Rivet analyses
title: BESIII_2015_I1393996
$e^+e^-\to (DD^*)^0\pi^0$ for $\sqrt{s}=4.226$ and 4.257 GeV
Experiment: BESIII (BEPC)
Inspire ID: 1393996
Status: VALIDATED NOHEPDATA SINGLEWEIGHT
Authors: - Peter Richardson
References: - Phys.Rev.Lett. 115 (2015) 22, 222002
Beams: e+ e-
Beam energies: (2.1, 2.1); (2.1, 2.1)GeV
Run details: - e+ e- to hadrons, pi0 set stable
Measurement of mass distributions for $e^+e^-\to (DD^)^0\pi^0$ for $\sqrt{s}=4.226$ and 4.257 GeV by BES. The cross section for $e^+e^-\to Z_c(3885)^0\pi^0\to (DD^)^0\pi^0$ is also measured. As there is no PDG code for the $Z_c(3885)^0$ we take it to be the first unused exotic $c\bar{c}$ value 9030443, although this can be changed using the PID option.
Source code:BESIII_2015_I1393996.cc
```c++ // -- C++ --
include "Rivet/Analysis.hh"
include "Rivet/Projections/FinalState.hh"
include "Rivet/Projections/UnstableParticles.hh"
namespace Rivet {
/// @brief e+ e- > Z0 pi0 class BESIII_2015_I1393996 : public Analysis { public:
/// Constructor
RIVET_DEFAULT_ANALYSIS_CTOR(BESIII_2015_I1393996);
/// @name Analysis methods
/// @{
/// Book histograms and initialise projections before the run
void init() {
// set the PDG code
_pid = getOption<double>("PID", 9030443);
// projections
declare(FinalState(), "FS");
// histograms
if (isCompatibleWithSqrtS(4.226))
_sqs = "4.226";
else if (isCompatibleWithSqrtS(4.257))
_sqs = "4.257";
raiseBeamErrorIf(_sqs.empty());
for (size_t ix = 0; ix < 2; ++ix) {
book(_h["4.257"s + toString(ix)], 2, ix + 1, 1);
book(_h["4.226"s + toString(ix)], 2, ix + 1, 2);
}
book(_h["2"], 3, 1, 1);
book(_sigma, 1, 1, 1);
}
/// Perform the per-event analysis
void analyze(const Event& event) {
Particles fs = apply<FinalState>(event, "FS").particles();
Particles DD, other;
for (const Particle& p : fs) {
Particle parent = p;
while (!parent.parents().empty()) {
parent = parent.parents()[0];
if (parent.abspid() == 411 || parent.abspid() == 413 || parent.abspid() == 421
|| parent.abspid() == 423)
break;
}
if ((parent.abspid() == 411 || parent.abspid() == 421) && !parent.parents().empty()) {
Particle Dstar = parent.parents()[0];
if (Dstar.abspid() == 413 || Dstar.abspid() == 423) parent = Dstar;
}
if (parent.abspid() == 411 || parent.abspid() == 413 || parent.abspid() == 421
|| parent.abspid() == 423) {
bool found = false;
for (const auto& D : DD) {
// D already in list
if (fuzzyEquals(D.mom(), parent.mom())) {
found = true;
break;
}
}
if (!found) DD.push_back(parent);
}
else {
other.push_back(p);
}
}
// D Dbar + neutral pion
if (DD.size() != 2 || other.size() != 1) vetoEvent;
if (DD[0].pid() * DD[1].pid() > 0) vetoEvent;
if (other[0].pid() != 111) vetoEvent;
// D pi mass greater than 2.1
for (unsigned int ix = 0; ix < 2; ++ix) {
if (DD[ix].abspid() % 10 == 1 && (DD[ix].momentum() + other[0].momentum()).mass() < 2.1) vetoEvent;
}
double mass = (DD[0].momentum() + DD[1].momentum()).mass();
unsigned int iloc = 0;
// D+ D*+
if ((DD[0].abspid() == 413 && DD[1].abspid() == 411)
|| (DD[1].abspid() == 413 && DD[0].abspid() == 411)) {
iloc = 0;
}
// D0 D*0
else if ((DD[0].abspid() == 423 && DD[1].abspid() == 421)
|| (DD[1].abspid() == 423 && DD[0].abspid() == 421)) {
iloc = 1;
}
// otherwise veto event
else
vetoEvent;
_h[_sqs + toString(iloc)]->fill(mass);
_h["2"]->fill(mass);
// parent Z0
if (DD[0].parents()[0].pid() == _pid && DD[1].parents()[0].pid() == _pid
&& fuzzyEquals(DD[0].parents()[0].mom(), DD[1].parents()[0].mom()))
_sigma->fill(_sqs);
}
/// Normalise histograms etc., after the run
void finalize() {
// distributions
normalize(_h, 1.0, false);
// cross section
scale(_sigma, crossSection() / sumOfWeights() / picobarn);
}
/// @}
/// @name Histograms
/// @{
BinnedHistoPtr<string> _sigma;
map<string, Histo1DPtr> _h;
string _sqs = "";
int _pid;
/// @}
};
RIVET_DECLARE_PLUGIN(BESIII_2015_I1393996);
} ```