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+<title>New-Gauge-Boson Processes</title>
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+<form method='post' action='NewGaugeBosonProcesses.php'>
+
+<h2>New-Gauge-Boson Processes</h2>
+
+This page contains the production of new <i>Z'^0</i> and
+<i>W'^+-</i> gauge bosons, e.g. within the context of a new
+<i>U(1)</i> or <i>SU(2)</i> gauge group, and also a
+(rather speculative) horizontal gauge boson <i>R^0</i>.
+Left-right-symmetry scenarios also contain new gauge bosons,
+but are described
+<?php $filepath = $_GET["filepath"];
+echo "<a href='LeftRightSymmetryProcesses.php?filepath=".$filepath."' target='page'>";?>separately</a>.
+
+<h3><i>Z'^0</i></h3>
+
+This group only contains one subprocess, with the full
+<i>gamma^*/Z^0/Z'^0</i> interference structure for couplings
+to fermion pairs. It is possible to pick only a subset, e.g, only
+the pure <i>Z'^0</i> piece. No higher-order processes are
+available explicitly, but the ISR showers contain automatic
+matching to the <i>Z'^0</i> + 1 jet matrix elements, as for
+the corresponding <i>gamma^*/Z^0</i> process.
+
+<br/><br/><strong>NewGaugeBoson:ffbar2gmZZprime</strong> <input type="radio" name="1" value="on"><strong>On</strong>
+<input type="radio" name="1" value="off" checked="checked"><strong>Off</strong>
+ (<code>default = <strong>off</strong></code>)<br/>
+Scattering <i>f fbar ->Z'^0</i>.
+Code 3001.
+
+
+<br/><br/><table><tr><td><strong>Zprime:gmZmode </td><td> (<code>default = <strong>0</strong></code>; <code>minimum = 0</code>; <code>maximum = 6</code>)</td></tr></table>
+Choice of full <ei>gamma^*/Z^0/Z'^0</ei> structure or not in
+the above process. Note that, with the <ei>Z'^0</ei> part switched
+off, this process is reduced to what already exists among
+<aloc href="ElectroweakProcesses">electroweak processes</aloc>,
+so those options are here only for crosschecks.
+<br/>
+<input type="radio" name="2" value="0" checked="checked"><strong>0 </strong>: full <ei>gamma^*/Z^0/Z'^0</ei> structure, with interference included.<br/>
+<input type="radio" name="2" value="1"><strong>1 </strong>: only pure <ei>gamma^*</ei> contribution.<br/>
+<input type="radio" name="2" value="2"><strong>2 </strong>: only pure <ei>Z^0</ei> contribution.<br/>
+<input type="radio" name="2" value="3"><strong>3 </strong>: only pure <ei>Z'^0</ei> contribution.<br/>
+<input type="radio" name="2" value="4"><strong>4 </strong>: only the <ei>gamma^*/Z^0</ei> contribution, including interference.<br/>
+<input type="radio" name="2" value="5"><strong>5 </strong>: only the <ei>gamma^*/Z'^0</ei> contribution, including interference.<br/>
+<input type="radio" name="2" value="6"><strong>6 </strong>: only the <ei>Z^0/Z'^0</ei> contribution, including interference.<br/>
+<br/><b>Note</b>: irrespective of the option used, the particle produced
+will always be assigned code 32 for <ei>Z'^0</ei>, and open decay channels
+is purely dictated by what is set for the <ei>Z'^0</ei>.
+
+<p/>
+The couplings of the <i>Z'^0</i> to quarks and leptons can
+either be assumed universal, i.e. generation-independent, or not.
+In the former case eight numbers parametrize the vector and axial
+couplings of down-type quarks, up-type quarks, leptons and neutrinos,
+respectively. Depending on your assumed neutrino nature you may
+want to restrict your freedom in that sector, but no limitations
+are enforced by the program. The default corresponds to the same
+couplings as that of the Standard Model <i>Z^0</i>, with axial
+couplings <i>a_f = +-1</i> and vector couplings
+<i>v_f = a_f - 4 e_f sin^2(theta_W)</i>, with
+<i>sin^2(theta_W) = 0.23</i>. Without universality
+the same eight numbers have to be set separately also for the
+second and the third generation. The choice of fixed axial and
+vector couplings implies a resonance width that increases linearly
+with the <i>Z'^0</i> mass.
