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  1. J. Connes, Rev. Opt. 40, 45, 116, 171, 231 (1961). See also J. Connes, “Spectroscopic Studies Using Fourier Transformations”, NAVWEPS Rept. 8099, NOTS TP 3157, U.S. Naval Ordnance, Test Station, China Lake, California (January1963).
  2. E. E. Bell, Infrared Phys. 6, 57 (1966).
    [CrossRef]
  3. J. M. Dowling, J. Opt. Soc. Am. 54, 663 (1964).
    [CrossRef]
  4. A. Filler, J. Opt. Soc. Am. 54, 762 (1964).
    [CrossRef]
  5. R. T. Hall, D. Vrabec, J. M. Dowling, Appl. Opt. 5, 1147 (1966).
    [CrossRef] [PubMed]
  6. T. Williams, J. Opt. Soc. Am. 50, 1159 (1960).
    [CrossRef]
  7. E. V. Loewenstein, J. Opt. Soc. Am. 50, 1163 (1960).
    [CrossRef]

1966

1964

1961

J. Connes, Rev. Opt. 40, 45, 116, 171, 231 (1961). See also J. Connes, “Spectroscopic Studies Using Fourier Transformations”, NAVWEPS Rept. 8099, NOTS TP 3157, U.S. Naval Ordnance, Test Station, China Lake, California (January1963).

1960

Bell, E. E.

E. E. Bell, Infrared Phys. 6, 57 (1966).
[CrossRef]

Connes, J.

J. Connes, Rev. Opt. 40, 45, 116, 171, 231 (1961). See also J. Connes, “Spectroscopic Studies Using Fourier Transformations”, NAVWEPS Rept. 8099, NOTS TP 3157, U.S. Naval Ordnance, Test Station, China Lake, California (January1963).

Dowling, J. M.

Filler, A.

Hall, R. T.

Loewenstein, E. V.

Vrabec, D.

Williams, T.

Appl. Opt.

Infrared Phys.

E. E. Bell, Infrared Phys. 6, 57 (1966).
[CrossRef]

J. Opt. Soc. Am.

Rev. Opt.

J. Connes, Rev. Opt. 40, 45, 116, 171, 231 (1961). See also J. Connes, “Spectroscopic Studies Using Fourier Transformations”, NAVWEPS Rept. 8099, NOTS TP 3157, U.S. Naval Ordnance, Test Station, China Lake, California (January1963).

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Figures (2)

Fig. 1
Fig. 1

I(ν) solid curve and IL(ν) for L = 0.200 −1, dashed curve. The inset shows I(ν) − IL(ν) at the same scale.

Fig. 2
Fig. 2

Spectrum signal-to-noise curves (A, B, and C) and maximum intensity to side lobe intensity curve (D). See text for explanation.

Equations (5)

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N S = ( L / 4 ν c ) 1 2 N I = ( L Δ x / 2 ) 1 2 N I ,
I L ( ν ) = k I ( ν ) ( 1 - exp ( - 2 π L ) { cos 2 π L ( ν - ν 0 ) - [ ( ν - ν 0 ) / ] sin 2 π L ( ν - ν 0 ) } ) ,
I L ( v 0 ) = k I ( v 0 ) ( 1 - exp ( - 2 π L ) ] ,
S S / N S = k [ 1 - exp ( - 2 π L ( 2 π L ) 1 2 ] ,
I F [ I ( ν 2 ) - I L ( ν 2 ) ] - [ I ( ν 1 ) - I L ( ν 1 ) ] .

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