Abstract

We correct errors that were made in “LADAR resolution improvement using receivers with squeezed-vacuum injection and phase-sensitive amplification,” J. Opt. Soc. Am. B 27, A63–A72 (2010) .

© 2010 Optical Society of America

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References

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  1. Z. Dutton, J. H. Shapiro, and S. Guha, “LADAR resolution improvement using receivers enhanced with squeezed-vacuum injection and phase-sensitive amplification,” J. Opt. Soc. Am. B 27, A63–A72 (2010).
    [CrossRef]

2010

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Equations (14)

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E ̂ ( ρ , t ) = G E ̂ R ( ρ , t ) + G 1 E ̂ R ( ρ , t ) .
T ̃ r ( f ) d ρ Re [ T ( ρ ) ] e i 2 π f ρ .
n r ( f 1 ) n r ( f 2 ) = S n d n d ( f 1 ) 2 [ δ ( f 1 f 2 ) + δ ( f 1 + f 2 ) ] ,
n i ( f 1 ) n i ( f 2 ) = S n d n d ( f 1 ) 2 [ δ ( f 1 f 2 ) δ ( f 1 + f 2 ) ] .
Y d ( f x ) = Y d ( f x ) S n d n d ( f x ) ,
y d ( x ) = d f x Y d ( f x ) e i 2 π f x x = G eff η I T τ p ω λ d x Re [ T ( x ) ] m ( x x ) + n d ( x ) ,
m ( x ) = d f x A ( λ L f x ) S n d n d ( f x ) e i 2 π f x x
n d ( x 1 ) n d ( x 2 ) = δ ( x 1 x 2 ) .
r c = d x ( 4 ( λ L ) 2 π R 2 ) 1 4 m ( x θ 0 L ) + m ( x + θ 0 L ) 2 2 y d ( x ) ,
r = d x ( 4 ( λ L ) 2 π R 2 ) 1 4 m ( x ) 2 y d ( x ) ,
r s = d x ( 4 ( λ L ) 2 π R 2 ) 1 4 m ( x θ 0 L ) m ( x + θ 0 L ) 2 2 y d ( x ) .
Λ 1 = [ 4 G eff η n ¯ C 1 2 + C 0 + C 2 2 ( 2 G eff η n ¯ C 0 + 1 ) C 1 0 2 ( 2 G eff η n ¯ C 0 + 1 ) C 1 ( 2 G eff η n ¯ C 0 + 1 ) C 0 0 0 0 C 0 C 2 ] ,
Λ 2 = [ Λ 0 0 T [ G eff η n ¯ ( C 0 C 2 ) + 1 ] ( C 0 C 2 ) ]
Λ = [ [ G eff η n ¯ ( C 0 + C 2 ) + 1 ] ( C 0 + C 2 ) 2 [ G eff η n ¯ ( C 0 + C 2 ) + 1 ] C 1 2 [ G eff η n ¯ ( C 0 + C 2 ) + 1 ] C 1 2 G eff η n ¯ C 1 2 + C 0 ] .

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