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  1. R. H. McFarland and E. A. Soltysik, Phys. Rev. 127, 2090 (1962).
    [CrossRef]
  2. I. C. Percival and M. J. Seaton, Phil. Trans. Roy. Soc. (London) 251, 113 (1958).
    [CrossRef]
  3. H. R. M. Moussa, Ph.D. thesis, University of Leiden (1967).
  4. B. L. Moiseiwitsch and S. J. Smith, Rev. Mod. Phys. 40, 238 (1968).
    [CrossRef]

1968 (1)

B. L. Moiseiwitsch and S. J. Smith, Rev. Mod. Phys. 40, 238 (1968).
[CrossRef]

1962 (1)

R. H. McFarland and E. A. Soltysik, Phys. Rev. 127, 2090 (1962).
[CrossRef]

1958 (1)

I. C. Percival and M. J. Seaton, Phil. Trans. Roy. Soc. (London) 251, 113 (1958).
[CrossRef]

McFarland, R. H.

R. H. McFarland and E. A. Soltysik, Phys. Rev. 127, 2090 (1962).
[CrossRef]

Moiseiwitsch, B. L.

B. L. Moiseiwitsch and S. J. Smith, Rev. Mod. Phys. 40, 238 (1968).
[CrossRef]

Moussa, H. R. M.

H. R. M. Moussa, Ph.D. thesis, University of Leiden (1967).

Percival, I. C.

I. C. Percival and M. J. Seaton, Phil. Trans. Roy. Soc. (London) 251, 113 (1958).
[CrossRef]

Seaton, M. J.

I. C. Percival and M. J. Seaton, Phil. Trans. Roy. Soc. (London) 251, 113 (1958).
[CrossRef]

Smith, S. J.

B. L. Moiseiwitsch and S. J. Smith, Rev. Mod. Phys. 40, 238 (1968).
[CrossRef]

Soltysik, E. A.

R. H. McFarland and E. A. Soltysik, Phys. Rev. 127, 2090 (1962).
[CrossRef]

Phil. Trans. Roy. Soc. (London) (1)

I. C. Percival and M. J. Seaton, Phil. Trans. Roy. Soc. (London) 251, 113 (1958).
[CrossRef]

Phys. Rev. (1)

R. H. McFarland and E. A. Soltysik, Phys. Rev. 127, 2090 (1962).
[CrossRef]

Rev. Mod. Phys. (1)

B. L. Moiseiwitsch and S. J. Smith, Rev. Mod. Phys. 40, 238 (1968).
[CrossRef]

Other (1)

H. R. M. Moussa, Ph.D. thesis, University of Leiden (1967).

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Figures (1)

Fig. 1
Fig. 1

Variation of polarization factor, α, with wavelength for a Hilger D 330 monochromator with an EMI.6256B photomultiplier.

Equations (8)

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I ( θ ) = ( I / 4 π ) [ 3 ( 100 - P cos 2 θ ) / ( 300 - P ) ] ,
P = 100 ( I - I ) / ( I + I ) ;
α = k / k ,
I ( 90 ° ) = ( I / 4 π ) × [ 300 / ( 300 - P ) ] .
I ( 90 ° ) = S ( 90 ° ) / k × ( α + 1 ) [ I / I + 1 ] / 2 [ α ( I / I ) + 1 ] ,
2 k = k + k .
I = ( 4 π / k ) [ S ( 90 ° ) ( α + 1 ) ( I + 2 I ) / 3 ( α I + I ) ] .
I = 4 π S ( 90 ° ) / k .