AB INITIO-BASED MEAN FIELD THEORY OF SITE OCCUPATION IN BINARY SIGMA PHASES
E. Kabliman
OU
TL
INE
2
1. Introduction: 1. Binary Ο-phases
2. Fe-Cr phase diagram
3. Magnetic properties
4. Ο-phase structure
5. Aim
2. Ab initio-based mean field theory: 1. Helmholtzβs free energy
2. Total energy expansion
3. EMTO-CPA
4. Convergence of total energy expansion
5. Entropic contributions
6. Site occupancies
3. Results [FeCr]: 1. Effect of magnetic state
2. Structural variations
3. Final site distribution
4. Results [other Ο-phases]: 1. ReW
2. CoCr
3. FeV
5. Summary
3
Ο-phase (light plates). Nicrofer 3127. after annealing at 700ΠΎ Π‘ during 6000 hours
Ο-phase formation = technological problem
J.L. Garin and R.L. Mannheim. J. Mat. Prog. Tech. 209, 3143 (2009)
J. VΕestal et al. Comp.Mat.Sc. 38, 298 (2006)
Ο-phase : β’ has a lamellar morphology β’ nucleates near grains boundaries (concentration of elements, e.g. Cr and Mo, is favorable) and on carbide particles
PROBLEM of Ο-phase precipitation : β’ decreases ductility and corrosion resistance β’ increases brittleness and cracks formation
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
4
Ο-phase in binary alloys
β’ atomic radii of the alloy components must be similar β’ Fe-Cr system has the smallest VF at room T.
V.N
. B
yko
v an
d V
.A.
So
lovβ
ev: Z
hu
rn.
Str
uk
t. K
him
ii V
ol.
5 N
o. 2
, 28
8 (
196
4)
VF=βr/rav r β atomic radii
β’ room T: 8 of 41 systems has VF > 8% β’ elevated T: 2 of 41 systems has VF > 8%
In binary Ο-phases VF β€ 8 %
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
5
Fe-Cr phase diagram
HISTORY :
β’ 1923 Bain: A hard and nonmagnetic phase in Fe-Cr [Chem. Met. Eng. 28 (1923)]
β’ 1943 Cook, Jones: Crystal structure of Ο-phase [J. Iron Steel Inst. London 148
(1943)]
β’ At present: Ο-phase is found in more than 40 systems (Cr-Fe, Cr-Co, V-Fe, etc.)
4
brittle Ο-phase
Phase decomposition
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
6
Magnetic properties
J. Cieslak, M. Reissner et al. Phys. Stat. Sol. (a) 205, No. 8 (2008)
[ TC measured only in Fe-Cr and Fe-V ]
Fe1-xCrx
Fe1-xCrx
Ave
rage
Β΅ p
er F
e at
om
C
uri
e te
mp
erat
ure
1. Introduction:
1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
7
Site ncoord nmult
(Wyck.pos.) x
at 923 K y
at 923 K z
at 923 K Emprical scheme
A 12 2(a) 0 0 0 (Mn,Fe,Co,Ni)
B 15 4(f) 0,39864(4) 0,39864(4) 0 (Ti,V,Cr,Mn,Mo)
C 14 8(i) 0,46349(4) 0,13122(4) 0 mixed
D 12 8(i) 0,73933(4) 0,06609(4) 0 (Mn,Fe,Co,Ni)
E 14 8(j) 0,18267(3) 0,18267(3) 0,25202(9) mixed
1. H.L. Yakel. Acta Cryst. B 39, 20 (1983) 2. J. S. Kasper, R. M. Waterstrat. Acta Cryst. 9, 289 (1956)
Ο-phase structure
Fe1-xCrx for x = 0.495, a = 0.87968 nm, c/a = 0.518. ncoord β site coordination numbers; nmult β site multiplicities
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
8
Aim
J. Cieslak, M. Reissner et al. Phys. Stat. Sol. (a) 205, No. 8 (2008)
Determine atomic site distribution in disordered Ο-phase as a function of T and x
Experiment β’ lack of data: site occupancies only at few T and x β’ difficulties:
β’ long annealing times and purity of a sample β’ Fe and Cr: similar X-ray scattering factors
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
Sigma-phase is a substitutionally disordered solid solution in paramagnetic state;
It has a low symmetry structure with undefined βexactβ atom-site correspondence;
How to describe electronic structure and total energy of such a system?
