<chapter name="Particle Data">
<h2>Particle Data</h2>
The structure and operation of the particle data table is described
<aloc href="ParticleDataScheme">here</aloc>. That page
also describes how default data properties can be changed. The
current page provides the actual default values.
<h3>Main settings</h3>
Apart from the data itself, the particle data table only contains
a few aspects that are available to change:
<modepick name="ParticleData:modeBreitWigner" default="4" min="0" max="4">
Selection of particle masses when the <code>mSel(id)</code> is called
to provide a new mass:
<option value="0">
mass is fixed at the nominal <ei>m_0</ei> value.
</option>
<option value="1">
particles registered as having a mass width are given a mass
in the range <ei>m_min < m < m_max</ei>, according
to a truncated nonrelativistic Breit-Wigner, i.e. linear in <ei>m</ei>.
</option>
<option value="2">
as above, except that the width is made mass-dependent:
<ei>Gamma = Gamma_0 * sqrt( (m^2 - m_thr^2) / (m_0^2 - m_thr^2) )</ei>
where <ei>m</ei> is the current mass, <ei>m_0</ei> the nominal one and
<ei>m_thr</ei> is the mass threshold, given by the sum of the nominal
masses of the decay products. In order to decouple production and decay
the threshold is defined as the branching-ratio-weighted average over
all allowed decay channels.
</option>
<option value="3">
particles registered as having a mass width are given a mass
in the range <ei>m_min < m < m_max</ei>, according
to a truncated relativistic Breit-Wigner, i.e. quadratic in <ei>m</ei>.
</option>
<option value="4">
as 3, but the width is modified as for 2, and the current mass is used
for its phase-space prefactor, i.e. <ei>m_0 Gamma_0 → m Gamma(m)</ei>.
</option>
<note>Note:</note> this mode only applies to normal hadronic
resonances like the <ei>rho</ei>. The more massive states of the
<code>isResonance()</code> type, like <ei>Z^0</ei> or top, are
considered separately.
</modepick>
<parm name="ParticleData:maxEnhanceBW" default="2.5" min="1." max="5.">
The modifications in options 2 and 4 above enhance the large-mass tail
of the Breit-Wigner distributions (the mass spectrum develops a dm/m divergence).
However, we expect form factors to dampen this tail at masses some distance
above the nominal one, so cut off the rise by requiring the actual
Breit-Wigner weight not to be more than a factor <code> maxEnhanceBW</code>
above the one obtained with options 1 or 3, respectively. This also
opens up for a simpler technical handling of mass selection in options
2 and 4, by using standard hit-and-miss Monte Carlo.
</parm>
<p/>
Since running masses are only calculated for the six quark flavours,
e.g. to obtain couplings to the Higgs boson(s), there is not an entry
in the normal tables for each particles, but only the six MSbar mass
values below, used as starting point for the running. In addition you
can pick an <ei>alpha_s(M_Z)</ei>, which is converted into a first-order
five-flavour Lambda that is used to determine the rate of the running.
(Without any match to four flavours below <ei>m_b</ei>; if desired, this
can be fixed by slightly shifted default mass values, since the routines
never should be called below the <ei>m_b</ei> scale anyway.)
<parm name="ParticleData:mdRun" default="0.006" min="0.003" max="0.008">
the d quark MSbar mass at 2 GeV scale.
</parm>
<parm name="ParticleData:muRun" default="0.003" min="0.001" max="0.006">
the u quark MSbar mass at 2 GeV scale.
</parm>
<parm name="ParticleData:msRun" default="0.095" min="0.060" max="0.150">
the s quark MSbar mass at 2 GeV scale.
</parm>
<parm name="ParticleData:mcRun" default="1.25" min="1.00" max="1.50">
the c quark MSbar mass at the mass scale itself.
</parm>
<parm name="ParticleData:mbRun" default="4.20" min="4.00" max="4.50">
the b quark MSbar mass at the mass scale itself.
</parm>
<parm name="ParticleData:mtRun" default="165.0" min="150.0" max="175.0">
the t quark MSbar mass at the mass scale itself.