+
+<p/>
+By a suitable choice of the parameters, it is possible to simulate
+just about any imaginable <i>Z'^0</i> scenario, with full
+interference effects in cross sections and decay angular
+distributions and generation-dependent couplings; the default values
+should mainly be viewed as placeholders. The conversion
+from the coupling conventions in a set of different <i>Z'^0</i>
+models in the literature to those used in PYTHIA is described by
+<a href="http://www.hep.uiuc.edu/home/catutza/nota12.ps">C.
+Ciobanu et al.</a>
+
+<br/><br/><strong>Zprime:universality</strong> <input type="radio" name="3" value="on" checked="checked"><strong>On</strong>
+<input type="radio" name="3" value="off"><strong>Off</strong>
+ (<code>default = <strong>on</strong></code>)<br/>
+If on then you need only set the first-generation couplings
+below, and these are automatically also used for the second and
+third generation. If off, then couplings can be chosen separately
+for each generation.
+
+
+<p/>
+Here are the couplings always valid for the first generation,
+and normally also for the second and third by trivial analogy:
+
+<br/><br/><table><tr><td><strong>Zprime:vd </td><td></td><td> <input type="text" name="4" value="-0.693" size="20"/> (<code>default = <strong>-0.693</strong></code>)</td></tr></table>
+vector coupling of <i>d</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:ad </td><td></td><td> <input type="text" name="5" value="-1." size="20"/> (<code>default = <strong>-1.</strong></code>)</td></tr></table>
+axial coupling of <i>d</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vu </td><td></td><td> <input type="text" name="6" value="0.387" size="20"/> (<code>default = <strong>0.387</strong></code>)</td></tr></table>
+vector coupling of <i>u</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:au </td><td></td><td> <input type="text" name="7" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+axial coupling of <i>u</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:ve </td><td></td><td> <input type="text" name="8" value="-0.08" size="20"/> (<code>default = <strong>-0.08</strong></code>)</td></tr></table>
+vector coupling of <i>e</i> leptons.
+
+
+<br/><br/><table><tr><td><strong>Zprime:ae </td><td></td><td> <input type="text" name="9" value="-1." size="20"/> (<code>default = <strong>-1.</strong></code>)</td></tr></table>
+axial coupling of <i>e</i> leptons.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vnue </td><td></td><td> <input type="text" name="10" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+vector coupling of <i>nu_e</i> neutrinos.
+
+
+<br/><br/><table><tr><td><strong>Zprime:anue </td><td></td><td> <input type="text" name="11" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+axial coupling of <i>nu_e</i> neutrinos.
+
+
+<p/>
+Here are the further couplings that are specific for
+a scenario with <code>Zprime:universality</code> switched off:
+
+<br/><br/><table><tr><td><strong>Zprime:vs </td><td></td><td> <input type="text" name="12" value="-0.693" size="20"/> (<code>default = <strong>-0.693</strong></code>)</td></tr></table>
+vector coupling of <i>s</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:as </td><td></td><td> <input type="text" name="13" value="-1." size="20"/> (<code>default = <strong>-1.</strong></code>)</td></tr></table>
+axial coupling of <i>s</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vc </td><td></td><td> <input type="text" name="14" value="0.387" size="20"/> (<code>default = <strong>0.387</strong></code>)</td></tr></table>
+vector coupling of <i>c</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:ac </td><td></td><td> <input type="text" name="15" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+axial coupling of <i>c</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vmu </td><td></td><td> <input type="text" name="16" value="-0.08" size="20"/> (<code>default = <strong>-0.08</strong></code>)</td></tr></table>
+vector coupling of <i>mu</i> leptons.