9
SUBSTITUTIONAL DISORDERED SYSTEMS
Methods for total energy calculations
Supercells approach: straightforward method, use of big periodic supercells
Cluster expansion formalism: expansion of total energies in terms of the effective cluster interactions (strucutre inversion method)
Special quasirandom structures: reproduce the most relevant radial correlation functions of an infinite random structure
Methods for electronic structure calculations
Virtual crystal approximation: real disordered system is replaced by an virtual one-component one
Coherent potential approximation: provide the same scattering properties of the one-component effective medium as the average of alloy components, embedded in this effective medium
Locally self-consistent Greenβs function: introduction of local interaction zone around every atom, inside which an atom βfeelsβ ist real local environment, but outside βseesβ only the CPA effective medium
EMTO-CPA
Some of slides on EMTO-CPA were kindly provided by Prof. A. Ruban (KTH, Sweden)
ATOMIC SPHERES METHODS
β’ Augmented plane waves (APW)
β’ Muffin-tin orbitals (MTO) ASA, exact MTO (EMTO)
β’ Linearized APW and MTO (LAPW and LMTO)
β’ (Linearized) augmented plane wave method ((L)APW) + local orbitals
β’ Full-potential LAPW and LMTO methods
β’ Various Greenβs function method (KKR, KKR-CPA, etc)
Fig. 2.1
13
Partial wave Back-extrapolated partial wave Screened spherical wave
Kinked partial wave or exact muffin-tin
orbital
SSW Partial wave
BPW
They are basis functions of the EMTO method
The solution of the Kohn-Sham equation is then given by
Their linear combination:
A. Ruban
Applications of the EMTO method: advantages
and disadvantages
The EMTO is the method to calculate electronic structure and
total energies of ordered and random alloys as in the bulk as
well as at surfaces and interfaces .
As soon as the total energy is obtained, it can be used for
calculations of different thermodynamic properties, like
enthalpies of formation, solution, segregation, ordering
energies and so on.
It can be also used for calculations of the elastic properties:
in most cases there is very little information about elastic
constants of alloys.
A. Ruban
Metals and alloys in the paramagnetic state
Paramagnetic state in magnets is usually due to randomly
oriented spin magnetic moment on atoms.
Theoretically it can be presented by the so-called disordered
local magnetic moment (DLM) model, in which such a system
considered as equiatomic random alloy of atoms with spin-up
and spin-down orientation.
It is extremely difficult (close to impossible at the present
time) to treat alloys in the DLM state using such methods as
VASP, where a supercell approach is required. However, this
is extremely easy in the case of EMTO, where such a random
alloy is treated using coherent potential approximation (CPA).
A. Ruban
Greenβs function
SchrΓΆdinger (Kohn-Sham) equation
A. Ruban
Coherent potential approximation (CPA)
(isomorphous single-site approximation)
Since wave function is not self-averaging quantity, the Greenβs
technique be used in order to have a consistent theory.
