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Polymer-metal nanocomposites for functional …€¦ · constituents by VPD ... Joint DFG/JSPS...
Transcript of Polymer-metal nanocomposites for functional …€¦ · constituents by VPD ... Joint DFG/JSPS...
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PolymerPolymer--metal nanocomposites for metal nanocomposites for functionalfunctionalapplications*applications*
F. Faupel, V. Zaporojtchenko, A. Biswas, R. Adelung, F. Faupel, V. Zaporojtchenko, A. Biswas, R. Adelung, H. Takele, U. SchH. Takele, U. Schüürmann, H. rmann, H. GreveGreve
Chair for MulticomponentChair for Multicomponent Materials Materials ChristianChristian--Albrechts University KielAlbrechts University Kiel
**supportedsupported by Technologyby Technology FoundationFoundation SchleswigSchleswig--Holstein (TSH)Holstein (TSH)
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OutlineOutline
• Properties of nanocomposites• Preparation
- Co-evaporation- Co-sputtering
• Examples:- Magnetic composites for > 1 GHz- Ultra-thin optical filters- Near percolation composites- Multifunctional composites
• Summary and outlook
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Nanocomposite - new class of materials
Metal cluster1 - 100 nm
Matrix material: Polymer
Magnetic Fe-Co-Ni clusters in Teflon-AF
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Some properties of nanocomposites
♦ Optical- d << λ ⇒ no light scattering ⇒ transparent magnets,
magneto-optical devices- Surface plasmon absorption ⇒ ultra thin filters- Tunable n ⇒ Bragg reflectors, sensors
♦ Electrical - R variation > 1010 ⇒ sensors
♦ Magnetic- Dielectric matrix ⇒ no eddy currents- Eddy current cut off frequency ∝ d -2 ⇒ inductors at f > 1 GHz- Spin-dependent tunneling ⇒ TMR devices- Nanorods by self organization ⇒ perpendicular recording > 1 Tb/cm2
♦ Catalytic- Very high surface area ⇒ reactive membranes
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Possible structures of nanocomposites :1D, 2D or 3D, multilayers, fragments
Cu on PMDA/ODA Ag/PMMAfragments
Ts = 400°C
Preparation:
mixing two or moreconstituents by VPD
-co-deposition-co-sputtering-plasma deposition-hybrid process-induced crystallization
AFM
TEM
20 nm
Teflon AF + Au clusters
Teflon AF + Ag clusters
14 nm MultilayerAu/Ag/ Teflon - host
Au nanowiresin Teflon AF
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Vapor phase deposition of composites - attractive optionfor implementation in microelectronic processing
Co-evaporation
Advantages• dry, solvent-free• thick films• low defect density• high purity• good process contro•deposition conformability
PolymersPolyimide, Polyamide, PU(polycondensation of monomers)Teflon AF, FEP, PMMA etc.(thermal decomposition and repolymerization on substrate)
quarz
microbalane
1
quarzmicrobalance2
metal evaporator polymer
evaporator
shuttersubstrate
UHV chamber
V. Zaporojtchenko et al., Microel. Eng. 50, 465 (2000)
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Co-evaporation of monomers +metal Polyimide with Cu
ONN
O
O
O
O
PMDA-ODA
Imidization of polyamic acid
Annealing imidization + metal aggregation
pyromellitic dianhydride
oxydianiline
Behnke, Zaporojtchenko, Strunskus, Faupel -Micromat, (2000), 1052.
200 °C 250 °C 300 °C
30 °C 100 °C 150 °C
60 nm
60 nm 60 nm 60 nm
60 nm60 nm
Effect of annealing temperature on cluster size for Cu in PMDA-ODA
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Tailoring of the size distribution
Effect of heating rate
2 °C/min 8 °C/min 12 °C/min
+ 30 min at 250 °C
Immobilization by imidization crucial!
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Also metal-polymer interaction is importantMetal mobility determined by chemical reactivity!
Ni
Same conditions:2 °C/min, 250 °C
Cu
Problem for reactive metals : cluster oxidation
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VPD of composites based on Teflon AF®
CC C C
O
F F
OF
F F
F
CCF3 CF3
m
n
Thermal decompositionand repolymerizationonon substrate
• Advantage: protection of clusters• Problem: low metal condensation coefficient
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Effect of low C in Teflon AF- Ni composite
280 nm
Filling Factor < 1 %
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Surface Processes
Monomers and metal atomsarriving on substrate
a) adsorption adsorptionb) diffusion repolymerizationc) agglomeration cross-linkingd) desorptione) diffusionf) coalescenceg) embedding
• substrate temperature• evaporation rates• condensation coefficient
Parameter
V. Zaporojtchenko et al. - Surface Sci. 532,300 (2003)
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Condensation coefficient
C very low for polymers with low surface energy!
