3 <title>Particle Data</title>
4 <link rel="stylesheet" type="text/css" href="pythia.css"/>
5 <link rel="shortcut icon" href="pythia32.gif"/>
11 The structure and operation of the particle data table is described
12 <a href="ParticleDataScheme.html" target="page">here</a>. That page
13 also describes how default data properties can be changed. The
14 current page provides the actual default values.
16 <h3>Main settings</h3>
18 Apart from the data itself, the particle data table only contains
19 a few aspects that are available to change:
21 <p/><code>mode </code><strong> ParticleData:modeBreitWigner </strong>
22 (<code>default = <strong>4</strong></code>; <code>minimum = 0</code>; <code>maximum = 4</code>)<br/>
23 Selection of particle masses when the <code>mass(id)</code> is called
24 to provide a new mass:
25 <br/><code>option </code><strong> 0</strong> :
26 mass is fixed at the nominal <i>m_0</i> value.
28 <br/><code>option </code><strong> 1</strong> :
29 particles registered as having a mass width are given a mass
30 in the range <i>m_min < m < m_max</i>, according
31 to a truncated nonrelativistic Breit-Wigner, i.e. linear in <i>m</i>.
33 <br/><code>option </code><strong> 2</strong> :
34 as above, except that the width is made mass-dependent:
35 <i>Gamma = Gamma_0 * sqrt( (m^2 - m_thr^2) / (m_0^2 - m_thr^2) )</i>
36 where <i>m</i> is the current mass, <i>m_0</i> the nominal one and
37 <i>m_thr</i> is the mass threshold, given by the sum of the nominal
38 masses of the decay products. In order to decouple production and decay
39 the threshold is defined as the branching-ratio-weighted average over
40 all allowed decay channels.
42 <br/><code>option </code><strong> 3</strong> :
43 particles registered as having a mass width are given a mass
44 in the range <i>m_min < m < m_max</i>, according
45 to a truncated relativistic Breit-Wigner, i.e. quadratic in <i>m</i>.
47 <br/><code>option </code><strong> 4</strong> :
48 as 3, but the width is modified as for 2, and the current mass is used
49 for its phase-space prefactor, i.e. <i>m_0 Gamma_0 -> m Gamma(m)</i>.
51 <br/><b>Note:</b> this mode only applies to normal hadronic
52 resonances like the <i>rho</i>. The more massive states of the
53 <code>isResonance()</code> type, like <i>Z^0</i> or top, are
54 considered separately.
57 <p/><code>parm </code><strong> ParticleData:maxEnhanceBW </strong>
58 (<code>default = <strong>2.5</strong></code>; <code>minimum = 1.</code>; <code>maximum = 5.</code>)<br/>
59 The modifications in options 2 and 4 above enhance the large-mass tail
60 of the Breit-Wigners (the mass spectrum develops a dm/m divergence).
61 However, we expect form factors to dampen this tail at masses some distance
62 above the nominal one, so cut off the rise by requiring the actual
63 Breit-Wigner weight not to be more than a factor <code> maxEnhanceBW</code>
64 above the one obtained with options 1 or 3, respectively. This also
65 opens up for a simpler technical handling of mass selection in options
66 2 and 4, by using standard hit-and-miss Monte Carlo.
70 Since running masses are only calculated for the six quark flavours,
71 e.g. to obtain couplings to the Higgs boson(s), there is not an entry
72 in the normal tables for each particles, but only the six MSbar mass
73 values below, used as starting point for the running. In addition you
74 can pick an <i>alpha_s(M_Z)</i>, which is converted into a first-order
75 five-flavour Lambda that is used to determine the rate of the running.
76 (Without any match to four flavours below <i>m_b</i>; if desired, this
77 can be fixed by slightly shifted default mass values, since the routines
78 never should be called below the <i>m_b</i> scale anyway.)
80 <p/><code>parm </code><strong> ParticleData:mdRun </strong>
81 (<code>default = <strong>0.006</strong></code>; <code>minimum = 0.003</code>; <code>maximum = 0.008</code>)<br/>
82 the d quark MSbar mass at 2 GeV scale.
85 <p/><code>parm </code><strong> ParticleData:muRun </strong>
86 (<code>default = <strong>0.003</strong></code>; <code>minimum = 0.001</code>; <code>maximum = 0.006</code>)<br/>
87 the u quark MSbar mass at 2 GeV scale.
