Quantitative phase imaging method based on an analytical nonparaxial partially coherent phase optical transfer function: erratum

Yijun Bao; Thomas K. Gaylord

doi:10.1364/JOSAA.34.001329

Abstract

A correction is given for Eq. (8) in J. Opt. Soc. Am. A 33, 2125 (2016) [CrossRef] .

In our paper [1], Eq. (8) has inconsistent units. The corrected equation is

F (μ, η) = \frac{μ^{2}}{{(μ^{2} + η^{2})}^{3 / 2}} μ_{y, \max}^{'} \sqrt{γ^{2} - μ_{y, \max}^{' 2}} + (\frac{μ^{2}}{{(μ^{2} + η^{2})}^{3 / 2}} γ^{2} - \frac{η^{2}}{2 \sqrt{μ^{2} + η^{2}}}) \arcsin (\frac{μ_{y, \max}^{'}}{γ}) .

The previous error does not affect any of the results or conclusions, since our calculations were based on the correct equation.

REFERENCES

1. Y. Bao and T. K. Gaylord, “Quantitative phase imaging method based on an analytical nonparaxial partially coherent phase optical transfer function,” J. Opt. Soc. Am. A 33, 2125–2136 (2016). [CrossRef]

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Equations (1)

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F (μ, η) = \frac{μ^{2}}{{(μ^{2} + η^{2})}^{3 / 2}} μ_{y, \max}^{'} \sqrt{γ^{2} - μ_{y, \max}^{' 2}} + (\frac{μ^{2}}{{(μ^{2} + η^{2})}^{3 / 2}} γ^{2} - \frac{η^{2}}{2 \sqrt{μ^{2} + η^{2}}}) \arcsin (\frac{μ_{y, \max}^{'}}{γ}) .

Abstract

REFERENCES

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Equations (1)

Journal of the Optical Society of America A