+
+
+<br/><br/><table><tr><td><strong>Zprime:amu </td><td></td><td> <input type="text" name="17" value="-1." size="20"/> (<code>default = <strong>-1.</strong></code>)</td></tr></table>
+axial coupling of <i>mu</i> leptons.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vnumu </td><td></td><td> <input type="text" name="18" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+vector coupling of <i>nu_mu</i> neutrinos.
+
+
+<br/><br/><table><tr><td><strong>Zprime:anumu </td><td></td><td> <input type="text" name="19" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+axial coupling of <i>nu_mu</i> neutrinos.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vb </td><td></td><td> <input type="text" name="20" value="-0.693" size="20"/> (<code>default = <strong>-0.693</strong></code>)</td></tr></table>
+vector coupling of <i>b</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:ab </td><td></td><td> <input type="text" name="21" value="-1." size="20"/> (<code>default = <strong>-1.</strong></code>)</td></tr></table>
+axial coupling of <i>b</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vt </td><td></td><td> <input type="text" name="22" value="0.387" size="20"/> (<code>default = <strong>0.387</strong></code>)</td></tr></table>
+vector coupling of <i>t</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:at </td><td></td><td> <input type="text" name="23" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+axial coupling of <i>t</i> quarks.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vtau </td><td></td><td> <input type="text" name="24" value="-0.08" size="20"/> (<code>default = <strong>-0.08</strong></code>)</td></tr></table>
+vector coupling of <i>tau</i> leptons.
+
+
+<br/><br/><table><tr><td><strong>Zprime:atau </td><td></td><td> <input type="text" name="25" value="-1." size="20"/> (<code>default = <strong>-1.</strong></code>)</td></tr></table>
+axial coupling of <i>tau</i> leptons.
+
+
+<br/><br/><table><tr><td><strong>Zprime:vnutau </td><td></td><td> <input type="text" name="26" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+vector coupling of <i>nu_tau</i> neutrinos.
+
+
+<br/><br/><table><tr><td><strong>Zprime:anutau </td><td></td><td> <input type="text" name="27" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+axial coupling of <i>nu_tau</i> neutrinos.
+
+
+<p/>
+The coupling to the decay channel <i>Z'^0 -> W^+ W^-</i> is
+more model-dependent. By default it is therefore off, but can be
+switched on as follows. Furthermore, we have left some amount of
+freedom in the choice of decay angular correlations in this
+channel, but obviously alternative shapes could be imagined.
+
+<br/><br/><table><tr><td><strong>Zprime:coup2WW </td><td></td><td> <input type="text" name="28" value="0." size="20"/> (<code>default = <strong>0.</strong></code>; <code>minimum = 0.</code>)</td></tr></table>
+the coupling <i>Z'^0 -> W^+ W^-</i> is taken to be this number
+times <i>m_W^2 / m_Z'^2</i> times the <i>Z^0 -> W^+ W^-</i>
+coupling. Thus a unit value corresponds to the
+<i>Z^0 -> W^+ W^-</i> coupling, scaled down by a factor
+<i>m_W^2 / m_Z'^2</i>, and gives a <i>Z'^0</i> partial
+width into this channel that again increases linearly. If you
+cancel this behaviour, by letting <code>Zprime:coup2WW</code> be
+proportional to <i>m_Z'^2 / m_W^2</i>, you instead obtain a
+partial width that goes like the fifth power of the <i>Z'^0</i>
+mass. These two extremes correspond to the "extended gauge model"
+and the "reference model", respectively, of [<a href="Bibliography.php" target="page">Alt89</a>].
+Note that this channel only includes the pure <i>Z'</i> part,
+while <i>f fbar -> gamma^*/Z^*0 -> W^+ W^-</i> is available
+as a separate electroweak process.
