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first import of structure, PYTHIA8 and DELPHES
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1	<html>
2	<head>
3	<title>Flavour Selection</title>
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8
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27
28	<form method='post' action='FlavourSelection.php'>
29
30	<h2>Flavour Selection</h2>
31
32	The <code>StringFlav</code> class handles the choice of a new flavour
33	in the fragmentation process, and the production of a new hadron
34	from a set of input flavours. It is mainly used by the string
35	fragmentation machinery (including ministrings), but also e.g.
36	in some particle decays and for some beam-remnant cases. The basic
37	concepts are in agreement with [<a href="Bibliography.php" target="page">And83</a>]. The baryon-sector
38	implementation is based on the <code>MSTJ(12)=3</code> option of
39	PYTHIA 6, i.e. new SU(6) weights scheme with at most one popcorn meson.
40
41	<p/>
42	The relative production rates of different particle species is
43	influenced by the parameters below. Some have only an impact on
44	one specific quantity, but most directly or indirectly have
45	consequences for many observables. Therefore the values to use have
46	to be viewed in the context of a complete <?php $filepath = $_GET["filepath"];
47	echo "<a href='Tunes.php?filepath=".$filepath."' target='page'>";?>tune</a>.
48
49	<h3>New flavours</h3>
50
51	The main parameters of the selection of a new flavour are
52
53	<br/><br/><table><tr><td><strong>StringFlav:probStoUD </td><td></td><td> <input type="text" name="1" value="0.19" size="20"/>   (<code>default = <strong>0.19</strong></code>; <code>minimum = 0.0</code>; <code>maximum = 1.0</code>)</td></tr></table>
54	the suppression of <i>s</i> quark production relative to ordinary
55	<i>u</i> or <i>d</i> one.
56
57
58	<br/><br/><table><tr><td><strong>StringFlav:probQQtoQ </td><td></td><td> <input type="text" name="2" value="0.09" size="20"/>   (<code>default = <strong>0.09</strong></code>; <code>minimum = 0.0</code>; <code>maximum = 1.0</code>)</td></tr></table>
59	the suppression of diquark production relative to quark production,
60	i.e. of baryon relative to meson production.
61
62
63	<br/><br/><table><tr><td><strong>StringFlav:probSQtoQQ </td><td></td><td> <input type="text" name="3" value="1.00" size="20"/>   (<code>default = <strong>1.00</strong></code>; <code>minimum = 0.0</code>; <code>maximum = 1.0</code>)</td></tr></table>
64	the suppression of strange diquark production relative to light
65	diquark production, over and above the one already given by
66	<code>probStoU</code>.
67
68
69	<br/><br/><table><tr><td><strong>StringFlav:probQQ1toQQ0 </td><td></td><td> <input type="text" name="4" value="0.027" size="20"/>   (<code>default = <strong>0.027</strong></code>; <code>minimum = 0.0</code>; <code>maximum = 1.0</code>)</td></tr></table>
70	the suppression of spin 1 diquark production relative to spin 0 one,
71	apart from the factor of 3 enhancement of spin 1 from counting the
72	number of states.
73
74
75	<h3>Standard-meson production</h3>
76
77	The bulk of the particle production corresponds to the lowest-lying
78	pseudoscalar and vector multiplets. Their production rates are
79	determined by the parameters in this section.
80
81	<p/>
82	For a given set of flavours, produced according to the probabilities
83	outlined above, the ratio of vector-to-pseudocalar meson production
84	is described by the parameters below.
85	The maximum allowed rate for each case has been set according to
86	spin-counting rules, but we expect the real rates to be lower,
87	especially for lighter mesons, owing to the vector-pseudoscalar
88	mass splitting.
89
90	<br/><br/><table><tr><td><strong>StringFlav:mesonUDvector </td><td></td><td> <input type="text" name="5" value="0.62" size="20"/>   (<code>default = <strong>0.62</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
91	the relative production ratio vector/pseudoscalar for light
92	(<i>u</i>, <i>d</i>) mesons.
93
94	<br/><br/><table><tr><td><strong>StringFlav:mesonSvector </td><td></td><td> <input type="text" name="6" value="0.725" size="20"/>   (<code>default = <strong>0.725</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
95	the relative production ratio vector/pseudoscalar for strange mesons.
