e e k t bos z b - max planck societybemod12/slides/neugebauer_bemod12.pdf · mpie, dept....
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![Page 1: e E k T BOS Z B - Max Planck Societybemod12/Slides/Neugebauer_Bemod12.pdf · MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012 Do we have to go beyond](https://reader031.vdocuments.site/reader031/viewer/2022031405/5c41a4fb93f3c338b424b18a/html5/thumbnails/1.jpg)
MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Long time scale simulations to determine accurate ab initio free energies
Jörg Neugebauer, Blazej Grabowski, and Tilmann Hickel
Max-Planck-Institut für Eisenforschung, Düsseldorf, Germany Department of Computational Materials Design
?
{ }∑ −=
I
BBOS
R
TkEeZ
/
T [°
C]
C [wt.%] 0 0
400
800
1200
1 2 3
+
+
+
+
Partition function
Phase diagram
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Do we have to go beyond experiment? Calorimetric measurements
fcc Al fcc/bcc Mg
Fundamental input for all thermodynamic databases → But: Scatter of ~0.3 … 1 kB
Point defects (vacancies): Formation energies and entropies Al
Exp. DFT Ef (eV) 0.7 0.6 S (kB) 2.4 0.2
![Page 3: e E k T BOS Z B - Max Planck Societybemod12/Slides/Neugebauer_Bemod12.pdf · MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012 Do we have to go beyond](https://reader031.vdocuments.site/reader031/viewer/2022031405/5c41a4fb93f3c338b424b18a/html5/thumbnails/3.jpg)
MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Do we have to go beyond experiment?
Even chemical trends are hard to derive from existing data
Key quantity to design novel high-strength steels Additional complication → magnetism
Stacking fault energies (fcc Fe-Mn)
![Page 4: e E k T BOS Z B - Max Planck Societybemod12/Slides/Neugebauer_Bemod12.pdf · MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012 Do we have to go beyond](https://reader031.vdocuments.site/reader031/viewer/2022031405/5c41a4fb93f3c338b424b18a/html5/thumbnails/4.jpg)
MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Accuracy
Free energy difference between bcc and fcc iron
empirical potentials experiment
fcc bcc bcc
~1meV
Energy resolution better 1 meV! → Can we achieve such accuracy with present day ab initio techniques?
Comp. Mat. Sci. 41, 297 (2008)
![Page 5: e E k T BOS Z B - Max Planck Societybemod12/Slides/Neugebauer_Bemod12.pdf · MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012 Do we have to go beyond](https://reader031.vdocuments.site/reader031/viewer/2022031405/5c41a4fb93f3c338b424b18a/html5/thumbnails/5.jpg)
MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Ab initio Thermodynamics
Statistical averages over coordinates, magnetic moments, occupations, chemical compositions
{ }( )xTV
TkfZRE BiIIIBOS
exTVZ,,
/,...,,,),,( σ
−=
{ }( ){ } xTVfZR
TkfZRE
iIII
BiIIIBOS
e,,,...,,,
/,...,,,∑ −=σ
σ
{ }{ }{ }
xTVR
TkifIIZRE
I
Bfixed
IBOS
e,,
/,...,,;
∑
−
=
σ
Vibrational excitations
{ }{ }{ }
xTVf
TkIIZIRfE
i
Bfixed
iBOS
e,,
/,...,,;
∑
−
×σ
Electronic excitations
Adiabatic approximation
+ cross terms e.g. electron-phonon interactions
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Statistical averages with 1meV accuracy
Accuracy considerations
adiabnonmagT FFFFFFETVF −= ++++++= vacelahqh
K0),(
~0.1 meV/atom ~0.1 meV/atom
challenging < 1 meV/atom
( ) ( ){ }( )dttREt
TEtt
ttI
BOS
t∫∆+
=∞→∆ ∆=
0
0
1lim
a few hours/days 107 configurations (~ 10 temperature steps)
![Page 7: e E k T BOS Z B - Max Planck Societybemod12/Slides/Neugebauer_Bemod12.pdf · MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012 Do we have to go beyond](https://reader031.vdocuments.site/reader031/viewer/2022031405/5c41a4fb93f3c338b424b18a/html5/thumbnails/7.jpg)
MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Are contributions beyond quasiharmonic
approximation relevant?
![Page 8: e E k T BOS Z B - Max Planck Societybemod12/Slides/Neugebauer_Bemod12.pdf · MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012 Do we have to go beyond](https://reader031.vdocuments.site/reader031/viewer/2022031405/5c41a4fb93f3c338b424b18a/html5/thumbnails/8.jpg)
MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Free energy
Phonons
Expan- sion
Calphad GGA LDA Exp.
20
10
0
ω [
meV
] 0
-80
-160
-240
-320
-400
-480
F [m
eV/a
tom
]
200 400 600 800 T[K]
1.0
0.5
0
C P [
meV
/(K
atom
)]
0 300 600 T[K] 0 300 600
2
1
0
∆ x
[%]
Γ X K Γ L
Al
Example: Bulk (fcc) Aluminum
Heat capacity
Tmelting
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Can we use empirical potentials to describe
anharmonic contributions
How to sample over 107 configurations with
ab initio accuracy?
