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3	<title>Higgs Processes</title>
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29
30	<h2>Higgs Processes</h2>
31
32	This page documents Higgs production within and beyond the Standard Model
33	(SM and BSM for short). This includes several different processes and,
34	for the BSM scenarios, a large set of parameters that would only be fixed
35	within a more specific framework such as MSSM. Three choices can be made
36	irrespective of the particular model:
37
38	<br/><br/><strong>Higgs:cubicWidth</strong> <input type="radio" name="1" value="on"><strong>On</strong>
39	<input type="radio" name="1" value="off" checked="checked"><strong>Off</strong>
40	(<code>default = <strong>off</strong></code>)<br/>
41	The partial width of a Higgs particle to a pair of gauge bosons,
42	<i>W^+ W^-</i> or <i>Z^0 Z^0</i>, depends cubically on the
43	Higgs mass. When selecting the Higgs according to a Breit-Wigner,
44	so that the actual mass <i>mHat</i> does not agree with the
45	nominal <i>m_Higgs</i> one, an ambiguity arises which of the
46	two to use [<a href="Bibliography.php" target="page">Sey95</a>]. The default is to use a linear
47	dependence on <i>mHat</i>, i.e. a width proportional to
48	<i>m_Higgs^2 * mHat</i>, while <code>on</code> gives a
49	<i>mHat^3</i> dependence. This does not affect the widths to
50	fermions, which only depend linearly on <i>mHat</i>.
51	This flag is used both for SM and BSM Higgses.
52
53
54	<br/><br/><strong>Higgs:runningLoopMass</strong> <input type="radio" name="2" value="on" checked="checked"><strong>On</strong>
55	<input type="radio" name="2" value="off"><strong>Off</strong>
56	(<code>default = <strong>on</strong></code>)<br/>
57	The partial width of a Higgs particle to a pair of gluons or photons,
58	or a <i>gamma Z^0</i> pair, proceeds in part through quark loops,
59	mainly <i>b</i> and <i>t</i>. There is some ambiguity what kind
60	of masses to use. Default is running MSbar ones, but alternatively
61	fixed pole masses are allowed (as was standard in PYTHIA 6), which
62	typically gives a noticeably higher cross section for these channels.
63	(For a decay to a pair of fermions, such as top, the running mass is
64	used for couplings and the fixed one for phase space.)
65
66
67	<br/><br/><strong>Higgs:clipWings</strong> <input type="radio" name="3" value="on" checked="checked"><strong>On</strong>
68	<input type="radio" name="3" value="off"><strong>Off</strong>
69	(<code>default = <strong>on</strong></code>)<br/>
70	The Breit-Wigner shape of a Higgs is nontrivial, owing to the rapid
71	width variation with the mass of a Higgs. This imples that a Higgs
72	of low nominal mass may still acquire a non-negligible high-end tail.
73	The validity of the calculation may be questioned in these wings.
74	With this option on, the <code>Higgs:wingsFac</code> value is used to
75	cut away the wings.
76
77
78	<br/><br/><table><tr><td><strong>Higgs:wingsFac </td><td></td><td> <input type="text" name="4" value="50." size="20"/>   (<code>default = <strong>50.</strong></code>; <code>minimum = 0.</code>)</td></tr></table>
79	With <code>Higgs:clipWings</code> on, all Higgs masses which deviate
80	from the nominal one by more than <code>Higgs:wingsFac</code>
81	times the nominal width are forbidden. This is achieved by setting
82	the <code>mMin</code> and <code>mMax</code> values of the Higgs states
83	at initialization (but never so as to allow a wider range than already
84	set by the user, alternatively by the default values).
85
86
87	<h3>Standard-Model Higgs, basic processes</h3>
88
89	This section provides the standard set of processes that can be
90	run together to provide a reasonably complete overview of possible
91	production channels for a single SM Higgs.
92	The main parameter is the choice of Higgs mass, which can be set in the
93	normal <code>ParticleData</code> database; thereafter the properties
94	within the SM are essentially fixed.
95
96	<br/><br/><strong>HiggsSM:all</strong> <input type="radio" name="5" value="on"><strong>On</strong>
97	<input type="radio" name="5" value="off" checked="checked"><strong>Off</strong>
98	(<code>default = <strong>off</strong></code>)<br/>
99	Common switch for the group of Higgs production within the Standard Model.
100
101
102	<br/><br/><strong>HiggsSM:ffbar2H</strong> <input type="radio" name="6" value="on"><strong>On</strong>
103	<input type="radio" name="6" value="off" checked="checked"><strong>Off</strong>
104	(<code>default = <strong>off</strong></code>)<br/>
105	Scattering <i>f fbar -> H^0</i>, where <i>f</i> sums over available
106	flavours except top. Related to the mass-dependent Higgs point coupling
107	to fermions, so at hadron colliders the bottom contribution will
108	dominate.
109	Code 901.
110
111
112	<br/><br/><strong>HiggsSM:gg2H</strong> <input type="radio" name="7" value="on"><strong>On</strong>
113	<input type="radio" name="7" value="off" checked="checked"><strong>Off</strong>
114	(<code>default = <strong>off</strong></code>)<br/>
115	Scattering <i>g g -> H^0</i> via loop contributions primarily from
116	top.
117	Code 902.
118
119
120	<br/><br/><strong>HiggsSM:gmgm2H</strong> <input type="radio" name="8" value="on"><strong>On</strong>
121	<input type="radio" name="8" value="off" checked="checked"><strong>Off</strong>
122	(<code>default = <strong>off</strong></code>)<br/>
123	Scattering <i>gamma gamma -> H^0</i> via loop contributions primarily
124	from top and <i>W</i>.
125	Code 903.
126
127
128	<br/><br/><strong>HiggsSM:ffbar2HZ</strong> <input type="radio" name="9" value="on"><strong>On</strong>
129	<input type="radio" name="9" value="off" checked="checked"><strong>Off</strong>
130	(<code>default = <strong>off</strong></code>)<br/>
131	Scattering <i>f fbar -> H^0 Z^0</i> via <i>s</i>-channel <i>Z^0</i>
132	exchange.
133	Code 904.
134
135
136	<br/><br/><strong>HiggsSM:ffbar2HW</strong> <input type="radio" name="10" value="on"><strong>On</strong>
137	<input type="radio" name="10" value="off" checked="checked"><strong>Off</strong>
138	(<code>default = <strong>off</strong></code>)<br/>
139	Scattering <i>f fbar -> H^0 W^+-</i> via <i>s</i>-channel <i>W^+-</i>
140	exchange.
141	Code 905.
142
143
144	<br/><br/><strong>HiggsSM:ff2Hff(t:ZZ)</strong> <input type="radio" name="11" value="on"><strong>On</strong>
145	<input type="radio" name="11" value="off" checked="checked"><strong>Off</strong>
146	(<code>default = <strong>off</strong></code>)<br/>
147	Scattering <i>f f' -> H^0 f f'</i> via <i>Z^0 Z^0</i> fusion.
148	Code 906.
149
150
151	<br/><br/><strong>HiggsSM:ff2Hff(t:WW)</strong> <input type="radio" name="12" value="on"><strong>On</strong>
152	<input type="radio" name="12" value="off" checked="checked"><strong>Off</strong>
153	(<code>default = <strong>off</strong></code>)<br/>
154	Scattering <i>f_1 f_2 -> H^0 f_3 f_4</i> via <i>W^+ W^-</i> fusion.
155	Code 907.
156
157
158	<br/><br/><strong>HiggsSM:gg2Httbar</strong> <input type="radio" name="13" value="on"><strong>On</strong>
159	<input type="radio" name="13" value="off" checked="checked"><strong>Off</strong>
160	(<code>default = <strong>off</strong></code>)<br/>
161	Scattering <i>g g -> H^0 t tbar</i> via <i>t tbar</i> fusion
162	(or, alternatively put, Higgs radiation off a top line).
163	Warning: unfortunately this process is rather slow, owing to a
164	lengthy cross-section expression and inefficient phase-space selection.
165	Code 908.
166
167
168	<br/><br/><strong>HiggsSM:qqbar2Httbar</strong> <input type="radio" name="14" value="on"><strong>On</strong>
169	<input type="radio" name="14" value="off" checked="checked"><strong>Off</strong>
170	(<code>default = <strong>off</strong></code>)<br/>
171	Scattering <i>q qbar -> H^0 t tbar</i> via <i>t tbar</i> fusion
172	(or, alternatively put, Higgs radiation off a top line).
173	Warning: unfortunately this process is rather slow, owing to a
174	lengthy cross-section expression and inefficient phase-space selection.
175	Code 909.
176
177
178	<h3>Standard-Model Higgs, further processes</h3>
179
180	A number of further production processes has been implemented, that
181	are specializations of some of the above ones to the high-<i>pT</i>
182	region. The sets therefore could not be used simultaneously
183	without unphysical doublecounting, as further explained below.
184	They are not switched on by the <code>HiggsSM:all</code> flag, but
185	have to be switched on for each separate process after due consideration.
186
187	<p/>
188	The first three processes in this section are related to the Higgs
189	point coupling to fermions, and so primarily are of interest for
190	<i>b</i> quarks. It is here useful to begin by reminding that
191	a process like <i>b bbar -> H^0</i> implies that a <i>b/bbar</i>
192	is taken from each incoming hadron, leaving behind its respective
193	antiparticle. The initial-state showers will then add one
194	<i>g -> b bbar</i> branching on either side, so that effectively
195	the process becomes <i>g g -> H0 b bbar</i>. This would be the
196	same basic process as the <i>g g -> H^0 t tbar</i> one used for top.
197	The difference is that (a) no PDF's are defined for top and
198	(b) the shower approach would not be good enough to provide sensible
199	kinematics for the <i>H^0 t tbar</i> subsystem. By contrast, owing
200	to the <i>b</i> being much lighter than the Higgs, multiple
201	gluon emissions must be resummed for <i>b</i>, as is done by PDF's
202	and showers, in order to obtain a sensible description of the total
203	production rate, when the <i>b</i> quarks predominantly are produced
204	at small <i>pT</i> values.
205
206	<br/><br/><strong>HiggsSM:qg2Hq</strong> <input type="radio" name="15" value="on"><strong>On</strong>
207	<input type="radio" name="15" value="off" checked="checked"><strong>Off</strong>
208	(<code>default = <strong>off</strong></code>)<br/>
209	Scattering <i>q g -> H^0 q</i>. This process gives first-order
210	corrections to the <i>f fbar -> H^0</i> one above, and should only be
211	used to study the high-<i>pT</i> tail, while <i>f fbar -> H^0</i>
212	should be used for inclusive production. Only the dominant <i>c</i>
213	and <i>b</i> contributions are included, and generated separately
214	for technical reasons. Note that another first-order process would be
215	<i>q qbar -> H^0 g</i>, which is not explicitly implemented here,
216	but is obtained from showering off the lowest-order process. It does not
217	contain any <i>b</i> at large <i>pT</i>, however, so is less
218	interesting for many applications.
