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Köpp, S.; Kostin, M.; Mahmood, A. H.; Csorna, S. E.; Dankó, I.; McLean, K. W.; Zhao-yu, XU; Godang, R.; Bonvicini, G.; Cinabro, D.; Dubrovin, M.; McGee, Steven; Zhou, G. J.; Bornheim, A.; Lipeles, E.; Pappas, S. P.; Śchmidtler, M.; Shapiro, A.; Sun, W.; Weinstein, A. J.; Jaffe, D. E.; Masek, G.; Paar, H. P.; Asner, D. M.; Eppich, A.; Hill, T. S.; Morrison, R. J.; Briere, R. A.; Chen, G. P.; Ferguson, T.; Vogel, H.; Gritsan, A. V.; Alexander, J.; Baker, R. C.; Bebek, C.; Berger, B. E.; Berkelman, K.; Blanc, F.; Boisvert, V.; Cassel, D. G.; Drell, P. S.; Duboscq, J. E.; Ecklund, K. M.; Ehrlich, R.; Foland, A.; Gaidarev, P.; Gibbons, L.; Gittelman, B.; Gray, S. W.; Hartill, D. L.; Heltsley, B. K.; Hopman, P. I.; Hsu, L.; Jones, C. D.; Kandaswamy, J.; Kreinick, D. L.; Lohner, M.; Magerkurth, A.; Meyer, T. O.; Mistry, N. B.; Nordberg, E.; Palmer, M.; Patterson, J. R.; Peterson, D.; Riley, D.; Romano, A.; Thayer, J. G.; Urner, D.; Valant-Spaight, B.; Viehhauser, G. H. A.; Warburton, A.; Avery, P.; Prescott, C.; Rubiera, A. I.; Stoeck, H.; Yelton, J.; Brandenburg, G.; Ershov, A.; Kim, D. Y.-J.; Wilson, Richard; Bergfeld, T.; Eisenstein, B. I.; Ernst, J.; Gladding, G. E.; Gollin, G. D.; Hans, R. M.; Johnson, E.; Karliner, I.; Marsh, M. A.; Plager, C.; Sedlack, C.; Selen, M.; Thaler, J. J.; Williams, J. C.; Edwards, K. W.; Janicek, R.; Patel, P. M.; Sadoff, A. J.; Ammar, R.; Bean, A.; Besson, D.; Zhao, X.; Anderson, S.; Frolov, V. V.; Kubota, Y.; Lee, S. J.; Mahapatra, R.; O’Neill, J. J.; Poling, R.; Riehle, T.; Smith, A. J. S.; Stepaniak, C. J.; Urheim, J.; Ahmed, S.; Alam, M. S.; Athar, S. B.; Jian, L.; Liu, Ling; Saleem, M.; Timm, S.; Wappler, F. R.; Anastassov, A.; Eckhart, E.; Gan, K. K.; Gwon, C.; Hart, T.; Honscheid, K.; Hufnagel, D.; Kagan, H.; Kass, R.; Pedlar, T. K.; Schwarthoff, H.; Thayer, J. B.; Toerne, E. von; Zoeller, M. M.; Richichi, S. J.; Severini, H.; Skubic, P.; Undrus, A.; Savinov, V.; Chen, S.; Fast, J. E.; Hinson, J. W.; Lee, J.; Miller, D. H.; Shibata, E. I.; Shipsey, I. P. J.; Pavlunin, V.; Cronin-Hennessy, D.; Lyon, A. L.; Thorndike, E. H.; Coan, T. E.; Fadeyev, V.; Gao, Y. S.; Maravin, Y.; Narsky, I.; Stroynowski, R.; Ye, J.; Włodek, T.; Artuso, M.; Ayad, R.; Boulahouache, C.; Bukin, K.; Dambasuren, E.; Majumder, G.; Moneti, G. C.; Mountain, R.; Schuh, S.; Skwarnicki, T.; Stone, S.; Wang, J. C.; Wolf, A.; Wu, J.

doi:10.1103/physrevd.63.092001

Cited by 116 publications

(37 citation statements)

References 19 publications

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“…As a cross-check, one may consider the previous Dalitz plot fit results obtained by the CLEO experiment [34]. Since we adopted the same phase conventions, a comparison of the amplitudes and phases should straightforward.…”

