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Volumn 61, Issue 5, 2000, Pages 549011-549019

Dynamical evolution of the scalar condensate in heavy ion collisions

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EID: 12944277100     PISSN: 05562813     EISSN: 1089490X     Source Type: Journal    
DOI: 10.1103/PhysRevC.61.054901     Document Type: Article
Times cited : (7)

References (34)
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    • 0000409178 scopus 로고
    • J. Schwinger, J. Math. Phys. 2, 407 (1961); L. V. Keldysh, Zh. Eksp. Teor. Fiz. 47, 1515 (1964) Sov. Phys. JETP 20, 1018 (1964)].
    • (1964) Zh. Eksp. Teor. Fiz. , vol.47 , pp. 1515
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  • 6
    • 0000452993 scopus 로고
    • J. Schwinger, J. Math. Phys. 2, 407 (1961); L. V. Keldysh, Zh. Eksp. Teor. Fiz. 47, 1515 (1964) Sov. Phys. JETP 20, 1018 (1964)].
    • (1964) Sov. Phys. JETP , vol.20 , pp. 1018
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    • T. S. Biró, D. Molnár, Z. H. Feng, and L. P. Csernai, Phys. Rev. D 55, 6900 (1997); D. Molnár, L. P. Csernai, and Zs. Lázár, ibid. 58, 114018 (1998).
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    • Molnár, D.1    Csernai, L.P.2    Lázár, Zs.3
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    • A. Bochkarev and J. Kapusta, Phys. Rev. D 54, 4066 (1996); S. Jeon and J. Kapusta, ibid. 54, 6475 (1996).
    • (1996) Phys. Rev. D , vol.54 , pp. 6475
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    • R(p) is the real part of the pole, one finds that the wave decays like exp(-Γ(p)t/2). The origin of the factor of 2 is that Γ represents the loss rate for the number density whereas Γ/2 is the rate for the amplitude. See, for example, H. A. Weldon, Phys. Rev. D 28, 2007 (1983). This physics may be represented in a real Klein-Gordon wave equation by the dissipative term Γφ.
    • (1983) Phys. Rev. D , vol.28 , pp. 2007
    • Weldon, H.A.1
  • 27
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    • J. L. Basdevant and B. W. Lee, Phys. Lett. 29B, 437 (1969); Phys. Rev. D 2, 1680 (1970).
    • (1970) Phys. Rev. D , vol.2 , pp. 1680


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