order - disorder phase transitions in metallic alloys
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Order - Disorder Phase Transitions in Metallic Alloys. Ezio Bruno and Francesco Mammano , Messina, Italy. collaborations: Antonio Milici , Leon Zingales (Messina) Yang Wang (Pittsburg). - PowerPoint PPT PresentationTRANSCRIPT
Order-Disorder Phase Transitions in Metallic Alloys
Ezio Bruno and Francesco Mammano, Messina, Italy
collaborations:
Antonio Milici, Leon Zingales (Messina)
Yang Wang (Pittsburg)
Bronze Age little statue from Olimpia (Greece)
Bronze Age helmet probably from Magna Grecia (Souther Italy).
The dawn of metallurgy coincides with the beginning of human history. In the earl Bronze Age, metallic alloys technologies brought new efficient tools thus permitting the development of agriculture and towns. The availability of sufficient food and the henceforth born complex social organization freed the people from the necessity of hunting for surviving and allowed the discovery of writing. Since then, almost any human handcraft is made of metallic alloys.
The development of new technologies in high-tech areas, such as medical prosthesis or jet engines, requires a careful design of alloys mechanical properties. The determination of the phase diagrams is crucial to this purpose since the performances of alloys are strongly influenced by the various crystalline phases of which they are made.
fcc, disordered ’ fcc, ordered bcc, ordered
A new experimental method for alloy phase diagrams measurements [Zhao, J.-C. Adv. Eng. Mater. 3, 143 (2001)]
A
B
Metallic alloys
Fixed “geometrical” lattice
Different chemical species
SRO
Warren-Cowley Short-Range Order Parameter
random alloys
ordered compoundssegregation
-1 1
ordereddisorderedsegregated
0
TE
MP
ER
AT
UR
Ehigh
low
need for a theory
• ab initio
• finite T
• able to deal with metallic alloys (regardless of the ordering status)
• able to make quantitative predictions about ordering or segregation
• should contain the electronic structure
SRO vs. T
phase diagrams
Existing schemes strenghts problemsPerturbative theories
based on CPA
(Concentration waves, GPM)
Spectral properties electrostatics
perturbative
Theories based on effective Ising Hamiltonians
(Connolly-Williams, CVM)
convergence
(how many clusters?)
iiii kVqa -0.2
-0.1
0
0.1
0.2
-0.2 -0.1 0 0.1 0.2
ZnCu
V
q
Cu0.50Zn 0.50 bcc
1024 atoms sample simulating a random alloy
‘qV’ laws
ai , ki aA , kA if the site i is occupied by a A atom
aB, kB if the site i is occupied by a B atom
ieli Zrrdqi
j
jiji qMV 2
Faulkner, Wang &Stocks, 1995LSMS Density Functional theory calculations
The distribution of chargesin random alloys is
continuous
bcc random Cu0.50Zn0.50
•To date ‘qV’ laws are only a numerical evidence, i.e. a proof within DFT is still missing.
•Deviations from ‘qV’ laws (if any) are not larger than numerical errors in LSMS or LSGS, at least for the systems already investigated.
•Not clear wether or not ‘qV’ laws are due to the approximations made (spherical potentials, LDA)
•Arbitrariety in the choice of the crystal partition in ‘atomic volumes’,
However : Different partitions (e.g. like in Singh &
Gonis, Phys. Rev. B 49, 1642 (1994) ) always lead to linear ‘qV’ laws (actual values of the coefficients are a function of the chosen partition, see Ruban & Skriver, Phys. Rev. B 66, 024201 (2002) )
ieli Zrrdqi
i
It is possible to obtain the qV laws using a Coherent Potential Approximation that
includes Local Fields (CPA+LF)
[Bruno, Zingales & Milici, Phys. Rev. B. 66, 245107, (2002)]
CPA+LF analysis of ‘qV’ laws
CPA+LF simulates the Madelung field V by an external field that is non zero only within the impurity site
aA, aB are related to the response of the impurity sites to
kA, kB are not independent:
at =0 a q0 =k
global electroneutrality implies cA q0A +cB q0
B =0
iiii kVqa
kA- kB is related to some
electronegativity difference
Charge Excess Functional (CEF) theory
Linear ‘qV’ laws
iiii kVqa
j
jiji qMV 2
Ground state charge excesses satisfy the linear eqs.
