C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)

C_N(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)

C_N(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)

SRC(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)

SRC(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)

C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)

C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs

<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs

<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs

<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs

$K^{0}_{S}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class I+II (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class III+IV (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class V+VI (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class VII+VIII (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class IX+X (pp at $\sqrt{s}=7$ TeV).

$2K^{0}_{S}/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Lambda+\bar{\Lambda})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Xi^{-}+\bar{\Xi}^{+})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Omega^{-}+\bar{\Omega}^{+})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$\pi^{+}+\pi^{-}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$p+\bar{p}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$K^{0}_{S}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Lambda+\bar{\Lambda}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Xi^{-}+\bar{\Xi}^{+}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Omega^{-}+\bar{\Omega}^{+}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$(\Lambda+\bar{\Lambda})/2K^{0}_{S}$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of charged particle multiplicity density at midrapidity.

$(p+\bar{p})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of charged particle multiplicity density at midrapidity.

$(2K^{0}_{S})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Lambda+\bar{\Lambda})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Xi^{-}+\bar{\Xi}^{+})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Omega^{-}+\bar{\Omega}^{+})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

Event multiplicity classes, their corresponding fraction of the INEL>0 cross-section and their corresponding average charged particle density at midrapidity ($|\eta|<0.5$). The value of in the inclusive (INEL>0) class is 5.96 $\pm$ 0.23. The uncertainties are the quadratic sum of statistical and systematic contributions.

pion <uQ>3 as a function of pT in pp collision.

kaon <uQ>3 as a function of pT in pp collision.

proton <uQ>3 as a function of pT in pp collision.

pion <uQ>4 as a function of pT in pp collision.

kaon <uQ>4 as a function of pT in pp collision.

proton <uQ>4 as a function of pT in pp collision.

pion <uQ>5 as a function of pT in pp collision.

kaon <uQ>5 as a function of pT in pp collision.

proton <uQ>5 as a function of pT in pp collision.

pion <uQ>2 as a function of pT for centrality: 0-1%.

pion <uQ>2 as a function of pT for centrality: 20-30%.

pion <uQ>2 as a function of pT for centrality: 40-50%.

kaon <uQ>2 as a function of pT for centrality: 0-1%.

kaon <uQ>2 as a function of pT for centrality: 20-30%.

kaon <uQ>2 as a function of pT for centrality: 40-50%.

proton <uQ>2 as a function of pT for centrality: 0-1%.

proton <uQ>2 as a function of pT for centrality: 20-30%.

proton <uQ>2 as a function of pT for centrality: 40-50%.

pion <uQ>3 as a function of pT for centrality: 0-1%.

pion <uQ>3 as a function of pT for centrality: 20-30%.

pion <uQ>3 as a function of pT for centrality: 40-50%.

kaon <uQ>3 as a function of pT for centrality: 0-1%.

kaon <uQ>3 as a function of pT for centrality: 20-30%.

kaon <uQ>3 as a function of pT for centrality: 40-50%.

proton <uQ>3 as a function of pT for centrality: 0-1%.

proton <uQ>3 as a function of pT for centrality: 20-30%.

proton <uQ>3 as a function of pT for centrality: 40-50%.

pion <uQ>4 as a function of pT for centrality: 0-1%.

pion <uQ>4 as a function of pT for centrality: 20-30%.

pion <uQ>4 as a function of pT for centrality: 40-50%.

kaon <uQ>4 as a function of pT for centrality: 0-1%.

kaon <uQ>4 as a function of pT for centrality: 20-30%.

kaon <uQ>4 as a function of pT for centrality: 40-50%.

proton <uQ>4 as a function of pT for centrality: 0-1%.

proton <uQ>4 as a function of pT for centrality: 20-30%.

proton <uQ>4 as a function of pT for centrality: 40-50%.

pion <uQ>5 as a function of pT for centrality: 0-1%.

pion <uQ>5 as a function of pT for centrality: 20-30%.

