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How complexity can help: the case
of aluminum-based intermetallics
Jean-Marie DUBOIS
Institut Jean Lamour
UMR 7198 CNRS – Université de Lorraine
jean-marie.dubois@ijl.nancy-universite.fr
Esther BELIN-FERRÉ
Laboratoire Chimie-Physique Matière et Rayonnement
UMR 7614 CNRS Université Pierre et Marie Curie
esther.belin-ferre@upmc.fr

This lecture is dedicated to Prof.
Hans-Rainer Trebin, who retires
from his position as Professor of
the University of Stuttgart,
Germany, and head of the
Institute for Theoretical and
Applied Physics.

MRS Brazil - Florianopolis

Sept. 23-27, 2012

2

1
Outline

1- The old paradigm of crystallography
2- Few old examples of periodic, complex metallic alloys
(CMAs)
3- The specific case of quasicrystals
4- Synthesis
5- Complexity in metallic alloys
6- Transport properties versus complexity
7- Few, complexity-dependent, applications of CMAs
8- Conclusion
MRS Brazil - Florianopolis

Sept. 23-27, 2012

3

The old paradigm of crystallography

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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2
The periodic tiling of 2D-space

1/6 of 2π: 6 tiles	


1/4 of 2π: 4 tiles
4 tiles around each
vertex:

1/3 of 2π: 3 tiles

No void, no overlap.

MRS Brazil - Florianopolis

Sept. 23-27, 2012

5

Not always that easy!
135°
α = 2(π- π /5)/2 = 4π/5 = 144°
1/5 of 2π
1
τ

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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3
THE discovery in 1982

3D reciprocal space: same
symmetry as that of the
icosahedron or the pentagonal
dodecahedron
MRS Brazil - Florianopolis

Danny Shechtman,
Technion, Haifa

Sept. 23-27, 2012

7

Few old examples of periodic,
complex metallic alloys (CMAs)

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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4
The early days …
1930s to 60s	

Al12Mo

Linus Pauling and
his collaborators
(Samson,
Schoemaker, etc.)

T-AlZnMg

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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The example of the Bergman phase
(Al,Zn)49 Mg32

G. Bergman, J.L.T. Waugh, L. Pauling, Nature 169, 1057 (1952)

•  Cubic

structure Im3
•  Unit cell a = 14.16 Å,
•  ~162 atoms/cell
Al
Mg
Zn

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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5
Another, even more complex, example: β-Al3Mg2
Feuerbacher et al.
Z. Krystallographie (2006)

Al
Al/Mg
Mg

1832 atomic positions,
but only 1178 occupied.
Lattice parameter:
Al
Mg

a = 2.824 nm.

MRS Brazil - Florianopolis

Sept. 23-27, 2012

11

Two essential characteristics of complexity: 1
Atomic layers like Russian dolls:

The Al-Zn-Mg
Bergman phase
Drawings: courtesy of U. Mizutani
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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6
Two essential characteristics of complexity: 2
Pronounced cluster structure

i- Large unit cell
cF1168-Al3Mg2




a = 2.8239(1) nm

V = 22.5189 nm3#
Courtesy Uichiro Mizutani, 2005.

ii- Significant amount of disorder
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Sept. 23-27, 2012

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10-fold symmetry: twinning ?

MRS Brazil - Florianopolis

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The specific case of quasicrystals

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Discoverers of quasicrystals

1982-1985
Not all co-discoverers
shown on this picture!

5 f	


10 f	

12 f	


MRS Brazil - Florianopolis

8 f	


Sept. 23-27, 2012

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8
No evidence of translation symmetry anymore
Perfect icosahedral
point group
symmetry in
reciprocal space
Perfect
pentagonal tiling
along specific
directions in real
space, with no
twinning!
Courtesy of P. A. Thiel,
Ames Labs, USA.
MRS Brazil - Florianopolis

Sept. 23-27, 2012

17

Two main types of quasicrystals
Icosahedral:
Aperiodic in 3D

Decagonal:
Aperiodic in 2D,
Periodic in 1D

Quasiperiodic planes stacked periodically
Courtesy: P. A. Thiel, Ames Labs, USA.

