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1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 | <chapter name="Left-Right-Symmetry Processes">
<h2>Left-Right-Symmetry Processes</h2>
At current energies, the world is left-handed, i.e. the Standard Model
contains an <ei>SU(2)_L</ei> group. Left-right symmetry at some larger
scale implies the need for an <ei>SU(2)_R</ei> group. Thus the particle
content is expanded by right-handed <ei>Z_R^0</ei> and <ei>W_R^+-</ei>
and right-handed neutrinos. The Higgs fields have to be in a triplet
representation, leading to doubly-charged Higgs particles, one set for
each of the two <ei>SU(2)</ei> groups. Also the number of neutral and
singly-charged Higgs states is increased relative to the Standard Model,
but a search for the lowest-lying states of this kind is no different
from e.g. the freedom already accorded by the MSSM Higgs scenarios.
<p/>
PYTHIA implements the scenario of <ref>Hui97</ref>.
<p/>
The <ei>W_R^+-</ei> has been implemented as a simple copy of the
ordinary <ei>W^+-</ei>, with the exception that it couples to
right-handed neutrinos instead of the ordinary left-handed ones.
Thus the standard CKM matrix is used in the quark sector, and the
same vector and axial coupling strengths, leaving only the mass as
free parameter. The <ei>Z_R^0</ei> implementation (without interference
with the photon or the ordinary <ei>Z^0</ei>) allows decays both to
left- and right-handed neutrinos, as well as other fermions, according
to one specific model ansatz. Obviously both the <ei>W_R^+-</ei>
and the <ei>Z_R^0</ei> descriptions are likely to be simplifications,
but provide a starting point.
<p/>
For the doubly-charged Higgs bosons, the main decay modes implemented are
<ei>H_L^++ -> W_L^+ W_L^+, l_i^+ l_j^+ </ei> (<ei>i, j</ei> generation
indices) and <ei>H_R^++ -> W_R^+ W_R^+, l_i^+ l_j^+</ei>.
<p/>
The right-handed neutrinos can be allowed to decay further. Assuming them
to have a mass below that of <ei>W_R^+-</ei>, they decay to three-body
states via a virtual <ei>W_R^+-</ei>, <ei>nu_Rl -> l+- f fbar'</ei>,
where both lepton charges are allowed owing to the Majorana character
of the neutrinos. If there is a significant mass splitting, also
sequential decays <ei>nu_Rl -> l+- l'-+ nu'_Rl</ei> are allowed.
Currently the decays are isotropic in phase space. If the neutrino
masses are close to or above the <ei>W_R^</ei> ones, this description
has to be substituted by a sequential decay via a real <ei>W_R^</ei>
(not implemented, but actually simpler to do than the one here).
<h3>Production processes</h3>
A few different production processes have been implemented, which normally
would not overlap and therefore could be run together.
<flag name="LeftRightSymmmetry:all" default="off">
Common switch for the group of implemented processes within a
left-right-symmetric scenario.
</flag>
<flag name="LeftRightSymmmetry:ffbar2ZR" default="off">
Scatterings <ei>f fbar -> Z_R^0</ei>.
Code 3101.
</flag>
<flag name="LeftRightSymmmetry:ffbar2WR" default="off">
Scatterings <ei><f fbar' -> W_R^+</ei>.
Code 3102.
</flag>
<flag name="LeftRightSymmmetry:ll2HL" default="off">
Scatterings <ei>l_i l_j -> H_L^--</ei>.
Code 3121.
</flag>
<flag name="LeftRightSymmmetry:lgm2HLe" default="off">
Scatterings <ei>l_i gamma -> H_L^-- e^+</ei>.
Code 3122.
</flag>
<flag name="LeftRightSymmmetry:lgm2HLmu" default="off">
Scatterings <ei>l_i gamma -> H_L^-- mu^+</ei>.
Code 3123.