pion <uQ>5 as a function of pT for centrality: 40-50%.

kaon <uQ>5 as a function of pT for centrality: 0-1%.

kaon <uQ>5 as a function of pT for centrality: 20-30%.

kaon <uQ>5 as a function of pT for centrality: 40-50%.

proton <uQ>5 as a function of pT for centrality: 0-1%.

proton <uQ>5 as a function of pT for centrality: 20-30%.

proton <uQ>5 as a function of pT for centrality: 40-50%.

pion v2 as a function of pT for centrality: 0-1%.

pion v2 as a function of pT for centrality: 0-5%.

pion v2 as a function of pT for centrality: 5-10%.

pion v2 as a function of pT for centrality: 10-20%.

pion v2 as a function of pT for centrality: 20-30%.

pion v2 as a function of pT for centrality: 30-40%.

pion v2 as a function of pT for centrality: 40-50%.

kaon v2 as a function of pT for centrality: 0-1%.

kaon v2 as a function of pT for centrality: 0-5%.

kaon v2 as a function of pT for centrality: 5-10%.

kaon v2 as a function of pT for centrality: 10-20%.

kaon v2 as a function of pT for centrality: 20-30%.

kaon v2 as a function of pT for centrality: 30-40%.

kaon v2 as a function of pT for centrality: 40-50%.

proton v2 as a function of pT for centrality: 0-1%.

proton v2 as a function of pT for centrality: 0-5%.

proton v2 as a function of pT for centrality: 5-10%.

proton v2 as a function of pT for centrality: 10-20%.

proton v2 as a function of pT for centrality: 20-30%.

proton v2 as a function of pT for centrality: 30-40%.

proton v2 as a function of pT for centrality: 40-50%.

pion v3 as a function of pT for centrality: 0-1%.

pion v3 as a function of pT for centrality: 0-5%.

pion v3 as a function of pT for centrality: 5-10%.

pion v3 as a function of pT for centrality: 10-20%.

pion v3 as a function of pT for centrality: 20-30%.

pion v3 as a function of pT for centrality: 30-40%.

pion v3 as a function of pT for centrality: 40-50%.

kaon v3 as a function of pT for centrality: 0-1%.

kaon v3 as a function of pT for centrality: 0-5%.

kaon v3 as a function of pT for centrality: 5-10%.

kaon v3 as a function of pT for centrality: 10-20%.

kaon v3 as a function of pT for centrality: 20-30%.

kaon v3 as a function of pT for centrality: 30-40%.

kaon v3 as a function of pT for centrality: 40-50%.

proton v3 as a function of pT for centrality: 0-1%.

proton v3 as a function of pT for centrality: 0-5%.

proton v3 as a function of pT for centrality: 5-10%.

proton v3 as a function of pT for centrality: 10-20%.

proton v3 as a function of pT for centrality: 20-30%.

proton v3 as a function of pT for centrality: 30-40%.

proton v3 as a function of pT for centrality: 40-50%.

pion v4 as a function of pT for centrality: 0-1%.

pion v4 as a function of pT for centrality: 0-5%.

pion v4 as a function of pT for centrality: 5-10%.

pion v4 as a function of pT for centrality: 10-20%.

pion v4 as a function of pT for centrality: 20-30%.

pion v4 as a function of pT for centrality: 30-40%.

pion v4 as a function of pT for centrality: 40-50%.

kaon v4 as a function of pT for centrality: 0-1%.

kaon v4 as a function of pT for centrality: 0-5%.

kaon v4 as a function of pT for centrality: 5-10%.

kaon v4 as a function of pT for centrality: 10-20%.

kaon v4 as a function of pT for centrality: 20-30%.

kaon v4 as a function of pT for centrality: 30-40%.

kaon v4 as a function of pT for centrality: 40-50%.

proton v4 as a function of pT for centrality: 0-1%.

proton v4 as a function of pT for centrality: 0-5%.

