| 63ba5337 |
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 < m < 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 < m < 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"/> |
| 328 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000025 1000022"/> |
| 329 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000025 1000023"/> |
| 330 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000025 1000025"/> |
| 331 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000035 1000022"/> |
| 332 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000035 1000023"/> |
| 333 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000035 1000025"/> |
| 334 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000035 1000035"/> |
| 335 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000024 -1000024"/> |
| 336 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000024 -1000037"/> |
| 337 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000037 -1000024"/> |
| 338 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000037 -1000037"/> |
| 339 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000001 -1000001"/> |
| 340 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="2000001 -2000001"/> |
| 341 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000001 -2000001"/> |
| 342 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="-1000001 2000001"/> |
| 343 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000002 -1000002"/> |
| 344 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="2000002 -2000002"/> |
| 345 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000002 -2000002"/> |
| 346 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="-1000002 2000002"/> |
| 347 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000003 -1000003"/> |
| 348 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="2000003 -2000003"/> |
| 349 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000003 -2000003"/> |
| 350 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="-1000003 2000003"/> |
| 351 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000004 -1000004"/> |
| 352 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="2000004 -2000004"/> |
| 353 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000004 -2000004"/> |
| 354 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="-1000004 2000004"/> |
| 355 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000005 -1000005"/> |
| 356 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="2000005 -2000005"/> |
| 357 | <channel onMode="1" bRatio="0.0000000" meMode="103" products="1000005 -2000005"/> |
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| 9291 | |
| 9292 | </chapter> |
| 9293 | |
| 9294 | <!-- Copyright (C) 2012 Torbjorn Sjostrand --> |
git://git.uio.no / u / mrichter / AliRoot.git / blame