Table 2.

Variable input parameters of the ATLAS pMSSM scan and the range over which these parameters are scanned

Parameter	Description	Scanned range
$m_{{\tilde{L}}_1}$	1$\mathrm{st}$/2$\mathrm{nd}$ gen. SU(2) doublet soft breaking slepton mass	$[90\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{E}}_1}$	1$\mathrm{st}$/2$\mathrm{nd}$ gen. SU(2) singlet soft breaking slepton mass	$[90\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{L}}_3}$	3$\mathrm{rd}$ gen. SU(2) doublet soft breaking slepton mass	$[90\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{E}}_3}$	3$\mathrm{rd}$ gen. SU(2) singlet soft breaking slepton mass	$[90\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{Q}}_1}$	1$\mathrm{st}$/2$\mathrm{nd}$ gen. SU(2) doublet soft breaking squark mass	$[200\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{U}}_1}$	1$\mathrm{st}$/2$\mathrm{nd}$ gen. SU(2) singlet soft breaking squark mass	$[200\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{D}}_1}$	1$\mathrm{st}$/2$\mathrm{nd}$ gen. SU(2) singlet soft breaking squark mass	$[200\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{Q}}_3}$	3$\mathrm{rd}$ gen. SU(2) doublet soft breaking squark mass	$[100\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{U}}_3}$	3$\mathrm{rd}$ gen. SU(2) singlet soft breaking squark mass	$[100\mathrm{GeV},4\mathrm{TeV}]$
$m_{{\tilde{D}}_3}$	3$\mathrm{rd}$ gen. SU(2) singlet soft breaking squark mass	$[100\mathrm{GeV},4\mathrm{TeV}]$
$A_t$	Stop trilinear coupling	$[-8\mathrm{TeV},8\mathrm{TeV}]$
$A_b$	Sbottom trilinear coupling	$[-4\mathrm{TeV},4\mathrm{TeV}]$
$A_{\mathit{\tau }}$	Stau trilinear coupling	$[-4\mathrm{TeV},4\mathrm{TeV}]$
$|\mathit{\mu }|$	Higgsino mass parameter	$[80\mathrm{GeV},4\mathrm{TeV}]$
$|M_1|$	Bino mass parameter	$[0\mathrm{TeV},4\mathrm{TeV}]$
$|M_2|$	Wino mass parameter	$[70\mathrm{GeV},4\mathrm{TeV}]$
$M_3$	Gluino mass parameter	$[200\mathrm{GeV},4\mathrm{TeV}]$
$M_A$	Pseudoscalar Higgs mass	$[100\mathrm{GeV},4\mathrm{TeV}]$
$\tan \mathit{\beta }$	Ratio of vacuum expectation values	$[1,60]$