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| 2 | <head> |
| 3 | <title>Particle Data</title> |
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| 28 | <form method='post' action='ParticleData.php'> |
| 29 | |
| 30 | <h2>Particle Data</h2> |
| 31 | |
| 32 | The structure and operation of the particle data table is described |
| 33 | <?php $filepath = $_GET["filepath"]; |
| 34 | echo "<a href='ParticleDataScheme.php?filepath=".$filepath."' target='page'>";?>here</a>. That page |
| 35 | also describes how default data properties can be changed. The |
| 36 | current page provides the actual default values. |
| 37 | |
| 38 | <h3>Main settings</h3> |
| 39 | |
| 40 | Apart from the data itself, the particle data table only contains |
| 41 | a few aspects that are available to change: |
| 42 | |
| 43 | <br/><br/><table><tr><td><strong>ParticleData:modeBreitWigner </td><td> (<code>default = <strong>4</strong></code>; <code>minimum = 0</code>; <code>maximum = 4</code>)</td></tr></table> |
| 44 | Selection of particle masses when the <code>mass(id)</code> is called |
| 45 | to provide a new mass: |
| 46 | <br/> |
| 47 | <input type="radio" name="1" value="0"><strong>0 </strong>: mass is fixed at the nominal <ei>m_0</ei> value. <br/> |
| 48 | <input type="radio" name="1" value="1"><strong>1 </strong>: particles registered as having a mass width are given a mass in the range <ei>m_min < m < m_max</ei>, according to a truncated nonrelativistic Breit-Wigner, i.e. linear in <ei>m</ei>. <br/> |
| 49 | <input type="radio" name="1" value="2"><strong>2 </strong>: 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. <br/> |
| 50 | <input type="radio" name="1" value="3"><strong>3 </strong>: particles registered as having a mass width are given a mass in the range <ei>m_min < m < m_max</ei>, according to a truncated relativistic Breit-Wigner, i.e. quadratic in <ei>m</ei>. <br/> |
| 51 | <input type="radio" name="1" value="4" checked="checked"><strong>4 </strong>: 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>. <br/> |
| 52 | <br/><b>Note:</b> this mode only applies to normal hadronic |
| 53 | resonances like the <ei>rho</ei>. The more massive states of the |
| 54 | <code>isResonance()</code> type, like <ei>Z^0</ei> or top, are |
| 55 | considered separately. |
| 56 | |
| 57 | <br/><br/><table><tr><td><strong>ParticleData:maxEnhanceBW </td><td></td><td> <input type="text" name="2" value="2.5" size="20"/> (<code>default = <strong>2.5</strong></code>; <code>minimum = 1.</code>; <code>maximum = 5.</code>)</td></tr></table> |
| 58 | The modifications in options 2 and 4 above enhance the large-mass tail |
| 59 | of the Breit-Wigners (the mass spectrum develops a dm/m divergence). |
| 60 | However, we expect form factors to dampen this tail at masses some distance |
| 61 | above the nominal one, so cut off the rise by requiring the actual |
| 62 | Breit-Wigner weight not to be more than a factor <code> maxEnhanceBW</code> |
| 63 | above the one obtained with options 1 or 3, respectively. This also |
| 64 | opens up for a simpler technical handling of mass selection in options |
| 65 | 2 and 4, by using standard hit-and-miss Monte Carlo. |
| 66 | |
| 67 | |
| 68 | <p/> |
