2) Stimuli 2) Stimuli responsiveresponsive polyelectrolytepolyelectrolyte coatingscoatings
Samuel Dodoo, Anna Burmistrova, Kornelia Gawlitza, Adrian Carl, Marcel Richter, Regine v. Klitzing
Stranski-LaboratoriumTechnical University of Berlin, Germany
Polymer coatings: MotivationPolymer coatings: Motivation
Nano- and Mesoscopic polymer films (thickness: 1 – 1000 nm)External stimuli: temperature, ionic strength, pH, humidity …
Sensitivity <=> Stability
Design and characterisationof stimuli responsive
surface coatings
CH3 CH3
OCH3
N*
N+
*
Cl
n
m
CH3
**
SO 3
n
Na+-
**
NH3
n
Cl+
*
n
OR
OO
OR
OOO
OROR
OR
OR
R=COO-Na+
Decher, G.; Hong, J.D.; Schmitt, J. Thin Solid Films 1992, 210, 831.
OR
OO
OH
OO
OHOH
CH2 OH
CH2OCH2CH2OH
O(CH2CH2O)2
CH2CHCH2
OH
N+
CH3
CH3
CH3
Cl
Polycations Polyanions
JR400
PAH
CMC
P(DADMAC-NMVA)
PSS
HA
LayerLayer--byby--layer techniquelayer technique
1) Ion 1) Ion specificspecific EffectsEffects
=> Increasing interaction between anions and polycations
0 2 4 6 8 10 12
0
100
200
300
400
500
600
700
Cl-
F-
Thic
knes
s, d
/ Å
Number of layers, N
Br-
Ion specific effects: Effect of anionsIon specific effects: Effect of anions
Increasing ion diameter (decreasing hydration shell)
PSS/PDADMAC
[NaX]=0.25mol/l Si
coiled
dBr-Br-
Br- Br-
Si
flatd
F-
F-
F-
J.E. Wong, R.v.K, Macromolecules, submitted
Ion specific effects:Ion specific effects: AFM studiesAFM studies
(PSS/PDADAMAC)6 prepared in 0.25 mol/l salt
NaCl
RMS 15 Å
CsClNaBr
25 Å 21 Å
Increasing roughness
with increasing ion size
J.E. Wong, R.v.K, Macromolecules, accepted
Different types of multilayer growingDifferent types of multilayer growing
0 2 4 6 8 10
thic
knes
s
number of layers
Kovacevic et al., Langmuir, 2002Biesheuvel et al. Langmuir, 2004Garza et al. , Langmuir 2004
-+-+-+-
+Si
linear
Different types of multilayer growingDifferent types of multilayer growing
0 2 4 6 8 10
thic
knes
s
number of layers
Kovacevic et al., Langmuir, 2002Biesheuvel et al. Langmuir, 2004Garza et al. , Langmuir 2004
-+-+-+-
+Si
linear
exponential
Different types of multilayer growingDifferent types of multilayer growing
0 2 4 6 8 10
thic
knes
s
number of layers
Kovacevic et al., Langmuir, 2002Biesheuvel et al. Langmuir, 2004Garza et al. , Langmuir 2004
-+-
+Si
2 4 6 8 10 120
100
200
300
400
500
600
700 100%, 0.1 mol/l 75%, 0.1 mol/l
th
ickn
ess
/ Å
number of adsorbed layers
Preparation in NaBr, 2 different PDADMAC charge densities
Effect of degree of chargeEffect of degree of charge
2 4 6 8 10 120
100
200
300
400
500
600
700 100%, 0.1 mol/l 75%, 0.1 mol/l 100%, 0.25 mol/l
th
ickn
ess
/ Å
number of adsorbed layers
Preparation in NaBr, 2 different PDADMAC charge densities
Effect of ionic strengthEffect of ionic strength
Transition from linear to exponential increase by increasing ionic strength
2 4 6 8 10 120
100
200
300
400
500
600
700 100%, 0.1 mol/l 75%, 0.1 mol/l 100%, 0.25 mol/l 75%, 0.25 mol/l
th
ickn
ess
/ Å
number of adsorbed layers
Preparation in NaBr, 2 different PDADMAC charge densities
Effect of degree of chargeEffect of degree of charge
Effect of polymer charge density on the type of growth
2 4 6 8 10 120
100
200
300
400
500
600
700 75%, 0.25 mol/l NaBr
th
ickn
ess
/ Å
number of adsorbed layers
Effect of type of saltEffect of type of salt
2 4 6 8 10 120
100
200
300
400
500
600
700 75%, 0,25 mol/l NaBr 75%, 0,25 mol/l NaCl
th
ickn
ess
/ Å
number of adsorbed layers
Comparison NaBr <-> NaCl
Tuning of type of growth by changing salt during preparation
Effect of type of saltEffect of type of salt
)Dtx(
πDtMC(x,t)
4exp
2
2−=
Deposition of the probing layer
O
O
O
NH
O OH
SC
**
NH3
m *
*
NH3
n
-20 -10 0 10 2020
40
60
80
100
120
140
160 after bleaching after treatment
Gre
y va
lue
/a.u
.