+
+
+<br/><br/><table><tr><td><strong>Zprime:anglesWW </td><td></td><td> <input type="text" name="29" value="0." size="20"/> (<code>default = <strong>0.</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.</code>)</td></tr></table>
+in the decay chain <i>Z'^0 -> W^+ W^- ->f_1 fbar_2 f_3 fbar_4</i>
+the decay angular distributions is taken to be a mixture of two
+possible shapes. This parameter gives the fraction that is distributed
+as in Higgs <i>h^0 -> W^+ W^-</i> (longitudinal bosons),
+with the remainder (by default all) is taken to be the same as for
+<i>Z^0 -> W^+ W^-</i> (a mixture of transverse and longitudinal
+bosons).
+
+
+<p/>
+A massive <i>Z'^0</i> is also likely to decay into Higgs bosons
+and potentially into other now unknown particles. Such possibilities
+clearly are quite model-dependent, and have not been included
+for now.
+
+<h3><i>W'^+-</i></h3>
+
+The <i>W'^+-</i> implementation is less ambitious than the
+<i>Z'^0</i>. Specifically, while indirect detection of a
+<i>Z'^0</i> through its interference contribution is
+a possible discovery channel in lepton colliders, there is no
+equally compelling case for <i>W^+-/W'^+-</i> interference
+effects being of importance for discovery, and such interference
+has therefore not been implemented for now. Related to this, a
+<i>Z'^0</i> could appear on its own in a new <i>U(1)</i> group,
+while <i>W'^+-</i> would have to sit in a <i>SU(2)</i> group
+and thus have a <i>Z'^0</i> partner that is likely to be found
+first. Only one process is implemented but, like for the
+<i>W^+-</i>, the ISR showers contain automatic matching to the
+<i>W'^+-</i> + 1 jet matrix elements.
+
+<br/><br/><strong>NewGaugeBoson:ffbar2Wprime</strong> <input type="radio" name="30" value="on"><strong>On</strong>
+<input type="radio" name="30" value="off" checked="checked"><strong>Off</strong>
+ (<code>default = <strong>off</strong></code>)<br/>
+Scattering <i>f fbar' -> W'^+-</i>.
+Code 3021.
+
+
+<p/>
+The couplings of the <i>W'^+-</i> are here assumed universal,
+i.e. the same for all generations. One may set vector and axial
+couplings freely, separately for the <i>q qbar'</i> and the
+<i>l nu_l</i> decay channels. The defaults correspond to the
+<i>V - A</i> structure and normalization of the Standard Model
+<i>W^+-</i>, but can be changed to simulate a wide selection
+of models. One limitation is that, for simplicity, the same
+Cabibbo--Kobayashi--Maskawa quark mixing matrix is assumed as for
+the standard <i>W^+-</i>. Depending on your assumed neutrino
+nature you may want to restrict your freedom in the lepton sector,
+but no limitations are enforced by the program.
+
+<br/><br/><table><tr><td><strong>Wprime:vq </td><td></td><td> <input type="text" name="31" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+vector coupling of quarks.
+
+
+<br/><br/><table><tr><td><strong>Wprime:aq </td><td></td><td> <input type="text" name="32" value="-1." size="20"/> (<code>default = <strong>-1.</strong></code>)</td></tr></table>
+axial coupling of quarks.
+
+
+<br/><br/><table><tr><td><strong>Wprime:vl </td><td></td><td> <input type="text" name="33" value="1." size="20"/> (<code>default = <strong>1.</strong></code>)</td></tr></table>
+vector coupling of leptons.
+
+
+<br/><br/><table><tr><td><strong>Wprime:al </td><td></td><td> <input type="text" name="34" value="-1." size="20"/> (<code>default = <strong>-1.</strong></code>)</td></tr></table>
+axial coupling of leptons.
+
+
+<p/>
+The coupling to the decay channel <i>W'^+- -> W^+- Z^0</i> is
+more model-dependent, like for <i>Z'^0 -> W^+ W^-</i> described
+above. By default it is therefore off, but can be
+switched on as follows. Furthermore, we have left some amount of
+freedom in the choice of decay angular correlations in this
+channel, but obviously alternative shapes could be imagined.
