1. transitions monitored by strong interactions: a new determination of the KL–KS mass difference
- Author
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R. Le Gac, M. Schafer, P.-R. Kettle, J. R. Fry, R. Gamet, D. Zimmerman, A. Muller, L. Sakeliou, Per Carlson, L. Tauscher, A. Ealet, P. Bargassa, D. Zavrtanik, H.-J. Gerber, P. Bloch, P. Pavlopoulos, M.B. Chertok, P. Weber, F. Blanc, Sotirios Vlachos, T. Ruf, B. L. Roberts, K. Jon-And, Marcin Wladyslaw Wolter, G. Polivka, Panagiotis Kokkas, J. Derre, A. Angelopoulos, B. Pagels, Andrej Filipcic, M. Mikuž, D. Francis, Nikolaos Manthos, Lukas A. Schaller, W. Fetscher, O. Wigger, Jeffrey Boone Miller, E. Gabathuler, R. Rickenbach, Mats Danielsson, F. Henry-Couannier, C. Thibault, M. Fidecaro, O. Behnke, A. Haselden, F. Montanet, C. Eleftheriadis, A. Benelli, F. Leimgruber, A. Schopper, C.W.E. van Eijk, T. Nakada, P.J. Hayman, Michael C. Carroll, Marc Dejardin, R.W. Hollander, I. Papadopoulos, G. Backenstoss, V. Bertin, Elie Aslanides, R. Kreuger, C. Touramanis, Igor Mandić, A. Go, G. Marel, T. Schietinger, F. Touchard, and E. Cawley
- Subjects
Physics ,Nuclear physics ,Nuclear and High Energy Physics ,Particle physics ,Amplitude ,CPT symmetry ,High Energy Physics::Phenomenology ,High Energy Physics::Experiment ,Strangeness ,Nuclear Experiment - Abstract
The CPLEAR set-up (modified) has been used to determine the KL–KS mass difference by a method where neutral-kaon strangeness oscillations are monitored through kaon strong interactions, rather than semileptonic decays, thus requiring no assumptions on CPT invariance for the decay amplitudes. The result, Δm=(0.5343±0.0063stat±0.0025syst)×1010ℏ/s, provides a valuable input for CPT tests.
- Published
- 2001
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