96
97	<br/><br/><table><tr><td><strong>StringFlav:mesonCvector </td><td></td><td> <input type="text" name="7" value="1.06" size="20"/>   (<code>default = <strong>1.06</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
98	the relative production ratio vector/pseudoscalar for charm mesons.
99
100	<br/><br/><table><tr><td><strong>StringFlav:mesonBvector </td><td></td><td> <input type="text" name="8" value="3.0" size="20"/>   (<code>default = <strong>3.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
101	the relative production ratio vector/pseudoscalar for bottom mesons.
102
103
104	<p/>
105	Inside each light-quark meson nonet, an octet-singlet mixing angle
106	describes the mixing of the two flavour-diagonal isoscalar = 0 states.
107	(For terminology and details see [<a href="Bibliography.php" target="page">Yao06</a>], chapter 14 on the
108	quark model.)
109	This angle is needed to specify the probability for such a <i>q qbar</i>
110	state to project onto a specific meson. More transparent formuale are
111	obtained by introducing the angle <i>alpha = theta + 54.7</i> degrees:
112	<br/><i>
113	f = (uubar + ddbar)/sqrt(2) * sin(alpha) + ssbar * cos(alpha)<br/>
114	f' = (uubar + ddbar)/sqrt(2) * cos(alpha) - ssbar * sin(alpha)
115	</i><br/>
116
117	<br/><br/><table><tr><td><strong>StringFlav:thetaPS </td><td></td><td> <input type="text" name="9" value="-15." size="20"/>   (<code>default = <strong>-15.</strong></code>; <code>minimum = -90.</code>; <code>maximum = 90.</code>)</td></tr></table>
118	gives the mixing angle <i>theta_PS</i> in the pseudoscalar meson sector
119	(which is rather poorly determined), expressed in degrees.
120	Here <i>f</i> is associated with <i>eta'</i> and <i>f'</i> with
121	<i>eta</i>. (This standard but counterintuitive choice is fixed up
122	in the code by replacing <i>alpha -> 90^0 - alpha</i> so that
123	<i>eta <-> eta'</i>; relative signs do not matter since we are
124	interested in probabilities only.)
125
126
127	<br/><br/><table><tr><td><strong>StringFlav:thetaV </td><td></td><td> <input type="text" name="10" value="36." size="20"/>   (<code>default = <strong>36.</strong></code>; <code>minimum = -90.</code>; <code>maximum = 90.</code>)</td></tr></table>
128	gives the mixing angle <i>theta_V</i> in the vector meson sector
129	(which is somewhat better determined), expressed in degrees.
130	Here <i>f</i> is associated with <i>omega</i> and <i>f'</i>
131	with <i>phi</i>.
132
133
134	<p/>
135	Further, the simple model overestimates the production of <i>eta</i>
136	and, in particular, <i>eta'</i> mesons, which can be rectified by
137
138	<br/><br/><table><tr><td><strong>StringFlav:etaSup </td><td></td><td> <input type="text" name="11" value="0.63" size="20"/>   (<code>default = <strong>0.63</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.</code>)</td></tr></table>
139	the additional suppression of <i>eta</i> production, multiplying the
140	normal production probability. Thus 0 means no <i>eta</i> at all
141	are produced, while 1 means full rate.
142
143
144	<br/><br/><table><tr><td><strong>StringFlav:etaPrimeSup </td><td></td><td> <input type="text" name="12" value="0.12" size="20"/>   (<code>default = <strong>0.12</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.</code>)</td></tr></table>
145	the additional suppression of <i>eta'</i> production, multiplying the
146	normal production probability. Thus 0 means no <i>eta'</i> at all
147	are produced, while 1 means full rate.
148
149
150	<h3>Excited-meson production</h3>
151
152	Several excited mesons, ie. with radial or orbital excitations, have been
153	observed at non-negligible production rates. Extrapolated to all states
154	a fair fraction of all particle production might proceed through such
155	states. There are big uncertainties, however, since these excited
156	mesons in many cases are extremely poorly known. This also means that
157	the modelling of their production and decay is very primitive, and
158	even that the inclusion of the production of such states may lead to a
159	degraded agreement with data. Currently the default is that all such
160	production is switched off.
