Limits on neutral<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>D</mml:mi></mml:math>mixing in semileptonic decays

Cawlfield, C.; Eisenstein, B. I.; Gollin, G. D.; Karliner, I.; Kim, D.; Lowrey, N.; Naik, P.; Sedlack, C.; Selen, M.; Williams, James S.; Wiss, J.; Edwards, K. W.; Besson, D.; Pedlar, T. K.; Cronin-Hennessy, D.; Gao, K. Y.; Gong, D. T.; Kubota, Y.; Klein, T.; Lang, B. W.; Li, S. Z.; Poling, R.; Scott, A. W.; Smith, A. J. S.; Dobbs, S.; Metreveli, Z.; Seth, K. K.; Tomaradze, A.; Zweber, P.; Ernst, J.; Mahmood, A. H.; Arms, K.; Gan, K. K.; Severini, H.; Asner, D. M.; Dytman, S. A.; Love, W. A.; Mehrabyan, S.; Muêller, J.; Savinov, V.; Li, Z.; López, A.; Méndez, H.; Vargas, J. E. Ramirez; Huang, G. S.; Miller, D. H.; Pavlunin, V.; Sanghi, B.; Shibata, E. I.; Shipsey, I. P. J.; Adams, G. S.; Chasse, M.; Cravey, M.; Cummings, J. P.; Dankó, I.; Napolitano, J.; He, Q.; Muramatsu, H.; Park, C. S.; Park, W.; Thorndike, E. H.; Coan, T. E.; Gao, Y. S.; Liu, F.; Stroynowski, R.; Artuso, M.; Boulahouache, C.; Blusk, S.; Butt, J.; Dambasuren, E.; Dorjkhaidav, O.; Li, J.; Menaa, N.; Mountain, R.; Nandakumar, R.; Redjimi, R.; Sia, R.; Skwarnicki, T.; Stone, S.; Wang, J. C.; Zhang, K.; Csorna, S. E.; Bonvicini, G.; Cinabro, D.; Dubrovin, M.; McGee, Steven; Bornheim, A.; Pappas, S. P.; Weinstein, A. J.; Nelson, H. N.; Briere, R. A.; Chen, G. P.; Chen, J.; Ferguson, T.; Tatishvili, G.; Vogel, H.; Watkins, M. E.; Rosner, Jonathan L.; Adam, N.; Alexander, J. P.; Berkelman, K.; Cassel, D. G.; Credé, V.; Duboscq, J. E.; Ecklund, K. M.; Ehrlich, R.; Fields, L.; Gibbons, L. K.; Gittelman, B.; Gray, R.; Gray, S. W.; Hartill, D. L.; Heltsley, B. K.; Hertz, D.; Hsu, L.; Jones, C. D.; Kandaswamy, J.; Kreinick, D. L.; Кузнецов, В. Е.; Mahlke-Krüger, H.; Meyer, T. O.; Onyisi, P. U. E.; Patterson, J. R.; Peterson, D.; Pivarski, J.; Riley, D.; Rýd, A.; Sadoff, A. J.; Schwarthoff, H.; Shepherd, M. R.; Stroiney, S.; Sun, W.; Urner, D.; Wilksen, T.; Weinberger, M.; Athar, S. B.; Avery, P.; Breva-Newell, L.; Patel, R.; Potlia, V.; Stoeck, H.; Yelton, J.; Rubin, P.

doi:10.1103/physrevd.71.077101

Cited by 34 publications

(17 citation statements)

References 10 publications

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“…All input measurements are listed in Tables 216-218. The observable R M = (x 2 + y 2 )/2 is calculated from D 0 → K + − ν decays [743][744][745][746] [748,749], BABAR [734], CDF [750], and LHCb [736]; earlier measurements have much less precision and are not used. The observables from D 0 → K 0 S π + π − decays are measured in two ways: assuming CP conservation (D 0 and D 0 decays are combined), and allowing for CP violation (D 0 and D 0 decays are fitted separately).…”

Section: Input Observablesmentioning

confidence: 99%

Averages of $b$-hadron, $c$-hadron, and $τ$-lepton properties as of summer 2014

Amhis,

Banerjee,

Ben-Haim

et al. 2014

Preprint

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246

506

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This article reports world averages of measurements of b-hadron, c-hadron, and τlepton properties obtained by the Heavy Flavor Averaging Group (HFAG) using results available through summer 2014. For the averaging, common input parameters used in the various analyses are adjusted (rescaled) to common values, and known correlations are taken into account. The averages include branching fractions, lifetimes, neutral meson mixing parameters, CP violation parameters, parameters of semileptonic decays and CKM matrix elements.

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Section: Input Observablesmentioning

confidence: 99%

Averages of $b$-hadron, $c$-hadron, and $τ$-lepton properties as of summer 2014

Amhis,

Banerjee,

Ben-Haim

et al. 2014

Preprint

Self Cite

246

506

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show abstract

“…59,60 More recently, E791, CLEO, Belle, and BABAR have reported measurements. 61,62,63,64,65 The E791 analysis estimates the missing momentum of the neutrino by using the measured decay vertex positions of the D * + and the D 0 , the kaon and lepton momenta, and attributing the D 0 mass to the secondary decay. This results in a twofold ambiguity, which is resolved by always choosing the higher-momentum solution for the D 0 (motivated by MC studies).…”

Section: Analysis Of Wrong-sign Semileptonic Decaysmentioning

confidence: 99%

Charm Meson Mixing: An Experimental Review

Chavez

Cowan²,

Lockman

2012

Int. J. Mod. Phys. A

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We review current experimental results on charm mixing and CP violation. We survey experimental techniques, including time-dependent, time-independent, and quantumcorrelated measurements. We review techniques that use a slow pion tag from D * + → π + D 0 + c.c. decays and those that do not, and cover two-body and multi-body D 0 decay modes. We provide a summary of D-mixing results to date and comment on future experimental prospects at the LHC and other new or planned facilities.

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“…CLEO thus reports the first observation of a dipion transition outside of a 3 S 1 system, and a preliminary width of Γ(χ b (2P) → χ b (1P)π + π − ) ≈ 0.9keV . Further details can be found in [20].…”

Section: Observation Ofmentioning

confidence: 99%