| 69 | Since running masses are only calculated for the six quark flavours, |
| 70 | e.g. to obtain couplings to the Higgs boson(s), there is not an entry |
| 71 | in the normal tables for each particles, but only the six MSbar mass |
| 72 | values below, used as starting point for the running. In addition you |
| 73 | can pick an <i>alpha_s(M_Z)</i>, which is converted into a first-order |
| 74 | five-flavour Lambda that is used to determine the rate of the running. |
| 75 | (Without any match to four flavours below <i>m_b</i>; if desired, this |
| 76 | can be fixed by slightly shifted default mass values, since the routines |
| 77 | never should be called below the <i>m_b</i> scale anyway.) |
| 78 | |
| 79 | <br/><br/><table><tr><td><strong>ParticleData:mdRun </td><td></td><td> <input type="text" name="3" value="0.006" size="20"/> (<code>default = <strong>0.006</strong></code>; <code>minimum = 0.003</code>; <code>maximum = 0.008</code>)</td></tr></table> |
| 80 | the d quark MSbar mass at 2 GeV scale. |
| 81 | |
| 82 | |
| 83 | <br/><br/><table><tr><td><strong>ParticleData:muRun </td><td></td><td> <input type="text" name="4" value="0.003" size="20"/> (<code>default = <strong>0.003</strong></code>; <code>minimum = 0.001</code>; <code>maximum = 0.006</code>)</td></tr></table> |
| 84 | the u quark MSbar mass at 2 GeV scale. |
| 85 | |
| 86 | |
| 87 | <br/><br/><table><tr><td><strong>ParticleData:msRun </td><td></td><td> <input type="text" name="5" value="0.095" size="20"/> (<code>default = <strong>0.095</strong></code>; <code>minimum = 0.060</code>; <code>maximum = 0.150</code>)</td></tr></table> |
| 88 | |
| 89 | the s quark MSbar mass at 2 GeV scale. |
| 90 | |
| 91 | <br/><br/><table><tr><td><strong>ParticleData:mcRun </td><td></td><td> <input type="text" name="6" value="1.25" size="20"/> (<code>default = <strong>1.25</strong></code>; <code>minimum = 1.00</code>; <code>maximum = 1.50</code>)</td></tr></table> |
| 92 | |
| 93 | the c quark MSbar mass at the mass scale itself. |
| 94 | |
| 95 | <br/><br/><table><tr><td><strong>ParticleData:mbRun </td><td></td><td> <input type="text" name="7" value="4.20" size="20"/> (<code>default = <strong>4.20</strong></code>; <code>minimum = 4.00</code>; <code>maximum = 4.50</code>)</td></tr></table> |
| 96 | the b quark MSbar mass at the mass scale itself. |
| 97 | |
| 98 | |
| 99 | <br/><br/><table><tr><td><strong>ParticleData:mtRun </td><td></td><td> <input type="text" name="8" value="165.0" size="20"/> (<code>default = <strong>165.0</strong></code>; <code>minimum = 150.0</code>; <code>maximum = 175.0</code>)</td></tr></table> |
| 100 | the t quark MSbar mass at the mass scale itself. |
| 101 | |
| 102 | |
| 103 | <br/><br/><table><tr><td><strong>ParticleData:alphaSvalueMRun </td><td></td><td> <input type="text" name="9" value="0.125" size="20"/> (<code>default = <strong>0.125</strong></code>; <code>minimum = 0.10</code>; <code>maximum = 0.20</code>)</td></tr></table> |
| 104 | the <i>alpha_s(M_Z)</i> value used to define tha rate at which MSbar |
| 105 | masses run. |
| 106 | |
| 107 | |
| 108 | |
| 109 | <h3>Comments on the data</h3> |
| 110 | |
| 111 | The starting point for the current data is the 2006 Review of Particle |