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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9
Where the atoms are in the bulk
A ⇒ AB
L
L
S
L
L
S
L
S
L
L
S
L

≈ 2 nm
Takakura et al., Acta Cryst. 2001

B⇒A
A
AB
ABA
ABAAB
ABAABABA
etc.

…
ABAABABAABAAB…
Non-periodic AND
Num(A)/Num(B) = τ =
(1+√5)/2 ≈ 1.618…

Synthesis

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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10
Preparation of single crystals
Several techniques exist to grow single crystals
of complex metallic alloys with high structural
quality:
Czochralsky pulling technique
Flux growth method
≈ 8 cm

Courtesy:
M. Feuerbacher, Juelich

Courtesy: I. Fisher & P. Canfield, Ames
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Preparation by metallurgical methods
Not only laboratory samples:
Slowly solidified ingot

Composition: Al71Cu9Cr10Fe10 (at%)
PVD coating for thermal
insulation of a helicopter
turbine blade

Batches of up to 1 000 kg of atomized powder
produced in 1993-94
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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11
Most CMAs are thermodynamically stable

Al62.5Cu25Fe12.5
ω-Al70Cu20Fe10

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Complexity

12
CMAs: Structure changes dramatically with conc.
βC

Hierarchical clusters
clusters
atoms

If glue atoms are omitted,
fractal dimension < 3
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Complexity in one, single number
In reciprocal space:

In real space:

Complexity index:

2kF
	


βC = Ln(Nunit cell)
Tri-Al Mn

Shannon entropy of a single 11 4
constituent compound: S = α βC + K

βC(bcc) = Ln(2)
βC(fcc) = 2 Ln(2)

βC(ico) << ∞
Jones zone

βC(ico) ≈ Ln(6.1023) ≈ 54
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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13
Transport properties versus complexity

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Electron transport in CMAs
Belin-Ferré, Klanjšek, Jagličić, Dolinšek, Dubois, J. Phys. Cond. Matter 17 (2005) 6911.

Size of the unit cell

Conductivity:
Mott type: ρ ∝ n(EF)-2
2

( N ( E ) % S free e 2 
σ = & free F # F 3 F
' N ( EF ) $ 12π 
Mizutani, J. Phys. Cond. Matter
10 (1998) 4609.

Conductivity:
Einstein type: ρ ∝ n(EF)-1
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Electron conductivity at 4K

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Sept. 23-27, 2012

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4K Conductivity: an example of SOC?

Contains NO
transition metal!

MRS Brazil - Florianopolis

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RT thermal diffusity vs complexity

κ = α ρ CP
ρ ≈ Cte
κ ≈ A σ300K + B
Therefore: α α σ	


At 300K, CP ≈ 3R ;

MRS Brazil - Florianopolis

Sept. 23-27, 2012

31

Self-organised criticality (SOC)
Frequency of the avalanche (Log of)

Slope ≈ -1

Size of the avalanche (Log of)
Per Bak 1948-2002
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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16
Other examples of SOC
Connectivity
of the web

Earthquakes of
magnitude m

MRS Brazil - Florianopolis

Sept. 23-27, 2012

33

SOC

SOC is an intermediate state, between order and disorder.
SOC is metastable, although it may last (nearly) for ever
(e.g. California’s earthquakes)
SOC is characterized by a power law:
N(m) = m-α
with α ≈ 1.
The SOC state in Al-based intermetallics is sampled thanks
to the formation of compounds of varying unit cell size.
In reminiscence of avalanches on a sand pile, it must be
related to hopping of electrons.
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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17
Applications related to complexity

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Applications based on transport properties

There is a certain range of concentrations within which nearly
identical properties are found: industrial exploitation is feasible!
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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18
Most CMAs applications exploit complexity
1988:
Frying pans (Dubois)
1992:
Solar light absorbers (Eisenhammer, Machizaud &
Dubois)
1993: Thermal barriers (Dubois)
High performance maraging steels (Nilsson)
ca 2000: Anti-fretting coatings (Dubois & Merstallinger)
Zero-TCR resistors (Dolinšek)
Advanced catalysts based on leached AlCuFe (Tsai)
…
2008:
Selective Laser Sintereded polymer-CMA composites
(Kenzari & Fournée)
Metal-matrix composites (Singh, Fleury, Eckert, …)
2010: Thermal memory cell (Dolinšek)
Dual thermo-electric rectifiers (Takeuchi)
2012: High-performance, low cost Al13Fe4 catalyst (Ambruster)
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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A new, commercial technology based on CMAs
Polyamidematrix
composite
reinforced by
atomized
Al-Cu-Fe-B
icosahedral
particules, which
was assembled
by Selective
Laser Sintering.
Used for a
Formula I race
car by Renault.

