Introduction to Heusler compounds:
From the case of Fe 2 VAl
Chin Shan Lue (呂欽山)
2017-03-28-NTU
Outline
1) Introduction to Heusler compounds Full-Heusler compounds
Half-Heusler compounds 2) Case study of Fe
2VAl
3) Promising characteristics of Heusler compounds Thermoelectric properties
Spintronic applications
Topological materials
4) Summary
Full-Heusler compounds: X
2YZ Half-Heusler compounds: XYZ
Heusler compounds
First full-Heusler Cu2MnAl in 1903
More than 1000 real Heusler compounds
Fritz Heusler (Germany)
First half-Heusler NiMnSb in 1951
L
21 structure
Cu2MnAl-type
16 atoms per unit cell
Fe2VAl, Ru2NbGa, Ni2MnGa (HT), …
B2 structure
CsCl-type
2 atoms per unit cell
Co2MnAl, Ru2NbAl, Ru2VAl, …
Common crystal structures of Heusler compounds
Anti-site disorder
First determination of crystal structure for Cu2MnAl by Otto Heusler in 1934
DO
3structure
BiF3-type
16 atoms per unit cell Fe3Al; Fe3Ga; Fe3Si, ...
C1
bstructure
MgAgAs-type
12 atoms per unit cell
NiMnSb, NiZrSn, CoTiSb, …
Half-Heusler XYZ
X = Y
X + void
Binary compounds X
3Z
Various properties of Heusler compounds
Ferromagnetism: Co2MnZ, Pd2Mn(In,Sn), …
Superconductivity: Pd2YSn (TC = 4.9 K), Ni2NbSn, Pd2ErSn, …
Shape memory behavior: Ni2MnGa (Martensitic transformation TM = 220 K), … Semiconducting: Fe2VAl, Ru2TaAl, IrNbSb, NiHfSn, CoTiSb, …
Unusual physical behavior in Fe
2VAl
Paramagnetic behavior in Fe
2VAl by Webster & Ziebeck in 1983
(Fe1-xVx)3Al
x=0.33 Fe2VAl
Semiconductor-like in ρ Tc = 0 K Fe3Al Tc = 790 K
semimetal
Possible 3d heavy fermion for Fe
2VAl
Low-T C = C
e+ C
ph= g T + b T
3C/T = g + b T
2Expected behavior for ordinary semimetals (low Fermi-level DOS)
g = 14 mJ/mol K
2e F
B
th
k N ( E ) m 3
2
2g
Sommerfeld coefficient based on free electron model
100 50
*
e
e th
xp
m m g
g for Fe
2VAl
g = 1.07 mJ/mol K2
Semimetallic Ru2TaAl
e
3
th xp
g g
from C. M. Wei et al.
Simple concept for heavy fermions
CeAl3 g =1620 mJ/mol K2 CeCu6 g =1300 mJ/mol K2 UBe13 g =1100 mJ/mol K2 U2Zn17 g = 500 mJ/mol K2
…….
hybridization
It is less likely to observe heavy fermion behavior in d-electron systems since the corresponding wave-functions of d-orbitals are more dispersive.
DOS
E EF
E
k EF
f-electrons f-electron heavy fermions
Spinel LiV2O4 g = 420 mJ/mol K2
d-electron heavy fermion???
PRL 78, 3729 (1997); PRL 85, 1052 (2000) PRL 89, 267201 (2002); PRL 99, 167402 (2007)Nat. Comm. 3, 981 (2012); PRL 113, 236402 (2014);
...….