161
162	<p/>
163	Parameters are provided to switch them on. By demand, this machinery
164	has been made more flexible than in the past. Therefore one parameter is
165	provided for each combination of heaviest flavour
166	(<i>u/d</i>, <i>s</i>, <i>c</i> or <i>b</i>) and
167	multiplet produced. In each case the production rate is normalized to
168	that of the lowest-lying pseudoscalar of the same flavour content, as for
169	the vector-meson rates introduced above. The multiplets available are the
170	four obtained for one unit of orbital angular momentum, in the
171	nonrelativistic classification. Using <i>J</i> to denote the sum of
172	quark spin <i>S</i> and orbital angular momentum <i>L</i>, i.e. what
173	would normally be called the spin of the meson, one has:
174	<ul>
175	<li>a pseudovector multiplet with <i>L=1, S=0, J=1</i>;</li>
176	<li>a scalar multiplet with <i>L=1, S=1, J=0</i>;</li>
177	<li>a pseudovector multiplet with <i>L=1, S=1, J=1</i>;</li>
178	<li>a tensor multiplet with <i>L=1, S=1, J=2</i>.</li>
179	</ul>
180
181	The maximum allowed rate for each case has been set according to
182	spin-counting rules, but we expect the real rates to be significantly
183	lower, owing to mass suppression.
184
185	<br/><br/><table><tr><td><strong>StringFlav:mesonUDL1S0J1 </td><td></td><td> <input type="text" name="13" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
186	the relative pseudovector production ratio
187	<i>(L=1,S=0,J=1)</i>/pseudoscalar
188	for light (<i>u</i>, <i>d</i>) mesons.
189
190
191	<br/><br/><table><tr><td><strong>StringFlav:mesonUDL1S1J0 </td><td></td><td> <input type="text" name="14" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.</code>)</td></tr></table>
192	the relative scalar production ratio
193	<i>(L=1,S=1,J=0)</i>/pseudoscalar
194	for light (<i>u</i>, <i>d</i>) mesons.
195
196
197	<br/><br/><table><tr><td><strong>StringFlav:mesonUDL1S1J1 </td><td></td><td> <input type="text" name="15" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
198	the relative pseudovector production ratio
199	<i>(L=1,S=1,J=1)</i>/pseudoscalar
200	for light (<i>u</i>, <i>d</i>) mesons.
201
202
203	<br/><br/><table><tr><td><strong>StringFlav:mesonUDL1S1J2 </td><td></td><td> <input type="text" name="16" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 5.</code>)</td></tr></table>
204	the relative tensor production ratio
205	<i>(L=1,S=1,J=2)</i>/pseudoscalar
206	for light (<i>u</i>, <i>d</i>) mesons.
207
208
209	<br/><br/><table><tr><td><strong>StringFlav:mesonSL1S0J1 </td><td></td><td> <input type="text" name="17" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
210	the relative pseudovector production ratio
211	<i>(L=1,S=0,J=1)</i>/pseudoscalar
212	for strange mesons.
213
214
215	<br/><br/><table><tr><td><strong>StringFlav:mesonSL1S1J0 </td><td></td><td> <input type="text" name="18" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.</code>)</td></tr></table>
216	the relative scalar production ratio
217	<i>(L=1,S=1,J=0)</i>/pseudoscalar
218	for strange mesons.
219
220
221	<br/><br/><table><tr><td><strong>StringFlav:mesonSL1S1J1 </td><td></td><td> <input type="text" name="19" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
222	the relative pseudovector production ratio
223	<i>(L=1,S=1,J=1)</i>/pseudoscalar
224	for strange mesons.
225
226
227	<br/><br/><table><tr><td><strong>StringFlav:mesonSL1S1J2 </td><td></td><td> <input type="text" name="20" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 5.</code>)</td></tr></table>
228	the relative tensor production ratio
229	<i>(L=1,S=1,J=2)</i>/pseudoscalar
230	for strange mesons.
231
232
233	<br/><br/><table><tr><td><strong>StringFlav:mesonCL1S0J1 </td><td></td><td> <input type="text" name="21" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
234	the relative pseudovector production ratio
235	<i>(L=1,S=0,J=1)</i>/pseudoscalar
236	for charm mesons.
237
238
239	<br/><br/><table><tr><td><strong>StringFlav:mesonCL1S1J0 </td><td></td><td> <input type="text" name="22" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.</code>)</td></tr></table>
240	the relative scalar production ratio
241	<i>(L=1,S=1,J=0)</i>/pseudoscalar
242	for charm mesons.
