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Amplitude analysis of the B+π+π+π decay

R. Aaij et al. (LHCb Collaboration)
Phys. Rev. D 101, 012006 – Published 21 January 2020
Physics logo See Viewpoint: CP Violations Newly Observed in Beauty Meson Decays
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Abstract

The results of an amplitude analysis of the charmless three-body decay B+π+π+π, in which CP-violation effects are taken into account, are reported. The analysis is based on a data sample corresponding to an integrated luminosity of 3fb1 of pp collisions recorded with the LHCb detector. The most challenging aspect of the analysis is the description of the behavior of the π+πS-wave contribution, which is achieved by using three complementary approaches based on the isobar model, the K-matrix formalism, and a quasi-model-independent procedure. Additional resonant contributions for all three methods are described using a common isobar model, and include the ρ(770)0, ω(782) and ρ(1450)0 resonances in the π+π P-wave, the f2(1270) resonance in the π+π D-wave, and the ρ3(1690)0 resonance in the π+π F-wave. Significant CP-violation effects are observed in both S- and D-waves, as well as in the interference between the S- and P-waves. The results from all three approaches agree and provide new insight into the dynamics and the origin of CP-violation effects in B+π+π+π decays.

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  • Received 16 September 2019

DOI:https://doi.org/10.1103/PhysRevD.101.012006

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

© 2020 CERN, for the LHCb Collaboration

Physics Subject Headings (PhySH)

  1. Research Areas
  1. Physical Systems
  1. Properties
Particles & Fields

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CP Violations Newly Observed in Beauty Meson Decays

Published 21 January 2020

Measurements show large matter-versus-antimatter differences in three-pion decays of B mesons, yielding new insights into the strong interaction dynamics that control these decays.

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Observation of Several Sources of CP Violation in B+π+π+π Decays

R. Aaij et al. (LHCb Collaboration)
Phys. Rev. Lett. 124, 031801 (2020)

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Vol. 101, Iss. 1 — 1 January 2020

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  • Figure 1
    Figure 1

    Invariant-mass fit model for (a) B and (b) B+ candidates reconstructed in the π π+ π final state for the combined 2011 and 2012 data taking samples. Points with error bars represent the data while the components comprising the model are listed in the plot legend.

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  • Figure 2
    Figure 2

    Conventional Dalitz-plot distributions for (a) B+ and (b) B, and square Dalitz-plot (defined in Sec. 5a1) distributions for (c) B+ and (d) B candidate decays to π±π+π. Depleted regions are due to the D¯0 veto.

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  • Figure 3
    Figure 3

    Square Dalitz-plot distributions for the (left) B+ and (right) B signal efficiency models, smoothed using a two-dimensional cubic spline. Depleted regions are due to the D¯0 veto.

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  • Figure 4
    Figure 4

    Square Dalitz-plot distributions for the (left) B+ and (right) B combinatorial background models, scaled to represent their respective yields in the signal region.

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  • Figure 5
    Figure 5

    Square Dalitz-plot distribution for the misidentified B+K+π+π background model, scaled to represent its yield in the signal region.

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  • Figure 6
    Figure 6

    Fit projections of each model (a) in the low-mlow region and (b) in the full range of mhigh, with the corresponding asymmetries shown beneath in panels (c) and (d). The normalized residual or pull distribution, defined as the difference between the bin value less the fit value over the uncertainty on the number of events in that bin, is shown below each fit projection.

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  • Figure 7
    Figure 7

    Fit projections of each model on mlow (a) in the region below the ρ(770)0 resonance and (b) in the ρ(770)0 region, with the corresponding asymmetries shown beneath in panels (c) and (d). The pull distribution is shown below each fit projection.

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  • Figure 8
    Figure 8

    Fit projections of each model on mlow (a) in the region around the f2(1270) resonance and (b) in the high-mhigh region, with the corresponding asymmetries shown beneath in panels (c) and (d). The pull distribution is shown below each fit projection.

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  • Figure 9
    Figure 9

    Fit projections of each model on cosθhel (a) in the region around the ρ(770)0 resonance and (b) in the f2(1270) region, with the corresponding asymmetries shown beneath in panels (c) and (d). The pull distribution is shown below each fit projection.

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  • Figure 10
    Figure 10

    Fit projections of each model on cosθhel in the regions (a) below and (b) above the ρ(770)0 resonance pole, with the corresponding asymmetries shown beneath in panels (c) and (d). The pull distribution is shown below each fit projection.

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  • Figure 11
    Figure 11

    Fit projections of each model (a) on cosθhel in the ρ3(1690) region, with (b) the corresponding asymmetry shown beneath. The pull distribution is shown below each fit projection.

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  • Figure 12
    Figure 12

    Raw difference in the number of B and B+ candidates in the low-mlow region, for (a) positive, and (b) negative cosine of the helicity angle. The pull distribution is shown below each fit projection.