Approx. 20 cm

S. Kenzari & V. Fournée, French Patent n°2950826
(2009), PCT n° WO2011/039469 (2011).
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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19
SLSed Polymer matrix composites
Pin-on-Disk test

Disk

Load Fn
Pin: e.g.
hard steel

Friction coefficient (µ)

Tangential force Ft

(a)

0,35

0,3

0,25

0,2

0,15

0,1

PA+AlCuFeB
PA+Al
PA

0

Friction coefficient: µ = Ft/Fn
Friction coefficient against hard
steel in air for various
composites

Friction coefficient (µ)

0,35

20

40

60

80

100

Sliding distance (m)

(b)

0,3

0,25

0,2
PA+AlCuFeB
Carbon fibers
Glass fibers
Glass
PA

0,15

0,1

0

20

40

60

80

100

Sliding distance (m)

S. Kenzari et al. Materials & Design, 35 (2011) 691.
MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Sept. 23-27, 2012

40

Selective Laser Sintering (1)

MRS Brazil - Florianopolis

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Selective Laser Sintering (2)
IR light

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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Sept. 23-27, 2012

42

Selective Laser Sintering (3)

MRS Brazil - Florianopolis

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Selective Laser Sintering (4)

MRS Brazil - Florianopolis

Sept. 23-27, 2012

43

Optical conductivity
1 104

0

Energy (eV)

0.04

0.08

0.12

0.16

Optical conductivity σ(ω) (Ω-1.cm-1)

10000	

i-Al-Cu-Fe-B
0%-Al-Cr-Fe
50%-Al-Cr-Fe
80%-Al-Cr-Fe
100%-Al-Cr-Fe

Drude peak	


8000
8000	


6000
6000	


γ-Al-Cr-Fe	


4000
4000	


Ο1-Al-Cr-Fe	


2000
2000	


Ico-Al-Cu-Fe-B	

0

0

200

400

600

800

1000
-1

1200

1400

Wavenumber (cm )

No Drude peak	

V. Demange et al. PRB 6-14 (2002) 144205 1.

High IR light
absorption

MRS Brazil - Florianopolis

Sept. 23-27, 2012

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22
Conclusion

MRS Brazil - Florianopolis

Sept. 23-27, 2012

45

Conclusion
Properties:
✿ Several properties of Al-based CMAs scale as power
laws of the complexity index βC : this is taken as an
example of Self-Organized Criticality (SOC).

Applications:
v 
Several applications may result:
ü  Thermal barriers for low (< 200 K) and high (800 < T
> 1200 K) applications
ü  Infra-red absorbers
ü  Low-stick coatings for frying pans
ü  Non-fretting parts for high vacuum technologies
ü  Etc.
MRS Brazil - Florianopolis

Sept. 23-27, 2012

46

23
Acknowledgements
Special thanks to Hervé Combeau, IJL, for very interesting
discussions about SOC
And to our sponsors:

MRS Brazil - Florianopolis

Sept. 23-27, 2012

47

Sept. 23-27, 2012

48

Thank you for your attention!

MRS Brazil - Florianopolis

24

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How complexity can help: the case of Aluminum-based intermetallics.