| 112 | Physics [<a href="Bibliography.php" target="page">Yao06</a>]. All known particle masses, widths and lifetimes |
| 113 | have been set accordingly, while not-yet-measured particles are kept at |
| 114 | their values from PYTHIA 6. Decay channels and their branching |
| 115 | ratios remain a major worry: many particles do not have one single solidly |
| 116 | measured branching ratio, and many further do not have known branching |
| 117 | ratios that add up to (the neighbourhood of) unity. |
| 118 | |
| 119 | <p/> |
| 120 | Uncertainties are especially big for the scalar, pseudovector and tensor |
| 121 | <i>L = 1</i> multiplets available in PYTHIA. We note that |
| 122 | some distributions become better described when these multiplets are |
| 123 | included in the generation, while others become worse. It is tempting to |
| 124 | associate this lackluster performance with the primitive knowledge. |
| 125 | Not even the multiplets themselves are particularly well known. |
| 126 | It used to be that the <i>a_0(980)</i> and <i>f_0(980)</i> |
| 127 | were considered to be members of the scalar multiplet. Nowadays they are |
| 128 | commonly assumed to be either four-quark states or of some other exotic |
| 129 | character. This means that the PYTHIA 8 PDG particle codes |
| 130 | have been changed for these particles, relative to what was used in |
| 131 | PYTHIA 6 based on previous PDG editions. Specifically their |
| 132 | numbers are now in the 9000000 series, and they have been replaced in the |
| 133 | scalar multiplet by <i>a_0(1450)</i> and <i>f_0(1370)</i>. |
| 134 | |
| 135 | <p/> |
| 136 | For charm and bottom mesons the jungle of partial measurements makes |
| 137 | it very difficult to construct fully consistent sets of decay channels. |
| 138 | This part of the program has not yet been brought up to date to the |
| 139 | 2006 RPP. Instead the LHCb decay tables (for EvtGen, but without |
| 140 | using the EvtGen matrix-element machinery) and the DELPHI tune for |
| 141 | PYTHIA 6 is being used. (This also includes a few non-c/b |
| 142 | hadrons that only occur in the c/b decay tables.) This has the |
| 143 | advantage that many tests have been made for consistency, but the |
| 144 | disadvantage that it is not always in agreement with the latest |
| 145 | measurements of some specific decay channels. The decays based |
| 146 | on the LHCb tables (with some modifications) are 411, 421, 431, 441, |
| 147 | 445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122, |
| 148 | 14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441, |
| 149 | 100443, 100553, 9000111, 9000211. Correspondingly the decays based on |
| 150 | the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332, |
| 151 | 5132, 5232 and 5332. |
| 152 | |
| 153 | <h3>The data itself</h3> |
| 154 | |
| 155 | Here comes the default particle data used in the program. Do not touch. |
| 156 | The meaning of the various properties and the format used are explained |
| 157 | <?php $filepath = $_GET["filepath"]; |
| 158 | echo "<a href='ParticleDataScheme.php?filepath=".$filepath."' target='page'>";?>here</a> and the |
| 159 | <code>meMode</code> codes <?php $filepath = $_GET["filepath"]; |
| 160 | echo "<a href='ParticleDecays.php?filepath=".$filepath."' target='page'>";?>here</a>. |
