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The yields for hadrons and even light nuclei measured at midrapidity inrelativistic heavy ion collisions are found to be dictated exclusively by theirthermal Boltzmann factor for a common temperature of approximately 155 MeV. Thereason for the validity of the thermal model description is widely discussed.Here, we offer a new type of argument in its favor.

Why does the thermal model for hadron production in heavy ion collisions work?