Abstract

First and second approximations to the change in variance of the line profile arising from dispersion and other physical aberrations are obtained by means of series expansions. To a first approximation the increase in variance (in 2θ) due to dispersion is 4μ3 tan4θ/λ3, and the change in variance resulting from other physical aberrations is 4R1μ3 tan2θ/λ2, where μ3 is the third moment of the line profile about its centroid and R1 is the derivative with respect to λ of the logarithm of the physical factor in question. In the first approximation the effects of the angular-velocity factor, the polarization factor, the trigonometric factor specific to the instrument, and such response variations as absorption in the filter and the quantum-counting efficiency are additive. In the second approximation cross terms appear.

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