243
244
245	<br/><br/><table><tr><td><strong>StringFlav:mesonCL1S1J1 </td><td></td><td> <input type="text" name="23" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
246	the relative pseudovector production ratio
247	<i>(L=1,S=1,J=1)</i>/pseudoscalar
248	for charm mesons.
249
250
251	<br/><br/><table><tr><td><strong>StringFlav:mesonCL1S1J2 </td><td></td><td> <input type="text" name="24" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 5.</code>)</td></tr></table>
252	the relative tensor production ratio
253	<i>(L=1,S=1,J=2)</i>/pseudoscalar
254	for charm mesons.
255
256
257	<br/><br/><table><tr><td><strong>StringFlav:mesonBL1S0J1 </td><td></td><td> <input type="text" name="25" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
258	the relative pseudovector production ratio
259	<i>(L=1,S=0,J=1)</i>/pseudoscalar
260	for bottom mesons.
261
262
263	<br/><br/><table><tr><td><strong>StringFlav:mesonBL1S1J0 </td><td></td><td> <input type="text" name="26" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.</code>)</td></tr></table>
264	the relative scalar production ratio
265	<i>(L=1,S=1,J=0)</i>/pseudoscalar
266	for bottom mesons.
267
268
269	<br/><br/><table><tr><td><strong>StringFlav:mesonBL1S1J1 </td><td></td><td> <input type="text" name="27" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 3.</code>)</td></tr></table>
270	the relative pseudovector production ratio
271	<i>(L=1,S=1,J=1)</i>/pseudoscalar
272	for bottom mesons.
273
274
275	<br/><br/><table><tr><td><strong>StringFlav:mesonBL1S1J2 </td><td></td><td> <input type="text" name="28" value="0.0" size="20"/>   (<code>default = <strong>0.0</strong></code>; <code>minimum = 0.</code>; <code>maximum = 5.</code>)</td></tr></table>
276	the relative tensor production ratio
277	<i>(L=1,S=1,J=2)</i>/pseudoscalar
278	for bottom mesons.
279
280
281	<p/>
282	In addition, an octet-singlet mixing angle is needed for each multiplet,
283	as for the pseudoscalar and vector multiplets above. Only for the
284	tensor multiplet does any determination exist; for the other multiplets
285	default has been chose so that <i>ssbar</i> does not mix with the light
286	quarks, and so that the <i>ssbar</i> state is the heavier of the two.
287
288	<br/><br/><table><tr><td><strong>StringFlav:thetaL1S0J1 </td><td></td><td> <input type="text" name="29" value="35.3" size="20"/>   (<code>default = <strong>35.3</strong></code>; <code>minimum = -90.</code>; <code>maximum = 90.</code>)</td></tr></table>
289	gives the mixing angle <i>theta</i> in the <i>(L=1,S=0,J=1)</i>
290	pseudovector meson sector, expressed in degrees.
291
292
293	<br/><br/><table><tr><td><strong>StringFlav:thetaL1S1J0 </td><td></td><td> <input type="text" name="30" value="35.3" size="20"/>   (<code>default = <strong>35.3</strong></code>; <code>minimum = -90.</code>; <code>maximum = 90.</code>)</td></tr></table>
294	gives the mixing angle <i>theta</i> in the <i>(L=1,S=1,J=0)</i>
295	scalar meson sector, expressed in degrees.
296
297
298	<br/><br/><table><tr><td><strong>StringFlav:thetaL1S1J1 </td><td></td><td> <input type="text" name="31" value="35.3" size="20"/>   (<code>default = <strong>35.3</strong></code>; <code>minimum = -90.</code>; <code>maximum = 90.</code>)</td></tr></table>
299	gives the mixing angle <i>theta</i> in the <i>(L=1,S=1,J=1)</i>
300	pseudovector meson sector, expressed in degrees.
301
302
303	<br/><br/><table><tr><td><strong>StringFlav:thetaL1S1J2 </td><td></td><td> <input type="text" name="32" value="28.0" size="20"/>   (<code>default = <strong>28.0</strong></code>; <code>minimum = -90.</code>; <code>maximum = 90.</code>)</td></tr></table>
304	gives the mixing angle <i>theta</i> in the <i>(L=1,S=1,J=2)</i>
305	tensor meson sector, expressed in degrees.