In the CPA random alloy is substituted
by perfectly ordered (CPA) effective
medium, whose scattering properties
satisfy the condition:
These non-linear equations are solved self-consistently A. Ruban
AB INITIO BASED MEAN FIELD THEORY
19
20
Ab initio based mean field theory :
πΉ = πΈπ‘ππ‘ β ππ
π»ππππ = πΈ0 + πβ(1)πΏππΌ ,π
ππΌ=1,5
+1
2 πβπ½ ,π
(2)πΏππΌ ;ππΏππ½ ;π
π ,πβπππΌ ,π½=1,5
+1
3 πβπ½πΎ ,π‘
(3)πΏππΌ ;ππΏππ½ ;ππΏππΎ ;π
π ,π ,πβπ‘π‘πΌ ,π½ ,πΎ=1,5
+ β―
πΏππΌ ,π = ππΌ ,π β ππΌ ,π€βπππ ππΌ β‘ ππΌ ,π πππ ππΌ .π = 1 ππ πΆπ ππ‘ π ππ‘π π
πΈπ‘ππ‘ ππΌ = πΈ0 π₯ + ππΌ π½πΌ 1 ππΌ
4
πΌ=1
.
ππΌ β π ππ‘π ππ’ππ‘πππππππ‘π¦, ππΌ β πΆπ π π’ππππ‘π‘πππ ππππ’πππππ¦
π½πΌ 1
= ππΈπ‘ππ‘πππΌ
βππΈπ‘ππ‘πππΈ
|ππΌ=π₯=ππππ π‘
Helmholtzβs free energy
β’ JΞ±(1) are relative effective chemical potentials at given x, which describe
preference of Cr atoms to occupy site Ξ± with respect to site E.
β’ JΞ±(1) are indeed enough to calculate Cr site occupancies.
Fe1-xCrx
Effective on-site interactions with respect to the E site
IDEA :
site sublattice
pairs
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
21
Total energy expansion
Problem of CW method: Number of different pair ECI just within a polyhedron of closest sites is 20, while number of non-equivalent multi-site interactions is much larger even within such short distances.
π»ππππ = πΈ0 + πβ 1 πΏππΌ,π
ππΌ=1,5
+1
2 πβπ½,π
2 πΏππΌ;ππΏππ½;π
π,πβπππΌ,π½=1,5
+1
3 πβπ½πΎ,π‘
3 πΏππΌ;ππΏππ½;ππΏππΎ;π
π,π,πβπ‘π‘πΌ,π½,πΎ=1,5
+β―
Fe1-xCrx
~ 130 atoms
bcc : i = 2-3 fcc : i = 1-2 Ο-A : i = 3 Ο-B : i = 6 Ο-C : i = 8 Ο-D : i = 8 Ο-E : i = 9
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
22
Effective pair cluster interactions
Free energy of Ο-phase can be quite accurately presented in terms of concentration-independent cluster interactions
Dominating terms in this expansion can be on-site interactions
Single-site mean-field approximation will be sufficient to provide a reasonably accurate description of configurational effects at high temperatures
xCr=0.5 xCr=0.6
SGPM
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
23
Effective on-site interactions
πΈπ‘ππ‘ ππΌ = πΈ0 π₯ + ππΌ π½πΌ 1 ππΌ
4
πΌ=1
ππΌ β π ππ‘π ππ’ππ‘πππππππ‘π¦, ππΌ β πΆπ π ππ‘π ππππ’πππππ¦
π5 =30
π5β
1
π5 ππΌππΌ
4
πΌ=1
π½πΌ 1 =
ππΈπ‘ππ‘πππΌ
βππΈπ‘ππ‘πππΈ
|ππΌ=π₯=ππππ π‘
β’ JΞ±(1) are relative effective chemical potentials at given x,
which describe preference of Cr atoms to occupy site Ξ± with
respect to site E.
β’ Etot are found in coherent potential approximation (CPA)
implemented on exact muffin-tin orbitals (EMTO) method
in order to simulate disordered atomic distribution in Ο-phase.