proton v4 as a function of pT for centrality: 5-10%.

proton v4 as a function of pT for centrality: 10-20%.

proton v4 as a function of pT for centrality: 20-30%.

proton v4 as a function of pT for centrality: 30-40%.

proton v4 as a function of pT for centrality: 40-50%.

pion v5 as a function of pT for centrality: 0-1%.

pion v5 as a function of pT for centrality: 0-5%.

pion v5 as a function of pT for centrality: 5-10%.

pion v5 as a function of pT for centrality: 10-20%.

pion v5 as a function of pT for centrality: 20-30%.

pion v5 as a function of pT for centrality: 30-40%.

pion v5 as a function of pT for centrality: 40-50%.

kaon v5 as a function of pT for centrality: 0-1%.

kaon v5 as a function of pT for centrality: 0-5%.

kaon v5 as a function of pT for centrality: 5-10%.

kaon v5 as a function of pT for centrality: 10-20%.

kaon v5 as a function of pT for centrality: 20-30%.

kaon v5 as a function of pT for centrality: 30-40%.

kaon v5 as a function of pT for centrality: 40-50%.

proton v5 as a function of pT for centrality: 0-1%.

proton v5 as a function of pT for centrality: 0-5%.

proton v5 as a function of pT for centrality: 5-10%.

proton v5 as a function of pT for centrality: 10-20%.

proton v5 as a function of pT for centrality: 20-30%.

proton v5 as a function of pT for centrality: 30-40%.

proton v5 as a function of pT for centrality: 40-50%.

pion delta2 as a function of pT for centrality: 0-1%.

pion delta2 as a function of pT for centrality: 0-5%.

pion delta2 as a function of pT for centrality: 5-10%.

pion delta2 as a function of pT for centrality: 10-20%.

pion delta2 as a function of pT for centrality: 20-30%.

pion delta2 as a function of pT for centrality: 30-40%.

pion delta2 as a function of pT for centrality: 40-50%.

kaon delta2 as a function of pT for centrality: 0-1%.

kaon delta2 as a function of pT for centrality: 0-5%.

kaon delta2 as a function of pT for centrality: 5-10%.

kaon delta2 as a function of pT for centrality: 10-20%.

kaon delta2 as a function of pT for centrality: 20-30%.

kaon delta2 as a function of pT for centrality: 30-40%.

kaon delta2 as a function of pT for centrality: 40-50%.

proton delta2 as a function of pT for centrality: 0-1%.

proton delta2 as a function of pT for centrality: 0-5%.

proton delta2 as a function of pT for centrality: 5-10%.

proton delta2 as a function of pT for centrality: 10-20%.

proton delta2 as a function of pT for centrality: 20-30%.

proton delta2 as a function of pT for centrality: 30-40%.

proton delta2 as a function of pT for centrality: 40-50%.

pion delta3 as a function of pT for centrality: 0-1%.

pion delta3 as a function of pT for centrality: 0-5%.

pion delta3 as a function of pT for centrality: 5-10%.

pion delta3 as a function of pT for centrality: 10-20%.

pion delta3 as a function of pT for centrality: 20-30%.

pion delta3 as a function of pT for centrality: 30-40%.

pion delta3 as a function of pT for centrality: 40-50%.

kaon delta3 as a function of pT for centrality: 0-1%.

kaon delta3 as a function of pT for centrality: 0-5%.

kaon delta3 as a function of pT for centrality: 5-10%.

kaon delta3 as a function of pT for centrality: 10-20%.

kaon delta3 as a function of pT for centrality: 20-30%.

kaon delta3 as a function of pT for centrality: 30-40%.

kaon delta3 as a function of pT for centrality: 40-50%.

proton delta3 as a function of pT for centrality: 0-1%.

proton delta3 as a function of pT for centrality: 0-5%.

proton delta3 as a function of pT for centrality: 5-10%.

proton delta3 as a function of pT for centrality: 10-20%.

proton delta3 as a function of pT for centrality: 20-30%.

