Update to pythi8.170
[u/mrichter/AliRoot.git] / PYTHIA8 / pythia8170 / xmldoc / ParticleData.xml
1 <chapter name="Particle Data">
2
3 <h2>Particle Data</h2>
4
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.
9
10 <h3>Main settings</h3>
11
12 Apart from the data itself, the particle data table only contains 
13 a few aspects that are available to change:
14
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:
18 <option value="0">
19 mass is fixed at the nominal <ei>m_0</ei> value.
20 </option>
21 <option value="1">
22 particles registered as having a mass width are given a mass 
23 in the range <ei>m_min &lt; m &lt; m_max</ei>, according
24 to a truncated nonrelativistic Breit-Wigner, i.e. linear in <ei>m</ei>.
25 </option>
26 <option value="2">
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. 
34 </option>
35 <option value="3"> 
36 particles registered as having a mass width are given a mass 
37 in the range <ei>m_min &lt; m &lt; m_max</ei>, according
38 to a truncated relativistic Breit-Wigner, i.e. quadratic in <ei>m</ei>.
39 </option>
40 <option value="4"> 
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>.
43 </option>
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.
48 </modepick>
49
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.
59 </parm>
60
61 <p/>
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.)
71
72 <parm name="ParticleData:mdRun" default="0.006" min="0.003" max="0.008">
73 the d quark MSbar mass at 2 GeV scale.
74 </parm>
75
76 <parm name="ParticleData:muRun" default="0.003" min="0.001" max="0.006">
77 the u quark MSbar mass at 2 GeV scale.
78 </parm>
79
80 <parm name="ParticleData:msRun" default="0.095" min="0.060" max="0.150">
81 </parm>
82 the s quark MSbar mass at 2 GeV scale.
83
84 <parm name="ParticleData:mcRun" default="1.25" min="1.00" max="1.50">
85 </parm>
86 the c quark MSbar mass at the mass scale itself.
87
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.
90 </parm>
91
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.
94 </parm>
95
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
98 masses run.
99 </parm>
100
101
102 <h3>Comments on the data</h3>
103
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. 
111
112 <p/>
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>.
127
128 <p/>
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, 
144 5132, 5232 and 5332. 
145
146 <h3>The data itself</h3>
147
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>.
152
153 <particle id="0" name="void" spinType="0" chargeType="0" colType="0" m0="0.0">
154 </particle>
155
156 <particle id="1" name="d" antiName="dbar" spinType="2" chargeType="-1" colType="1"
157           m0="0.33000">
158 </particle>
159
160 <particle id="2" name="u" antiName="ubar" spinType="2" chargeType="2" colType="1"
161           m0="0.33000">
162 </particle>
163
164 <particle id="3" name="s" antiName="sbar" spinType="2" chargeType="-1" colType="1"
165           m0="0.50000">
166 </particle>
167
168 <particle id="4" name="c" antiName="cbar" spinType="2" chargeType="2" colType="1"
169           m0="1.50000">
170 </particle>
171
172 <particle id="5" name="b" antiName="bbar" spinType="2" chargeType="-1" colType="1"
173           m0="4.80000">
174 </particle>
175
176 <particle id="6" name="t" antiName="tbar" spinType="2" chargeType="2" colType="1"
177           m0="171.00000" mWidth="1.40000" mMin="86.00000" mMax="0.00000">
178  <channel onMode="1" bRatio="0.0000300" products="24 1"/>
179  <channel onMode="1" bRatio="0.0017650" products="24 3"/>
180  <channel onMode="1" bRatio="0.9982050" products="24 5"/>
181  <channel onMode="0" bRatio="0.0000000" products="37 5"/>
182 </particle>
183
184 <particle id="7" name="b'" antiName="b'bar" spinType="2" chargeType="-1" colType="1"
185           m0="400.00000">
186  <channel onMode="1" bRatio="0.0000000" products="-24 2"/>
187  <channel onMode="1" bRatio="0.0000000" products="-24 4"/>
188  <channel onMode="1" bRatio="0.0000000" products="-24 6"/>
189  <channel onMode="1" bRatio="1.0000000" products="-24 8"/>
190 </particle>
191