ij jijii kqMqa 2
Can be derived from a functional quadratic in the qi
E. Bruno, III International Alloy Conference, Estoril (2002)E. Bruno, L. Zingales and Y. Wang, Phys. Rev. Lett. 91, 166401 (2003)
q , 1
2ai qi bi 2
i Mij qi q j
ij qi
i
Charge Excess Functional (CEF) theory
E. Bruno, III International Alloy Conference, Estoril (2002)E. Bruno, L. Zingales and Y. Wang, Phys. Rev. Lett. 91, 166401 (2003)
Linear ‘qV’ laws
iiii kVqa
j
jiji qMV 2
Ground state charge excesses satisfy the linear eqs.
ij jijii kqMqa 2
Charge electroneutrality
qii 0
q , 1
2ai qi bi 2
i Mij qi q j
ij qi
i
Charge Excess Functional (CEF) theory
Linear ‘qV’ laws
iiii kVqa
j
jiji qMV 2
Ground state charge excesses satisfy the linear eqs.
ij jijii kqMqa 2
E. Bruno, III International Alloy Conference, Estoril (2002)E. Bruno, L. Zingales and Y. Wang, Phys. Rev. Lett. 91, 166401 (2003)
q , 1
2ai qi bi 2
i Mij qi q j
ij qi
i
Charge Excess Functional (CEF) theory
Linear ‘qV’ laws
iiii kVqa
j
jiji qMV 2
Ground state charge excesses satisfy the linear eqs.
ij jijii kqMqa 2
Madelung Energy
E. Bruno, III International Alloy Conference, Estoril (2002)E. Bruno, L. Zingales and Y. Wang, Phys. Rev. Lett. 91, 166401 (2003)
q , 1
2ai qi bi 2
i Mij qi q j
ij qi
i
Charge Excess Functional (CEF) theory
Linear ‘qV’ laws
iiii kVqa
j
jiji qMV 2
Ground state charge excesses satisfy the linear eqs.
ij jijii kqMqa 2
“Elastic” local charge relaxation energy
E. Bruno, III International Alloy Conference, Estoril (2002)E. Bruno, L. Zingales and Y. Wang, Phys. Rev. Lett. 91, 166401 (2003)
i
iij
jiiji
iii qqqMbqaq 2
21
,
ai qi bi 2 Mij q jj
qii 0
The Charge Excess Functional (CEF):
Euler-Lagrange equations:
‘qV’ laws: ai qi + Vi = ki
Charge electroneutrality
j
jiji qMV 2
iii kba E. Bruno, III International Alloy Conference, Estoril (2002)E. Bruno, L. Zingales and Y. Wang, Phys. Rev. Lett. 91, 166401 (2003)
bcc random Cu0.50Zn0.50
Ab initio calculations
CEF calculations
CEF-CPA calculations
• The CEF provides the distribution of local charge excesses and the electrostatics of metallic alloys regardless of the amount of order that is present. Differences with respect to LSMS are comparable with numerical errors.
• CEF parameters (3 for a binary alloy) depend on the mean alloy concentration only. Hence they can be calculated for one supercell and used for any other supercell at the same mean conc.
• The CEF is based on a coarse graining of the electronic density, (r), i.e.: electronic degrees of freedom are reduced to one for each
atom, the local charge excess qi.
• The CEF theory is founded on the ‘qV’ laws. Need for understanding the limits of their validity.
• What is the relationship between the ‘true’ energy (e.g. from Kohn-Sham calculations) and the value of the CEF functional at its minimum ?
j
jijiiMAD qMq,
CEF predictions:
By eliminating the Madelung terms via the Euler-Lagrange equations:
qqba
ii ,, 2
i
jijiiii
i qMqbqa 2
2
ij
jiiji
iiiTOT qqMbqaqE 2
21
,
“local energies” linear vs. local charge excesses
-3.665
-3.655
-0.2 -0.1 0charge shifts q
i (a.u.)
