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  1. Herbert E. Ives and G. R. Stilwell, J. Opt. Soc. Am. 31, 14 (1941).
  2. Encyclopedia Britannica, ninth and tenth editions, article, "Radiation." International Congress of Mathematics, Cambridge (1912), p. 208.
  3. E. Edser, Phil. Mag. 28, 508 (1914).
  4. J. Larmor, Phil. Mag. 28, 702 (1914).
  5. M. Abraham, Theorie der Elektricitat (Leipzig, Teubner, 1905), P. 335โ€“6.
  6. H. A. Lorentz, The Theory of Electrons (New York, Stechert, 1923), P. 62. "As to the amplitude, it is changed in exactly the same ratio as the frequency, so that the reflected intensity is diminished by a motion in one direction and increased by a motion in the other direction."

Abraham, M.

M. Abraham, Theorie der Elektricitat (Leipzig, Teubner, 1905), P. 335โ€“6.

Edser, E.

E. Edser, Phil. Mag. 28, 508 (1914).

Ives, Herbert E.

Herbert E. Ives and G. R. Stilwell, J. Opt. Soc. Am. 31, 14 (1941).

Larmor, J.

J. Larmor, Phil. Mag. 28, 702 (1914).

Lorentz, H. A.

H. A. Lorentz, The Theory of Electrons (New York, Stechert, 1923), P. 62. "As to the amplitude, it is changed in exactly the same ratio as the frequency, so that the reflected intensity is diminished by a motion in one direction and increased by a motion in the other direction."

Stilwell, G. R.

Herbert E. Ives and G. R. Stilwell, J. Opt. Soc. Am. 31, 14 (1941).

Other (6)

Herbert E. Ives and G. R. Stilwell, J. Opt. Soc. Am. 31, 14 (1941).

Encyclopedia Britannica, ninth and tenth editions, article, "Radiation." International Congress of Mathematics, Cambridge (1912), p. 208.

E. Edser, Phil. Mag. 28, 508 (1914).

J. Larmor, Phil. Mag. 28, 702 (1914).

M. Abraham, Theorie der Elektricitat (Leipzig, Teubner, 1905), P. 335โ€“6.

H. A. Lorentz, The Theory of Electrons (New York, Stechert, 1923), P. 62. "As to the amplitude, it is changed in exactly the same ratio as the frequency, so that the reflected intensity is diminished by a motion in one direction and increased by a motion in the other direction."

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