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<title>Particle Data</title>
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<link rel="stylesheet" type="text/css" href="pythia.css"/>
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<link rel="shortcut icon" href="pythia32.gif"/>
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The structure and operation of the particle data table is described
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<a href="ParticleDataScheme.html" target="page">here</a>. That page
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also describes how default data properties can be changed. The
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current page provides the actual default values.
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<h3>Main settings</h3>
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Apart from the data itself, the particle data table only contains
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a few aspects that are available to change:
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<p/><code>mode </code><strong> ParticleData:modeBreitWigner </strong>
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(<code>default = <strong>4</strong></code>; <code>minimum = 0</code>; <code>maximum = 4</code>)<br/>
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Selection of particle masses when the <code>mass(id)</code> is called
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to provide a new mass:
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<br/><code>option </code><strong> 0</strong> :
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mass is fixed at the nominal <i>m_0</i> value.
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<br/><code>option </code><strong> 1</strong> :
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particles registered as having a mass width are given a mass
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in the range <i>m_min < m < m_max</i>, according
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to a truncated nonrelativistic Breit-Wigner, i.e. linear in <i>m</i>.
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<br/><code>option </code><strong> 2</strong> :
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as above, except that the width is made mass-dependent:
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<i>Gamma = Gamma_0 * sqrt( (m^2 - m_thr^2) / (m_0^2 - m_thr^2) )</i>
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where <i>m</i> is the current mass, <i>m_0</i> the nominal one and
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<i>m_thr</i> is the mass threshold, given by the sum of the nominal
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masses of the decay products. In order to decouple production and decay
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the threshold is defined as the branching-ratio-weighted average over
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all allowed decay channels.
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<br/><code>option </code><strong> 3</strong> :
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particles registered as having a mass width are given a mass
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in the range <i>m_min < m < m_max</i>, according
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to a truncated relativistic Breit-Wigner, i.e. quadratic in <i>m</i>.
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<br/><code>option </code><strong> 4</strong> :
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as 3, but the width is modified as for 2, and the current mass is used
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for its phase-space prefactor, i.e. <i>m_0 Gamma_0 -> m Gamma(m)</i>.
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<br/><b>Note:</b> this mode only applies to normal hadronic
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resonances like the <i>rho</i>. The more massive states of the
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<code>isResonance()</code> type, like <i>Z^0</i> or top, are
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considered separately.
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<p/><code>parm </code><strong> ParticleData:maxEnhanceBW </strong>
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(<code>default = <strong>2.5</strong></code>; <code>minimum = 1.</code>; <code>maximum = 5.</code>)<br/>
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The modifications in options 2 and 4 above enhance the large-mass tail
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of the Breit-Wigners (the mass spectrum develops a dm/m divergence).
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However, we expect form factors to dampen this tail at masses some distance
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above the nominal one, so cut off the rise by requiring the actual
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Breit-Wigner weight not to be more than a factor <code> maxEnhanceBW</code>
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above the one obtained with options 1 or 3, respectively. This also
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opens up for a simpler technical handling of mass selection in options
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2 and 4, by using standard hit-and-miss Monte Carlo.
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Since running masses are only calculated for the six quark flavours,
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e.g. to obtain couplings to the Higgs boson(s), there is not an entry
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in the normal tables for each particles, but only the six MSbar mass
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values below, used as starting point for the running. In addition you
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can pick an <i>alpha_s(M_Z)</i>, which is converted into a first-order
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five-flavour Lambda that is used to determine the rate of the running.
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(Without any match to four flavours below <i>m_b</i>; if desired, this
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can be fixed by slightly shifted default mass values, since the routines
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never should be called below the <i>m_b</i> scale anyway.)
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<p/><code>parm </code><strong> ParticleData:mdRun </strong>
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(<code>default = <strong>0.006</strong></code>; <code>minimum = 0.003</code>; <code>maximum = 0.008</code>)<br/>
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the d quark MSbar mass at 2 GeV scale.
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<p/><code>parm </code><strong> ParticleData:muRun </strong>
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(<code>default = <strong>0.003</strong></code>; <code>minimum = 0.001</code>; <code>maximum = 0.006</code>)<br/>
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the u quark MSbar mass at 2 GeV scale.