219	Code 911.
220
221
222	<br/><br/><strong>HiggsSM:gg2Hbbbar</strong> <input type="radio" name="16" value="on"><strong>On</strong>
223	<input type="radio" name="16" value="off" checked="checked"><strong>Off</strong>
224	(<code>default = <strong>off</strong></code>)<br/>
225	Scattering <i>g g -> H^0 b bbar</i>. This process is yet one order
226	higher of the <i>b bbar -> H^0</i> and <i>b g -> H^0 b</i> chain,
227	where now two quarks should be required above some large <i>pT</i>
228	threshold.
229	Warning: unfortunately this process is rather slow, owing to a
230	lengthy cross-section expression and inefficient phase-space selection.
231	Code 912.
232
233
234	<br/><br/><strong>HiggsSM:qqbar2Hbbbar</strong> <input type="radio" name="17" value="on"><strong>On</strong>
235	<input type="radio" name="17" value="off" checked="checked"><strong>Off</strong>
236	(<code>default = <strong>off</strong></code>)<br/>
237	Scattering <i>q qbar -> H^0 b bbar</i> via an <i>s</i>-channel
238	gluon, so closely related to the previous one, but typically less
239	important owing to the smaller rate of (anti)quarks relative to
240	gluons.
241	Warning: unfortunately this process is rather slow, owing to a
242	lengthy cross-section expression and inefficient phase-space selection.
243	Code 913.
244
245
246	<p/>
247	The second set of processes are predominantly first-order corrections
248	to the <i>g g -> H^0</i> process, again dominated by the top loop.
249	We here only provide the kinematical expressions obtained in the
250	limit that the top quark goes to infinity, but scaled to the
251	finite-top-mass coupling in <i>g g -> H^0</i>. (Complete loop
252	expressions are available e.g. in PYTHIA 6.4 but are very lengthy.)
253	This provides a reasonably accurate description for "intermediate"
254	<i>pT</i> values, but fails when the <i>pT</i> scale approaches
255	the top mass.
256
257	<br/><br/><strong>HiggsSM:gg2Hg(l:t)</strong> <input type="radio" name="18" value="on"><strong>On</strong>
258	<input type="radio" name="18" value="off" checked="checked"><strong>Off</strong>
259	(<code>default = <strong>off</strong></code>)<br/>
260	Scattering <i>g g -> H^0 g</i> via loop contributions primarily
261	from top.
262	Code 914.
263
264
265	<br/><br/><strong>HiggsSM:qg2Hq(l:t)</strong> <input type="radio" name="19" value="on"><strong>On</strong>
266	<input type="radio" name="19" value="off" checked="checked"><strong>Off</strong>
267	(<code>default = <strong>off</strong></code>)<br/>
268	Scattering <i>q g -> H^0 q</i> via loop contributions primarily
269	from top. Not to be confused with the <code>HiggsSM:qg2Hq</code>
270	process above, with its direct fermion-to-Higgs coupling.
271	Code 915.
272
273
274	<br/><br/><strong>HiggsSM:qqbar2Hg(l:t)</strong> <input type="radio" name="20" value="on"><strong>On</strong>
275	<input type="radio" name="20" value="off" checked="checked"><strong>Off</strong>
276	(<code>default = <strong>off</strong></code>)<br/>
277	Scattering <i>q qbar -> H^0 g</i> via an <i>s</i>-channel gluon
278	and loop contributions primarily from top. Is strictly speaking a
279	"new" process, not directly derived from <i>g g -> H^0</i>, and
280	could therefore be included in the standard mix without doublecounting,
281	but is numerically negligible.
282	Code 916.
283
284
285	<h3>Beyond-the-Standard-Model Higgs, introduction</h3>
286
287	Further Higgs multiplets arise in a number of scenarios. We here
288	concentrate on the MSSM scenario with two Higgs doublets, but with
289	flexibility enough that also other two-Higgs-doublet scenarios could
290	be represented by a suitable choice of parameters. Conventionally the
291	Higgs states are labelled <i>h^0, H^0, A^0</i> and <i>H^+-</i>.
292	If the scalar and pseudocalar states mix the resulting states are
293	labelled <i>H_1^0, H_2^0, H_3^0</i>. In process names and parameter
294	explanations both notations will be used, but for settings labels
295	we have adapted the shorthand hybrid notation <code>H1</code> for
296	<i>h^0(H_1^0)</i>, <code>H2</code> for <i>H^0(H_2^0)</i> and
297	<code>A3</code> for <i>A^0(H_3^0)</i>. (Recall that the
298	<code>Settings</code> database does not distinguish upper- and lowercase
299	characters, so that the user has one thing less to worry about, but here
300	it causes probles with <i>h^0</i> vs. <i>H^0</i>.) We leave the issue
301	of mass ordering between <i>H^0</i> and <i>A^0</i> open, and thereby
302	also that of <i>H_2^0</i> and <i>H_3^0</i>.
303
304	<br/><br/><strong>Higgs:useBSM</strong> <input type="radio" name="21" value="on"><strong>On</strong>
305	<input type="radio" name="21" value="off" checked="checked"><strong>Off</strong>
306	(<code>default = <strong>off</strong></code>)<br/>
307	Master switch to initialize and use the two-Higgs-doublet states.
308	If off, only the above SM Higgs processes can be used, with couplings
309	as predicted in the SM. If on, only the below BSM Higgs processes can
310	be used, with couplings that can be set freely, also found further down
311	on this page.
312
313
314	<h3>Beyond-the-Standard-Model Higgs, basic processes</h3>
315
316	This section provides the standard set of processes that can be
317	run together to provide a reasonably complete overview of possible
318	production channels for a single neutral Higgs state in a two-doublet
319	scenarios such as MSSM. The list of processes for neutral states closely
320	mimics the one found for the SM Higgs. Some of the processes
321	vanish for a pure pseudoscalar <i>A^0</i>, but are kept for flexiblity
322	in cases of mixing with the scalar <i>h^0</i> and <i>H^0</i> states,
323	or for use in the context of non-MSSM models. This should work well to
324	represent e.g. that a small admixture of the "wrong" parity would allow
325	a process such as <i>q qbar -> A^0 Z^0</i>, which otherwise is forbidden.
326	However, note that the loop integrals e.g. for <i>g g -> h^0/H^0/A^0</i>
327	are hardcoded to be for scalars for the former two particles and for a
328	pseudoscalar for the latter one, so absolute rates would not be
329	correctly represented in the case of large scalar/pseudoscalar mixing.
330
331	<br/><br/><strong>HiggsBSM:all</strong> <input type="radio" name="22" value="on"><strong>On</strong>
332	<input type="radio" name="22" value="off" checked="checked"><strong>Off</strong>
333	(<code>default = <strong>off</strong></code>)<br/>
334	Common switch for the group of Higgs production beyond the Standard Model,
335	as listed below.
336
337
338	<h4>1) <i>h^0(H_1^0)</i> processes</h4>
339
340	<br/><br/><strong>HiggsBSM:allH1</strong> <input type="radio" name="23" value="on"><strong>On</strong>
341	<input type="radio" name="23" value="off" checked="checked"><strong>Off</strong>
342	(<code>default = <strong>off</strong></code>)<br/>
343	Common switch for the group of <i>h^0(H_1^0)</i> production processes.
344
345
346	<br/><br/><strong>HiggsBSM:ffbar2H1</strong> <input type="radio" name="24" value="on"><strong>On</strong>
347	<input type="radio" name="24" value="off" checked="checked"><strong>Off</strong>
348	(<code>default = <strong>off</strong></code>)<br/>
349	Scattering <i>f fbar -> h^0(H_1^0)</i>, where <i>f</i> sums over available
350	flavours except top.
351	Code 1001.
352
353
354	<br/><br/><strong>HiggsBSM:gg2H1</strong> <input type="radio" name="25" value="on"><strong>On</strong>
355	<input type="radio" name="25" value="off" checked="checked"><strong>Off</strong>
356	(<code>default = <strong>off</strong></code>)<br/>
357	Scattering <i>g g -> h^0(H_1^0)</i> via loop contributions primarily from
358	top.
359	Code 1002.
360
361
362	<br/><br/><strong>HiggsBSM:gmgm2H1</strong> <input type="radio" name="26" value="on"><strong>On</strong>
363	<input type="radio" name="26" value="off" checked="checked"><strong>Off</strong>
364	(<code>default = <strong>off</strong></code>)<br/>
365	Scattering <i>gamma gamma -> h^0(H_1^0)</i> via loop contributions
366	primarily from top and <i>W</i>.
367	Code 1003.
368
369
370	<br/><br/><strong>HiggsBSM:ffbar2H1Z</strong> <input type="radio" name="27" value="on"><strong>On</strong>
371	<input type="radio" name="27" value="off" checked="checked"><strong>Off</strong>
372	(<code>default = <strong>off</strong></code>)<br/>
373	Scattering <i>f fbar -> h^0(H_1^0) Z^0</i> via <i>s</i>-channel
374	<i>Z^0</i> exchange.
375	Code 1004.
376
377
378	<br/><br/><strong>HiggsBSM:ffbar2H1W</strong> <input type="radio" name="28" value="on"><strong>On</strong>
379	<input type="radio" name="28" value="off" checked="checked"><strong>Off</strong>
380	(<code>default = <strong>off</strong></code>)<br/>
381	Scattering <i>f fbar -> h^0(H_1^0) W^+-</i> via <i>s</i>-channel
382	<i>W^+-</i> exchange.
383	Code 1005.
384
385
386	<br/><br/><strong>HiggsBSM:ff2H1ff(t:ZZ)</strong> <input type="radio" name="29" value="on"><strong>On</strong>
387	<input type="radio" name="29" value="off" checked="checked"><strong>Off</strong>
388	(<code>default = <strong>off</strong></code>)<br/>
389	Scattering <i>f f' -> h^0(H_1^0) f f'</i> via <i>Z^0 Z^0</i> fusion.
390	Code 1006.
391
392
393	<br/><br/><strong>HiggsBSM:ff2H1ff(t:WW)</strong> <input type="radio" name="30" value="on"><strong>On</strong>
394	<input type="radio" name="30" value="off" checked="checked"><strong>Off</strong>
395	(<code>default = <strong>off</strong></code>)<br/>
396	Scattering <i>f_1 f_2 -> h^0(H_1^0) f_3 f_4</i> via <i>W^+ W^-</i>
397	fusion.
398	Code 1007.
399
400
401	<br/><br/><strong>HiggsBSM:gg2H1ttbar</strong> <input type="radio" name="31" value="on"><strong>On</strong>
402	<input type="radio" name="31" value="off" checked="checked"><strong>Off</strong>
403	(<code>default = <strong>off</strong></code>)<br/>
404	Scattering <i>g g -> h^0(H_1^0) t tbar</i> via <i>t tbar</i> fusion
405	(or, alternatively put, Higgs radiation off a top line).