proton delta3 as a function of pT for centrality: 30-40%.

proton delta3 as a function of pT for centrality: 40-50%.

pion delta4 as a function of pT for centrality: 0-1%.

pion delta4 as a function of pT for centrality: 0-5%.

pion delta4 as a function of pT for centrality: 5-10%.

pion delta4 as a function of pT for centrality: 10-20%.

pion delta4 as a function of pT for centrality: 20-30%.

pion delta4 as a function of pT for centrality: 30-40%.

pion delta4 as a function of pT for centrality: 40-50%.

kaon delta4 as a function of pT for centrality: 0-1%.

kaon delta4 as a function of pT for centrality: 0-5%.

kaon delta4 as a function of pT for centrality: 5-10%.

kaon delta4 as a function of pT for centrality: 10-20%.

kaon delta4 as a function of pT for centrality: 20-30%.

kaon delta4 as a function of pT for centrality: 30-40%.

kaon delta4 as a function of pT for centrality: 40-50%.

proton delta4 as a function of pT for centrality: 0-1%.

proton delta4 as a function of pT for centrality: 0-5%.

proton delta4 as a function of pT for centrality: 5-10%.

proton delta4 as a function of pT for centrality: 10-20%.

proton delta4 as a function of pT for centrality: 20-30%.

proton delta4 as a function of pT for centrality: 30-40%.

proton delta4 as a function of pT for centrality: 40-50%.

pion delta5 as a function of pT for centrality: 0-1%.

pion delta5 as a function of pT for centrality: 0-5%.

pion delta5 as a function of pT for centrality: 5-10%.

pion delta5 as a function of pT for centrality: 10-20%.

pion delta5 as a function of pT for centrality: 20-30%.

pion delta5 as a function of pT for centrality: 30-40%.

pion delta5 as a function of pT for centrality: 40-50%.

kaon delta5 as a function of pT for centrality: 0-1%.

kaon delta5 as a function of pT for centrality: 0-5%.

kaon delta5 as a function of pT for centrality: 5-10%.

kaon delta5 as a function of pT for centrality: 10-20%.

kaon delta5 as a function of pT for centrality: 20-30%.

kaon delta5 as a function of pT for centrality: 30-40%.

kaon delta5 as a function of pT for centrality: 40-50%.

proton delta5 as a function of pT for centrality: 0-1%.

proton delta5 as a function of pT for centrality: 0-5%.

proton delta5 as a function of pT for centrality: 5-10%.

proton delta5 as a function of pT for centrality: 10-20%.

proton delta5 as a function of pT for centrality: 20-30%.

proton delta5 as a function of pT for centrality: 30-40%.

proton delta5 as a function of pT for centrality: 40-50%.

pion Integrated v2 as a function of centrality percentile:.

kaon Integrated v2 as a function of centrality percentile:.

proton Integrated v2 as a function of centrality percentile:.

pion Integrated v3 as a function of centrality percentile:.

kaon Integrated v3 as a function of centrality percentile:.

proton Integrated v3 as a function of centrality percentile:.

pion Integrated v4 as a function of centrality percentile:.

kaon Integrated v4 as a function of centrality percentile:.

proton Integrated v4 as a function of centrality percentile:.

pion Integrated v5 as a function of centrality percentile:.

kaon Integrated v5 as a function of centrality percentile:.

proton Integrated v5 as a function of centrality percentile:.

Data (bold boxes) and background estimates (colour fill) for m_beta vs. m_betagamma for the gluino R-hadron search (1000 GeV). The blue thin-line boxes illustrate the expected signal (on top of background) for the given R-hadron mass hypothesis. The black dashed vertical/horizontal lines at 500 GeV show the mass selection (signal region in the top-right). Two events pass this selection.

Expected (dashed black line) and observed (solid red line) 95% CL upper limits on the cross section as a function of mass for the production of long-lived gluino R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. The observed 8 TeV Run-1 limit and theory prediction [arXiv:1411.6795] are shown in dash-dotted and dotted lines, respectively.

