Autor: |
S. Wallis-Plachner, C. A. Meyer, C.J. Batty, V. Crede, K. K. Seth, K. Peters, B.S. Zou, I. Uman, H. Matthäy, N.P. Hessey, M. A. Faessler, J. Kisiel, K.M. Crowe, R.P. Haddock, D. Walther, H. Kalinowsky, U. Wiedner, U. Strohbusch, P. Kammel, U. Kurilla, P. Blüm, Herbert Koch, K. Braune, Eberhard Klempt, D.V. Bugg, M. Suffert, R. Landua, F. Meyer-Wildhagen, C. Regenfus, C.A. Baker, Bruce Barnett, U. Thoma, B. Pick, W. Dünnweber, M. Benayoun, Claude Amsler, Michael Doser, R. Ouared, F. H. Heinsius, Marcel Kunze, O. Kortner, D. Jamnik, D. Engelhardt, Č. Zupančič, W. Roethel, M. Ratajczak, Pàl Hidas |
Rok vydání: |
2006 |
Předmět: |
|
Zdroj: |
Physics Letters B. 639:165-171 |
ISSN: |
0370-2693 |
DOI: |
10.1016/j.physletb.2006.06.010 |
Popis: |
Prominent K K ¯ resonances observed in the in-flight annihilation of p ¯ p into K + K − π 0 include f 2 ( 1270 ) , f 0 ( 1500 ) , f 2 ′ ( 1525 ) , ϕ ( 1680 ) / ρ ( 1700 ) and a state at 1750 MeV / c 2 consistent with f 0 ( 1710 ) . The reaction cross sections σ ( p ¯ p → X ( K + K − ) π 0 ) are obtained by means of a partial wave analysis. When these are combined with known K K ¯ partial widths, the resulting production rates of presumably non- n n ¯ states, X = f 0 ( 1710 ) and f 2 ′ ( 1525 ) , are found to be suppressed by an order of magnitude compared to f 0 ( 1500 ) and f 2 ( 1270 ) , respectively. |
Databáze: |
OpenAIRE |
Externí odkaz: |
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