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CMS-BPH-15-009 ; CERN-EP-2020-188
Angular analysis of the decay B+K(892)+μ+μ in proton-proton collisions at s= 8 TeV
JHEP 04 (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 fb1. 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.
Figures & Tables Summary References CMS Publications
Figures

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Figure 1:
Definition of the angular observables θK (left), θ (middle), and ϕ (right) for the decay B+K+μ+μ.

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Figure 2:
The signal efficiency as a function of cosθK (upper row) and cosθ (lower row) from simulation for the q2 ranges indicated. The vertical bars indicate the statistical uncertainty. The curves show the projection of the fitted result obtained from the two-dimensional fit, as described in the text.

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Figure 2-a:
The signal efficiency as a function of cosθK from simulation for the q2 range indicated. The vertical bars indicate the statistical uncertainty. The curve shows the projection of the fitted result obtained from the two-dimensional fit, as described in the text.

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Figure 2-b:
The signal efficiency as a function of cosθK from simulation for the q2 range indicated. The vertical bars indicate the statistical uncertainty. The curve shows the projection of the fitted result obtained from the two-dimensional fit, as described in the text.

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Figure 2-c:
The signal efficiency as a function of cosθK from simulation for the q2 range indicated. The vertical bars indicate the statistical uncertainty. The curve shows the projection of the fitted result obtained from the two-dimensional fit, as described in the text.

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Figure 2-d:
The signal efficiency as a function of cosθ from simulation for the q2 range indicated. The vertical bars indicate the statistical uncertainty. The curve shows the projection of the fitted result obtained from the two-dimensional fit, as described in the text.

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Figure 2-e:
The signal efficiency as a function of cosθ from simulation for the q2 range indicated. The vertical bars indicate the statistical uncertainty. The curve shows the projection of the fitted result obtained from the two-dimensional fit, as described in the text.

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Figure 2-f:
The signal efficiency as a function of cosθ from simulation for the q2 range indicated. The vertical bars indicate the statistical uncertainty. The curve shows the projection of the fitted result obtained from the two-dimensional fit, as described in the text.

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Figure 3:
The K0Sπ+μ+μ invariant mass (upper row), cosθK (middle row), and cosθ (lower row) distributions for each q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled areas, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 3-a:
The K0Sπ+μ+μ invariant mass distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 3-b:
The K0Sπ+μ+μ invariant mass distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 3-c:
The K0Sπ+μ+μ invariant mass distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 3-d:
The K0Sπ+μ+μ cosθK distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 3-e:
The K0Sπ+μ+μ cosθK distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 3-f:
The K0Sπ+μ+μ cosθK distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 3-g:
The K0Sπ+μ+μ cosθ distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 3-h:
The K0Sπ+μ+μ cosθ distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 3-i:
The K0Sπ+μ+μ cosθ distribution for the indeicated q2 range is shown for data, along with the fit projections. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 4:
The cosθK (upper row) and cosθ (lower row) distributions for each q2 range is shown for data in the invariant mass region 5.18 <m< 5.38 GeV, along with the fit projections for the same region. The vertical bars on the data points indicate the statistical uncertainty. The filled areas, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 4-a:
The cosθK distribution for the indicated q2 range is shown for data in the invariant mass region 5.18 <m< 5.38 GeV, along with the fit projections for the same region. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 4-b:
The cosθK distribution for the indicated q2 range is shown for data in the invariant mass region 5.18 <m< 5.38 GeV, along with the fit projections for the same region. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 4-c:
The cosθK distribution for the indicated q2 range is shown for data in the invariant mass region 5.18 <m< 5.38 GeV, along with the fit projections for the same region. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 4-d:
The cosθ distribution for the indicated q2 range is shown for data in the invariant mass region 5.18 <m< 5.38 GeV, along with the fit projections for the same region. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 4-e:
The cosθ distribution for the indicated q2 range is shown for data in the invariant mass region 5.18 <m< 5.38 GeV, along with the fit projections for the same region. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 4-f:
The cosθ distribution for the indicated q2 range is shown for data in the invariant mass region 5.18 <m< 5.38 GeV, along with the fit projections for the same region. The vertical bars on the data points indicate the statistical uncertainty. The filled area, dashed line, and solid line represent the signal, background, and total contributions, respectively.

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Figure 5:
The measured values of AFB (left) and FL (right) versus q2 for B+K+μ+μ decays are shown with filled squares, centered on the q2 bin. The statistical (total) uncertainty is shown by inner (outer) vertical bars. The vertical shaded regions correspond to the regions dominated by B+K+J/ψ and B+K+ψ(2S) decays. The SM predictions and associated uncertainties are shown by the filled circles and vertical bars, with the points slightly offset from the center of the q2 bin for clarity.

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Figure 5-a:
The measured values of AFB versus q2 for B+K+μ+μ decays are shown with filled squares, centered on the q2 bin. The statistical (total) uncertainty is shown by inner (outer) vertical bars. The vertical shaded regions correspond to the regions dominated by B+K+J/ψ and B+K+ψ(2S) decays. The SM predictions and associated uncertainties are shown by the filled circles and vertical bars, with the points slightly offset from the center of the q2 bin for clarity.

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Figure 5-b:
The measured values of FL versus q2 for B+K+μ+μ decays are shown with filled squares, centered on the q2 bin. The statistical (total) uncertainty is shown by inner (outer) vertical bars. The vertical shaded regions correspond to the regions dominated by B+K+J/ψ and B+K+ψ(2S) decays. The SM predictions and associated uncertainties are shown by the filled circles and vertical bars, with the points slightly offset from the center of the q2 bin for clarity.
Tables

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Table 1:
Sources of systematic uncertainties and the effect on AFB and FL. The values given are absolute and the ranges indicate the variation over the q2 bins.

