Abstract

A discussion of the elementary theory of the astigmatism of the concave grating. A spherocylindrical lens placed in front of the plate serves to produce a stigmatic image of the slit and increases the speed of the instrument by about 25× and doubles the dispersion, allowing the full theoretical resolving power to be realized.

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References

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  1. Runge and Mannknopf, Zeits. f. Physik 45, 13 (1927).
  2. Lacroûte, Comptes rendus 194, 1803 (1932).
  3. Oldenberg, J. O. S. A. 22, 441 (1932).
  4. Back and Goudsmit, Zeits. f. Physik 47, footnote p. 179 (1928).

Back,

Back and Goudsmit, Zeits. f. Physik 47, footnote p. 179 (1928).

Goudsmit,

Back and Goudsmit, Zeits. f. Physik 47, footnote p. 179 (1928).

Lacroûte,

Lacroûte, Comptes rendus 194, 1803 (1932).

Mannknopf,

Runge and Mannknopf, Zeits. f. Physik 45, 13 (1927).

Oldenberg,

Oldenberg, J. O. S. A. 22, 441 (1932).

Runge,

Runge and Mannknopf, Zeits. f. Physik 45, 13 (1927).

Other (4)

Runge and Mannknopf, Zeits. f. Physik 45, 13 (1927).

Lacroûte, Comptes rendus 194, 1803 (1932).

Oldenberg, J. O. S. A. 22, 441 (1932).

Back and Goudsmit, Zeits. f. Physik 47, footnote p. 179 (1928).

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