/usr/share/doc/pythia8-doc/html/SUSYProcesses.html is in pythia8-doc-html 8.1.86-1.2.
This file is owned by root:root, with mode 0o644.
The actual contents of the file can be viewed below.
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 214 215 216 217 218 219 220 221 222 223 224 225 226 227 228 229 230 231 232 233 234 235 236 237 238 239 240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 270 271 272 273 274 275 276 277 278 279 280 281 282 283 284 285 286 287 288 289 290 291 292 293 294 295 296 297 298 299 300 301 302 303 304 305 306 307 308 309 310 311 312 313 314 315 316 317 318 319 320 321 322 323 324 325 326 327 328 329 330 331 332 333 334 335 336 337 338 339 340 341 342 343 344 345 346 347 348 349 350 351 352 353 354 355 356 357 358 359 360 361 362 363 364 365 366 367 368 369 370 371 372 | <html>
<head>
<title>SUSY Processes</title>
<link rel="stylesheet" type="text/css" href="pythia.css"/>
<link rel="shortcut icon" href="pythia32.gif"/>
</head>
<body>
<h2>SUSY</h2>
<p>
Here is collected processes involving supersymmetric particle
production, with the exception of the (extended) Higgs sector.
Since the number of separate but closely related processes is so big,
there will not be switches for each separate process but only for a
reasonable set of subgroups. However, the general switches
<code>SUSY:idA</code> and <code>SUSY:idB</code>,valternatively
vectors <code>SUSY:idVecA</code> and <code>SUSY:idVecB</code>,
may be used in conjunction with any of these groups to provide
some additional flexibility to concentrate on processes involving
only specific (s)particle final states, see below.
</p>
<p>
Most of the SUSY implementation in PYTHIA 8 has been written by
N. Desai and is documented in [<a href="Bibliography.html" target="page">Des11</a>]. Please give due
credit to external contributions to PYTHIA 8, such as this one, by
including the original work in your list of references when using this
implementation. The cross section formulae are mostly taken from
[<a href="Bibliography.html" target="page">Boz07</a>] and [<a href="Bibliography.html" target="page">Fuk11</a>].
</p>
<p>Since the implementation of SUSY processes was only recently
completed [<a href="Bibliography.html" target="page">Des11</a>], case-by-case validations against other codes
are still recommended. A set of default validations have
already been carried out by the authors, comparing to
the PYTHIA 6 SUSY implementation and to the XSUSY code,
using an sps1a spectrum. Explicit
validations of the non-trivial SLHA2-specific extensions have
generally not been carried out yet, with the exception of the R-parity
violating single-sparticle production cross sections. Please report
the results of any user validations you may carry out to the authors.
</p>
<br/><b>Important Note on SLHA:</b>
In order to simulate SUSY processes it is required to read in the
couplings and masses relevant for the scenario to be studied. This
is done with the help of the SUSY Les Houches Accord (SLHA), including
the SLHA2 extensions and generalizations. (Internally, the SLHA2
conventions are used. SLHA1 spectra are automatically translated into
SLHA2 notation during initialization.) The
reading of a relevant SLHA file <b>must</b> be set up, as described
on <a href="SUSYLesHouchesAccord.html" target="page">the SLHA page</a>.
Attempting to generate SUSY processes without a properly initialized
SLHA spectrum is strongly discouraged and may lead to unexpected
results. Always check for warnings and errors reported by the SLHA
reader during the initialization stage.
<h3>SUSY Processes</h3>
<br/><b>Note 1:</b> Decays of SUSY particles are described
separately <a href="#decays">below</a>.
<br/><b>Note 2:</b> One special possibility is that the gluino or
some squark(s) are sufficiently long-lived to hadronize. See
<a href="RHadrons.html" target="page">the R-hadrons page</a> for further details.
<br/><b>Note 3:</b> lepton- and photon-initial states are not yet available.
Only quark/gluon-initiated <i>2 → 2</i> and <i>2 → 1</i> (RPV)
processes have been implemented.
<br/><b>Note 4:</b> cross sections will be correctly folded with open
branching fractions of cascade decays, but at present any difference between
particle and antiparticle decay tables is not taken into account. This
possibility will be included in a future update.
<p/><code>flag </code><strong> SUSY:all </strong>
(<code>default = <strong>off</strong></code>)<br/>
Common switch for production of supersymmetric particles, i.e.
particles with R-parity -1.