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<p/><code>parm </code><strong> ParticleData:msRun </strong>
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(<code>default = <strong>0.095</strong></code>; <code>minimum = 0.060</code>; <code>maximum = 0.150</code>)<br/>
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the s quark MSbar mass at 2 GeV scale.
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<p/><code>parm </code><strong> ParticleData:mcRun </strong>
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(<code>default = <strong>1.25</strong></code>; <code>minimum = 1.00</code>; <code>maximum = 1.50</code>)<br/>
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the c quark MSbar mass at the mass scale itself.
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<p/><code>parm </code><strong> ParticleData:mbRun </strong>
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(<code>default = <strong>4.20</strong></code>; <code>minimum = 4.00</code>; <code>maximum = 4.50</code>)<br/>
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the b quark MSbar mass at the mass scale itself.
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<p/><code>parm </code><strong> ParticleData:mtRun </strong>
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(<code>default = <strong>165.0</strong></code>; <code>minimum = 150.0</code>; <code>maximum = 175.0</code>)<br/>
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the t quark MSbar mass at the mass scale itself.
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<p/><code>parm </code><strong> ParticleData:alphaSvalueMRun </strong>
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(<code>default = <strong>0.125</strong></code>; <code>minimum = 0.10</code>; <code>maximum = 0.20</code>)<br/>
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the <i>alpha_s(M_Z)</i> value used to define tha rate at which MSbar
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<h3>Comments on the data</h3>
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The starting point for the current data is the 2006 Review of Particle
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Physics [<a href="Bibliography.html" target="page">Yao06</a>]. All known particle masses, widths and lifetimes
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have been set accordingly, while not-yet-measured particles are kept at
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their values from PYTHIA 6. Decay channels and their branching
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ratios remain a major worry: many particles do not have one single solidly
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measured branching ratio, and many further do not have known branching
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ratios that add up to (the neighbourhood of) unity.
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Uncertainties are especially big for the scalar, pseudovector and tensor
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<i>L = 1</i> multiplets available in PYTHIA. We note that
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some distributions become better described when these multiplets are
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included in the generation, while others become worse. It is tempting to
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associate this lackluster performance with the primitive knowledge.
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Not even the multiplets themselves are particularly well known.
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It used to be that the <i>a_0(980)</i> and <i>f_0(980)</i>
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were considered to be members of the scalar multiplet. Nowadays they are
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commonly assumed to be either four-quark states or of some other exotic
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character. This means that the PYTHIA 8 PDG particle codes
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have been changed for these particles, relative to what was used in
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PYTHIA 6 based on previous PDG editions. Specifically their
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numbers are now in the 9000000 series, and they have been replaced in the
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scalar multiplet by <i>a_0(1450)</i> and <i>f_0(1370)</i>.
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For charm and bottom mesons the jungle of partial measurements makes
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it very difficult to construct fully consistent sets of decay channels.
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This part of the program has not yet been brought up to date to the
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2006 RPP. Instead the LHCb decay tables (for EvtGen, but without
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using the EvtGen matrix-element machinery) and the DELPHI tune for
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PYTHIA 6 is being used. (This also includes a few non-c/b
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hadrons that only occur in the c/b decay tables.) This has the
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advantage that many tests have been made for consistency, but the
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disadvantage that it is not always in agreement with the latest
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measurements of some specific decay channels. The decays based
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on the LHCb tables (with some modifications) are 411, 421, 431, 441,
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445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122,
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14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441,
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100443, 100553, 9000111, 9000211. Correspondingly the decays based on
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the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332,
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<h3>The data itself</h3>
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Here comes the default particle data used in the program. Do not touch.
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The meaning of the various properties and the format used are explained
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<a href="ParticleDataScheme.html" target="page">here</a> and the
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<code>meMode</code> codes <a href="ParticleDecays.html" target="page">here</a>.
