Obsolete version removed.

[u/mrichter/AliRoot.git] / PYTHIA8 / pythia8130 / xmldoc / ParticleData.xml

diff --git a/PYTHIA8/pythia8130/xmldoc/ParticleData.xml b/PYTHIA8/pythia8130/xmldoc/ParticleData.xml
deleted file mode 100644 (file)
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--- a/PYTHIA8/pythia8130/xmldoc/ParticleData.xml
+++ /dev/null
@@ -1,7897 +0,0 @@
-<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>mass(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 &lt; m &lt; 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 &lt; m &lt; m_max</ei>, according
-to a truncated nonrelativistic 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-Wigners (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 name="ParticleData:muRun" default="0.003" min="0.001" max="0.006">
-the u quark MSbar mass at 2 GeV scale.
-
-<parm name="ParticleData:msRun" default="0.095" min="0.060" max="0.150">
-the s quark MSbar mass at 2 GeV scale.
-
-<parm name="ParticleData:mcRun" default="1.25" min="1.00" max="1.50">
-the c quark MSbar mass at the mass scale itself.
-
-<parm name="ParticleData:mbRun" default="4.20" min="4.00" max="4.50">
-the b quark MSbar mass at the mass scale itself.
-
-<parm name="ParticleData:mtRun" default="165.0" min="150.0" max="175.0">
-the t quark MSbar mass at the mass scale itself.
-
-<parm name="ParticleData:alphaSvalueMRun" default="0.125" min="0.10" max="0.20">
-the <ei>alpha_s(M_Z)</ei> value used to define tha rate at which MSbar
-masses run.
-
-
-<h3>Comments on the data</h3>
-
-The starting point for the current data is the 2006 Review of Particle 
-Physics <ref>Yao06</ref>. All known particle masses, widths and lifetimes
-have been set accordingly, while 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="0.0">
-</particle>
-
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-</particle>
-
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-</particle>
-
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-          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"
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-</particle>
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-<!-- Copyright (C) 2008 Torbjorn Sjostrand -->