Fe1-xCrx
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
No local environment effects LSGF
No local atomic relaxations Wien2k
24
Check of Coherent Potential Approximation
Locally self-consistent Greenβs function technique
2 supercells (SC1 and SC2) = (4x4x4) of 1920 atoms
Local interaction zone = polyhedron of the nearest neighbors for every site (A,B,C,D,E)
CPA results are in a very good agreement with those of LSGF calculations for supercells
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
25
Check of EMTO and local atomic relaxations
Etot is calculated by: β’ full-potential linearized augmented plane wave + local orbitals method (WIEN2k code) β’ exact muffin-tin orbitals method (EMTO code)
Site Exp. [1] 923 K
Final 0 K
A 0.125 Cr 0.0 Cr
B 0.750 Cr 1.0 Cr
C 0.625 Cr 0.375 Cr
D 0.163 Cr 0.0 Cr
E 0.663 Cr 1.0 Cr
1. H.L. Yakel, Acta Cryst. B 39, 20 (1983) 2. A. Zubkov and B.Mogutnov, Dokl. Ak. Nauk SSSR 311, 388 (1990) 3. D. Read and E. Thomas, J. Phys. Chem. Sol. 29, 1569 (1968)
Calculated (WIEN2k)
Measured
a 0.86433 nm 0.87968 nm [1]
c/a 0.518 0.518 [1]
Ef 5 kJ/mol 6.5 kJ/mol [2]
ΞΌ 0.53 ΞΌB 0.20 ΞΌB [3]
Site relaxations < 0.1 kJ/mol
[Good agreement ]
Fe0.5Cr0.5
limit of CPA
β’ EMTO and Wien2k obtain the same equilibrium (final) atomic distribution
β’ Site relaxations in Ο-FeCr are negligible
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
26
Convergence of total energy expansion
πΈπ‘ππ‘ ππΌ = πΈ0 π₯ + ππΌ π½πΌ 1 ππΌ
4
πΌ=1
+ ππΌππ½ π½πΌπ½ 2 ππΌππ½
4
πΌ ,π½=1
π½πΌ 1
= ππΈπ‘ππ‘πππΌ
βππΈπ‘ππ‘πππΈ
|ππΌ=π₯=0.5
Mean least-squares fit π± πΆ π
: 89 various Ο-phase configurations
for x = 0.50 in DLM state
ECI A B C D E
π½ πΌ 1
16.0951 0.8670 1.4796 15.4150 0
JΞ±(1) 16.4062 0.4688 1.7812 14.3438 0
π½ πΌπ½ 2
A B C D E
A -1.1983 -0.3714 -0.6475 -0.4568 0
B -0.4896 -0.3899 -0.4631 0
C -0.5680 -0.4065 0
D -0.6397 0
E 0
β’ π½ πΌ 1 : root-mean-square error ~ 0.2 mRy/atom
β’ π½ πΌ 1
+ π½ πΌπ½ 2 : root-mean-square error ~ 0.2 mRy/atom
β’ Total energies calculated without/with effective pair interactions π½ πΌπ½ 2
are similar
β’ Chemical potentials JΞ±(1) reproduce well the on-site interactions from
mean least squares fit π½ πΌ 1
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
πΉ = πΈπ‘ππ‘ β π(πππππ + πππππ + ππ£πππ )
πππππ = βππ΅ πβ πβ ln πβ + 1 β πβ ln 1 β πβ
5
πΌ=1
πππππ = ππ΅ πβ[
5
πΌ=1
πβ ln ππΌπΆπ + 1 + 1 β πβ ln ππΌ
πΉπ + 1 ]
ππ£πππ = πππππππ‘ππ
27
Entropy contributions to free energy
Magnetism:
β’ In order to simulate paramagnetic state
at finite T disordered local moment
(DLM) state is used.
β’ Longitudinal spin fluctuations (LSF)
are high temperature magnetic excitations
and induce modified spin magnetic
moments on the alloy components.
