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References

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  1. L. Beiser, Appl. Opt. 22, 1264 (1983).
    [CrossRef] [PubMed]
  2. L. Beiser, Appl. Opt. 17, 1161 (1978).
    [CrossRef] [PubMed]
  3. L. Beiser, “Laser Scanning Systems,” in Laser Applications, Vol. 2 (Academic, New York, 1974), pp. 53–159.
  4. W.-H. Lee, Appl. Opt. 16, 1392 (1977).
    [CrossRef] [PubMed]
  5. L. D. Dickson, G. T. Sincerbox, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 163 (1982).
  6. C. J. Kramer, Proc. Soc. Photo-Opt. Instrum. Eng. 390 (1983).
  7. S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
    [CrossRef]

1983

L. Beiser, Appl. Opt. 22, 1264 (1983).
[CrossRef] [PubMed]

C. J. Kramer, Proc. Soc. Photo-Opt. Instrum. Eng. 390 (1983).

1982

L. D. Dickson, G. T. Sincerbox, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 163 (1982).

1980

S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
[CrossRef]

1978

1977

Beiser, L.

L. Beiser, Appl. Opt. 22, 1264 (1983).
[CrossRef] [PubMed]

L. Beiser, Appl. Opt. 17, 1161 (1978).
[CrossRef] [PubMed]

L. Beiser, “Laser Scanning Systems,” in Laser Applications, Vol. 2 (Academic, New York, 1974), pp. 53–159.

Case, S. K.

S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
[CrossRef]

Dickson, L. D.

L. D. Dickson, G. T. Sincerbox, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 163 (1982).

Gerbig, V.

S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
[CrossRef]

Kramer, C. J.

C. J. Kramer, Proc. Soc. Photo-Opt. Instrum. Eng. 390 (1983).

Lee, W.-H.

Sincerbox, G. T.

L. D. Dickson, G. T. Sincerbox, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 163 (1982).

Appl. Opt.

Opt. Eng.

S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
[CrossRef]

Proc. Soc. Photo-Opt. Instrum. Eng.

L. D. Dickson, G. T. Sincerbox, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 163 (1982).

C. J. Kramer, Proc. Soc. Photo-Opt. Instrum. Eng. 390 (1983).

Other

L. Beiser, “Laser Scanning Systems,” in Laser Applications, Vol. 2 (Academic, New York, 1974), pp. 53–159.

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Figures (1)

Fig. 1
Fig. 1

Rotational scanner displaced from the mechanical fulcrum providing (A) unity scan ratio, (B) scan ratio m > 1. The deflecting element is shown underilluminated. When overilluminated, the full aperture delimits the output beam, of which only the principal ray is shown for simplicity.

Equations (15)

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N = θ D a λ ( 1 + r / f ) elements / scan
m = θ / ϕ .
Δ N = Δ θ D a λ ( 1 + r mf ) .
r 0 = r sin ϕ ½ sin θ ½ = r / m ,
m = sin θ ½ sin ϕ ½ ,
N = θ D a λ ( 1 + r m f ) .
m = m ( 1 θ ½ 2 / 6 1 ϕ ½ 2 / 6 )
N = θ D a λ [ 1 + r mf ( 1 ϕ ½ 2 / 6 1 θ ½ 2 / 6 ) ] .
1 θ ½ 2 / 6 m 2 1 θ ½ 2 / 6 < 1 + ɛ
θ ½ 2 < 6 ɛ 1 + ɛ 1 / m 2 .
when m = 3 , θ ½ < 0.61 = 35 ° when m = 2 , θ ½ < 0.84 = 48 ° } ,
N = θ D a λ [ 1 + r mf ( 1 + ɛ ) ] ,
( 1 + r mf ) + ( r mf ɛ ) ,
N = θ D a λ ( 1 + r mf ) .
N = ϕ D a λ ( m + r f ) ,

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