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  1. J. Gayles, A. W. Lohmann, W. L. Peticolas, Appl. Phys. Lett. 11, 310 (1967).
    [CrossRef]
  2. C. A. Arguello, D. L. Rousseau, S. P. S. Porto, L. E. Cheesman, J. F. Scott, to be published.
  3. V. Chandrasekharan, Proc. Ind. Acad. Sci. A25, 256 (1947).
  4. F. A. Jenkins, H. E. White, Fundamentals of Optics (McGraw-Hill Book Company, Inc., New York, 1957).

1967

J. Gayles, A. W. Lohmann, W. L. Peticolas, Appl. Phys. Lett. 11, 310 (1967).
[CrossRef]

1947

V. Chandrasekharan, Proc. Ind. Acad. Sci. A25, 256 (1947).

Arguello, C. A.

C. A. Arguello, D. L. Rousseau, S. P. S. Porto, L. E. Cheesman, J. F. Scott, to be published.

Chandrasekharan, V.

V. Chandrasekharan, Proc. Ind. Acad. Sci. A25, 256 (1947).

Cheesman, L. E.

C. A. Arguello, D. L. Rousseau, S. P. S. Porto, L. E. Cheesman, J. F. Scott, to be published.

Gayles, J.

J. Gayles, A. W. Lohmann, W. L. Peticolas, Appl. Phys. Lett. 11, 310 (1967).
[CrossRef]

Jenkins, F. A.

F. A. Jenkins, H. E. White, Fundamentals of Optics (McGraw-Hill Book Company, Inc., New York, 1957).

Lohmann, A. W.

J. Gayles, A. W. Lohmann, W. L. Peticolas, Appl. Phys. Lett. 11, 310 (1967).
[CrossRef]

Peticolas, W. L.

J. Gayles, A. W. Lohmann, W. L. Peticolas, Appl. Phys. Lett. 11, 310 (1967).
[CrossRef]

Porto, S. P. S.

C. A. Arguello, D. L. Rousseau, S. P. S. Porto, L. E. Cheesman, J. F. Scott, to be published.

Rousseau, D. L.

C. A. Arguello, D. L. Rousseau, S. P. S. Porto, L. E. Cheesman, J. F. Scott, to be published.

Scott, J. F.

C. A. Arguello, D. L. Rousseau, S. P. S. Porto, L. E. Cheesman, J. F. Scott, to be published.

White, H. E.

F. A. Jenkins, H. E. White, Fundamentals of Optics (McGraw-Hill Book Company, Inc., New York, 1957).

Appl. Phys. Lett.

J. Gayles, A. W. Lohmann, W. L. Peticolas, Appl. Phys. Lett. 11, 310 (1967).
[CrossRef]

Proc. Ind. Acad. Sci.

V. Chandrasekharan, Proc. Ind. Acad. Sci. A25, 256 (1947).

Other

F. A. Jenkins, H. E. White, Fundamentals of Optics (McGraw-Hill Book Company, Inc., New York, 1957).

C. A. Arguello, D. L. Rousseau, S. P. S. Porto, L. E. Cheesman, J. F. Scott, to be published.

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Figures (3)

Fig. 1
Fig. 1

Modulation of laser scattering intensity from linear and circular birefringence. The photograph was taken at θ = π/4 and ϕ = π/4. The 2.48-mm nodal separation is due to linear birefringence and the 28.31-mm nodal separation is due to circular birefringence.

Fig. 2
Fig. 2

Modulation of laser scattering intensity in a saturated (+)-β-maltose solution. The photograph was taken at θ = (π/2) and the 6328-Å line of the He–Ne laser was used.

Fig. 3
Fig. 3

The dispersion of the circular birefringence of (+)-β-maltose over the range 4500–6300 Å.

Equations (8)

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I ( θ , z ) [ 1 - cos 2 ϕ cos 2 θ - sin 2 ϕ sin 2 θ x cos ( 2 π Δ n z / λ ) ] ,
F 0 = x 0 A + y 0 B e i β = ( x 0 + i y 0 ) C R e i γ R + ( x 0 - i y 0 ) C L e i γ L ,
F ( z ) = ( x 0 + i y 0 ) C R exp [ i ( γ R + k z n R ) ] + ( x 0 - i y 0 ) C L exp [ i ( γ L + k z n L ) ] ,
F = ξ ^ · F ,
F ( z , θ ) = - F x sin θ + F y cos θ = i C R exp [ i ( γ R + k z n R + θ ) ] - i C L exp [ i ( γ L + k z n L - θ ) ] .
I ( θ , z ) 1 - ( 2 C R C L ) / ( C R 2 + C L 2 ) cos ( γ R - γ L + k Δ n z + 2 θ ) ,
( 2 C R C L ) / ( C R 2 + C L 2 ) = ± 1.
Δ z = 2 π / k Δ n = λ / Δ n .

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