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  • Open Access

Measurement of the branching ratio of π0 Dalitz decay using KLπ0π0π0 decays

E. Abouzaid et al.
Phys. Rev. D 100, 032003 – Published 5 August 2019

Abstract

We present a measurement of B(π0e+eγ)/B(π0γγ), the Dalitz branching ratio, using data taken in 1999 by the E832 KTeV experiment at Fermi National Accelerator Laboratory. We use neutral pions from fully reconstructed KL decays in flight; the measurement is based on 60 thousand KLπ0π0π0γγγγe+eγ decays. We normalize to KLπ0π0π06γ decays. We find B(π0e+eγ)/B(π0γγ) (me+e>15MeV/c2)=[3.920±0.016(stat)±0.036(syst)]×103. Using the Mikaelian and Smith prediction for the e+e mass spectrum, we correct the result to the full e+e mass range. The corrected result is B(π0e+eγ)/B(π0γγ)=[1.1559±0.0047(stat)±0.0106(syst)]%. This result is consistent with previous measurements, and the uncertainty is a factor of 3 smaller than any previous measurement.

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  • Received 6 February 2019

DOI:https://doi.org/10.1103/PhysRevD.100.032003

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.

Published by the American Physical Society

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Vol. 100, Iss. 3 — 1 August 2019

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Images

  • Figure 1
    Figure 1

    Schematic of the KTeV detector. Note that the vertical and horizontal scales are different.

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  • Figure 2
    Figure 2

    Distribution of difference from the average value for ratio of number of events before to number of events after hardware prescale is applied, in units of statistical standard deviations.

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  • Figure 3
    Figure 3

    Reconstructed e+eγ mass for data (dots) and Monte Carlo (histogram). (a) Data and nominal MC. (b) Data and MC with no radiative corrections. (c) Data/MC ratio for nominal MC. (d) Data/MC ratio for MC with no radiative corrections. All nominal selection criteria have been applied except for the e+eγ mass requirement.

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  • Figure 4
    Figure 4

    Reconstructed e+e mass for data (dots) and Monte Carlo (histogram). (a) Data and nominal MC. (b) Data and MC with no virtual radiative corrections. (c) Data/MC ratio for nominal MC. (d) Data/MC ratio for MC with no virtual radiative corrections. All nominal selection criteria have been applied except for the e+e mass requirement and the cell separation requirement. These plots include events with minimum cell separation values of one or greater.

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  • Figure 5
    Figure 5

    Deviation of sum-of-distance (SOD) from nominal value of 6.35 mm for data (dots) and Monte Carlo (histogram). Note the different vertical scales for the two plots. (a) Data and nominal MC. (b) Data and MC with no simulation of accidental activity.

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  • Figure 6
    Figure 6

    The B(π0e+eγ)/B(π0γγ) measurement versus cell separation. The Dalitz events that contribute to the result in each of the first six bins have a minimum cell separation equal to the bin number. The last bin includes events with minimum cell separation greater than or equal to six. The error bars represent the independent statistical uncertainty in each bin. The solid line is the weighted average, and the dashed horizontal lines indicate the statistical uncertainty on the weighted average.

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  • Figure 7
    Figure 7

    Comparison of the B(π0e+eγ)/B(π0γγ) branching ratio result to previous theoretical [2, 3, 4, 5, 6, 7, 8] and experimental [9, 18, 19, 20, 21] results. A new world average for experimental results is also shown. The hatched region shows the area within one sigma of the new world average.

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