main507.cc and 
main508.cc. 
 
 
The particles in the scenarios considered here are a mix of established 
PDG ones (51 - 55) and extensions thereof ( 56 - 59), as follows: 
| 51 | Scalar DM (currently unused); | 
| 52 | Fermionic DM (chi_1); | 
| 53 | Vector DM (currently unused); | 
| 54 | Scalar (or pseudoscalar) mediator (S); | 
| 55 | Vector (or axial vector) mediator (Z'); | 
| 56 | Charged scalar partner (l^~); | 
| 57 | Singly charged partner (chi^+); | 
| 58 | Neutral partner (chi_2); | 
| 59 | Doubly charged partner (chi^++). | 
flag   DM:gg2S2XX   
 (default = off)flag   DM:gg2S2XXj   
 (default = off)parm   Sdm:vf   
 (default = 0.1)parm   Sdm:af   
 (default = 0)parm   Sdm:vX   
 (default = 1.0)parm   Sdm:aX   
 (default = 0)Zp:decayMode. 
 
mode   Zp:decayMode   
 (default = 0; minimum = 0; maximum = 3)option  0 : X Xbar 
   
option  1 : q qbar (dijets) 
   
option  2 : l lbar (charged dileptons) 
   
option  3 : nu nubar + X Xbar (invisible) 
   
   
 
flag   DM:ffbar2Zp2XX   
 (default = off)flag   DM:ffbar2ZpH   
 (default = off)Zp:coupH. 
Interference with gamma/Z currently not implemented therefore this is 
only suitable when Z' → X Xbar.  This can be ensured 
using 
55:onMode = off 
55:onIfAny = 52 
   
 
flag   DM:ffbar2Zp2XXj   
 (default = off)flag   DM:qg2Zp2XXj   
 (default = off)parm   Zp:vX   
 (default = 1.)parm   Zp:aX   
 (default = 0.)flag   Zp:kineticMixing   
 (default = off)Zp:gZp and the separate fermion couplings by 
Zp:vu through Zp:av. In the alternative, 
with kinetic mixing on, the coupling to the DM is still given by 
Zp:gZp, but the mixing parameter Zp:epsilon 
now specifies how the separate fermion couplings are related to their 
U(1)_Y values. 
   
 
parm   Zp:gZp   
 (default = 0.1)parm   Zp:vu   
 (default = 1.)parm   Zp:au   
 (default = 0.)parm   Zp:vd   
 (default = 1.)parm   Zp:ad   
 (default = 0.)parm   Zp:vl   
 (default = 1.)parm   Zp:al   
 (default = 0.)parm   Zp:vv   
 (default = 1.)parm   Zp:av   
 (default = 0.)parm   Zp:epsilon   
 (default = 0.1)parm   Zp:coupH   
 (default = 0.1)Zp:epsilon. 
   
 
 
DM:DYtype. 
 
 The first model consists of co-annihilation with a scalar with 
leptonic quantum numbers and which couples to a right-handed SM lepton 
and a Dirac fermion Dark Matter via Yukawa couplings.  It is possible 
to choose lepton flavour violating couplings. 
 
 The next model is a generalisation of the mixed gaugino sector 
of Supersymmetry parametrised by one SM singlet and one SU(2) N-plet 
which mix to form Dark matter.  N = 2, 3 and 5 are supported by the 
code.  The main motivation for this choice is to provide a fully 
flexible implementation to calculate production of long-lived 
particles at the LHC.  The resultant spectrum consists of one neutral 
partner, one singly charged partner, and one doubly charged partner 
(in the case of the 5-plet).  The only free parameters are masses of 
the singlet and N-plet and the mixing suppression scale. This 
determines both production and decay of the particles and can cover a 
range of signatures including displaced leptons and vertices, 
long-lived, kinked or disappearing tracks. 
 
flag   DM:qqbar2DY   
 (default = off)mode   DM:DYtype   
 (default = 1; minimum = 1; maximum = 4)option  1 :  Scalar lepton production.  Coupling to electrons, 
muons and taus can be fixed by DM:yuk1, DM:yuk2, 
and DM:yuk3 respectively.    
option  2 :  Production of charged partners (i.e. "charginos").   
option  3 :  Production of doubly charged partners.   
option  4 :  Production of neutral and singly-charged partners.   
 
   
 
 
The Yukawa couplings can be set using 
parm   DM:yuk1   parm   DM:yuk2   parm   DM:yuk3   mode   DM:Nplet   
 (default = 2; minimum = 1; maximum = 3)option  1 :  Doublet    
option  2 :  Triplet    
option  3 :  Quintuplet    
   
 
parm   DM:M1   parm   DM:M2   parm   DM:Lambda