18th Magnetic Materials Center Seminar
June 5, 2006, 16:00
7th floor seminar room, Sengen
Development of new quaternary Heusler alloy systems for
Spintronic applications
S. Vijay Karthik
Half-metallic ferromagnetic materials possess a gap in the minority band (viz. semiconducting),
whereas exhibits metallic behavior in the majority band, in other words, the
electrons at the Fermi level have 100% spin polarization. Currently, the most promising
materials which exhibit high spin polarization and high Curie temperature are believed to
be C1b type half-Heusler and L21 type full-Heusler alloys. Galanakis et al studied the
quaternary Heusler alloys and found the possibility of obtaining new half-metallic
systems. In this presentation, the microstructure, 3DAP analysis, and spin polarization of
the polycrystalline bulk quaternary Co2Cr1-xFexAl, Co2Fe1-xVxAl and Co2Cr1-xVxAl alloys
shall be discussed. Also, a brief overview on the possibility of obtaining high spin
polarization and Curie temperature required for spintronic applications from the Heusler
alloy systems such as Co2FeZ (where Z = Al, Ga, Ge, Sb, In), Co2MnSb, CoMnSb,
CoFeSb and zinc-blend CrSb shall be studied.
Effect of structural disorder on Spin polarization in half-metals
A. Rajanikanth
Spin polarization of half-metals is strongly effected by the structural disorder.
From the theoretical calculations by Picozzi et al, a site disorder of 8% will completely
destroy the half-metallicity in Co2MnSi and Co2MnGe. In order to see the effect of
structural disorder on spin-polarization, thin films of L21 and A2 structural ordering were
grown on SiO2 substrate and spin polarization is measured by point contact Andreev
reflection method. Using Nb as a superconducting tip a spin polarization of 58% for L21
ordered and 35% for A2 ordered thin films of Co2MnGe were obtained. Similarly a spin
polarization of 58% for L21 ordered Co2MnSi and 52% for A2 ordered thin films were
obtained. Our recent measurements on the spin polarization of Co2FeSi both in the bulk
and thin films have shown a spin polarization of only 49%, because of the weak L21
ordering. With the substitution of Si with Al by Co2FeSi0.5Al0.5, the spin polarization
value increases drastically to 61%. The possible reasons for the increase in spin
polarization will be discussed.
NdFeB multilayers for highest energy product
Zsolt Gercsi
Exchange coupled hard / soft nanocomposite magnets were predicted to exhibit
remarkably high maximum energy product (BH)max over 120 MGOe. In such composite
structures, a magnetically soft phase with high saturation magnetization (Ms) is added to
the hard magnetic one, which has lower Ms value. If the thickness of the soft phase is
smaller than 2dh (dh- exchange length of hard phase), the n the Ms value of composite
material can be improved, meanwhile the Hc value of hard phase is maintained.
Nevertheless, it is not easy to achieve such a high energy product. So far,
maximum energy products of around 50-60 MGOe were reported. The main reasons for
this difference are the size of nanograins, their distribution and alignment.
In order to achieve high maximum energy product, Br/Bs ratio must be maximized by
introducing texture into the structure and also the particle size must be reduced into the
single domain region. Another important criterion is to minimize the exchange coupling
between single domain particles, which averages out the magnetocrystalline anisotropy.
In this talk, my research progress on exchange coupled NdFeB / FeCo thin films
prepared by dc magnetron / rf sputtering techniques will be presented.
