Abstract
A heavy quark antiquark potential is suggested connecting asymptotic freedom and quark confinement in a unified way. Theα g (q 2) calculated using Borel summation technique with three loop agrees with the two loopβ-function up tog 2/4π≅ 1.1 but changes appreciably afterg 2/4π=1.5. The potential so derived satisfactorily explains the \(c\bar c\)and \(b\bar b\)spectrum.
Similar content being viewed by others
References
Andrews Det al 1980Phys. Rev. Lett. 44 1108
Augustin J Eet al 1974Phys. Rev. Lett. 33 1453
Barnett R, Michael Banett and Schlatter D 1982 SLAC publication-2883/Feb 1982
Creutz M 1980aPhys. Rev. D21 2308
Creutz M 1980bPhys. Rev. Lett. 45 313
Deo B B and Barik B K 1983Phys. Rev. D27 249
Eichten E, Gottfried K, Kinoshitta T, Lane K D and Yan T M 1978Phys. Rev. D17 3090
Eichten E, Gottfried K, Kinoshitta T, Lane K D and Yan T M 1980Phys. Rev. D21 203
Kogut J B, Pearson R B, Shigemitsu J 1979Phys. Rev. Lett. 43 484
Khuri N N 1979Phys. Lett. 82B 83
Richardson J L 1979Phys. Lett. 82B 272
Sanda A I 1979Phys. Rev. Lett. 42 1658
Tarasov O V, Vladiminov A A, Zharkov A Yu 1980Phys. Lett. 93B 429
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Barik, B.K., Deo, B.B. An effective potential for heavy quark antiquark bound system. Pramana - J Phys 25, 663–671 (1985). https://doi.org/10.1007/BF02847727
Received:
Revised:
Issue Date:
DOI: https://doi.org/10.1007/BF02847727