+
+<br/><br/><table><tr><td><strong>Wprime:coup2WZ </td><td></td><td> <input type="text" name="35" value="0." size="20"/> (<code>default = <strong>0.</strong></code>; <code>minimum = 0.</code>)</td></tr></table>
+the coupling <i>W'^0 -> W^+- Z^0</i> is taken to be this number
+times <i>m_W^2 / m_W'^2</i> times the <i>W^+- -> W^+- Z^0</i>
+coupling. Thus a unit value corresponds to the
+<i>W^+- -> W^+- Z^0</i> coupling, scaled down by a factor
+<i>m_W^2 / m_W'^2</i>, and gives a <i>W'^+-</i> partial
+width into this channel that increases linearly with the
+<i>W'^+-</i> mass. If you cancel this behaviour, by letting
+<code>Wprime:coup2WZ</code> be proportional to <i>m_W'^2 / m_W^2</i>,
+you instead obtain a partial width that goes like the fifth power
+of the <i>W'^+-</i> mass. These two extremes correspond to the
+"extended gauge model" and the "reference model", respectively,
+of [<a href="Bibliography.php" target="page">Alt89</a>].
+
+
+<br/><br/><table><tr><td><strong>Wprime:anglesWZ </td><td></td><td> <input type="text" name="36" value="0." size="20"/> (<code>default = <strong>0.</strong></code>; <code>minimum = 0.</code>; <code>maximum = 1.</code>)</td></tr></table>
+in the decay chain <i>W'^+- -> W^+- Z^0 ->f_1 fbar_2 f_3 fbar_4</i>
+the decay angular distributions is taken to be a mixture of two
+possible shapes. This parameter gives the fraction that is distributed
+as in Higgs <i>H^+- -> W^+- Z^0</i> (longitudinal bosons),
+with the remainder (by default all) is taken to be the same as for
+<i>W^+- -> W^+- Z^0</i> (a mixture of transverse and longitudinal
+bosons).
+
+
+<p/>
+A massive <i>W'^+-</i> is also likely to decay into Higgs bosons
+and potentially into other now unknown particles. Such possibilities
+clearly are quite model-dependent, and have not been included
+for now.
+
+<h3><i>R^0</i></h3>
+
+The <i>R^0</i> boson (particle code 41) represents one possible
+scenario for a horizontal gauge boson, i.e. a gauge boson
+that couples between the generations, inducing processes like
+<i>s dbar -> R^0 -> mu^- e^+</i>. Experimental limits on
+flavour-changing neutral currents forces such a boson to be fairly
+heavy. In spite of being neutral the antiparticle is distinct from
+the particle: one carries a net positive generation number and
+the other a negative one. This particular model has no new
+parameters beyond the <i>R^0</i> mass. Decays are assumed isotropic.
+For further details see [<a href="Bibliography.php" target="page">Ben85</a>].
+
+<br/><br/><strong>NewGaugeBoson:ffbar2R0</strong> <input type="radio" name="37" value="on"><strong>On</strong>
+<input type="radio" name="37" value="off" checked="checked"><strong>Off</strong>
+ (<code>default = <strong>off</strong></code>)<br/>
+Scattering <i>f_1 fbar_2 -> R^0 -> f_3 fbar_4</i>, where
+<i>f_1</i> and <i>fbar_2</i> are separated by <i>+-</i> one
+generation and similarly for <i>f_3</i> and <i>fbar_4</i>.
+Thus possible final states are e.g. <i>d sbar</i>, <i>u cbar</i>
+<i>s bbar</i>, <i>c tbar</i>, <i>e- mu+</i> and
+<i>mu- tau+</i>.
+Code 3041.
