• 1 (BaBar Collaboration)
  • 2 (CLEO Collaboration) R) (2006)
  • 3
  • 4
  • 4 ;
  • 4 ;
  • 4 ;
  • 4 ; and
  • 5
  • 6 (Particle Data Group)
  • 7
  • 8
  • 9 [arXiv:1209.6450 [hep-exp]]
  • 10
  • 10
  • 10 and Yu.A. Simonov
  • 10
  • 10 [arXiv:1106.2284 [hepph]]
  • 10 and
  • 11 See, for example
  • 11
  • 11
  • 11
  • 11 (2003) [hep-ph/0308277]
  • 11
  • 11
  • 11
  • 11
  • 11
  • 11
  • 11 &
  • 12 (BESIII Collaboration)
  • 13
  • 14
  • 15 [arXiv:1304.1301 [hep-ph]]
  • 15
  • 15
  • 15
  • 15 and C.-Y. Cui et al [arXiv:1304.1850]
  • 16 (BESIII Collaboration) [arXiv:1308.2760 [hep-ex]]
  • 16 and M. Ablikim et al. (BESIII Collaboration) [arXiv:1309.1896 [hep-ex]]
  • 17 (2013)
  • 17 and
  • 17 See, also
  • 18 (BESIII Collaboration), Nucl. Istrum. and Methods Phys. Res., Sect. A 614, 345 (2010)
  • 19 Nucl. Istrum. and Methods Phys. Res., Sect. A 462, 152 (2001)
  • 20
  • 20 ;
  • 21 Nucl. Istrum. and Methods Phys. Res., Sect. A 506, 250 (2003)
  • 22
  • 23 Chinese Phys. C 32, 599 (2008)
  • 24
  • 25 We minimize the effect of the D mass resolution by plotting Mrecoil = RM(πD) + M(D) - mD, where RM(πD) is the recoil mass inferred from four-momentum conservation and M(D) is the measured D mass
  • 26 (BESIII Collaboration)
  • 27 See, for example arXiv: and references cited therein [hep-ph/0001206]
  • 28 We use a second-order QED calculation and unpublished BESIII energy-dependent measurements of σ(e+ e- → πD ¯D∗) to compute the radiative correction
  • 28 see