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Surface Enhanced Raman Spectroscopy SERS

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Title: Surface Enhanced Raman Spectroscopy SERS


1
Surface Enhanced Raman Spectroscopy (SERS)
  • BMEN 489/689

2
Raman Spectroscopy Review
  • Allows indirect probing of vibrational states
    in molecules.
  • Unique spectral signatures provide means of
    molecular identification
  • Used extensively for identification of chemical
    constituents in liquid mixtures (i.e. in
    petroleum industry)
  • Can be used in biomedicine as well

3
Optical Activity in Molecules
  • Rotational Spectra Molecular system rotates
    about axis perpendicular to internuclear axis
    (low energy)
  • Vibrational Spectra Nuclei vibrate about
    equilibrium positions (medium energy)
  • Electronic Spectra Change in electronic
    configuration (high energy)

4
Vibrational Spectra
  • Quantum mechanics tells us we get discrete states
    within the potential well
  • For parabolic well En (n½)h?0

5
Electronic Spectra
  • Optical absorption emission arises from change
    in electronic configuration

6
Vibrational Spectroscopy
  • Vibrational states can be accessed utilizing two
    methods
  • Infrared Spectroscopy Direct absorption of low
    energy light
  • Raman Spectroscopy Inelastic scattering with
    energy transfer to molecule (Stokes Line) or
    energy transfer from the molecule (anti-Stokes
    Line)

7
Vibrational Spectroscopy
  • CO2 Example
  • Infrared active is permanent dipole moment
    changes as in bending
  • Raman active if polarizability changes as in
    symmetric stretch

8
Vibrational Spectroscopy
  • Raman and Infrared spectroscopy are complementary
    due to selection rules
  • Highly symmetric polyatomic molecules with center
    of inversion are IR active
  • Homonuclear diatomic molecules are Raman active
  • Non-symmetric molecules demonstrate both
    modalities

9
Raman Spectroscopy
  • Briefly descend into the math
  • Induced dipole
  • µind aE0cos(?t)
  • Polarizability
  • a a0 a1cos(?1t)
  • Internal motion modulates the induced dipole
    moment
  • µind a0 E0cos(?t) Rayleigh
  • ½ a1E0cos(? - ?1)t Stokes
  • ½ a1E0cos(? ?1)t anti-Stokes

10
Raman Spectroscopy
  • Both rotational and vibrational states can be
    observed but rotational states are difficult to
    spectrally separate
  • Uses inelastic scattering

?
?
Stokes band transfers energy to the molecule
11
Raman Spectrum (Shift)
  • Cycloxenane excited at 1064nm
  • Spectrum independent of excitation
  • Exact peak values depend on molecular conformation

12
Raman Spectroscopy
  • Generally, the Raman intensity, IR, can be
    written as
  • However, sR tends to be very small (i.e.
    10-30cm2/molecule)
  • So, we have to use lots of laser power and wait a
    long time

13
Surface Enhanced Raman
  • In the 1970s, it was observed that rough metal
    surfaces produced enhanced Raman signals (up to
    106)
  • Observations
  • Required roughened (10-100nm) surface of highly
    reflective metals
  • Raman intensity generally falls off with
    increasing vibrational frequency
  • Raman shifts are sometimes shifted from standard
    Raman and new peaks appear

14
Surface Enhanced Raman
  • The effect was also observed in metal
    nanoparticles (NP) we will use this as the
    basis for our explaination
  • Recall the dielectric function for a metal
  • At resonance for NP
  • em -2 eH

15
Surface Field Enhancement
  • At resonance, we also observe a field enhancement
    at the surface of the NP when in resonance

Kelly et al., J. Chem. Phys. B 107, 668 (2003).
16
Surface Field Enhancement
  • So, the particle acts as an antenna and
    concentrates the incident field at the
    nanoparticle surface can be 10-100x
  • Can plot the Poynting vector of the incident
    radiation and absorption around the sphere

Below resonance, particle polarizes in phase and
thus reduces the field inside and slightly
increases field outside
As resonance, particle polarizes resonantly and
greatly enhances the field at the particle
17
Surface Field Enhancement
  • Additionally, the nanoparticle enhances the Raman
    scattered field as well can be 10-100x as well
  • Overall, the Raman signal actually experiences a
    surface enhancement proportional to

Can be 108!
18
Field Decay
  • If we move away from the surface, the dipole
    decay has to be considered
  • Single molecule
  • Monolayer

19
Surface Enhanced Raman
  • So what does this tell us?
  • Want em to be small (low loss) near the
    resonance metals
  • Because signal depends on both E2laser(?) and
    E2Raman(?), as ?-? gets larger, G will get
    smaller since the resonance condition is NOT met
    at both ? and ?

20
Chemical Enhancement
  • When molecules are adsorbed to the surface, their
    electronic states can interact with the states in
    the metal and produce new transitions
  • True nature of this still not fully understood
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