Effect of nanoscale geometry on molecular conformation: Vibrational Sum-Frequency Generation of...
-
Upload
eugene-leonard -
Category
Documents
-
view
217 -
download
1
Transcript of Effect of nanoscale geometry on molecular conformation: Vibrational Sum-Frequency Generation of...
Effect of nanoscale geometry on molecular conformation:
Vibrational Sum-Frequency Generation of alkaynethiols on metal nanoparticles
Achani Yatawara, Andrey N. Bordenyuk and Alexander V. Benderskii*
Department of ChemistryWayne State University
Detroit, MI 48202
by
Champika N. Weeraman
Nanoscale geometry – molecular conformation
►Expect a relationship between the substrate geometry (nano scale) and conformation of the adsorbed molecule
vs.vs.
Nanoscale geometry – molecular conformation
Flat surface
Curved surface
Molecular conformation in nanostructured materials
Bio sensors-bio markers
Aerosols
Gratzel-solar cells
P E ENL ( ) ( , , ) : ( ) ( )( ) 1 22
1 2 1 2
I PSFGNL
2 2 2 ( )
( )2 0
Sum-frequency generation (SFG) originates from induced polarization
g
e
Virtual State
2 ( )IR
1 ( )VIS ( )SFG
In media without inversion symmetry
SFG= IR+ vis
S()
SFG - CCD image
Spectrally narrow (temporally long) Vis pulse
IR
IR
vis
vis
Broad-band IR pulse
(temporally short)
+
( )2 0 In media with inversion symmetry
Vibrational sum frequency generation (VSFG)
►Broad band VSFG
Case II:
gauche defects
Case I:
all trans (zig-zag)
strong CH3 transitions,weak CH2 transitions
Flat Surface
Experiment
More CH2 transitions
Curved surface
Increase surface curvature
Change of Molecular conformationSFG sensitivity ?
8000
6000
4000
2000
0S
FG
inte
nsity
(a.
u.)
30002950290028502800IR frequency (cm
-1)
d+ r+ d- r+FR r-
►Strong CH3 stretch transitions (r+,r+FR,r-)
►Weak CH2 stretch transitions (d+,d-)►predominantly trans zig-zag molecule arrangement with few gauche defects
Chain length~1.6 nm
TEM images:1-DDT capped Au and AgNPs(I) Gold nanoparticles
(II) Silver nanoparticles
20 nm
(b)
20 nm
(c)
100 nm
(d)
20 nm
(a)
<d>=1.8 nm<d>=1.8 nm <d>=2.9 nm<d>=2.9 nm <d>=7.4 nm<d>=7.4 nm <d>=23 nm<d>=23 nm
20 nm
(a)
20 nm
(b)
100 nm
(c)
100 nm
(d)
20 nm
(a)
20 nm
(b)
<d>=1.8 nm<d>=1.8 nm <d>=3.6 nm<d>=3.6 nm <d>=7.9 nm<d>=7.9 nm <d>=24.6 nm<d>=24.6 nm
Meliorum Technologies, Inc.
d+ r+ d- r-op
VSFG 1-DDTcapped AuNps (SSP polarization)
► Both CH2 stretch and CH3 stretch transitions easily observable
► Increase of relative intensity of CH2 stretch vs. CH3 stretch with decreasing particle size
4
3
2
1
0
VS
FG
inte
nsity
(a.
u)
30002950290028502800
Frequency (cm-1
)
23 nm
7.4 nm
2.9 nm
1.8 nm
SFG Spectral Fitting: Quantitative analysis of SFG spectra
Bj = amplitudeΓj = Lorentzian line widthωj = transition frequencyANR= nonresonant contribution
Intensity of mode j; X BSSP j j,( )2 2 2
I X I ISFG SSP IR SSP IR IR IR vis vis ( ) ( ) ( ) ( )( ) 2 2
Intensity of SFG signal (SSP polarization, SFG-Vis-IR)
Effective non linear susceptibility: Multi-Lorentzian app.