| 161 | |
| 162 | <p/>particle: id="0" name="void" spinType="0" chargeType="0" colType="0" m0="0.0"> |
| 163 | |
| 164 | <p/>particle: id="1" name="d" antiName="dbar" spinType="2" chargeType="-1" colType="1" |
| 165 | m0="0.33000" |
| 166 | |
| 167 | <p/>particle: id="2" name="u" antiName="ubar" spinType="2" chargeType="2" colType="1" |
| 168 | m0="0.33000" |
| 169 | |
| 170 | <p/>particle: id="3" name="s" antiName="sbar" spinType="2" chargeType="-1" colType="1" |
| 171 | m0="0.50000" |
| 172 | |
| 173 | <p/>particle: id="4" name="c" antiName="cbar" spinType="2" chargeType="2" colType="1" |
| 174 | m0="1.50000" |
| 175 | |
| 176 | <p/>particle: id="5" name="b" antiName="bbar" spinType="2" chargeType="-1" colType="1" |
| 177 | m0="4.80000" |
| 178 | |
| 179 | <p/>particle: id="6" name="t" antiName="tbar" spinType="2" chargeType="2" colType="1" |
| 180 | m0="171.00000" mWidth="1.40000" mMin="86.00000" mMax="0.00000" |
| 181 | <br/> channel: onMode="1" bRatio="0.0000300" products="24 1" |
| 182 | <br/> channel: onMode="1" bRatio="0.0017650" products="24 3" |
| 183 | <br/> channel: onMode="1" bRatio="0.9982050" products="24 5" |
| 184 | <br/> channel: onMode="0" bRatio="0.0000000" products="37 5" |
| 185 | |
| 186 | <p/>particle: id="7" name="b'" antiName="b'bar" spinType="2" chargeType="-1" colType="1" |
| 187 | m0="400.00000" |
| 188 | <br/> channel: onMode="1" bRatio="0.0000000" products="-24 2" |
| 189 | <br/> channel: onMode="1" bRatio="0.0000000" products="-24 4" |
| 190 | <br/> channel: onMode="1" bRatio="0.0000000" products="-24 6" |
| 191 | <br/> channel: onMode="1" bRatio="1.0000000" products="-24 8" |
| 192 | |
| 193 | <p/>particle: id="8" name="t'" antiName="t'bar" spinType="2" chargeType="2" colType="1" |
| 194 | m0="400.00000" |
| 195 | <br/> channel: onMode="1" bRatio="0.0000000" products="24 1" |
| 196 | <br/> channel: onMode="1" bRatio="0.0000000" products="24 3" |
| 197 | <br/> channel: onMode="1" bRatio="0.0000000" products="24 5" |
| 198 | <br/> channel: onMode="1" bRatio="1.0000000" products="24 7" |
| 199 | |
| 200 | <p/>particle: id="11" name="e-" antiName="e+" spinType="2" chargeType="-3" colType="0" |
| 201 | m0="5.110e-04" |
| 202 | |
| 203 | <p/>particle: id="12" name="nu_e" antiName="nu_ebar" spinType="2" chargeType="0" colType="0" |
| 204 | m0="0.00000" |
| 205 | |
| 206 | <p/>particle: id="13" name="mu-" antiName="mu+" spinType="2" chargeType="-3" colType="0" |
| 207 | m0="0.10566" tau0="6.58654e+05" |
| 208 | <br/> channel: onMode="1" bRatio="1.0000000" meMode="22" products="-12 11 14" |
| 209 | |
| 210 | <p/>particle: id="14" name="nu_mu" antiName="nu_mubar" spinType="2" chargeType="0" colType="0" |
| 211 | m0="0.00000" |
| 212 | |
| 213 | <p/>particle: id="15" name="tau-" antiName="tau+" spinType="2" chargeType="-3" colType="0" |
| 214 | m0="1.77682" tau0="8.71100e-02" |
| 215 | <br/> channel: onMode="1" bRatio="0.108924" meMode="1521" products="16 -211" |
| 216 | <br/> channel: onMode="1" bRatio="0.006885" meMode="1521" products="16 -321" |
| 217 | <br/> channel: onMode="1" bRatio="0.178345" meMode="1531" products="16 11 -12" |
| 218 | <br/> channel: onMode="1" bRatio="0.173545" meMode="1531" products="16 13 -14" |
