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References

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  1. L. Beiser, Appl. Opt. 17, 1161 (1978).
    [CrossRef] [PubMed]
  2. O. Bryngdahl, Opt. Commun. 15, 237 (1975); S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
    [CrossRef]
  3. R. V. Pole, H.-P. Wollenmann, Appl. Opt. 14, 976 (1975).
    [CrossRef] [PubMed]
  4. C. S. Ih, Appl. Opt. 16, 2137 (1977).
    [CrossRef] [PubMed]
  5. L. Beiser, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 175 (1981).
  6. C. Kramer, Laser Focus70 (June1981).
  7. L. Beiser, “Laser Scanning Systems,” in Laser Applications, Vol. 2 (Academic, New York, 1974), pp. 53–159.

1981

L. Beiser, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 175 (1981).

C. Kramer, Laser Focus70 (June1981).

1978

1977

1975

O. Bryngdahl, Opt. Commun. 15, 237 (1975); S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
[CrossRef]

R. V. Pole, H.-P. Wollenmann, Appl. Opt. 14, 976 (1975).
[CrossRef] [PubMed]

Beiser, L.

L. Beiser, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 175 (1981).

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.

Bryngdahl, O.

O. Bryngdahl, Opt. Commun. 15, 237 (1975); S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
[CrossRef]

Ih, C. S.

Kramer, C.

C. Kramer, Laser Focus70 (June1981).

Pole, R. V.

Wollenmann, H.-P.

Appl. Opt.

Laser Focus

C. Kramer, Laser Focus70 (June1981).

Opt. Commun.

O. Bryngdahl, Opt. Commun. 15, 237 (1975); S. K. Case, V. Gerbig, Opt. Eng. 19, 711 (1980).
[CrossRef]

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

L. Beiser, Proc. Soc. Photo-Opt. Instrum. Eng. 299, 175 (1981).

Other

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

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Figures (2)

Fig. 1
Fig. 1

Positive lenticular element executing translational scan: (a) overilluminated, delimits flux tube D; (b) underilluminated, accepts smaller flux tube d.

Fig. 2
Fig. 2

Positive lenticular element executing angular scan. Cylindrical z axis normal to plane of paper through fulcrum O. Only underilluminated condition shown for simplicity.

Equations (9)

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N = θ D 0 a λ ,
N = θ D a λ + S δ
= N θ + N s ,
N d = s / δ d
N d = ( α d ) / ( a λ ) ,
N d θ = ( θ + α ) d a λ
= θ d a λ + s δ d
= N θ d + N d .
N = θ D d a λ ( 1 + r f ) ,

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