Inclusive cross section - PowerPoint PPT Presentation

Physics Results from Tevatron Run II

Physics Results from Tevatron Run II. Daria Zieminska Indiana University mail to: daria@fnal.gov (for the D0 and CDF Collaborations) Lattice 2004 Fermilab, June 26, 2004. Tevatron Run II rich physics program.

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469 views • 36 slides

Strong Interaction, Quarks + Gluons

Strong Interaction, Quarks + Gluons. Quark Model Partons Gluons + QCD. Introduction to Particle Physics - Max Klein – Lecture 4 - Liverpool University 4.3.13. M.Klein 4.3.2013 L4. Light Quarks. Light quarks are u,d,s , with masses much smaller than M p.

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Tagged Neutron candidates observed in MIPP data

Tagged Neutron candidates observed in MIPP data. Neutron spectra for various beam momenta. Proton spectra for various beam momenta. Pion spectra for various beam momenta. Expected tagged neutral beam rates. General scaling law of particle fragmentation.

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Three-Body Break-Up Processes at Higher Energies

Three-Body Break-Up Processes at Higher Energies. Hang Liu Charlotte Elster Walter Gl öckle. Supported by: U.S. DOE, NERSC. Full Faddeev. The Solution of Three-Body Amplitude T at Different Orders in Two-Body t -Matrix. 1 st order. 2 nd order. 3 rd order. 4 th order.

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MCFM Studies

MCFM Studies. Neil Delwadia. Last Meeting…. Varied QCD and QCD_fac scales in order to evaluate systematic errors Learned that there was greater error in cross section calculation when scales were stretched in opposite directions. Past Week. Varied measure of energy of decay products

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2p2h or not 2p2h?

2p2h or not 2p2h?. TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: A A A A. 1p1h: CCQE for Fermi gas. 2p2h :. M. Martini @ Fermilab. Inclusive cross section:. M. Martini, PRC 80 (2009). Nieves et al., arXiv:1102.2777.

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170 views • 5 slides

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