192 <particle id="8" name="t'" antiName="t'bar" spinType="2" chargeType="2" colType="1"
193           m0="400.00000">
194  <channel onMode="1" bRatio="0.0000000" products="24 1"/>
195  <channel onMode="1" bRatio="0.0000000" products="24 3"/>
196  <channel onMode="1" bRatio="0.0000000" products="24 5"/>
197  <channel onMode="1" bRatio="1.0000000" products="24 7"/>
198 </particle>
199
200 <particle id="11" name="e-" antiName="e+" spinType="2" chargeType="-3" colType="0"
201           m0="5.110e-04">
202 </particle>
203
204 <particle id="12" name="nu_e" antiName="nu_ebar" spinType="2" chargeType="0" colType="0"
205           m0="0.00000">
206 </particle>
207
208 <particle id="13" name="mu-" antiName="mu+" spinType="2" chargeType="-3" colType="0"
209           m0="0.10566" tau0="6.58654e+05">
210  <channel onMode="1" bRatio="1.0000000" meMode="22" products="-12 11 14"/>
211 </particle>
212
213 <particle id="14" name="nu_mu" antiName="nu_mubar" spinType="2" chargeType="0" colType="0"
214           m0="0.00000">
215 </particle>
216
217 <particle id="15" name="tau-" antiName="tau+" spinType="2" chargeType="-3" colType="0"
218           m0="1.77682" tau0="8.71100e-02">
219  <channel onMode="1" bRatio="0.108924" meMode="1521" products="16 -211"/>
220  <channel onMode="1" bRatio="0.006885" meMode="1521" products="16 -321"/>
221  <channel onMode="1" bRatio="0.178345" meMode="1531" products="16 11 -12"/>
222  <channel onMode="1" bRatio="0.173545" meMode="1531" products="16 13 -14"/>
223  <channel onMode="1" bRatio="0.254890" meMode="1532" products="16 111 -211"/>
224  <channel onMode="1" bRatio="0.001513" meMode="1532" products="16 311 -321"/>
225  <channel onMode="1" bRatio="0.000263" meMode="1532" products="16 221 -321"/>
226  <channel onMode="1" bRatio="0.008957" meMode="1533" products="16 -211 -311"/>
227  <channel onMode="1" bRatio="0.004491" meMode="1533" products="16 111 -321"/>
228  <channel onMode="1" bRatio="0.092370" meMode="1541" products="16 111 111 -211"/>
229  <channel onMode="1" bRatio="0.089813" meMode="1541" products="16 -211 -211 211"/>
230  <channel onMode="1" bRatio="0.003757" meMode="1542" products="16 111 -211 -311"/>
231  <channel onMode="1" bRatio="0.003292" meMode="1542" products="16 -211 211 -321"/>
232  <channel onMode="1" bRatio="0.001519" meMode="1542" products="16 -211 -321 321"/>
233  <channel onMode="1" bRatio="0.001518" meMode="1542" products="16 111 311 -321"/>
234  <channel onMode="1" bRatio="0.001087" meMode="1542" products="16 130 -211 310"/>
235  <channel onMode="1" bRatio="0.000555" meMode="1542" products="16 111 111 -321"/>
236  <channel onMode="1" bRatio="0.000235" meMode="1542" products="16 130 130 -211"/>
237  <channel onMode="1" bRatio="0.000235" meMode="1542" products="16 -211 310 310"/>
238  <channel onMode="1" bRatio="0.001744" meMode="1543" products="16 111 -211 221"/>
239  <channel onMode="1" bRatio="0.001762" meMode="1544" products="16 22  111 -211"/>
240  <channel onMode="1" bRatio="0.044435" meMode="1551" products="16 111 -211 -211 211"/>
241  <channel onMode="1" bRatio="0.010313" meMode="1551" products="16 111 111 111 -211"/>
242  <channel onMode="1" bRatio="0.004935" meMode="1561" products="16 111 111 -211 -211 211"/>
243  <channel onMode="1" bRatio="0.000957" meMode="1561" products="16 111 111 111 111 -211"/>
244  <channel onMode="1" bRatio="0.000834" meMode="1561" products="16 -211 -211 -211 211 211"/>
245  <channel onMode="1" bRatio="0.000225" meMode="0" products="16 -211 -211 211 221"/>
246  <channel onMode="1" bRatio="0.000145" meMode="0" products="16 111 111 -211 221"/>
247  <channel onMode="1" bRatio="0.000135" meMode="0" products="16 111 111 -211 223"/>
248  <channel onMode="1" bRatio="0.000118" meMode="0" products="16 -211 -211 211 223"/>
249  <channel onMode="1" bRatio="0.000400" meMode="0" products="16 223 -321"/>
250  <channel onMode="1" bRatio="0.000397" meMode="0" products="16 111 111 111 -321"/>
251  <channel onMode="1" bRatio="0.000307" meMode="0" products="16 111 -211 211 -321"/>
252  <channel onMode="1" bRatio="0.000280" meMode="0" products="16 221 -323"/>