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Heat capacity of bulk Aluminum
200 400 600 800 T[K]
3.9
3.6
3.3
3.0
Hea
t ca
paci
ty [
k B]
Ab initio qh,el + Mishin et al.[1] ah
Ab initio qh,el + Ercolessi-Adams[2] ah
Ab initio qh,el + Mei-Davenport[3] ah
Ab initio quasiharmonic + electronic
Experiment[4]
None of the available empirical potentials is able to describe the anharmonic contribution
[1] Y. Mishin, et al., Phys. Rev. B 59, 3393 (1999). [2] F. Ercolessi and J. B. Adams, Europhys. Lett. 26, 583 (1994). [3] J. Mei and J. Davenport, Phys. Rev. B 46, 21 (1992). [4] D. A. Ditmars, et al., Int. J. of Thermophys. 6, 499 (1985).
Tmelting
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Coarse graining configuration space
Thermodynamic integration
( ) ( ){ }( )∑=N
iiI
BOS tREN
TU1
Main challenge: Reduce number of (ab inition) configurations by several orders of magnitude
from MD or MC
Two major concepts
Free energy perturbation
![Page 12: e E k T BOS Z B - Max Planck Societybemod12/Slides/Neugebauer_Bemod12.pdf · MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012 Do we have to go beyond](https://reader031.vdocuments.site/reader031/viewer/2022031405/5c41a4fb93f3c338b424b18a/html5/thumbnails/12.jpg)
MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Thermodynamic Integration
Key idea: Compute free energy change between reference system A and real system B
( ) ( )∫ ∂
∂=→∆
1
0
λλλ
λ
dUBAF ( ) ( )ABA UUUU −+= λλwith
0 2000 4000
12
11
10
9
8
Ener
gy [
meV
/ato
m]
MD steps
MD simulation in TI-step Application straightforward if good reference is available Typically the number of configurations can be reduced by 1-2 orders of magnitude → several 104 configurations Not affordable on highest ab initio level
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Free energy perturbation
Key idea: Compute free energy change between reference system A and real system B
( )AB
ABB Tk
EETkBAF
−−−=→∆ expln
Performance increases with quality of reference For large differences to reference the method becomes inefficient/ fails For the targeted accuracy less efficient than thermodynamic integration
P
{ }IR
A
B
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
How to boost coarse graining?
Cycles in thermodynamic integration ( ) ( )∫ ∂
∂=→∆
1
0
λλλ
λ
dUBAF
λ integration (2-10 steps)
Thermodynamic average (103…104 MD steps)
→ Improved ref. reduces step number
0 2000 4000
12
11
10
9
8
Ener
gy
MD steps
Performance bottleneck
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Solution
λ integration (2-10 steps)
Thermodynamic average (103…104 MD steps)
→ Improved reference reduces step number → Here: Quasiharmonic reference
0 2000 4000
12
11
10
9
8
Ener
gy
MD steps
→ Use free energy perturbation approach → Use low/medium converged DFT as reference
→ Typically reduces number of configurations by 102
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Performance of the new approach • Wavefunction extrapolation • Thermodyn. integr. (TI) with Langevin dynamics • Ensemble average instead of time average (parallelization) • Up-sampling in λ−ΤΙ step • etc.
0 2000 4000
12
11
10
9
8
Ener
gy [
meV
/ato
m]
MD steps
Low convergence parameters efficient calculation
MD simulation in TI-step
0 40 80 MD steps
16
15
14
13
12 Ener
gy [
meV
/ato
m]
High convergence parameters few MD steps
Up-sampling
uncorrelated
Grabowski et al., Phys. Rev. B79, 134106 (2009).
Required CPU time (logarithmic)
Molecular dynamics
Thermodyn. Integration UP-TILD
110
year
s
1.1
year
s
20 d
ays
Efficient coarse graining reduces number of configurations from 107 to a few 102 !
→ Opens the way to a fully ab initio determination of free energies
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Benchmark against experiment
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Thermal expansion coefficient
Excellent agreement with experiment Systematic trend: LDA and GGA provide approximate measure of error bars
Temperature (K)
Experiment
Thermal expansion coefficient of Al
F (V,T) = Fel(V,T)+Fqh(V,T) + Fqh,el(V,T) + Fah(V,T) + Fvac(V,T) + Fint(V,T)
Grabowski,Ismer, Hickel, Neugebauer, Phys. Rev. B 79, 134106 (2009)
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Heat Capacity
DFT gives lower bound to all recent experiments
F (V,T) = Fel(V,T)+Fqh(V,T) + Fqh,el(V,T) + Fah(V,T) + Fvac(V,T) + Fint(V,T)
Heat capacity of Al
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Applications
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Assessment of experimental data
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Calcium: Heat capacity
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Calcium: Heat capacity
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Newly developed approaches allow to systematically improve performance of DFT to describe finite temperature properties
Ab initio thermodynamics (Conclusions)
Accuracy often exceeds experimental data even of stable phases
→ Provide excellent basis to compute thermodynamic data
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Thanks to the department
CM Department (2011)
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MPIE, Dept. Computational Materials Design BEMOD, Dresden, March 26 - 29, 2012
Thanks for your attention