PPT-A New Dynamical Picture for the Production and Decay of the

X Y Z and P c Charmoniumlike Exotics Richard Lebed Modern Exotic Hadrons Institute for Nuclear Theory November 2015 X3872 Z4475 Y4260 LHCb CMS BES III QCD. NN. = 200 GeV in STAR experiment at RHIC. Jaiby Joseph . Ajish. 11/2/2011. Outline. Quick summary of my contributions. Introduction. Why . collide nuclei at high energies?. RHIC, STAR. Physics at RHIC. T. Sato Osaka U./KEK . Motivation. Analysis of meson production reaction and dynamical coupled channel model. extracting resonance parameters. Resonance mass and width. Role of reaction dynamics on resonance properties. A. iichi. . Iwazaki. Nishogakusha University. High energy heavy ion collisions. Generation of color electric . a. nd magnetic fields. according to . a model of . color glass condensate. t. hermalized. s. tudy of . hadron. . r. esonances and strangeness production. Hiroyuki Kamano. (RCNP, Osaka U.). in collaboration with. B. Julia-Diaz (Barcelona U.), T.-S. H. Lee (Argonne),. A. Matsuyama (Shizuoka U.), S. Nakamura (. ICM. , Paris, . France. ETH, Zurich, Switzerland. Dynamic. Causal . Modelling. of . fMRI. . timeseries. . Overview. 1 DCM: introduction. 2 Dynamical systems theory. 4 Bayesian inference. . 5 Conclusion. NN. = 200 GeV in STAR experiment at RHIC. Jaiby Joseph . Ajish. 11/2/2011. Outline. Quick summary of my contributions. Introduction. Why . collide nuclei at high energies?. RHIC, STAR. Physics at RHIC. Phenomenology of Vectorlike Confinement. Can Kılıç. , University of Texas at Austin. work done with: Takemichi Okui (arXiv: 1001.4526, JHEP 1004:128, 2010 ). Takemichi Okui, Raman Sundrum (arXiv: 0906.0577, JHEP 1002:018, 2010). Siwei. . Liu. 1,. Yang Zhou. 1. , Richard Palumbo. 2. , & Jane-Ling Wang. 1. 1. UC Davis; . 2. University of Rhode Island. Motivating Study. Physiological synchrony between romantic partners during nonverbal conditions. Xiaohui XIE. Supervisor: Dr. Hon . Wah. TAM. 2. Outline. Problem background and introduction. Analysis for dynamical systems with time delay. Introduction of dynamical systems. Delayed dynamical systems approach.  . The decay rate.  . Lorentz Invariant Phase Space. The decay rate.  . The decay rate.  . Decay amplitude. Describes the interactions during the decay.. The Feynman diagrams. The Feynman diagrams. Symmetry Breaking. Craig Roberts. Physics Division. Q. C. D. ’s Challenges. Dynamical . Chiral. Symmetry Breaking. Very unnatural pattern of bound state masses; . . e.g., . Lagrangian. (. pQCD. Presenter: . Skhathisomusa. . Mthembu. Supervisor: Prof. Bruce . Mellado. Project Guidance: Dr. . Mukesh. Kumar,. Prof. Alan Cornell. Top associated Higgs production. . Small H > VV branching fraction, enhanced . beta decay. . They are designated by beta (β). There are two forms of beta decay, . β. −.  and . β. +. , which respectively give rise to the electron and the positron.. . The generalized atomic equation for beta decay is as follows. : . universal term for all weak-interaction transitions. . between two neighboring isobars. three different forms. β. -. , . β. +. & . EC. (. capture of an atomic electron.