Table 1.

List of experimental constraints used in this work, including experimental and (where applicable) theoretical errors: supersymmetric theory uncertainties in the interpretations of one-sided experimental limits are indicated by [$\dots$]

Observable	Source Th./Ex.	Constraint
$m_t$ [GeV]	[93]	$173.2\pm 0.87$
$\mathrm{\Delta }{\mathit{\alpha }}_{\mathrm{had}}^{(5)}(M_Z)$	[93]	$0.02756\pm 0.00010$
$M_Z$ [GeV]	[93, 94]	$91.1875\pm 0.0021$
${\mathrm{\Gamma }}_Z$ [GeV]	[93–96]	$2.4952\pm 0.0023\pm 0.{001}_{\mathrm{SUSY}}$
${\mathit{\sigma }}_{\mathrm{had}}^0$ [nb]	[93–96]	$41.540\pm 0.037$
$R_l$	[93–96]	$20.767\pm 0.025$
$A_{\mathrm{fb}}(\ell )$	[93–96]	$0.01714\pm 0.00095$
$A_{\ell }(P_{\mathit{\tau }})$	[93–96]	0.1465 $\pm$ 0.0032
$R_{\mathrm{b}}$	[93–96]	0.21629 $\pm$ 0.00066
$R_{\mathrm{c}}$	[93–96]	0.1721 $\pm$ 0.0030
$A_{\mathrm{fb}}(b)$	[93–96]	0.0992 $\pm$ 0.0016
$A_{\mathrm{fb}}(c)$	[93–96]	0.0707 $\pm$ 0.0035
$A_b$	[93–96]	0.923 $\pm$ 0.020
$A_c$	[93–96]	0.670 $\pm$ 0.027
$A_{\ell }(\mathrm{SLD})$	[93–96]	0.1513 $\pm$ 0.0021
${sin}^2{\mathit{\theta }}_{\mathrm{w}}^{\ell }(Q_{\mathrm{fb}})$	[93–96]	0.2324 $\pm$ 0.0012
$M_W$ [GeV]	[93–96]	$80.385\pm 0.015\pm 0.{010}_{\mathrm{SUSY}}$
$a_{\mathit{\mu }}^{\mathrm{EXP}}-a_{\mathit{\mu }}^{\mathrm{SM}}$	[65–74]	$(30.2\pm 8.8\pm 2.0_{\mathrm{SUSY}})\times {10}^{-10}$
$M_h$ [GeV]	[97–101]/[93]	$125.7\pm 0.4\pm 1.5_{\mathrm{SUSY}}$
BR${}_{\mathrm{b}\to \mathrm{s}\mathit{\gamma }}^{\mathrm{EXP}/\mathrm{SM}}$	[81, 102–106]	$1.089\pm 0.{070}_{\mathrm{EXP}}$
		$\pm 0.{080}_{\mathrm{SM}}\pm 0.{050}_{\mathrm{SUSY}}$
BR$(B_{s,d}\to {\mathit{\mu }}^{+}{\mathit{\mu }}^{-})$	[14–16, 107–111]	CMS & LHCb
BR${}_{\mathrm{B}\to \mathit{\tau }\mathit{\nu }}^{\mathrm{EXP}/\mathrm{SM}}$	[81, 112–114]	$1.39\pm 0.{28}_{\mathrm{EXP}}\pm 0.{13}_{\mathrm{SM}}$
${\mathrm{BR}}_{B\to X_s\ell \ell }^{\mathrm{EXP}/\mathrm{SM}}$	[81, 115]	$0.99\pm 0.32$
BR${}_{K\to \mathit{\mu }\mathit{\nu }}^{\mathrm{EXP}/\mathrm{SM}}$	[112, 113, 116]	$1.008\pm 0.{014}_{\mathrm{EXP}+\mathrm{TH}}$
BR${}_{K\to \mathit{\pi }\mathit{\nu }\overline{\mathit{\nu }}}^{\mathrm{EXP}/\mathrm{SM}}$	[117, 118]	$<4.5$
$\mathrm{\Delta }{M}_{B_s}^{\mathrm{EXP}/\mathrm{SM}}$	[117, 119]	$0.97\pm 0.{20}_{\mathrm{SM}}$
$\frac{\mathrm{\Delta }{M}_{B_s}^{\mathrm{EXP}/\mathrm{SM}}}{\mathrm{\Delta }{M}_{B_d}^{\mathrm{EXP}/\mathrm{SM}}}$	[112, 113, 119]	$0.86\pm 0.{14}_{\mathrm{SM}}$
$\mathrm{\Delta }{\mathit{ϵ}}_K^{\mathrm{EXP}/\mathrm{SM}}$	[81, 117]	$1.14\pm 0.{10}_{\mathrm{EXP}+\mathrm{TH}}$
${\mathrm{\Omega }}_{\mathrm{CDM}}{h}^2$	[120–123]	$0.1186\pm 0.0022\pm 0.{0120}_{\mathrm{SUSY}}$
${\mathit{\sigma }}_p^{\mathrm{SI}}$	[84]	$(m_{{\tilde{\mathit{\chi }}}_1^0},{\mathit{\sigma }}_p^{\mathrm{SI}})$ plane
jets + ${/E}_T$	[10]	$(m_0,m_{1/2})$ plane
$H/A,H^{\pm }$	[124, 125]	$(M_A,tan\mathit{\beta })$ plane