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Charm Dalitz Plot Analysis Formalism and Results
a
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– 1–
CHARM DALITZ PLOT ANALYSIS FORMALISM
AND RESULTS (EXPANDED RPP-2004 VERSION)
Written November 2003 by D. Asner (University of Pittsburgh)
Introduction: Charm meson decay dynamics have been stud-
ied extensively over the last decade. Recent studies of multi-
body decays of charm mesons probe a variety of physics includ-
ing doubly-Cabibbo suppressed decays [1], searches for CP vi-
olation [1,2,3], the properties of established light mesons [4,5,6]
and the properties of ππ [1,6,7] and Kπ [8] S-wave states.
Future studies could improve sensitivity to D0–D0 mixing [9].
Weak nonleptonic decays of charm mesons are expected
to proceed dominantly through resonant two-body decays in
several theoretical models [10]; see Ref. [11] for a review of res-
onance phenomenology. These amplitudes are calculated with
the Dalitz plot analysis technique [12], which uses the mininum
number of independent observable quantities. For three-body
final states when the parent particle is a scalar, the decay
rate [13] is
Γ =
1
(2π)3 32
√
s3
|M|2 dm212dm223, (1)
where mij is the invariant mass of i ? j and the coefficient of
the amplitude includes all kinematic factors. The scatter plot
in m212 versus m
2
23 is called a Dalitz plot. If |M|2 is constant
the allowed region of the plot will be populated uniformly with
events. Any variation in |M|2 over the Dalitz plot is due to
dynamical rather than kinematical effects.
Formalism: The amplitude of the process, D → rc, r → ab, is
given by
Mr (L,mab, mbc) =
∑
λ
〈ab|rλ〉Tr (mab) 〈crλ|D〉 (2)
= Z (L, ~p, ~q)BDL (|~p|)BrL (|~q|)Tr (mab) ,
where the sum is over the helicity states λ of the intermediate
resonance particle r, a and b are the daughter particles of
the resonance r, c is the spectator particle, L is the orbital
angular momentum between r and c, ~p is the momentum of
CITATION: S. Eidelman et al., Phys. Lett. B 592, 1 (2004) (URL: /)
February 7, 2008 07:43
– 2–
c in the r res
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