Adequacy of the Classical Potentials for the study of...
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Adequacy of theClassical Potentials
for the study ofThermodynamic Propertiesof Transition Metal Clusters
Zacharias G. Fthenakis���, Antonis N. Andriotis�
�Institute of Electronic Structure and Laser - FORTH
�Department of Physics, University of Crete
Talk – p.1
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Talk – p.2
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Talk – p.3
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Talk – p.4
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Talk – p.5
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Talk – p.6
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� Lennard - Jones
� Morse
� Erkoc I
� Cleri - Rosato
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� Erkoc II, Erkoc III
� Uppenbrink - Wales
� EAM (Johnson, ...)Annual Reviews of Computational Physics IX - edited by
Dietrich Stauffer - World Scientific - 2001
S. Erkoc - Empirical Potential Energy Functions Used in the
Simulations of Material Properties
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Talk – p.8
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0 1000 2000 3000Temperature (
oK)
0
0.1
0.2
0.3
0.4
0.5
Ene
rgy
(eV
)
Energy per atom for the Ni3 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IIJohnson
Talk – p.9
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0 100 200 300 400 500Temperature (
oK)
0
0.02
0.04
0.06
0.08
0.1
Ene
rgy
(eV
)
Energy per atom for the Ni3 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.10
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0 1000 2000 3000Temperature (
oK)
0
2
4
6
8
10
Cv(
k B)
Cv per atom for the Ni3 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IIJohnson
Talk – p.11
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0 100 200 300 400 500Temperature (
oK)
1
1.2
1.4
1.6
1.8
2
Cv(
k B)
Cv per atom for the Ni3 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.12
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0 1000 2000 3000Temperature (
oK)
0
0.1
0.2
0.3
Lind
eman
n In
dex
(δ)
Lindemann Index for the Ni3 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.13
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0 1000 2000 3000Temperature (
oK)
0.5
1
1.5
2
µ(µ B
)
Magnetic moment per atom for the Ni3 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − Rosato Erkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.14
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0 1000 2000 3000Temperature (
0K)
0
0.2
0.4
0.6
0.8
1
Ene
rgy
(eV
)
Energy per atom for the Ni4 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.15
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0 100 200 300 400 500Temperature (
oK)
0
0.02
0.04
0.06
0.08
0.1
Ene
rgy
(eV
)
Energy per atom for the Ni4 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.16
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0 1000 2000 3000Temperature (
oK)
0
2
4
6
8
10
Cv(
k B)
Cv per atom for the Ni4 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IIJohnson
Talk – p.17
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0 100 200 300 400 500Temperature (oK)
1.5
1.7
1.9
2.1
2.3
2.5
Cv(
k B)
Cv per atom for the Ni4 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.18
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0 500 1000 1500 2000 2500 3000Temperature (
oK)
0
0.1
0.2
0.3
0.4
Lind
eman
n In
dex
δ
Lindemann Index for the Ni4 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.19
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0 1000 2000 3000Temperature (
oK)
0.5
1
1.5
2
Mag
netic
Mom
ent µ
(µB)
Magnetic Moment per atom for the Ni4 cluster
Lennerd − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.20
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0 1000 2000 3000 4000Temperature (
oK)
0
0.2
0.4
0.6
0.8
Ene
rgy
(eV
)
Energy per atom for the Ni5 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.21
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0 100 200 300 400 500Temperature (
oK)
0
0.02
0.04
0.06
0.08
0.1
Ene
rgy
(eV
)
Energy per atom for the Ni5 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.22
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0 1000 2000 3000Temperature (
oK)
1
2
3
4
5
Cv(
k B)
Cv per atom for the Ni5 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IIJohnson
Talk – p.23
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0 100 200 300 400 500Temperature (
oK)
1.4
1.8
2.2
2.6
3
Cv(
k B)
Cv per atom for the Ni5 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.24
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0 500 1000 1500 2000 2500 3000Temperature (
oK)
0
0.04
0.08
0.12
0.16
0.2
0.24
0.28
0.32
0.36
0.4
Lind
eman
n In
dex
(δ)
Lindemann Index for the Ni5 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.25
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0 1000 2000 3000Temperature (
oK)
0.5
1
1.5
2
µ(µ Β
)
Magnetic Moment per atom for the Ni5 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IIJohnson
Talk – p.26
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0 1000 2000 3000Temperature (