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  • Figure 13
    Figure 13

    The (top) isobar, (middle) K-matrix and (bottom) QMI S-wave results where panels (a), (c) and (e) show the magnitude squared while panels (b), (d) and (f) show the phase motion. Discontinuities in the phase motion are due to presentation in the range [180°,180°]. Red curves indicate B+ while blue curves represent B decays, with the statistical and total uncertainties bounded by the dark and light bands, respectively (incorporating only the dominant systematic uncertainties). Note that the overall scale of the squared magnitude contains no physical meaning, but is simply a manifestation of the different scale factors and conventions adopted by each of the three amplitude analysis approaches.

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  • Figure 14
    Figure 14

    Comparison of results for the CP-averaged S-wave obtained in the three different approaches, where panel (a) shows the magnitude squared while panel (b) shows the phase motion. Discontinuities in the phase motion are due to presentation in the range [180°,180°]. The blue curve indicates the isobar S-wave, the amber curve indicates the K-matrix S-wave, and the green points with error bars represent the QMI S-wave. The band or error bars in each case represent the total uncertainty, incorporating the dominant systematic uncertainties. As the integral of the |A|2 plot in each approach is proportional to its respective S-wave fit fraction, the overall scale of the K-matrix and QMI plots are set relative to the isobar S-wave fit fraction in order to facilitate comparison between the three approaches.

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  • Figure 15
    Figure 15

    Data and fit model projections in the f2(1270) region with (a) freely varied f2(1270) resonance parameters, and (b) with an additional spin-2 component with mass and width parameters determined by the fit.

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  • Figure 16
    Figure 16

    Central values (points) and statistical 68% Gaussian confidence regions (ellipses) for the complex coefficients associated with the f2(1270) resonance under various systematic assumptions for the B+ (solid) and B (dashed) decay amplitude models. The nominal result and statistical uncertainty is given in black, while the results of the dominant systematic variations to the nominal model (per Sec. 6) are given by the colored ellipses, as noted in the legend, for each of the (a) isobar, (b) K-matrix and (c) QMI S-wave approaches. The model-specific systematic uncertainties are discussed in Sec. 6.

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  • Figure 17
    Figure 17

    Signed χ2 distributions indicating the agreement between the isobar model fit and the data for (a) B+ and (b) B decays.

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  • Figure 18
    Figure 18

    Signed χ2 distributions indicating the agreement between the K-matrix model fit and the data for (a) B+ and (b) B decays.

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  • Figure 19
    Figure 19

    The K-matrix S-wave projections for the secondary solution, where panel (a) shows the magnitude squared while panel (b) shows the phase motion. The red curve indicates B+, while the blue curve represents B decays. The light bands represent the 68% confidence interval around the central values, including statistical uncertainties only.

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  • Figure 20
    Figure 20

    Signed χ2 distributions indicating the agreement between the QMI model fit and the data for (a) B+ and (b) B decays.

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  • Figure 21
    Figure 21

    Fit projections on mlow of the result with the isobar S-wave model (a) in the low-mlow region, (b) below the ρ(770)0 region, (c) in the ρ(770)0 region, and (d) in the f2(1270) region. The thick blue curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend in Fig. 23.

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  • Figure 22
    Figure 22

    Fit projections on mhigh of the result with the isobar S-wave model (a) in the full mhigh range, (b) in the high-mhigh region, and on cosθhel (c) in the ρ(770)0 region and (d) in the f2(1270) region. The thick blue curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend in Fig. 23.

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  • Figure 23
    Figure 23

    Fit projections on cosθhel of the result with the isobar S-wave model in the region (a) below and (b) above the ρ(770)0 mass, and (c) in the ρ3(1690)0 region. The thick blue curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend.

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  • Figure 24
    Figure 24

    Fit projections on mlow of the result with the K-matrix S-wave model (a) in the low-mlow region, (b) below the ρ(770)0 region, (c) in the ρ(770)0 region, and (d) in the f2(1270) region. The thick amber curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend in Fig. 26.

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  • Figure 25
    Figure 25

    Fit projections on mhigh of the result with the K-matrix S-wave model (a) in the full mhigh range, (b) in the high-mhigh region, and on cosθhel (c) in the ρ(770)0 region), and (d) in the f2(1270) region. The thick amber curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend in Fig. 26.

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  • Figure 26
    Figure 26

    Fit projections on cosθhel of the result with the K-matrix S-wave model in the region (a) below and (b) above the ρ(770)0 mass, and (c) in the ρ3(1690)0 region. The thick amber curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend.

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  • Figure 27
    Figure 27

    Fit projections on mlow of the result with the QMI S-wave model (a) in the low-mlow region, (b) below the ρ(770)0 region, (c) in the ρ(770)0 region, and (d) in the f2(1270) region. The thick dark-green curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend in Fig. 29.

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  • Figure 28
    Figure 28

    Fit projections on mhigh of the result with the QMI S-wave model (a) in the full mhigh range, (b) in the high-mhigh region, and on cosθhel in (c) the ρ(770)0 region, and (d) in the f2(1270) region. The thick dark-green curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend in Fig. 29.

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  • Figure 29
    Figure 29

    Fit projections on cosθhel of the result with the isobar S-wave model in the region (a) below and (b) above the ρ(770)0 mass, and (c) in the ρ3(1690)0 region. The thick blue curve represents the total model, and the colored curves represent the contributions of individual model components (not including interference effects), as per the legend.

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