Thermal EM Radiation from Deconfined Nuclear Matter

Based on Jean-François Paquet (Vanderbilt) / McGill Physics seminar — dNγ/d²pT dy & effective temperature

Why does the spectrum look "hotter" when the plasma expands?

Heat wave analogy: A heat wave (like the Doppler shift) can make two things go up together—e.g. ice cream sales and drowning rates—so they appear correlated. The real cause is the heat wave. Here, transverse expansion is the real cause: it blue-shifts the photons, so the spectrum looks like it has a higher temperature than the true local one. That "measured heat" is the effective temperature Teff.

Takeaway: The "motion blur" of the collision makes the data look more energetic. Toggle "Local" vs "Effective" below to see how expansion stretches the spectrum.

250
0.00

Photon energy spectrum (dNγ/d²pT dy) — inverse slope → Teff

Transverse expansion uμ (schematic)

Physics takeaway

ConceptNon-specialistExpert
Doppler shift "Motion blur" that makes data look more energetic Blue-shift of thermal distribution due to uμ
Effective temperature "Measured heat" including the explosion's speed Teff ≈ Tlocal √[(1+v)/(1−v)]
Energy spectrum "Light signature" of the exploding nuclear matter dNγ/d²pT dy vs pT (GeV)

Validation (causal correlation)

Expansion → spectral hardening is enforced by hydrodynamic causality. No spurious relationships (e.g. Redskins Rule / stork statistics).

Causal check: v → Teff consistent