Sirunyan, AM; Tumasyan, A; Adam, W; Bergauer, T; Dragicevic, M; Escalante Del Valle, A; Frühwirth, R; Jeitler, M; Krammer, N; Lechner, L; Liko, D; Mikulec, I; Pitters, FM; Rad, N; Schieck, J; Schöfbeck, R; Spanring, M; Templ, S; Waltenberger, W; Wulz, C-E; Zarucki, M; Chekhovsky, V; Litomin, A; Makarenko, V; Suarez Gonzalez, J; Darwish, MR; De Wolf, EA; Janssen, X; Kello, T; Lelek, A; Pieters, M; Rejeb Sfar, H; Van Haevermaet, H; Van Mechelen, P; Van Putte, S; Van Remortel, N; Blekman, F; Bols, ES; Chhibra, SS; D’Hondt, J; De Clercq, J; Lontkovskyi, D; Lowette, S; Marchesini, I; Moortgat, S; Morton, A; Müller, D; Python, Q; Tavernier, S; Van Doninck, W; Van Mulders, P; Beghin, D; Bilin, B; Clerbaux, B; De Lentdecker, G; Dorney, B; Favart, L; Grebenyuk, A; Kalsi, AK; Makarenko, I; Moureaux, L; Pétré, L; Popov, A; Postiau, N; Starling, E; Thomas, L; Vander Velde, C; Vanlaer, P; Vannerom, D; Wezenbeek, L; Cornelis, T; Dobur, D; Gruchala, M; Khvastunov, I; Mestdach, G; Niedziela, M; Roskas, C; Skovpen, K; Tytgat, M; Verbeke, W; Vermassen, B; Vit, M; Bruno, G; Bury, F; Caputo, C

doi:10.1007/jhep04(2021)124

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Angular analysis of the decay B+→ K∗(892)+μ+μ− in proton-proton collisions at s = 8 TeV

2021

Sirunyan, AM;
Tumasyan, A;
Adam, W;
Bergauer, T;
Dragicevic, M;
Escalante Del Valle, A;
Frühwirth, R;
Jeitler, M;
Krammer, N;
Lechner, L;
Liko, D;
Mikulec, I;
Pitters, FM;
Rad, N;
Schieck, J;
Schöfbeck, R;
Spanring, M;
Templ, S;
Waltenberger, W;
Wulz, C-E;
Zarucki, M;
Chekhovsky, V;
Litomin, A;
Makarenko, V;
Suarez Gonzalez, J;
Darwish, MR;
De Wolf, EA;
Janssen, X;
Kello, T;
Lelek, A;
Pieters, M;
Rejeb Sfar, H;
Van Haevermaet, H;
Van Mechelen, P;
Van Putte, S;
Van Remortel, N;
Blekman, F;
Bols, ES;
Chhibra, SS;
D’Hondt, J;
De Clercq, J;
Lontkovskyi, D;
Lowette, S;
Marchesini, I;
Moortgat, S;
Morton, A;
Müller, D;
Python, Q;
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Published Web Location

https://doi.org/10.1007/jhep04(2021)124

Abstract

Angular distributions of the decay B+→ K∗(892)+μ+μ− are studied using events collected with the CMS detector in s = 8 TeV proton-proton collisions at the LHC, corresponding to an integrated luminosity of 20.0 fb−1. The forward-backward asymmetry of the muons and the longitudinal polarization of the K∗(892)+ meson are determined as a function of the square of the dimuon invariant mass. These are the first results from this exclusive decay mode and are in agreement with a standard model prediction. [Figure not available: see fulltext.]

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UC Riverside

Angular analysis of the decay B+→ K∗(892)+μ+μ− in proton-proton collisions at s = 8 TeV

Published Web Location