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Effective potential for heavy quark antiquark bound system

Abstract

A heavy quark antiquark potential is suggested connecting asymptotic freedom and quark confinement in a unified way. The ..cap alpha../sub g/(q/sup 2/) calculated using Borel summation technique with three loop agrees with the two loop ..beta..-function up to g/sup 2//4..pi.. -- 1.1 but changes appreciably after g/sup 2//4..pi.. = 1.5. The potential so derived satisfactorily explains the c overlined c and b overlined b spectrum. 13 refs., 4 figures, 3 tables.
Publication Date:
Dec 01, 1985
Product Type:
Journal Article
Reference Number:
AIX-18-067460; EDB-87-113428
Resource Relation:
Journal Name: Pramana; (India); Journal Volume: 25:6
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; QUARKS; BOUND STATE; POTENTIALS; ANTIPARTICLES; COUPLING CONSTANTS; D STATES; LANDAU QUASI PARTICLES; MASS; P STATES; S STATES; VACUUM POLARIZATION; ANTIMATTER; ELEMENTARY PARTICLES; ENERGY LEVELS; POSTULATED PARTICLES; QUASI PARTICLES; 645204* - High Energy Physics- Particle Interactions & Properties-Theoretical- Strong Interactions & Properties
OSTI ID:
6398765
Research Organizations:
Nimapara Coll., Orissa State, India. Dept. of Physics; Utkal Univ., Bhubaneswar, India. Dept. of Physics
Country of Origin:
India
Language:
English
Other Identifying Numbers:
Journal ID: CODEN: PRAMC
Submitting Site:
INIS
Size:
Pages: 663-671
Announcement Date:
Jul 01, 1987

Citation Formats

Barik, B K, and Deo, B B. Effective potential for heavy quark antiquark bound system. India: N. p., 1985. Web.
Barik, B K, & Deo, B B. Effective potential for heavy quark antiquark bound system. India.
Barik, B K, and Deo, B B. 1985. "Effective potential for heavy quark antiquark bound system." India.
@misc{etde_6398765,
title = {Effective potential for heavy quark antiquark bound system}
author = {Barik, B K, and Deo, B B}
abstractNote = {A heavy quark antiquark potential is suggested connecting asymptotic freedom and quark confinement in a unified way. The ..cap alpha../sub g/(q/sup 2/) calculated using Borel summation technique with three loop agrees with the two loop ..beta..-function up to g/sup 2//4..pi.. -- 1.1 but changes appreciably after g/sup 2//4..pi.. = 1.5. The potential so derived satisfactorily explains the c overlined c and b overlined b spectrum. 13 refs., 4 figures, 3 tables.}
journal = []
volume = {25:6}
journal type = {AC}
place = {India}
year = {1985}
month = {Dec}
}