+
+
+<input type="hidden" name="saved" value="1"/>
+
+<?php
+echo "<input type='hidden' name='filepath' value='".$_GET["filepath"]."'/>"?>
+
+<table width="100%"><tr><td align="right"><input type="submit" value="Save Settings" /></td></tr></table>
+</form>
+
+<?php
+
+if($_POST["saved"] == 1)
+{
+$filepath = $_POST["filepath"];
+$handle = fopen($filepath, 'a');
+
+if($_POST["1"] != "off")
+{
+$data = "NewGaugeBoson:ffbar2gmZZprime = ".$_POST["1"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["2"] != "0")
+{
+$data = "Zprime:gmZmode = ".$_POST["2"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["3"] != "on")
+{
+$data = "Zprime:universality = ".$_POST["3"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["4"] != "-0.693")
+{
+$data = "Zprime:vd = ".$_POST["4"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["5"] != "-1.")
+{
+$data = "Zprime:ad = ".$_POST["5"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["6"] != "0.387")
+{
+$data = "Zprime:vu = ".$_POST["6"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["7"] != "1.")
+{
+$data = "Zprime:au = ".$_POST["7"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["8"] != "-0.08")
+{
+$data = "Zprime:ve = ".$_POST["8"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["9"] != "-1.")
+{
+$data = "Zprime:ae = ".$_POST["9"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["10"] != "1.")
+{
+$data = "Zprime:vnue = ".$_POST["10"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["11"] != "1.")
+{
+$data = "Zprime:anue = ".$_POST["11"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["12"] != "-0.693")
+{
+$data = "Zprime:vs = ".$_POST["12"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["13"] != "-1.")
+{
+$data = "Zprime:as = ".$_POST["13"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["14"] != "0.387")
+{
+$data = "Zprime:vc = ".$_POST["14"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["15"] != "1.")
+{
+$data = "Zprime:ac = ".$_POST["15"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["16"] != "-0.08")
+{
+$data = "Zprime:vmu = ".$_POST["16"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["17"] != "-1.")
+{
+$data = "Zprime:amu = ".$_POST["17"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["18"] != "1.")
+{
+$data = "Zprime:vnumu = ".$_POST["18"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["19"] != "1.")
+{
+$data = "Zprime:anumu = ".$_POST["19"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["20"] != "-0.693")
+{
+$data = "Zprime:vb = ".$_POST["20"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["21"] != "-1.")
+{
+$data = "Zprime:ab = ".$_POST["21"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["22"] != "0.387")
+{
+$data = "Zprime:vt = ".$_POST["22"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["23"] != "1.")
+{
+$data = "Zprime:at = ".$_POST["23"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["24"] != "-0.08")
+{
+$data = "Zprime:vtau = ".$_POST["24"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["25"] != "-1.")
+{
+$data = "Zprime:atau = ".$_POST["25"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["26"] != "1.")
+{
+$data = "Zprime:vnutau = ".$_POST["26"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["27"] != "1.")
+{
+$data = "Zprime:anutau = ".$_POST["27"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["28"] != "0.")
+{
+$data = "Zprime:coup2WW = ".$_POST["28"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["29"] != "0.")
+{
+$data = "Zprime:anglesWW = ".$_POST["29"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["30"] != "off")
+{
+$data = "NewGaugeBoson:ffbar2Wprime = ".$_POST["30"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["31"] != "1.")
+{
+$data = "Wprime:vq = ".$_POST["31"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["32"] != "-1.")
+{
+$data = "Wprime:aq = ".$_POST["32"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["33"] != "1.")
+{
+$data = "Wprime:vl = ".$_POST["33"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["34"] != "-1.")
+{
+$data = "Wprime:al = ".$_POST["34"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["35"] != "0.")
+{
+$data = "Wprime:coup2WZ = ".$_POST["35"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["36"] != "0.")
+{
+$data = "Wprime:anglesWZ = ".$_POST["36"]."\n";
+fwrite($handle,$data);
+}
+if($_POST["37"] != "off")
+{
+$data = "NewGaugeBoson:ffbar2R0 = ".$_POST["37"]."\n";
+fwrite($handle,$data);
+}
+fclose($handle);
+}
+
+?>
+</body>
+</html>
+
+<!-- Copyright (C) 2013 Torbjorn Sjostrand -->
+
git://git.uio.no / u / mrichter / AliRoot.git / blobdiff