X A eB
iSSP IR NRi j
j
( ) ( )( )
2
I R Гj
Гj
Size dependent SFG spectragauche defects
Chain length ~1.6 nm
d+/r+
1.1
1.0
0.9
0.8
0.7
0.6
Am
plitu
de r
atio
2520151050Mean Diameter (nm)
Chain length ~1.6 nm
d-/r-
3.0
2.5
2.0
1.5
1.0
0.5
0.0A
mpl
itude
rat
io2520151050
Mean Diameter (nm)
VSFG 1-DDT capped AgNPs (SSP polarization)VSFG 1-DDT capped AgNPs (SSP polarization)
4
3
2
1
0
Inte
nsit
y (a
.u)
300029502900285028002750
Frequency (cm-1
)
dd++ rr--(op)(op)dd--rr++
3.6 nm
7.9 nm
24.6 nm
1.8 nm►Transitions are broader than AuNPs(AuNPs: 10-12cm-1 AgNPs: 15-23cm-1)
► Weaker thiol-Ag bond compared to thiol-Au bond
2.0
1.5
1.0Am
plitu
de r
atio
2520151050Mean diameter (nm)
2.5
2.0
1.5
1.0
0.5d+/r+
d-/r-
R
L
RΦ
V aL0
x L R /
Cylindrical volumeCylindrical volume for alkyl chain for alkyl chain
Conical volumeConical volume between between spheres of radii spheres of radii RR and and R+LR+L
Additional volume Additional volume for for gauchegauche defects defects
ΦΦ = solid angle= solid angleLL = chain length= chain lengthRR = particle radius = particle radiusaa = area per head = area per head groupgroup
Size dependentSize dependent gauchegauche defectsdefects
V R L R 3
3 3( )Φ
( )RV V
Vx x
0
0
21
3
Trans- gaucheTrans- gauche free energy difference and Isomerization barrier are comparable to kT free energy difference and Isomerization barrier are comparable to kT
Geometrical modelGeometrical model
Size dependent gauche defects
R
L
RΦ20
0
1( )
3
V VR x x
V
/x L R
d+/r+
1.1
1.0
0.9
0.8
0.7
0.6
Am
plitu
de r
atio
2520151050Mean Diameter (nm)
d-/r-
3.0
2.5
2.0
1.5
1.0
0.5
0.0
Am
plitu
de r
atio
2520151050
Mean Diameter (nm)
0.6
0.4
0.2
Am
plitu
de r
atio
2520151050Mean diameter (nm)
0.5
0.4
0.3
0.2
0.1
0.0
d+/r+
d-/r-
dd++
rr--(op)(op)
dd--rr++
0.6
0.5
0.4
0.3
0.2
0.1
Am
plit
ude
rati
o
2520151050Mean diameter (nm)
1.2
1.0
0.8
0.6
0.4
0.2
d+/r+
d-/r-
VSFG spectra: Au and AgNPs (PPP polarization)
Gold nanoparticles Silver nanoparticles AuNPs
AgNPs
dd++
rr--(op)(op)dd--rr++
4
3
2
1
0
VS
FG
inte
nsit
y (a
.u.)
300029002800
Frequency (cm-1
)
1.8 nm
3.6 nm
7.9 nm
24.6 nm2.0
1.0
0.0
VS
FG
Int
ensi
ty (
a.u)
30002950290028502800
Frequency (cm-1
)
1.8 nm
2.9 nm
7.4 nm
23 nm
z
y
C3vθ
α
ψIRvis
SFG P
S
φ
x
ijk ijk lm nlm n
lm nN U( ),
( )( , , )2 2
X N d d d fijk ijk( ) ( )( , , ) ( , , )2 2
X N d fijk ijk( ) ( )( ) ( )2 2
I X eff ( )2 2
Euler matrix Molecularhyperpolarizability
Orientation angle (θ) Azimuthal angle (ψ) Torsional angle (φ)
Distribution function
Assumed random distribution for φ and ψ angles
SFG intensity
From experimental geometry and beam polarization
Molecular orientation analysis
1.2
1.0
0.8
0.6
0.4
0.2
0.0
d+
/r+
am
plitu
de ra
tio1801501209060300
c (deg)
A. SSP
B. PPP
Molecular orientation analysis
1.0
0.8
0.6
0.4
0.2
0.0
r+in
tens
ity
(SS
P)
1801501209060300
c (deg)
1.0
0.8
0.6
0.4
0.2
0.0
d+in
tens
ity
(SS
P)
1801501209060300
c (deg)
0 π
f(θ)
θθc
z
θc
θC3
z
AuNPsAuNPs
AgNPsAgNPs1.6
1.2
0.8Am
plit
ude
rati
o
2520151050Mean diameter (nm)
0.6
0.5
0.4
0.3
0.2
0.1d
+/r
+(SSP)
d+/r
+(PPP)
1.6
1.4
1.2
1.0
0.8
0.6Am
plit
ude
rati
o
2520151050Mean Diameter (nm)
0.7
0.6
0.5
0.4
0.3
0.2
0.1
d+/r
+(SSP)
d+/r
+(PPP)
0 π
f(θ)
θθc
z
θc
θC3
z
Conclusions
►Alkylthiols on nanoscale materials (gold and silver Nps) possess significant amount of gauche defects comparing with the SAM on planar gold
► Increasing amount of gauche defects with decreasing particle size can be understood in terms of the conical volume available for the chain on a curved surface
► Vibrational sum frequency generation is a powerful spectroscopic tool to characterized the molecular conformation on nanostructured materials
