By E. Bergstrand, A. Maréchal, M. Françon, H. Wolter
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Additional info for Grundlagen der Optik / Fundamentals of Optics
BLONDLOT: C. R. Acad. Sci. Paris 117,543 (1893). TROWBRIDGE and DUANE: Phil. Mag. (5) 40, 211 (1895). SAUNDERS: Phys. Rev. 4, 81 (1897). References. 43 [80J McLEAN (air): Phil. Mag. (5) 48, 115 (1899)· [81J MERCIER: J. Phys. Radium (6) 5,168 (1924). [82J Summary by BLONDLOT and GUTTON: Rapp. pres au congres into de phys. 2, 268 (1900). Wires versus air. [83J GUTTON: J. de Phys. (5) 2, 196 (1912). [84J SOMMERFELD: Ann. Phys. 67, 223 (1899). [85J MERCIER: Ann. Phys. 20, 5 (1923). [86J [87J [88J [89J Cavity resonator.
Rotational Spectrum. 1 ) where h is PLANCK'S constant, v the frequency, B = s:aj with I the actual moment of inertia, J the rotational quantum number. The last term describes the frequency shift due to centrifugal distorsion and is small for low numbers of J. V, B, D are expressed in reciprocal wave lengths (cm. -1). IX) In 1952 RANK, RUTH and VAN DER SLUIS [95J determined Band D for the ground state by measuring v of the rotation-vibration bands of HCN in the spectralregion 8000 to 9000 A. They observed the absorption after a 215 m.
Y) HARRESS in 1912, carried out an experiment with a moving solid body . It was in the form of a horizontal rotating ring of rods of fused quartz. The light was put in and out vertically E to reflecting prisms at the centre of the ring. On account of HARRESS' death in the c war the result was not fully Fig. 28. ZEEMAN'S arrangement for moving solid bodies. definite. 0) In 1914 to 1920 ZEEMAN [108J carried out the most careful observations of the dragging coefficient in fluids as well as in solid bodies.
Grundlagen der Optik / Fundamentals of Optics by E. Bergstrand, A. Maréchal, M. Françon, H. Wolter