$R_\text{CP}$ plotted as a function of approximated $x_p$ for $-1.0 < y_b < 0.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $-1.0 < y_b < 0.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $-1.0 < y_b < 0.0$ and $2.0 < y^* < 3.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $0.0 < y_b < 1.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $0.0 < y_b < 1.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $0.0 < y_b < 1.0$ and $2.0 < y^* < 4.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $1.0 < y_b < 2.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $1.0 < y_b < 2.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $1.0 < y_b < 2.0$ and $2.0 < y^* < 3.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $2.0 < y_b < 3.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $2.0 < y_b < 3.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_p$ for $3.0 < y_b < 4.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $-3.0 < y_b < -2.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $-2.0 < y_b < -1.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $-2.0 < y_b < -1.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $-1.0 < y_b < 0.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $-1.0 < y_b < 0.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $-1.0 < y_b < 0.0$ and $2.0 < y^* < 3.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $0.0 < y_b < 1.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $0.0 < y_b < 1.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $0.0 < y_b < 1.0$ and $2.0 < y^* < 4.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $1.0 < y_b < 2.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $1.0 < y_b < 2.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $1.0 < y_b < 2.0$ and $2.0 < y^* < 3.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $2.0 < y_b < 3.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $2.0 < y_b < 3.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_{Pb}$ for $3.0 < y_b < 4.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $-3.0 < y_b < -2.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $-2.0 < y_b < -1.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $-2.0 < y_b < -1.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $-1.0 < y_b < 0.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $-1.0 < y_b < 0.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $-1.0 < y_b < 0.0$ and $2.0 < y^* < 3.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $0.0 < y_b < 1.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $0.0 < y_b < 1.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $0.0 < y_b < 1.0$ and $2.0 < y^* < 4.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $1.0 < y_b < 2.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $1.0 < y_b < 2.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $1.0 < y_b < 2.0$ and $2.0 < y^* < 3.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $2.0 < y_b < 3.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $2.0 < y_b < 3.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$R_\text{CP}$ plotted as a function of approximated $x_\mathrm{F}$ for $3.0 < y_b < 4.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $40.0 < p_{\text{T,Avg}} \text{ [GeV]} < 49.6$ and $0.0 < y^{*} < 1.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $40.0 < p_{\text{T,Avg}} \text{ [GeV]} < 49.6$ and $0.0 < y^{*} < 1.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $49.6 < p_{\text{T,Avg}} \text{ [GeV]} < 61.4$ and $0.0 < y^{*} < 1.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $49.6 < p_{\text{T,Avg}} \text{ [GeV]} < 61.4$ and $0.0 < y^{*} < 1.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $61.4 < p_{\text{T,Avg}} \text{ [GeV]} < 76.1$ and $0.0 < y^{*} < 1.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $61.4 < p_{\text{T,Avg}} \text{ [GeV]} < 76.1$ and $0.0 < y^{*} < 1.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $40.0 < p_{\text{T,Avg}} \text{ [GeV]} < 49.6$ and $1.0 < y^{*} < 2.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $40.0 < p_{\text{T,Avg}} \text{ [GeV]} < 49.6$ and $1.0 < y^{*} < 2.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $49.6 < p_{\text{T,Avg}} \text{ [GeV]} < 61.4$ and $1.0 < y^{*} < 2.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $49.6 < p_{\text{T,Avg}} \text{ [GeV]} < 61.4$ and $1.0 < y^{*} < 2.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $61.4 < p_{\text{T,Avg}} \text{ [GeV]} < 76.1$ and $1.0 < y^{*} < 2.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $61.4 < p_{\text{T,Avg}} \text{ [GeV]} < 76.1$ and $1.0 < y^{*} < 2.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $40.0 < p_{\text{T,Avg}} \text{ [GeV]} < 49.6$ and $2.0 < y^{*} < 4.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $40.0 < p_{\text{T,Avg}} \text{ [GeV]} < 49.6$ and $2.0 < y^{*} < 4.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $49.6 < p_{\text{T,Avg}} \text{ [GeV]} < 61.4$ and $2.0 < y^{*} < 4.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $49.6 < p_{\text{T,Avg}} \text{ [GeV]} < 61.4$ and $2.0 < y^{*} < 4.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $0-10$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $61.4 < p_{\text{T,Avg}} \text{ [GeV]} < 76.1$ and $2.0 < y^{*} < 4.0$.

