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CMS-PAS-BPH-15-009
Angular analysis of the decay ${\mathrm B^{+} \to \mathrm K^{*+} \mu^{+} \mu^{-}}$ in proton-proton collisions at $\sqrt{s}= $ 8 TeV
Abstract: Angular distributions of the decay ${\mathrm B^{+} \to \mathrm K^{*+} \mu^{+} \mu^{-}}$ are studied using events collected with the CMS detector from $\sqrt{s}= $ 8 TeV proton-proton collisions, corresponding to an integrated luminosity of 20.0 fb$^{-1}$. The forward-backward asymmetry of the muons and the longitudinal polarization of the $\mathrm K^{*+}$ meson are determined for an integrated sample and as a function of the dimuon invariant mass squared. These are the first results from this exclusive decay mode and are in agreement with standard model predictions.
Figures & Tables Summary References CMS Publications
Figures

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Figure 1:
The signal efficiency as a function $\cos\theta _{\mathrm{K}} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 1-a:
The signal efficiency as a function $\cos\theta _{\mathrm{K}} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 1-b:
The signal efficiency as a function $\cos\theta _{\mathrm{K}} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 1-c:
The signal efficiency as a function $\cos\theta _{\mathrm{K}} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 1-d:
The signal efficiency as a function $\cos\theta _{\mathrm{K}} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 2:
The signal efficiency as a function $\cos\theta _{\ell} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 2-a:
The signal efficiency as a function $\cos\theta _{\ell} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 2-b:
The signal efficiency as a function $\cos\theta _{\ell} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 2-c:
The signal efficiency as a function $\cos\theta _{\ell} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 2-d:
The signal efficiency as a function $\cos\theta _{\ell} $ for different ${q^2}$ ranges. The vertical bars indicate the statistical uncertainty. The curves show the fitted result, as described in the text.

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Figure 3:
The fitted $\mathrm{B^{+}}$ invariant mass, $\mathrm {m}$, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 3-a:
The fitted $\mathrm{B^{+}}$ invariant mass, $\mathrm {m}$, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 3-b:
The fitted $\mathrm{B^{+}}$ invariant mass, $\mathrm {m}$, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 3-c:
The fitted $\mathrm{B^{+}}$ invariant mass, $\mathrm {m}$, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 3-d:
The fitted $\mathrm{B^{+}}$ invariant mass, $\mathrm {m}$, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 4:
The fitted angular variable $\cos\theta _{\mathrm{K}}$, for each ${q^2}$ range from the three dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 4-a:
The fitted angular variable $\cos\theta _{\mathrm{K}}$, for each ${q^2}$ range from the three dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 4-b:
The fitted angular variable $\cos\theta _{\mathrm{K}}$, for each ${q^2}$ range from the three dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 4-c:
The fitted angular variable $\cos\theta _{\mathrm{K}}$, for each ${q^2}$ range from the three dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 4-d:
The fitted angular variable $\cos\theta _{\mathrm{K}}$, for each ${q^2}$ range from the three dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars represent the statistical uncertainty.

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Figure 5:
The fitted angular variable $\cos\theta _{\ell} $, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars on the points represent the statistical uncertainty.

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Figure 5-a:
The fitted angular variable $\cos\theta _{\ell} $, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars on the points represent the statistical uncertainty.

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Figure 5-b:
The fitted angular variable $\cos\theta _{\ell} $, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars on the points represent the statistical uncertainty.

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Figure 5-c:
The fitted angular variable $\cos\theta _{\ell} $, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars on the points represent the statistical uncertainty.

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Figure 5-d:
The fitted angular variable $\cos\theta _{\ell} $, for each ${q^2}$ range from the three-dimensional fit to the data. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively. The vertical bars on the points represent the statistical uncertainty.