</parm>
<parm name="ParticleData:alphaSvalueMRun" default="0.125" min="0.10" max="0.20">
the <ei>alpha_s(M_Z)</ei> value used to define the rate at which MSbar
masses run.
</parm>
<h3>Comments on the data</h3>
Much of the current data has been updated based on the 2012 Review of Particle
Physics <ref>Ber12</ref>, while some is still based on the 2006 RPP
<ref>Yao06</ref>. All known particle masses, widths and lifetimes
have been set accordingly, while most not-yet-measured particles are kept at
their values from PYTHIA 6. Decay channels and their branching
ratios remain a major worry: many particles do not have one single solidly
measured branching ratio, and many further do not have known branching
ratios that add up to (the neighbourhood of) unity.
<p/>
Uncertainties are especially big for the scalar, pseudovector and tensor
<ei>L = 1</ei> multiplets available in PYTHIA. We note that
some distributions become better described when these multiplets are
included in the generation, while others become worse. It is tempting to
associate this lackluster performance with the primitive knowledge.
Not even the multiplets themselves are particularly well known.
It used to be that the <ei>a_0(980)</ei> and <ei>f_0(980)</ei>
were considered to be members of the scalar multiplet. Nowadays they are
commonly assumed to be either four-quark states or of some other exotic
character. This means that the PYTHIA 8 PDG particle codes
have been changed for these particles, relative to what was used in
PYTHIA 6 based on previous PDG editions. Specifically their
numbers are now in the 9000000 series, and they have been replaced in the
scalar multiplet by <ei>a_0(1450)</ei> and <ei>f_0(1370)</ei>.
<p/>
For charm and bottom mesons the jungle of partial measurements makes
it very difficult to construct fully consistent sets of decay channels.
This part of the program has not yet been brought up to date to the
2006 RPP. Instead the LHCb decay tables (for EvtGen, but without
using the EvtGen matrix-element machinery) and the DELPHI tune for
PYTHIA 6 is being used. (This also includes a few non-c/b
hadrons that only occur in the c/b decay tables.) This has the
advantage that many tests have been made for consistency, but the
disadvantage that it is not always in agreement with the latest
measurements of some specific decay channels. The decays based
on the LHCb tables (with some modifications) are 411, 421, 431, 441,
445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122,
14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441,
100443, 100553, 9000111, 9000211. Correspondingly the decays based on
the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332,
5132, 5232 and 5332.
<h3>The data itself</h3>
Here comes the default particle data used in the program. Do not touch.
The meaning of the various properties and the format used are explained
<aloc href="ParticleDataScheme">here</aloc> and the
<code>meMode</code> codes <aloc href="ParticleDecays">here</aloc>.
<particle id="0" name="void" spinType="0" chargeType="0" colType="0"
m0="0.00000">
</particle>
<particle id="1" name="d" antiName="dbar" spinType="2" chargeType="-1" colType="1"
m0="0.33000">
</particle>
<particle id="2" name="u" antiName="ubar" spinType="2" chargeType="2" colType="1"
m0="0.33000">
</particle>
<particle id="3" name="s" antiName="sbar" spinType="2" chargeType="-1" colType="1"
m0="0.50000">
</particle>
<particle id="4" name="c" antiName="cbar" spinType="2" chargeType="2" colType="1"
m0="1.50000">
</particle>
<particle id="5" name="b" antiName="bbar" spinType="2" chargeType="-1" colType="1"
m0="4.80000">
</particle>
<particle id="6" name="t" antiName="tbar" spinType="2" chargeType="2" colType="1"
m0="171.00000" mWidth="1.40000" mMin="86.00000" mMax="0.00000">
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m0="5.110e-04">
</particle>
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m0="0.00000">
</particle>
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m0="0.10566" tau0="6.58654e+05">
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<particle id="14" name="nu_mu" antiName="nu_mubar" spinType="2" chargeType="0" colType="0"
m0="0.00000">
</particle>
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</chapter>
<!-- Copyright (C) 2014 Torbjorn Sjostrand -->
Marcin Chrzaszcz