406	Warning: unfortunately this process is rather slow, owing to a
407	lengthy cross-section expression and inefficient phase-space selection.
408	Code 1008.
409
410
411	<br/><br/><strong>HiggsBSM:qqbar2H1ttbar</strong> <input type="radio" name="32" value="on"><strong>On</strong>
412	<input type="radio" name="32" value="off" checked="checked"><strong>Off</strong>
413	(<code>default = <strong>off</strong></code>)<br/>
414	Scattering <i>q qbar -> h^0(H_1^0) t tbar</i> via <i>t tbar</i> fusion
415	(or, alternatively put, Higgs radiation off a top line).
416	Warning: unfortunately this process is rather slow, owing to a
417	lengthy cross-section expression and inefficient phase-space selection.
418	Code 1009.
419
420
421	<h4>2) <i>H^0(H_2^0)</i> processes</h4>
422
423	<br/><br/><strong>HiggsBSM:allH2</strong> <input type="radio" name="33" value="on"><strong>On</strong>
424	<input type="radio" name="33" value="off" checked="checked"><strong>Off</strong>
425	(<code>default = <strong>off</strong></code>)<br/>
426	Common switch for the group of <i>H^0(H_2^0)</i> production processes.
427
428
429	<br/><br/><strong>HiggsBSM:ffbar2H2</strong> <input type="radio" name="34" value="on"><strong>On</strong>
430	<input type="radio" name="34" value="off" checked="checked"><strong>Off</strong>
431	(<code>default = <strong>off</strong></code>)<br/>
432	Scattering <i>f fbar -> H^0(H_2^0)</i>, where <i>f</i> sums over available
433	flavours except top.
434	Code 1021.
435
436
437	<br/><br/><strong>HiggsBSM:gg2H2</strong> <input type="radio" name="35" value="on"><strong>On</strong>
438	<input type="radio" name="35" value="off" checked="checked"><strong>Off</strong>
439	(<code>default = <strong>off</strong></code>)<br/>
440	Scattering <i>g g -> H^0(H_2^0)</i> via loop contributions primarily from
441	top.
442	Code 1022.
443
444
445	<br/><br/><strong>HiggsBSM:gmgm2H2</strong> <input type="radio" name="36" value="on"><strong>On</strong>
446	<input type="radio" name="36" value="off" checked="checked"><strong>Off</strong>
447	(<code>default = <strong>off</strong></code>)<br/>
448	Scattering <i>gamma gamma -> H^0(H_2^0)</i> via loop contributions primarily
449	from top and <i>W</i>.
450	Code 1023.
451
452
453	<br/><br/><strong>HiggsBSM:ffbar2H2Z</strong> <input type="radio" name="37" value="on"><strong>On</strong>
454	<input type="radio" name="37" value="off" checked="checked"><strong>Off</strong>
455	(<code>default = <strong>off</strong></code>)<br/>
456	Scattering <i>f fbar -> H^0(H_2^0) Z^0</i> via <i>s</i>-channel
457	<i>Z^0</i> exchange.
458	Code 1024.
459
460
461	<br/><br/><strong>HiggsBSM:ffbar2H2W</strong> <input type="radio" name="38" value="on"><strong>On</strong>
462	<input type="radio" name="38" value="off" checked="checked"><strong>Off</strong>
463	(<code>default = <strong>off</strong></code>)<br/>
464	Scattering <i>f fbar -> H^0(H_2^0) W^+-</i> via <i>s</i>-channel
465	<i>W^+-</i> exchange.
466	Code 1025.
467
468
469	<br/><br/><strong>HiggsBSM:ff2H2ff(t:ZZ)</strong> <input type="radio" name="39" value="on"><strong>On</strong>
470	<input type="radio" name="39" value="off" checked="checked"><strong>Off</strong>
471	(<code>default = <strong>off</strong></code>)<br/>
472	Scattering <i>f f' -> H^0(H_2^0) f f'</i> via <i>Z^0 Z^0</i> fusion.
473	Code 1026.
474
475
476	<br/><br/><strong>HiggsBSM:ff2H2ff(t:WW)</strong> <input type="radio" name="40" value="on"><strong>On</strong>
477	<input type="radio" name="40" value="off" checked="checked"><strong>Off</strong>
478	(<code>default = <strong>off</strong></code>)<br/>
479	Scattering <i>f_1 f_2 -> H^0(H_2^0) f_3 f_4</i> via <i>W^+ W^-</i> fusion.
480	Code 1027.
481
482
483	<br/><br/><strong>HiggsBSM:gg2H2ttbar</strong> <input type="radio" name="41" value="on"><strong>On</strong>
484	<input type="radio" name="41" value="off" checked="checked"><strong>Off</strong>
485	(<code>default = <strong>off</strong></code>)<br/>
486	Scattering <i>g g -> H^0(H_2^0) t tbar</i> via <i>t tbar</i> fusion
487	(or, alternatively put, Higgs radiation off a top line).
488	Warning: unfortunately this process is rather slow, owing to a
489	lengthy cross-section expression and inefficient phase-space selection.
490	Code 1028.
491
492
493	<br/><br/><strong>HiggsBSM:qqbar2H2ttbar</strong> <input type="radio" name="42" value="on"><strong>On</strong>
494	<input type="radio" name="42" value="off" checked="checked"><strong>Off</strong>
495	(<code>default = <strong>off</strong></code>)<br/>
496	Scattering <i>q qbar -> H^0(H_2^0) t tbar</i> via <i>t tbar</i> fusion
497	(or, alternatively put, Higgs radiation off a top line).
498	Warning: unfortunately this process is rather slow, owing to a
499	lengthy cross-section expression and inefficient phase-space selection.
500	Code 1029.
501
502	<h4>3) <i>A^0(H_3^0)</i> processes</h4>
503
504	<br/><br/><strong>HiggsBSM:allA3</strong> <input type="radio" name="43" value="on"><strong>On</strong>
505	<input type="radio" name="43" value="off" checked="checked"><strong>Off</strong>
506	(<code>default = <strong>off</strong></code>)<br/>
507	Common switch for the group of <i>A^0(H_3^0)</i> production processes.
508
509
510	<br/><br/><strong>HiggsBSM:ffbar2A3</strong> <input type="radio" name="44" value="on"><strong>On</strong>
511	<input type="radio" name="44" value="off" checked="checked"><strong>Off</strong>
512	(<code>default = <strong>off</strong></code>)<br/>
513	Scattering <i>f fbar -> A^0(H_3^0)</i>, where <i>f</i> sums over available
514	flavours except top.
515	Code 1041.
516
517
518	<br/><br/><strong>HiggsBSM:gg2A3</strong> <input type="radio" name="45" value="on"><strong>On</strong>
519	<input type="radio" name="45" value="off" checked="checked"><strong>Off</strong>
520	(<code>default = <strong>off</strong></code>)<br/>
521	Scattering <i>g g -> A^0(A_3^0)</i> via loop contributions primarily from
522	top.
523	Code 1042.
524
525
526	<br/><br/><strong>HiggsBSM:gmgm2A3</strong> <input type="radio" name="46" value="on"><strong>On</strong>
527	<input type="radio" name="46" value="off" checked="checked"><strong>Off</strong>
528	(<code>default = <strong>off</strong></code>)<br/>
529	Scattering <i>gamma gamma -> A^0(A_3^0)</i> via loop contributions primarily
530	from top and <i>W</i>.
531	Code 1043.
532
533
534	<br/><br/><strong>HiggsBSM:ffbar2A3Z</strong> <input type="radio" name="47" value="on"><strong>On</strong>
535	<input type="radio" name="47" value="off" checked="checked"><strong>Off</strong>
536	(<code>default = <strong>off</strong></code>)<br/>
537	Scattering <i>f fbar -> A^0(A_3^0) Z^0</i> via <i>s</i>-channel
538	<i>Z^0</i> exchange.
539	Code 1044.
540
541
542	<br/><br/><strong>HiggsBSM:ffbar2A3W</strong> <input type="radio" name="48" value="on"><strong>On</strong>
543	<input type="radio" name="48" value="off" checked="checked"><strong>Off</strong>
544	(<code>default = <strong>off</strong></code>)<br/>
545	Scattering <i>f fbar -> A^0(A_3^0) W^+-</i> via <i>s</i>-channel
546	<i>W^+-</i> exchange.
547	Code 1045.
548
549
550	<br/><br/><strong>HiggsBSM:ff2A3ff(t:ZZ)</strong> <input type="radio" name="49" value="on"><strong>On</strong>
551	<input type="radio" name="49" value="off" checked="checked"><strong>Off</strong>
552	(<code>default = <strong>off</strong></code>)<br/>
553	Scattering <i>f f' -> A^0(A_3^0) f f'</i> via <i>Z^0 Z^0</i> fusion.
554	Code 1046.
555
556
557	<br/><br/><strong>HiggsBSM:ff2A3ff(t:WW)</strong> <input type="radio" name="50" value="on"><strong>On</strong>
558	<input type="radio" name="50" value="off" checked="checked"><strong>Off</strong>
559	(<code>default = <strong>off</strong></code>)<br/>
560	Scattering <i>f_1 f_2 -> A^0(A_3^0) f_3 f_4</i> via <i>W^+ W^-</i> fusion.
561	Code 1047.
562
563
564	<br/><br/><strong>HiggsBSM:gg2A3ttbar</strong> <input type="radio" name="51" value="on"><strong>On</strong>
565	<input type="radio" name="51" value="off" checked="checked"><strong>Off</strong>
566	(<code>default = <strong>off</strong></code>)<br/>
567	Scattering <i>g g -> A^0(A_3^0) t tbar</i> via <i>t tbar</i> fusion
568	(or, alternatively put, Higgs radiation off a top line).
569	Warning: unfortunately this process is rather slow, owing to a
570	lengthy cross-section expression and inefficient phase-space selection.
571	Code 1048.
572
573
574	<br/><br/><strong>HiggsBSM:qqbar2A3ttbar</strong> <input type="radio" name="52" value="on"><strong>On</strong>
575	<input type="radio" name="52" value="off" checked="checked"><strong>Off</strong>
576	(<code>default = <strong>off</strong></code>)<br/>
577	Scattering <i>q qbar -> A^0(A_3^0) t tbar</i> via <i>t tbar</i> fusion
578	(or, alternatively put, Higgs radiation off a top line).
579	Warning: unfortunately this process is rather slow, owing to a
580	lengthy cross-section expression and inefficient phase-space selection.