306
307
308	<h3>Baryon production</h3>
309
310	The relative rate of baryon production is mainly given by the quark
311	and diquark production parameters above, plus SU(6) Clebsch-Gordans.
312	The one modifiable parameter related to these coefficients is
313
314	<br/><br/><table><tr><td><strong>StringFlav:decupletSup </td><td></td><td> <input type="text" name="33" value="1.0" size="20"/>   (<code>default = <strong>1.0</strong></code>; <code>minimum = 0.0</code>; <code>maximum = 1.0</code>)</td></tr></table>
315	the suppression, relative to default SU(6) factors, of decuplet
316	baryon production. Default corresponds to no suppression, while 0
317	corresponds to no decuplet production at all.
318
319
320	<p/>
321	In addition, if popcorn production is allowed, wherein a set of mesons
322	(<i>M</i>) may be producted in between the baryon (<i>B</i>) and
323	the antibaryon (<i>Bbar</i>), a set of further parameters is introduced.
324	Currently only the simplest scenario is implemented, wherein at most
325	one intermediate meson may be produced.
326
327	<br/><br/><table><tr><td><strong>StringFlav:popcornRate </td><td></td><td> <input type="text" name="34" value="0.5" size="20"/>   (<code>default = <strong>0.5</strong></code>; <code>minimum = 0.</code>; <code>maximum = 2.0</code>)</td></tr></table>
328	gives the relative rates of <i>B Bbar</i> and <i>B M Bbar</i>
329	production, roughly as
330	<br/><i>
331	Prob(B M Bbar) / (Prob(B Bbar) + Prob(B M Bbar)) =
332	popcornRate / (0.5 + popcornRate)
333	</i><br/>
334	(the complete expression depends on all the quark and diquark production
335	parameters and is therefore not so useful).
336
337
338	<br/><br/><table><tr><td><strong>StringFlav:popcornSpair </td><td></td><td> <input type="text" name="35" value="0.5" size="20"/>   (<code>default = <strong>0.5</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.0</code>)</td></tr></table>
339	extra suppression for having an <i>s sbar</i> pair shared between
340	the <i>B</i> and <i>Bbar</i> in a <i>B M Bbar</i> configuration.
341
342
343	<br/><br/><table><tr><td><strong>StringFlav:popcornSmeson </td><td></td><td> <input type="text" name="36" value="0.5" size="20"/>   (<code>default = <strong>0.5</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.0</code>)</td></tr></table>
344	extra suppression for having a strange meson <i>M</i> in a
345	<i>B M Bbar</i> configuration.
346
347
348	<p/>
349	Finally, there are some indications that leading-baryon production
350	may be further suppressed. A proper description should probably be
351	based on a suppression of early production times [<a href="Bibliography.php" target="page">Ede97</a>],
352	but we here only implement a simpler version where production near
353	the end of a string, as defined by rank, is suppressed. The more
354	detailed studies suggest that leading <i>c</i> and <i>b</i> baryon
355	production will be less suppressed, so we leave it open to set
356	light- and heavy-baryon suppression separately.
357
358	<br/><br/><strong>StringFlav:suppressLeadingB</strong> <input type="radio" name="37" value="on"><strong>On</strong>
359	<input type="radio" name="37" value="off" checked="checked"><strong>Off</strong>
360	(<code>default = <strong>off</strong></code>)<br/>
361	Suppress leading-baryon production.
362	<br/><code>option </code><strong> off</strong> : No suppression.
363	<br/><code>option </code><strong> on</strong> : Suppress the production of a diquark in the string
364	breaking closest to a quark end of a string, by either of the factors
365	below. This suppresses the production of first-rank baryons by the same
366	amount. Indirectly also the second-rank and, if popcorn production is
367	switched on, third-rank (anti)baryon production is affected.
368
369
370	<br/><br/><table><tr><td><strong>StringFlav:lightLeadingBSup </td><td></td><td> <input type="text" name="38" value="0.5" size="20"/>   (<code>default = <strong>0.5</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.0</code>)</td></tr></table>
371	extra suppression of leading-baryon production for a light-quark
372	jet, i.e. <i>d</i>, <i>u</i> or <i>s</i>, when
373	<code>suppressLeadingB = on</code>. Thus 0 means no leading-baryon
374	production at all, while 1 means full rate.
