thermodynamics and kinetics study of growth behavior of sono-electrodeposited cu thin films sabita...
Post on 22-Dec-2015
217 views
TRANSCRIPT
Thermodynamics and Kinetics study of growth behavior of sono-electrodeposited Cu thin films
Sabita Rout, A. Mallik, B. C. [email protected] [email protected]
Department of Metallurgical and Materials EngineeringNational Institute of Technology, Rourkela
SEQUENCE OF PRESENTATION
Growth of thin films – an insight
The growth parable
Sono-electrodeposition technique
Experimental /Results and discussion
Conclusions
References
Harper et.al, Journal of applied Physics, 86 (1999) 2516-2524
(Property change with variation of grain size)
(Time bound Grain growth)
Growth of thin films
The growth Parable
Model 1Different sizes
Model 2Sequence of different sizes
Model 3Same sizes
Model 4Sequence of same sizes
Sources Grain boundaries Stacking faults Dislocations Surface energy Elastic strain Pinning particles
Grain growth mechanism Ostwald ripening Triple junctions Zener pinning
Two modes of grain growth Normal grain growth Abnormal grain growth
(Growth models)
Normal grain growth Abnormal grain growth
Follows a parabolic law
Diameter of grains comparable to the film thickness
Growth is slow and steady
A monomodal distribution of grain sizes after growth
Grain boundary velocity is given by
Diameter of grains exceeds ten times the film thickness
Growth is rapid and abrupt
A bimodal distribution of grain sizes after growth
)/exp()/( RTa
GmTVGCv KtDD 20
Normal vs. abnormal grain growth
• Extreme fast mass transport
• Affects the crystallization process
• Degassing at the electrode surface
Sono-electrodepositionThe coupled effect of electrochemistry and ultrasound
(A cavitation bubble)
(The equipment)
(The effects)
cavitation
Reaction kinetics - > cyclic voltammetry
Cyclic Voltammetry of copper deposits at (a)Sonicntion (b) Silent
Bath temp (°C) Oxidation potential (V)
Cathodic efficiency
5 +0.567 1.6
10 +0.626 0.79
15 +0.626 0.92
20 +0.626 0.72
25 +0.626 0.84
-0.8 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 0.8 1.0 1.2-0.12
-0.10
-0.08
-0.06
-0.04
-0.02
0.00
0.02
0.04
0.06
0.08
0.10
0.12
0.14
Cu
rren
t (A
)
Potential (V)
5C 10C 15C 20C 25C
ab
Portela et.al , Electrochimica Acta, 51 (2006) 3261-3268
(Deposition at -0.3V)
0 5 10 15 20
-0.035
-0.030
-0.025
-0.020
-0.015
Cur
rent
/A
Time/sec
5C 10C 15C 20C 25C
Nucleation mechanism - > Chrono amperometry analysis:
Mallik et.al , Electrochemical and Solid State Letters, 12 (2009) F46-F49 Han et.al, Electrochimica Acta, 54 (2009) 3419-3427
20 °CBath temp (°C)
Imax (A/cm2)
tmax(s) D x 10-9 (cm2 s-1 )
N x 1010 (cm-2 )
5 0.0228 1.726 1.1673 4.5604
10 0.0184 0.885 1.2246 3.273
15 0.0175 1.139 1.4257 2.1844
20 0.0162 1.349 1.447 1.8171
25 0.0238 1.685 3.9011 0.5396
Table: Characteristic kinetic parameters of current transients obtained for sonicated copper deposits
(Deposition at silent condition)
(DSC thermograms at scan rate of 5°/min )
Thermodynamics and Kinetics - > DSC analysis:
Copper deposition at (°C) Activation energy (eV/atom)
5 0.85
10 2.90
15 1.51
20 1.50
25 1.35
Kissinger equation
Heat release increases with decrease in temperature The exothermic peak observed around 320°C Activation energy is in the range, 0.85-2.9 eV
0.001500.001510.001520.001530.001540.001550.001560.001570.001580.001590.001600.001610.001620.00163
-11.4
-11.2
-11.0
-10.8
-10.6
-10.4
-10.2
-10.0
-9.8
5C 10C 15C 20C 25C
Ln
(/T
m2
)
1/Tm(1/K)
Table: Activation energies
Temperature (°C)
S. E (mN/m) Before DSC
S.E (mN/m)After DSC
5 59.92 55.62
10 51.58 34.24
15 45.84 67.86
20 41.77 43.21
25 30.48 32.30
Growth mode - >surface energy
Table: Surface energy values
Decrease in temperature – increase in SE Fluctuations in SE after thermal treatment – abnormal to normal growth behavior
(Water on deposit )
(SE determination by Owens-Wendt &
Kaelble (OW) method)
40 50 60 70 80 90 100
0100200300400500600700800900