581	Code 1049.
582
583	<h4>4) <i>H+-</i> processes</h4>
584
585	<br/><br/><strong>HiggsBSM:allH+-</strong> <input type="radio" name="53" value="on"><strong>On</strong>
586	<input type="radio" name="53" value="off" checked="checked"><strong>Off</strong>
587	(<code>default = <strong>off</strong></code>)<br/>
588	Common switch for the group of <i>H^+-</i> production processes.
589
590
591	<br/><br/><strong>HiggsBSM:ffbar2H+-</strong> <input type="radio" name="54" value="on"><strong>On</strong>
592	<input type="radio" name="54" value="off" checked="checked"><strong>Off</strong>
593	(<code>default = <strong>off</strong></code>)<br/>
594	Scattering <i>f fbar' -> H^+-</i>, where <i>f, fbar'</i> sums over
595	available incoming flavours. Since couplings are assumed
596	generation-diagonal, in practice this means <i>c sbar -> H^+</i>
597	and <i>s cbar -> H^-</i>.
598	Code 1061.
599
600
601	<br/><br/><strong>HiggsBSM:bg2H+-t</strong> <input type="radio" name="55" value="on"><strong>On</strong>
602	<input type="radio" name="55" value="off" checked="checked"><strong>Off</strong>
603	(<code>default = <strong>off</strong></code>)<br/>
604	Scattering <i>b g -> H^+ tbar</i>. At hadron colliders this is the
605	dominant process for single-charged-Higgs production.
606	Code 1062.
607
608
609	<h4>5) Higgs-pair processes</h4>
610
611	<br/><br/><strong>HiggsBSM:allHpair</strong> <input type="radio" name="56" value="on"><strong>On</strong>
612	<input type="radio" name="56" value="off" checked="checked"><strong>Off</strong>
613	(<code>default = <strong>off</strong></code>)<br/>
614	Common switch for the group of Higgs pair-production processes.
615
616
617	<br/><br/><strong>HiggsBSM:ffbar2A3H1</strong> <input type="radio" name="57" value="on"><strong>On</strong>
618	<input type="radio" name="57" value="off" checked="checked"><strong>Off</strong>
619	(<code>default = <strong>off</strong></code>)<br/>
620	Scattering <i>f fbar -> A^0(H_3) h^0(H_1)</i>.
621	Code 1081.
622
623
624	<br/><br/><strong>HiggsBSM:ffbar2A3H2</strong> <input type="radio" name="58" value="on"><strong>On</strong>
625	<input type="radio" name="58" value="off" checked="checked"><strong>Off</strong>
626	(<code>default = <strong>off</strong></code>)<br/>
627	Scattering <i>f fbar -> A^0(H_3) H^0(H_2)</i>.
628	Code 1082.
629
630
631	<br/><br/><strong>HiggsBSM:ffbar2H+-H1</strong> <input type="radio" name="59" value="on"><strong>On</strong>
632	<input type="radio" name="59" value="off" checked="checked"><strong>Off</strong>
633	(<code>default = <strong>off</strong></code>)<br/>
634	Scattering <i>f fbar -> H^+- h^0(H_1)</i>.
635	Code 1083.
636
637
638	<br/><br/><strong>HiggsBSM:ffbar2H+-H2</strong> <input type="radio" name="60" value="on"><strong>On</strong>
639	<input type="radio" name="60" value="off" checked="checked"><strong>Off</strong>
640	(<code>default = <strong>off</strong></code>)<br/>
641	Scattering <i>f fbar -> H^+- H^0(H_2)</i>.
642	Code 1084.
643
644
645	<br/><br/><strong>HiggsBSM:ffbar2H+H-</strong> <input type="radio" name="61" value="on"><strong>On</strong>
646	<input type="radio" name="61" value="off" checked="checked"><strong>Off</strong>
647	(<code>default = <strong>off</strong></code>)<br/>
648	Scattering <i>f fbar -> H+ H-</i>.
649	Code 1085.
650
651
652	<h3>Beyond-the-Standard-Model Higgs, further processes</h3>
653
654	This section mimics the above section on "Standard-Model Higgs,
655	further processes", i.e. it contains higher-order corrections
656	to the processes already listed. The two sets therefore could not
657	be used simultaneously without unphysical doublecounting.
658	They are not controlled by any group flag, but have to be switched
659	on for each separate process after due consideration. We refer to
660	the standard-model description for a set of further comments on
661	the processes.
662
663	<h4>1) <i>h^0(H_1^0)</i> processes</h4>
664
665	<br/><br/><strong>HiggsBSM:qg2H1q</strong> <input type="radio" name="62" value="on"><strong>On</strong>
666	<input type="radio" name="62" value="off" checked="checked"><strong>Off</strong>
667	(<code>default = <strong>off</strong></code>)<br/>
668	Scattering <i>q g -> h^0 q</i>. This process gives first-order
669	corrections to the <i>f fbar -> h^0</i> one above, and should only be
670	used to study the high-<i>pT</i> tail, while <i>f fbar -> h^0</i>
671	should be used for inclusive production. Only the dominant <i>c</i>
672	and <i>b</i> contributions are included, and generated separately
673	for technical reasons. Note that another first-order process would be
674	<i>q qbar -> h^0 g</i>, which is not explicitly implemented here,
675	but is obtained from showering off the lowest-order process. It does not
676	contain any <i>b</i> at large <i>pT</i>, however, so is less
677	interesting for many applications.
678	Code 1011.
679
680
681	<br/><br/><strong>HiggsBSM:gg2H1bbbar</strong> <input type="radio" name="63" value="on"><strong>On</strong>
682	<input type="radio" name="63" value="off" checked="checked"><strong>Off</strong>
683	(<code>default = <strong>off</strong></code>)<br/>
684	Scattering <i>g g -> h^0 b bbar</i>. This process is yet one order
685	higher of the <i>b bbar -> h^0</i> and <i>b g -> h^0 b</i> chain,
686	where now two quarks should be required above some large <i>pT</i>
687	threshold.
688	Warning: unfortunately this process is rather slow, owing to a
689	lengthy cross-section expression and inefficient phase-space selection.
690	Code 1012.
691
692
693	<br/><br/><strong>HiggsBSM:qqbar2H1bbbar</strong> <input type="radio" name="64" value="on"><strong>On</strong>
694	<input type="radio" name="64" value="off" checked="checked"><strong>Off</strong>
695	(<code>default = <strong>off</strong></code>)<br/>
696	Scattering <i>q qbar -> h^0 b bbar</i> via an <i>s</i>-channel
697	gluon, so closely related to the previous one, but typically less
698	important owing to the smaller rate of (anti)quarks relative to
699	gluons.
700	Warning: unfortunately this process is rather slow, owing to a
701	lengthy cross-section expression and inefficient phase-space selection.
702	Code 1013.
703
704
705	<br/><br/><strong>HiggsBSM:gg2H1g(l:t)</strong> <input type="radio" name="65" value="on"><strong>On</strong>
706	<input type="radio" name="65" value="off" checked="checked"><strong>Off</strong>
707	(<code>default = <strong>off</strong></code>)<br/>
708	Scattering <i>g g -> h^0 g</i> via loop contributions primarily
709	from top.
710	Code 1014.
711
712
713	<br/><br/><strong>HiggsBSM:qg2H1q(l:t)</strong> <input type="radio" name="66" value="on"><strong>On</strong>
714	<input type="radio" name="66" value="off" checked="checked"><strong>Off</strong>
715	(<code>default = <strong>off</strong></code>)<br/>
716	Scattering <i>q g -> h^0 q</i> via loop contributions primarily
717	from top. Not to be confused with the <code>HiggsBSM:qg2H1q</code>
718	process above, with its direct fermion-to-Higgs coupling.
719	Code 1015.
720
721
722	<br/><br/><strong>HiggsBSM:qqbar2H1g(l:t)</strong> <input type="radio" name="67" value="on"><strong>On</strong>
723	<input type="radio" name="67" value="off" checked="checked"><strong>Off</strong>
724	(<code>default = <strong>off</strong></code>)<br/>
725	Scattering <i>q qbar -> h^0 g</i> via an <i>s</i>-channel gluon
726	and loop contributions primarily from top. Is strictly speaking a
727	"new" process, not directly derived from <i>g g -> h^0</i>, and
728	could therefore be included in the standard mix without doublecounting,
729	but is numerically negligible.
730	Code 1016.
731
732
733	<h4>2) <i>H^0(H_2^0)</i> processes</h4>
734
735	<br/><br/><strong>HiggsBSM:qg2H2q</strong> <input type="radio" name="68" value="on"><strong>On</strong>
736	<input type="radio" name="68" value="off" checked="checked"><strong>Off</strong>
737	(<code>default = <strong>off</strong></code>)<br/>
738	Scattering <i>q g -> H^0 q</i>. This process gives first-order
739	corrections to the <i>f fbar -> H^0</i> one above, and should only be
740	used to study the high-<i>pT</i> tail, while <i>f fbar -> H^0</i>
741	should be used for inclusive production. Only the dominant <i>c</i>
742	and <i>b</i> contributions are included, and generated separately
743	for technical reasons. Note that another first-order process would be
744	<i>q qbar -> H^0 g</i>, which is not explicitly implemented here,
745	but is obtained from showering off the lowest-order process. It does not
746	contain any <i>b</i> at large <i>pT</i>, however, so is less
747	interesting for many applications.
748	Code 1031.
749
750
751	<br/><br/><strong>HiggsBSM:gg2H2bbbar</strong> <input type="radio" name="69" value="on"><strong>On</strong>
752	<input type="radio" name="69" value="off" checked="checked"><strong>Off</strong>
753	(<code>default = <strong>off</strong></code>)<br/>
754	Scattering <i>g g -> H^0 b bbar</i>. This process is yet one order
755	higher of the <i>b bbar -> H^0</i> and <i>b g -> H^0 b</i> chain,
756	where now two quarks should be required above some large <i>pT</i>
757	threshold.
758	Warning: unfortunately this process is rather slow, owing to a
759	lengthy cross-section expression and inefficient phase-space selection.
760	Code 1032.
761
762
763	<br/><br/><strong>HiggsBSM:qqbar2H2bbbar</strong> <input type="radio" name="70" value="on"><strong>On</strong>
764	<input type="radio" name="70" value="off" checked="checked"><strong>Off</strong>
765	(<code>default = <strong>off</strong></code>)<br/>
766	Scattering <i>q qbar -> H^0 b bbar</i> via an <i>s</i>-channel
767	gluon, so closely related to the previous one, but typically less
768	important owing to the smaller rate of (anti)quarks relative to
769	gluons.
770	Warning: unfortunately this process is rather slow, owing to a
771	lengthy cross-section expression and inefficient phase-space selection.
772	Code 1033.
773
774
775	<br/><br/><strong>HiggsBSM:gg2H2g(l:t)</strong> <input type="radio" name="71" value="on"><strong>On</strong>
776	<input type="radio" name="71" value="off" checked="checked"><strong>Off</strong>
777	(<code>default = <strong>off</strong></code>)<br/>
778	Scattering <i>g g -> H^0 g</i> via loop contributions primarily
779	from top.