Thran, Kiene, Zaporojtchenko, Faupel, Phys. Rev. Lett., Vol. 82, (1999), 1903 ff.
Teflon AF: C ~ 2 ·10-3
metalamountarrivingmetalamountadsorbedC =
C for Ag on some polymers
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Influence of atomic mobility and condensation coefficient on morphology of composites (TEM study)
50nm
Columnar growth aspect ratio 100:5
Spherical clusters
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Tandem + ion beam assisted depositionsubstrate
.
quarz
microbalance quarz microbalance
metal evaporator polymer
evaporatorion beam
Random nucleation
Preferred nucleation by IBAD
J. Zekonite,V. Zaporojtchenko,U.Schuermann, F.FaupelPolym. Surf. Modification V3, 243 (2004)
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Tandem evaporation + annealingHigh filling despite low C
Ni in Teflon AF
No cluster oxidation! A. Biswas et al., Nano Letters 3, (2003) 69.
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Nanocomposites by RF co-sputteringPTFE/Ag
T: target S: substrate Sh: shutter,W: window Ar-gas inletP: pump C: cooling q: quartz monitor
-Ag ; O -fluorine; •-carbon)
300 298 296 294 292 290 288 286 284
sputtered PTFE+Ag f=31,2%
CF3
CF2
CF
FxC - CFx
coun
ts/s
Binding energy [eV]
RF = 13.56 MHz
Schürman et al., Workshop Nanocomposite, Kiel 2003
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Transition 2D to 3Ddeposition + embedding metal particles
by thermal treatment or vapour induced crystallisation
Acetone
solvent provides chain mobility for polymer crystallisation
embedding of gold clusters has been observed after crystallisation
Macromolecule 2004
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XTEM after Crystallisation
50 nm
Clusters are narrowly dispersed in the Polymer but at different depths
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Transition 2D -1D Nanowires via cracks
Nucleation at cracksVery small C
R. Adelung et al., Nature Materials 3, 375 (2004)
Metal depositionStarting material Crack formation
Example: Au wires on Teflon
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Optical nanocompositesApplications• Ultrathin optical filters• Bragg reflectors, sensors• Magnetooptical systems
ωplasmon tuned by:• nature of metal• cluster size, shape, distance • dielectric matrix
300 400 500 600 700 800
458 nm
norm
. Ext
inct
ion
[a.u
.]
Wavelength [nm]
60% 48% 37%_percolation 28% 20%
PTFE/Agfilling factor
Surface plasmon resonance: charge density oscillation ⇒ strong absorptionin visible range for nanoparticles of Au, Ag, Cu, ...
Strong field enhancement ⇒ surface enhanced Raman spectroscopy biosensors
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Nanocomposites with variable optical propertiesnear percolation
400 500 600 700 8000,0
0,2
0,4
0,6
0,8
1,0
1,2
546.5 568 nm532 nm
Abs
orba
nce
(-)
Wavelength (nm)
8.5% 14.7% 21.3% 33.2% 44.0%
Tailoring of refractive index n = 1.38 1.94 0.96f = 0 21% 50%
Percolation: f ~ 47%Au/Teflon
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Multilayer composites
20 nm
Teflon AF + Au clusters
Teflon AF + Ag clusters
Biswas, et al., Appl. Phys. Lett., Vol 84, (2004), 2655 ff
400 500 600 700 800 900
538 nm
437 nm
Abso
rptio
n (a
.u.)
