Distribution of the $\left(\mathrm{d}E/\mathrm{d}x-\langle\mathrm{d}E/\mathrm{d}x\rangle_{\rm ^{3}He}\right)/\sigma^{\rm ^{3}He}_{\mathrm{d}E/\mathrm{d}x}$ method used to extract the signal of $^3\overline{\rm{He}}$ (left), and distribution of $(\Delta t - \Delta t_{\rm d}^{\rm exp})/\sigma_{\rm TOF}$ used to extract the signal of $\overline{\rm{d}}$ (right). The regions highlighted in green represent the regions of the signal integration, different for the two signal extraction methods.

The $\Delta M$ distribution (left) and the extracted $v_2$ (right) of deuteron candidates as a function of $\Delta M$ for $0.8 $ $< p_{\rm T}$ $< 1.6$ GeV/$c$ in the centrality interval 0$-$20$\%$ in Xe$-$Xe collisions. The statistical uncertainties on the data points are represented by bars. The measurement is carried out at midrapidity, i.e., $\left|y\right|< 0.5$.

Transverse-momentum differential yields of the average of deuterons and antideuterons in different centrality classes (left panel), and of the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ (right panel) in the centrality class (0$-$90$\%$). Dotted lines show the Blast-Wave individual fit to the $p_{\rm T}$ spectra. Statistical and systematic uncertainties are shown as vertical bars and boxes, respectively.

Deuteron-to-proton (top panel) and $^3$He-to-proton (bottom panel) yield ratios as a function of the average charged-particle multiplicity density. All yields are measured at midrapidity, i.e., $\left|y\right|< $ 0.5 for pp, Xe$-$Xe and Pb$-$Pb collisions, and $-1< \left|y\right|< 0$ for p$-$Pb collisions. Statistical uncertainties are shown as vertical lines, whereas systematic ones are shown as boxes. The coalescence predictions are shown as bands, whose width represents the model uncertainty. The black and green lines correspond to the expectations of two different hypotheses of the CSM.

Deuteron-to-pion (top panel), and $^3$He-to-pion (bottom panel) yield ratios as a function of the charged-particle multiplicity density. All yields are measured at midrapidity, i.e., $\left|y\right|< $ 0.5 for pp, Xe$-$Xe and Pb$-$Pb collisions, and $-1< \left|y\right|< 0$ for p$-$Pb collisions. Lines represent statistical uncertainties, whereas boxes show systematic ones. The solid lines correspond to the expectations of two implementations of the CSM, see text for details.

Coalescence parameters $B_2$ (left panel) and $B_3$ (right panel) as a function of $p_{\mathrm T}$/$A$, measured for deuterons and $^3$He, respectively. Statistical uncertainties are represented as vertical lines whereas boxes represent the systematic ones.

(Anti)deuteron $v_2$ measured at $|y| < 0.5$ in the centrality classes 0$-$20$\%$ (left) and 20$-$40$\%$ (right) in comparison with the Blast-Wave predictions obtained from simultaneous fits of the $p_{\rm T}$ spectra and $v_2$ of pions, kaons, and protons. Statistical and systematic uncertainties are represented by bars and boxes, respectively.

(Anti)deuteron $v_2$ measured in the centrality classes 0$-$20$\%$ (left) and 20$-$40$\%$ (right) in comparison with the coalescence predictions based on the mass-number scaling. Statistical and systematic uncertainties are shown as bars and boxes, respectively. The flow of deuterons is measured at midrapidity, i.e., $\left|y\right|< $ 0.5.

Thermal fit to the measured hadron yields in Xe$-$Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV, performed with two different implementations of the statistical hadronization model, namely the Thermal-FIST  and the GSI-Heidelberg model . The yields shown for each given species are the average of the particle and antiparticle yields. In the bottom panel, the ratios of data to the model calculations are shown.