8-12 July 2013
Africa/Johannesburg timezone
<a href="http://events.saip.org.za/internalPage.py?pageId=13&confId=32"><font color=#ff0000>SAIP2013 PROCEEDINGS AVAILABLE</font></a>

Magnetic properties of the (Cr<sub>100-<i>x</i></sub>Al<sub><i>x</i></sub>)<sub>99</sub>V<sub>1</sub> alloy system

9 Jul 2013, 14:10
20m
Oral Presentation Track A - Division for Condensed Matter Physics and Materials DCMPM2

Speaker

Mr Blessed Muchono (University of Johannesburg)

Apply to be<br> considered for a student <br> &nbsp; award (Yes / No)?

Yes

Level for award<br>&nbsp;(Hons, MSc, <br> &nbsp; PhD)?

PhD

Would you like to <br> submit a short paper <br> for the Conference <br> Proceedings (Yes / No)?

Yes

Main supervisor (name and email)<br>and his / her institution

Professor ARE Pronsloo, alettap@uj.ac.za, University of Johannesburg

Abstract content <br> &nbsp; (Max 300 words)

The magnetic phase diagram of the Cr100-xAlx alloy system is unique amongst Cr alloy systems because it exhibits a deep minimum at the triple point concentration xc ≈ 2, where the incommensurate spin-density-wave (SDW) and commensurate SDW phases coexist with the paramagnetic (P) phase [1]. The interesting properties of this system were previously explored by the addition of 5 at.% Mo to form a (Cr100-xAlx)95Mo5 alloy system [2]. Antiferromagnetism (AFM) in this system was suppressed to below 4 K in the range 2 ≤ x ≤ 6 [2]. Mo suppresses AFM in Cr and its alloys through electron hole pair breaking effects due to electron scattering [1]. For comparison, the present study investigates the magnetic properties of the Cr100-xAlx system further through the addition of V. This reduces the AFM in Cr alloys through a mechanism different to that associated with Mo by reducing the electron-to-atom ratio [1]. Electrical resistivity (ρ), Seebeck coefficient (S) and magnetic susceptibility (χ) measurements, as a function of temperature in the range 2 K ≤ T ≤ 390 K, were carried out on the (Cr100-xAlx)99V1 alloy system, with 0 < x < 7. Néel temperatures (TN) obtained from all these measurements decrease with Al concentration, disappearing near x ≈ 1.5, again reappearing for x > 4.5. ρ(T) and S(T) for samples with x ≥ 6.1 show smeared anomalies making the determination of TN difficult. However, these anomalies are sharp in χ(T), proving that it is an important tool in probing AFM in this system. The present results show that the addition of just 1 at.% V to the Cr100-xAlx alloy system suppresses AFM in the concentration range 1.5 ≤ x ≤ 4.5. This behaviour is similar to that of the (Cr100-xAlx)95Mo5 alloy system [2].

[1] Fawcett E, Alberts H L, Galkin V Yu, Noakes D R and Yakhmi J V 1994 Rev Mod. Phys. 66 25
[2] Smit P and Alberts H L 1986 J. Phys. F: 16 L191

Primary author

Mr Blessed Muchono (University of Johannesburg)

Co-authors

Prof. Aletta Prinsloo (University of Johannesburg) Dr Charles Sheppard (University of Johannesburg)

Presentation Materials

Peer reviewing

Paper