90 <p/><code>parm </code><strong> ParticleData:msRun </strong>
91 (<code>default = <strong>0.095</strong></code>; <code>minimum = 0.060</code>; <code>maximum = 0.150</code>)<br/>
93 the s quark MSbar mass at 2 GeV scale.
95 <p/><code>parm </code><strong> ParticleData:mcRun </strong>
96 (<code>default = <strong>1.25</strong></code>; <code>minimum = 1.00</code>; <code>maximum = 1.50</code>)<br/>
98 the c quark MSbar mass at the mass scale itself.
100 <p/><code>parm </code><strong> ParticleData:mbRun </strong>
101 (<code>default = <strong>4.20</strong></code>; <code>minimum = 4.00</code>; <code>maximum = 4.50</code>)<br/>
102 the b quark MSbar mass at the mass scale itself.
105 <p/><code>parm </code><strong> ParticleData:mtRun </strong>
106 (<code>default = <strong>165.0</strong></code>; <code>minimum = 150.0</code>; <code>maximum = 175.0</code>)<br/>
107 the t quark MSbar mass at the mass scale itself.
110 <p/><code>parm </code><strong> ParticleData:alphaSvalueMRun </strong>
111 (<code>default = <strong>0.125</strong></code>; <code>minimum = 0.10</code>; <code>maximum = 0.20</code>)<br/>
112 the <i>alpha_s(M_Z)</i> value used to define tha rate at which MSbar
117 <h3>Comments on the data</h3>
119 The starting point for the current data is the 2006 Review of Particle
120 Physics [<a href="Bibliography.html" target="page">Yao06</a>]. All known particle masses, widths and lifetimes
121 have been set accordingly, while not-yet-measured particles are kept at
122 their values from PYTHIA 6. Decay channels and their branching
123 ratios remain a major worry: many particles do not have one single solidly
124 measured branching ratio, and many further do not have known branching
125 ratios that add up to (the neighbourhood of) unity.
128 Uncertainties are especially big for the scalar, pseudovector and tensor
129 <i>L = 1</i> multiplets available in PYTHIA. We note that
130 some distributions become better described when these multiplets are
131 included in the generation, while others become worse. It is tempting to
132 associate this lackluster performance with the primitive knowledge.
133 Not even the multiplets themselves are particularly well known.
134 It used to be that the <i>a_0(980)</i> and <i>f_0(980)</i>
135 were considered to be members of the scalar multiplet. Nowadays they are
136 commonly assumed to be either four-quark states or of some other exotic
137 character. This means that the PYTHIA 8 PDG particle codes
138 have been changed for these particles, relative to what was used in
139 PYTHIA 6 based on previous PDG editions. Specifically their
140 numbers are now in the 9000000 series, and they have been replaced in the
141 scalar multiplet by <i>a_0(1450)</i> and <i>f_0(1370)</i>.
144 For charm and bottom mesons the jungle of partial measurements makes
145 it very difficult to construct fully consistent sets of decay channels.
146 This part of the program has not yet been brought up to date to the
147 2006 RPP. Instead the LHCb decay tables (for EvtGen, but without
148 using the EvtGen matrix-element machinery) and the DELPHI tune for
149 PYTHIA 6 is being used. (This also includes a few non-c/b
150 hadrons that only occur in the c/b decay tables.) This has the
151 advantage that many tests have been made for consistency, but the
152 disadvantage that it is not always in agreement with the latest
153 measurements of some specific decay channels. The decays based
154 on the LHCb tables (with some modifications) are 411, 421, 431, 441,
155 445, 511, 521, 531, 541, 3124, 4122, 4124, 5122, 10441, 10443, 13122,
156 14122, 20443, 23122, 30313, 30323, 30443, 33122, 100113, 100213, 100441,
157 100443, 100553, 9000111, 9000211. Correspondingly the decays based on
158 the DELPHI tables are 415, 425, 435, 515, 525, 535, 4132, 4232, 4332,
161 <h3>The data itself</h3>
163 Here comes the default particle data used in the program. Do not touch.
164 The meaning of the various properties and the format used are explained
165 <a href="ParticleDataScheme.html" target="page">here</a> and the
166 <code>meMode</code> codes <a href="ParticleDecays.html" target="page">here</a>.
