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Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University of Colorado, Boulder Funded by the National Science Foundation

Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

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Page 1: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes

Peter Andersen and Kathy RowlenDepartment of Chemistry and Biochemistry

University of Colorado, Boulder

Funded by the National Science Foundation

Page 2: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

1970’s surface enhanced Raman scattering

1980’s 106 enhancement of Raman scattering

1980’s second harmonic generation

1997 1014 enhancement of Raman scattering

2000 106 enhancement of fluorescence in nanorods

2001 surface plasmon optics

Surface Plasmons: coherent oscillations of electron density at metal/dielectric interface

Enhanced Optical Processes from Nanometric Noble Metal Particles

Page 3: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Enhanced Optical Transmission

Ebbesen et al. “Extraordinary Optical TransmissionThrough Sub-Wavelength Hole Arrays”

Nature, 1998, 391, 667-669

Page 4: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Saloman et al. Phys. Rev. Lett. 2001, 86(6), 1110

• 200 nm Ag film v.d. onto quartz• focused ion beam lithography• 150 nm holes• 600 nm to micron spacing

Page 5: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Ghaemi et al. Phys. Rev. B 1998, 58(11), 6779

Page 6: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Thio et al., J. Opt. Soc. Am. B., 1999, 16(10), 1743

Measured Near-Field Distribution

Closest to simulated c (previous), hole d = 500 nm

Page 7: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Ebbesen et al. Nature 1998, 391,667

• 200 nm thick Ag• 150 nm holes• 900 nm spacing

• Transmission efficiency =fraction of light transmitted/fraction of surface area holes = 2.

• More than twice the lightthat impinges on the holes is transmitted through the film!

Page 8: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Ebbesen et al. Nature 1998, 391,667

• Hole spacing determines peak position

•Peak position independent of hole d

• Independent of metal (Ag, Cr, Au)

• Must be metal (Ge doesn’t work)

Page 9: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

T scales with d2, independent of

versus (d/ )4 for Bethe sub- aperture

=500 nm

Page 10: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Not cavity resonance since peak position (in spectrum)does not significantly depend on hole dimensions

Not waveguiding because film thickness too small (200 nm)

Surface plasmon tunneling?

Surface plasmon scattering?

Enhancement / Transport Mechanism?

Page 11: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

•For a surface that can support a surface plasmon, the wave vector, ksp is:

 

 •The difference between the in-plane wave vector of light,

ki, and the surface plasmon wave vector, ksp, can be

compensated for by diffraction on periodic surface structure: 

2/1

2

sm

smi

spk

max 2 2( , )

m s

m soi j ai j

min 2 2( , ) s

oi j ai j

Page 12: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University
Page 13: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Grupp et al., Appl. Phys. Lett. 2000, 77(11), 1569

Ag

Ag/Ni

Ni

Page 14: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Grupp et al., Appl. Phys. Lett. 2000, 77(11), 1569

Transmission relatively independent of wall metal

Page 15: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Sonnichsen et al., Appl. Phys. Lett. 2000, 76(2), 140

Further evidence for surface plasmon involvement

Page 16: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Sonnichsen et al., Appl. Phys. Lett. 2000, 76(2), 140

Page 17: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Saloman et al. Phys. Rev. Lett. 2001, 86(6), 1110

Left: Calculated near-fieldtransmission intensity[(c) = 300 d, 900 nm a, 800 nm ]

Calculated intensityenhancement nearhole edge ~ 500x

15 nm above 100 nm above

Page 18: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Thio et al., Physica B, 2000, 279, 90

Page 19: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Grupp et al. Adv. Matr. 1999, 11(10), 860

Page 20: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Thio et al., Physica B, 2000, 279, 90

Surface Plasmon Activated Devices

Page 21: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Grupp et al. Adv. Matr. 1999, 11(10), 860

Transmission through single holewith array of dimples

Single hole in smooth surface

Page 22: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Thio, Lezec, Ebbesen Physica B, 2000, 279, 90

For coherent 670 nm lightT is 60x greater than typicalNSOM tapered fiber with200 nm aperture

Page 23: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Applications, Applications, Applications!

Reflection mode?

SERS at edges?

Field in channel?

Page 24: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Surface Plasmon Optics:

• use SP’s for manipulation of optical fields

• SP lenses, mirrors and flashlights (e.g., Smolynaninov et al. Phys. Rev. B. 1997, 56(3) 1601-1611.)

Page 25: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Optical Enhancement via Surface Plasmon Coupling

h Field enhanced detection region

Light harvesting indentations

Surface plasmon mirrorTransmission channel

Surface plasmon lense

Page 26: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Si substrate Spin coat substrate with PMMA resist

Expose to electron beam

Develop in MIBK/IPA

Metalize by vapor deposition

Electron-Beam Nanolithography (Peter Andersen)

Page 27: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Reflection Grating Behavior

Page 28: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

First Attempt: Top-View AFM

Page 29: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

AFM Micrograph of Second Attempt!

Page 30: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

target ao 450 nm measured ao 450 nm

Grating Constant (ao)

Page 31: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

Lens Pinhole Au MirrorNd:YAG Laser

= / 2sin

Photolithography (Michele Jacobson)

Page 32: Magnificent Optical Properties of Noble Metal Spheres, Rods and Holes Peter Andersen and Kathy Rowlen Department of Chemistry and Biochemistry University

To be continued…..