{ DLM + LSF }
Site DLM Β΅(Fe)
DLM Β΅(Cr)
+LSF Β΅(Fe)
+LSF Β΅(Cr)
A 0.0 0 0.89 0.28
B 1.45 0 1.63 0.43
C 1.26 0 1.48 0.34
D 0.04 0 1.06 0.32
E 0.82 0 1.09 0.32
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
Ο 28
P. Korzhavyi et al. Mat. Res. Soc. Symp. Proc. V 842, S4.10.1 (2005)
H at 0 K
H
H β TSconf
H β T(Sconf+Smagn)
at 1000 K
Approach : 32 ordered (end-member) configurations and DLM model
Importance of magnetism 1. Introduction:
1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
ππΉ
πππΌ=ππΈπ‘ππ‘πππΌ
β π ππππππ
πππΌ+ππππππ
πππΌ = 0
π5 =30
π5β
1
π5 ππΌππΌ
4
πΌ=1
ππΉ
πππΌ= π½πΌ
1 ππΌ + ππ΅πππΌ ππππΌ β ππ 1 β ππΌ
β ππ΅πππΌ πππ5 β ππ 1 β π5 +ππ΅πππΌ ππ ππΌπΉπ + 1
β ππ΅πππΌ ππ π5πΉπ + 1 β ππ΅πππΌ ππ ππΌ
πΆπ + 1
+ππ΅πππΌ ππ π5πΆπ + 1
29
Equilibrium site occupancies cΞ±
πβ =ππΆ
π + πβ
where
πβ = π β
1ππ΅
π½β 1
π5
1 β π5
(π5πΉπ + 1)
(ππΌπΉπ + 1)
(ππΌπΆπ + 1)
(π5πΆπ + 1)
(by Cr atoms)
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
30
Effect of magnetic state on site occupations
Fe0.5Cr0.5
B
B (A,D)
Effective on-site interactions JΞ±
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
T β 0 K : integer site occupation is defined by Etot and described by the effective on-site interactions JΞ±. high T : partial site occupation is driven by Sconf, while Smagn corrects cΞ± in (A,D) and B due to proper account of magnetism
31
Structural variations and ¡α (T)
V expansion : increases available space around (A,D) and occupation by large Cr β not favored β distortion within kagome layers. c/a expansion : decreases available space around E and increases around C.
T dependence of ¡α(Fe,Cr) Jα
Structural parameters
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
32
Final site distribution vs T
β’ Preferences in atomic site distribution according to the empirical scheme of ordering
β’ Good agreement with experimental data at finite T and results obtained by Wienk at T = 0 K
Fe0.5Cr0.5
Including all effetcs (magnetism, structural changes and T effects)
Site Emprical scheme
A (Mn,Fe,Co,Ni)
B (Ti,V,Cr,Mn,Mo)
C mixed
D (Mn,Fe,Co,Ni)
E mixed
Wie
n2k
1. Introduction:
1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
33
Previous work
32 = 25 end-member compounds (total energy by LMTO-ASA)
24 effective cluster interactions were calculated by Connoly-Williams method
Magnetism was neglected
Results at high T disagree with experiment
Results at T = 0 K disagree with Wien2k
Site occupancy
M.H.F. Sluiter et al. PRL75 , 3142(1995)
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
34
Final site distribution vs x
β’ Linear dependence of the site occupancies on composition x β’ Good agreement with experimental data
EK, P.Blaha, K. Schwarz, A.V. Ruban, B. Johansson, PRB 83, 092201 (2011)
Fe1-xCrx
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
35
Test : Re0.5W0.5 system β(AR) = 2 pm
β’ Preferences in atomic site distribution according to the empirical scheme of ordering
β’ Reverse occupation of C and E site in contrast to Fe-Cr β’ Agreement with the earlier published work
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
Site Emprical scheme
A (Mn,Fe,Co,Ni)
B (Ti,V,Cr,Mn,Mo)
C mixed
D (Mn,Fe,Co,Ni)
E mixed
C. Berne et al. PRB64 ,144103 (2001)
36
Test : Co0.5Cr0.5 system β(AR) = 3 pm