253  <channel onMode="1" bRatio="0.000238" meMode="0" products="16 111 111 -211 -311"/>
254  <channel onMode="1" bRatio="0.000225" meMode="0" products="16 -211 -211 211 -311"/>
255  <channel onMode="1" bRatio="0.000297" meMode="0" products="16 111 -211 -311 311"/>
256  <channel onMode="1" bRatio="0.000059" meMode="0" products="16 111 -211 -321 321"/>
257 </particle>
258
259 <particle id="16" name="nu_tau" antiName="nu_taubar" spinType="2" chargeType="0" colType="0"
260           m0="0.00000">
261 </particle>
262
263 <particle id="17" name="tau'-" antiName="tau'+" spinType="2" chargeType="-3" colType="0"
264           m0="400.00000">
265  <channel onMode="1" bRatio="1.0000000" products="-24 18"/>
266 </particle>
267
268 <particle id="18" name="nu'_tau" antiName="nu'_taubar" spinType="2" chargeType="0" colType="0"
269           m0="400.00000">
270  <channel onMode="1" bRatio="1.0000000" products="24 17"/>
271 </particle>
272
273 <particle id="21" name="g" spinType="3" chargeType="0" colType="2"
274           m0="0.00000">
275 </particle>
276
277 <particle id="22" name="gamma" spinType="3" chargeType="0" colType="0"
278           m0="0.00000">
279 </particle>
280
281 <particle id="23" name="Z0" spinType="3" chargeType="0" colType="0"
282           m0="91.18760" mWidth="2.49520" mMin="10.00000" mMax="0.00000">
283  <channel onMode="1" bRatio="0.1539950" products="1 -1"/>
284  <channel onMode="1" bRatio="0.1194200" products="2 -2"/>
285  <channel onMode="1" bRatio="0.1539840" products="3 -3"/>
286  <channel onMode="1" bRatio="0.1192590" products="4 -4"/>
287  <channel onMode="1" bRatio="0.1522720" products="5 -5"/>
288  <channel onMode="1" bRatio="0.0335760" products="11 -11"/>
289  <channel onMode="1" bRatio="0.0668060" products="12 -12"/>
290  <channel onMode="1" bRatio="0.0335760" products="13 -13"/>
291  <channel onMode="1" bRatio="0.0668060" products="14 -14"/>
292  <channel onMode="1" bRatio="0.0335000" products="15 -15"/>
293  <channel onMode="1" bRatio="0.0668060" products="16 -16"/>
294 </particle>
295
296 <particle id="24" name="W+" antiName="W-" spinType="3" chargeType="3" colType="0"
297           m0="80.38500" mWidth="2.08500" mMin="10.00000" mMax="0.00000">
298  <channel onMode="1" bRatio="0.3213690" products="-1 2"/>
299  <channel onMode="1" bRatio="0.0164940" products="-1 4"/>
300  <channel onMode="1" bRatio="0.0165020" products="-3 2"/>
301  <channel onMode="1" bRatio="0.3206150" products="-3 4"/>
302  <channel onMode="1" bRatio="0.0000100" products="-5 2"/>
303  <channel onMode="1" bRatio="0.0005910" products="-5 4"/>
304  <channel onMode="1" bRatio="0.1081660" products="-11 12"/>
305  <channel onMode="1" bRatio="0.1081660" products="-13 14"/>
306  <channel onMode="1" bRatio="0.1080870" products="-15 16"/>
307 </particle>
308
309 <particle id="25" name="h0(H_1)" spinType="1" chargeType="0" colType="0"
310           m0="125.00000" mWidth="0.00374" mMin="50.00000" mMax="0.00000">
311  <channel onMode="1" bRatio="0.0000009" products="1 -1"/>
312  <channel onMode="1" bRatio="0.0000002" products="2 -2"/>
313  <channel onMode="1" bRatio="0.0002361" products="3 -3"/>
314  <channel onMode="1" bRatio="0.0335602" products="4 -4"/>
315  <channel onMode="1" bRatio="0.5876728" products="5 -5"/>
316  <channel onMode="1" bRatio="0.0000000" products="6 -6"/>
317  <channel onMode="1" bRatio="0.0000000" products="11 -11"/>
318  <channel onMode="1" bRatio="0.0002445" products="13 -13"/>
319  <channel onMode="1" bRatio="0.0690800" products="15 -15"/>
320  <channel onMode="1" bRatio="0.0630585" products="21 21"/>
321  <channel onMode="1" bRatio="0.0028438" products="22 22"/>
322  <channel onMode="1" bRatio="0.0017601" products="22 23"/>
323  <channel onMode="1" bRatio="0.0259708" products="23 23"/>
324  <channel onMode="1" bRatio="0.2155720" products="24 -24"/>
325  <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000022 1000022"/>
326  <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000023 1000022"/>
327  <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000023 1000023"/>
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