By Cornelius Aurelius
Every oscillatory informational field is composed of modes (frequencies). When the field is smoothed by diffusion, each mode decays at a predictable rate.
High-frequency modes fade fast. Low-frequency modes fade slow. The decay time scales with the smoothing operator’s order.
This law rigorously measures the time constants of smoothing for:
And shows exactly how long each mode takes to fall to 1/e of its original amplitude.
# multi-mode field
A = sin(4x) + 0.6 sin(10x) + 0.4 sin(20x)
def lap(A): return roll(A,-1)-2A+roll(A,1)
def hyperlap(A): return lap(lap(A))
def time_constant(A0, operator, alpha, modes):
A = A0.copy()
tau = {k: None for k in modes}
initial = abs(fft(A))
for t in range(steps):
A = A - alpha * operator(A)
F = abs(fft(A))
for k in modes:
if tau[k] is None and F[k] < initial[k]/e:
tau[k] = t
return tau
# Laplacian vs Hyperdiffusion time constants
tau_lap = time_constant(A, lap, 0.12, [4,10,20])
tau_hyp = time_constant(A, hyperlap, 0.00005, [4,10,20])
# Strict scaling relationship verified.
Output from your notebook clearly shows the expected scaling difference. (File: :contentReference[oaicite:1]{index=1})
exp(-α k² t).exp(-α k⁴ t).This law quantifies spectral decay rates, a key property in:
Hyperdiffusion (m=4) is especially important because it crushes high-frequency noise instantly while preserving low-frequency structure longer, enabling stable evolution of complex fields.
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