| 219 | <br/> channel: onMode="1" bRatio="0.254890" meMode="1532" products="16 111 -211" |
| 220 | <br/> channel: onMode="1" bRatio="0.001513" meMode="1532" products="16 311 -321" |
| 221 | <br/> channel: onMode="1" bRatio="0.000263" meMode="1532" products="16 221 -321" |
| 222 | <br/> channel: onMode="1" bRatio="0.008957" meMode="1533" products="16 -211 -311" |
| 223 | <br/> channel: onMode="1" bRatio="0.004491" meMode="1533" products="16 111 -321" |
| 224 | <br/> channel: onMode="1" bRatio="0.092370" meMode="1541" products="16 111 111 -211" |
| 225 | <br/> channel: onMode="1" bRatio="0.089813" meMode="1541" products="16 -211 -211 211" |
| 226 | <br/> channel: onMode="1" bRatio="0.003757" meMode="1542" products="16 111 -211 -311" |
| 227 | <br/> channel: onMode="1" bRatio="0.003292" meMode="1542" products="16 -211 211 -321" |
| 228 | <br/> channel: onMode="1" bRatio="0.001519" meMode="1542" products="16 -211 -321 321" |
| 229 | <br/> channel: onMode="1" bRatio="0.001518" meMode="1542" products="16 111 311 -321" |
| 230 | <br/> channel: onMode="1" bRatio="0.001087" meMode="1542" products="16 130 -211 310" |
| 231 | <br/> channel: onMode="1" bRatio="0.000555" meMode="1542" products="16 111 111 -321" |
| 232 | <br/> channel: onMode="1" bRatio="0.000235" meMode="1542" products="16 130 130 -211" |
| 233 | <br/> channel: onMode="1" bRatio="0.000235" meMode="1542" products="16 -211 310 310" |
| 234 | <br/> channel: onMode="1" bRatio="0.001744" meMode="1543" products="16 111 -211 221" |
| 235 | <br/> channel: onMode="1" bRatio="0.001762" meMode="1544" products="16 22 111 -211" |
| 236 | <br/> channel: onMode="1" bRatio="0.044435" meMode="1551" products="16 111 -211 -211 211" |
| 237 | <br/> channel: onMode="1" bRatio="0.010313" meMode="1551" products="16 111 111 111 -211" |
| 238 | <br/> channel: onMode="1" bRatio="0.004935" meMode="1561" products="16 111 111 -211 -211 211" |
| 239 | <br/> channel: onMode="1" bRatio="0.000957" meMode="1561" products="16 111 111 111 111 -211" |
| 240 | <br/> channel: onMode="1" bRatio="0.000834" meMode="1561" products="16 -211 -211 -211 211 211" |
| 241 | <br/> channel: onMode="1" bRatio="0.000225" meMode="0" products="16 -211 -211 211 221" |
| 242 | <br/> channel: onMode="1" bRatio="0.000145" meMode="0" products="16 111 111 -211 221" |
| 243 | <br/> channel: onMode="1" bRatio="0.000135" meMode="0" products="16 111 111 -211 223" |
| 244 | <br/> channel: onMode="1" bRatio="0.000118" meMode="0" products="16 -211 -211 211 223" |
| 245 | <br/> channel: onMode="1" bRatio="0.000400" meMode="0" products="16 223 -321" |
| 246 | <br/> channel: onMode="1" bRatio="0.000397" meMode="0" products="16 111 111 111 -321" |
| 247 | <br/> channel: onMode="1" bRatio="0.000307" meMode="0" products="16 111 -211 211 -321" |
| 248 | <br/> channel: onMode="1" bRatio="0.000280" meMode="0" products="16 221 -323" |
| 249 | <br/> channel: onMode="1" bRatio="0.000238" meMode="0" products="16 111 111 -211 -311" |
| 250 | <br/> channel: onMode="1" bRatio="0.000225" meMode="0" products="16 -211 -211 211 -311" |
| 251 | <br/> channel: onMode="1" bRatio="0.000297" meMode="0" products="16 111 -211 -311 311" |
| 252 | <br/> channel: onMode="1" bRatio="0.000059" meMode="0" products="16 111 -211 -321 321" |
| 253 | |
