Jan 14 – 15, 2026
Europe/Kyiv timezone

The Rating Quality for Theoretical Description of Experimental Data

Jan 14, 2026, 4:30 PM
30m

Speakers

Sergey Omelchenko (Institute for Nuclear Research NAS of Ukraine)Dr Valery Pugatch (Institute for Nuclear Research NAS of Ukraine)

Description

The Rating Quality for Theoretical Description of Experimental Data

S. O. Omelchenko, V. M. Pugatch
Institute for Nuclear Research, National Academy of Sciences of Ukraine, Kyiv, Ukraine

$1.$ $Introduction.$ A new multi-parameter score-rating methodology for assessing the quality of theoretical description of experimental data in heavy-ion physics [1-11] is proposed. The approach overcomes the limitations of the traditional single-value criterion $\chi^2/\mathrm{ndf}$, which provides only an integral measure of agreement between theory and experiment.
The methodology is based on dividing the phase space into seven physically motivated kinematic regions of transverse momentum $p_T$ distributions and particle ratios, corresponding to different underlying physical regimes. For each region, the quality of agreement is quantified by a score $Q_i \in [10;1000]$ defined on a scale, ranging from very poor to excellent agreement.
A comprehensive rating $R$ is constructed through a systematic procedure that includes region definition, weighting according to physical significance, aggregation of local scores, uncertainty estimation, stability checks, and visualization. This framework enables a transparent and comparative assessment of theoretical models, revealing their region-specific performance and complementarity.
$2.$ $Methodology.$ The phase space is divided into seven kinematic regions corresponding to different physical regimes: thermal spectra ($p_T < 0.8$ GeV/$c$), radial flow, hard processes relevant to QGP formation ($2.5$--$4.0$ GeV/$c$), medium-energy jets, high-energy jets with quenching, and the perturbative QCD regime ($p_T > 10$ GeV/$c$).
For each region, the local statistic is defined as:
$$R_i = \frac{\chi_i^2}{\nu_i}, \qquad \nu_i = N_i - k$$ where $N_i$ is the number of data points and $k$ is the number of model parameters. $3.$ $Score$ $Assignment.$ Based on the value of $R_i$, a quality score $Q_i$ is assigned using a scale, ranging from $Q_i = 1000$ for excellent agreement to $Q_i = 10$ for very poor agreement. $4.$ $Weighting$ $and$ $Aggregation.$ Weight coefficients reflect the physical significance of different kinematic regions. The aggregated quality measures include weighted averaging, geometric mean, minimum score, and dispersion penalties. $5.$ $Results$ $and$ $Discussion.$ The methodology was applied to LHC data for $K^0_S$ mesons and $\Lambda$ hyperons in $p$-$Pb$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV. The analysis demonstrates model complementarity and sensitivity to nuclear shadowing effects. $6.$ $Conclusions.$ The proposed score-rating methodology provides a transparent and robust framework for ranking theoretical models in heavy-ion physics and is well suited for systematic studies of LHC Run 3 data and beyond. $References$
[1] ALICE Collaboration, Phys.Lett.B 846 (2024) 137875.
[2] U.Heinz, R.Snellings, Ann.Rev.Nucl.Part.Sci. 63 (2013) 123.
[3] J.E. Bernhard et al., Phys.Rev.C 103 (2021) 054904.
[4] K.Werner et al., Phys.Rev.C 85 (2013) 064907.
[5] Z.W.Lin et al., Phys.Rev.C 72 (2005) 064901.
[6] JET Collaboration, J.Phys.G 47 (2020) 065101.
[7] CMS Collaboration, JHEP 04 (2017) 039.
[8] T.Sjöstrand et al., Comput.Phys.Commun. 191 (2015) 159.
[9] X.N.Wang, M.Gyulassy, Phys.Rev.D 44 (1991) 3501.
[10] J.S.Moreland et al., Phys.Rev.C 92 (2015) 011901.
[11] W.Cassing, E.L.Bratkovskaya, Nucl.Phys.A 831 (2009) 215.

Primary author

Sergey Omelchenko (Institute for Nuclear Research NAS of Ukraine)

Co-author

Dr Valery Pugatch (Institute for Nuclear Research NAS of Ukraine)

Presentation materials