Eig
enva
lues
(R
yd.) bcc
fcc
Pd 4p3/2 core statesin Cu0.5Pd0.5 alloysbcc (2 samples) and fcc (3 samples)
PCPA calculations
[Ujfalussy et al.,Phys. Rev. B 61, 12005
(2000)]
-0.02
0
0.02
0.04
-0.1 0 0.1
Ei-E
i,Mad
Ei,Mad
Ei
qi (a.u.)
r=0.99998
PCPA calculations for Cu0.50 Pd0.50
Within LDA and CPA-based theories for alloys of specified mean at. concentration all the site-diagonal electronic properties are unique functions of
the site chemical occupation, Z, and of the Madelung potential Vi.
It follows that once the functional forms are determined (e.g. from PCPA
calculs.) the knowledge of the distribution of the Vi (e.g. from CEF calculs.) is
sufficient to determine any site-diagonal electronic property.
PCPA on sample A
CEF coefficients
CEF on sample B
Oi= O(Vi) p(V)
properties of sample B
rrr
rr i
LDAi
i
ii
Vde
Vr
ZerW
i
,,,2
2
,
Ei,t
EEE CCF Gt
ri,
j
iijiii qMeVq 2, r
Kohn-Sham eff. potential
s.s. scattering matrices
Fermi level,
CPA coherent medium
ITE
RA
TIO
NS
0 1
ordereddisordered
A
B
SROWarren-Cowley Short-Range Order Parameter
Random alloys
Intermetallic compounds
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
0 1
ordereddisordered
Order-Disorder phase transition
SRO
0
50 CuZn
Cou
nts
q0-0.2 0.2
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
T=10 KSRO=1
0 1
ordereddisordered
0
50
CuZn
Cou
nts
q0-0.2 0.2
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
T=300 KSRO=0.95
0 1
ordereddisordered
0
CuZn
Cou
nts
q0-0.2 0.2
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
T=400 KSRO=0.67
0 1
ordereddisordered
0
10 CuZn
Cou
nts
q0-0.2 0.2
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
T=430 KSRO=0.48
0 1
ordereddisordered
0
10 CuZn
Cou
nts
q0-0.2 0.2
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
T=450 KSRO=0.34
0 1
ordereddisordered
0
10
CuZn
Cou
nts
q0-0.2 0.2
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
T=800 KSRO=0.15
0 1
ordereddisordered
0
10
CuZn
Cou
nts
q0-0.2 0.2
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
T=3200 KSRO=0
0 1
ordereddisordered
0
0.05
0.09
0.1
0.11
0.12
0.13
0.14
0
0.25
0 0.5 1(1/2,1/2,1/2)
<q>
<2q>
<q>2
<3q>
<q>3
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
SRO(1/2,1/2,1/2)
T
Moments of the charge distributions vs. SRO
0
50 CuZn
Cou
nts
q0-0.2 0.2
0 1
ordereddisordered
0
10
CuZn
Cou
nts
q0-0.2 0.2
Charge polydisperse Charge monodisperse
Summary
1. The CEF theory constitutes a simple, very realistic model for the energetics of metallic alloys
2. The CEF can be regarded as a coarse grained density functional ((r) qi). If the CEF parameters are extracted from PCPA
calculations, then the energy from CEF coincide with total electronic energy from the PCPA theory.
3. A MonteCarlo-CEF algorithm allows for the study of order-disorder phase transitions.
0
0.1
Cu-Cu
0
0.1
Zn-Zn
0
0.1
0.2
0 2 4 6
Cu-Zn
Nor
mal
ised
fre
quen
cyDistribution of interaction energies for nearest neighbours
ji
jiijM qqME,
R ijij RR
M
1
Madelung energy
2q
qq jiij
Interaction strength for the (i,j) pair
0
0.1
Cu-Cu
0
0.1
Zn-Zn
0
0.1
0.2
0 2 4 6
Cu-Zn
Nor
mal
ised
fre
quen
cyDistribution of interaction energies for nearest neighbours
ji
jiijM qqME,
R ijij RR
M
1
2q
qq jiij
The variation of has effects similar to the variation of R in
ionic glasses
Charge correlations in random alloys
-1
-0.5
0
0 0.5 1
ij=<q
iq
j>/<q>2
(1/2,1/2,1/2)
(1/2,1/2,1/2)
bcc random Cu0.50Zn0.50
Zn n1=4
bcc random Cu0.50Zn0.50
Zn n1=4n2=3
Zn n1=4
bcc random Cu0.50Zn0.50
Zn n1=4n2=3
Zn n1=4