Section: Parametermentioning

confidence: 99%

“…the K * − (892) and K * 0 (892), the results for the amplitudes and phases seem reasonably similar. It must be noted that they excluded the Table 7.4: Fit results for the RS Dalitz plot fit of the CLEO analysis [34].…”

Section: Parametermentioning

confidence: 99%

“…To parametrize them, we use the Blatt-Weisskopf penetration form factors with the same convention used by the CLEO experiment [34]. In Table 2.1 the parametrization of the form factors is given 6 .…”

Section: Blatt-weisskopf Penetration Factorsmentioning

confidence: 99%

“…In order to specify the matrix element |M| 2 defined in Section 2.2.1, an Isobar model approach is adopted [33,34]. The basic idea in this model is that the original three-body decay (in our case the D 0 decay) can be considered as a two steps phenomenon: the D 0 decays into a long living particle (typically a pion or a kaon) and into a resonance.…”

Section: M| 2 Parametrization: the Isobar Modelmentioning

confidence: 99%

“…which used the same convention [34]. The ρ + (770) amplitude and phase are fixed to 1 and 0 respectively.…”

mentioning

confidence: 99%

See 4 more Smart Citations

Measurement of D0 - $\bar{D}$0 Mixing With a Time-Dependent Amplitude Analysis of D0 → K+ π- π0

Pelliccioni

2013

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Section: Parametermentioning

confidence: 99%

Section: Parametermentioning

confidence: 99%

Section: Blatt-weisskopf Penetration Factorsmentioning

confidence: 99%

Section: M| 2 Parametrization: the Isobar Modelmentioning

confidence: 99%

“…which used the same convention [34]. The ρ + (770) amplitude and phase are fixed to 1 and 0 respectively.…”

mentioning

confidence: 99%

See 3 more Smart Citations

Measurement of D0 - $\bar{D}$0 Mixing With a Time-Dependent Amplitude Analysis of D0 → K+ π- π0

Pelliccioni

2013

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B, D and K decays

Buchalla¹,

Komatsubara²,

Muheim³

et al. 2009

Flavor in the Era of the LHC

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Recent Beijing Spectroscopy (BES) results

Weiguo

2008

Sci. China Ser. G-Phys. Mech. Astron.

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Recent experimental results from Beijing Spectroscopy (BES) are reviewed, including the hadron spectroscopy from J/\ decays, and a number of new states are found or confirmed, including V, N, X(1835), ZM threshold enhancement in J/\oJZM , a broad resonance in J/\oK K S 0 , decay studies of \ (2S) and F CJ , as well as the results of \ (3770) nondecays. The current status of BEPCII/BESIII, the major upgrade of BEPC/BESII, is also reported. Beijing Spectroscopy, hadron spectroscopy, charm physics, BEPCII The results in this paper are based on the data collected at Beijing Electron-Positron Collider. Beijing Spectroscopy (BES) was upgraded to BESII in 1997, and had been taking data till the end of April in 2004, with a data sample including 58 M J/\ events, 14 M \ (2S) events and data around \ (3770) with a luminosity of about 27 pb 1 . Many results have been obtained from those data, and about 80 papers have been published on the famous international journals, such as Phys Rev Lett, Phys Lett B and Phys Rev D, in which more than 10 papers were published on Phys Rev Lett. This article is divided into several sub-sessions about the results from J/\, \ (2S) and \(3770),There has been evidence for a low mass pole in the early DM2 [1] and BESI [2] data on J/\ to ZS S . A huge event concentration in the I = 0 S-wave S S channel was seen in the region of m S S around 500 600 MeV in a pp central production experiment [3] . This peak is too large to be explained as a background [4] . There have been many studies on the possible resonance structure in SS elastic scattering [5] . It was later proved that the V(sigma) resonance is unavoidable in the chiral perturbation theory in order to explain the S S scattering phase shift data [6] . E791 experiment

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Dalitz analysis of the decayD0→K−π+<

Cited by 116 publications

References 19 publications

Measurement of D<sup>0</sup> - $\bar{D}$<sup>0</sup> Mixing With a Time-Dependent Amplitude Analysis of D<sup>0</sup> → K<sup>+ </sup>π<sup>-</sup> π<sup>0</sup>

Measurement of D<sup>0</sup> - $\bar{D}$<sup>0</sup> Mixing With a Time-Dependent Amplitude Analysis of D<sup>0</sup> → K<sup>+ </sup>π<sup>-</sup> π<sup>0</sup>

B, D and K decays

Recent Beijing Spectroscopy (BES) results

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