Abstract

International Advisory Committee Prof. Allison M. Okamura (IEEE Fellow), Stanford University, United States Conference Committees Chair Prof. Dennis Lieu, University of California, Berkeley, United States Program Committee Chairs Prof. Dr. Jan Awrejcewicz, Lodz University of Technology, Poland Marina Barulina, Institute of Precision Mechanics and Control, Russian Academy of Sciences, Russia Technical Committee Chairs Prof. He Xu, Harbin Engineering University, ChinaProf. Kunhong Liu, Xiamen University, ChinaProf. Kwanho You, Sungkyunkwan University, South KoreaProf. Mohamed bin Hussein, Universiti Technologi Malaysia, MalaysiaAssoc. Prof. Yi Jin, University of Science and Technology of China, ChinaAssoc. Prof. Jie Yang, Dalian University of Technology, ChinaAssoc. Prof. Dirman Hanafi, Universiti Tun Hussein Onn Malaysia, MalaysiaAssoc. Prof. Dr. Vyacheslav Petrenko,North-Caucasus Federal University, RussiaAssoc. Prof. Dr. Maria Lapina, North-Caucasus Federal University, RussiaAsst. Prof. Abdel-Hameed Badawy, New Mexico State University, USADr. Zahid Akhtar, University of Memphis, USADr.Hsien-I Lin, National Taipei University of Technology, TaiwanDr. Lihong Zheng, Charles Sturt University, AustraliaDr. Adrian Kampa, Silesian University of Technology, PolandSze-Teng Liong, Feng Chia University, TaiwanMuath Alrammal, Higher Colleges of Technology, United Arabe of EmiratesMunir Naveed, Higher Colleges of Technology, United Arabe of EmiratesSuman Deb, NIT Agartala, IndiaNirmalya Kar, National Institute of Technology Agartala, IndiaAshim Saha, National Institute of Technology Agartala, IndiaIbragim Suleimenov, Almaty University of Power Engineering and Telecommunications,KazakhstanAkhat Bakirov, Almaty University of Power Engineering and Telecommunications, KazakhstanSebastian Heil, Chemnitz Technical University, Germany

Highlights

  • Heavy quarkonia are the bound states of charm and bottom quarks

  • Three different mixed decay time distributions can be distinguished depending on the type of neutral D final state: (a) semileptonic final states, (b) non-CP

  • The low-lying hadron spectrum is described by a linear effective mass term and a hyperfine interaction with a one-gluon exchange color factor

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Summary

Introduction

Heavy quarkonia are the bound states of charm and bottom quarks. They are strong interaction analogs of positronium. Heavy quarkonia spectroscopy is a good testing ground for theories of strong interactions: QCD in both perturbative and non-perturbative. Belle (B -> K c‘) Belle ( c‘) BaBar () CLEO (). 0 20 40 60 80 100 120 140 160 180 200 M(/)-M(c/) (MeV) 0 (IV) (IV) CLEO. Heavy Quarkonium Spectroscopy To set the stage for our discussion of the new mesons, it is useful to recall our previous, apparently numerically accurate understanding of the spectrum of M [GeV] (4415) (4040) ’(3686) ’c 2+ 1+ 0+ J/ c S. Implications of the New Results on g-2 Measurement of the Total Hadronic Cross–Section at e+e–° Machines Electric Dipole Moment Measurements in a Storage Ring.

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