<p/><code>mode </code><strong> SUSY:idA </strong>
(<code>default = <strong>0</strong></code>; <code>minimum = 0</code>)<br/>
Option to limit the sum over possible outgoing states in SUSY
<i>2 → 2</i> processes to ones including a specific particle
identity code. The default corresponds to summing over all possible
indices. A non-zero value of <code>SUSY:idA</code> selects only processes
that contain the state corresponding to that particular particle identity
code in the fundamental <i>2 → 2</i> scattering process (summed
over particle/antiparticle). It is the user's responsibility to ensure
that (a subset of) the processes to be simulated actually include this
particle at the <i>2 → 2</i> level; thus, asking for the lightest
neutralino (code 1000021) to be present in a squark-squark production
process will give no match.
<p/><code>mode </code><strong> SUSY:idB </strong>
(<code>default = <strong>0</strong></code>; <code>minimum = 0</code>)<br/>
As for <code>SUSY:idA</code>, but requires an additional particle
with PDG code <code>SUSY:idB</code> to be present in the <i>2 → 2</i>
process. Thus, using <code>SUSY:idA</code> and <code>SUSY:idB</code>
a specific subprocess can be selected. Again only the absolute sign is
used, i.e. the summation over particle and antiparticle is retained.
Also the order of <code>SUSY:idA</code> and <code>SUSY:idB</code> is
irrelevant; since both possible orderings are checked for a match
with the two outgoing particles. (Although not recommended, should
<code>SUSY:idA</code> be zero and <code>SUSY:idB</code> nonzero
a match is searched for just like in the normal case with
<code>SUSY:idA</code> nonzero and <code>SUSY:idB</code> zero.)
<p/><code>mvec </code><strong> SUSY:idVecA </strong>
(<code>default = <strong>0</strong></code>; <code>minimum = 0</code>)<br/>
As for <code>SUSY:idA</code>, but as a vector of PDG codes.
(Character-string input of such vectors should be as a
comma-separated list, without any blanks.) Thus, it selects only
processes that have a final-state particle corresponding to one
of the identity codes in this vector. Note that, to activate this,
<code>SUSY:idA</code> must be equal to zero; if not then the match
to <code>SUSY:idA</code> takes precedence.
<p/><code>mvec </code><strong> SUSY:idVecB </strong>
(<code>default = <strong>0</strong></code>; <code>minimum = 0</code>)<br/>
As for <code>SUSY:idB</code>, but as a vector of PDG codes.
(Character-string input of such vectors should be as a
comma-separated list, without any blanks.) As above, to activate this,
<code>SUSY:idB</code> must be equal to zero; if not then the match to
<code>SUSY:idB</code> takes precedence. For the matching, either of
<code>SUSY:idA</code> and <code>SUSY:idVecA</code> may be combined with
either of <code>SUSY:idB</code> and <code>SUSY:idVecB</code>.
As above one of the two outgoing SUSY particles must match one of the
particles in <code>SUSY:id(Vec)A</code> and the other one of the
particles in <code>SUSY:id(Vec)B</code> when both are nonzero.
<p/><code>mode </code><strong> SUSY:sin2thetaWMode </strong>
(<code>default = <strong>2</strong></code>; <code>minimum = 1</code>; <code>maximum = 3</code>)<br/>
The value of <i>sin2(thetaW)</i> should be taken from
<br/><code>option </code><strong> 1</strong> : SM value, defined at <i>M_Z</i>, taken from
PYTHIA's <code>StandardModel:sin2thetaW</code> parameter.
<br/><code>option </code><strong> 2</strong> : SUSY value, defined at <i>M_SUSY</i>, derived from the
running gauge couplings in <code>BLOCK GAUGE</code> in the SLHA
file. Note: if no such block is present in the input file, this option
will default back to option 1 above, i.e., the SM value.
<br/><code>option </code><strong> 3</strong> : Pole value, defined by <i>1 - M_W^2/M_Z^2</i>,
using the pole masses stored in the SLHA <code>BLOCK MASS</code>, or,
alternatively, PYTHIA's internal pole masses if no such block is
present.
<h4>Gluino Pair Production</h4>
<p/><code>flag </code><strong> SUSY:gg2gluinogluino </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of gluinos by gluon-gluon initial states.
<p/><code>flag </code><strong> SUSY:qqbar2gluinogluino </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of gluinos by quark-antiquark annihilation and
<i>t</i>-channel squark exchange. The cross section
expression follows [<a href="Bibliography.html" target="page">Fuk11</a>] and include the possibility
of non-minimal flavour violation through misalignment of quarks with
squarks. Only the MFV case has been explicitly validated.