Wavelength (nm)
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Multilayer periodic systemwith alternative high-and low-index layers
( Bragg Reflector )
Glass substrate Polymer n=1.38
Ag composite n= 2.2
400 600 8000
5
10
15
20
25
30
35
40 Reflexion
Ref
lect
ance
%
wavelength [nm]
100nm250nm
Spectral reflectance for 4x2 layersAg/ PTFE
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The working principle of the sensing based onTeflon composite layers: thickness, mass, density change
of polymer matrix ( Bragg Reflector or QCM)
400 600 8000
5
10
15
20
25
30
35
40 Reflexion
Ref
lect
ance
%
wavelength [nm]
Expose to organic vapor Wavelength shift after vapor exposure
alternative high-and low-index layers
TeflonTeflon composite
QCM-Sensor sensitivitydepend on composite selectivity
to organic vapors
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Magnetic nanocompositesInductive components in mobile communications
Hysteresis losses andlimit of the cut-off frequency
5-10 nm
Best solution- nanocompositehigh ρ ,Ms, FMR
moderate anisotropyEnergy to create Bloch wall >saved magnetostatic energy
Single DomainParticles
• Insulating matrix ⇒ no eddy currents
• Tuning of alloy without need of high ρ• Orientation of easy axis possible by field during
annealing or deposition
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Magnetic nanocomposites with single domain particles
-200 -150 -100 -50 0 50 100 150 200
-1,00
-0,75
-0,50
-0,25
0,00
0,25
0,50
0,75
1,00
in-plane 0° ("easy" axis) in-plane 90° ("hard" axis)
M /
MSbu
lk
magnetic field / [mT]
VSM - Vibrating Sample Magnetometry(Smart materials Group CAESAR Bonn)
0,01 0,1 1 10
0
100
200
300
400
Hc = 10 mT (100 Oe)Vibrating Sample Magnetometry
(110)
bcc
(211)(200)
frequency / [GHz]
real part µ' imaginary part µ''
ac p
erm
eabi
lity
High Frequency permeability measurementscut-off and FMR frequency > 2 GHz
FeNiCo Clusters in Teflon AF matrix
H.Greve et al. Keynote Lecture Nano 2004
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Tunneling magneto-resistance
Spin-dependent electron tunneling betweensuperparamagnetic clusters
Joint DFG/JSPS project with S. Deki, Kobe Univ.
Dispersion of Au-Co clusters by thermal decomposition of polyacrylonitrile matrix
∆ρ/ρ0 ∝ [L(mH/kT)/L(mHs/kT)]2
L: Langevin function
80 % at low H!
Nabika et el., J. Mater. Chem. 12, 2408 (2002)
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f < fc: insulating
f > fc: metallic structure
2 3 4 5 6 7 810-4
10-3
10-2
10-1
100
101
102
103
104
105
106
107
Resi
stiv
ity (O
hm*c
m)
EDX Intensity Ag/F
Electrical properties near percolationResistivity variation 1010
PTFE /Ag on glass
fc ~ 32 -36 %
0,0027 0,0028 0,0029 0,0030 0,0031 0,0032 0,0033 0,0034 0,0035300G
400G
500G
600G
700G
Ea=0.24 eV
R heating (020704) Linear Fit of GlassHeat_F
Res
ista
nce
(log
Ω)
1/T (1/K)
Thermally activated tunneling
R~ exp (Ea/kT)
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Electrical properties of Ag/PTFE nanocompositesnear percolation
resistivity variation by substrate elongation
0,000 0,001 0,002 0,003 0,004 0,0050
2
4
6
8
10
0,20 0,25 0,30 0,35 0,40 0,45100µ
100m
100
100k
100M
SP
EZ. W
IDE
RST
AND
(Ohm
*cm
)
Ag-FÜLLFAKTOR
Substratausdehnung
Wid
erst
and
[Ω] x
109
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Summary and outlook
Nanocomposites: - novel magnetic, optical, electrical,chemical properties
Vapor phase deposition: - wide range of size and filling,narrow size distrib., alloys
Demonstr.applications: - softmagnetic ultra-high frequency materials
- ultra-thin multiwavelengths color filters and sensors
Outlook: - sensors based on near-percolation effect and piezoelectric substrates
- reactive membranes
- tunneling magnetoresistance materials- ultra-high density magnetic recording - transparent magnetic nanocompositesFurther information: http://www.tf.uni-kiel.de/matwis/matv/
e-mail [email protected]
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Magnetic applicationInductive components in mobile communications
F - ( 0,8- 3GHz)Hysteresis losses and
limit of the cut-off frequencyBest solution- nanocomposite
high ρ ,Ms, fmoderate anisotropy
Ikeda et al - 2002 JAP(FeNiCo - J.o.M.a.M.M.)
~70 nm~6 nm
Single DomainParticles
Energy to create Bloch wall >saved magnetostatic energy
Eddy currents ~
ρ: resistivity d: particle diameter~10 nm
2w dρf ∝
S0kFMR MµHf ∝
Ferromagnetic resonance frequencyHk : anisotropy fieldMS : saturation magnetizationµ : permeability
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Tailoring the filling factor
• Substrate T• Deposition rates• Pinning
Metal volume fraction
1,5 2,0 2,5 3,0 3,5
0,05
0,10
0,15
0,20
0,25
fillin
g fa
ctor
, Con
dens
atio
n co
effic
ient
Ratio of deposition rates (M/P)
f c
polmet
polVm
fρρ
ρ−
−=
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Surface Processes
metal atoms arriving on substratea) adsorptionb) diffusionc) agglomerationd) desorptione) diffusion into bulkf) coalescence in bulkg) embedding of clusters
• substrate temperature• evaporation rates• condensation coefficient
Parameters
Nucleation also at defects and free radicals!V. Zaporojtchenko et al., Surface Sci. 532, 300 (2003)
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Teflon AF-Au composites
High filling even for extremely low sticking
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Polyimide-Cu composites
• Co-evaporation of monomers and Cu• Annealing ⇒ imidization + metal aggregation
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Alloy clusters
2,5 5,0 7,5 10,0 12,5 15,00
10
20
30
40
50
Volu
me
Frac
tion
(%)
Nanoparticle Size (nm)
(110)
bcc
(211)(200)
• No oxidation• narrow size distribution!