375
376
377	<br/><br/><table><tr><td><strong>StringFlav:heavyLeadingBSup </td><td></td><td> <input type="text" name="39" value="0.9" size="20"/>   (<code>default = <strong>0.9</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.0</code>)</td></tr></table>
378	extra suppression of leading-baryon production for a heavy-quark
379	jet, i.e. <i>c</i> or <i>b</i>, when
380	<code>suppressLeadingB = on</code>. Thus 0 means no leading-baryon
381	production at all, while 1 means full rate.
382
383
384	<input type="hidden" name="saved" value="1"/>
385
386	<?php
387	echo "<input type='hidden' name='filepath' value='".$_GET["filepath"]."'/>"?>
388
389	<table width="100%"><tr><td align="right"><input type="submit" value="Save Settings" /></td></tr></table>
390	</form>
391
392	<?php
393
394	if($_POST["saved"] == 1)
395	{
396	$filepath = $_POST["filepath"];
397	$handle = fopen($filepath, 'a');
398
399	if($_POST["1"] != "0.19")
400	{
401	$data = "StringFlav:probStoUD = ".$_POST["1"]."\n";
402	fwrite($handle,$data);
403	}
404	if($_POST["2"] != "0.09")
405	{
406	$data = "StringFlav:probQQtoQ = ".$_POST["2"]."\n";
407	fwrite($handle,$data);
408	}
409	if($_POST["3"] != "1.00")
410	{
411	$data = "StringFlav:probSQtoQQ = ".$_POST["3"]."\n";
412	fwrite($handle,$data);
413	}
414	if($_POST["4"] != "0.027")
415	{
416	$data = "StringFlav:probQQ1toQQ0 = ".$_POST["4"]."\n";
417	fwrite($handle,$data);
418	}
419	if($_POST["5"] != "0.62")
420	{
421	$data = "StringFlav:mesonUDvector = ".$_POST["5"]."\n";
422	fwrite($handle,$data);
423	}
424	if($_POST["6"] != "0.725")
425	{
426	$data = "StringFlav:mesonSvector = ".$_POST["6"]."\n";
427	fwrite($handle,$data);
428	}
429	if($_POST["7"] != "1.06")
430	{
431	$data = "StringFlav:mesonCvector = ".$_POST["7"]."\n";
432	fwrite($handle,$data);
433	}
434	if($_POST["8"] != "3.0")
435	{
436	$data = "StringFlav:mesonBvector = ".$_POST["8"]."\n";
437	fwrite($handle,$data);
438	}
439	if($_POST["9"] != "-15.")
440	{
441	$data = "StringFlav:thetaPS = ".$_POST["9"]."\n";
442	fwrite($handle,$data);
443	}
444	if($_POST["10"] != "36.")
445	{
446	$data = "StringFlav:thetaV = ".$_POST["10"]."\n";
447	fwrite($handle,$data);
448	}
449	if($_POST["11"] != "0.63")
450	{
451	$data = "StringFlav:etaSup = ".$_POST["11"]."\n";
452	fwrite($handle,$data);
453	}
454	if($_POST["12"] != "0.12")
455	{
456	$data = "StringFlav:etaPrimeSup = ".$_POST["12"]."\n";
457	fwrite($handle,$data);
458	}
459	if($_POST["13"] != "0.0")
460	{
461	$data = "StringFlav:mesonUDL1S0J1 = ".$_POST["13"]."\n";
462	fwrite($handle,$data);
463	}
464	if($_POST["14"] != "0.0")
465	{
466	$data = "StringFlav:mesonUDL1S1J0 = ".$_POST["14"]."\n";
467	fwrite($handle,$data);
468	}
469	if($_POST["15"] != "0.0")
470	{
471	$data = "StringFlav:mesonUDL1S1J1 = ".$_POST["15"]."\n";
472	fwrite($handle,$data);
473	}
474	if($_POST["16"] != "0.0")
475	{
476	$data = "StringFlav:mesonUDL1S1J2 = ".$_POST["16"]."\n";
477	fwrite($handle,$data);
478	}
479	if($_POST["17"] != "0.0")
480	{
481	$data = "StringFlav:mesonSL1S0J1 = ".$_POST["17"]."\n";