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<p/>particle: id="0" name="void" spinType="0" chargeType="0" colType="0" m0="0.0">
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<p/>particle: id="1" name="d" antiName="dbar" spinType="2" chargeType="-1" colType="1"
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<p/>particle: id="2" name="u" antiName="ubar" spinType="2" chargeType="2" colType="1"
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<p/>particle: id="3" name="s" antiName="sbar" spinType="2" chargeType="-1" colType="1"
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<p/>particle: id="4" name="c" antiName="cbar" spinType="2" chargeType="2" colType="1"
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<p/>particle: id="5" name="b" antiName="bbar" spinType="2" chargeType="-1" colType="1"
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<p/>particle: id="6" name="t" antiName="tbar" spinType="2" chargeType="2" colType="1"
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m0="171.00000" mWidth="1.40000" mMin="86.00000" mMax="0.00000"
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<br/> channel: onMode="1" bRatio="0.0000300" products="24 1"
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<br/> channel: onMode="1" bRatio="0.0017650" products="24 3"
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<br/> channel: onMode="1" bRatio="0.9982050" products="24 5"
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<br/> channel: onMode="0" bRatio="0.0000000" products="37 5"
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<p/>particle: id="7" name="b'" antiName="b'bar" spinType="2" chargeType="-1" colType="1"
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<br/> channel: onMode="1" bRatio="0.0000000" products="-24 2"
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<br/> channel: onMode="1" bRatio="0.0000000" products="-24 4"
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<br/> channel: onMode="1" bRatio="1.0000000" products="-24 8"
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<p/>particle: id="8" name="t'" antiName="t'bar" spinType="2" chargeType="2" colType="1"
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<br/> channel: onMode="1" bRatio="0.0000000" products="24 1"
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<br/> channel: onMode="1" bRatio="0.0000000" products="24 3"
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<br/> channel: onMode="1" bRatio="0.0000000" products="24 5"
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<br/> channel: onMode="1" bRatio="1.0000000" products="24 7"
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<p/>particle: id="11" name="e-" antiName="e+" spinType="2" chargeType="-3" colType="0"
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<p/>particle: id="12" name="nu_e" antiName="nu_ebar" spinType="2" chargeType="0" colType="0"
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<p/>particle: id="13" name="mu-" antiName="mu+" spinType="2" chargeType="-3" colType="0"
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m0="0.10566" tau0="6.58654e+05"
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<br/> channel: onMode="1" bRatio="1.0000000" meMode="22" products="-12 11 14"
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<p/>particle: id="14" name="nu_mu" antiName="nu_mubar" spinType="2" chargeType="0" colType="0"
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<p/>particle: id="15" name="tau-" antiName="tau+" spinType="2" chargeType="-3" colType="0"
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m0="1.77699" tau0="8.71100e-02"
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<br/> channel: onMode="1" bRatio="0.108924" meMode="1521" products="16 -211"
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<br/> channel: onMode="1" bRatio="0.006885" meMode="1521" products="16 -321"
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<br/> channel: onMode="1" bRatio="0.178345" meMode="1531" products="16 11 -12"
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<br/> channel: onMode="1" bRatio="0.173545" meMode="1531" products="16 13 -14"
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<br/> channel: onMode="1" bRatio="0.254890" meMode="1532" products="16 111 -211"
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<br/> channel: onMode="1" bRatio="0.001513" meMode="1532" products="16 311 -321"
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<br/> channel: onMode="1" bRatio="0.000263" meMode="1532" products="16 221 -321"
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<br/> channel: onMode="1" bRatio="0.008957" meMode="1533" products="16 -211 -311"
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<br/> channel: onMode="1" bRatio="0.092370" meMode="1541" products="16 111 111 -211"
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<br/> channel: onMode="1" bRatio="0.089813" meMode="1541" products="16 -211 -211 211"
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<br/> channel: onMode="1" bRatio="0.044435" meMode="1551" products="16 111 -211 -211 211"
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<br/> channel: onMode="1" bRatio="0.010313" meMode="1551" products="16 111 111 111 -211"
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<br/> channel: onMode="1" bRatio="0.003757" meMode="0" products="16 111 -211 -311"
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<br/> channel: onMode="1" bRatio="0.003292" meMode="0" products="16 -211 211 -321"
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<br/> channel: onMode="1" bRatio="0.001087" meMode="0" products="16 130 -211 310"
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<br/> channel: onMode="1" bRatio="0.000235" meMode="0" products="16 130 130 -211"
