'Hadrons' diaporamas de présentation

A journey through time with the Higgs particle Gordon J. Aubrecht, II Columbus Science Pub, 2 October 2012.

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Slides for Bochum 2007

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AXEL-2009 Introduction to Particle Accelerators

AXEL-2009 Introduction to Particle Accelerators. Transfer lines, injection and ejection Transfer lines: Transverse matching Single turn injection Multi-turn injection for protons and heavy ions Charge exchange injection for protons Leptons, betatron and synchrotron injection

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6 of the gluon fields are independent linear combinations of the simple gluon fields we enumerated

r g or g r. 6 of the gluon fields are independent linear combinations of the simple gluon fields we enumerated. G m 1 = (rg + gr)/ ? 2 G m 4 = (bg + gb)/ ? 2 G m 6 = (rb + br)/ ? 2 G m 2 =-i( rg - gr)/ ? 2 G m 5 =-i( bg - gb)/ ? 2 G m 7 =-i( rb + br)/ ? 2.

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Hard cross sections at first order in QCD

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Particle Physics Study

Particle Physics Study. 2009/07/27 Grass. From Luigi DiLella , Summer Student Program 2005. Outline. Before We Move to Particle Physics Neutrinos Fundamental Interaction Particle Interactions and Conservation Laws Quarks Elastic Scattering and Ine lastic Scattering

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Masayasu Harada (Nagoya Univ.)

Dilepton Production from Dropping Rho in the Vector Manifestation. Masayasu Harada (Nagoya Univ.). at Chiral 07 (Osaka, November 14, 2007). based on M.H. and C.Sasaki, Phys.Rev.D74:114006,2006. see also M.H. and K.Yamawaki, Phys. Rept. 381 , 1 (2003)

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Charged Particles

Charged Particles. Charged particles can come from nuclear decay. Nuclear physics figures into particle detection. Use terminology from nuclear physics. Isotopes share Z Isotones share N. Nucleus consists of protons and neutrons. Protons: Z ( atomic number ) Neutrons: N

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Two Particle Production in Proton-Nucleus Collisions

Two Particle Production in Proton-Nucleus Collisions. Jamal Jalilian-Marian Institute for Nuclear Theory University of Washington. Probing the CGC. Deep Inelastic Scattering: ep(A) ---> eX Structure functions: F 2 , F L Particle production Nucleus - Nucleus Collisions

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A Blast-wave Model with Two Freeze-outs

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Baryon Predictions

Baryon Predictions. Wave functions of Baryons. Baryon Magnetic Moments Baryon masses. Need to explain Parity and Charge Conjugation. Hadrons Magnetic moments. m q related to the intrinsic spin S of the quark. m = (q/mc) S and therefore for each spin-up quark:.

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A piece of pQCD in Heavy Ion Collisions

A piece of pQCD in Heavy Ion Collisions. Youngil Kwon IPAP Yonsei Univ. 1. We describe parton model and its link to the heavy ion collision. 2. We describe our efforts in PHENIX single muon analysis along this goal.

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Dilepton Radiation Measured in PHENIX probing the Strongly Interacting Matter Created at RHIC

Dilepton Radiation Measured in PHENIX probing the Strongly Interacting Matter Created at RHIC. Y. Akiba (RIKEN Nishina Center) for PHENIX Collaboration Quark Matter 2009 Knoxville, TN, USA April 2 nd , 2009. Electromagentic probes (photon and lepton pairs). e +. e -. g*. g.

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TI8/WIC Incident & UJ87/UA87 Radiation Levels & Analysis

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Interferometry of direct photons in Pb+Pb collisions at 158 AGeV

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A Blast-wave Model with two Freeze-outs

A Blast-wave Model with two Freeze-outs. Motivation A Blast-wave model with two freeze-outs Results Conclusion. Kang Seog Lee ( ??? ). HIM 2011.12.10. Chemical analysis of hadron ratios. Thermal analysis of mt spectra of hadrons.

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The Mysterious Nucleus

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Quarks and more.. What forces hold the atom together?

Quarks and more.. What forces hold the atom together?. Electromagnetic likes repel, opposites attract (+ or -). Strong Force interacts with hadrons or nucleons so the protons and neutrons binds them together works only at distances smaller than 1 quadrillionth of a meter!!!.

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GCOE International Summer School

GCOE International Summer School. Hadrons and Nuclei under Extreme Conditions. The main building H111.

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