A superparamagnetic iron-oxide nanoparticle (SPION) sitting in an oscillating field H(t) = H0cos(2πft) can lose its magnetic moment's alignment lag as heat through two independent channels, combined as parallel relaxation rates:
1/τ = 1/τ_N + 1/τ_B
Néel (internal spin flips over the anisotropy barrier):
τ_N = τ0 · exp(K_a·V_core / k_B·T), τ0 ≈ 1 ns
Brownian (whole particle physically rotates in the fluid):
τ_B = 3·η·V_hyd / k_B·T
Linear-response heating (Rosensweig, 2002):
P = μ0·π·χ0·H0²·f · (2πfτ) / (1 + (2πfτ)²)
SAR = P / (ρ·φ) [W per gram of magnetic material]
τ_N grows exponentially with core volume, so small cores relax by fast internal spin flips (Néel-dominant, particle body itself never turns). τ_B grows only linearly with hydrodynamic volume and with the fluid's viscosity η, so larger cores or thicker fluids favour whole-particle rotation (Brownian-dominant). The faster of the two channels wins and sets τ_eff — that in turn sets the phase lag δ = atan(2πfτ_eff) between M(t) and H(t), which is exactly the area enclosed by the M–H hysteresis loop (top-right plot) and, multiplied by frequency, the heating power (SAR).
- Core diameter — below ≈9 nm Néel relaxation is essentially instant and dominates; above ≈15 nm the anisotropy barrier makes Néel flips astronomically slow and Brownian rotation takes over.
- Frequency & amplitude — SAR scales with f·H0² near resonance-free linear response, but a real treatment field is capped (H0·f ≲ 5×109 A/m·s) to avoid eddy-current heating of healthy tissue — the clinically used range is roughly 100–500 kHz at 5–30 kA/m.
- Medium — a denser tumor matrix raises η and slows Brownian rotation, which is one reason clinical trials (e.g. NanoTherm®, MagForce) tune core size so Néel relaxation carries most of the heating once particles are embedded in tissue rather than free-flowing in blood.