oK)
0
0.2
0.4
0.6
0.8
Ene
rgy
(eV
)
Energy per atom for the Ni6 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.27
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0 100 200 300 400 500Temperature (
oK)
0
0.02
0.04
0.06
0.08
0.1
Ene
rgy
(eV
)
Energy per atom for the Ni6 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.28
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0 1000 2000 3000Temperature (
oK)
1
2
3
4
5
6
Cv(
k B)
Cv per atom for the Ni6 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IIJohnson
Talk – p.29
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0 100 200 300 400 500Temperature (
oK)
1.5
1.9
2.3
2.7
3.1
3.5
Cv(
k B)
Cv per atom for the Ni6 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.30
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0 500 1000 1500 2000 2500 3000Temperature (
oK)
0
0.1
0.2
0.3
0.4
Lind
eman
n In
dex
δ
Lindemann Index for the Ni6 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.31
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0 1000 2000 3000Temperature (
oK)
0.5
1
1.5
2
µ(µ B
)
Magnetic moment per atom for the Ni6 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.32
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0 1000 2000 3000Temperature (
oK)
0
0.2
0.4
0.6
0.8
Ene
rgy
(eV
)
Energy per atom for the Ni7 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.33
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0 100 200 300 400 500Temperature (
oK)
0
0.02
0.04
0.06
0.08
0.1
Ene
rgy
(eV
)
Energy per atom for the Ni7 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.34
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0 1000 2000 3000Temperature (
oK)
1
3
5
7
Cv(
k B)
Cv per atom for the Ni7 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IIJohnson
Talk – p.35
![Page 36: Adequacy of the Classical Potentials for the study of …esperia.iesl.forth.gr/~fthenak/presentation_Thess.pdf · 2007. 4. 10. · Adequacy of the Classical Potentials for the study](https://reader035.fdocuments.us/reader035/viewer/2022071107/5fe22e0874b38d097d3792c4/html5/thumbnails/36.jpg)
0 100 200 300 400 500Temperature (
oK)
1
2
3
4
Cv(
k B)
Cv per atom for the Ni7 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IIJohnson
Talk – p.36
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0 500 1000 1500 2000 2500 3000Temperature (
oK)
0
0.04
0.08
0.12
0.16
0.2
0.24
0.28
0.32
0.36
0.4
Lind
eman
n In
dex
(δ)
Lindemann Index for the Ni7 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.37
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0 1000 2000 3000Temperature (
oK)
0.5
1
1.5
2
µ(µ B
)
Magnetic moment per atom for the Ni7 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.38
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0 1000 2000 3000Temperature (
oK)
0
0.2
0.4
0.6
0.8
Ene
rgy
(eV
)
Energy per atom for the Ni8 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.39
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0 100 200 300 400 500Temperature (
oK)
0
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0.04
0.06
0.08
0.1
Ene
rgy
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Energy per atom for the Ni8 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.40
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0 1000 2000 3000Temperature (
oK)
2
2.4
2.8
3.2
3.6
4
Cv(
kB)
Cv per atom for the Ni8 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.41
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0 100 200 300 400 500Temperature (
oK)
2
2.4
2.8
3.2
3.6
Cv(
kB)
Cv per atom for the Ni8 cluster
Lennard−JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.42
![Page 43: Adequacy of the Classical Potentials for the study of …esperia.iesl.forth.gr/~fthenak/presentation_Thess.pdf · 2007. 4. 10. · Adequacy of the Classical Potentials for the study](https://reader035.fdocuments.us/reader035/viewer/2022071107/5fe22e0874b38d097d3792c4/html5/thumbnails/43.jpg)
0 500 1000 1500 2000Temperature (
oK)
0
0.04
0.08
0.12
0.16
0.2
0.24
0.28
0.32
0.36
0.4
Lind
eman
n In
dex
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Lindemann Index for the Ni8 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − WalesUppenbrink − WalesJohnson
Talk – p.43
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0 1000 2000 3000Temperature (
oK)
0.5
1
1.5
2
µ(µ B
)
Magnetic moment per atom for the Ni8 cluster
Lennard − JonesMorseErkoc ISutton − Chen ISutton − Chen IISutton − Chen IIICleri − RosatoErkoc IIErkoc IIIUppenbrink − Wales IUppenbrink − Wales IJohnson
Talk – p.44
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Potentials
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1000
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2000
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pera
ture
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Melting Temperature
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Talk – p.45
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Acknowledgments
� Supported through EU-GROWTH researchproject AMMARE (G5RD-CT-2001-00478)
� Computational Support Dr. S. Stamatiadis
Talk – p.46
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