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References

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  1. R. W. Ditchburn, in Light (Interscience, New York, 1963), pp. 437–438, 432–433.
  2. A. Sommerfeld, in Optics (Academic, New York, 1964), pp. 72–75.
  3. H. V. Soule, in Electro-Optical Photography at Low Illumination Levels (Wiley, New York, 1968), p. 185.

Ditchburn, R. W.

R. W. Ditchburn, in Light (Interscience, New York, 1963), pp. 437–438, 432–433.

Sommerfeld, A.

A. Sommerfeld, in Optics (Academic, New York, 1964), pp. 72–75.

Soule, H. V.

H. V. Soule, in Electro-Optical Photography at Low Illumination Levels (Wiley, New York, 1968), p. 185.

Other (3)

R. W. Ditchburn, in Light (Interscience, New York, 1963), pp. 437–438, 432–433.

A. Sommerfeld, in Optics (Academic, New York, 1964), pp. 72–75.

H. V. Soule, in Electro-Optical Photography at Low Illumination Levels (Wiley, New York, 1968), p. 185.

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Figures (1)

Fig. 1
Fig. 1

Geometry of wide-angle laser beam scanner.

Equations (12)

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ν D = ( 2 Ω / λ ¯ ) e
Δ ν D = ( 2 Ω / λ ¯ ) d 0 ,
θ s = 4 cos - 1 ( e / R 0 ) ,
ν = ν ¯ + ν D ,
ν D = ( 2 / λ ¯ ) v
v = v cos θ ,
v = Ω r .
ν D = ( 2 Ω / λ ¯ ) e = ( 2 v max / λ ¯ ) ( e / R 0 ) ,
Δ ν D = ( 2 Ω / λ ¯ ) d 0 = ( 2 v max / λ ¯ ) ( d 0 / R 0 ) .
Q = Δ ν D / ν D = d 0 / e .
e / ν D = d 0 / Δ ν D 2 × 10 - 7 .
θ s = 4 cos - 1 ( e / R 0 ) .

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