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...rotvino) • D. Zeppenfeld (University of Karlsruhe, Germany) • P. Zerwas (DESY) • C. Zhang (IHEP, Beijing) • K. Zuber (Oxford University) 4. Naming scheme for hadrons We introduced in the 1986 edition =-=[2]-=- a new naming scheme for the hadrons. Changes from older terminology affected mainly the heavier mesons made of u, d, and s quarks. Otherwise, the only important change to known hadrons was that the F...

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...syst#ematic influence from this effect by choosing the normalization factor between energy and magnedic field so that t,he fitted resonance mass is equal to the nominal mass MTtls) = 9460.0 f 0.2 MeV =-=[27]-=-. For t,he limited energy range of our scans the beam energy is a linear function of the magnetic field B. 8.1 ITee of the Y(lS) We first fit each scan individually to t,he funct,ion eq. 13 with four ...

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...University of Florida) • M. Zeller (Yale University) • D. Zeppenfeld (University of Wisconsin) • C. Zhang (IHEP, Beijing) Introduction 7 3. Naming scheme for hadrons We introduced in the 1986 edition =-=[2]-=- a new naming scheme for the hadrons. Changes from older terminology affected mainly the heavier mesons made of u, d, and s quarks. Otherwise, the only important change to known hadrons was that the F...

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...University of Florida) • M. Zeller (Yale University) • D. Zeppenfeld (University of Wisconsin) • C. Zhang (IHEP, Beijing) Introduction 7 3. Naming scheme for hadrons We introduced in the 1986 edition =-=[2]-=- a new naming scheme for the hadrons. Changes from older terminology affected mainly the heavier mesons made of u, d, and s quarks. Otherwise, the only important change to known hadrons was that the F...