$\langle T_{\text{AB}} \rangle$ normalized per-event dijet yields in $60-90$% collisions as a function of $\langle y_{\text{b}} \rangle$ for $61.4 < p_{\text{T,Avg}} \text{ [GeV]} < 76.1$ and $2.0 < y^{*} < 4.0$.

Dielectron pair $p_{T}$ spectrum for $0.18 < m_{\rm ee} < 0.34$ GeV/$c^{2}$ in Pb--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for the 0--10\% centrality class. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $0.2 < p_{\rm T,e} < 10$ GeV/$c$.

Dielectron pair $p_{\rm T}$ spectrum for $1.2 < m_{\rm ee} < 2.6$ GeV/$c^{2}$ in Pb--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for the 0--10\% centrality class. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $0.2 < p_{\rm T,e} < 10$ GeV/$c$.

Dielectron pair DCA spectrum for $2.6 < m_{\rm ee} < 3.1$ GeV/$c^{2}$ in Pb--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for the 0--10\% centrality class. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $0.4 < p_{\rm T,e} < 10$ GeV/$c$. Dielectrons are measured in $0 < p_{\rm T,ee} < 8$ GeV/$c$.

Dielectron pair DCA spectrum for $1.2 < m_{\rm ee} < 2.6$ GeV/$c^{2}$ in Pb--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for the 0--10\% centrality class. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $0.4 < p_{\rm T,e} < 10$ GeV/$c$. Dielectrons are measured in $0 < p_{\rm T,ee} < 8$ GeV/$c$. Upper limits at 90\% C.L. are also set.

Direct photon fraction as a function of $p_{\rm T}$ in Pb--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for the 0--10\% centrality class.

Direct photon $p_{\rm T}$ spectrum in Pb--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for the 0--10\% centrality class.

Direct photon dN/dy in Pb--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for the 0--10\% centrality class.

Rho distribution of ME+30MeV recoil jet R=0.5 for AuAu 0-15% at sqrt{s_{NN}}=200 GeV from MB event sample.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 9-11 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 11-15 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 15-20 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 9-11 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 11-15 GeV.

Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 15-20 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 9-11 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 11-15 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 15-20 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 9-11 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 11-15 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 15-20 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 9-11 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 11-15 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 15-20 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 9-11 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 11-15 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 15-20 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 9-11 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 11-15 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 9-11 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 11-15 GeV.

Ratio of SE and ME recoil jet distributions for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 9-11 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 11-15 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 15-20 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 9-11 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 11-15 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 15-20 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger ME-subtracted uncorrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 9-11 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 11-15 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 15-20 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 9-11 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 11-15 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 15-20 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger corrected recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 9-11 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 11-15 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 15-20 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 9-11 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 11-15 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 15-20 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 11-15 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 9-11 GeV.

Per trigger corrected recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 11-15 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 9-11 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 11-15 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma E_{T,trig}= 15-20 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 9-11 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 11-15 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and gamma E_{T,trig}= 15-20 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 9-11 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.5 and pi0 E_{T,trig}= 11-15 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 9-11 GeV.

I_AA AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and pi0 E_{T,trig}= 11-15 GeV.

Yield Ratio R=0.2/R=0.5 pp at sqrt{s}=200 GeV pi0 E_{T,trig}= 9-11 GeV.

Yield Ratio R=0.2/R=0.5 pp at sqrt{s}=200 GeV pi0 E_{T,trig}= 11-15 GeV.

Yield Ratio R=0.2/R=0.5 pp at sqrt{s}=200 GeV gamma E_{T,trig}= 15-20 GeV.