168 <p/>particle: id="0" name="void" spinType="0" chargeType="0" colType="0" m0="0.0">
170 <p/>particle: id="1" name="d" antiName="dbar" spinType="2" chargeType="-1" colType="1"
173 <p/>particle: id="2" name="u" antiName="ubar" spinType="2" chargeType="2" colType="1"
176 <p/>particle: id="3" name="s" antiName="sbar" spinType="2" chargeType="-1" colType="1"
179 <p/>particle: id="4" name="c" antiName="cbar" spinType="2" chargeType="2" colType="1"
182 <p/>particle: id="5" name="b" antiName="bbar" spinType="2" chargeType="-1" colType="1"
185 <p/>particle: id="6" name="t" antiName="tbar" spinType="2" chargeType="2" colType="1"
186 m0="171.00000" mWidth="1.40000" mMin="86.00000" mMax="0.00000"
187 <br/> channel: onMode="1" bRatio="0.0000300" products="24 1"
188 <br/> channel: onMode="1" bRatio="0.0017650" products="24 3"
189 <br/> channel: onMode="1" bRatio="0.9982050" products="24 5"
190 <br/> channel: onMode="0" bRatio="0.0000000" products="37 5"
192 <p/>particle: id="7" name="b'" antiName="b'bar" spinType="2" chargeType="-1" colType="1"
194 <br/> channel: onMode="1" bRatio="0.0000000" products="-24 2"
195 <br/> channel: onMode="1" bRatio="0.0000000" products="-24 4"
196 <br/> channel: onMode="1" bRatio="0.0000000" products="-24 6"
197 <br/> channel: onMode="1" bRatio="1.0000000" products="-24 8"
199 <p/>particle: id="8" name="t'" antiName="t'bar" spinType="2" chargeType="2" colType="1"
201 <br/> channel: onMode="1" bRatio="0.0000000" products="24 1"
202 <br/> channel: onMode="1" bRatio="0.0000000" products="24 3"
203 <br/> channel: onMode="1" bRatio="0.0000000" products="24 5"
204 <br/> channel: onMode="1" bRatio="1.0000000" products="24 7"
206 <p/>particle: id="11" name="e-" antiName="e+" spinType="2" chargeType="-3" colType="0"
209 <p/>particle: id="12" name="nu_e" antiName="nu_ebar" spinType="2" chargeType="0" colType="0"
212 <p/>particle: id="13" name="mu-" antiName="mu+" spinType="2" chargeType="-3" colType="0"
213 m0="0.10566" tau0="6.58654e+05"
214 <br/> channel: onMode="1" bRatio="1.0000000" meMode="22" products="-12 11 14"
216 <p/>particle: id="14" name="nu_mu" antiName="nu_mubar" spinType="2" chargeType="0" colType="0"
219 <p/>particle: id="15" name="tau-" antiName="tau+" spinType="2" chargeType="-3" colType="0"
220 m0="1.77682" tau0="8.71100e-02"
221 <br/> channel: onMode="1" bRatio="0.108924" meMode="1521" products="16 -211"
222 <br/> channel: onMode="1" bRatio="0.006885" meMode="1521" products="16 -321"
223 <br/> channel: onMode="1" bRatio="0.178345" meMode="1531" products="16 11 -12"
224 <br/> channel: onMode="1" bRatio="0.173545" meMode="1531" products="16 13 -14"
225 <br/> channel: onMode="1" bRatio="0.254890" meMode="1532" products="16 111 -211"
226 <br/> channel: onMode="1" bRatio="0.001513" meMode="1532" products="16 311 -321"
227 <br/> channel: onMode="1" bRatio="0.000263" meMode="1532" products="16 221 -321"
228 <br/> channel: onMode="1" bRatio="0.008957" meMode="1533" products="16 -211 -311"
229 <br/> channel: onMode="1" bRatio="0.004491" meMode="1533" products="16 111 -321"
230 <br/> channel: onMode="1" bRatio="0.092370" meMode="1541" products="16 111 111 -211"
231 <br/> channel: onMode="1" bRatio="0.089813" meMode="1541" products="16 -211 -211 211"
232 <br/> channel: onMode="1" bRatio="0.003757" meMode="1542" products="16 111 -211 -311"
233 <br/> channel: onMode="1" bRatio="0.003292" meMode="1542" products="16 -211 211 -321"
234 <br/> channel: onMode="1" bRatio="0.001519" meMode="1542" products="16 -211 -321 321"
235 <br/> channel: onMode="1" bRatio="0.001518" meMode="1542" products="16 111 311 -321"
236 <br/> channel: onMode="1" bRatio="0.001087" meMode="1542" products="16 130 -211 310"
237 <br/> channel: onMode="1" bRatio="0.000555" meMode="1542" products="16 111 111 -321"
238 <br/> channel: onMode="1" bRatio="0.000235" meMode="1542" products="16 130 130 -211"
239 <br/> channel: onMode="1" bRatio="0.000235" meMode="1542" products="16 -211 310 310"
240 <br/> channel: onMode="1" bRatio="0.001744" meMode="1543" products="16 111 -211 221"
241 <br/> channel: onMode="1" bRatio="0.001762" meMode="1544" products="16 22 111 -211"
242 <br/> channel: onMode="1" bRatio="0.044435" meMode="1551" products="16 111 -211 -211 211"
243 <br/> channel: onMode="1" bRatio="0.010313" meMode="1551" products="16 111 111 111 -211"
244 <br/> channel: onMode="1" bRatio="0.004935" meMode="1561" products="16 111 111 -211 -211 211"
