How a quantum proton becomes a hot liquid express

Original: "Hydrodynamic Initial Conditions in Small Systems from Proton Phase-Space Entropy"
arXiv:2604.12691 · 2026-04-14 · CC BY 4.0 · 1 min
The quantum state of a proton resembles a mosaic, from which hydrodynamics assembles the big picture.

📄 Showing the "Simple" version — "Advanced" is not ready yet. Add it to favorites to help prioritize it.

At the Large Hadron Collider, not only nuclei but also individual protons collide. Even in such small systems, collective behavior resembling the flow of a liquid is observed. But the proton is a quantum object; its state is described by a wave function, not by temperature and pressure. How does the classical picture emerge from the quantum 'mosaic'?

Hydrodynamics requires initial conditions set by the entropy flux — a measure of disorder. The quantum state of a proton is a projection of a pure state, whose entropy is zero.

Entropy is a measure of uncertainty: a pure state has zero entropy, like a perfectly assembled puzzle where every piece is in its place.

The authors propose using the Weyl entropy, which arises from coarse-graining phase space — averaging over small cells. Such entropy is always positive and provides a semiclassical measure of the number of accessible microstates at a given resolution. It is precisely this entropy that allows linking the quantum wave function of the proton to the classical initial conditions for hydrodynamics.

This is akin to translating a mosaic into a painting: if you look at the mosaic too closely, you see individual pieces (quantum states), but step back, and they merge into a unified canvas (hydrodynamic description). The Weyl entropy is the tool that measures the degree of this merging.

Original abstract

as written by the authors arXiv:2604.12691

The experimental observation of collective behaviour in proton-proton and proton-nucleus collisions poses a fundamental theoretical question regarding the proper characterization of the initial state underlying hydrodynamic evolution. While relativistic hydrodynamics requires an initial condition (IC) characterized by an entropy current, corresponding to a maximally mixed state, the microscopic description of the proton is based on inherently quantum objects, that are projections of pure states. We show that the appropriate matching between proton wave function and classical hydrodynamics emerges from the coarse-graining of its phase-space distribution quantified by the Wehrl-like entropy. This entropy provides a semi-classical, positive-definite measure of the density of accessible microstates at a given resolution scale, and therefore constitutes the appropriate quantity to characterize entropy deposition in small collision systems.

The Weyl entropy is named after the physicist who introduced the concept of coherent states — peculiar 'bridges' between the quantum and classical worlds.

Scientists
Ludwig BoltzmannRudolf ClausiusJacob BekensteinStephen HawkingJames Clerk MaxwellEdward Witten
Concepts
hydrodynamics proton dynamics initial conditions equation of state function boltzmann entropy electron liquid liquid water proton structure third law of thermodynamics principle of maximum entropy enthalpy state hydrogen protoplanetary disk chemistry water phase behavior hydrogen atmosphere bohr radius thermodynamic stability Navier-Stokes equations deuterium