s-electrons
Band structure calculations for Fe
2VAl
郭光宇
Electronic structure, local moments, and transport in Fe2VAl, D. J. Singh & I. I. Mazin, Phys. Rev. B 57, 14352 (1998)
Excitonic correlations in the intermetallic Fe2VAl, R. Weht & W. E. Pickett, Phys. Rev. B 58, 6855 (1998)
Electronic structure and magnetism of Fe3-xVxX (X=Si, Ga, and Al) alloys by the KKR-CPA method, A. Bansil, et al., Phys. Rev. B 60, 13396 (1999)
Hybridization-induced band gaps in transition-metal aluminides, M. Weinert & R. E. Watson, Phys. Rev. B 58, 9732 (1998)
N(E
F) = 0.08 states/eV atom
NMR evidence for semimetallic behavior in Fe
2VAl
Low V-3d N(E
F) = 0.11 states/eV atom Thermally excited carriers
across electronic bands near E
FKorringa relation 1/T
1T ~ C[N(E
F)]
2Activation energy E
A~ 0.27 eV
Question of possible 3d heavy fermion for Fe
2VAl
Small g = 1.5 mJ/mol K
2Sample-dependent
Field-dependent
False heavy fermion behavior in Fe
2VAl
For non-interacting magnetic clusters with spin J >1/2, the magnetic specific heat can be generated by the so-called multi- level Schottky function as
T k
H x g
B
B
unit formula
per population
% 36 . 0
7 . 3 ) 1 2 (
3
f
J J g
J
B
BThe low-T upturn in C is not intrinsic;
It is reasonably associated with magnetic clusters due to anti-site disorder in real samples.
Ru2TaAl
Effects of magnetic clusters in Fe
2VAl, Fe
2VGa and Fe
2TiSn
“Weak ferromagnetism induced by atomic disorder in Fe2TiSn”, A. Ślebarski, M. B. Maple, et al., Phys. Rev. B 62, 3296 (2000)
“Kondo-type behavior in Fe2-xMxTiSn(M=Co,Ni)”,
A. Ślebarski, M. B. Maple, et al., Phys. Rev. B 63, 214416 (2001)
“Fe−3s core-level splitting and local magnetism in Fe2VAl”, Phys. Rev. B 63, 054419 (2001)
“Superparamagnetism and magnetic defects in Fe2VAl and Fe2VGa”, J. Phys.: Condens. Matter 13, 1585 (2001)
“Structure and magnetic order in Fe2+xV1-xAl”, J. Phys.: Condens. Matter 13, 5487 (2001)
“NMR and Mössbauer study of spin dynamics and electronic structure of Fe2+xV1-xAl and Fe2VGa”,
Phys. Rev. B 67, 224425 (2003)
“Transport and magnetic properties of the Heusler-type Fe2-xV1+xAl system (−0.01⩽x⩽0.08)”,
Phys. Rev. B 71, 094425 (2005)
“Evidence for cluster glass behavior in Fe2VAl Heusler alloys”, Phys. Rev. B 78, 064401 (2008)
Band structure calculations for Fe
2VAl
郭光宇
Electronic structure, local moments, and transport in Fe2VAl, D. J. Singh & I. I. Mazin, Phys. Rev. B 57, 14352 (1998)
Excitonic correlations in the intermetallic Fe2VAl, R. Weht & W. E. Pickett, Phys. Rev. B 58, 6855 (1998)
Electronic structure and magnetism of Fe3-xVxX (X=Si, Ga, and Al) alloys by the KKR-CPA method, A. Bansil, et al., Phys. Rev. B 60, 13396 (1999)
Hybridization-induced band gaps in transition-metal aluminides, M. Weinert & R. E. Watson, Phys. Rev. B 58, 9732 (1998)
More first-principles calculations on Fe
2VAl
“Electronic structure and x-ray magnetic circular dichroism in Heusler-type Fe2-xV1+xAl: First-principles calculations”,
Phys. Rev. B 77, 134444 (2008)
“Density functional study of elastic and vibrational properties of the Heusler- type alloys Fe2VAl and Fe2VGa”,
Phys. Rev. B 80, 125108 (2009)
“Electronic and thermoelectric properties of Fe2VAl: The role of defects and disorder”,
Phys. Rev. B 83, 205204 (2011)
“Effect of onsite Coulomb repulsion on thermoelectric properties of full- Heusler compounds with pseudogaps”,
Phys. Rev. B 84, 125104 (2011)
“Low-Dimensional transport and large thermoelectric power factors in bulk semiconductors by band engineering of highly directional electronic states”, Phys. Rev. Lett. 114, 136601 (2015)
“Quantum many-body intermetallics: Phase stability of Fe3Al and small-gap formation in Fe2VAl”,
Phys. Rev. B 95, 045114 (2017)
……
Thermoelectric materials
RSC Advances 5, 52 (2015)
Thermoelectric generator module
ZT: Figure of merit 熱電優質
ZT = 1 → 10.8%
ZT = 2 → 16.4%
T
c/T
h= 0.5 2 .