245 <br/> channel: onMode="1" bRatio="0.000957" meMode="1561" products="16 111 111 111 111 -211"
246 <br/> channel: onMode="1" bRatio="0.000834" meMode="1561" products="16 -211 -211 -211 211 211"
247 <br/> channel: onMode="1" bRatio="0.000225" meMode="0" products="16 -211 -211 211 221"
248 <br/> channel: onMode="1" bRatio="0.000145" meMode="0" products="16 111 111 -211 221"
249 <br/> channel: onMode="1" bRatio="0.000135" meMode="0" products="16 111 111 -211 223"
250 <br/> channel: onMode="1" bRatio="0.000118" meMode="0" products="16 -211 -211 211 223"
251 <br/> channel: onMode="1" bRatio="0.000400" meMode="0" products="16 223 -321"
252 <br/> channel: onMode="1" bRatio="0.000397" meMode="0" products="16 111 111 111 -321"
253 <br/> channel: onMode="1" bRatio="0.000307" meMode="0" products="16 111 -211 211 -321"
254 <br/> channel: onMode="1" bRatio="0.000280" meMode="0" products="16 221 -323"
255 <br/> channel: onMode="1" bRatio="0.000238" meMode="0" products="16 111 111 -211 -311"
256 <br/> channel: onMode="1" bRatio="0.000225" meMode="0" products="16 -211 -211 211 -311"
257 <br/> channel: onMode="1" bRatio="0.000297" meMode="0" products="16 111 -211 -311 311"
258 <br/> channel: onMode="1" bRatio="0.000059" meMode="0" products="16 111 -211 -321 321"
260 <p/>particle: id="16" name="nu_tau" antiName="nu_taubar" spinType="2" chargeType="0" colType="0"
263 <p/>particle: id="17" name="tau'-" antiName="tau'+" spinType="2" chargeType="-3" colType="0"
265 <br/> channel: onMode="1" bRatio="1.0000000" products="-24 18"
267 <p/>particle: id="18" name="nu'_tau" antiName="nu'_taubar" spinType="2" chargeType="0" colType="0"
269 <br/> channel: onMode="1" bRatio="1.0000000" products="24 17"
271 <p/>particle: id="21" name="g" spinType="3" chargeType="0" colType="2"
274 <p/>particle: id="22" name="gamma" spinType="3" chargeType="0" colType="0"
277 <p/>particle: id="23" name="Z0" spinType="3" chargeType="0" colType="0"
278 m0="91.18760" mWidth="2.49520" mMin="10.00000" mMax="0.00000"
279 <br/> channel: onMode="1" bRatio="0.1539950" products="1 -1"
280 <br/> channel: onMode="1" bRatio="0.1194200" products="2 -2"
281 <br/> channel: onMode="1" bRatio="0.1539840" products="3 -3"
282 <br/> channel: onMode="1" bRatio="0.1192590" products="4 -4"
283 <br/> channel: onMode="1" bRatio="0.1522720" products="5 -5"
284 <br/> channel: onMode="1" bRatio="0.0335760" products="11 -11"
285 <br/> channel: onMode="1" bRatio="0.0668060" products="12 -12"
286 <br/> channel: onMode="1" bRatio="0.0335760" products="13 -13"
287 <br/> channel: onMode="1" bRatio="0.0668060" products="14 -14"
288 <br/> channel: onMode="1" bRatio="0.0335000" products="15 -15"
289 <br/> channel: onMode="1" bRatio="0.0668060" products="16 -16"
291 <p/>particle: id="24" name="W+" antiName="W-" spinType="3" chargeType="3" colType="0"
292 m0="80.38500" mWidth="2.08500" mMin="10.00000" mMax="0.00000"
293 <br/> channel: onMode="1" bRatio="0.3213690" products="-1 2"
294 <br/> channel: onMode="1" bRatio="0.0164940" products="-1 4"
295 <br/> channel: onMode="1" bRatio="0.0165020" products="-3 2"
296 <br/> channel: onMode="1" bRatio="0.3206150" products="-3 4"
297 <br/> channel: onMode="1" bRatio="0.0000100" products="-5 2"
298 <br/> channel: onMode="1" bRatio="0.0005910" products="-5 4"
299 <br/> channel: onMode="1" bRatio="0.1081660" products="-11 12"
300 <br/> channel: onMode="1" bRatio="0.1081660" products="-13 14"
301 <br/> channel: onMode="1" bRatio="0.1080870" products="-15 16"
303 <p/>particle: id="25" name="h0(H_1)" spinType="1" chargeType="0" colType="0"
304 m0="125.00000" mWidth="0.00374" mMin="50.00000" mMax="0.00000"
305 <br/> channel: onMode="1" bRatio="0.0000009" products="1 -1"
306 <br/> channel: onMode="1" bRatio="0.0000002" products="2 -2"
307 <br/> channel: onMode="1" bRatio="0.0002361" products="3 -3"
308 <br/> channel: onMode="1" bRatio="0.0335602" products="4 -4"
309 <br/> channel: onMode="1" bRatio="0.5876728" products="5 -5"
310 <br/> channel: onMode="1" bRatio="0.0000000" products="6 -6"
311 <br/> channel: onMode="1" bRatio="0.0000000" products="11 -11"
312 <br/> channel: onMode="1" bRatio="0.0002445" products="13 -13"
313 <br/> channel: onMode="1" bRatio="0.0690800" products="15 -15"
314 <br/> channel: onMode="1" bRatio="0.0630585" products="21 21"
315 <br/> channel: onMode="1" bRatio="0.0028438" products="22 22"
316 <br/> channel: onMode="1" bRatio="0.0017601" products="22 23"
