Abstract

The Dalitz plot analysis technique is used to study the resonant substructures of $B^{-} \to D^{+} \pi^{-} \pi^{-}$ decays in a data sample corresponding to 3.0 ${\rm fb}^{-1}$ of $pp$ collision data recorded by the LHCb experiment during 2011 and 2012. A model-independent analysis of the angular moments demonstrates the presence of resonances with spins 1, 2 and 3 at high $D^{+}\pi^{-}$ mass. The data are fitted with an amplitude model composed of a quasi-model-independent function to describe the $D^{+}\pi^{-}$ S-wave together with virtual contributions from the $D^{*}(2007)^{0}$ and $B^{*0}$ states, and components corresponding to the $D^{*}_{2}(2460)^{0}$, $D^{*}_{1}(2680)^{0}$, $D^{*}_{3}(2760)^{0}$ and $D^{*}_{2}(3000)^{0}$ resonances. The masses and widths of these resonances are determined together with the branching fractions for their production in $B^{-} \to D^{+} \pi^{-} \pi^{-}$ decays. The $D^{+}\pi^{-}$ S-wave has phase motion consistent with that expected due to the presence of the $D^{*}_{0}(2400)^{0}$ state. These results constitute the first observations of the $D^{*}_{3}(2760)^{0}$ and $D^{*}_{2}(3000)^{0}$ resonances.

Highlights

  • There is strong theoretical and experimental interest in charm meson spectroscopy because it provides opportunities to study QCD predictions within the context of different models [1,2,3,4,5]

  • Quantum numbers are only known for states studied in amplitude analyses of multibody B meson decays, since analyses of promptly produced excited charm states only determine whether the spin-parity is natural (i.e. JP 1⁄4 0þ; 1−; 2þ; ...) or unnatural (i.e. JP 1⁄4 0−; 1þ; 2−; ...), not the resonance spin

  • One challenge for Dalitz plot (DP) analyses with large data samples is the modeling of broad resonances that interfere with nonresonant amplitudes in the same partial wave

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Summary

INTRODUCTION

There is strong theoretical and experimental interest in charm meson spectroscopy because it provides opportunities to study QCD predictions within the context of different models [1,2,3,4,5]. Progress has been strong for excited charm-strange (cs) mesons [14,15,16,17,18] These studies have in addition revealed several new states at higher masses, most of which have not yet been confirmed by analyses of independent data samples. One challenge for DP analyses with large data samples is the modeling of broad resonances that interfere with nonresonant amplitudes in the same partial wave. Inclusion of both contributions in an amplitude fit can violate unitarity in the decay matrix element, and gives results that are difficult to interpret due to large interference effects.

LHCb DETECTOR
SELECTION REQUIREMENTS
DETERMINATION OF SIGNAL AND BACKGROUND YIELDS
STUDY OF ANGULAR MOMENTS
DALITZ PLOT ANALYSIS FORMALISM
Signal efficiency
Background studies
Dalitz plot fit results
VIII. SYSTEMATIC UNCERTAINTIES
Background
RESULTS AND SUMMARY
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