χc1 and χc2 Resonance Parameters with the Decays χc1,c2 →j /ψμ+μ-

Standard

χc1 and χc2 Resonance Parameters with the Decays χc1,c2 →j /ψμ+μ-. / The LHCb Collaboration.

In: Physical Review Letters, Vol. 119, No. 22, 221801, 28.11.2017.

Research output: Contribution to journal › Article › peer-review

Harvard

The LHCb Collaboration 2017, 'χc1 and χc2 Resonance Parameters with the Decays χc1,c2 →j /ψμ+μ-', Physical Review Letters, vol. 119, no. 22, 221801. https://doi.org/10.1103/PhysRevLett.119.221801

APA

The LHCb Collaboration (2017). χc1 and χc2 Resonance Parameters with the Decays χc1,c2 →j /ψμ+μ-. Physical Review Letters, 119(22), [221801]. https://doi.org/10.1103/PhysRevLett.119.221801

Vancouver

The LHCb Collaboration. χc1 and χc2 Resonance Parameters with the Decays χc1,c2 →j /ψμ+μ-. Physical Review Letters. 2017 Nov 28;119(22):221801. doi: 10.1103/PhysRevLett.119.221801

Author

The LHCb Collaboration. / χc1 and χc2 Resonance Parameters with the Decays χc1,c2 →j /ψμ+μ-. In: Physical Review Letters. 2017 ; Vol. 119, No. 22.

BibTeX

@article{3b70918733bc4df4aa2479a2aa49ed61,

title = "χc1 and χc2 Resonance Parameters with the Decays χc1,c2 →j /ψμ+μ-",

abstract = "The decays χc1→J/ψμ+μ- and χc2→J/ψμ+μ- are observed and used to study the resonance parameters of the χc1 and χc2 mesons. The masses of these states are measured to be m(χc1)=3510.71±0.04(stat)±0.09(syst) MeV and m(χc2)=3556.10±0.06(stat)±0.11(syst) MeV, where the knowledge of the momentum scale for charged particles dominates the systematic uncertainty. The momentum-scale uncertainties largely cancel in the mass difference m(χc2)-m(χc1)=45.39±0.07(stat)±0.03(syst) MeV. The natural width of the χc2 meson is measured to be Γ(χc2)=2.10±0.20(stat)±0.02(syst) MeV. These results are in good agreement with and have comparable precision to the current world averages.",

keywords = "CHARMONIUM, STATES, TOOL",

author = "{The LHCb Collaboration} and R. Aaij and B. Adeva and M. Adinolfi and Z. Ajaltouni and S. Akar and J. Albrecht and F. Alessio and M. Alexander and {Alfonso Albero}, A. and S. Ali and G. Alkhazov and {Alvarez Cartelle}, P. and Alves, {A. A.} and S. Amato and S. Amerio and Y. Amhis and L. An and L. Anderlini and G. Andreassi and M. Andreotti and Andrews, {J. E.} and Appleby, {R. B.} and F. Archilli and P. D'Argent and {Arnau Romeu}, J. and A. Artamonov and M. Artuso and E. Aslanides and M. Atzeni and G. Auriemma and M. Baalouch and I. Babuschkin and S. Bachmann and Back, {J. J.} and A. Badalov and C. Baesso and S. Baker and V. Balagura and W. Baldini and A. Baranov and Barlow, {R. J.} and C. Barschel and S. Barsuk and W. Barter and F. Baryshnikov and A. Bondar and S. Eidelman and P. Krokovny and L. Shekhtman and V. Vorobyev",

note = "Publisher Copyright: {\textcopyright} 2017 CERN, for the LHCb Collaboration.",

year = "2017",

month = nov,

day = "28",

doi = "10.1103/PhysRevLett.119.221801",

language = "English",

volume = "119",

journal = "Physical Review Letters",

issn = "0031-9007",

publisher = "American Physical Society",

number = "22",

}

RIS

TY - JOUR

T1 - χc1 and χc2 Resonance Parameters with the Decays χc1,c2 →j /ψμ+μ-

AU - The LHCb Collaboration

AU - Aaij, R.

AU - Adeva, B.

AU - Adinolfi, M.

AU - Ajaltouni, Z.

AU - Akar, S.

AU - Albrecht, J.

AU - Alessio, F.

AU - Alexander, M.

AU - Alfonso Albero, A.

AU - Ali, S.

AU - Alkhazov, G.

AU - Alvarez Cartelle, P.

AU - Alves, A. A.

AU - Amato, S.

AU - Amerio, S.

AU - Amhis, Y.

AU - An, L.

AU - Anderlini, L.

AU - Andreassi, G.

AU - Andreotti, M.

AU - Andrews, J. E.

AU - Appleby, R. B.

AU - Archilli, F.

AU - D'Argent, P.

AU - Arnau Romeu, J.

AU - Artamonov, A.

AU - Artuso, M.

AU - Aslanides, E.

AU - Atzeni, M.

AU - Auriemma, G.

AU - Baalouch, M.

AU - Babuschkin, I.

AU - Bachmann, S.

AU - Back, J. J.

AU - Badalov, A.

AU - Baesso, C.

AU - Baker, S.

AU - Balagura, V.

AU - Baldini, W.

AU - Baranov, A.

AU - Barlow, R. J.

AU - Barschel, C.

AU - Barsuk, S.

AU - Barter, W.

AU - Baryshnikov, F.

AU - Bondar, A.

AU - Eidelman, S.

AU - Krokovny, P.

AU - Shekhtman, L.

AU - Vorobyev, V.

PY - 2017/11/28

Y1 - 2017/11/28

N2 - The decays χc1→J/ψμ+μ- and χc2→J/ψμ+μ- are observed and used to study the resonance parameters of the χc1 and χc2 mesons. The masses of these states are measured to be m(χc1)=3510.71±0.04(stat)±0.09(syst) MeV and m(χc2)=3556.10±0.06(stat)±0.11(syst) MeV, where the knowledge of the momentum scale for charged particles dominates the systematic uncertainty. The momentum-scale uncertainties largely cancel in the mass difference m(χc2)-m(χc1)=45.39±0.07(stat)±0.03(syst) MeV. The natural width of the χc2 meson is measured to be Γ(χc2)=2.10±0.20(stat)±0.02(syst) MeV. These results are in good agreement with and have comparable precision to the current world averages.

AB - The decays χc1→J/ψμ+μ- and χc2→J/ψμ+μ- are observed and used to study the resonance parameters of the χc1 and χc2 mesons. The masses of these states are measured to be m(χc1)=3510.71±0.04(stat)±0.09(syst) MeV and m(χc2)=3556.10±0.06(stat)±0.11(syst) MeV, where the knowledge of the momentum scale for charged particles dominates the systematic uncertainty. The momentum-scale uncertainties largely cancel in the mass difference m(χc2)-m(χc1)=45.39±0.07(stat)±0.03(syst) MeV. The natural width of the χc2 meson is measured to be Γ(χc2)=2.10±0.20(stat)±0.02(syst) MeV. These results are in good agreement with and have comparable precision to the current world averages.

KW - CHARMONIUM

KW - STATES

KW - TOOL

UR - http://www.scopus.com/inward/record.url?scp=85037680860&partnerID=8YFLogxK

U2 - 10.1103/PhysRevLett.119.221801

DO - 10.1103/PhysRevLett.119.221801

M3 - Article

C2 - 29286773

AN - SCOPUS:85037680860

VL - 119

JO - Physical Review Letters

JF - Physical Review Letters

SN - 0031-9007

IS - 22

M1 - 221801

ER -

ID: 9869465