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Volume 08

Innovative Energy & Research

ISSN: 2576-1463

Advanced Energy Materials 2019

July 11-12, 2019

July 11-12, 2019 | Zurich, Switzerland

21

st

International Conference on

Advanced Energy Materials and Research

Magnetic instability in heavily n-doped Fe-based full Heusler compounds: Origin and impact on

thermoelectric properties

Fabio Ricci, Sébastien Lemal, Matthieu J Verstraete

and

Philippe Ghosez

University of Liège, Belgium

F

e

2

YZ full Heusler compounds, on which first principles on density functional theory (DFT) simulations predict

very large thermoelectric power factor (PF), are promising candidates for thermoelectric applications. The

building blocks of their interesting thermoelectric properties are the carriers belonging to the Fe-eg orbitals that

can be opportunely engineered to maximize PF. These anti-bonding states are represented by a flat band (mainly

composed of Fe dx

2

-y

2

character) along the ΓX direction of the Brillouin Zone, related to the highly directional Fe-

Fe bond, becoming dispersive along the other directions. This band satisfies the “flat-and-dispersive” requirements

proposed by Mahan and Sofo and leads to one-dimensional transport strongly enhancing the PF. However, due to

its strongly localized nature, explicit n-doping may induce a Stoner instability driving the system to a half-metallic

phase. The present study, performed through DFT using both hybrid functional and GGA+U methods on Fe

2

YZ

1-

x

A

x

(Y = Ti, V, Nb, Ta, Z=Al, Si, Sn, Ga and A=Si, P, Sb, Ge) n-doped systems, shows that the appearance of such a

magnetic phase is strictly linked to the Fe-eg and Y-site eg orbital hybridization and that it possesses a pure electronic

origin, independent on the dopant species. Although the Stoner instability can provide half-metallicity with coupled

thermomagnetic responses, the PF is typically reduced in the half-metallic phase due to a reduction of the number

of carriers available at the Fermi level. In certain cases, however, the values of the PF are still large (for Fe

2

TaGa

1-x

Ge

x

or Fe

2

TiSi

1-x

P

x

PF is between 9 and 15 10

-3

W K

-2

m

-1

at 600 K, for example) which stays promising for thermoelectric

applications. Going further, we elucidate the possibility to exploit the broader nature of 4d and 5d orbitals at the

bottom of the conduction band to overcome the magnetic phase appearance in the doping range of interest.

Biography

Fabio Ricci did his PhD on both simulations and experimental measurements on magnetic properties of materials (diluted magnetic semiconductors and soft

magnetic materials) by means of the magneto-optical Kerr effect. Subsequently, he worked on theoretical simulations on Fe-based superconductors, principally

iron-chalcogenides. He developed and implemented in the ABINIT code the formalism for the non-collinear magnetism in the density functional perturbation

theory and, at the same time, started to work on the theoretical engineering of thermoelectric properties of the Fe-based full-Heusler compounds.

fabio.ricci@uliege.be

Fabio Ricci et al., Innov Ener Res 2019, Volume 08