</flag>
<flag name="LeftRightSymmmetry:lgm2HLtau" default="off">
Scatterings <ei>l_i gamma -> H_L^-- tau^+</ei>.
Code 3124.
</flag>
<flag name="LeftRightSymmmetry:ff2HLff" default="off">
Scatterings <ei>f_1 f_2 -> H_L^-- f_3 f_4</ei> via <ei>WW</ei> fusion.
Code 3125.
</flag>
<flag name="LeftRightSymmmetry:ffbar2HLHL" default="off">
Scatterings <ei>f fbar -> H_L^++ H_L^--</ei>.
Code 3126.
</flag>
<flag name="LeftRightSymmmetry:ll2HR" default="off">
Scatterings <ei>l_i l_j -> H_R^--</ei>.
Code 3141.
</flag>
<flag name="LeftRightSymmmetry:lgm2HRe" default="off">
Scatterings <ei>l_i gamma -> H_R^-- e^+</ei>.
Code 3142.
</flag>
<flag name="LeftRightSymmmetry:lgm2HRmu" default="off">
Scatterings <ei>l_i gamma -> H_R^-- mu^+</ei>.
Code 3143.
</flag>
<flag name="LeftRightSymmmetry:lgm2HRtau" default="off">
Scatterings <ei>l_i gamma -> H_R^-- tau^+</ei>.
Code 3144.
</flag>
<flag name="LeftRightSymmmetry:ff2HRff" default="off">
Scatterings <ei>f_1 f_2 -> H_R^-- f_3 f_4</ei> via <ei>WW</ei> fusion.
Code 3145.
</flag>
<flag name="LeftRightSymmmetry:ffbar2HRHR" default="off">
Scatterings <ei>f fbar -> H_R^++ H_L^--</ei>.
Code 3146.
</flag>
<h3>Parameters</h3>
The basic couplings of the model are
<parm name="LeftRightSymmmetry:gL" default="0.64" min="0.0">
lefthanded coupling <ei>g_L = e / sin(theta)</ei>.
</parm>
<parm name="LeftRightSymmmetry:gR" default="0.64" min="0.0">
righthanded coupling <ei>g_R</ei>, assumed the same as <ei>g_L</ei>.
</parm>
<parm name="LeftRightSymmmetry:vL" default="5." min="0.0">
vacuum expectation value <ei>v_L</ei> (in GeV) for the left-triplet.
</parm>
<p/>
The corresponding vacuum expectation value <ei>v_R</ei> is assumed
given by <ei>v_R = sqrt(2) M_WR / g_R</ei> and is not stored explicitly.
<p/>
The Yukawa couplings of a lepton pair to a <ei>H^--</ei>, assumed the
same for <ei>H_L^--</ei> and <ei>H_R^--</ei>, is described by a symmetric
3-by-3 matrix. The default matrix is dominated by the diagonal elements
and especially by the <ei>tau tau</ei> one.
<parm name="LeftRightSymmmetry:coupHee" default="0.1" min="0.0">
Yukawa coupling for <ei>H^-- -> e- e-</ei>.
</parm>
<parm name="LeftRightSymmmetry:coupHmue" default="0.01" min="0.0">
Yukawa coupling for <ei>H^-- -> mu- e-</ei>.
</parm>
<parm name="LeftRightSymmmetry:coupHmumu" default="0.1" min="0.0">
Yukawa coupling for <ei>H^-- -> mu- mu-</ei>.
</parm>
<parm name="LeftRightSymmmetry:coupHtaue" default="0.01" min="0.0">
Yukawa coupling for <ei>H^-- -> tau- e-</ei>.
</parm>
<parm name="LeftRightSymmmetry:coupHtaumu" default="0.01" min="0.0">
Yukawa coupling for <ei>H^-- -> tau- mu-</ei>.
</parm>
<parm name="LeftRightSymmmetry:coupHtautau" default="0.3" min="0.0">
Yukawa coupling for <ei>H^-- -> tau- tau-</ei>.
</parm>
</chapter>
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