Distance/µm
Mobility: Fluorescence Recovery after Mobility: Fluorescence Recovery after PhotobleachingPhotobleaching (FRAP)(FRAP)
Polyanion/polycation D / cm2/sPSS/PAH < 10-15
PSS/PDADMAC 10-14
PSS/PDADMAC (75 %) 10-13
PSS/PDADMAC (NaBr) 10-13
HA/PDADMAC 10-11
FITC-PAH
P. Nazaran, R.v.K. et al. J. Phys. Chem B (2007)
Internal structure: Exposure to high ionic strengthInternal structure: Exposure to high ionic strength
0 2 4 61E-5
1E-4
1E-3
0.01
0.1
1
0.4 0.8 1.2 1.6 2.0 2.4 2.8
1E-4
1E-3
0.01
D2O 1M NaCl 3M NaCl 4M NaCl
Ref
lect
ivity
tth / deg
tth / deg
Ref
lect
vity
silicon substrate
td
Si/PEI/[(PSS/PAH)2/d-PSS/PAH]6
0 1 2 3 4
1.00
1.02
1.04
1.06 t d
Nor
mal
ized
thic
knes
s
NaCl concentration / M
⇒ Film swelling for cNaCl ≥ 3 M⇒ Non-homogeneous swelling
R. Steitz, R.v.K. (Adam, ILL Grenoble)
Swelling: Swelling: ““freefree”” water vs. water vs. ““voidvoid”” water (neutron water (neutron reflectometryreflectometry))
d2/d1 φfree φvoid φtotal
(PSS/PDADMAC)9 1.79 0.44 0.10 0.54
(PSS/PAH)9 1.60 0.38 0.11 0.49
(PSS/PAH)9/PSS 1.57 0.36 0.10 0.46
d1
D2O liquid or vapor
d2
φfree
φvoid
Silicon substrate
d1
vacuum
S. Dodoo, J.E. Wong, R. Steitz, R.v.K.
Swelling in water: Effect of preparation parametersSwelling in water: Effect of preparation parameters
S. Dodoo, R. Steitz, R.v.K.
0,2
0,3
0,4
0,5
0,6 0.10 M 0.25 M 0.50 M
wat
er c
onte
nt
NaF NaCl NaBr
(PSS/PDADMAC)6
Addition of different amount and type of salt during preparation
=> Increasing water content with increasing ionic strength
and increasing anion polarizibility
Intrinsically compensatedLess mobile (Glassy)Lower amount water
Low Ionic strengthChloride ion100% charged PE
High Ionic strengthBromide ion75% charged PE
Extrinsically compensatedMore mobile (Liquefied)Higher amount of water
Conclusion: ion specific effectsConclusion: ion specific effects
Treatment:Dissolution of complexes byIncreasing ionic strength (stronger for bromide)
Preparationconditions
2) 2) TemperatureTemperature effectseffects
Temperature induced increase in the mobility:
Transition from a glassy state to a swollen and liquefied structure accompanied with softening of the film.
