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Canonical statistical model analysis of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>p</mml:mi><mml:mtext>โˆ’</mml:mtext><mml:mi>p</mml:mi></mml:mrow></mml:math> , <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>p</mml:mi></mml:math> -Pb, and Pb-Pb collisions at energies available at the CERN Large Hadron Collider

Canonical statistical model analysis of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>p</mml:mi><mml:mtext>โˆ’</mml:mtext><mml:mi>p</mml:mi></mml:mrow></mml:math> , <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>p</mml:mi></mml:math> -Pb, and Pb-Pb collisions at energies available at the CERN Large Hadron Collider

The system-size dependence of hadrochemistry at vanishing baryon density is considered within the canonical statistical model (CSM) with local exact conservation of three conserved charges, allowing for a possibility of strangeness undersaturation, i.e., ${\ensuremath{\gamma}}_{S}\ensuremath{\le}1$. Exact baryon number conservation is found to be even more important than that of strangeness in โ€ฆ