<h4>Associated Squark-Gluino Production</h4>
<p/><code>flag </code><strong> SUSY:qg2squarkgluino </strong>
(<code>default = <strong>off</strong></code>)<br/>
Associated production of a squark with a gluino. The cross section
expression follows [<a href="Bibliography.html" target="page">Fuk11</a>] and include the possibility
of non-minimal flavour violation through misalignment of quarks with
squarks. Only the MFV case has been explicitly validated.
<h4>Squark Pair Production</h4>
<p/><code>flag </code><strong> SUSY:gg2squarkantisquark </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of a scalar quark together with a scalar antiquark by
gluon annihilation via <i>s</i>-channel gluon exchange, <i>t</i>- and
<i>u</i>-channel squark exchange, and the direct 4-point coupling.
The cross section expression follows [<a href="Bibliography.html" target="page">Boz07</a>].
Only the MFV case has been explicitly validated.
<p/><code>flag </code><strong> SUSY:qqbar2squarkantisquark </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of a scalar quark together with a scalar antiquark
by quark-antiquark annihilation.
For same-isospin <i>~q~q*</i> production (i.e., <i>~u~u*</i>,
<i>~u~c*</i>, ...), the <i>s</i>-channel gluon, photon, and
<i>Z</i> and <i>t</i>-channel gluino contributions have so far
been implemented (i.e., the <i>t</i>-channel neutralino contributions
are neglected). For opposite-isospin <i>~q~q*</i> production
(<i>~u~d*</i>, <i>~u~s*</i>, ...), the <i>s</i>-channel <i>W</i>
and <i>t</i>-channel gluino contributions have been implemented
(i.e., the <i>t</i>-channel neutralino contributions are neglected).
The cross section expressions follow [<a href="Bibliography.html" target="page">Boz07</a>].
Only the MFV case has been explicitly validated.
(Note to PYTHIA 6 users:
in older PYTHIA 6 versions, a bug caused the <i>~t1~t2*</i> cross to be
overcounted by a factor of 2. Starting from version 6.4.24, that
generator now agrees with the implementation here.)
<p/><code>flag </code><strong> SUSY:qqbar2squarkantisquark:onlyQCD </strong>
(<code>default = <strong>off</strong></code>)<br/>
When switched <code>on</code> this flag switches off all but the
<i>s</i>-channel gluon contribution in the
calculation of same-isospin squark-antisquark production cross
sections. Intended for reference only. For the most
accurate physics simulation, leave this flag in the <code>off</code>
position.
<p/><code>flag </code><strong> SUSY:qq2squarksquark </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of scalar quarks (squark-squark and its charge
conjugate process; for squark-antisquark production see above)
by <i>t</i>- and <i>u</i>-channel gluino, neutralino, and
chargino exchange. The cross section expressions follow [<a href="Bibliography.html" target="page">Boz07</a>].
Only the MFV case has been explicitly validated.
(Note to PYTHIA 6 users: PYTHIA 6 only included the gluino exchange
contribution, which typically dominates due to the size of the strong
coupling; for counterchecks,
the flag <code>SUSY:qq2squarksquark:onlyQCD</code>
below can be switched on to eliminate the chargino and neutralino
contributions.)
<p/><code>flag </code><strong> SUSY:qq2squarksquark:onlyQCD </strong>
(<code>default = <strong>off</strong></code>)<br/>
When switched <code>on</code> this flag causes the <i>t</i>- or
<i>u</i>-channel neutralino and chargino contributions to be
ignored in the calculation of squark pair production cross sections.
Intended for reference only. For the most accurate physics simulation,
leave this flag in the <code>off</code> position.
<h4>Neutralino and Chargino Pair Production</h4>
<p/><code>flag </code><strong> SUSY:qqbar2chi0chi0 </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of neutralinos by quark-antiquark annihilation. With
four neutralino species this gives ten separate processes, codes
1201 - 1210. The cross section expressions follow [<a href="Bibliography.html" target="page">Boz07</a>].
Only the MFV case has been explicitly validated.
<p/><code>flag </code><strong> SUSY:qqbar2chi+-chi0 </strong>
(<code>default = <strong>off</strong></code>)<br/>
Associated chargino-neutralino production by quark-antiquark
annihilation. With four neutralino species, two chargino ones, and
maintaining charge conjugate processes separate, this gives 16
separate processes, codes 1221 - 1236. The cross section expressions
follow [<a href="Bibliography.html" target="page">Boz07</a>].
Only the MFV case has been explicitly validated.
