. 2015 Oct 29;75:510. doi: 10.1140/epjc/s10052-015-3726-9

Table 1.

Summary of the ATLAS analyses and signal regions used in this paper. Each signal region is identified by the acronym of the corresponding analysis followed by the original name of the signal region defined either in the published paper or in Appendix B.2. A dash in the signal region name column indicates that the analysis does not use the concept of signal region

Analysis name and corresponding reference	Analysis acronym	Original signal region name	Model targeted
Multijet final states [16]	t0L	SRA1-4	${\tilde{t}}_{1}^{} \to t {\tilde{χ}}_{1}^{0}$
		SRB	${\tilde{t}}_{1}^{} \to t {\tilde{χ}}_{1}^{0}$
		SRC1-3	${\tilde{t}}_{1}^{} {\tilde{t}}_{1}^{} \to b t {\tilde{χ}}_{1}^{0} {\tilde{χ}}_{1}^{\pm}$ with $m_{{\tilde{χ}}_{1}^{\pm}} = 2 m_{{\tilde{χ}}_{1}^{0}}$
One-lepton final states [17]	t1L	tN_diag	${\tilde{t}}_{1}^{} \to t {\tilde{χ}}_{1}^{0}$ with $m_{{\tilde{t}}_{1}^{}} \sim m_{t} + m_{{\tilde{χ}}_{1}^{0}}$
		tN_med, tN_high, tN_boost	${\tilde{t}}_{1}^{} \to t {\tilde{χ}}_{1}^{0}$
		bCa_low, bCa_med, bCb_med1,	${\tilde{t}}_{1}^{} \to b {\tilde{χ}}_{1}^{\pm}$
		bCb_high, bCb_med2, bCc_diag
		bCd_bulk, bCd_high1, bCd_high2
		3body	${\tilde{t}}_{1}^{} \to b W {\tilde{χ}}_{1}^{0}$ (three-body decay)
		tNbC_mix	${\tilde{t}}_{1}^{} {\tilde{t}}_{1}^{} \to b t {\tilde{χ}}_{1}^{0} {\tilde{χ}}_{1}^{\pm}$ with $m_{{\tilde{χ}}_{1}^{\pm}} = 2 m_{{\tilde{χ}}_{1}^{0}}$
Two-lepton final states [18]	t2L	L90, L100, L110, L120, H160	${\tilde{t}}_{1}^{} \to b {\tilde{χ}}_{1}^{\pm}$ , three-body decay
Two-lepton final states [18]	t2L	M1-4	${\tilde{t}}_{1}^{} \to t {\tilde{χ}}_{1}^{0}$
Final states from compressed stop decays [19]	tc	M1-3	${\tilde{t}}_{1}^{} / {\tilde{b}}_{1}^{} \to anything$ with $m_{{\tilde{t}}_{1}^{}} \sim m_{{\tilde{χ}}_{1}^{0}}$
Final states from compressed stop decays [19]	tc	C1-2	${\tilde{t}}_{1}^{} \to c {\tilde{χ}}_{1}^{0}$
Final states with a $Z$ boson [20]	t2t1Z	SR2A, SR2B, SR2C, SR3A, SR3B	${\tilde{t}}_{2}^{} \to {\tilde{t}}_{1}^{} Z$ and ${\tilde{t}}_{2}^{} \to {\tilde{t}}_{1}^{} h$
Final states with two $b$ -jets and $E_{T}^{miss}$ [21]	b0L	SRA, SRB	${\tilde{b}}_{1}^{} \to b {\tilde{χ}}_{1}^{0}$ and ${\tilde{t}}_{1}^{} \to b {\tilde{χ}}_{1}^{\pm}$ with $m_{{\tilde{χ}}_{1}^{\pm}} \sim m_{{\tilde{χ}}_{1}^{0}}$
Final states with two leptons at intermediate $m_{T2}$ (Appendix B.2.1)	WW	SR1–7	${\tilde{t}}_{1}^{} \to b {\tilde{χ}}_{1}^{\pm}$ with $m_{{\tilde{χ}}_{1}^{\pm}} = m_{{\tilde{t}}_{1}^{}} - 10$ GeV and
	WW	SR1–7	${\tilde{t}}_{1}^{} \to b ℓ ν {\tilde{χ}}_{1}^{0}$ (three- and four-body decays)
Final states containing two top quarks and a Higgs boson (Appendix B.2.2)	t2t1h	–	${\tilde{t}}_{2}^{} \to {\tilde{t}}_{1}^{} h$
Final states containing a top and a $b$ -quark (Appendix B.2.3)	tb	SR1-5	${\tilde{t}}_{1}^{} {\tilde{t}}_{1}^{} \to b {\tilde{χ}}_{1}^{\pm} t {\tilde{χ}}_{1}^{0}$ with $m_{{\tilde{χ}}_{1}^{\pm}} \sim m_{{\tilde{χ}}_{1}^{0}}$ and pMSSM models
Final states with three $b$ -jets [62]	g3b	SR-0 $ℓ$ -4j-A, SR-0 $ℓ$ -4j-B, SR-0 $ℓ$ -4j-C,	Gluino-mediated ${\tilde{t}}_{1}^{}$ and ${\tilde{b}}_{1}^{}$ production,
		SR-0 $ℓ$ -7j-A, SR-0 $ℓ$ -7j-B, SR-0 $ℓ$ -7j-C,	${\tilde{b}}_{1}^{} \to {\tilde{χ}}_{2}^{0} b \to {\tilde{χ}}_{1}^{0} h b$
		SR-1 $ℓ$ -6j-A, SR-1 $ℓ$ -6j-B, SR-1 $ℓ$ -7j-C
Strongly produced final states with two same-sign or three leptons [63]	SS3L	SR3b, SR0b, SR1b,	Generic gluino and squark production, ${\tilde{b}}_{1}^{} \to t {\tilde{χ}}_{1}^{\pm}$
	SS3L	SR3Llow, S3Lhigh
Spin correlation in $t \bar{t}$ production events [64]	SC	–	${\tilde{t}}_{1}^{} \to t {\tilde{χ}}_{1}^{0}$ with $m_{{\tilde{t}}_{1}^{}} \sim m_{t} + m_{{\tilde{χ}}_{1}^{0}}$
$t \bar{t}$ production cross section [65]	xsec	–	${\tilde{t}}_{1}^{} \to t {\tilde{χ}}_{1}^{0}$ , three-body decay