  • 1. How complexity can help: the case of aluminum-based intermetallics Jean-Marie DUBOIS Institut Jean Lamour UMR 7198 CNRS – Université de Lorraine jean-marie.dubois@ijl.nancy-universite.fr Esther BELIN-FERRÉ Laboratoire Chimie-Physique Matière et Rayonnement UMR 7614 CNRS Université Pierre et Marie Curie esther.belin-ferre@upmc.fr This lecture is dedicated to Prof. Hans-Rainer Trebin, who retires from his position as Professor of the University of Stuttgart, Germany, and head of the Institute for Theoretical and Applied Physics. MRS Brazil - Florianopolis Sept. 23-27, 2012 2 1
  • 2. Outline 1- The old paradigm of crystallography 2- Few old examples of periodic, complex metallic alloys (CMAs) 3- The specific case of quasicrystals 4- Synthesis 5- Complexity in metallic alloys 6- Transport properties versus complexity 7- Few, complexity-dependent, applications of CMAs 8- Conclusion MRS Brazil - Florianopolis Sept. 23-27, 2012 3 The old paradigm of crystallography MRS Brazil - Florianopolis Sept. 23-27, 2012 4 2
  • 3. The periodic tiling of 2D-space 1/6 of 2π: 6 tiles 1/4 of 2π: 4 tiles 4 tiles around each vertex: 1/3 of 2π: 3 tiles No void, no overlap. MRS Brazil - Florianopolis Sept. 23-27, 2012 5 Not always that easy! 135° α = 2(π- π /5)/2 = 4π/5 = 144° 1/5 of 2π 1 τ MRS Brazil - Florianopolis Sept. 23-27, 2012 6 3
  • 4. THE discovery in 1982 3D reciprocal space: same symmetry as that of the icosahedron or the pentagonal dodecahedron MRS Brazil - Florianopolis Danny Shechtman, Technion, Haifa Sept. 23-27, 2012 7 Few old examples of periodic, complex metallic alloys (CMAs) MRS Brazil - Florianopolis Sept. 23-27, 2012 8 4
  • 5. The early days … 1930s to 60s Al12Mo Linus Pauling and his collaborators (Samson, Schoemaker, etc.) T-AlZnMg MRS Brazil - Florianopolis Sept. 23-27, 2012 9 The example of the Bergman phase (Al,Zn)49 Mg32 G. Bergman, J.L.T. Waugh, L. Pauling, Nature 169, 1057 (1952) •  Cubic structure Im3 •  Unit cell a = 14.16 Å, •  ~162 atoms/cell Al Mg Zn MRS Brazil - Florianopolis Sept. 23-27, 2012 10 5
  • 6. Another, even more complex, example: β-Al3Mg2 Feuerbacher et al. Z. Krystallographie (2006) Al Al/Mg Mg 1832 atomic positions, but only 1178 occupied. Lattice parameter: Al Mg a = 2.824 nm. MRS Brazil - Florianopolis Sept. 23-27, 2012 11 Two essential characteristics of complexity: 1 Atomic layers like Russian dolls: The Al-Zn-Mg Bergman phase Drawings: courtesy of U. Mizutani MRS Brazil - Florianopolis Sept. 23-27, 2012 12 6
  • 7. Two essential characteristics of complexity: 2 Pronounced cluster structure i- Large unit cell cF1168-Al3Mg2
 
