1 <chapter name="Particle Data">
5 The structure and operation of the particle data table is described
6 <aloc href="ParticleDataScheme">here</aloc>. That page
7 also describes how default data properties can be changed. The
8 current page provides the actual default values.
10 <h3>Main settings</h3>
12 Apart from the data itself, the particle data table only contains
13 a few aspects that are available to change:
15 <modepick name="ParticleData:modeBreitWigner" default="4" min="0" max="4">
16 Selection of particle masses when the <code>mass(id)</code> is called
17 to provide a new mass:
19 mass is fixed at the nominal <ei>m_0</ei> value.
22 particles registered as having a mass width are given a mass
23 in the range <ei>m_min < m < m_max</ei>, according
24 to a truncated nonrelativistic Breit-Wigner, i.e. linear in <ei>m</ei>.
27 as above, except that the width is made mass-dependent:
28 <ei>Gamma = Gamma_0 * sqrt( (m^2 - m_thr^2) / (m_0^2 - m_thr^2) )</ei>
29 where <ei>m</ei> is the current mass, <ei>m_0</ei> the nominal one and
30 <ei>m_thr</ei> is the mass threshold, given by the sum of the nominal
31 masses of the decay products. In order to decouple production and decay
32 the threshold is defined as the branching-ratio-weighted average over
33 all allowed decay channels.
36 particles registered as having a mass width are given a mass
37 in the range <ei>m_min < m < m_max</ei>, according
38 to a truncated nonrelativistic Breit-Wigner, i.e. quadratic in <ei>m</ei>.
41 as 3, but the width is modified as for 2, and the current mass is used
42 for its phase-space prefactor, i.e. <ei>m_0 Gamma_0 -> m Gamma(m)</ei>.
44 <note>Note:</note> this mode only applies to normal hadronic
45 resonances like the <ei>rho</ei>. The more massive states of the
46 <code>isResonance()</code> type, like <ei>Z^0</ei> or top, are
47 considered separately.
50 <parm name="ParticleData:maxEnhanceBW" default="2.5" min="1." max="5.">
51 The modifications in options 2 and 4 above enhance the large-mass tail
52 of the Breit-Wigners (the mass spectrum develops a dm/m divergence).
53 However, we expect form factors to dampen this tail at masses some distance
54 above the nominal one, so cut off the rise by requiring the actual
55 Breit-Wigner weight not to be more than a factor <code> maxEnhanceBW</code>
56 above the one obtained with options 1 or 3, respectively. This also
57 opens up for a simpler technical handling of mass selection in options
58 2 and 4, by using standard hit-and-miss Monte Carlo.
62 Since running masses are only calculated for the six quark flavours,
63 e.g. to obtain couplings to the Higgs boson(s), there is not an entry
64 in the normal tables for each particles, but only the six MSbar mass
65 values below, used as starting point for the running. In addition you
66 can pick an <ei>alpha_s(M_Z)</ei>, which is converted into a first-order
67 five-flavour Lambda that is used to determine the rate of the running.
68 (Without any match to four flavours below <ei>m_b</ei>; if desired, this
69 can be fixed by slightly shifted default mass values, since the routines
70 never should be called below the <ei>m_b</ei> scale anyway.)
72 <parm name="ParticleData:mdRun" default="0.006" min="0.003" max="0.008">
73 the d quark MSbar mass at 2 GeV scale.
76 <parm name="ParticleData:muRun" default="0.003" min="0.001" max="0.006">
77 the u quark MSbar mass at 2 GeV scale.
80 <parm name="ParticleData:msRun" default="0.095" min="0.060" max="0.150">
82 the s quark MSbar mass at 2 GeV scale.
84 <parm name="ParticleData:mcRun" default="1.25" min="1.00" max="1.50">
86 the c quark MSbar mass at the mass scale itself.
88 <parm name="ParticleData:mbRun" default="4.20" min="4.00" max="4.50">
89 the b quark MSbar mass at the mass scale itself.
92 <parm name="ParticleData:mtRun" default="165.0" min="150.0" max="175.0">
93 the t quark MSbar mass at the mass scale itself.
96 <parm name="ParticleData:alphaSvalueMRun" default="0.125" min="0.10" max="0.20">
97 the <ei>alpha_s(M_Z)</ei> value used to define tha rate at which MSbar
102 <h3>Comments on the data</h3>
104 The starting point for the current data is the 2006 Review of Particle
105 Physics <ref>Yao06</ref>. All known particle masses, widths and lifetimes
106 have been set accordingly, while not-yet-measured particles are kept at
107 their values from PYTHIA 6. Decay channels and their branching
108 ratios remain a major worry: many particles do not have one single solidly
109 measured branching ratio, and many further do not have known branching
110 ratios that add up to (the neighbourhood of) unity.
113 Uncertainties are especially big for the scalar, pseudovector and tensor
114 <ei>L = 1</ei> multiplets available in PYTHIA. We note that
115 some distributions become better described when these multiplets are
116 included in the generation, while others become worse. It is tempting to
117 associate this lackluster performance with the primitive knowledge.
118 Not even the multiplets themselves are particularly well known.
119 It used to be that the <ei>a_0(980)</ei> and <ei>f_0(980)</ei>
120 were considered to be members of the scalar multiplet. Nowadays they are
121 commonly assumed to be either four-quark states or of some other exotic
122 character. This means that the PYTHIA 8 PDG particle codes
123 have been changed for these particles, relative to what was used in
124 PYTHIA 6 based on previous PDG editions. Specifically their
125 numbers are now in the 9000000 series, and they have been replaced in the
126 scalar multiplet by <ei>a_0(1450)</ei> and <ei>f_0(1370)</ei>.
129 For charm and bottom mesons the jungle of partial measurements makes
130 it very difficult to construct fully consistent sets of decay channels.
131 This part of the program has not yet been brought up to date to the
132 2006 RPP. Instead the LHCb decay tables (for EvtGen, but without
133 using the EvtGen matrix-element machinery) and the DELPHI tune for
134 PYTHIA 6 is being used. (This also includes a few non-c/b
135 hadrons that only occur in the c/b decay tables.) This has the
136 advantage that many tests have been made for consistency, but the
137 disadvantage that it is not always in agreement with the latest
138 measurements of some specific decay channels. The decays based
139 on the LHCb tables (with some modifications) are 411, 421, 431, 441,
140 445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122,
141 14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441,
142 100443, 100553, 9000111, 9000211. Correspondingly the decays based on
143 the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332,
146 <h3>The data itself</h3>
148 Here comes the default particle data used in the program. Do not touch.
149 The meaning of the various properties and the format used are explained
150 <aloc href="ParticleDataScheme">here</aloc> and the
151 <code>meMode</code> codes <aloc href="ParticleDecays">here</aloc>.
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160 <particle id="2" name="u" antiName="ubar" spinType="2" chargeType="2" colType="1"
164 <particle id="3" name="s" antiName="sbar" spinType="2" chargeType="-1" colType="1"
168 <particle id="4" name="c" antiName="cbar" spinType="2" chargeType="2" colType="1"
172 <particle id="5" name="b" antiName="bbar" spinType="2" chargeType="-1" colType="1"
176 <particle id="6" name="t" antiName="tbar" spinType="2" chargeType="2" colType="1"
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207 <particle id="13" name="mu-" antiName="mu+" spinType="2" chargeType="-3" colType="0"
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8009 <!-- Copyright (C) 2010 Torbjorn Sjostrand -->