780	Code 1034.
781
782
783	<br/><br/><strong>HiggsBSM:qg2H2q(l:t)</strong> <input type="radio" name="72" value="on"><strong>On</strong>
784	<input type="radio" name="72" value="off" checked="checked"><strong>Off</strong>
785	(<code>default = <strong>off</strong></code>)<br/>
786	Scattering <i>q g -> H^0 q</i> via loop contributions primarily
787	from top. Not to be confused with the <code>HiggsBSM:qg2H1q</code>
788	process above, with its direct fermion-to-Higgs coupling.
789	Code 1035.
790
791
792	<br/><br/><strong>HiggsBSM:qqbar2H2g(l:t)</strong> <input type="radio" name="73" value="on"><strong>On</strong>
793	<input type="radio" name="73" value="off" checked="checked"><strong>Off</strong>
794	(<code>default = <strong>off</strong></code>)<br/>
795	Scattering <i>q qbar -> H^0 g</i> via an <i>s</i>-channel gluon
796	and loop contributions primarily from top. Is strictly speaking a
797	"new" process, not directly derived from <i>g g -> H^0</i>, and
798	could therefore be included in the standard mix without doublecounting,
799	but is numerically negligible.
800	Code 1036.
801
802
803	<h4>3) <i>A^0(H_3^0)</i> processes</h4>
804
805	<br/><br/><strong>HiggsBSM:qg2A3q</strong> <input type="radio" name="74" value="on"><strong>On</strong>
806	<input type="radio" name="74" value="off" checked="checked"><strong>Off</strong>
807	(<code>default = <strong>off</strong></code>)<br/>
808	Scattering <i>q g -> A^0 q</i>. This process gives first-order
809	corrections to the <i>f fbar -> A^0</i> one above, and should only be
810	used to study the high-<i>pT</i> tail, while <i>f fbar -> A^0</i>
811	should be used for inclusive production. Only the dominant <i>c</i>
812	and <i>b</i> contributions are included, and generated separately
813	for technical reasons. Note that another first-order process would be
814	<i>q qbar -> A^0 g</i>, which is not explicitly implemented here,
815	but is obtained from showering off the lowest-order process. It does not
816	contain any <i>b</i> at large <i>pT</i>, however, so is less
817	interesting for many applications.
818	Code 1051.
819
820
821	<br/><br/><strong>HiggsBSM:gg2A3bbbar</strong> <input type="radio" name="75" value="on"><strong>On</strong>
822	<input type="radio" name="75" value="off" checked="checked"><strong>Off</strong>
823	(<code>default = <strong>off</strong></code>)<br/>
824	Scattering <i>g g -> A^0 b bbar</i>. This process is yet one order
825	higher of the <i>b bbar -> A^0</i> and <i>b g -> A^0 b</i> chain,
826	where now two quarks should be required above some large <i>pT</i>
827	threshold.
828	Warning: unfortunately this process is rather slow, owing to a
829	lengthy cross-section expression and inefficient phase-space selection.
830	Code 1052.
831
832
833	<br/><br/><strong>HiggsBSM:qqbar2A3bbbar</strong> <input type="radio" name="76" value="on"><strong>On</strong>
834	<input type="radio" name="76" value="off" checked="checked"><strong>Off</strong>
835	(<code>default = <strong>off</strong></code>)<br/>
836	Scattering <i>q qbar -> A^0 b bbar</i> via an <i>s</i>-channel
837	gluon, so closely related to the previous one, but typically less
838	important owing to the smaller rate of (anti)quarks relative to
839	gluons.
840	Warning: unfortunately this process is rather slow, owing to a
841	lengthy cross-section expression and inefficient phase-space selection.
842	Code 1053.
843
844
845	<br/><br/><strong>HiggsBSM:gg2A3g(l:t)</strong> <input type="radio" name="77" value="on"><strong>On</strong>
846	<input type="radio" name="77" value="off" checked="checked"><strong>Off</strong>
847	(<code>default = <strong>off</strong></code>)<br/>
848	Scattering <i>g g -> A^0 g</i> via loop contributions primarily
849	from top.
850	Code 1054.
851
852
853	<br/><br/><strong>HiggsBSM:qg2A3q(l:t)</strong> <input type="radio" name="78" value="on"><strong>On</strong>
854	<input type="radio" name="78" value="off" checked="checked"><strong>Off</strong>
855	(<code>default = <strong>off</strong></code>)<br/>
856	Scattering <i>q g -> A^0 q</i> via loop contributions primarily
857	from top. Not to be confused with the <code>HiggsBSM:qg2H1q</code>
858	process above, with its direct fermion-to-Higgs coupling.
859	Code 1055.
860
861
862	<br/><br/><strong>HiggsBSM:qqbar2A3g(l:t)</strong> <input type="radio" name="79" value="on"><strong>On</strong>
863	<input type="radio" name="79" value="off" checked="checked"><strong>Off</strong>
864	(<code>default = <strong>off</strong></code>)<br/>
865	Scattering <i>q qbar -> A^0 g</i> via an <i>s</i>-channel gluon
866	and loop contributions primarily from top. Is strictly speaking a
867	"new" process, not directly derived from <i>g g -> A^0</i>, and
868	could therefore be included in the standard mix without doublecounting,
869	but is numerically negligible.
870	Code 1056.
871
872
873	<h3>Parameters for Beyond-the-Standard-Model Higgs production and decay</h3>
874
875	This section offers a big flexibility to set couplings of the various
876	Higgs states to fermions and gauge bosons, and also to each other.
877	The intention is that, for scenarios like MSSM, you should use standard
878	input from the <?php $filepath = $_GET["filepath"];
879	echo "<a href='SUSYLesHouchesAccord.php?filepath=".$filepath."' target='page'>";?>SUSY Les Houches
880	Accord</a>, rather than having to set it all yourself. In other cases,
881	however, the freedom is there for you to use. Kindly note that some
882	of the internal calculations of partial widths from the parameters provided
883	do not include mixing between the scalar and pseudoscalar states.
884
885	<p/>
886	Masses would be set in the <code>ParticleData</code> database,
887	while couplings are set below. When possible, the couplings of the Higgs
888	states are normalized to the corresponding coupling within the SM.
889	When not, their values within the MSSM are indicated, from which
890	it should be straightforward to understand what to use instead.
891	The exception is some couplings that vanish also in the MSSM, where the
892	normalization has been defined in close analogy with nonvanishing ones.
893	Some parameter names are asymmetric but crossing can always be used,
894	i.e. the coupling for <i>A^0 -> H^0 Z^0</i> obviously is also valid
895	for <i>H^0 -> A^0 Z^0</i> and <i>Z^0 -> H^0 A^0</i>.
896	Note that couplings usually appear quadratically in matrix elements.
897
898	<br/><br/><table><tr><td><strong>HiggsH1:coup2d </td><td></td><td> <input type="text" name="80" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
899	The <i>h^0(H_1^0)</i> coupling to down-type quarks.
900
901
902	<br/><br/><table><tr><td><strong>HiggsH1:coup2u </td><td></td><td> <input type="text" name="81" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
903	The <i>h^0(H_1^0)</i> coupling to up-type quarks.
904
905
906	<br/><br/><table><tr><td><strong>HiggsH1:coup2l </td><td></td><td> <input type="text" name="82" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
907	The <i>h^0(H_1^0)</i> coupling to (charged) leptons.
908
909
910	<br/><br/><table><tr><td><strong>HiggsH1:coup2Z </td><td></td><td> <input type="text" name="83" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
911	The <i>h^0(H_1^0)</i> coupling to <i>Z^0</i>.
912
913
914	<br/><br/><table><tr><td><strong>HiggsH1:coup2W </td><td></td><td> <input type="text" name="84" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
915	The <i>h^0(H_1^0)</i> coupling to <i>W^+-</i>.
916
917
918	<br/><br/><table><tr><td><strong>HiggsH1:coup2Hchg </td><td></td><td> <input type="text" name="85" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
919	The <i>h^0(H_1^0)</i> coupling to <i>H^+-</i> (in loops).
920	Is <i>sin(beta - alpha) + cos(2 beta) sin(beta + alpha) /
921	(2 cos^2theta_W)</i> in the MSSM.
922
923
924	<br/><br/><table><tr><td><strong>HiggsH2:coup2d </td><td></td><td> <input type="text" name="86" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
925	The <i>H^0(H_2^0)</i> coupling to down-type quarks.
926
927
928	<br/><br/><table><tr><td><strong>HiggsH2:coup2u </td><td></td><td> <input type="text" name="87" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
929	The <i>H^0(H_2^0)</i> coupling to up-type quarks.
930
931
932	<br/><br/><table><tr><td><strong>HiggsH2:coup2l </td><td></td><td> <input type="text" name="88" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
933	The <i>H^0(H_2^0)</i> coupling to (charged) leptons.
934
935
936	<br/><br/><table><tr><td><strong>HiggsH2:coup2Z </td><td></td><td> <input type="text" name="89" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
937	The <i>H^0(H_2^0)</i> coupling to <i>Z^0</i>.
938
939
940	<br/><br/><table><tr><td><strong>HiggsH2:coup2W </td><td></td><td> <input type="text" name="90" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
941	The <i>H^0(H_2^0)</i> coupling to <i>W^+-</i>.
942
943
944	<br/><br/><table><tr><td><strong>HiggsH2:coup2Hchg </td><td></td><td> <input type="text" name="91" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
945	The <i>H^0(H_2^0)</i> coupling to <i>H^+-</i> (in loops).
946	Is <i>cos(beta - alpha) + cos(2 beta) cos(beta + alpha) /
947	(2 cos^2theta_W)</i> in the MSSM.
948
949
950	<br/><br/><table><tr><td><strong>HiggsH2:coup2H1H1 </td><td></td><td> <input type="text" name="92" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
951	The <i>H^0(H_2^0)</i> coupling to a <i>h^0(H_1^0)</i> pair.
952	Is <i>cos(2 alpha) cos(beta + alpha) - 2 sin(2 alpha)
953	sin(beta + alpha)</i> in the MSSM.