1000110012001300140015001600
Inte
ns
ity
(arb
.un
its
)
2(degree)
Cu(111)
Cu(200)Cu(022) Cu(113)
5C
10C
15C
20C
25C
C(1011)S(0214)
Cl(721)S(062)
XRD plots of copper deposits (a) before DSC (b) after DSC
XRD analysis
Size and strain calculated from XRD plots for copper thin film (A) before DSC (B) after DSC
Bath temperatur
e (°C)
Size (nm) Strain x 10-3
5 12.4416 5.5025
10 22.3809 4.0702
15 53.159 2.1285
20 65.5048 1.815
25 182.5815 0.2787
40 50 60 70 80 90 100
0
50
100
150
200
250
300
350
400
450
500
Inte
ns
ity
(arb
.un
its
)
2(degree)
15C 20C 25C
Cu(111)
Cu(200)
Cu(022) Cu(113)S(062) S(0214)
Cl(721)
C(1011)
Bath temperature
(°C)
Size (nm) Strain x 10-3
15 102.119 1.81075
20 116.4013 1.0675
25 230.5810 0.0475
a b
A B
SEM analysis both before and after DSC:
a
c d
(SEM images of copper deposited at 5°C, 10°C, 15°C, 20°C, 25°C under sonication condition (a-e) as
deposited (f-j) after DSC)
a b c d e
f g h i j
Model-4Model-1
Model-1
i j
Conclusions
Better adherence of deposit by sono-electrodeposition.
The appearance of exothermic peak signifies occurrence of grain growth.
Determination of activation energy provides information about the kinetics of grain growth.
Whether proposed growth mechanism are the correct way to explore grain growth, will remain unclear until further investigations down to single grain or monolayer films
References
1. J. M. Zhang, K. W. Xu, V. Ji. Competition between surface and strain energy during grain growth in free-standing and attached Ag and Cu films on Si substrates. Applied surface science 187 (2002) 60-67.
2. J. M. E. Harper, C. Cabral, P. C. Andricacos, L. Gignac, I. C. Noyan. Mechanisms for microstructure evolution in electroplated copper thin films near room temperature. Journal of applied physics 86 (1999) 2516-2525.
3. F. P. Luce, P. F. P. Fichtner, L. F. Schelp. Abnormal grain growth behavior in nanostructured Al thin films on SiO2/Si
substrate. Material Research Society 1150 (2009) RR03-06.4. C. Detavernier, S.Rossnagel, C. Noyan, S. Cabral. Thermodynamics and kinetics of room-temperature microstructural
evolution in copper films. Journal of applied physics 94 (2003) 2874-2881.5. A. Mallik, A. Bankoti, B. C. Ray. A Study on the Modification of Conventional Electrochemical Crystallization under
Sonication: The Phenomena of Secondary Nucleation. Electrochemical and Solid-State Letters 12 (2009) F-46-F-49.6. R. Cow, R. Blindt, R. Chivers, M. Povey. A study on the primary and secondary nucleation of ice by power ultrasound.
Ultrasonics 43 (2005) 227-230.7. D. Bera, S. C. Kuiry, S. Seal. Kinetics and Growth Mechanism of Electrodeposited Palladium Nanocrystallites . Journal of
Physical Chemistry 108 (2004) 556-562.8. R. Finsy. On the Critical Radius in Ostwald Ripening. Langmuir 20 (2004) 2975-2976.9. K. B. Yin, Y.D. Xia, C. Y. Chan, W. Q. Zhang. The kinetics and mechanism of room-temperature microstructural evolution
in electroplated copper foils. Scripta Materialia 58 (2008) 65-68.10. S. Villain, P. Knauth, G. Schwitzgebel. Electrodeposition of Nanocrystalline Silver: Study of Grain Growth by
Measurement of Reversible Electromotive Force. Journal of Physical Chemistry 101 (1997) 7452-7454. 11. H. E. Kissinger. Reaction Kinetics in Differential Thermal Analysis. Analytical Chemistry 29 (1957) 1702-1706.12. L. Zhou, H. Zhang, D. J. Srolovitz. A size effect in grain boundary migration: A molecular dynamics study of bicrystal
thin films. Acta Materialia 53 (2005) 5273-5279.13. S. K. Donthu, M. Vora, S. K. Lahiri, C. V. Thompson. Activation Energy Determination for Recrystallization in
Electroplated-copper films using Differential Scanning Calorimetry. Journal of Electronic Materials 32 (2003) 531-534.14. P. Knauth, A. Charai, P. Gas. Grain growth of pure nickel and of Ni-Si solid solution studied by Differential Scanning
Calorimetry of nanometer-sized crystals. Scripta Metallurgica Materialia 28 (1993) 325-330.
Thank u