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Volumn 69, Issue 9, 2004, Pages 17-

Behavior of charmonium systems after deconfinement

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EID: 3042638968     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.69.094507     Document Type: Article
Times cited : (471)

References (48)
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    • QCD TARO Collaboration, Ph. de Forcrand, Phys. Rev. D 63, 054501 (2001). See also Ref. 36 for an early attempt to extract pole mass from finite temperature temporal correlators.
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    • F. Karsch and I. Wetzorke, in Proceedings of Strong and Electroweak Matter 2000 (World Scientific, Singapore, 2001), p. 193
    • F. Karsch and I. Wetzorke, in Proceedings of Strong and Electroweak Matter 2000 (World Scientific, Singapore, 2001), p. 193.
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    • CP-PACS Collaboration, T. Yamazaki, Phys. Rev. D 65, 014501 (2002).
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    • P. Petreczky, hep-lat/0310059. See also Ref. 35.
    • Petreczky, P.1
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    • M. Le Bellac, Thermal Field Theory (Cambridge University Press, Cambridge, England, 1996)
    • M. Le Bellac, Thermal Field Theory (Cambridge University Press, Cambridge, England, 1996).
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    • Lüscher, M.1
  • 27
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    • For example, for the pseudoscalar mesons we get (Formula presented) (set IA), (Formula presented) (IB), (Formula presented) (IC), (Formula presented) (II), and (Formula presented) (III) for (Formula presented) using Eq. (13). For the heavy-light pseudoscalars, it has been reported that a relation like (Formula presented) works quite well for the meson masses; see, for example, UKQCD Collaboration, K. Bowler, Nucl. Phys. B619, 507 (2001). For our heavy-heavy mesons, while consistent within errors, such a relation seems to underestimate the difference between kinetic and pole mass of the meson.
    • (2001) Nucl. Phys. , vol.B619 , pp. 507
    • Bowler, K.1
  • 41
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    • F. Karsch and E. Laermann, in Quark-Gluon Plasma, edited by R.C. Hwa (World Scientific, Singapore, 2003), Vol. 3
    • F. Karsch and E. Laermann, in Quark-Gluon Plasma, edited by R.C. Hwa (World Scientific, Singapore, 2003), Vol. 3.


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