954
955
956	<br/><br/><table><tr><td><strong>HiggsH2:coup2A3A3 </td><td></td><td> <input type="text" name="93" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
957	The <i>H^0(H_2^0)</i> coupling to an <i>A^0(H_3^0)</i> pair.
958	Is <i>cos(2 beta) cos(beta + alpha)</i> in the MSSM.
959
960
961	<br/><br/><table><tr><td><strong>HiggsH2:coup2H1Z </td><td></td><td> <input type="text" name="94" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
962	The <i>H^0(H_2^0)</i> coupling to a <i>h^0(H_1^0) Z^0</i> pair.
963	Vanishes in the MSSM.
964
965
966	<br/><br/><table><tr><td><strong>HiggsH2:coup2A3H1 </td><td></td><td> <input type="text" name="95" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
967	The <i>H^0(H_2^0)</i> coupling to an <i>A^0(H_3^0) h^0(H_1^0)</i> pair.
968	Vanishes in the MSSM.
969
970
971	<br/><br/><table><tr><td><strong>HiggsH2:coup2HchgW </td><td></td><td> <input type="text" name="96" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
972	The <i>H^0(H_2^0)</i> coupling to a <i>H^+- W-+</i> pair.
973	Is <i>sin(beta - alpha)</i> in the MSSM.
974
975
976	<br/><br/><table><tr><td><strong>HiggsA3:coup2d </td><td></td><td> <input type="text" name="97" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
977	The <i>A^0(H_3^0)</i> coupling to down-type quarks.
978
979
980	<br/><br/><table><tr><td><strong>HiggsA3:coup2u </td><td></td><td> <input type="text" name="98" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
981	The <i>A^0(H_3^0)</i> coupling to up-type quarks.
982
983
984	<br/><br/><table><tr><td><strong>HiggsA3:coup2l </td><td></td><td> <input type="text" name="99" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
985	The <i>A^0(H_3^0)</i> coupling to (charged) leptons.
986
987
988	<br/><br/><table><tr><td><strong>HiggsA3:coup2H1Z </td><td></td><td> <input type="text" name="100" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
989	The <i>A^0(H_3^0)</i> coupling to a <i>h^0(H_1^0) Z^0</i> pair.
990	Is <i>cos(beta - alpha)</i> in the MSSM.
991
992
993	<br/><br/><table><tr><td><strong>HiggsA3:coup2H2Z </td><td></td><td> <input type="text" name="101" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
994	The <i>A^0(H_3^0)</i> coupling to a <i>H^0(H_2^0) Z^0</i> pair.
995	Is <i>sin(beta - alpha)</i> in the MSSM.
996
997
998	<br/><br/><table><tr><td><strong>HiggsA3:coup2Z </td><td></td><td> <input type="text" name="102" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
999	The <i>A^0(H_3^0)</i> coupling to <i>Z^0</i>.
1000	Vanishes in the MSSM.
1001
1002
1003	<br/><br/><table><tr><td><strong>HiggsA3:coup2W </td><td></td><td> <input type="text" name="103" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
1004	The <i>A^0(H_3^0)</i> coupling to <i>W^+-</i>.
1005	Vanishes in the MSSM.
1006
1007
1008	<br/><br/><table><tr><td><strong>HiggsA3:coup2H1H1 </td><td></td><td> <input type="text" name="104" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
1009	The <i>A^0(H_3^0)</i> coupling to a <i>h^0(H_1^0)</i> pair.
1010	Vanishes in the MSSM.
1011
1012
1013	<br/><br/><table><tr><td><strong>HiggsA3:coup2Hchg </td><td></td><td> <input type="text" name="105" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
1014	The <i>A^0(H_3^0)</i> coupling to <i>H^+-</i>.
1015	Vanishes in the MSSM.
1016
1017
1018	<br/><br/><table><tr><td><strong>HiggsA3:coup2HchgW </td><td></td><td> <input type="text" name="106" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
1019	The <i>A^0(H_3^0)</i> coupling to a <i>H^+- W-+</i> pair.
1020	Is 1 in the MSSM.
1021
1022
1023	<br/><br/><table><tr><td><strong>HiggsHchg:tanBeta </td><td></td><td> <input type="text" name="107" value="5." size="20"/>   (<code>default = <strong>5.</strong></code>)</td></tr></table>
1024	The <i>tan(beta)</i> value, which leads to an enhancement of the
1025	<i>H^+-</i> coupling to down-type fermions and suppression to
1026	up-type ones. The same angle also appears in many other places,
1027	but this particular parameter is only used for the charged-Higgs case.
1028
1029
1030	<br/><br/><table><tr><td><strong>HiggsHchg:coup2H1W </td><td></td><td> <input type="text" name="108" value="1." size="20"/>   (<code>default = <strong>1.</strong></code>)</td></tr></table>
1031	The <i>H^+-</i> coupling to a <i>h^0(H_1^0) W^+-</i> pair.
1032	Is <i>cos(beta - alpha)</i> in the MSSM.
1033
1034
1035	<br/><br/><table><tr><td><strong>HiggsHchg:coup2H2W </td><td></td><td> <input type="text" name="109" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
1036	The <i>H^+-</i> coupling to a <i>H^0(H_2^0) W^+-</i> pair.
1037	Is <i>sin(beta - alpha)</i> in the MSSM.
1038
1039
1040	<p/>
1041	Another set of parameters are not used in the production stage but
1042	exclusively for the description of angular distributions in decays.
1043
1044	<br/><br/><table><tr><td><strong>HiggsH1:parity </td><td>   (<code>default = <strong>1</strong></code>; <code>minimum = 0</code>; <code>maximum = 3</code>)</td></tr></table>
1045	possibility to modify angular decay correlations in the decay of a
1046	<ei>h^0(H_1)</ei> decay <ei>Z^0 Z^0</ei> or <ei>W^+ W^-</ei> to four
1047	fermions. Currently it does not affect the partial width of the
1048	channels, which is only based on the above parameters.
1049	<br/>
1050	<input type="radio" name="110" value="0"><strong>0 </strong>: isotropic decays.<br/>
1051	<input type="radio" name="110" value="1" checked="checked"><strong>1 </strong>: assuming the <ei>h^0(H_1)</ei> is a pure scalar (CP-even), as in the MSSM.<br/>
1052	<input type="radio" name="110" value="2"><strong>2 </strong>: assuming the <ei>h^0(H_1)</ei> is a pure pseudoscalar (CP-odd).<br/>
1053	<input type="radio" name="110" value="3"><strong>3 </strong>: assuming the <ei>h^0(H_1)</ei> is a mixture of the two, including the CP-violating interference term. The parameter <ei>eta</ei>, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to <ei>eta</ei> and the CP-odd one to <ei>eta^2</ei>.<br/>
1054
1055	<br/><br/><table><tr><td><strong>HiggsH1:etaParity </td><td></td><td> <input type="text" name="111" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
1056	The <i>eta</i> value of CP-violation in the
1057	<code>HiggsSM:parity = 3</code> option.
1058
1059
1060	<br/><br/><table><tr><td><strong>HiggsH2:parity </td><td>   (<code>default = <strong>1</strong></code>; <code>minimum = 0</code>; <code>maximum = 3</code>)</td></tr></table>
1061	possibility to modify angular decay correlations in the decay of a
1062	<ei>H^0(H_2)</ei> decay <ei>Z^0 Z^0</ei> or <ei>W^+ W^-</ei> to four
1063	fermions. Currently it does not affect the partial width of the
1064	channels, which is only based on the above parameters.
1065	<br/>
1066	<input type="radio" name="112" value="0"><strong>0 </strong>: isotropic decays.<br/>
1067	<input type="radio" name="112" value="1" checked="checked"><strong>1 </strong>: assuming the <ei>H^0(H_2)</ei> is a pure scalar (CP-even), as in the MSSM.<br/>
1068	<input type="radio" name="112" value="2"><strong>2 </strong>: assuming the <ei>H^0(H_2)</ei> is a pure pseudoscalar (CP-odd).<br/>
1069	<input type="radio" name="112" value="3"><strong>3 </strong>: assuming the <ei>H^0(H_2)</ei> is a mixture of the two, including the CP-violating interference term. The parameter <ei>eta</ei>, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to <ei>eta</ei> and the CP-odd one to <ei>eta^2</ei>.<br/>
1070
1071	<br/><br/><table><tr><td><strong>HiggsH2:etaParity </td><td></td><td> <input type="text" name="113" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
1072	The <i>eta</i> value of CP-violation in the
1073	<code>HiggsSM:parity = 3</code> option.
1074
1075
1076	<br/><br/><table><tr><td><strong>HiggsA3:parity </td><td>   (<code>default = <strong>2</strong></code>; <code>minimum = 0</code>; <code>maximum = 3</code>)</td></tr></table>
1077	possibility to modify angular decay correlations in the decay of a
1078	<ei>A^0(H_3)</ei> decay <ei>Z^0 Z^0</ei> or <ei>W^+ W^-</ei> to four
1079	fermions. Currently it does not affect the partial width of the
1080	channels, which is only based on the above parameters.
1081	<br/>
1082	<input type="radio" name="114" value="0"><strong>0 </strong>: isotropic decays.<br/>
1083	<input type="radio" name="114" value="1"><strong>1 </strong>: assuming the <ei>A^0(H_3)</ei> is a pure scalar (CP-even).<br/>
1084	<input type="radio" name="114" value="2" checked="checked"><strong>2 </strong>: assuming the <ei>A^0(H_3)</ei> is a pure pseudoscalar (CP-odd), as in the MSSM.<br/>
1085	<input type="radio" name="114" value="3"><strong>3 </strong>: assuming the <ei>A^0(H_3)</ei> is a mixture of the two, including the CP-violating interference term. The parameter <ei>eta</ei>, see below, sets the strength of the CP-odd admixture, with the interference term being proportional to <ei>eta</ei> and the CP-odd one to <ei>eta^2</ei>.<br/>
1086
1087	<br/><br/><table><tr><td><strong>HiggsA3:etaParity </td><td></td><td> <input type="text" name="115" value="0." size="20"/>   (<code>default = <strong>0.</strong></code>)</td></tr></table>
1088	The <i>eta</i> value of CP-violation in the
1089	<code>HiggsSM:parity = 3</code> option.
1090
1091
1092	<input type="hidden" name="saved" value="1"/>
1093
1094	<?php
1095	echo "<input type='hidden' name='filepath' value='".$_GET["filepath"]."'/>"?>
1096
1097	<table width="100%"><tr><td align="right"><input type="submit" value="Save Settings" /></td></tr></table>
1098	</form>
1099
1100	<?php
1101
1102	if($_POST["saved"] == 1)
1103	{
1104	$filepath = $_POST["filepath"];
1105	$handle = fopen($filepath, 'a');
1106
1107	if($_POST["1"] != "off")
1108	{
1109	$data = "Higgs:cubicWidth = ".$_POST["1"]."\n";
1110	fwrite($handle,$data);
1111	}
1112	if($_POST["2"] != "on")
1113	{
1114	$data = "Higgs:runningLoopMass = ".$_POST["2"]."\n";
1115	fwrite($handle,$data);
1116	}
1117	if($_POST["3"] != "on")
1118	{
1119	$data = "Higgs:clipWings = ".$_POST["3"]."\n";
1120	fwrite($handle,$data);
1121	}
1122	if($_POST["4"] != "50.")