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Figure 6:
The angular variable $\cos\theta _{\mathrm{K}}$ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 6-a:
The angular variable $\cos\theta _{\mathrm{K}}$ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 6-b:
The angular variable $\cos\theta _{\mathrm{K}}$ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 6-c:
The angular variable $\cos\theta _{\mathrm{K}}$ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 6-d:
The angular variable $\cos\theta _{\mathrm{K}}$ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 7:
The angular variable $\cos\theta _{\ell} $ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 7-a:
The angular variable $\cos\theta _{\ell} $ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 7-b:
The angular variable $\cos\theta _{\ell} $ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 7-c:
The angular variable $\cos\theta _{\ell} $ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 7-d:
The angular variable $\cos\theta _{\ell} $ for the events in the signal region 5.18 $ < m < $ 5.38 GeV, overlayed with the corresponding signal, background and total pdfs obtained from the final fit, for each ${q^2}$ range. The filled area, dashed lines, and solid lines represent the signal, background, and total contributions, respectively.

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Figure 8:
The measured values of ${A_\mathrm {FB}}$ and ${F_\mathrm {L}}$ versus ${q^2}$ for ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} \mu^{+} \mu^{-}}$ decays. The statistical (total) uncertainty is shown by inner (outer) vertical bars. The vertical shaded regions correspond to the ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} {\mathrm{J}/\psi} (\mu^{+} \mu^{-})}$ and ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} \psi(\text{2S})(\mu^{+} \mu^{-})}$ dominated regions. The blue band shows the SM predictions for the corresponding ${q^2}$ range.

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Figure 8-a:
The measured values of ${A_\mathrm {FB}}$ and ${F_\mathrm {L}}$ versus ${q^2}$ for ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} \mu^{+} \mu^{-}}$ decays. The statistical (total) uncertainty is shown by inner (outer) vertical bars. The vertical shaded regions correspond to the ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} {\mathrm{J}/\psi} (\mu^{+} \mu^{-})}$ and ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} \psi(\text{2S})(\mu^{+} \mu^{-})}$ dominated regions. The blue band shows the SM predictions for the corresponding ${q^2}$ range.

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Figure 8-b:
The measured values of ${A_\mathrm {FB}}$ and ${F_\mathrm {L}}$ versus ${q^2}$ for ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} \mu^{+} \mu^{-}}$ decays. The statistical (total) uncertainty is shown by inner (outer) vertical bars. The vertical shaded regions correspond to the ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} {\mathrm{J}/\psi} (\mu^{+} \mu^{-})}$ and ${\mathrm{B^{+}} \to {{\mathrm{K}} ^{*+}} \psi(\text{2S})(\mu^{+} \mu^{-})}$ dominated regions. The blue band shows the SM predictions for the corresponding ${q^2}$ range.
Tables

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Table 1:
Sources of systematic uncertainties and the effect on ${A_\mathrm {FB}}$ and ${F_\mathrm {L}}$. The values given are absolute and the ranges indicate the variation over the four ${q^2}$ bins.