, with
, 1
1 ) 1
(
2 max
h c
h h c
c
h
T T
S T Z
T T T
Z T Z T
T
T
Thermoelectric efficiency
: Generated electrical energy/Absorbed heat energyThermoelectric performance ZT = S
2T/
(
e+
l)Physical approach based on Mott equation,
DOS
EF E
S: Seebeck coefficient
: electrical resistivity
e: electronic thermal conductivity
l: lattice thermal conductivity
EF
E
e
E
E N E
N S e
( )
) ( 1 1
Chemical approach by partially substituting heavy elements and/or vacancies to enhance the phonons scattering and thus reduce the contribution of
l.
Naive expectation:
S = 200 V/K
= 1000 W-cm
= 2 W/m-K
ZT=1 at 500 K
Full-Heusler compounds with L
21-type structure
Total number of valence electrons per formula unit VEC = Z
t= 24
A simple rule with number of valence electrons
In principles → Semiconductors In reality → Semimetals
Half-Heusler compounds with C
b1-type structure
Total number of valence electrons per formula unit VEC = Z
t= 18 In principles → Semiconductors
In reality → Semimetals
Fe2VAl, Fe2VGa, Fe2TiSn, Ru2NbGa, Ru2TaAl, Ru2TiSi, ….
NiTiSn, NiZrSn, NiHfSn, CoTiSb, FeVSb….
Thermoelectric studies of Fe
2VAl and related compounds
Nishino et al., Phys. Rev. B 63, 233303 (2001)
C. S. Lue & Y. K. Kuo, Phys. Rev. B 66, 085121 (2002)
High Large S
Nishino’s group
Phys. Rev. B 71, 094425 (2005) Phys. Rev. B 71, 245112 (2005) Phys. Rev. B 74, 115115 (2006)
………
C. S. Lue & Y. K. Kuo,
J. Appl. Phys. 96, 2681 (2004) Phys. Rev. B 71, 064202 (2005) Phys. Rev. B 72, 054116 (2005) Phys. Rev. B 75, 064202 (2007) Phys. Rev. B 78, 165117 (2008) Other groups
J. Alloys Compd. 349, 37 (2003) Phys. Rev. B 77, 224415 (2008) J. Appl. Phys. 111, 093710 (2012)
……..
Thermoelectric studies of Fe
2VAl-based compounds
J. Appl. Phys. 115, 033704 (2014)
Optimized ZT ~ 0.2
Thermoelectric studies of half-Heusler compounds with Z
t= 18
“Gap at the Fermi level in the intermetallic vacancy system RNiSn (R=Ti,Zr,Hf)”, Z. Phys. B 75, 116 (1989).
“Narrow band in the intermetallic compounds MNiSn (M=Ti,Zr,Hf)”, Z. Phys. B 80, 353 (1990).
“Band gap and stability in the ternary intermetallic compounds NiSnM (M=Ti,Zr,Hf):
A first principles study”,
Phys. Rev. B 51, 10443 (1995).
…..
“Effect of substitutions and defects in half-Heusler FeVSb studied by electron transport measurements and KKR-CPA electronic structure calculations”, Phys. Rev. B 70, 184207 (2004).
“Electronic structure and thermoelectric properties of half-Heusler Zr0.5Hf0.5NiSn by first-principles calculations”,
Appl. Phys. Lett. 113, 193705 (2013).
...
“Effect of Ti substitution on the thermoelectric properties of (Zr,Hf)NiSn half-Heusler compounds”, Appl. Phys. Lett. 86, 082105 (2005).