1123	{
1124	$data = "Higgs:wingsFac = ".$_POST["4"]."\n";
1125	fwrite($handle,$data);
1126	}
1127	if($_POST["5"] != "off")
1128	{
1129	$data = "HiggsSM:all = ".$_POST["5"]."\n";
1130	fwrite($handle,$data);
1131	}
1132	if($_POST["6"] != "off")
1133	{
1134	$data = "HiggsSM:ffbar2H = ".$_POST["6"]."\n";
1135	fwrite($handle,$data);
1136	}
1137	if($_POST["7"] != "off")
1138	{
1139	$data = "HiggsSM:gg2H = ".$_POST["7"]."\n";
1140	fwrite($handle,$data);
1141	}
1142	if($_POST["8"] != "off")
1143	{
1144	$data = "HiggsSM:gmgm2H = ".$_POST["8"]."\n";
1145	fwrite($handle,$data);
1146	}
1147	if($_POST["9"] != "off")
1148	{
1149	$data = "HiggsSM:ffbar2HZ = ".$_POST["9"]."\n";
1150	fwrite($handle,$data);
1151	}
1152	if($_POST["10"] != "off")
1153	{
1154	$data = "HiggsSM:ffbar2HW = ".$_POST["10"]."\n";
1155	fwrite($handle,$data);
1156	}
1157	if($_POST["11"] != "off")
1158	{
1159	$data = "HiggsSM:ff2Hff(t:ZZ) = ".$_POST["11"]."\n";
1160	fwrite($handle,$data);
1161	}
1162	if($_POST["12"] != "off")
1163	{
1164	$data = "HiggsSM:ff2Hff(t:WW) = ".$_POST["12"]."\n";
1165	fwrite($handle,$data);
1166	}
1167	if($_POST["13"] != "off")
1168	{
1169	$data = "HiggsSM:gg2Httbar = ".$_POST["13"]."\n";
1170	fwrite($handle,$data);
1171	}
1172	if($_POST["14"] != "off")
1173	{
1174	$data = "HiggsSM:qqbar2Httbar = ".$_POST["14"]."\n";
1175	fwrite($handle,$data);
1176	}
1177	if($_POST["15"] != "off")
1178	{
1179	$data = "HiggsSM:qg2Hq = ".$_POST["15"]."\n";
1180	fwrite($handle,$data);
1181	}
1182	if($_POST["16"] != "off")
1183	{
1184	$data = "HiggsSM:gg2Hbbbar = ".$_POST["16"]."\n";
1185	fwrite($handle,$data);
1186	}
1187	if($_POST["17"] != "off")
1188	{
1189	$data = "HiggsSM:qqbar2Hbbbar = ".$_POST["17"]."\n";
1190	fwrite($handle,$data);
1191	}
1192	if($_POST["18"] != "off")
1193	{
1194	$data = "HiggsSM:gg2Hg(l:t) = ".$_POST["18"]."\n";
1195	fwrite($handle,$data);
1196	}
1197	if($_POST["19"] != "off")
1198	{
1199	$data = "HiggsSM:qg2Hq(l:t) = ".$_POST["19"]."\n";
1200	fwrite($handle,$data);
1201	}
1202	if($_POST["20"] != "off")
1203	{
1204	$data = "HiggsSM:qqbar2Hg(l:t) = ".$_POST["20"]."\n";
1205	fwrite($handle,$data);
1206	}
1207	if($_POST["21"] != "off")
1208	{
1209	$data = "Higgs:useBSM = ".$_POST["21"]."\n";
1210	fwrite($handle,$data);
1211	}
1212	if($_POST["22"] != "off")
1213	{
1214	$data = "HiggsBSM:all = ".$_POST["22"]."\n";
1215	fwrite($handle,$data);
1216	}
1217	if($_POST["23"] != "off")
1218	{
1219	$data = "HiggsBSM:allH1 = ".$_POST["23"]."\n";
1220	fwrite($handle,$data);
1221	}
1222	if($_POST["24"] != "off")
1223	{
1224	$data = "HiggsBSM:ffbar2H1 = ".$_POST["24"]."\n";
1225	fwrite($handle,$data);
1226	}
1227	if($_POST["25"] != "off")
1228	{
1229	$data = "HiggsBSM:gg2H1 = ".$_POST["25"]."\n";
1230	fwrite($handle,$data);
1231	}
1232	if($_POST["26"] != "off")
1233	{
1234	$data = "HiggsBSM:gmgm2H1 = ".$_POST["26"]."\n";
1235	fwrite($handle,$data);
1236	}
1237	if($_POST["27"] != "off")
1238	{
1239	$data = "HiggsBSM:ffbar2H1Z = ".$_POST["27"]."\n";
1240	fwrite($handle,$data);
1241	}
1242	if($_POST["28"] != "off")
1243	{
1244	$data = "HiggsBSM:ffbar2H1W = ".$_POST["28"]."\n";
1245	fwrite($handle,$data);
1246	}
1247	if($_POST["29"] != "off")
1248	{
1249	$data = "HiggsBSM:ff2H1ff(t:ZZ) = ".$_POST["29"]."\n";
1250	fwrite($handle,$data);
1251	}
1252	if($_POST["30"] != "off")
1253	{
1254	$data = "HiggsBSM:ff2H1ff(t:WW) = ".$_POST["30"]."\n";
1255	fwrite($handle,$data);
1256	}
1257	if($_POST["31"] != "off")
1258	{
1259	$data = "HiggsBSM:gg2H1ttbar = ".$_POST["31"]."\n";
1260	fwrite($handle,$data);
1261	}
1262	if($_POST["32"] != "off")
1263	{
1264	$data = "HiggsBSM:qqbar2H1ttbar = ".$_POST["32"]."\n";
1265	fwrite($handle,$data);
1266	}
1267	if($_POST["33"] != "off")
1268	{
1269	$data = "HiggsBSM:allH2 = ".$_POST["33"]."\n";
1270	fwrite($handle,$data);
1271	}
1272	if($_POST["34"] != "off")
1273	{
1274	$data = "HiggsBSM:ffbar2H2 = ".$_POST["34"]."\n";
1275	fwrite($handle,$data);
1276	}
1277	if($_POST["35"] != "off")
1278	{
1279	$data = "HiggsBSM:gg2H2 = ".$_POST["35"]."\n";
1280	fwrite($handle,$data);
1281	}
1282	if($_POST["36"] != "off")
1283	{
1284	$data = "HiggsBSM:gmgm2H2 = ".$_POST["36"]."\n";
1285	fwrite($handle,$data);
1286	}
1287	if($_POST["37"] != "off")
1288	{
1289	$data = "HiggsBSM:ffbar2H2Z = ".$_POST["37"]."\n";
1290	fwrite($handle,$data);
1291	}
1292	if($_POST["38"] != "off")
1293	{
1294	$data = "HiggsBSM:ffbar2H2W = ".$_POST["38"]."\n";
1295	fwrite($handle,$data);
1296	}
1297	if($_POST["39"] != "off")
1298	{
1299	$data = "HiggsBSM:ff2H2ff(t:ZZ) = ".$_POST["39"]."\n";
1300	fwrite($handle,$data);
1301	}
1302	if($_POST["40"] != "off")
1303	{
1304	$data = "HiggsBSM:ff2H2ff(t:WW) = ".$_POST["40"]."\n";
1305	fwrite($handle,$data);
1306	}
1307	if($_POST["41"] != "off")
1308	{
1309	$data = "HiggsBSM:gg2H2ttbar = ".$_POST["41"]."\n";
1310	fwrite($handle,$data);
1311	}
1312	if($_POST["42"] != "off")
1313	{
1314	$data = "HiggsBSM:qqbar2H2ttbar = ".$_POST["42"]."\n";
1315	fwrite($handle,$data);
1316	}
1317	if($_POST["43"] != "off")
1318	{
1319	$data = "HiggsBSM:allA3 = ".$_POST["43"]."\n";
1320	fwrite($handle,$data);
1321	}
1322	if($_POST["44"] != "off")
1323	{
1324	$data = "HiggsBSM:ffbar2A3 = ".$_POST["44"]."\n";
1325	fwrite($handle,$data);
1326	}
1327	if($_POST["45"] != "off")
1328	{
1329	$data = "HiggsBSM:gg2A3 = ".$_POST["45"]."\n";
1330	fwrite($handle,$data);
1331	}
1332	if($_POST["46"] != "off")
1333	{
1334	$data = "HiggsBSM:gmgm2A3 = ".$_POST["46"]."\n";
1335	fwrite($handle,$data);
1336	}
1337	if($_POST["47"] != "off")
1338	{
1339	$data = "HiggsBSM:ffbar2A3Z = ".$_POST["47"]."\n";
1340	fwrite($handle,$data);
1341	}
1342	if($_POST["48"] != "off")
1343	{
1344	$data = "HiggsBSM:ffbar2A3W = ".$_POST["48"]."\n";
1345	fwrite($handle,$data);
1346	}
1347	if($_POST["49"] != "off")
1348	{
1349	$data = "HiggsBSM:ff2A3ff(t:ZZ) = ".$_POST["49"]."\n";
1350	fwrite($handle,$data);
1351	}
1352	if($_POST["50"] != "off")
1353	{
1354	$data = "HiggsBSM:ff2A3ff(t:WW) = ".$_POST["50"]."\n";
1355	fwrite($handle,$data);
1356	}
1357	if($_POST["51"] != "off")
1358	{
1359	$data = "HiggsBSM:gg2A3ttbar = ".$_POST["51"]."\n";
1360	fwrite($handle,$data);
1361	}
1362	if($_POST["52"] != "off")
1363	{
1364	$data = "HiggsBSM:qqbar2A3ttbar = ".$_POST["52"]."\n";
1365	fwrite($handle,$data);
1366	}
1367	if($_POST["53"] != "off")
1368	{
1369	$data = "HiggsBSM:allH+- = ".$_POST["53"]."\n";
1370	fwrite($handle,$data);
1371	}
1372	if($_POST["54"] != "off")
1373	{
1374	$data = "HiggsBSM:ffbar2H+- = ".$_POST["54"]."\n";
1375	fwrite($handle,$data);
1376	}
1377	if($_POST["55"] != "off")
1378	{
1379	$data = "HiggsBSM:bg2H+-t = ".$_POST["55"]."\n";
1380	fwrite($handle,$data);
1381	}
1382	if($_POST["56"] != "off")
1383	{
1384	$data = "HiggsBSM:allHpair = ".$_POST["56"]."\n";
1385	fwrite($handle,$data);
1386	}
1387	if($_POST["57"] != "off")
1388	{
1389	$data = "HiggsBSM:ffbar2A3H1 = ".$_POST["57"]."\n";
1390	fwrite($handle,$data);
1391	}
1392	if($_POST["58"] != "off")
1393	{
1394	$data = "HiggsBSM:ffbar2A3H2 = ".$_POST["58"]."\n";
1395	fwrite($handle,$data);
1396	}
1397	if($_POST["59"] != "off")
1398	{
1399	$data = "HiggsBSM:ffbar2H+-H1 = ".$_POST["59"]."\n";
1400	fwrite($handle,$data);
1401	}
1402	if($_POST["60"] != "off")
1403	{
1404	$data = "HiggsBSM:ffbar2H+-H2 = ".$_POST["60"]."\n";