317 <br/> channel: onMode="1" bRatio="0.0259708" products="23 23"
318 <br/> channel: onMode="1" bRatio="0.2155720" products="24 -24"
319 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000022 1000022"
320 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000023 1000022"
321 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000023 1000023"
322 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000025 1000022"
323 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000025 1000023"
324 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000025 1000025"
325 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000035 1000022"
326 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000035 1000023"
327 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000035 1000025"
328 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000035 1000035"
329 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000024 -1000024"
330 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000024 -1000037"
331 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000037 -1000024"
332 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000037 -1000037"
333 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000001 -1000001"
334 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000001 -2000001"
335 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000001 -2000001"
336 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000001 2000001"
337 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000002 -1000002"
338 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000002 -2000002"
339 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000002 -2000002"
340 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000002 2000002"
341 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000003 -1000003"
342 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000003 -2000003"
343 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000003 -2000003"
344 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000003 2000003"
345 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000004 -1000004"
346 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000004 -2000004"
347 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000004 -2000004"
348 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000004 2000004"
349 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000005 -1000005"
350 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000005 -2000005"
351 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000005 -2000005"
352 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000005 2000005"
353 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000006 -1000006"
354 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000006 -2000006"
355 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000006 -2000006"
356 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000006 2000006"
357 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000011 -1000011"
358 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000011 -2000011"
359 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000011 -2000011"
360 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000011 2000011"
361 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000012 -1000012"
362 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000012 -2000012"
363 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000012 -2000012"
364 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000012 2000012"
365 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000013 -1000013"
366 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000013 -2000013"
367 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000013 -2000013"
368 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000013 2000013"
369 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000014 -1000014"
370 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000014 -2000014"
371 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000014 -2000014"
372 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="-1000014 2000014"
373 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="1000015 -1000015"
374 <br/> channel: onMode="1" bRatio="0.0000000" meMode="103" products="2000015 -2000015"
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8892 <!-- Copyright (C) 2012 Torbjorn Sjostrand -->