Yield Ratio R=0.2/R=0.5 AuAu at sqrt{s_{NN}}=200 GeV pi0 E_{T,trig}= 9-11 GeV.

Yield Ratio R=0.2/R=0.5 AuAu at sqrt{s_{NN}}=200 GeV pi0 E_{T,trig}= 11-15 GeV.

Yield Ratio R=0.2/R=0.5 AuAu at sqrt{s_{NN}}=200 GeV gamma E_{T,trig}= 15-20 GeV.

Figure 2a, full-event

Figure 2b, subevent

Figure 3

Figure 4

I_{AA} of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV for R = 0.5 of pi^{0}+jet with E_{T,trig}= 11-15 GeV.

Yield Ratio R=0.2/R=0.5 of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV of gamma_{dir}+jet with E_{T,trig}= 15-20 GeV.

Yield Ratio R=0.2/R=0.5 of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV of pi^{0}+jet with E_{T,trig}= 11-15 GeV.

Yield Ratio R=0.2/R=0.5 of p+p collisions at sqrt{s_{NN}} = 200 GeV of gamma_{dir}+jet with E_{T,trig}= 15-20 GeV.

Yield Ratio R=0.2/R=0.5 of p+p collisions at sqrt{s_{NN}} = 200 GeV of pi^{0}+jet with E_{T,trig}= 11-15 GeV.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 10-20\% multiplicity class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 20-30\% multiplicity class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 30-40\% multiplicity class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 40-50\% multiplicity class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 50-70\% multiplicity class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 70-100\% multiplicity class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in pp collisions at \sqrt{s}$ = 5.02 TeV for 0-100\% multiplicity class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe Xe collisions at \sqrt{s_{NN}}$ = 5.44 TeV for 0-30\% centrality class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe Xe collisions at \sqrt{s_{NN}}$ = 5.44 TeV for 30-50\% centrality class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe Xe collisions at \sqrt{s_{NN}}$ = 5.44 TeV for 50-70\% centrality class.

$p_{\rm T}$-distributions of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe Xe collisions at \sqrt{s_{NN}}$ = 5.44 TeV for 70-90\% centrality class.

$p_{\rm T}$-integrated yield d$N$/d$y$ of K$^{*}$ (average of particle and anti-particle) meson measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.

Mean $p_{\rm T}$ of K$^{*}$ (average of particle and anti-particle) meson measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.

$p_{\rm T}$-integrated yield d$N$/d$y$ of K$^{*}$ (average of particle and anti-particle) meson measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Mean $p_{\rm T}$ of K$^{*}$ (average of particle and anti-particle) meson measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$-integrated yield ratio of $\rm{K}^{*}$ (average of particleand anti-particle) to K (average of particle and anti-particle) measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.

$p_{\rm T}$-integrated yield ratio of $\rm{K}^{*}$ (average of particleand anti-particle) to K (average of particle and anti-particle) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Lower limit of the hadronic phase lifetime measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.

Lower limit of the hadronic phase lifetime measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Kinetic freeze out temperature measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV.

$p_{\rm T}$ differential ratio $\rm{K}^{*}$ (average of particleand anti-particle) to K (average of particle and anti-particle) measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV for $p_{\rm T}$ range 0.4-2.0 GeV/$\it{c}.

$p_{\rm T}$ differential ratio $\rm{K}^{*}$ (average of particleand anti-particle) to K (average of particle and anti-particle) measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV for $p_{\rm T}$ range 2.0-4.0 GeV/$\it{c}.

$p_{T}$-dependent nuclear modification factor of $\rm{K}^{*}$ (average of particle and anti-particle) meson measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV for 0-30\% centrality.

RAA of $\rm{K}^{*}$ (average of particle and anti-particle) meson as a function of system size measured in Xe-Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV for $p_{\rm T}$ range 4.0-12.0 GeV/$\it{c}.