β’ Preferences in atomic site distribution according to the empirical scheme of ordering
β’ Site occupation similiar to the Fe-Cr system
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
Site Emprical scheme
A (Mn,Fe,Co,Ni)
B (Ti,V,Cr,Mn,Mo)
C mixed
D (Mn,Fe,Co,Ni)
E mixed
37
πΉ = πΈπ‘ππ‘ β π(πππππ + πππππ + ππ£πππ )
πΈπ‘ππ‘ ππΌ = πΈ0 π₯ + ππΌ [ π½πΌ 1
+ π½πΌ πππππ₯
]ππΌ
4
πΌ=1
ππΌ β π ππ‘π ππ’ππ‘πππππππ‘π¦, ππΌ β π π ππ‘π ππππ’πππππ¦
π½πΌ 1
= ππΈπ‘ππ‘πππΌ
βππΈπ‘ππ‘πππΈ
|ππΌ=π₯=ππππ π‘
π½πΌ πππππ₯
= πΈπππππ₯ /ππ‘ππ
Effective on-site interactions VΞ±(1)
with respect to the E site
Fe0.5V0.5: local atomic relaxations β(AR) = 8 pm
ECI A B C D E
JΞ±(1) 24.0938 -7.7813 0.3750 19.8750 0
JΞ±(1) +JΞ±
(relax) 21.9375 -7.4062 0.3750 18.1875 0
EMTO-CPA
β’ Contributions from local atomic relaxations to effective on-site interactions in Fe-V are small
β’ Contributions in other systems with β(AR) β€ 8 pm are expected to be also negligible
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
38
Test : Fe-V system β(AR) = 8 pm
β’ Preferences in atomic site distribution according to the empirical scheme of ordering
β’ Nearly full occupation of (A,D,) and B in contrast to Fe-Cr system [due to bigger β(AR)]
Site Emprical scheme
A (Mn,Fe,Co,Ni)
B (Ti,V,Cr,Mn,Mo)
C mixed
D (Mn,Fe,Co,Ni)
E mixed
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
39
Test : Fe-V system β(AR) = 8 pm
β’ Linear dependence of the site occupancies on composition x β’ Reasonable agreement with experimental data β’ With increase of β(AR) full occupation of sublattices is more
pronounced
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
40
Summary :
Ab initio based mean field theory was suggested to calculate the Cr site occupancies in the Fe-Cr Ο-phase.
4 effective on-site interaction parameters are enough to simulate the atomic site distribution in Ο-phase
The calculated Cr site occupancies are in a good agreement with the results obtained by the FP-LAPW method (WIEN2k) at T = 0K and available experimental data at finite T.
It was shown that the Fe-Cr Ο-phase exhibits a non-trivial magnetic behaviour at high T, which affects the site occupation by Fe and Cr atoms. The structural variation (volume and c/a) can lead to an additional atomic redistribution.
The proposed method works also for the other binary Ο-phases. In particularly, Re-W, Co-Cr, Fe-V systems have been tested and results agree with empirical scheme of ordering.
The proposed method can be further applied for the ternary Ο-phases.
1. Introduction: 1. Binary Ο-phases 2. Fe-Cr phase-diagram 3. Magnetic properties 4. Ο-phase structure 5. Aim
2. Ab initio MF theory:
1. Helmholtβz free energy 2. Total energy expansion 3. EMTO-CPA 4. Convergence of expansion 5. Entropic contributions 6. Site occupancies
3. Results [FeCr] : 1. Effect of magnetic state 2. Structural varitations 3. Final site distribution
4. Results [other Ο-s] : 1. ReW 2. CoCr 3. FeV
5. Summary
AC
KN
OW
LE
DG
EM
EN
TS
41
Prof. A. V. Ruban Applied materials Physics Department of Materials Science and Engineering The Royal Institute of Technology (KTH) BrinellvΓ€gen 23, SE-100 44 Stockholm, Sweden
Prof. P. Blaha Prof. K. Schwarz Institute of Materials Chemistry, Vienna University of Technology Getreidemarkt 9/165-TC, A-1060 Vienna, Austria
and WIEN2k group