Erratum to

Search for B decays to final states with the η c meson (Journal of High Energy Physics, (2015), 2015, 6, (132), 10.1007/JHEP06(2015)132)

The Belle Collaboration

Research output: Contribution to journalComment/debate

Abstract

(Figure presented.)Figure 1. Corrected figure 10. The combined fit projections of the ηcη invariant mass distributions in case of the η→γ γ(left) and η→ π+π-π0 (right) modes corresponding to the search for the X(3915) resonance. (Figure presented.) Figure 2. Corrected figure 11. The ηcπ0 invariant mass distribution corresponding to the search for the X(3915) resonance. We have found an error in the fit of the ηcη and ηcπ0 invariant masses that is used to search for the X(3915) state. The corrected fits are shown in figures 1 and 2. The resonance parameters are fixed to the world average values (3918 MeV/c2 and 20 MeV/c2 for mass and width correspondingly). The fit results are summarized in table 1. Changes in the fits of the X(3915) resonance lead to changes of the corresponding upper limits. The corrected upper limits on the X(3915) production and decay branching fraction products are summarized in table 2. All other results of the paper are correct. (Table presented.) Table 2. Corrected entry of table 8. Results of branching fraction measurements for the B decays containing intermediate X(3915).

Original languageEnglish
Article number88
JournalJournal of High Energy Physics
Volume2017
Issue number2
DOIs
Publication statusPublished - 2017 Feb 1

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mesons
physics
decay
mass distribution
energy
entry
projection
products

ASJC Scopus subject areas

  • Nuclear and High Energy Physics

Cite this

Erratum to : Search for B decays to final states with the η c meson (Journal of High Energy Physics, (2015), 2015, 6, (132), 10.1007/JHEP06(2015)132). / The Belle Collaboration.

In: Journal of High Energy Physics, Vol. 2017, No. 2, 88, 01.02.2017.

Research output: Contribution to journalComment/debate

@article{0870db7f41384060b28a5fc962d8a983,
title = "Erratum to: Search for B decays to final states with the η c meson (Journal of High Energy Physics, (2015), 2015, 6, (132), 10.1007/JHEP06(2015)132)",
abstract = "(Figure presented.)Figure 1. Corrected figure 10. The combined fit projections of the ηcη invariant mass distributions in case of the η→γ γ(left) and η→ π+π-π0 (right) modes corresponding to the search for the X(3915) resonance. (Figure presented.) Figure 2. Corrected figure 11. The ηcπ0 invariant mass distribution corresponding to the search for the X(3915) resonance. We have found an error in the fit of the ηcη and ηcπ0 invariant masses that is used to search for the X(3915) state. The corrected fits are shown in figures 1 and 2. The resonance parameters are fixed to the world average values (3918 MeV/c2 and 20 MeV/c2 for mass and width correspondingly). The fit results are summarized in table 1. Changes in the fits of the X(3915) resonance lead to changes of the corresponding upper limits. The corrected upper limits on the X(3915) production and decay branching fraction products are summarized in table 2. All other results of the paper are correct. (Table presented.) Table 2. Corrected entry of table 8. Results of branching fraction measurements for the B decays containing intermediate X(3915).",
author = "{The Belle Collaboration} and A. Vinokurova and A. Kuzmin and S. Eidelman and A. Abdesselam and I. Adachi and H. Aihara and K. Arinstein and Asner, {D. M.} and T. Aushev and R. Ayad and Bakich, {A. M.} and V. Bansal and V. Bhardwaj and B. Bhuyan and A. Bobrov and A. Bondar and A. Bozek and M. Bračko and Browder, {T. E.} and V. Chekelian and Cheon, {B. G.} and K. Chilikin and R. Chistov and K. Cho and Choi, {S. K.} and Y. Choi and D. Cinabro and J. Dingfelder and Z. Doležal and Z. Dr{\'a}sal and A. Drutskoy and D. Dutta and D. Epifanov and H. Farhat and Fast, {J. E.} and T. Ferber and V. Gaur and N. Gabyshev and A. Garmash and R. Gillard and Goh, {Y. M.} and B. Golob and J. Haba and K. Hayasaka and H. Hayashii and He, {X. H.} and Hou, {W. S.} and K. Inami and A. Ishikawa and Eunil Won",
year = "2017",
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AU - The Belle Collaboration

AU - Vinokurova, A.

