'High pt' presentation slideshows

Phenomenology of SUSY Models with Non-universal Sfermions

Phenomenology of SUSY Models with Non-universal Sfermions. Kazuki Sakurai (Nagoya U. ? KEK? Cambridge U. ). In collaboration with. S.-G. Kim, N.Maekawa, K.I.Nagao, M.M.Nojiri, Y.Shimizu, M.Takeuchi. 2009/3/9 ???????????? @ ??. Introduction.

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Anisotropic flow in a B oltzmann kinetic approach at fixed h /s(T)

619 views • 52 slides

Rare B decays (at the LHC) as a probe of b ? s transitions

Rare B decays (at the LHC) as a probe of b ? s transitions. Framework LHC & experiments b ? s g b ? s l + l - B (s) ? m + m - LHC Schedule Summary. Gerhard Raven NIKHEF & Vrije Universiteit, Amsterdam. ITEP Meeting on The Future of Heavy Flavour Physics. Disclaimers.

637 views • 51 slides

10 12 Degrees in the Shade: Physics of the quark-gluon plasma

10 12 Degrees in the Shade: Physics of the quark-gluon plasma. Craig Ogilvie. Motivation: non-perturbative quantum chromodynamics (QCD) Results from RHIC Properties of quark-gluon plasma to study QCD Outstanding questions, next steps. Perturbation series in a s.

584 views • 45 slides

Constraints induced by Finite Plasma Formation Time on some Physics Observables at RHIC

Constraints induced by Finite Plasma Formation Time on some Physics Observables at RHIC. Vlad Pantuev, SUNY at Stony Brook. See V.P. hep-ph/0506095, hep-ph/0509207 and www.phenix.bnl.gov/WWW/publish/pantuev/Formation_Time_BNL.ppt. Outline: Demonstrate where long formation time comes from

544 views • 44 slides

QCD Results from the Tevatron

QCD Results from the Tevatron. Ashish Kumar, SUNY at Buffalo (on behalf of CDF & D0 Collaborations). Aspen 2011 : New Data from the Energy Frontier Aspen Center of Physics Feb 12-18, 2011. Outline. Fermilab Tevatron , CDF and D0 Detectors Motivation Photons Jets

464 views • 34 slides

Searches for heavy resonances with the ATLAS detector

Searches for heavy resonances with the ATLAS detector. Madalina Stanescu-Bellu (DESY, Germany) 16-20 Dec HEP2013, Valparaiso, CHILE. Heavy Resonances. excited states of heavy particles decay fast (10 -23 s) into lighter particles before it reaches our detectors

443 views • 33 slides

Part 2 Some details about LHC Some details about the CMS subdetectors QCD measurements

G. Mantovani Some of the first physics analyses with CMS at the CERN-LHC (QCD, UE, multipartonic interactions). Part 2 Some details about LHC Some details about the CMS subdetectors QCD measurements. The collider. To be sensitive to most HE physical processes one needs

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at CERN SPS

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A Very High Momentum Particle Identification Detector for the ALICE experiment at the LHC.

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365 views • 27 slides

Color Glass Condensate at RHIC

Color Glass Condensate at RHIC. Jamal Jalilian-Marian Institute for Nuclear Theory Seattle, Washington. OUTLINE. Quantum Chromo Dynamics Perturbative QCD Parton Model Semi-Classical QCD Color Glass Condensate Color Quantum Fluid Semi-Classical QCD at RHIC Indications Tests.

435 views • 24 slides

Azimuthal Anisotropy and the QGP

Azimuthal Anisotropy and the QGP. Yasuo MIAKE, Univ. of Tsukuba. Why I Iike azimuthal anisotropy Tsukuba strategy for RHIC-PHENIX What is found at RHIC. Reaction Plane. Almond shape. Reasons why I love azimuthal anisotropy. Info. on mean free path ? vs. R

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Characterizing non-equilibrium and radial flow at RHIC with Tsallis statistics

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Efforts by Yonsei towards ALICE

Efforts by Yonsei towards ALICE. Y. Kwon (Yonsei Univ.). NA. LHC. SPS. ALICE. WA. pQCD & factorization?. (for sufficiently large scale). Factorization:. hadron. High pT particle. hadron. parton distribution functions x a = momentum fraction of parton a in hadron A.

329 views • 20 slides

Dr. Richard St. Denis Glasgow University On behalf of the CDF and D0 Collaborations

Dr. Richard St. Denis Glasgow University On behalf of the CDF and D0 Collaborations Moriond 2010 Electroweak, La Thuile, Italy March 6-March 13, 2010. Tevatron Results on SM Higgs Search in the High Mass Region. Outline. Search Foundation and Higgs detection modes

361 views • 20 slides

Elliptic flow of electrons from heavy flavor decays in?s NN = 200 GeV Au+Au collisions @ PHENIX

Elliptic flow of electrons from heavy flavor decays in?s NN = 200 GeV Au+Au collisions @ PHENIX. Shingo Sakai for PHENIX Collaborations (Univ. of Tsukuba JSPS). Outline. Introduction Analysis Discussion D meson v 2 charm v 2 B meson contribution

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Strange and Non-Strange Particle Ratios as a Function of p T and centrality in STAR at RHIC

Strange and Non-Strange Particle Ratios as a Function of p T and centrality in STAR at RHIC. B. Norman, Kent State University, and the STAR Collaboration. Outline. Physics Motivation Particle identification Topological ID of K +/- (kinks) Ring Imaging CHerenkov detector (RICH)

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Motivation Measurement Results Summary

Paper - 5 Trasverse momentum and collision energy dependence of high pT hadron suppression in Au+Au collisions at ultrarelativistic energies. Motivation Measurement Results Summary. Jaiby Joseph CNR Talk - 5. Motivation.

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Measurement of Azimuthal Anisotropy for High p T Charged Hadrons at RHIC-PHENIX

non central collision. 2.0-4.0 GeV/c 1.0-2.0 GeV/c 0.2-1.0 GeV/c. z. ?. ?. Beam axis. Reaction plane. ?. x. x (Reaction Plane). PHENIX Collaborators. Large energy loss. Small energy loss. Reaction Plane. 1.0-2.0 GeV/c 0.2-1.0 GeV/c. 2.0-4.0 GeV/c 1.0-2.0 GeV/c 0.2-1.0 GeV/c.

109 views • 1 slides