . Walerian. . Majewski. , Department of Physics . Northern Virginia Community College, Annandale, VA . Experiments. Hello, and welcome to my Presentation!. 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. 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-. 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.

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