<p/><code>flag </code><strong> SUSY:qqbar2chi+chi- </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of charginos by quark-antiquark annihilation. With
two chargino species and maintaining mutually charge conjugate
processes separate, this gives four separate processes, codes
1241 - 1244. The cross section expressions follow [<a href="Bibliography.html" target="page">Boz07</a>].
Only the MFV case has been explicitly validated.
<h4>Associated Neutralino/Chargino + Squark/Gluino Production</h4>
<p/><code>flag </code><strong> SUSY:qg2chi0squark </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of neutralinos from quark-gluon initial states.
The cross section expressions follow [<a href="Bibliography.html" target="page">Boz07</a>].
Only the MFV case has been explicitly validated.
<p/><code>flag </code><strong> SUSY:qg2chi+-squark </strong>
(<code>default = <strong>off</strong></code>)<br/>
Associated chargino-squark production from quark-gluon initial states.
annihilation. The cross section expressions
follow [<a href="Bibliography.html" target="page">Boz07</a>].
Only the MFV case has been explicitly validated.
<p/><code>flag </code><strong> SUSY:qqbar2chi0gluino </strong>
(<code>default = <strong>off</strong></code>)<br/>
Associated neutralino-gluino production by quark-antiquark
annihilation.
The cross section expressions follow
[<a href="Bibliography.html" target="page">Fuk11</a>]. Only the MFV case has been explicitly validated.
<p/><code>flag </code><strong> SUSY:qqbar2chi+-gluino </strong>
(<code>default = <strong>off</strong></code>)<br/>
Associated chargino-gluino production by quark-antiquark
annihilation. The cross section expressions follow
[<a href="Bibliography.html" target="page">Fuk11</a>]. Only the MFV case has been explicitly
validated. (Note to PYTHIA 6 users: small differences between
this implementation and PYTHIA 6 arise due
to slightly different treatments of the weak mixing angle,
which is fixed in PYTHIA 6, while it is computed from the SLHA input
in PYTHIA 8; see <code>SUSY:sin2thetaWMode</code> above.)
<h4>Slepton Production</h4>
<p/><code>flag </code><strong> SUSY:qqbar2sleptonantislepton </strong>
(<code>default = <strong>off</strong></code>)<br/>
Pair production of slepton-antislepton via s-channel W, Z and gamma
exchange. Includes both charged sleptons and sneutrinos but right
handed sneutrinos currently not supported.
<h4>R-parity violating squark production</h4>
<p/><code>flag </code><strong> SUSY:qq2antisquark </strong>
(<code>default = <strong>off</strong></code>)<br/>
Resonant squark production via R-parity violating UDD couplings. The
couplings must be input using the SLHA2 structure.
<a name="decays"></a>
<h3>Decays of SUSY Particles</h3>
Based on the parameters read in from the SLHA, PYTHIA 8 will normally
compute the decay modes of SUSY particles automatically, using the
<code>SusyResonanceDecays</code> class(es). Essentially all tree-level
2-body decays in the MSSM
have been implemented this way, excepting so far only those involving
Higgs bosons (either in the in- or out-state) or gravitinos.
Available channels so far include:
<ul>
<li>~q → q + ~chi</li>
<li>~q → ~q + W/Z</li>
<li>~q → q + q (RPV UDD)</li>
<li>~q → l + q (RPV LQD)</li>
<li>~g → ~q + q</li>
<li>~chi → ~chi + Z/W</li>
<li>~chi → ~q + q</li>
<li>~chi → ~l/~nu + l/nu</li>
<li>~chi0 → q + q + q (RPV UDD)</li>
<li>~l/~nu → l/nu + ~chi</li>
<li>~l/~nu → ~l/~nu + W/Z</li>
</ul>
All channels are still undergoing validation, so this
implementation should be considered preliminary.
Still missing but to be included in a forthcoming update
are: 3-body decays of charginos (via RPV), and 2-body decays of squarks and
gauginos with Higgs as one of the decay products.
Some 3-body decays have been implemented with Matrix Element weighting.
In particular, those for a neutralino to a lighter neutralino and a
fermion pair can be enabled.
<p/><code>flag </code><strong> SUSYResonance:3BodyMatrixElement </strong>
(<code>default = <strong>off</strong></code>)<br/>
When "on", the spin-averaged, squared matrix element is used
to sample the phase space for resonance decay. Currently, only
possible for a heavy neutralino decay to a light neutralino
and a fermion-antifermion pair.
</body>
</html>
<!-- Copyright (C) 2014 Torbjorn Sjostrand -->
|