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References

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  1. P. A. Ross, Phys. Rev.,  28, p. 425A; 1926.
    [Crossref]
  2. Webster and Hennings, Phys. Rev.,  21, pp. 301–311; 1923.
    [Crossref]
  3. D. L. Webster, Proc. Nat. Acad. Sci.,  6, pp. 264–272; 1920.
  4. F. W. Bubb, Phys. Rev.,  24, pp. 177–189; 1924.
    [Crossref]
  5. Bergen Davis, Phys. Rev.,  9, pp. 64–77; 1917.
    [Crossref]
  6. H. A. Kramers, Phil. Mag.,  46, pp. 836–871; 1923.
    [Crossref]

1926 (1)

P. A. Ross, Phys. Rev.,  28, p. 425A; 1926.
[Crossref]

1924 (1)

F. W. Bubb, Phys. Rev.,  24, pp. 177–189; 1924.
[Crossref]

1923 (2)

Webster and Hennings, Phys. Rev.,  21, pp. 301–311; 1923.
[Crossref]

H. A. Kramers, Phil. Mag.,  46, pp. 836–871; 1923.
[Crossref]

1920 (1)

D. L. Webster, Proc. Nat. Acad. Sci.,  6, pp. 264–272; 1920.

1917 (1)

Bergen Davis, Phys. Rev.,  9, pp. 64–77; 1917.
[Crossref]

Bubb, F. W.

F. W. Bubb, Phys. Rev.,  24, pp. 177–189; 1924.
[Crossref]

Davis, Bergen

Bergen Davis, Phys. Rev.,  9, pp. 64–77; 1917.
[Crossref]

Hennings,

Webster and Hennings, Phys. Rev.,  21, pp. 301–311; 1923.
[Crossref]

Kramers, H. A.

H. A. Kramers, Phil. Mag.,  46, pp. 836–871; 1923.
[Crossref]

Ross, P. A.

P. A. Ross, Phys. Rev.,  28, p. 425A; 1926.
[Crossref]

Webster,

Webster and Hennings, Phys. Rev.,  21, pp. 301–311; 1923.
[Crossref]

Webster, D. L.

D. L. Webster, Proc. Nat. Acad. Sci.,  6, pp. 264–272; 1920.

Phil. Mag. (1)

H. A. Kramers, Phil. Mag.,  46, pp. 836–871; 1923.
[Crossref]

Phys. Rev. (4)

P. A. Ross, Phys. Rev.,  28, p. 425A; 1926.
[Crossref]

Webster and Hennings, Phys. Rev.,  21, pp. 301–311; 1923.
[Crossref]

F. W. Bubb, Phys. Rev.,  24, pp. 177–189; 1924.
[Crossref]

Bergen Davis, Phys. Rev.,  9, pp. 64–77; 1917.
[Crossref]

Proc. Nat. Acad. Sci. (1)

D. L. Webster, Proc. Nat. Acad. Sci.,  6, pp. 264–272; 1920.

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Figures (3)

F. 1
F. 1

General scheme of apparatus for the application of the balanced foil method to the study of polarization.

F. 2
F. 2

Polarization of the general x-radiation.

F. 3
F. 3

Isochromats of the general x-radiation showing the relation of form to the direction of the electric vector.

Equations (1)

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P = I 1 I 2 I 1 + I 2