Expected (dashed black line) and observed (solid red line) 95% CL upper limits on the cross section as a function of mass for the production of bottom-squark R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. The observed 8 TeV Run-1 limit and theory prediction [arXiv:1411.6795] are shown in dash-dotted and dotted lines, respectively.

Expected (dashed black line) and observed (solid red line) 95% CL upper limits on the cross section as a function of mass for the production of top-squark R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. The observed 8 TeV Run-1 limit and theory prediction [arXiv:1411.6795] are shown in dash-dotted and dotted lines, respectively.

Final selection requirements as a function of the simulated R-hadron mass.

Summary of all studied systematic uncertainties. Ranges indicate a dependency on the R-hadron mass hypothesis (from low to high masses).

Expected signal yield (Nsig) and efficiency (eff.), estimated background (Nbkg) and observed number of events in data (Nobs) for the full mass range after the final selection using 3.2/fb of data. The stated uncertainties include both the statistical and systematic contribution.

Distribution of the truth-level beta for gluino R-hadrons in exemplary signal MC samples and muons in a Zmumu MC sample. All distributions have been normalised to one. The last bin contains the overflow of the histograms. The distributions illustrate the good discriminating power of the variables.

Distribution of the truth-level betagamma for gluino R-hadrons in exemplary signal MC samples and muons in a Zmumu MC sample. All distributions have been normalised to one. The last bin contains the overflow of the histograms. The distributions illustrate the good discriminating power of the variables.

Expected (dashed black line) and observed (solid red line) 95% confidence level upper limits on the cross section as a function of mass for the production of long-lived gluino R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. For meta-stable gluinos with a lifetime of 50 ns. (mass exclusion: about 1660 GeV expected, 1520 GeV observed).

Expected (dashed black line) and observed (solid red line) 95% confidence level upper limits on the cross section as a function of mass for the production of long-lived gluino R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. For meta-stable gluinos with a lifetime of 30 ns. (mass exclusion: about 1660 GeV expected, 1520 GeV observed).

Expected (dashed black line) and observed (solid red line) 95% confidence level upper limits on the cross section as a function of mass for the production of long-lived gluino R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. For meta-stable gluinos with a lifetime of 10 ns. (mass exclusion: about 1660 GeV expected, 1520 GeV observed).

Object-quality selection cut-flow with observed data and exemplary expected events (scaled to 3.2/fb for MC) in the gluino R-hadron search.

Object-quality selection cut-flow with observed data and exemplary expected events (scaled to 3.2/fb for MC) in the squark R-hadron search.

Expected signal yield (Nsig) and efficiency (eff.), estimated background (Nbkg) and observed number of events in data (Nobs) for the full mass range in the meta-stable gluino R-hadron search using 3.2/fb of data. The stated uncertainties include both the statistical and systematic contribution.

Comparison of data with estimated backgrounds in the $\tilde{E}_\text{T}^\text{miss}$ distribution with the TZCR1 event selection except for the requirement on $\tilde{E}_\text{T}^\text{miss}$. The variables $\tilde{E}_\text{T}^\text{miss}$ and $\tilde{m}_\text{T}$ are constructed in the same way as $E_\text{T}^\text{miss}$ and $m_\text{T}$ but treating the leading photon transverse momentum as invisible. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.

Comparison of data with estimated backgrounds in the $\tilde{m}_\text{T}$ distribution with the TZCR1 event selection except for the requirement on $\tilde{m}_\text{T}$. The variables $\tilde{E}_\text{T}^\text{miss}$ and $\tilde{m}_\text{T}$ are constructed in the same way as $E_\text{T}^\text{miss}$ and $m_\text{T}$ but treating the leading photon transverse momentum as invisible. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.

