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SUMMARY:Particle multiplicity fluctuations of quantum origin and   high-mu
 ltiplicity pp collision events
DTSTART;VALUE=DATE-TIME:20260923T075000Z
DTEND;VALUE=DATE-TIME:20260923T081000Z
DTSTAMP;VALUE=DATE-TIME:20260914T053145Z
UID:indico-contribution-523@indico.bitp.kiev.ua
DESCRIPTION:Speakers: Sergiy Akkelin (Bogolyubov Institute for Theoretical
  Physics of the National Academy of Sciences of Ukraine)\nThe multiplicity
  dependence of the two-particle Bose-Einstein momentum correlation radii i
 n pp collisions at the LHC has been measured at a fixed energy of collisio
 ns. One notable feature of these measurements is that the effective system
 ’s volume\, when extracted from the correlation radius parameters\, appe
 ars to scale nearly linearly with charged-particle multiplicity [1-3]\, ex
 cept for low multiplicities where initial state effects dominate and\, qui
 te unexpectedly\, except for very high multiplicities where\, at variance 
 with the expected behavior for emission from hydrodynamically expanding sy
 stems\, one sees systematic deviations from such a scaling behavior. That 
 is\, the striking feature of the data is that the correlation radius param
 eters become approximately independent of the particle multiplicity in the
  limit of very high multiplicities [1\,2]. The question naturally arises: 
 How can this controversy with hydrodynamics be resolved?\nIn Ref. [4]\, we
  argue that quantum-origin multiplicity fluctuations dominate the fluctuat
 ions in particle multiplicity in high-multiplicity pp collision events at 
 a fixed LHC energy. The quantum-to-classical transition of multiplicity fl
 uctuations happens when the interference term between the corresponding st
 ates becomes negligible. Until this happens\, superposition cannot be inte
 rpreted as a classical ensemble of its component states. To connect quantu
 m fluctuations of particle multiplicity to event-by-event multiplicity flu
 ctuations\, we introduce the statistical ensemble of the multiplicity fluc
 tuations of particles after the system’s freeze-out. We utilize the maxi
 mum entropy prescription to determine a quantum state at kinetic freeze-ou
 t and derive expressions for multiplicity-selected particle momentum spect
 ra and correlation functions by applying a fixed particle-number constrain
 t to this state. Then\, we study how multiplicity fluctuations at high mul
 tiplicities impact the multiplicity-selected particle momentum spectra and
  correlation functions. In particular\, we find that the effective system
 ’s volume should become approximately independent of the particle multip
 licity in the limit of very high multiplicities in multiplicity-selected c
 ollision events.\n\n\nReferences\n\n[1] ATLAS Collaboration\, Eur. Phys. J
 . C 75\, 466 (2015)\, https://doi.org/10.1140/epjc/s10052-015-3644-x\; 82\
 , 608 (2022)\,  https://doi.org/10.1140/epjc/s10052-022-10472-0 .\n[2] A. 
 M. Sirunyan et al. (CMS Collaboration)\, Phys. Rev. C 97\, 064912 (2018)\,
  https://doi.org/10.1103/PhysRevC.97.064912 \;  J. High Energy Phys. 03 (2
 020) 014\, https://doi.org/10.1007/JHEP03(2020)014 .\n[3] S. Acharya et al
 . (ALICE Collaboration)\, Phys. Rev. C 109\, 024915 (2024)\, https://doi.o
 rg/10.1103/PhysRevC.109.024915 .\n[4] S.V. Akkelin\, Phys. Rev. D 112\, 11
 6007 (2025)\,  https://doi.org/10.1103/k7mv-57bt .\n\nhttps://indico.bitp.
 kiev.ua/event/18/contributions/523/
LOCATION:Bogolyubov Institute for Theoretical Physics Conference Hall
URL:https://indico.bitp.kiev.ua/event/18/contributions/523/
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