 a = 2.8239(1) nm
 V = 22.5189 nm3# Courtesy Uichiro Mizutani, 2005. ii- Significant amount of disorder MRS Brazil - Florianopolis Sept. 23-27, 2012 13 Sept. 23-27, 2012 14 10-fold symmetry: twinning ? MRS Brazil - Florianopolis 7
  • 8. The specific case of quasicrystals MRS Brazil - Florianopolis Sept. 23-27, 2012 15 Discoverers of quasicrystals 1982-1985 Not all co-discoverers shown on this picture! 5 f 10 f 12 f MRS Brazil - Florianopolis 8 f Sept. 23-27, 2012 16 8
  • 9. No evidence of translation symmetry anymore Perfect icosahedral point group symmetry in reciprocal space Perfect pentagonal tiling along specific directions in real space, with no twinning! Courtesy of P. A. Thiel, Ames Labs, USA. MRS Brazil - Florianopolis Sept. 23-27, 2012 17 Two main types of quasicrystals Icosahedral: Aperiodic in 3D Decagonal: Aperiodic in 2D, Periodic in 1D Quasiperiodic planes stacked periodically Courtesy: P. A. Thiel, Ames Labs, USA. MRS Brazil - Florianopolis Sept. 23-27, 2012 18 9
  • 10. Where the atoms are in the bulk A ⇒ AB L L S L L S L S L L S L ≈ 2 nm Takakura et al., Acta Cryst. 2001 B⇒A A AB ABA ABAAB ABAABABA etc. … ABAABABAABAAB… Non-periodic AND Num(A)/Num(B) = τ = (1+√5)/2 ≈ 1.618… Synthesis MRS Brazil - Florianopolis Sept. 23-27, 2012 20 10
  • 11. Preparation of single crystals Several techniques exist to grow single crystals of complex metallic alloys with high structural quality: Czochralsky pulling technique Flux growth method ≈ 8 cm Courtesy: M. Feuerbacher, Juelich Courtesy: I. Fisher & P. Canfield, Ames MRS Brazil - Florianopolis Sept. 23-27, 2012 21 Preparation by metallurgical methods Not only laboratory samples: Slowly solidified ingot Composition: Al71Cu9Cr10Fe10 (at%) PVD coating for thermal insulation of a helicopter turbine blade Batches of up to 1 000 kg of atomized powder produced in 1993-94 MRS Brazil - Florianopolis Sept. 23-27, 2012 22 11
  • 12. Most CMAs are thermodynamically stable Al62.5Cu25Fe12.5 ω-Al70Cu20Fe10 MRS Brazil - Florianopolis Sept. 23-27, 2012 23 MRS Brazil - Florianopolis Sept. 23-27, 2012 24 Complexity 12
  • 13. CMAs: Structure changes dramatically with conc. βC Hierarchical clusters clusters atoms If glue atoms are omitted, fractal dimension < 3 MRS Brazil - Florianopolis Sept. 23-27, 2012 25 Complexity in one, single number In reciprocal space: In real space: Complexity index: 2kF βC = Ln(Nunit cell) Tri-Al Mn Shannon entropy of a single 11 4 constituent compound: S = α βC + K βC(bcc) = Ln(2) βC(fcc) = 2 Ln(2) βC(ico) << ∞ Jones zone βC(ico) ≈ Ln(6.1023) ≈ 54 MRS Brazil - Florianopolis Sept. 23-27, 2012 26 13
  • 14. Transport properties versus complexity MRS Brazil - Florianopolis Sept. 23-27, 2012 27 Electron transport in CMAs Belin-Ferré, Klanjšek, Jagličić, Dolinšek, Dubois, J. Phys. Cond. Matter 17 (2005) 6911. Size of the unit cell Conductivity: Mott type: ρ ∝ n(EF)-2 2 ( N ( E ) % S free e 2  σ = & free F # F 3 F ' N ( EF ) $ 12π  Mizutani, J. Phys. Cond. Matter 10 (1998) 4609. Conductivity: Einstein type: ρ ∝ n(EF)-1 MRS Brazil - Florianopolis Sept. 23-27, 2012 28 14
  • 15. Electron conductivity at 4K MRS Brazil - Florianopolis Sept. 23-27, 2012 29 Sept. 23-27, 2012 30 4K Conductivity: an example of SOC? Contains NO transition metal! MRS Brazil - Florianopolis 15
  • 16. RT thermal diffusity vs complexity κ = α ρ CP ρ ≈ Cte κ ≈ A σ300K + B Therefore: α α σ At 300K, CP ≈ 3R ; MRS Brazil - Florianopolis Sept. 23-27, 2012 31 Self-organised criticality (SOC) Frequency of the avalanche (Log of) Slope ≈ -1 Size of the avalanche (Log of) Per Bak 1948-2002 MRS Brazil - Florianopolis Sept. 23-27, 2012 32 16
