Hostname: page-component-6766d58669-kl59c Total loading time: 0 Render date: 2026-05-22T23:20:23.975Z Has data issue: false hasContentIssue false
  • English
  • Français

The magnetic properties of antimony

Published online by Cambridge University Press:  24 October 2008

D. Shoenberg  and
M.Zaki Uddin
D. Shoenberg
Affiliation:
Senior Rouse Ball Student, Trinity College
M.Zaki Uddin
Affiliation:
Trinity college
Get access Rights & Permissions [Opens in a new window]

Extract

The magnetic susceptibility of antimony both parallel and perpendicular to the trigonal axis is independent of field down to 4° K. The numerical value of the susceptibility parallel to the trigonal axis decreases with increasing temperature, similarly to that of bismuth, but perpendicular to the trigonal axis there is no temperature dependence. The results at higher temperatures are compared with earlier measurements and the comparison suggests that the susceptibility of antimony, like that of bismuth, is very sensitive to addition of foreign elements.

Information

Type
Research Article
Information
Mathematical Proceedings of the Cambridge Philosophical Society , Volume 32 , Issue 3 , October 1936 , pp. 499 - 502
Copyright
Copyright © Cambridge Philosophical Society 1936

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

Article purchase

Temporarily unavailable

References

* Shoenberg, and Uddin, , Proc. Roy. Soc. A (in press)Google Scholar, referred to as I.

* McLennan, and Cohen, , Trans. Roy. Soc. Can. 23 (1929), 159.Google Scholar

† This was verified also at 4° K.

* de Haas, and Alphen, van, Leiden Comm. No. 225b (1933).Google Scholar

* E 0 is the energy of the highest occupied electronic state and μ is the effective moment of the electrons, defined on the simplifying assumption that the energy surfaces in the second Brillouin zone are spherical. An account of the significance of these parameters is given in I, in connection with Peierl's theory of the field dependence of bismuth susceptibility.