'Scattering angle' diaporamas de présentation

Quantum Interference as the Source of Stereo-Dynamic Effects in NO-Rare Gas Scattering

Quantum Interference as the Source of Stereo-Dynamic Effects in NO-Rare Gas Scattering. A. Gijsbertsen, C.A. Taatjes * , D.W. Chandler * , H.V. Linnartz and S. Stolte. Department of Physical Chemistry, De Boelelaan 1083, 1081 HV Amsterdam. vrije Universiteit am sterdam.

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Kinetic Theory for Gases and Plasmas: Lecture 2: Plasma Kinetics

Kinetic Theory for Gases and Plasmas: Lecture 2: Plasma Kinetics. Russel Caflisch IPAM Mathematics Department, UCLA. Review of First Lecture. Velocity distribution function Molecular chaos Boltzmann equation H-theorem (entropy) Maxwellian equilibrium Fluid dynamic limit DSMC

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Geant4 Milagro Simulation

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Lectures 10-11

Lectures 10-11. Particle interactions with matter. 9.0 Overview. 9.3 Photons in matter Overview Photoelectric effect Raleigh scattering Compton scattering Pair production Comparison of cross-sections Z & A dependence of cross-sections

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Lectures 9-10

Lectures 9-10. Particle interactions with matter. 9.0 Overview. 9.3 Photons in matter Overview Photoelectric effect Raleigh scattering Compton scattering Pair production Comparison of cross-sections Z & A dependence of cross-sections

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DNB Day/Night Reflectance Salar de Uyuni , Bolivia Update 5/8/2013

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Decay asymmetry in non-mesonic weak decay of light L hypernuclei

Oct./13/2006 HYP2006@Mainz Univ. Decay asymmetry in non-mesonic weak decay of light L hypernuclei. T.Maruta KEK, JSPS fellow. KEK-PS E462/E508 collaborations. L polarization in n( p + , K + ) L. 1.05GeV/ c p +. accepted. P. L. p /p. E278. ?. K +. p +. K + scattering angle( j K ).

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The R-matrix Method for oriented molecules

The R-matrix Method for oriented molecules. e -. Jonathan Tennyson University College London. Jonathan Tennyson Department of Physics and Astronomy University College London. Outer region. Inner region. UCL, May 2004. Montreal Oct 2009. Lecture course on open quantum systems.

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Multiscale Methods for Coulomb Collisions in Plasmas

Multiscale Methods for Coulomb Collisions in Plasmas. Russel Caflisch IPAM Mathematics Department, UCLA. Collaborators. UCLA Richard Wang Yanghong Huang Livermore Labs Andris Dimits Bruce Cohen U Ferrarra Lorenzo Pareschi Giacomo Dimarco. Outline. Coulomb collision in plasmas

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Simulation Study of Muon Scattering For Tomography Reconstruction

Simulation Study of Muon Scattering For Tomography Reconstruction. D. Mitra A. Banerjee. K. Gnanvo M. Hohlmann. Presented at NSS-MIC 2009 Orlando. Florida Institute of Technology. Muon Scattering. Scattering angle Scattering function distribution: Approx. Normal (Bethe 1953).

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QUANTUM LOWER LIMIT ON SCATTERING ANGLE IN THE CALCULATION OF MULTIPLE TOUSCHEK-EFFECT

QUANTUM LOWER LIMIT ON SCATTERING ANGLE IN THE CALCULATION OF MULTIPLE TOUSCHEK-EFFECT. Sergei Nikitin BINP Russia IBS Mini Workshop, Cockcroft Institute, Daresbury 28-29 August 2007. Introduction Two definitions for a minimal scattering angle IBS parameters revision

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Deep Impact Projects (2)

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Numerical Model of an Internal Pellet Target

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Deep Impact Projects (2)

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4. Scattering processes

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OUTLINE of the TALK Description of the experiment Description of analysis

Preliminary Result of A N Measurement in p ? p ? Elastic Scattering at RHIC, at ? s = 200 GeV W?odek Guryn for pp2pp collaboration Brookhaven National Laboratory, Upton, NY, USA. OUTLINE of the TALK Description of the experiment Description of analysis Results and interpretation

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Analysis Summary

Analysis Summary. V. Blackmore CM32, RAL, 10/02/12. p - m Beam Contamination. Developed two techniques for determining the amount of p -contamination in our m beam.

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Polarized Positrons at Jefferson Lab

Polarized Positrons at Jefferson Lab Jonathan Dumas ( JLab /LPSC ), Joe Grames ( JLab ), Eric V outier (LPSC). Outlook. The Experiment. We investigate the idea of generating polarized positrons using the CEBAF polarized electron photoinjector . - low energy (e - beam energy ? 8.5 MeV )

97 views • 1 slides