0 .1M N aC l 1M N aC l 0 .1M N aB r 1M N aB r10 -15
10 -14
10 -13
10 -12
Ion ic cond ition o f film p repa ra tion
Diff
usio
n co
effic
ient
/ cm
²/sec
R oom tem p. 65° C
Effect of heatingEffect of heating
(PSS/PDADMAC[75%)])6 against water
DADMAC
N+
CH3CH3
Cl
Na-SS
Na+
SO3
O NH
CH3CH3
NIPAM
O NH
CH3CH3
SO3 H+
AMPS
OO
N
CH3CH3
+
DEAEM
• Block-copolymers
• statistical copolymers
EffectEffect of of chargecharge distributiondistribution: : NIPAMNIPAM--copolymerscopolymers
U. Voigt, V. Khrenov, K. Tauer, M. Hahn, W. Jaeger, R. v.K., J. Phys: Condens. Matter (2003)
0,00 0,02 0,04 0,06 0,0810-4
10-3
10-2
10-1
100
101
102
103
104
20 °C 40 °C 50 °C 60 °C
I/I0
Q [Å-1]
-100 0 100 200 500 600
2
3
4
5
6
7
D2O
Si
20 °C 40 °C 50 °C 60 °C
Nb
x 10
-6 [Å
-2]
z [Å]
Neutron reflectometry at solid/liquid interface: (PSS-b-PNIPAM/PDADMAC)n
Small decrease in thickness
Irreversible shrinking process
Irreversible annealing of the film
=> Strong interdigitation
10 20 30 40 50 60560
565
570
575
580
585
590
595
600
Film
thic
knes
s [Å
]
Temperature [°C]
R. Steitz, V. Leiner, K. Tauer, V. Khrenov, R.v.K. Appl. Phys. A (2002)
Effect of temperature on solvent swollen films Effect of temperature on solvent swollen films - +
Stimuli responsive coatings Stimuli responsive coatings
Strategy: Formation of stimuli-repsonsive coating by adsorption of microgel particles
=> Effect of geometrical confinement on sensitivity
ΔT ΔpH?
in bulk at interfaces
? ΔpH, ΔT
Hydrogel microparticles
Control of Control of hydrogelhydrogel particle densityparticle density
Explanation for 2D pattern: • Capillary attraction vs. dipolar repulsion• Shrinking of swollen (single) particles
After spin coating, pH 2
After rinsingin pH 2
S. Schmidt, T. Hellweg, H. Motschmann, R. v. K. Polymer (2008)
P(NIPAM-co-AA) particles on Si/PEI
0,2 0,4 0,6 0,8 1,0 1,2
1E-4
1E-3
0,01
0,1
1
0,4 0,5 0,6
0,01
0,02
0,03
0,04
Ref
lect
ivity
theta / deg
25°C 40°C 25°C
Ref
lect
ivity
theta / deg
Swelling / shrinking of Swelling / shrinking of hydrogelhydrogel particlesparticles
Neutron reflectometry => reversibility
(HMI 2006)
P(NIPAM-co-AA) particles (pH = 2)Ellipsometry => decrease in LCST
25°C, air 25°C, H2O 55°C, H2OSFM (amb./liquid) => Compactisation (T > LCST)
400 nm: 90% D2O200 nm: 80% D2O
15 μm
S. Schmidt, T. Hellweg, H. Motschmann, R. v. K. Polymer (2008)M. Karg, T. Hellweg, R.v.K. et al. Langmuir (2008) S. Schmidt, T. Hellweg, R.v.K., Langmuir (2008)
Fresh from the labFresh from the lab: Fluctuation length close to phase transition: Fluctuation length close to phase transition
GISANS (D16, ILL Grenoble)6.-17.11.2008
15 20 25 30 35 40 45 50 55 600
1
2
3
4
ξ / n
mT / °C
M. Medebach, R.v.K., Cooperation: P. Müller-Buschbaum, TU Munich
=> Increase in fluctuation length ξ close to Tc
Tc
P(NIPAM-co-AA) particles on Si/PEI (pH = 6)
Ornstein Zernike => fluctuation length ξ
Zone close to the surface
remains unaffected
Conclusion: Temperature sensitivityConclusion: Temperature sensitivity
Polyelectrolyte multilayers:
•Sensitivity to temperature rather low due to
interdigitation
Thermosensitive coatings by adsorption of hydrogel microparticles
• Control of particle density
• Reversible shrinkage and swelling
• Small shift of the LCST to lower temperature
• Unchanged interphase between solid surface
and „continuum“ of the particle
ΔT
-+-+-+-
+Si
New strategies for embedded biocatalysts:• Stabilisation of catalyst• Selective permeability• Easy separation• Fast response to external stimuli
Current projectsCurrent projects
Cooperation:CoE „Unicat“ (Berlin-Potsdam):M. Ansorge-Schumacher TU BerlinH. Möhwald MPI-KG, PotsdamRainer Haag, FU Berlin
Self-assembly at interfaces (bottom up)
GISANS: new set-up
at ISIS (BMBF project)
Patterned surfaces
10 – 50 nmhν (VIS)
Actuation by lightAu particles
(-> Photovoltaics)