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Sternheimer, Phys. , 127, 1220 (1962). 14. Kusch and V. W. Hughes, Encyclopediaof Physics, Vol. 37,Part I, Springer Verlag, Berlin. 1959. 15. N. FI Ramsey, Molecular Beams, Oxford University Press, Londoii, 1956, p. 397ff. ATOMIC POLARIZABILITIES 27 16. J. C . Zorn, G. E. Chamberlain, and V. W. Hughes, Phys. , 129, 2566 (1963). 17. R. S. b o x , Phys. , 110, 375 (1958). 18. D. R. Hartree and W. Hartree, Proc. Cumbridge Phil. , 34, 550 (1938). 19. F. Herman and S. , 1963. 20. C. Schwartz, private communication to Pollack et al.

J. Hirschfelder, C. F. Curtiss, and R. B. Bird, Molecular Theory ofLiquids and Gases, Wiley, New York, 1954. 11. J. G. , 33,57 (1931). 12. R. Buckingham, Proc. Roy. (London), A160,94 (1937). 13. R. M. Sternheimer, Phys. , 127, 1220 (1962). 14. Kusch and V. W. Hughes, Encyclopediaof Physics, Vol. 37,Part I, Springer Verlag, Berlin. 1959. 15. N. FI Ramsey, Molecular Beams, Oxford University Press, Londoii, 1956, p. 397ff. ATOMIC POLARIZABILITIES 27 16. J. C . Zorn, G. E. Chamberlain, and V. W. Hughes, Phys.

24 BENJAMIN BEDERSON AND EDWARD J. ROBINSON where Vo is the voltage at balance. 9. The beam 1 ) s,(2) profiles are shown in Figures 10 and 11. 004 in. OOl INCHES Fig. 11. Balance peak (left) and slightly unbalanced peak (right) for 3 P meta~ stable argon, MJ = + 2 substate, at about 17 kV. , respectively. Hence, a1/a2= 1, indicating that the state coming into balance first is indeed MJ = + 1. Measurements were then taken in the vicinity of the two argon peaks, and of the helium peak, at several values of the magnetic field.

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Advances in Chemical Physics [Vol 10 - Molecular Beams] by I. Prigogine


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