| 254 | <p/>particle: id="16" name="nu_tau" antiName="nu_taubar" spinType="2" chargeType="0" colType="0" |
| 255 | m0="0.00000" |
| 256 | |
| 257 | <p/>particle: id="17" name="tau'-" antiName="tau'+" spinType="2" chargeType="-3" colType="0" |
| 258 | m0="400.00000" |
| 259 | <br/> channel: onMode="1" bRatio="1.0000000" products="-24 18" |
| 260 | |
| 261 | <p/>particle: id="18" name="nu'_tau" antiName="nu'_taubar" spinType="2" chargeType="0" colType="0" |
| 262 | m0="400.00000" |
| 263 | <br/> channel: onMode="1" bRatio="1.0000000" products="24 17" |
| 264 | |
| 265 | <p/>particle: id="21" name="g" spinType="3" chargeType="0" colType="2" |
| 266 | m0="0.00000" |
| 267 | |
| 268 | <p/>particle: id="22" name="gamma" spinType="3" chargeType="0" colType="0" |
| 269 | m0="0.00000" |
| 270 | |
| 271 | <p/>particle: id="23" name="Z0" spinType="3" chargeType="0" colType="0" |
| 272 | m0="91.18760" mWidth="2.49520" mMin="10.00000" mMax="0.00000" |
| 273 | <br/> channel: onMode="1" bRatio="0.1539950" products="1 -1" |
| 274 | <br/> channel: onMode="1" bRatio="0.1194200" products="2 -2" |
| 275 | <br/> channel: onMode="1" bRatio="0.1539840" products="3 -3" |
| 276 | <br/> channel: onMode="1" bRatio="0.1192590" products="4 -4" |
| 277 | <br/> channel: onMode="1" bRatio="0.1522720" products="5 -5" |
| 278 | <br/> channel: onMode="1" bRatio="0.0335760" products="11 -11" |
| 279 | <br/> channel: onMode="1" bRatio="0.0668060" products="12 -12" |
| 280 | <br/> channel: onMode="1" bRatio="0.0335760" products="13 -13" |
| 281 | <br/> channel: onMode="1" bRatio="0.0668060" products="14 -14" |
| 282 | <br/> channel: onMode="1" bRatio="0.0335000" products="15 -15" |
| 283 | <br/> channel: onMode="1" bRatio="0.0668060" products="16 -16" |
| 284 | |
| 285 | <p/>particle: id="24" name="W+" antiName="W-" spinType="3" chargeType="3" colType="0" |
| 286 | m0="80.38500" mWidth="2.08500" mMin="10.00000" mMax="0.00000" |
| 287 | <br/> channel: onMode="1" bRatio="0.3213690" products="-1 2" |
| 288 | <br/> channel: onMode="1" bRatio="0.0164940" products="-1 4" |
| 289 | <br/> channel: onMode="1" bRatio="0.0165020" products="-3 2" |
| 290 | <br/> channel: onMode="1" bRatio="0.3206150" products="-3 4" |
| 291 | <br/> channel: onMode="1" bRatio="0.0000100" products="-5 2" |
| 292 | <br/> channel: onMode="1" bRatio="0.0005910" products="-5 4" |
| 293 | <br/> channel: onMode="1" bRatio="0.1081660" products="-11 12" |
| 294 | <br/> channel: onMode="1" bRatio="0.1081660" products="-13 14" |
| 295 | <br/> channel: onMode="1" bRatio="0.1080870" products="-15 16" |
| 296 | |
| 297 | <p/>particle: id="25" name="h0(H_1)" spinType="1" chargeType="0" colType="0" |
| 298 | m0="125.00000" mWidth="0.00374" mMin="50.00000" mMax="0.00000" |
| 299 | <br/> channel: onMode="1" bRatio="0.0000009" products="1 -1" |
| 300 | <br/> channel: onMode="1" bRatio="0.0000002" products="2 -2" |
| 301 | <br/> channel: onMode="1" bRatio="0.0002361" products="3 -3" |
| 302 | <br/> channel: onMode="1" bRatio="0.0335602" products="4 -4" |
| 303 | <br/> channel: onMode="1" bRatio="0.5876728" products="5 -5" |
| 304 | <br/> channel: onMode="1" bRatio="0.0000000" products="6 -6" |
| 305 | <br/> channel: onMode="1" bRatio="0.0000000" products="11 -11" |