AcknowledgementAcknowledgementss
The GroupThe GroupAdvisor: Advisor: Prof. Alex V. BenderskiiProf. Alex V. Benderskii
Dr. Andrey N. BordenyukDr. Andrey N. Bordenyuk
Dr. Igor StiopkinDr. Igor StiopkinHimali D. JayethilakeHimali D. JayethilakeAchani K. YatawaraAchani K. YatawaraFadel Y. ShalhoutFadel Y. ShalhoutAdib J. SaminAdib J. Samin
WSU start-up grantWSU research grantNano@Wayne
ACS-PRFGrant No.40868-G6
NSF CAREER Grant No. 0449720
Funding
Professor Winters’ group-WSUDr. Charles Dezalah
ECE-WSUProf. G. AunerDr. J. Smolinski
CIF-WSUDr. Yi LiuDr. Sam Shinozaki
Surface curvature Chain lengthVSFG spectra: 5nm AuNPs VSFG spectra: 50nm AuNPs
3.0
2.5
2.0
1.5
1.0
0.5
0.0
Inte
nsit
y (a
.u)
2960292028802840
Frequency (cm-1
)
C2-thiol
C12-thiol
C18-thiol
C6-thiolC6-thiol
C2-thiol
2.5
2.0
1.5
1.0
0.5
0.0
Inte
nsit
y (a
.u)
2960292028802840
Frequency (cm-1
)
C12-thiol
C18-thiol
1.0
0.8
0.6
0.4
0.2
0.0
r+in
tens
ity
(SS
P)
1801501209060300
c (deg)
1.0
0.8
0.6
0.4
0.2
0.0
d+in
tens
ity
(SS
P)
1801501209060300
c (deg)
1.2
1.0
0.8
0.6
Am
plit
ude
rati
o
2520151050Mean Diameter (nm)
d+/r
+
1.6
1.2
0.8
Am
plit
ude
rati
o
252015105Mean diameter (nm)
d+/r
+
AuNPsAuNPs
AgNPsAgNPs
dd++rr++
rr--(op)(op)
dd--
2.0
1.5
1.0
0.5
0.0
Abs
orba
nce
(a.u
)
30002950290028502800Frequency (cm
-1)
1.8 nm
2.9 nm
7.4 nm
23 nm
dd++ rr--(op)(op)
rr++dd--
2.5
2.0
1.5
1.0
0.5
0.0
Ram
an I
nten
sity
(a.
u)
30002950290028502800Raman Shift (cm
-1 )
1.8 nm
2.9 nm
7.4 nm
23 nm
IR and Raman spectra: 1-DDT gold nanoparticlesIR and Raman spectra: 1-DDT gold nanoparticlesIR spectraIR spectraRaman spectraRaman spectra
No size dependent spectral featuresNo size dependent spectral features
Possible interpretations: Possible interpretations: 1.1. Increasing fraction of Increasing fraction of gauchegauche
defects (SFG propenisty rules)defects (SFG propenisty rules)
2. Heterogeneity of local fields 2. Heterogeneity of local fields E(E(ωω))
E(ω, r)
r
No size-dependence in Raman spectra (should have same EM enhancement) Far off resonance:
λSPR~520 nm λSFG=665 nm
SFG Raman
IR
vis SFGpump Stokes
|v=0
|v=1
SSP polarization
1000
500
0
VS
FG
Inte
nsity
(a.
u.)
30002950290028502800Frequency (cm
-1)
CdSe
aac bbc ccc( ) ( ) ( ). , .2 2 23 4 0 1 0 0 aac bbc ccc
( ) ( ) ( ). , , .2 2 22 0 0 0 1 0 0
X L L L Xeffssp
y sfg y vis z IR yyz( ) , ( )( ) ( ) ( ) sin( )2 2
L L L Xz sfg x vis x IR sfg vis IR zxx( ) ( ) ( ) sin( ) co s( ) co s( )
X L L L Xeffppp
x sfg x vis z IR sfg vis IR xxz( ) , ( ) ( ) ( ) co s( ) co s( ) sin( )2
L L L Xx sfg z vis x IR sfg vis IR xzx( ) ( ) ( ) co s( ) sin( ) co s( )
L L L Xz sfg z vis z IR sfg vis IR zzz( ) ( ) ( ) sin( ) sin( ) sin( )
Molecular orientation analysis
Non-vanishing molecular hyperpolarizability C3v (r+)
Non-vanishing molecular hyperpolarizability C2v (d+)
Effective for polarization combination sfg-P, vis-P and IR-P X ( )2
Effective for polarization combination sfg-S, vis-S and IR-P X ( )2
Molecular orientation analysis
0.110
0.105
0.100
0.095
0.090
0.085
Inte
nsi
ty r
atio
(d
+/r
+)
150100500θc degrees
SSP polarization PPP polarization
0.070
0.060
0.050
0.040
0.030
0.020In
tens
ity r
atio
(d
+/r
+)
15010050θc degrees
►Qualitatively explains less intense d+ modes in PPP spectra for broad distribution of tilt angle θ.
800 nm40 nm bandwidth
803 nm26 nm bandwidth40 fs2 mJ/pulse, 1 kHz
Reflection geometry
IR output: 3-8 m 65-75 fs300 cm-1 bandwidth1-2 J/pulse
0.1 m precision
Shaped vis pulse:bandwidth 6 cm-1 Chirp control
Fs oscillator
Regenerative amplifier
2-pass amplifier
OPA with DFM
Optical delay stages
Sample
Monochromator
LN2-cooled CCD
Vis pulse shaping
Experimental Setup
OPA
Delay stages
Vis pulse shaping
Sample
CCD