1405	fwrite($handle,$data);
1406	}
1407	if($_POST["61"] != "off")
1408	{
1409	$data = "HiggsBSM:ffbar2H+H- = ".$_POST["61"]."\n";
1410	fwrite($handle,$data);
1411	}
1412	if($_POST["62"] != "off")
1413	{
1414	$data = "HiggsBSM:qg2H1q = ".$_POST["62"]."\n";
1415	fwrite($handle,$data);
1416	}
1417	if($_POST["63"] != "off")
1418	{
1419	$data = "HiggsBSM:gg2H1bbbar = ".$_POST["63"]."\n";
1420	fwrite($handle,$data);
1421	}
1422	if($_POST["64"] != "off")
1423	{
1424	$data = "HiggsBSM:qqbar2H1bbbar = ".$_POST["64"]."\n";
1425	fwrite($handle,$data);
1426	}
1427	if($_POST["65"] != "off")
1428	{
1429	$data = "HiggsBSM:gg2H1g(l:t) = ".$_POST["65"]."\n";
1430	fwrite($handle,$data);
1431	}
1432	if($_POST["66"] != "off")
1433	{
1434	$data = "HiggsBSM:qg2H1q(l:t) = ".$_POST["66"]."\n";
1435	fwrite($handle,$data);
1436	}
1437	if($_POST["67"] != "off")
1438	{
1439	$data = "HiggsBSM:qqbar2H1g(l:t) = ".$_POST["67"]."\n";
1440	fwrite($handle,$data);
1441	}
1442	if($_POST["68"] != "off")
1443	{
1444	$data = "HiggsBSM:qg2H2q = ".$_POST["68"]."\n";
1445	fwrite($handle,$data);
1446	}
1447	if($_POST["69"] != "off")
1448	{
1449	$data = "HiggsBSM:gg2H2bbbar = ".$_POST["69"]."\n";
1450	fwrite($handle,$data);
1451	}
1452	if($_POST["70"] != "off")
1453	{
1454	$data = "HiggsBSM:qqbar2H2bbbar = ".$_POST["70"]."\n";
1455	fwrite($handle,$data);
1456	}
1457	if($_POST["71"] != "off")
1458	{
1459	$data = "HiggsBSM:gg2H2g(l:t) = ".$_POST["71"]."\n";
1460	fwrite($handle,$data);
1461	}
1462	if($_POST["72"] != "off")
1463	{
1464	$data = "HiggsBSM:qg2H2q(l:t) = ".$_POST["72"]."\n";
1465	fwrite($handle,$data);
1466	}
1467	if($_POST["73"] != "off")
1468	{
1469	$data = "HiggsBSM:qqbar2H2g(l:t) = ".$_POST["73"]."\n";
1470	fwrite($handle,$data);
1471	}
1472	if($_POST["74"] != "off")
1473	{
1474	$data = "HiggsBSM:qg2A3q = ".$_POST["74"]."\n";
1475	fwrite($handle,$data);
1476	}
1477	if($_POST["75"] != "off")
1478	{
1479	$data = "HiggsBSM:gg2A3bbbar = ".$_POST["75"]."\n";
1480	fwrite($handle,$data);
1481	}
1482	if($_POST["76"] != "off")
1483	{
1484	$data = "HiggsBSM:qqbar2A3bbbar = ".$_POST["76"]."\n";
1485	fwrite($handle,$data);
1486	}
1487	if($_POST["77"] != "off")
1488	{
1489	$data = "HiggsBSM:gg2A3g(l:t) = ".$_POST["77"]."\n";
1490	fwrite($handle,$data);
1491	}
1492	if($_POST["78"] != "off")
1493	{
1494	$data = "HiggsBSM:qg2A3q(l:t) = ".$_POST["78"]."\n";
1495	fwrite($handle,$data);
1496	}
1497	if($_POST["79"] != "off")
1498	{
1499	$data = "HiggsBSM:qqbar2A3g(l:t) = ".$_POST["79"]."\n";
1500	fwrite($handle,$data);
1501	}
1502	if($_POST["80"] != "1.")
1503	{
1504	$data = "HiggsH1:coup2d = ".$_POST["80"]."\n";
1505	fwrite($handle,$data);
1506	}
1507	if($_POST["81"] != "1.")
1508	{
1509	$data = "HiggsH1:coup2u = ".$_POST["81"]."\n";
1510	fwrite($handle,$data);
1511	}
1512	if($_POST["82"] != "1.")
1513	{
1514	$data = "HiggsH1:coup2l = ".$_POST["82"]."\n";
1515	fwrite($handle,$data);
1516	}
1517	if($_POST["83"] != "1.")
1518	{
1519	$data = "HiggsH1:coup2Z = ".$_POST["83"]."\n";
1520	fwrite($handle,$data);
1521	}
1522	if($_POST["84"] != "1.")
1523	{
1524	$data = "HiggsH1:coup2W = ".$_POST["84"]."\n";
1525	fwrite($handle,$data);
1526	}
1527	if($_POST["85"] != "0.")
1528	{
1529	$data = "HiggsH1:coup2Hchg = ".$_POST["85"]."\n";
1530	fwrite($handle,$data);
1531	}
1532	if($_POST["86"] != "1.")
1533	{
1534	$data = "HiggsH2:coup2d = ".$_POST["86"]."\n";
1535	fwrite($handle,$data);
1536	}
1537	if($_POST["87"] != "1.")
1538	{
1539	$data = "HiggsH2:coup2u = ".$_POST["87"]."\n";
1540	fwrite($handle,$data);
1541	}
1542	if($_POST["88"] != "1.")
1543	{
1544	$data = "HiggsH2:coup2l = ".$_POST["88"]."\n";
1545	fwrite($handle,$data);
1546	}
1547	if($_POST["89"] != "1.")
1548	{
1549	$data = "HiggsH2:coup2Z = ".$_POST["89"]."\n";
1550	fwrite($handle,$data);
1551	}
1552	if($_POST["90"] != "1.")
1553	{
1554	$data = "HiggsH2:coup2W = ".$_POST["90"]."\n";
1555	fwrite($handle,$data);
1556	}
1557	if($_POST["91"] != "0.")
1558	{
1559	$data = "HiggsH2:coup2Hchg = ".$_POST["91"]."\n";
1560	fwrite($handle,$data);
1561	}
1562	if($_POST["92"] != "1.")
1563	{
1564	$data = "HiggsH2:coup2H1H1 = ".$_POST["92"]."\n";
1565	fwrite($handle,$data);
1566	}
1567	if($_POST["93"] != "1.")
1568	{
1569	$data = "HiggsH2:coup2A3A3 = ".$_POST["93"]."\n";
1570	fwrite($handle,$data);
1571	}
1572	if($_POST["94"] != "0.")
1573	{
1574	$data = "HiggsH2:coup2H1Z = ".$_POST["94"]."\n";
1575	fwrite($handle,$data);
1576	}
1577	if($_POST["95"] != "0.")
1578	{
1579	$data = "HiggsH2:coup2A3H1 = ".$_POST["95"]."\n";
1580	fwrite($handle,$data);
1581	}
1582	if($_POST["96"] != "0.")
1583	{
1584	$data = "HiggsH2:coup2HchgW = ".$_POST["96"]."\n";
1585	fwrite($handle,$data);
1586	}
1587	if($_POST["97"] != "1.")
1588	{
1589	$data = "HiggsA3:coup2d = ".$_POST["97"]."\n";
1590	fwrite($handle,$data);
1591	}
1592	if($_POST["98"] != "1.")
1593	{
1594	$data = "HiggsA3:coup2u = ".$_POST["98"]."\n";
1595	fwrite($handle,$data);
1596	}
1597	if($_POST["99"] != "1.")
1598	{
1599	$data = "HiggsA3:coup2l = ".$_POST["99"]."\n";
1600	fwrite($handle,$data);
1601	}
1602	if($_POST["100"] != "1.")
1603	{
1604	$data = "HiggsA3:coup2H1Z = ".$_POST["100"]."\n";
1605	fwrite($handle,$data);
1606	}
1607	if($_POST["101"] != "1.")
1608	{
1609	$data = "HiggsA3:coup2H2Z = ".$_POST["101"]."\n";
1610	fwrite($handle,$data);
1611	}
1612	if($_POST["102"] != "0.")
1613	{
1614	$data = "HiggsA3:coup2Z = ".$_POST["102"]."\n";
1615	fwrite($handle,$data);
1616	}
1617	if($_POST["103"] != "0.")
1618	{
1619	$data = "HiggsA3:coup2W = ".$_POST["103"]."\n";
1620	fwrite($handle,$data);
1621	}
1622	if($_POST["104"] != "0.")
1623	{
1624	$data = "HiggsA3:coup2H1H1 = ".$_POST["104"]."\n";
1625	fwrite($handle,$data);
1626	}
1627	if($_POST["105"] != "0.")
1628	{
1629	$data = "HiggsA3:coup2Hchg = ".$_POST["105"]."\n";
1630	fwrite($handle,$data);
1631	}
1632	if($_POST["106"] != "1.")
1633	{
1634	$data = "HiggsA3:coup2HchgW = ".$_POST["106"]."\n";
1635	fwrite($handle,$data);
1636	}
1637	if($_POST["107"] != "5.")
1638	{
1639	$data = "HiggsHchg:tanBeta = ".$_POST["107"]."\n";
1640	fwrite($handle,$data);
1641	}
1642	if($_POST["108"] != "1.")
1643	{
1644	$data = "HiggsHchg:coup2H1W = ".$_POST["108"]."\n";
1645	fwrite($handle,$data);
1646	}
1647	if($_POST["109"] != "0.")
1648	{
1649	$data = "HiggsHchg:coup2H2W = ".$_POST["109"]."\n";
1650	fwrite($handle,$data);
1651	}
1652	if($_POST["110"] != "1")
1653	{
1654	$data = "HiggsH1:parity = ".$_POST["110"]."\n";
1655	fwrite($handle,$data);
1656	}
1657	if($_POST["111"] != "0.")
1658	{
1659	$data = "HiggsH1:etaParity = ".$_POST["111"]."\n";
1660	fwrite($handle,$data);
1661	}
1662	if($_POST["112"] != "1")
1663	{
1664	$data = "HiggsH2:parity = ".$_POST["112"]."\n";
1665	fwrite($handle,$data);
1666	}
1667	if($_POST["113"] != "0.")
1668	{
1669	$data = "HiggsH2:etaParity = ".$_POST["113"]."\n";
1670	fwrite($handle,$data);
1671	}
1672	if($_POST["114"] != "2")
1673	{
1674	$data = "HiggsA3:parity = ".$_POST["114"]."\n";
1675	fwrite($handle,$data);
1676	}
1677	if($_POST["115"] != "0.")
1678	{
1679	$data = "HiggsA3:etaParity = ".$_POST["115"]."\n";
1680	fwrite($handle,$data);
1681	}
1682	fclose($handle);
1683	}
1684
1685	?>
1686	</body>
1687	</html>
1688
1689	<!-- Copyright (C) 2012 Torbjorn Sjostrand -->
1690

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