<P>The chi(b1)(3P) and chi(b2)(3P) states are observed through their gamma(3S)(gamma) decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a center-of-mass energy o...
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https://www.riss.kr/link?id=A107459300
Sirunyan, A. M. ; Tumasyan, A. ; Adam, W. ; Ambrogi, F. ; Asilar, E. ; Bergauer, T. ; Brandstetter, J. ; Dragicevic, M. ; Erö ; , J. ; Escalante Del Valle, A. ; Flechl, M. ; Frü ; hwirth, R. ; Ghete, V. M. ; Hrubec, J. ; Jeitler, M. ; Krammer, N. ; Krä ; tschmer, I. ; Liko, D. ; Madlener, T. ; Mikulec, I. ; Rad, N. ; Rohringer, H. ; Schieck, J. ; Schö ; fbeck, R. ; Spanring, M. ; Spitzbart, D. ; Taurok, A. ; Waltenberger, W. ; Wittmann, J. ; Wulz, C.-E. ; Zarucki, M. ; Chekhovsky, V. ; Mossolov, V. ; Suarez Gonzalez, J. ; De Wolf, E. A. ; Di Croce, D. ; Janssen, X. ; Lauwers, J. ; Pieters, M. ; Van De Klundert, M. ; Van Haevermaet, H. ; Van Mechelen, P. ; Van Remortel, N. ; Abu Zeid, S. ; Blekman, F. ; D’Hondt, J. ; De Bruyn, I. ; De Clercq, J. ; Deroover, K. ; Flouris, G. ; Lontkovskyi, D. ; Lowette, S. ; Marchesini, I. ; Moortgat, S. ; Moreels, L. ; Python, Q. ; Skovpen, K. ; Tavernier, S. ; Van Doninck, W. ; Van Mulders, P. ; Van Parijs, I. ; Beghin, D. ; Bilin, B. ; Brun,
2018
-
SCI,SCIE,SCOPUS
학술저널
092002
0
상세조회0
다운로드다국어 초록 (Multilingual Abstract)
<P>The chi(b1)(3P) and chi(b2)(3P) states are observed through their gamma(3S)(gamma) decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a center-of-mass energy o...
<P>The chi(b1)(3P) and chi(b2)(3P) states are observed through their gamma(3S)(gamma) decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 80.0 fb(-1). The gamma(3S) mesons are identified through their dimuon decay channel, while the low-energy photons are detected after converting to e(+)e(-) pairs in the silicon tracker, leading to a chi(b)(3P) mass resolution of 2.2 MeV. This is the first time that the J = 1 and 2 states are well resolved and their masses individually measured: 10513.42 +/- 0.41(stat) +/- 0.18(syst) MeV and 10524.02 +/- 0.57(stat) +/- 0.18(syst) MeV; they are determined with respect to the world-average value of gamma(3S) mass, which has an uncertainty of 0.5 MeV. The mass splitting is measured to be 10.60 +/- 0.64(stat) +/- 0.17(syst) MeV.</P>
Flatbands and Emergent Ferromagnetic Ordering in Fe3Sn2 Kagome Lattices
Spin Thermal Hall Conductivity of a Kagome Antiferromagnet