482	fwrite($handle,$data);
483	}
484	if($_POST["18"] != "0.0")
485	{
486	$data = "StringFlav:mesonSL1S1J0 = ".$_POST["18"]."\n";
487	fwrite($handle,$data);
488	}
489	if($_POST["19"] != "0.0")
490	{
491	$data = "StringFlav:mesonSL1S1J1 = ".$_POST["19"]."\n";
492	fwrite($handle,$data);
493	}
494	if($_POST["20"] != "0.0")
495	{
496	$data = "StringFlav:mesonSL1S1J2 = ".$_POST["20"]."\n";
497	fwrite($handle,$data);
498	}
499	if($_POST["21"] != "0.0")
500	{
501	$data = "StringFlav:mesonCL1S0J1 = ".$_POST["21"]."\n";
502	fwrite($handle,$data);
503	}
504	if($_POST["22"] != "0.0")
505	{
506	$data = "StringFlav:mesonCL1S1J0 = ".$_POST["22"]."\n";
507	fwrite($handle,$data);
508	}
509	if($_POST["23"] != "0.0")
510	{
511	$data = "StringFlav:mesonCL1S1J1 = ".$_POST["23"]."\n";
512	fwrite($handle,$data);
513	}
514	if($_POST["24"] != "0.0")
515	{
516	$data = "StringFlav:mesonCL1S1J2 = ".$_POST["24"]."\n";
517	fwrite($handle,$data);
518	}
519	if($_POST["25"] != "0.0")
520	{
521	$data = "StringFlav:mesonBL1S0J1 = ".$_POST["25"]."\n";
522	fwrite($handle,$data);
523	}
524	if($_POST["26"] != "0.0")
525	{
526	$data = "StringFlav:mesonBL1S1J0 = ".$_POST["26"]."\n";
527	fwrite($handle,$data);
528	}
529	if($_POST["27"] != "0.0")
530	{
531	$data = "StringFlav:mesonBL1S1J1 = ".$_POST["27"]."\n";
532	fwrite($handle,$data);
533	}
534	if($_POST["28"] != "0.0")
535	{
536	$data = "StringFlav:mesonBL1S1J2 = ".$_POST["28"]."\n";
537	fwrite($handle,$data);
538	}
539	if($_POST["29"] != "35.3")
540	{
541	$data = "StringFlav:thetaL1S0J1 = ".$_POST["29"]."\n";
542	fwrite($handle,$data);
543	}
544	if($_POST["30"] != "35.3")
545	{
546	$data = "StringFlav:thetaL1S1J0 = ".$_POST["30"]."\n";
547	fwrite($handle,$data);
548	}
549	if($_POST["31"] != "35.3")
550	{
551	$data = "StringFlav:thetaL1S1J1 = ".$_POST["31"]."\n";
552	fwrite($handle,$data);
553	}
554	if($_POST["32"] != "28.0")
555	{
556	$data = "StringFlav:thetaL1S1J2 = ".$_POST["32"]."\n";
557	fwrite($handle,$data);
558	}
559	if($_POST["33"] != "1.0")
560	{
561	$data = "StringFlav:decupletSup = ".$_POST["33"]."\n";
562	fwrite($handle,$data);
563	}
564	if($_POST["34"] != "0.5")
565	{
566	$data = "StringFlav:popcornRate = ".$_POST["34"]."\n";
567	fwrite($handle,$data);
568	}
569	if($_POST["35"] != "0.5")
570	{
571	$data = "StringFlav:popcornSpair = ".$_POST["35"]."\n";
572	fwrite($handle,$data);
573	}
574	if($_POST["36"] != "0.5")
575	{
576	$data = "StringFlav:popcornSmeson = ".$_POST["36"]."\n";
577	fwrite($handle,$data);
578	}
579	if($_POST["37"] != "off")
580	{
581	$data = "StringFlav:suppressLeadingB = ".$_POST["37"]."\n";
582	fwrite($handle,$data);
583	}
584	if($_POST["38"] != "0.5")
585	{
586	$data = "StringFlav:lightLeadingBSup = ".$_POST["38"]."\n";
587	fwrite($handle,$data);
588	}
589	if($_POST["39"] != "0.9")
590	{
591	$data = "StringFlav:heavyLeadingBSup = ".$_POST["39"]."\n";
592	fwrite($handle,$data);
593	}
594	fclose($handle);
595	}
596
597	?>
598	</body>
599	</html>
600
601	<!-- Copyright (C) 2012 Torbjorn Sjostrand -->

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