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Table 2:
The YS, AFB, and FL values from the fit for each q2 range. The first uncertainty is statistical and the second is systematic.
Summary
The first angular analysis of the exclusive decay B+K(892)+μ+μ, including the charge-conjugate state, has been performed using a sample of proton-proton collisions at a center-of-mass energy of 8 TeV. The data were collected with the CMS detector in 2012 at the LHC, and correspond to an integrated luminosity of 20.0 fb1. For each bin of the dimuon invariant mass squared (q2), a three-dimensional unbinned maximum likelihood fit is performed on the distributions of the K(892)(892)+μ+μ invariant mass and two decay angles. The muon forward-backward asymmetry, AFB, and the K(892)+ longitudinal polarization fraction, FL, are extracted from the fit in bins of q2 and found to be consistent with a standard model prediction.
References
1 CMS Collaboration CMS luminosity based on pixel cluster counting -- summer 2013 update CMS-PAS-LUM-13-001 CMS-PAS-LUM-13-001
2 CDF Collaboration Measurements of the angular distributions in the decays BK()μ+μ at CDF PRL 108 (2012) 081807 1108.0695
3 LHCb Collaboration Differential branching fraction and angular analysis of the decay B0K0μ+μ JHEP 08 (2013) 131 1304.6325
4 CMS Collaboration Angular analysis and branching fraction measurement of the decay B0K0μ+μ PLB 727 (2013) 77 CMS-BPH-11-009
1308.3409
5 CMS Collaboration Angular analysis of the decay B0K0μ+μ from pp collisions at s= 8 TeV PLB 753 (2016) 424 CMS-BPH-13-010
1507.08126
6 BaBar Collaboration Angular distributions in the decay BK+ PRD 79 (2009) 031102 0804.4412
7 Belle Collaboration Measurement of the differential branching fraction and forward-backward asymmetry for BK()+ PRL 103 (2009) 171801 0904.0770
8 C. Bobeth, G. Hiller, and D. van Dyk The benefits of ¯B¯K+ decays at low recoil JHEP 07 (2010) 098 1006.5013
9 C. Bobeth, G. Hiller, D. van Dyk, and C. Wacker The decay ¯B¯K+ at low hadronic recoil and model-independent ΔB= 1 constraints JHEP 01 (2012) 107 1111.2558
10 C. Bobeth, G. Hiller, and D. van Dyk General analysis of ¯B¯K()+ decays at low recoil PRD 87 (2012) 034016 1212.2321
11 A. Ali, G. Kramer, and G. Zhu BK+ decay in soft-collinear effective theory EPJC 47 (2006) 625 hep-ph/0601034
12 W. Altmannshofer et al. Symmetries and asymmetries of BKμ+μ decays in the standard model and beyond JHEP 01 (2009) 019 0811.1214
13 W. Altmannshofer, P. Paradisi, and D. M. Straub Model-independent constraints on new physics in bs transitions JHEP 04 (2012) 008 1111.1257
14 S. Jager and J. Martin Camalich On BV at small dilepton invariant mass, power corrections, and new physics JHEP 05 (2013) 043 1212.2263
15 S. Descotes-Genon, T. Hurth, J. Matias, and J. Virto Optimizing the basis of BK+ observables in the full kinematic range JHEP 05 (2013) 137 1303.5794
16 S. Descotes-Genon, L. Hofer, J. Matias, and J. Virto On the impact of power corrections in the prediction of BKμ+μ observables JHEP 12 (2014) 125 1407.8526
17 M. Alguer\'o et al. Are we overlooking lepton flavour universal new physics in bs? PRD 99 (2019) 075017 1809.08447
18 M. Alguer\'o et al. Emerging patterns of new physics with and without lepton flavour universal contributions EPJC 79 (2019) 714 1903.09578
19 CMS Collaboration Description and performance of track and primary-vertex reconstruction with the CMS tracker JINST 9 (2014) P10009 CMS-TRK-11-001
1405.6569
20 CMS Collaboration The CMS experiment at the CERN LHC JINST 3 (2008) S08004 CMS-00-001
21 CMS Collaboration The CMS trigger system JINST 12 (2017) P01020 CMS-TRG-12-001
1609.02366
22 CMS Collaboration Performance of CMS muon reconstruction in pp collision events at s= 7 TeV JINST 7 (2012) P10002 CMS-MUO-10-004
1206.4071
23 Particle Data Group, P. A. Zyla et al. Review of particle physics Prog. Theor. Exp. Phys. 2020 (2020) 083C01
24 T. Sjostrand, S. Mrenna, and P. Skands PYTHIA 6.4 physics and manual JHEP 05 (2006) 026 hep-ph/0603175
25 D. J. Lange The EvtGen particle decay simulation package NIMA 462 (2001) 152
26 GEANT4 Collaboration GEANT4 -- a simulation toolkit NIMA 506 (2003) 250
27 D. Bečirević and A. Tayduganov Impact of BK0+ on the new physics search in BK+ decay NPB 868 (2013) 368 1207.4004
28 J. Matias On the S-wave pollution of BK+ observables PRD 86 (2012) 094024 1209.1525
29 T. Blake, U. Egede, and A. Shires The effect of S-wave interference on the B0K0+ angular observables JHEP 03 (2013) 027 1210.5279
30 G. J. Feldman and R. D. Cousins Unified approach to the classical statistical analysis of small signals PRD 57 (1998) 3873 physics/9711021
Compact Muon Solenoid
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