Comparison of the observed data ($n_\text{obs}$) with the predicted background ($n_\text{exp}$) in the validation and signal regions. The background predictions are obtained using the background-only fit configuration. The bottom panel shows the significance of the difference between data and predicted background, where the significance is based on the total uncertainty ($\sigma_\text{tot}$).

Jet multiplicity distributions for events where exactly two signal leptons are selected. No correction factors are included in the background normalizations. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.

Jet multiplicity distributions for events where exactly one lepton plus one $\tau$ candidate are selected. No correction factors are included in the background normalizations. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.

The $E_\text{T}^\text{miss}$ distribution in SR1. In the plot, the full event selection in the corresponding signal region is applied, except for the requirement on $E_\text{T}^\text{miss}$. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin contains the overflow. Benchmark signal models are overlaid for comparison. The benchmark models are specified by the gluino and stop masses, given in TeV in the table.

The $m_\text{T}$ distribution in SR1. In the plot, the full event selection in the corresponding signal region is applied, except for the requirement on $m_\text{T}$. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin contains the overflow. Benchmark signal models are overlaid for comparison. The benchmark models are specified by the gluino and stop masses, given in TeV in the table.

Expected (black dashed) 95% excluded regions in the plane of $m_{\tilde{g}}$ versus $m_{\tilde{t}_1}$ for gluino-mediated stop production.

Observed (red solid) 95% excluded regions in the plane of $m_{\tilde{g}}$ versus $m_{\tilde{t}_1}$ for gluino-mediated stop production.

Expected (black dashed) 95% excluded regions in the plane of $m_{\tilde{t}_1}$ versus $m_{\tilde{\chi}_1^0}$ for direct stop production.

Observed (red solid) 95% excluded regions in the plane of $m_{\tilde{t}_1}$ versus $m_{\tilde{\chi}_1^0}$ for direct stop production.

The expected upper limits on $T$ quark pair production times the squared branching ratio for $T \rightarrow tZ$ as a function of the $T$ quark mass.

The observed upper limits on $T$ quark pair production times the squared branching ratio for $T \rightarrow tZ$ as a function of the $T$ quark mass.

The expected limits on $T$ quarks as a function of the branching ratios $B\left(T \rightarrow bW\right)$ and $B\left(T \rightarrow tH\right)$ for a $T$ quark with a mass of 800 GeV. The $T$ is assumed to decay in three possible ways: $T \to tZ$, $T \to tH$, and $T \to bW$.

The observed limits on $T$ quarks as a function of the branching ratios $B\left(T \rightarrow bW\right)$ and $B\left(T \rightarrow tH\right)$ for a $T$ quark with a mass of 800 GeV. The $T$ is assumed to decay in three possible ways: $T \to tZ$, $T \to tH$, and $T \to bW$.

The $m_\text{T}$ distribution in the WVR2-tail validation region which has the same preselection and jet $p_\text{T}$ requirements as SR2.

The $am_\text{T2}$ distribution in the WVR2-tail validation region which has the same preselection and jet $p_\text{T}$ requirements as SR2.

Large-radius jet mass ($R=1.2$), decomposed into the number of small-radius jet constituents. The lower panel shows the ratio of the total data to the total prediction (summed over all jet multiplicities). Events are required to have one lepton, four jets with $p_\text{T}>80,50,40,40$ GeV, at least one $b$-tagged jet, $E_\text{T}^\text{miss}>200$ GeV, and $m_\text{T}>30$ GeV.

Distribution of $m_\text{T2}^\tau$ in data for a selection enriched in $t\bar{t}$ events with one hadronically decaying $\tau$. Events that have no hadronic $\tau$ candidate (that passes the Loose identification criteria, as well as other requirements) are not shown in the plot.

Upper limits on the model cross-section in units of pb for the gluino-mediated stop models.

Upper limits on the model cross-section in units of pb for the models with direct stop pair production.

Illustration of the best expected signal region per signal grid point for the gluino-mediated stop models. This mapping is used for the final combined exclusion limits.

