Hourglass of Entropy: How Cold Atoms Keep Time ✛

Original: "Testing the problem of time with cold atoms"
· Giovanni Barontini
arXiv:2509.07745 · 2025-09-09 · CC BY 4.0 · 2 min
Physicists built an internal clock from the flow of entropy between parts of an isolated system and tested it on a Bose–Einstein condensate.

In the lab, time usually ticks on the wall: hands, digits, a frequency standard. But for the Universe, there are no external clocks. The Wheeler–DeWitt equation, the main law of quantum gravity, contains no time at all, and all fundamental theories lack an inbuilt arrow of time. One reliable asymmetry remains: the growth of entropy according to the second law of thermodynamics. Entropy is the sand in an hourglass, trickling from one bulb to the other, and its flow sets the pace of time.

Physicists at the Max Planck Institute of Quantum Optics built such a clock from a Bose–Einstein condensate: an ultracold cloud of about 24,000 rubidium-87 atoms in a single quantum state. A thin laser barrier split the cloud into two sectors: a dark, unobservable one and a bright one watched by cameras. For 120 ms, every 2 ms they recorded the density profile: atom number, center-of-mass position, and entropy of the bright sector. Entropic time was defined as the integral of entropy change along the trajectory of a scalar-field analog, which guarantees monotonicity as long as entropy and field change in the same direction.

When the barrier height is near its maximum, entropic time in the bright sector comes to a complete halt, even though 120 ms have passed on the lab clock: the system has reached an analog of heat death.

The result resembles a real hourglass: as long as sand is falling, time flows; when all sand has settled, time freezes. Entropic time grew almost monotonically for all barrier heights, with the rate set by the entropy flow: faster when there is exchange, zero when there is none. The total entropy of the mini-universe remained constant within uncertainty. Data ordered by entropic time reproduced the expansion and contraction cycles of the bright sector, and at high barrier the system approached “heat death,” where time stops. The derived Schrödinger equation with entropic time numerically reproduced the measured evolution of the condensate width with excellent agreement.

This is the first experiment where time is not imposed from outside by a lab chronometer but built from entropy exchange between subsystems. Previously, relational constructions of time were only discussed theoretically; now there is a controlled testbed. The cold-atom platform allows varying the Hamiltonian and testing different scenarios: choice of internal clock, behavior near singularities, reversibility via Loschmidt echo, analog black holes, and Vilenkin-type tunneling. The entropy hourglass can be flipped and restarted, or the shape of the bulbs can be changed to see how time flows in other mini-universes.

At a barrier height close to maximum, entropic time in the bright sector completely stops, even though 120 ms have passed on the laboratory clock: the system has reached an analog of heat death.

\tau(\lambda) = \frac{\sigma}{k_B} \int_{\lambda} \frac{dS}{d\phi} |d\phi|
Entropic time τ is proportional to the integral of the entropy change dS along the field trajectory φ, where σ is an arbitrary time unit and kB is the Boltzmann constant.
i\hbar \partial_\tau \psi(\tau, a) = \Phi(\tau)\psi(\tau, a) + \Lambda(\tau) H_{\text{geom}}\psi(\tau, a)
The evolution of the wave function ψ with respect to entropic time τ is determined by a global phase Φ and an entropy pump Λ multiplying the geometric Hamiltonian H_geom.
Scientists
Ludwig BoltzmannRudolf ClausiusJacob BekensteinWilhelm WienCharles BennettJohn von Neumann
Concepts
time evolution schrodingers cat Schrödinger equation Bose-Einstein condensate arrow of time laboratory experiment entropy driven self assembly Boltzmann equation schrodinger cat state observation atomistic simulation retrospective forecast atom trap Wheeler-DeWitt equation Gross–Pitaevskii equation ergodic theorem second law of thermodynamics entropy quantum dynamics quantum clock