Patent pending
Fe-Ni-Co clusters in Teflon AF(elevated deposition T)
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Eddy current losses
Eddy currents limit cut-off frequency
2w dρf ∝ ρ: resistivity
d: feature size (particle diameter)
Nanoparticles for > 1GHz
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Magnetic poperties
Vibrating sample magnetometry and TEM
20 nm
200 nm Fe54Ni29Co17 / Teflon AF nanocomposite film
-200 -150 -100 -50 0 50 100 150 200
-2
-1
0
1
2 (b)
Mom
ent (
Tesl
a)
Field (mT)
No degradation effects after 3 months!
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High frequency permeability measurements
0,01 0,1 1 10
0
100
200
300
400
frequency / [GHz]
real part µ' imaginary part µ''
ac p
erm
eabi
lity
Cut-off frequency > 2 GHz
Preliminary results!
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Electrical properties near percolation
PTFE /Ag on glass
0,000 0,001 0,002 0,003 0,004 0,005
2,0G
4,0G
6,0G
8,0G
10,0GSilber-PTFE-Nanokomposit (Ag-Gehalt:33%) auf Polymersubstrat
Wid
erst
and
[Ω]
Substratausdehnung
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Multifunctional nanocomposites
Co-sputtering of Teflon and Ag
300 400 500 600 700 800
0,0
0,5
1,0
1,5
2,0
2,5
3,0sput. PTFE+Ag
407 nm
411 nm
Abs
orpt
ion
[a.u
.]Wavelength [nm]
filling factor 26% filling factor 21%
--- 20 nm
hydrophobic (Teflon) hard (crosslincing)antibacterial (Ag) colored (plasmons)
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Nanostructuring by selforganization
Self-cleaning by Lotus effect
Metal clusters as nanomaskson Teflon film + sputtering
hydrophobic nanoneedles
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Magnetic nanorods
50nm
Rods:a = 5 nmc = 100 nm
Application:Recording > 1 Tb/cm2
Fe-Ni-Co rods on Teflon-AFby co-evaporation
Patent pending
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Adelung, et al, Nature Materials, 3, 375 (2004)
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Summary and outlook
Nanocomposites: - novel properties: magnetic, optical, electrical, ....
Vapor phase deposition: - wide range of d and f, narrow size distrib., alloys
Demonstrated: - magnetic ultra-high frequency materials- ultra-thin multiwavelengths filters
Self-organization ⇒ : - Nanorods, wires, dotted wires, needles
Outlook: - orientation of easy axis and alloy tuning- ultra-high density magnetic recording- near-percolation sensors - reactive membranes- TMR materials- reactive membranes
Further information: http://www.tf.uni-kiel.de/matwis/matv/[email protected]
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FMR - Ferromagnetic resonance frequency
magnetic moment will not follow an AC drive field > fFMR
S0kFMR MµHf ∝k
SH
Mµ =
MS
Hk
easy axis
hard axisHk : anisotropy fieldMS : saturation magnetizationµ : permeability
aim: MS high +Hk moderate
FMR in GHz range
tradeoff
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Electrical properties of nanocomposites near percolation
resistivity variation by plastic substrate elongationtemperature coefficient of resistance (TCR) ~ 0.1 !!!
20 30 40 50 60 70 80 90 100 110
10k
100k
Resistivity of Nanocomposite near Percolation on Polymer Substrate
Res
istiv
ity (Ω
cm)
Temperature (°C)
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Surface plasmon resonance (SPR) in nanocompositesSurface Plasmon Resonance
metal–dielectric nanocomposite is excited by light, photons are coupled at the metal–dielectric interface, causing an induced charged density oscillation and shows a strong absorption maximum at a particular wavelength, called the surface plasmon resonance (SPR) or plasmon polariton.
• amount of metal concentration• shape, size, and spatial distribution• distance between the clusters• incorporated metal particles• sorounding dielectric medium
300 400 500 600 700 800-0,2
0,0
0,2
0,4
0,6
0,8
1,0
1,2
Abso
rban
ce (-
)
Wavelength (nm)
4 % 8 % 16 % 29 % 40 %
Au-Teflon AF
Increasing metal volume concentration leads a plasmonband maximum shift to longer wavelengths.