Directional derivative of a clipped logarithmic acquisition time

ID: directional-derivative-of-a-clipped-logarithmic-acquisition-time

The directional derivative of a clipped logarithmic acquisition time describes the first-order recording extension when several envelope parameters change together at the acquisition threshold. For positive , write
The logarithmic tail-duration change at the zero-extension boundary article treats a fixed decay time and logarithmic input coordinate. Here consider a boundary point and an additive parameter direction .
The one-sided directional derivative uses positive step sizes:
The logarithmic chain rule gives the expression inside the maximum. Differentiating the prefactor contributes zero at the boundary because the clipped logarithm there is zero.
For an original example, let , and . Increase amplitude in direction while decreasing decay time in direction , with . The net fractional direction is , so per unit step. Reversing the direction gives derivative zero, not .
The derivative is positively homogeneous in the direction but is not linear, so no single gradient represents all threshold-crossing perturbations. Above threshold the usual smooth derivative applies; strictly below threshold all sufficiently small changes leave the extension zero. Gaussian input uncertainty at a clipped acquisition-time threshold can consequently produce a mass of outcomes exactly at zero rather than a symmetric distribution around a nominal duration. The directional calculation alone does not assign a confidence level.
This is a conditional optical-envelope calculation. Separating optical power from the receiver's electrical response remains necessary before its parameters describe missed light. NIST independently characterized the detector/cable/oscilloscope response in its pulse calibration procedure.[ref] A derivative can describe parameter sensitivity accurately while the envelope itself still needs experimental justification.

New to topics? Read the docs here!