Temperature as a Continuous Stream of Photons ✎

Original: "Temperature as a Dynamically Maintained Steady State: Photonic Mechanisms, Maintenance Cost, and the Limits of the Infinite-Reservoir Idealization"
· David Vaknin
arXiv:2601.22247 · 2026-01-29 · arXiv non-exclusive · independent analysis · 2 min
Thermal equilibrium is not frozen stillness but a continuous exchange of photons, and that exchange costs energy.

Temperature seems like something frozen: a substance has a temperature, and that's that. But look closer, and thermal equilibrium resembles a waterfall that appears motionless from the side even though it consists of a continuous stream of water. In the same way, any body at finite energy constantly exchanges photons with its surroundings. A photon is a quantum of electromagnetic radiation, and spontaneous emission is the spontaneous release of a photon by an excited system. Without a compensating influx of energy, the body cools, and equilibrium collapses.

The average photon energy in thermal radiation at room temperature (about 300 K) is roughly 0.07 eV, which corresponds to the infrared range. That is exactly why thermal cameras see in the IR spectrum.

Temperature used to be described as a static characteristic of a system in equilibrium, without asking what physically sustains that equilibrium. Now it is clear: thermal equilibrium is a dynamically maintained state in which a constant temperature is ensured by a continuous exchange of photons with the surroundings. The author has gathered known facts (spontaneous emission, the Stefan-Boltzmann law, the H-theorem) and shown that together they yield a single mechanism for maintaining temperature. The Maxwell distribution (the distribution of molecular speeds in a gas) is shaped by mechanical collisions, but the energy scale is set precisely by the boundary exchange.

An infinite thermal reservoir is not a physical object but the limit of a hierarchy of finite reservoirs, each of which is maintained by exchange on a larger scale.

Understanding the dynamic nature of temperature matters when designing cryostats, analyzing the thermal balance of planets and stars, and correctly interpreting experiments with small systems. The waterfall we see as a motionless wall of water actually consists of myriads of droplets continuously falling down. Temperature is likewise not a property of rest but a continuous flow of energy that has to be maintained.

The average photon energy in thermal radiation at room temperature (about 300 K) is roughly 0.07 eV, which corresponds to the infrared range. That is exactly why thermal cameras see in the IR spectrum.

\langle h\nu \rangle = \frac{\pi^4}{30\zeta(3)} k_B T \approx 2.701\, k_B T
The ratio of Bose-Einstein integrals gives the coefficient 2.701
u(\nu) = \frac{8\pi h\nu^3}{c^3} \frac{1}{e^{h\nu/k_B T} - 1}
Quantum distribution of thermal radiation energy
Scientists
Cecilia Payne-GaposchkinRalph FowlerMax PlanckEmile Clapeyron
Concepts
temperatureSaha equationzeroth law of thermodynamicsthird law of thermodynamicsideal gas lawMeissner effectCarnot's theorem