'Jet clustering' diaporamas de présentation

Machine Learning in High Energy Physics

Machine Learning in High Energy Physics. Satyaki Bhattacharya Saha Institute for Nuclear Physics. Machine Learning in High Energy Physics. Satyaki Bhattacharya Saha Institute of Nuclear Physics. Why machine learning ?. We are always looking for a faint signal against a large background

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Improved jet clustering algorithm with vertex information for multi-b final states

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Improved jet clustering algorithm with vertex information for multi-b final states

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From Quark to Jet: A Beautiful Journey Lecture 2

From Quark to Jet: A Beautiful Journey Lecture 2 Jet Clustering, Classification, and Personal Computing Tyler Dorland Deutsches Elektronen -Synchrotron (DESY) Inverted CERN School of Computing, 24-25 February 2014. Explaining the Title: An outline. Theoretical. Quarks

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Feasibility study of measurement of Higgs pair creation in a gamma-gamma collider

Feasibility study of measurement of Higgs pair creation in a gamma-gamma collider. Shin- ichi Kawada Advanced Sciences of Matter, Hiroshima University. Collaborators : Katsumasa Ikematsu (Univ. Siegen), Tohru Takahashi (Hiroshima Univ.),

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Feasibility study of Higgs pair production in a Photon Collider

Feasibility study of Higgs pair production in a Photon Collider. Tohru Takahashi Hiroshima University for S.Kawada , N.Maeda , K.Ikematsu , K.Fujii,Y.Kurihara ,,,. IWLC2010 CERN. Higgs Physics w/ PLCs. Two photon decay width of light higgs 2% ~ 8% for Mh = 129geV ~ 160GeV

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Status of ZHH analysis

Status of ZHH analysis. Taikan Suehara (ICEPP, U. Tokyo) J. Tian(KEK), T. Tanabe (Tokyo), K. Fujii(KEK) and all ILD colleagues. The only probe for Higgs potential: self coupling. SM force. The last force in SM A good probe for BSM with ~30% accuracy. SUSY case: Kanemura et al. (2011).

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ZHH with new jet clustering (from TIPP11 slides)

ZHH with new jet clustering (from TIPP11 slides). Taikan Suehara, Tomohiko Tanabe, Satoru Yamashita (The Univ. of Tokyo). ZHH in ILC. HHH coupling: a key to prove Higgs mechanism. m H =120 GeV. Double Higgs-strahlung: largest xsec around 500 GeV.

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Light Higgs Benchmark Analyses

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Status of the SISCone Note (Part I)

Status of the SISCone Note (Part I). JetMET Jan 17 2008 Frank Chlebana. Why Use SISCone. Cone-based algorithms that use starting seeds are collinear and infrared unsafe ? ambiguities arise comparing observation to theory. Seedless algorithms have taken a prohibitively long time to execute

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ILC DBD Common simulation and software tools

ILC DBD Common simulation and software tools . Akiya Miyamoto KEK ILC PAC 14 December 2012 at KEK. Introduction. Software tools for ILC have been developed by ILD and SiD independently but with good communication For DBD studies,

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