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Title: Dipion decays of heavy quarkonium in the field correlator method

Journal Article · · Physics of Atomic Nuclei
 [1]
  1. Institute of Theoretical and Experimental Physics (Russian Federation)

The mechanism of dipion transitions nS {sup {yields}}n'S {pi}{pi} (n = 3, 2; n' = 2, 1) in bottomonium and charmonium is studied with the use of the chiral string-breaking Lagrangian allowing for the emission of any number of {pi}(K, {nu}), and not containing fitting parameters. The transition amplitude contains two terms: M = a - b, where the first term (a) refers to subsequent one-pion emission, {Gamma} (nS) {yields} {pi} B bar B {yields} {pi} {Gamma} (n'S){pi} , and the second term (b) refers to two-pion emission, {Gamma} (nS) {yields} {pi} {pi} B bar B {yields} {pi} {pi} {Gamma} (n'S). The one parameter formula for the dipion mass distribution is derived, dw/dq {approx} (phase space) x vertical bar {eta} - x vertical bar {sup 2}, where x = (q{sup 2} - 4m{sub {pi}}{sup 2})/(q{sub max}{sup 2} - 4m{sub {pi}}{sup 2}), q{sup 2} m= M{sub {pi}{pi}}{sup 2}. The parameter {nu} dependent on the process is calculated, using SHO wave functions and imposing PCAC restrictions (Adler zero) on amplitudes a and b. The resulting dipion mass distributions are in agreement with experimental data.

OSTI ID:
21402563
Journal Information:
Physics of Atomic Nuclei, Vol. 71, Issue 6; Other Information: DOI: 10.1134/S1063778808060094; Copyright (c) 2008 Pleiades Publishing, Ltd.; ISSN 1063-7788
Country of Publication:
United States
Language:
English