Abstract

In a previous publication [Appl. Opt. 42, 6292 (2003)], information on page 6296 was presented inaccurately. These inaccuracies are corrected here.

© 2004 Optical Society of America

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References

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  1. D. L. Cohen, “Noise-equivalent change in radiance for misalignment noise in a double-sided interferogram,” Appl. Opt. 42, 6292–6304 (2003).
    [CrossRef] [PubMed]

2003 (1)

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Equations (14)

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G 1 σ = E F - i σ χ z ˜ BN χ | for   B 1 = H u σ M σ θ rms Z s 1 σ + Z b σ ,
G 2 σ = E F - i σ χ z ˜ BN χ | for   B 2 = H u σ M σ θ rms Z s 2 σ + Z b σ ,
Z s 1,2 σ = 1 / 4 A d Ω sc η | σ | R | σ | × τ a | σ | τ f | σ | B 1,2 | σ | ,
spectral radiance contaminated by misalignment noise =   H u σ M σ θ rms Z σ + θ 2 L σ   *   σ 2 Z σ - G 1 σ · B 2 σ - B 1 σ G 2 σ - G 1 σ + B 1 σ .
spectral radiance contaminated by misalignment noise = B sc σ + 4 θ 2 L σ   *   σ 2 Z σ A d Ω sc M σ θ rms η | σ | R | σ | τ a | σ | τ f | σ | .
4 θ 2 L σ   *   σ 2 Z σ A d Ω sc M σ θ rms η | σ | R | σ | τ a | σ | τ f | σ |
spectral radiance contaminated by misalignment noise = B sc σ + 4 a   Re ñ θ 2 L σ   *   σ 2 Z σ A d Ω sc M σ θ rms η | σ | R | σ | τ a | σ | τ f | σ | .
misalignment noise = 4 a   Re ñ θ 2 L σ   *   σ 2 Z σ A d Ω sc M σ θ rms η | σ | R | σ | τ a | σ | τ f | σ | .
E ñ θ 2 L σ = - L L   E ñ θ 2 χ exp - 2 π i σ χ d χ = 0 ,
NEdN tilt = 4 a J σ A d Ω sc M σ θ rms η | σ | R | σ | τ a | σ | τ f | σ | ,
J σ = E Re ñ θ 2 L σ   *   σ 2 Z σ 2 .
J σ = 1 4 - S θ 2 σ σ + σ 2 Z σ + σ   + σ - σ 2 Z σ - σ 2 d σ .
Ω sc A d = Ω FOV π r 2 ,
a A d Ω sc = 2 π 2 r 2 Ω FOV   ·   π r 2 = 2 π Ω FOV .

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