AU - Kuzmin, A.

AU - Eidelman, S.

AU - Abdesselam, A.

AU - Adachi, I.

AU - Aihara, H.

AU - Arinstein, K.

AU - Asner, D. M.

AU - Aushev, T.

AU - Ayad, R.

AU - Bakich, A. M.

AU - Bansal, V.

AU - Bhardwaj, V.

AU - Bhuyan, B.

AU - Bobrov, A.

AU - Bondar, A.

AU - Bozek, A.

AU - Bračko, M.

AU - Browder, T. E.

AU - Chekelian, V.

AU - Cheon, B. G.

AU - Chilikin, K.

AU - Chistov, R.

AU - Cho, K.

AU - Choi, S. K.

AU - Choi, Y.

AU - Cinabro, D.

AU - Dingfelder, J.

AU - Doležal, Z.

AU - Drásal, Z.

AU - Drutskoy, A.

AU - Dutta, D.

AU - Epifanov, D.

AU - Farhat, H.

AU - Fast, J. E.

AU - Ferber, T.

AU - Gaur, V.

AU - Gabyshev, N.

AU - Garmash, A.

AU - Gillard, R.

AU - Goh, Y. M.

AU - Golob, B.

AU - Haba, J.

AU - Hayasaka, K.

AU - Hayashii, H.

AU - He, X. H.

AU - Hou, W. S.

AU - Inami, K.

AU - Ishikawa, A.

AU - Won, Eunil

PY - 2017/2/1

Y1 - 2017/2/1

N2 - (Figure presented.)Figure 1. Corrected figure 10. The combined fit projections of the ηcη invariant mass distributions in case of the η→γ γ(left) and η→ π+π-π0 (right) modes corresponding to the search for the X(3915) resonance. (Figure presented.) Figure 2. Corrected figure 11. The ηcπ0 invariant mass distribution corresponding to the search for the X(3915) resonance. We have found an error in the fit of the ηcη and ηcπ0 invariant masses that is used to search for the X(3915) state. The corrected fits are shown in figures 1 and 2. The resonance parameters are fixed to the world average values (3918 MeV/c2 and 20 MeV/c2 for mass and width correspondingly). The fit results are summarized in table 1. Changes in the fits of the X(3915) resonance lead to changes of the corresponding upper limits. The corrected upper limits on the X(3915) production and decay branching fraction products are summarized in table 2. All other results of the paper are correct. (Table presented.) Table 2. Corrected entry of table 8. Results of branching fraction measurements for the B decays containing intermediate X(3915).

AB - (Figure presented.)Figure 1. Corrected figure 10. The combined fit projections of the ηcη invariant mass distributions in case of the η→γ γ(left) and η→ π+π-π0 (right) modes corresponding to the search for the X(3915) resonance. (Figure presented.) Figure 2. Corrected figure 11. The ηcπ0 invariant mass distribution corresponding to the search for the X(3915) resonance. We have found an error in the fit of the ηcη and ηcπ0 invariant masses that is used to search for the X(3915) state. The corrected fits are shown in figures 1 and 2. The resonance parameters are fixed to the world average values (3918 MeV/c2 and 20 MeV/c2 for mass and width correspondingly). The fit results are summarized in table 1. Changes in the fits of the X(3915) resonance lead to changes of the corresponding upper limits. The corrected upper limits on the X(3915) production and decay branching fraction products are summarized in table 2. All other results of the paper are correct. (Table presented.) Table 2. Corrected entry of table 8. Results of branching fraction measurements for the B decays containing intermediate X(3915).

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