| 306 | <br/> channel: onMode="1" bRatio="0.0002445" products="13 -13" |
| 307 | <br/> channel: onMode="1" bRatio="0.0690800" products="15 -15" |
| 308 | <br/> channel: onMode="1" bRatio="0.0630585" products="21 21" |
| 309 | <br/> channel: onMode="1" bRatio="0.0028438" products="22 22" |
| 310 | <br/> channel: onMode="1" bRatio="0.0017601" products="22 23" |
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| 3520 | <p/>particle: id="4214" name="Sigma*_c+" antiName="Sigma*_cbar-" spinType="4" chargeType="3" colType="0" |
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| 3524 | <p/>particle: id="4222" name="Sigma_c++" antiName="Sigma_cbar--" spinType="2" chargeType="6" colType="0" |
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| 3543 | <p/>particle: id="4303" name="cs_1" antiName="cs_1bar" spinType="3" chargeType="1" colType="-1" |
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| 3564 | <p/>particle: id="4332" name="Omega_c0" antiName="Omega_cbar0" spinType="2" chargeType="0" colType="0" |
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| 3570 | <p/>particle: id="4334" name="Omega*_c0" antiName="Omega*_cbar0" spinType="4" chargeType="0" colType="0" |
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| 3577 | <p/>particle: id="4412" name="Xi_cc+" antiName="Xi_ccbar-" spinType="2" chargeType="3" colType="0" |
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| 3584 | <p/>particle: id="4414" name="Xi*_cc+" antiName="Xi*_ccbar-" spinType="4" chargeType="3" colType="0" |
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| 3591 | <p/>particle: id="4422" name="Xi_cc++" antiName="Xi_ccbar--" spinType="2" chargeType="6" colType="0" |
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| 8836 | <br/> channel: onMode="1" bRatio="0.0000000" products="9900024 9900024" |
| 8837 | |
| 8838 | <p/>particle: id="9900110" name="rho_diff0" spinType="0" chargeType="0" colType="0" |
| 8839 | m0="0.00000" |
| 8840 | |
| 8841 | <p/>particle: id="9900210" name="pi_diffr+" antiName="pi_diffr-" spinType="0" chargeType="3" colType="0" |
| 8842 | m0="0.00000" |
| 8843 | |
| 8844 | <p/>particle: id="9900220" name="omega_di" spinType="0" chargeType="0" colType="0" |
| 8845 | m0="0.00000" |
| 8846 | |
| 8847 | <p/>particle: id="9900330" name="phi_diff" spinType="0" chargeType="0" colType="0" |
| 8848 | m0="0.00000" |
| 8849 | |
| 8850 | <p/>particle: id="9900440" name="J/psi_di" spinType="0" chargeType="0" colType="0" |
| 8851 | m0="0.00000" |
| 8852 | |
| 8853 | <p/>particle: id="9900441" name="ccbar[1S0(8)]" spinType="1" chargeType="0" colType="2" |
| 8854 | m0="3.10000" mWidth="0.01000" mMin="3.10000" mMax="3.10000" |
| 8855 | <br/> channel: onMode="1" bRatio="1.0000000" products="443 21" |
| 8856 | |
| 8857 | <p/>particle: id="9900443" name="ccbar[3S1(8)]" spinType="3" chargeType="0" colType="2" |
| 8858 | m0="3.10000" mWidth="0.01000" mMin="3.10000" mMax="3.10000" |
| 8859 | <br/> channel: onMode="1" bRatio="1.0000000" products="443 21" |
| 8860 | |
| 8861 | <p/>particle: id="9900551" name="bbbar[1S0(8)]" spinType="1" chargeType="0" colType="2" |
| 8862 | m0="9.50000" mWidth="0.01000" mMin="9.50000" mMax="9.50000" |
| 8863 | <br/> channel: onMode="1" bRatio="1.0000000" products="553 21" |
| 8864 | |
