Noise-whitened angle between spectral signal and nuisance shapes

ID: noise-whitened-angle-between-spectral-signal-and-nuisance-shapes

The noise-whitened angle between spectral signal and nuisance shapes measures their separation in units of measurement noise rather than raw plotting units. For nonzero shapes and a positive-definite covariance , choose a square whitening transformation with . The angle is
It is the ordinary Euclidean angle after whitening. Both parallel and antiparallel shapes are indistinguishable up to an unknown nuisance amplitude; the precision penalty depends on , as in noise penalty from nearly parallel signal and reference shapes.
For an original example, take raw shapes , and . The plotted shapes are orthogonal, but whitening gives and . Thus and . The second channel, which separates their signs, is noisy. Rejecting the nuisance multiplies the optimum variance by , or standard uncertainty by .
The invariance of noise-whitened spectral angles to the whitening factor follows from . Different valid square whitening factors can rotate the whitened coordinates without changing the angle. Likewise an invertible change of measurement units transforms both shapes and covariance, leaving the inverse-covariance expression unchanged. Rescaling only the displayed curves while leaving their noise model fixed is a different operation.
The covariance must describe the actual measured channels and shared errors, using the full propagation rule.[ref] If is singular, first restrict to its physically allowed range; an unrestricted inverse whitening factor does not exist.
The primary stimulated-Raman experiment described systematic spectral noise and subtraction of a pure-solvent reference.[ref] The angle above assesses which desired patterns remain distinguishable after such nuisance rejection under a stated covariance. It does not establish that an estimated reference shape or noise model is itself accurate.

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