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Search for the X(4140) state in B+J/ψϕK+ decays

R. Aaij et al. (LHCb Collaboration)
Phys. Rev. D 85, 091103(R) – Published 4 May 2012

Abstract

A search for the X(4140) state in B+J/ψϕK+ decays is performed with 0.37fb1 of pp collisions at s=7TeV collected by the LHCb experiment. No evidence for this state is found, in 2.4σ disagreement with a measurement by CDF. An upper limit on its production rate is set, B(B+X(4140)K+)×B(X(4140)J/ψϕ)/B(B+J/ψϕK+)<0.07 at 90% confidence level.

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  • Received 23 February 2012

DOI:https://doi.org/10.1103/PhysRevD.85.091103

This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

© 2012 CERN, for the LHCb Collaboration

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Vol. 85, Iss. 9 — 1 May 2012

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  • Figure 1
    Figure 1

    Mass distribution for B+J/ψϕK+ candidates in the data after the ±15MeV ϕ mass requirement. The fit of a Gaussian signal with a quadratic background (dashed line) is superimposed (solid red line).

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  • Figure 2
    Figure 2

    Invariant M(K+K) mass distribution selecting B+J/ψK+KK+ events in the ±2.5σ region around the B+ mass peak. The dashed line shows the two-body phase-space contribution. The small blue dotted ϕ peak on top of it illustrates the amount of the background ϕ mesons estimated from the fit to the B+ mass near-sidebands.

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  • Figure 3
    Figure 3

    Distribution of the mass difference M(J/ψϕ)M(J/ψ) for the B+J/ψϕK+ in the B+ (±2.5σ) and ϕ (±15MeV) mass windows. Fit of X(4140) signal on top of a smooth background is superimposed (solid red line). The dashed blue (dotted blue) line on top illustrates the expected X(4140) (X(4274)) signal yield from the CDF measurement [3]. The top and bottom plots differ by the background function (dashed black line) used in the fit: (a) an efficiency-corrected three-body phase-space (F1bkg); (b) a quadratic function multiplied by the efficiency-corrected three-body phase-space factor (F2bkg). The fit ranges are 1030–1400 and 1020–1400 MeV, respectively.

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  • Figure 4
    Figure 4

    Efficiency dependence on M(J/ψϕ)M(J/ψ) as determined from the simulation (points with error bars). The efficiency is normalized with respect to the efficiency of the ϕ signal fit to the B+J/ψϕK+ events distributed according to the phase-space model. A cubic polynomial was fitted to the simulated data (superimposed).

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