Radial cutoff diagnostics#

The cutoff radius is designed to answer a practical question:

Beyond what radius is a retained harmonic negligible according to both its integrated power and its pointwise radial amplitude?

It is not used to truncate the PETAL2D reconstruction.

Power-support radius#

For a retained harmonic define

\[ P_m(r)=\int_0^r|\rho_m(r')|^2r'\,dr'. \]

Given radial_power_tail_fraction = ε_P, the power-support radius is the smallest radius satisfying

\[ P_m(r_{m}^{\rm power})\ge(1-\varepsilon_P)P_m(R). \]

This controls integrated omitted power.

Amplitude-support radius#

Integrated power alone can place a radius inside a visually or physically meaningful low-amplitude outer lobe. Therefore PETAL2D also uses radial_relative_amplitude_threshold = ε_A and defines

\[ r_m^{\rm amp}=\sup\left\{r:\;|\rho_m(r)|\ge \varepsilon_A\max_{r'}|\rho_m(r')|\right\}. \]

The outermost crossing is used so oscillatory profiles cannot discard a later significant lobe.

Final cutoff radius#

\[ r_{m}^{\rm cutoff}=\max(r_m^{\rm power},r_m^{\rm amp}). \]

Consequently, beyond the cutoff radius both conditions hold: the remaining integrated power is sufficiently small and no sampled outer region exceeds the chosen relative amplitude threshold.

The defaults are

radial_power_tail_fraction = 1e-6
radial_relative_amplitude_threshold = 1e-3

corresponding to 99.9999% enclosed radial mode power and a 0.1% relative amplitude threshold.

Important

cutoff_radius is a radial-information diagnostic, not a claim that the field becomes exactly zero there. If a downstream calculation needs a finite radial domain, choosing a domain at or beyond the cutoff ensures that both configured tail criteria have been met. If the field itself must be forced to zero, use a smooth taper/window outside the physically relevant region rather than multiplying by a discontinuous hard step. A sharp truncation can introduce artificial kinks and high-frequency content.

Why two criteria are necessary#

For a normalized Gaussian-like tail, a radius containing 99% of the integrated power can still occur where the pointwise amplitude is around ten percent of its peak. Increasing the power percentage alone is not a universal solution because the relation between integrated weight and visible amplitude depends on radial shape. The combined criterion is explicitly designed to protect both notions of support.