Jump to content

Arrott plot

From Wikipedia, the free encyclopedia
This is an old revision of this page, as edited by Forbes72 (talk | contribs) at 02:32, 8 July 2022 (Details: space). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.
Arrott plot for a simple mean field ferromagnetic phase transition.

In condensed matter physics, an Arrott plot is a plot of the square of the magnetization of a substance, against the ratio of the applied magnetic field to magnetization at one (or several) fixed temperature(s). Arrott plots are an easy way of determining the presence of ferromagnetic order in a material.[1][2] They are named after American physicist Anthony Arrott who introduced them as a technique for studying magnetism in 1957.[3]

Details

According to the Landau theory applied to the mean field picture for magnetism, the free energy of a ferromagnetic material close to a phase transition can be written as:

where , the magnetization, is the order parameter, is the applied magnetic field, is the critical temperature, and are material constants.

Close to the phase transition, this gives a relation for the magnetization order parameter:

where is a dimensionless measure of the temperature.

Thus in a graph plotting vs. for various temperatures, the line without an intercept corresponds to the dependence at the critical temperature. Thus along with providing evidence for the existence of a ferromagnetic phase, the Arrott plot can also be used to determine the critical temperature for the phase transition.[4] [5]

Generalization

Giving the critical exponents explicitly in the equation, Arrott proposed:[6]

Where are free parameters. In classical Landau theory, and so this reduces to the linear versus plot, but allows more flexibility, since real ferromagnets do not always have critical exponents exactly consistent with a simple mean field theory ferromagnetism.

See also

References

  1. ^ Yeung, I.; Roshko, R.; Williams, G. (1986). "Arrott-plot criterion for ferromagnetism in disordered systems". Physical Review B. 34 (5): 3456–3457. Bibcode:1986PhRvB..34.3456Y. doi:10.1103/PhysRevB.34.3456.
  2. ^ du Trémolet de Lacheisserie, E., ed. (2005). Magnetism. Springer. ISBN 978-0-387-22967-6.
  3. ^ Arrott, A. (1957). "Criterion for Ferromagnetism from Observations of Magnetic Isotherms". Physical Review. 108 (6): 1394–1396. Bibcode:1957PhRv..108.1394A. doi:10.1103/PhysRev.108.1394.
  4. ^ Hadimani, R. L.; Melikhov, Y.; Snyder, J. E.; Jiles, D. C. (2008). "Determination of Curie temperature by Arrott plot technique in Gd5(SixGe1−x)4 for x>0.575". Journal of Magnetism and Magnetic Materials. 320 (20): e696 – e698. Bibcode:2008JMMM..320E.696H. doi:10.1016/j.jmmm.2008.04.035.
  5. ^ Farle, R. L.; Lewis, Y.; Baberschke, K. (1993). "Detailed analysis of the in sifu magneto-optic Kerr signal of gadoilinium films near the Curie temperature". Applied Physics Letters. 62 (21): 2728–2730. Bibcode:1993ApPhL..62.2728F. doi:10.1063/1.109246.
  6. ^ Arrott, Anthony; Noakes, John E. (1967-10-02). "Approximate Equation of State For Nickel Near its Critical Temperature". Physical Review Letters. 19 (14). American Physical Society (APS): 786–789. doi:10.1103/physrevlett.19.786. ISSN 0031-9007.