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Anomalous Behavior of Al 27 ( p , α ) Mg 24 Differential Cross Sections

Anomalous Behavior of Al 27 ( p , α ) Mg 24 Differential Cross Sections pendicular orientation have been made on both Nd'46 and Nd'43 and will be discussed in a complete paper on this subject. The main difficulty in the analysis of the data for the perpendicular orientation is in the fitting of the results to the spin-Hamiltonian (2). Formulas of fourth or higher order perturbation theory must be used to obtain sufficiently accurate values of the parameters inasmuch as, particularly in the case of Nd'43, the normal second- and third-order contributions to the hyperfine effects are very much larger than that coming from gN.LfNH I. We thank Eugene Wong for the preparation of the crystals used in these experiments. * This research was supported in part by the U. S. Atomic Energy Commission. 'G. Feher, Phys. Rev. 103, 834 (1956). 2 Dorain, Hutchison, and Wong (to be published). 3 B. Bleaney, Phil. Mag. 42, 441 (1951). 4 B. Bleaney (private communication). 5 R. J. Elliott and K. W. H. Stevens, Proc. Roy. Soc. (London) A218, 553 (1953). 6 Sayre, Sancier, and Freed, J. Chem. Phys. 23, 2060 (1955). 7 B. Bleaney, Proc. Phys. Soc. (London) A68, 937 (1955). (dv, d C.M. mb/st. 0.3 dMCM I mb/st. 1.5 I I i I http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Physical Review American Physical Society (APS)

Anomalous Behavior of Al 27 ( p , α ) Mg 24 Differential Cross Sections

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Publisher
American Physical Society (APS)
Copyright
Copyright © 1958 The American Physical Society
ISSN
1536-6065
DOI
10.1103/PhysRev.110.286
Publisher site
See Article on Publisher Site

Abstract

pendicular orientation have been made on both Nd'46 and Nd'43 and will be discussed in a complete paper on this subject. The main difficulty in the analysis of the data for the perpendicular orientation is in the fitting of the results to the spin-Hamiltonian (2). Formulas of fourth or higher order perturbation theory must be used to obtain sufficiently accurate values of the parameters inasmuch as, particularly in the case of Nd'43, the normal second- and third-order contributions to the hyperfine effects are very much larger than that coming from gN.LfNH I. We thank Eugene Wong for the preparation of the crystals used in these experiments. * This research was supported in part by the U. S. Atomic Energy Commission. 'G. Feher, Phys. Rev. 103, 834 (1956). 2 Dorain, Hutchison, and Wong (to be published). 3 B. Bleaney, Phil. Mag. 42, 441 (1951). 4 B. Bleaney (private communication). 5 R. J. Elliott and K. W. H. Stevens, Proc. Roy. Soc. (London) A218, 553 (1953). 6 Sayre, Sancier, and Freed, J. Chem. Phys. 23, 2060 (1955). 7 B. Bleaney, Proc. Phys. Soc. (London) A68, 937 (1955). (dv, d C.M. mb/st. 0.3 dMCM I mb/st. 1.5 I I i I

Journal

Physical ReviewAmerican Physical Society (APS)

Published: Apr 1, 1958

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