  • 17. Other examples of SOC Connectivity of the web Earthquakes of magnitude m MRS Brazil - Florianopolis Sept. 23-27, 2012 33 SOC SOC is an intermediate state, between order and disorder. SOC is metastable, although it may last (nearly) for ever (e.g. California’s earthquakes) SOC is characterized by a power law: N(m) = m-α with α ≈ 1. The SOC state in Al-based intermetallics is sampled thanks to the formation of compounds of varying unit cell size. In reminiscence of avalanches on a sand pile, it must be related to hopping of electrons. MRS Brazil - Florianopolis Sept. 23-27, 2012 34 17
  • 18. Applications related to complexity MRS Brazil - Florianopolis Sept. 23-27, 2012 35 Applications based on transport properties There is a certain range of concentrations within which nearly identical properties are found: industrial exploitation is feasible! MRS Brazil - Florianopolis Sept. 23-27, 2012 36 18
  • 19. Most CMAs applications exploit complexity 1988: Frying pans (Dubois) 1992: Solar light absorbers (Eisenhammer, Machizaud & Dubois) 1993: Thermal barriers (Dubois) High performance maraging steels (Nilsson) ca 2000: Anti-fretting coatings (Dubois & Merstallinger) Zero-TCR resistors (Dolinšek) Advanced catalysts based on leached AlCuFe (Tsai) … 2008: Selective Laser Sintereded polymer-CMA composites (Kenzari & Fournée) Metal-matrix composites (Singh, Fleury, Eckert, …) 2010: Thermal memory cell (Dolinšek) Dual thermo-electric rectifiers (Takeuchi) 2012: High-performance, low cost Al13Fe4 catalyst (Ambruster) MRS Brazil - Florianopolis Sept. 23-27, 2012 37 A new, commercial technology based on CMAs Polyamidematrix composite reinforced by atomized Al-Cu-Fe-B icosahedral particules, which was assembled by Selective Laser Sintering. Used for a Formula I race car by Renault. Approx. 20 cm S. Kenzari & V. Fournée, French Patent n°2950826 (2009), PCT n° WO2011/039469 (2011). MRS Brazil - Florianopolis Sept. 23-27, 2012 38 19
  • 20. SLSed Polymer matrix composites Pin-on-Disk test Disk Load Fn Pin: e.g. hard steel Friction coefficient (µ) Tangential force Ft (a) 0,35 0,3 0,25 0,2 0,15 0,1 PA+AlCuFeB PA+Al PA 0 Friction coefficient: µ = Ft/Fn Friction coefficient against hard steel in air for various composites Friction coefficient (µ) 0,35 20 40 60 80 100 Sliding distance (m) (b) 0,3 0,25 0,2 PA+AlCuFeB Carbon fibers Glass fibers Glass PA 0,15 0,1 0 20 40 60 80 100 Sliding distance (m) S. Kenzari et al. Materials & Design, 35 (2011) 691. MRS Brazil - Florianopolis Sept. 23-27, 2012 39 Sept. 23-27, 2012 40 Selective Laser Sintering (1) MRS Brazil - Florianopolis 20
  • 21. Selective Laser Sintering (2) IR light MRS Brazil - Florianopolis Sept. 23-27, 2012 41 Sept. 23-27, 2012 42 Selective Laser Sintering (3) MRS Brazil - Florianopolis 21
  • 22. Selective Laser Sintering (4) MRS Brazil - Florianopolis Sept. 23-27, 2012 43 Optical conductivity 1 104 0 Energy (eV) 0.04 0.08 0.12 0.16 Optical conductivity σ(ω) (Ω-1.cm-1) 10000 i-Al-Cu-Fe-B 0%-Al-Cr-Fe 50%-Al-Cr-Fe 80%-Al-Cr-Fe 100%-Al-Cr-Fe Drude peak 8000 8000 6000 6000 γ-Al-Cr-Fe 4000 4000 Ο1-Al-Cr-Fe 2000 2000 Ico-Al-Cu-Fe-B 0 0 200 400 600 800 1000 -1 1200 1400 Wavenumber (cm ) No Drude peak V. Demange et al. PRB 6-14 (2002) 144205 1. High IR light absorption MRS Brazil - Florianopolis Sept. 23-27, 2012 44 22
  • 23. Conclusion MRS Brazil - Florianopolis Sept. 23-27, 2012 45 Conclusion Properties: ✿ Several properties of Al-based CMAs scale as power laws of the complexity index βC : this is taken as an example of Self-Organized Criticality (SOC). Applications: v  Several applications may result: ü  Thermal barriers for low (< 200 K) and high (800 < T > 1200 K) applications ü  Infra-red absorbers ü  Low-stick coatings for frying pans ü  Non-fretting parts for high vacuum technologies ü  Etc. MRS Brazil - Florianopolis Sept. 23-27, 2012 46 23
  • 24. Acknowledgements Special thanks to Hervé Combeau, IJL, for very interesting discussions about SOC And to our sponsors: MRS Brazil - Florianopolis Sept. 23-27, 2012 47 Sept. 23-27, 2012 48 Thank you for your attention! MRS Brazil - Florianopolis 24