Illustration of the best expected signal region per signal grid point for models with direct stop pair production. This mapping is used for the final combined exclusion limits.

Expected $CL_s$ values for the gluino-mediated stop models.

Observed $CL_s$ values for the gluino-mediated stop models.

Expected $CL_s$ values for the direct stop pair production models.

Observed $CL_s$ values for the direct stop pair production models.

Expected limit using SR1 for models with direct stop pair production and an unpolarized stop (and bino LSP).

Expected limit using SR1 for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Expected limit using SR1 for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Observed limit using SR1 for models with direct stop pair production and an unpolarized stop (and bino LSP).

Observed limit using SR1 for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Observed limit using SR1 for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Expected limit using SR2 for models with direct stop pair production and an unpolarized stop (and bino LSP).

Expected limit using SR2 for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Expected limit using SR2 for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Observed limit using SR2 for models with direct stop pair production and an unpolarized stop (and bino LSP).

Observed limit using SR2 for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Observed limit using SR2 for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Expected limit using SR1+SR2 (best expected) for models with direct stop pair production and an unpolarized stop (and bino LSP).

Expected limit using SR1+SR2 (best expected) for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Expected limit using SR1+SR2 (best expected) for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Observed limit using SR1+SR2 (best expected) for models with direct stop pair production and an unpolarized stop (and bino LSP).

Observed limit using SR1+SR2 (best expected) for models with direct stop pair production with $\tilde{t}_1=\tilde{t}_L$ (and bino LSP).

Observed limit using SR1+SR2 (best expected) for models with direct stop pair production with $\tilde{t}_1\sim\tilde{t}_R$ (and bino LSP).

Acceptance for SR1 in the gluino-mediated stop models. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR1 in the direct stop pair production. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR2 in the gluino-mediated stop models. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR2 in the direct stop pair production. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR3 in the gluino-mediated stop models. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Acceptance for SR3 in the direct stop pair production. The acceptance is defined as the fraction of signal events that pass the analysis selection performed on generator-level objects, therefore emulating an ideal detector with perfect particle identification and no measurement resolution effects.

Efficiency for SR1 in the gluino-mediated stop models. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR1 in the direct stop pair production. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR2 in the gluino-mediated stop models. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR2 in the direct stop pair production. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR3 in the gluino-mediated stop models. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Efficiency for SR3 in the direct stop pair production. The efficiency is the ratio between the expected signal rate calculated with simulated data passing all the reconstruction level cuts applied to reconstructed objects, and the signal rate for an ideal detector (with perfect particle identification and no measurement resolution effects).

Median expected and observed 95% CL upper limits on the cross-section times branching ratio (sigma*B) for W'_SSM production for the exclusive muon and electron channels, and for both channels combined.

Ratio of fiducial cross sections measured for $W^{\pm} Z$ production at $\sqrt{s}=13$ TeV and $\sqrt{s}=8$ TeV. The first systematic uncertainty is the combined systematic uncertainty excluding the luminosity uncertainty, the second is the luminosity uncertainty.

Ratio of fiducial cross sections measured for $W^{+} Z$ and $W^{-} Z$ production.

Cross section extrapolated to total phase space and all W and Z boson decays. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the theory uncertainty and the third is the luminosity uncertainty.

The measured fiducial cross sections are corrected to the dressed level. The ratio of $C_{WZ}^{\textrm{dressed}}/C_{WZ}^{\textrm{Born}}$ factors presented in this table can be used to correct fiducial integrated cross sections from dressed to Born level.

Measured fiducial cross section as a function of the exclusive jet multiplicity, where jets are particle level jets with anti-kt R=0.4. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

The total cross section is measured at dressed level and can also be corrected to Born level use this acceptance correction factor.

Correlation matrix for the total uncertainties, including all sources of systematic and statistical uncertainties, for the differential cross section as a function of the exclusive jet multiplicity.

All correlated systematic relative uncertainties in percent on measured differential cross section as a function of the exclusive jet multiplicity.