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Table 2:
The signal yield with statistical uncertainty and the fitted ${A_\mathrm {FB}}$ and ${F_\mathrm {L}}$ values with statistical and systematic uncertainties, for each ${q^2}$ range.
Summary
The first angular analysis of the decay ${\mathrm{B^{+}}\to {\mathrm K^{*+}} \mu^{+} \mu^{-}}$ 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 and correspond to an integrated luminosity of 20.0 fb$^{-1}$ . For each bin of dimuon invariant mass squared (${q^2} $), a three-dimensional unbinned maximum-likelihood fit was performed to the distributions of the ${\mathrm K^{*+}} \mu^{+}\mu^{-}$ invariant mass and two decay angles. The forward-backward asymmetry, ${A_\mathrm{FB}} $, of the muon system and the longitudinal polarization of ${\mathrm K^{*+}} , {F_\mathrm{L}} $, are extracted from the fit and compared with predictions from a standard model prediction. The results are consistent with standard model expectations.
References
1 C. Bobeth, G. Hiller, and D. van Dyk The benefits of $ \overline{B} \to \overline{K}^* \ell^+ \ell^- $ decays at low recoil JHEP 07 (2010) 098 1006.5013
2 C. Bobeth, G. Hiller, D. van Dyk, and C. Wacker The decay $ \overline{B} \to \overline{K} \ell^+ \ell^- $ at low hadronic recoil and model-independent $ \delta b = $ 1 constraints JHEP 01 (2012) 107 1111.2558
3 C. Bobeth, G. Hiller, and D. van Dyk General analysis of $ \overline{B} \to \overline{K}{}^{(*)} \ell^+ \ell^- $ decays at low recoil PRD 87 (2012) 034016 1212.2321
4 A. Ali, G. Kramer, and G. Zhu $ B\to K^*\ell^+\ell^- $ decay in soft-collinear effective theory EPJC 47 (2006) 625 hep-ph/0601034
5 W. Altmannshofer et al. Symmetries and asymmetries of $ B \to K^{*} \mu^{+} \mu^{-} $ decays in the Standard Model and beyond JHEP 01 (2009) 019 0811.1214
6 W. Altmannshofer, P. Paradisi, and D. M. Straub Model-independent constraints on new physics in $ b \to s $ transitions JHEP 04 (2012) 008 1111.1257
7 S. Jager and J. Martin Camalich On $ B \to V \ell \ell $ at small dilepton invariant mass, power corrections, and new physics JHEP 05 (2013) 043 1212.2263
8 S. Descotes-Genon, T. Hurth, J. Matias, and J. Virto Optimizing the basis of $ B \to {K}^{*}\ell^+ \ell^- $ observables in the full kinematic range JHEP 05 (2013) 137 1303.5794
9 S. Descotes-Genon, L. Hofer, J. Matias, and J. Virto On the impact of power corrections in the prediction of $ B \to K^*\mu^+\mu^- $ observables JHEP 12 (2014) 125 1407.8526
10 M. Algueró et al. Are we overlooking lepton flavour universal new physics in $ b\to s\ell\ell $? PRD 99 (2019) 075017 1809.08447
11 M. Algueró et al. Emerging patterns of New Physics with and without Lepton Flavour Universal contributions EPJC 79 (2019) 714 1903.09578
12 CMS Collaboration CMS luminosity based on pixel cluster counting - summer 2013 update CMS-PAS-LUM-13-001 CMS-PAS-LUM-13-001
13 CDF Collaboration Measurements of the angular distributions in the decays $ B \to K^{(*)} \mu^+ \mu^- $ at CDF PRL 108 (2012) 081807 1108.0695
14 LHCb Collaboration Differential branching fraction and angular analysis of the decay $ B^{0} \to K^{*0} \mu^{+}\mu^{-} $ JHEP 08 (2013) 131 1304.6325
15 CMS Collaboration Angular analysis and branching fraction measurement of the decay $ B^0 \to K^{*0} \mu^+\mu^- $ PLB 727 (2013) 77 CMS-BPH-11-009
1308.3409
16 CMS Collaboration Angular analysis of the decay $ B^0 \to K^{*0} \mu^+ \mu^- $ from pp collisions at $ \sqrt{s} = $ 8 TeV PLB 753 (2016) 424 CMS-BPH-13-010
1507.08126
17 BaBar Collaboration Angular distributions in the decay $ B \to K^* \ell^+ \ell^- $ PRD 79 (2009) 031102 0804.4412
18 Belle Collaboration Measurement of the differential branching fraction and forward-backward asymmetry for $ B \to K^{(*)} \ell^+ \ell^- $ PRL 103 (2009) 171801 0904.0770
19 CMS Collaboration The CMS experiment at the CERN LHC JINST 3 (2008) S08004 CMS-00-001
20 CMS Collaboration The CMS trigger system JINST 12 (2017) P01020 CMS-TRG-12-001
1609.02366
21 T. Sjostrand, S. Mrenna, and P. Skands PYTHIA 6.4 physics and manual JHEP 05 (2006) 026 hep-ph/0603175
22 D. J. Lange The EvtGen particle decay simulation package NIMA 462 (2001) 152
23 GEANT4 Collaboration GEANT4---a simulation toolkit NIMA 506 (2003) 250
24 D. Be\vcirevi\'c and A. Tayduganov Impact of $ B\to K^{*0} \ell^+\ell^- $ on the New Physics search in $ B\to K^* \ell^+\ell^- $ decay NPB 868 (2013) 368 1207.4004
25 J. Matias On the S-wave pollution of $ B \to K^* \ell^+\ell^- $ observables PRD 86 (2012) 094024 1209.1525
26 T. Blake, U. Egede, and A. Shires The effect of $ S $-wave interference on the $ B^0 \rightarrow K^{*0} \ell^+ \ell^- $ angular observables JHEP 03 (2013) 027 1210.5279
27 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
LHC, CERN