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References

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  1. J. W. White, J. Opt. Soc. Am. 32, 285 (1942).
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  3. A. Weber, S. P. S. Porto, L. E. Cheesman, J. J. Barrett, J. Opt. Soc. Am. 57, 19 (1967).
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  4. T. Witkowicz, A. D. May, Appl. Opt. 14, 3092 (1975).
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  5. C. E. Hathaway, in The Raman Effect, Vol. 1, A. Anderson, Ed. (Marcel Dekker, New York, 1971), pp. 195–199.
  6. J. J. Barrett, N. I. Adams, J. Opt. Soc. Am. 58, 311 (1968).
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  7. R. A. Hill, A. J. Mulac, C. E. Hackett, Appl. Opt. 16, 2004 (1977).
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  10. T. G. Matthews, Appl. Opt. 21, 577 (1982).
    [CrossRef] [PubMed]

1982

1980

1977

1975

1974

1968

1967

1951

1942

Adams, N. I.

Barrett, J. J.

Byer, R. L.

Cheesman, L. E.

dimming, C.

Hackett, C. E.

Hartley, D. L.

Hathaway, C. E.

C. E. Hathaway, in The Raman Effect, Vol. 1, A. Anderson, Ed. (Marcel Dekker, New York, 1971), pp. 195–199.

Hill, R. A.

Matthews, T. G.

May, A. D.

Mulac, A. J.

Porto, S. P. S.

Stansbury, E. J.

Trutna, W. R.

Weber, A.

Welsh, H. L.

White, J. W.

Witkowicz, T.

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Figures (3)

Fig. 1
Fig. 1

Distance reduction of two laser beams by a prism.

Fig. 2
Fig. 2

Experimental arrangement for prism multipass cavity.

Fig. 3
Fig. 3

Vibrational Q-branch of N2 in a laminar premixed CH4–air–flame.

Equations (1)

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V = D f D i cos ( arcsin sin α n ) cos ( arcsin { n sin [ φ - arcsin ( sin α n ) ] } ) cos ( φ - arcsin sin α n ) cos α ,

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