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<br/> channel: onMode="1" bRatio="0.001762" meMode="0" products="16 22 111 -211"
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<br/> channel: onMode="1" bRatio="0.004935" meMode="0" products="16 111 111 -211 -211 211"
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<br/> channel: onMode="1" bRatio="0.001744" meMode="0" products="16 111 -211 221"
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<br/> channel: onMode="1" bRatio="0.000957" meMode="0" products="16 111 111 111 111 -211"
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<br/> channel: onMode="1" bRatio="0.000834" meMode="0" products="16 -211 -211 -211 211 211"
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<br/> channel: onMode="1" bRatio="0.000225" meMode="0" products="16 -211 -211 211 221"
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<br/> channel: onMode="1" bRatio="0.000145" meMode="0" products="16 111 111 -211 221"
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<br/> channel: onMode="1" bRatio="0.000400" meMode="0" products="16 223 -321"
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<br/> channel: onMode="1" bRatio="0.000397" meMode="0" products="16 111 111 111 -321"
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<br/> channel: onMode="1" bRatio="0.000280" meMode="0" products="16 221 -323"
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<br/> channel: onMode="1" bRatio="0.000297" meMode="0" products="16 111 -211 -311 311"
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<br/> channel: onMode="1" bRatio="0.000059" meMode="0" products="16 111 -211 -321 321"
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<p/>particle: id="16" name="nu_tau" antiName="nu_taubar" spinType="2" chargeType="0" colType="0"
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<p/>particle: id="17" name="tau'-" antiName="tau'+" spinType="2" chargeType="-3" colType="0"
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<br/> channel: onMode="1" bRatio="1.0000000" products="-24 18"
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<p/>particle: id="18" name="nu'_tau" antiName="nu'_taubar" spinType="2" chargeType="0" colType="0"
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<br/> channel: onMode="1" bRatio="1.0000000" products="24 17"
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<p/>particle: id="21" name="g" spinType="3" chargeType="0" colType="2"
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<p/>particle: id="22" name="gamma" spinType="3" chargeType="0" colType="0"
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<p/>particle: id="23" name="Z0" spinType="3" chargeType="0" colType="0"
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m0="91.18760" mWidth="2.49520" mMin="10.00000" mMax="0.00000"
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<br/> channel: onMode="1" bRatio="0.1539950" products="1 -1"
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<br/> channel: onMode="1" bRatio="0.1194200" products="2 -2"
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<br/> channel: onMode="1" bRatio="0.1539840" products="3 -3"
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<br/> channel: onMode="1" bRatio="0.1192590" products="4 -4"
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<br/> channel: onMode="1" bRatio="0.1522720" products="5 -5"
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<br/> channel: onMode="1" bRatio="0.0335760" products="11 -11"
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<br/> channel: onMode="1" bRatio="0.0668060" products="12 -12"
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<br/> channel: onMode="1" bRatio="0.0335760" products="13 -13"
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<br/> channel: onMode="1" bRatio="0.0668060" products="14 -14"
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<br/> channel: onMode="1" bRatio="0.0335000" products="15 -15"
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<br/> channel: onMode="1" bRatio="0.0668060" products="16 -16"
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<p/>particle: id="24" name="W+" antiName="W-" spinType="3" chargeType="3" colType="0"
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m0="80.40300" mWidth="2.14100" mMin="10.00000" mMax="0.00000"
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<br/> channel: onMode="1" bRatio="0.3213690" products="-1 2"
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<br/> channel: onMode="1" bRatio="0.0164940" products="-1 4"
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<br/> channel: onMode="1" bRatio="0.0165020" products="-3 2"
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<br/> channel: onMode="1" bRatio="0.3206150" products="-3 4"
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<br/> channel: onMode="1" bRatio="0.1080870" products="-15 16"
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<p/>particle: id="25" name="h0(H_1)" spinType="1" chargeType="0" colType="0"
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m0="125.00000" mWidth="0.00374" mMin="50.00000" mMax="0.00000"
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<br/> channel: onMode="1" bRatio="0.0000009" products="1 -1"
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<br/> channel: onMode="1" bRatio="0.0000002" products="2 -2"
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<br/> channel: onMode="1" bRatio="0.0002361" products="3 -3"
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<br/> channel: onMode="1" bRatio="0.0335602" products="4 -4"
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<br/> channel: onMode="1" bRatio="0.5876728" products="5 -5"
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<br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000011 -1000011"
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