“Thermoelectric performance of half-Heusler compounds TiNiSn and TiCoSb”, Appl. Phys. Lett. 105, 013709 (2009).
“Thermoelectric property study of nano-structured p-type half-Heuslers (Hf,Zr,Ti)CoSb0.8Sn0.2”, Advanced Energy Materials 3, 1195 (2013).
...
Thermoelectric materials based on half-Heusler compounds
Translational Materials Research 2, 025001 (2015)
Half-metallic Heusler compounds
Half-metals Half-Heusler
100% polarization
A semi-empirical general rule: Slater-Pauling curve
Half-Heusler compounds
Hybridization between Ni and Mn in minority bands in NiMnSb
I. Galanakis, P. H. Dederiches, N. Papanikolaou, Phys. Rev. B 66 134428 (2002).
Slater-Pauling curve for full-Heusler compounds
Full-Heusler compounds
Hybridization between Co-Co and Mn in minority bands in Co2MnSi(Ge)
I. Galanakis, P. H. Dederiches, and N. Papanikolaou, Phys. Rev. B 66 174429 (2002).
More first-principles calculations
Review article: J. Phys.:
Condens. Matter 19 315213 (2007).
“Computational investigation of half-Heusler compounds for spintronics applications”, Phys. Rev. B 95, 024411 (2017).
“First-principles calculation of the effects of partial alloy disorder on the static and dynamic magnetic properties of Co2MnSi”, Phys. Rev. B 95, 094425 (2017).
Spin-resolved DOS for Co2MnZ
Recent advances in the Heusler-based spin gapless semiconductors
HM SGS
Ti2CoSi
L21 structure Cu2MnAl-type XA structure
HgCu2Ti-type
Ti Co Si
Inverse Heusler
Generalized Slater-Pauling rule for inverse Heusler compounds
S. Skaftouros, K. Ozdogan, E. Sasioglu, I. Galanakis, Phys. Rev. B 87 024420 (2013).
Possible SGSs: Theoretical studies
Appl. Phys. Lett. 102 022402 (2013)
Phys. Rev. B 77 014427 (2008)
Phys. Rev. B 91 094409 (2015)
Possible SGSs: Experimental studies
Phys. Rev, Lett. 110, 100401 (2013)
Polycrystalline Mn2CoAl
Polycrystalline V3Al
Thin film Ti2MnAl Polycrystalline CrVTiAl
Phys. Status Solidi RRL 9 641 (2015) Phys. Rev. B 91 094409 (2015)
Appl. Phys. Lett. 121 053903 (2017)
Claudia Felser’s group
Topological materials in half-Heusler compounds
S. Chadov et al., Nature Materials 9, 541 (2010) Claudia Felser’s group
J. A. Logan et al., Nature Communications 9, 11993 (2016)
Band inversion
Topological materials in half-Heusler compounds
Hsin Lin et al., Nature Materials 9, 546 (2010)
Cava’s group
Evidence for topological behavior in half-Heusler compounds
“Observation of a topologically non-trivial surface state in half-Heusler PtLuSb (001) thin films”
J. A. Logan et al., Nature Communications 9, 11993 (2016)
“Large anomalous Hall effect in a half-Heusler antiferromagnet”
T. Suzuki et al., Nature Physics 12, 1119 (2016)
“Observation of unusual topological surface states in half-Heusler compounds LnPtBi (Ln=Lu, Y)”
Z. K. Liu et al., Nature Communications 7, 12924 (2016)
Topological materials in full-Heusler compounds
“Room-temperature magnetic topological Weyl fermion and nodal line semimetal states in half metallic Heusler Co2TiX (X=Si, Ge, or Sn)”
Guoqing Chang et al., Scientific Reports 6, 38839 (2016).
“Time-reversal-breaking Weyl fermions in magnetic Heusler alloys”
Zhijun Wang et al., Phys. Rev. Lett. 17, 236401 (2016).
Cava’s group
Single crystalline Co2ZrSn
Our group