| 8865 | <p/>particle: id="9900553" name="bbbar[3S1(8)]" spinType="3" chargeType="0" colType="2" |
| 8866 | m0="9.50000" mWidth="0.01000" mMin="9.50000" mMax="9.50000" |
| 8867 | <br/> channel: onMode="1" bRatio="1.0000000" products="553 21" |
| 8868 | |
| 8869 | <p/>particle: id="9902110" name="n_diffr0" antiName="n_diffrbar0" spinType="0" chargeType="0" colType="0" |
| 8870 | m0="0.00000" |
| 8871 | |
| 8872 | <p/>particle: id="9902210" name="p_diffr+" antiName="p_diffrbar-" spinType="0" chargeType="3" colType="0" |
| 8873 | m0="0.00000" |
| 8874 | |
| 8875 | <p/>particle: id="9910441" name="ccbar[3P0(8)]" spinType="1" chargeType="0" colType="2" |
| 8876 | m0="3.10000" mWidth="0.01000" mMin="3.10000" mMax="3.10000" |
| 8877 | <br/> channel: onMode="1" bRatio="1.0000000" products="443 21" |
| 8878 | |
| 8879 | <p/>particle: id="9910551" name="bbbar[3P0(8)]" spinType="1" chargeType="0" colType="2" |
| 8880 | m0="9.50000" mWidth="0.01000" mMin="9.50000" mMax="9.50000" |
| 8881 | <br/> channel: onMode="1" bRatio="1.0000000" products="553 21" |
| 8882 | |
| 8883 | <input type="hidden" name="saved" value="1"/> |
| 8884 | |
| 8885 | <?php |
| 8886 | echo "<input type='hidden' name='filepath' value='".$_GET["filepath"]."'/>"?> |
| 8887 | |
| 8888 | <table width="100%"><tr><td align="right"><input type="submit" value="Save Settings" /></td></tr></table> |
| 8889 | </form> |
| 8890 | |
| 8891 | <?php |
| 8892 | |
| 8893 | if($_POST["saved"] == 1) |
| 8894 | { |
| 8895 | $filepath = $_POST["filepath"]; |
| 8896 | $handle = fopen($filepath, 'a'); |
| 8897 | |
| 8898 | if($_POST["1"] != "4") |
| 8899 | { |
| 8900 | $data = "ParticleData:modeBreitWigner = ".$_POST["1"]."\n"; |
| 8901 | fwrite($handle,$data); |
| 8902 | } |
| 8903 | if($_POST["2"] != "2.5") |
| 8904 | { |
| 8905 | $data = "ParticleData:maxEnhanceBW = ".$_POST["2"]."\n"; |
| 8906 | fwrite($handle,$data); |
| 8907 | } |
| 8908 | if($_POST["3"] != "0.006") |
| 8909 | { |
| 8910 | $data = "ParticleData:mdRun = ".$_POST["3"]."\n"; |
| 8911 | fwrite($handle,$data); |
| 8912 | } |
| 8913 | if($_POST["4"] != "0.003") |
| 8914 | { |
| 8915 | $data = "ParticleData:muRun = ".$_POST["4"]."\n"; |
| 8916 | fwrite($handle,$data); |
| 8917 | } |
| 8918 | if($_POST["5"] != "0.095") |
| 8919 | { |
| 8920 | $data = "ParticleData:msRun = ".$_POST["5"]."\n"; |
| 8921 | fwrite($handle,$data); |
| 8922 | } |
| 8923 | if($_POST["6"] != "1.25") |
| 8924 | { |
| 8925 | $data = "ParticleData:mcRun = ".$_POST["6"]."\n"; |
| 8926 | fwrite($handle,$data); |
| 8927 | } |
| 8928 | if($_POST["7"] != "4.20") |
| 8929 | { |
| 8930 | $data = "ParticleData:mbRun = ".$_POST["7"]."\n"; |
| 8931 | fwrite($handle,$data); |
| 8932 | } |
| 8933 | if($_POST["8"] != "165.0") |
| 8934 | { |
| 8935 | $data = "ParticleData:mtRun = ".$_POST["8"]."\n"; |
| 8936 | fwrite($handle,$data); |
| 8937 | } |
| 8938 | if($_POST["9"] != "0.125") |
| 8939 | { |
| 8940 | $data = "ParticleData:alphaSvalueMRun = ".$_POST["9"]."\n"; |
| 8941 | fwrite($handle,$data); |
| 8942 | } |
| 8943 | fclose($handle); |
| 8944 | } |
| 8945 | |
| 8946 | ?> |
| 8947 | </body> |
| 8948 | </html> |
| 8949 | |
| 8950 | <!-- Copyright (C) 2012 Torbjorn Sjostrand --> |
git://git.uio.no / u / mrichter / AliRoot.git / blame