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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). / Belle Collaboration.

в: Journal of High Energy Physics, Том 2017, № 2, 88, 01.02.2017.

Результаты исследований: Научные публикации в периодических изданиях › комментарий, выступление › Рецензирование

Harvard

Belle Collaboration 2017, '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)', Journal of High Energy Physics, Том. 2017, № 2, 88. https://doi.org/10.1007/JHEP02(2017)088

APA

Belle Collaboration (2017). 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). Journal of High Energy Physics, 2017(2), [88]. https://doi.org/10.1007/JHEP02(2017)088

Vancouver

Belle Collaboration. 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). Journal of High Energy Physics. 2017 февр. 1;2017(2):88. doi: 10.1007/JHEP02(2017)088

Author

Belle Collaboration. / 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). в: Journal of High Energy Physics. 2017 ; Том 2017, № 2.

BibTeX

@article{e7edeb88c38e40af8069448a5d4511db,
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. Bra{\v c}ko 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. Dole{\v z}al 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 P. Krokovny and P. Lukin and D. Matvienko and V. Shebalin and B. Shwartz and V. Vorobyev and V. Zhulanov",
year = "2017",
month = feb,
day = "1",
doi = "10.1007/JHEP02(2017)088",
language = "English",
volume = "2017",
journal = "Journal of High Energy Physics",
issn = "1029-8479",
publisher = "Springer US",
number = "2",

}

RIS

TY - JOUR

T1 - Erratum to

T2 - 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)

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 - Krokovny, P.

AU - Lukin, P.

AU - Matvienko, D.

AU - Shebalin, V.

AU - Shwartz, B.

AU - Vorobyev, V.

AU - Zhulanov, V.

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).

UR - http://www.scopus.com/inward/record.url?scp=85013155812&partnerID=8YFLogxK

U2 - 10.1007/JHEP02(2017)088

DO - 10.1007/JHEP02(2017)088

M3 - Comment/debate

AN - SCOPUS:85013155812

VL - 2017

JO - Journal of High Energy Physics

JF - Journal of High Energy Physics

SN - 1029-8479

IS - 2

M1 - 88

ER -

ID: 10181861