Effect of Thin Coatings on Surface Plasmon-Enhanced Infrared Spectroscopy using Ni Mesh Microarrays...
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Transcript of Effect of Thin Coatings on Surface Plasmon-Enhanced Infrared Spectroscopy using Ni Mesh Microarrays...
![Page 1: Effect of Thin Coatings on Surface Plasmon-Enhanced Infrared Spectroscopy using Ni Mesh Microarrays Kenneth R. Rodriguez, Shannon Teeters- Kennedy, Hong.](https://reader036.fdocuments.us/reader036/viewer/2022062309/56649ed35503460f94be3ce5/html5/thumbnails/1.jpg)
Effect of Thin Coatings on Surface Plasmon-Enhanced Infrared
Spectroscopy using Ni Mesh Microarrays
Kenneth R. Rodriguez, Shannon Teeters-Kennedy, Hong Tian, Joseph Heer, Katie
Cilwa, and James V. Coe
Presentation for the 62nd Annual Spectroscopy Symposium
Ohio State UniversityJune 21, 2007
![Page 2: Effect of Thin Coatings on Surface Plasmon-Enhanced Infrared Spectroscopy using Ni Mesh Microarrays Kenneth R. Rodriguez, Shannon Teeters- Kennedy, Hong.](https://reader036.fdocuments.us/reader036/viewer/2022062309/56649ed35503460f94be3ce5/html5/thumbnails/2.jpg)
Presentation Overview
Surface Plasmons Extraordinary Transmission Surface Plasmon Spectroscopy (SPEIRA) Effect of Coatings TiO2 Coatings – Film Thickness Hexadecane Coatings – Stark Shifts
![Page 3: Effect of Thin Coatings on Surface Plasmon-Enhanced Infrared Spectroscopy using Ni Mesh Microarrays Kenneth R. Rodriguez, Shannon Teeters- Kennedy, Hong.](https://reader036.fdocuments.us/reader036/viewer/2022062309/56649ed35503460f94be3ce5/html5/thumbnails/3.jpg)
Analogies: Raindrops and Radio Waves
Raindrop transfers momentum and energy into waves on water surface
Raindrop Photo courtesy of M. Holt
e-
Electron transfers momentum and energy into waves of conducting electron plasma on metal surface. These waves are called “surface plasmons”
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Radio Waves, Plasmons, and Extraordinary Transmission
Radio waves cause oscillating surface currents in antenna, which can travel past transmission barriers
Transmitting antennas can “recreate” original radio waves from the oscillating currents.
Similarly, surface plasmons can carry light past “optically thick” metal films such as our Ni mesh.
O
pti
cally
thic
k
meta
l
Incoming Light
“Transmitted” Light
Surface Plasmon propagation
Radio Wave
Connecting Wire
Non-t
ransm
itti
ng
Barr
ier
Oscillating currents in metal surface
Radio Wave
3 m Thick
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Extraordinary Infrared Transmission1 using Nickel Mesh
6.5m
12.7m
6.5m
3 m thick
26% Open area
77% Light Transmitted at Primary Resonance
1 Ebbesen et. al., Nature, 391 (1998) 667; Williams et al., J. Phys. Chem. B 107 11871-79 (2003) 11871-79
69% of light that hits metal gets transmitted!
- + - + -
(1,0)+ Peak from SymmetricFront-Back Plasmon Coupling
- + - + -
+ - + - +
(1,0)- Peak from AsymmetricFront-Back Plasmon Coupling
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Advantages of Mesh-Based SPEIRA
SPEIRA (Surface Plasmon-Enhanced InfraRed Absorption) has the following advantages:
1) Enhanced Absorption Pathlengths (10 m, not 10 nm)2) Enhanced Surface Selectivity (Plasmons confined to
surface)3) Enhanced Electric Fields (3-D light energy “squeezed”
into 2-D) 4) Enhanced Access to NanoSpaces (Plasmons < 1 nm
Thick)At a very low cost! (~$300 / sheet )
![Page 7: Effect of Thin Coatings on Surface Plasmon-Enhanced Infrared Spectroscopy using Ni Mesh Microarrays Kenneth R. Rodriguez, Shannon Teeters- Kennedy, Hong.](https://reader036.fdocuments.us/reader036/viewer/2022062309/56649ed35503460f94be3ce5/html5/thumbnails/7.jpg)
“Infinite” Transmission Enhancement
![Page 8: Effect of Thin Coatings on Surface Plasmon-Enhanced Infrared Spectroscopy using Ni Mesh Microarrays Kenneth R. Rodriguez, Shannon Teeters- Kennedy, Hong.](https://reader036.fdocuments.us/reader036/viewer/2022062309/56649ed35503460f94be3ce5/html5/thumbnails/8.jpg)
TiO2 NanoCoatings
Compare to Raether’s Fig. 2.1.7
incidence
No angling
Coating Shift
Radiation Damping Shift
Rodriguez et al., JCP, In Press (2007)
•Resonance Shifts with Coating
•Transmission Attenuation (1-sided coating)
•Broader Resonances as measured by FWHM
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0 10 20 30 40 50 60 70 80 90 100 110Thickness (nm)
0
5
10
15
(1,0)+
Resonance Shifts due to Nanocoatings at incidence
)(radiation~x
Front-Back Coupling through the Holes
~
coating
...n)interactio(~ x
0
60
9075
105
)coating(~x x~
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`m `s `d C D
Ni/NiO -150 35 1 0.62 42
Ni -1965 35 1 0.14 20
`m ,s-67 7 1 0.76 24
22
32212
21)0,1(
~)(
724~)(
05.078.0~ dnmcm
dnmcm
Calculated fit for (1,0)+
~
-(
cm-1)
~
6.2cm-1 shift of the 105 nm TiO2 coating simulated
22
32
2 ~~~ dDdC Pockrand’s Theoretical Model for Coating Shift
I. Pockrand, Surf. Sci., 72, 577, (1978).
C & D values calculated from dielectric permittivities of Ni, TiO2, and Air
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Interaction of SP with a Vibration
Rodriguez et al., JCP, 126, 151101-5 (2007)
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Interaction of SP with a Vibration
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Stark Effects with FTIR Spectrometer
Stark shift of up to 3 cm-1 observed when CH2 rocking vibration near Plasmon Resonance
Hexadecane CH2 Rocking Vibration
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Conclusions
We can measure coating thicknesses and characterize oxidation using simple FTIR measurements on inexpensive mesh substrates.
We can generate Stark shifts of up to 3 cm-1 and get increased transmission due to interactions of surface plasmons with excited molecular vibrations in liquid films.
Mesh-based SPEIRA is a powerful and useful tool for spectroscopy on or near surfaces.
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ACKNOWLEDGEMENTS
Jim Coe (PI)
Kenneth
Rodriguez
Shannon Teeters- Kennedy
Katie Cilwa
Joe Heer
Hong Tian
CHE0413077