Sigma(1385)+ pT spectrum in IX V0M mult class

Sigma(1385)+ pT spectrum in X V0M mult class

Sigma(1385)- pT spectrum in I+II+III V0M mult class

Sigma(1385)- pT spectrum in IV+V+VI V0M mult class

Sigma(1385)- pT spectrum in VII+VIII V0M mult class

Sigma(1385)- pT spectrum in IX V0M mult class

Sigma(1385)- pT spectrum in X V0M mult class

Xi(1530)0 pT spectrum in I+II+III V0M mult class

Xi(1530)0 pT spectrum in IV+V+VI V0M mult class

Xi(1530)0 pT spectrum in VII+VIII V0M mult class

Xi(1530)0 pT spectrum in IX V0M mult class

Xi(1530)0 pT spectrum in X V0M mult class

Sigma(1385)+ pT spectrum ratio to MB in I+II+III V0M mult class

Sigma(1385)+ pT spectrum ratio to MB in IV+V+VI V0M mult class

Sigma(1385)+ pT spectrum ratio to MB in VII+VIII V0M mult class

Sigma(1385)+ pT spectrum ratio to MB in IX V0M mult class

Sigma(1385)+ pT spectrum ratio to MB in X V0M mult class

Sigma(1385)- pT spectrum ratio to MB in I+II+III V0M mult class

Sigma(1385)- pT spectrum ratio to MB in IV+V+VI V0M mult class

Sigma(1385)- pT spectrum ratio to MB in VII+VIII V0M mult class

Sigma(1385)- pT spectrum ratio to MB in IX V0M mult class

Sigma(1385)- pT spectrum ratio to MB in X V0M mult class

Xi(1530)0 pT spectrum ratio to MB in I+II+III V0M mult class

Xi(1530)0 pT spectrum ratio to MB in IV+V+VI V0M mult class

Xi(1530)0 pT spectrum ratio to MB in VII+VIII V0M mult class

Xi(1530)0 pT spectrum ratio to MB in IX V0M mult class

Xi(1530)0 pT spectrum ratio to MB in X V0M mult class

pT-integrated yields of sigma1385 in pp collisions as a function of the charged particle multiplicity density at mid-rapidity

meanpT of sigma1385 in pp collisions as a function of the charged particle multiplicity density at mid-rapidity

pT-integrated yields of Xi1530 in pp collisions as a function of the charged particle multiplicity density at mid-rapidity

meanpT of Xi1530 in pp collisions as a function of the charged particle multiplicity density at mid-rapidity

Sigma(1385)}+- pT spectrum ratio to 7 TeV

Xi(1530)0 pT spectrum ratio to 7 TeV

Ratio of the resonance to pion pT-integrated yield as a function of the charged-particle pseudorapidity density for $\Sigma(1385)^{\pm}$

Ratio of the resonance to pion pT-integrated yield as a function of the charged-particle pseudorapidity density for $\Xi(1530)^{0}$

Yield ratio of $\Sigma(1385)^{\pm}$ to $\Lambda$ as a function of the charged-particle pseudorapidity density

Yield ratio of $\Xi(1530)^{0}$ to $\Xi$ as a function of the charged-particle pseudorapidity density

Non-prompt J/$\psi$ fraction as a function of average number of participants in Pb-Pb at 5.02 TeV

Non-prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%

Prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%

Prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%. Global uncertainty 2.3%

Prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 10-30%. Global uncertainty 2.3%

Prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%. Global uncertainty 2.7%

Prompt J/$\psi$ nuclear modification factor as a function of average number of participants in Pb-Pb at 5.02 TeV. Global uncertainty 2.2%

Non-prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%. Global uncertainty 2.3%

Non-prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV,, centrality 10-30%. Global uncertainty 2.3%

Non-prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%. Global uncertainty 2.7%

Non-prompt J/$\psi$ nuclear modification factor as a function of average number of participants in Pb-Pb at 5.02 TeV. Global uncertainty 2.7%

Prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%

Non-prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.2 / 0.4 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.2 / 0.5 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.4 / 0.5 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ for $R=$ 0.2, for various $\mathrm{TT_{sig}}$ selections in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ for $R=$ 0.4, for various $\mathrm{TT_{sig}}$ selections in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.