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Sub-Diffraction Raman imaging by Near-Field Optical Microscopy

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Sub-Diffraction Raman imaging by Near-Field Optical Microscopy P. G. Gucciardi, S. Trusso, C. Vasi Istituto per i Processi Chimico-Fisici, sez. MESSINA, CNR, – PowerPoint PPT presentation

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Title: Sub-Diffraction Raman imaging by Near-Field Optical Microscopy


1
Sub-Diffraction Raman imaging by Near-Field
Optical Microscopy
P. G. Gucciardi, S. Trusso, C. Vasi Istituto per
i Processi Chimico-Fisici, sez. MESSINA, CNR,
Via La Farina 237, I-98123 MESSINA, Italy
S. Patanè I.N.F.M., Dipartimento di Fisica della
Materia e Tecnologie Fisiche Avanzate,Università
di Messina, Salita Sperone 31, I-98166 Messina,
Italy.
M. Allegrini I.N.F.M., Dipartimento di Fisica,
Università di Pisa, Via Buonarroti 2, I-56127
Pisa, Italy.
2
Abstract
Motivations
Difficulties
  • High spatial resolution 100 nm.
  • Added value simultaneous sample topography and
    elastic scattering images.
  • Exploitation of Surface enhancement effects
  • New Physics Gradient-Field Raman Effect.
  • Low efficiency of the Raman scattering.
  • Low throughput of the SNOM Fiber probes.
  • Very long acquisition times for Imaging purposes.
  • High mechanical and thermal stability are
    required.
  • Investigated Samples
  • Tetracyanoquinodimethane (TCNQ) crystal showing
    surface defects.
  • Localized Cu-TCNQ complexes embedded in a TCNQ
    thin film.

3
Far-Field Vs Near-Field Microscopy
Near-Field Microscopy
Far-Field Microscopy
  • Both the light source and the antenna are placed
    at several wavelengths from the sample.
  • The Lateral resolution is determined by the Abbe
    diffraction limit.
  • The sample is illuminated by a nanoscopic light
    source located close to the surface (10 nm).
  • The resolution is limited by the source diameter

4
Schematic of the Experiment
  • The sample is raster scanned by means of a
    piezo-tube under the probe.
  • SNOM probes commercial single mode optical
    fibers, tapered and coated by a thin CrAl film.
  • The apical aperture is 100 nm
  • Non-optical shear-force detection is
    accomplished for probe/sample distance
    stabilization, by means of a quartz tuning-fork.

5
Experimental setup
  • Excitation Ar laser line 514.5 nm.
  • Collection Nikon 50X objective, NA 0.5, WD
    10.6 mm.
  • Notch Filter Rejection Ratio 10-6.
  • Spectrometer Triax 190, single grating, 1200
    lines/mm, 190 mm focal.
  • Detector PMT in photon counting regime, 200-300
    dark cts/sec.
  • Shear-Force tuning-fork with etherodyne
    detection.
  • Signals Topography, Elastic, Raman.
  • Modes Illumination or Collection.

6
TCNQ
7,7,8,8 Tetracyanoquino-dimethane (TCNQ).
  • High Raman Efficiency.
  • The organometallic salt complexes can be
    discriminated based on the Raman shift of the
    vibrational peaks.
  • Can be deposited in thin film form or as a
    monocrystal.

C-H Bending 1202 cm-1
C?N Stretch
2225 cm -1
? 2208 cm -1
CC ring Stretch 1620 cm-1
CC wing Stretch 1445 cm -1
? 1380 cm -1
7
NanoRaman imaging of defects in TCNQ crystals
  • Surface defects are visible in the topography
    map.

Topography
  • Both the micro and nano Raman analysis evidence
    a corresponding scattering incerase.
  • The nanoRaman map shows sub-diffraction length
    details.

NanoRaman _at_ 1445 cm-1
MicroRaman _at_ 1445 cm-1
8
Another sample a CuTCNQ thin film
  • A thin TCNQ film (yellow) was deposited on a KBr
    substrate in vacuum conditions.
  • The sample was kept into contact with Cu powders
    giving rise to localized spots of Cu-TCNQ (blue)
    organometallic compounds.
  • Areas in which the film is scratched out evidence
    the presence of the substrate (white).

MicroRaman Spectra
Optical Microphotograph
TCNQ
Scratch
Cu-TCNQ
9
Our Target
  • Localization of
  • TCNQ.
  • CuTCNQ Local spots.
  • Scratches evidencing the KBr substrate.

On different length scales
Contrast mechanism
Absorption
  • Millimeter ? Microphotograph.
  • Micrometer ? MicroRaman.
  • Nanometer ? SNOM.

Raman Activity
Both
10
Localization of damaged areas by SNOM
Localization by Reflectivity
Topography
Reflectivity
  • Scratched areas can be localized through the
    analysis of the surface topography.
  • The elastic scattering signal is locally
    enhanced because of the higher reflectivity of
    the KBr substrate.

Localization by Raman Scattering
Topography
Raman _at_ 1445 cm-1
  • Two holes appear in the topography.
  • A vanishing Raman activity is found therein.
  • Lateral resolution 300 nm.

11
Localization of CuTCNQ by SNOM
Topography
Elastic Scattering
Topography shows no features ? NO SCRATCHES.
The stronger absorption of the CuTCNQ is evident
in the elastic scattering map.
  • Only 100 ms of integration time are required to
    get a Raman spectrum of TCNQ.
  • The CuTCNQ shows a Raman activity strongly
    reduced. Integration time 5 s.

The Raman map at 1445 cm-1 (Tint 100 ms per
point) shows the presence of areas of depleted
intensities which can be attributed to CuTCNQ.
Raman Spectra
Raman Map _at_ 1445 cm-1
12
Sub-diffraction Raman Imaging
RAMAN Map _at_1445 cm -1
Elastic Scattering
Raman Map
  • Integration time 100 ms per point. Total image
    acquisition time 1 hour.
  • The zoom was carried out in the TCNQ zone.
  • The dark clusters can be attributed to the
    presence of CuTCNQ complexes localized on
    sub-micron length scales.
  • The line profile allows to assess a lateral
    resolution better than 200 nm.

13
CuTCNQ
TOPOGRAPHY
A different locations shows bump-like features.
Scan width 10 10 ?m2
The bumps turn out to be TCNQ-rich zones.
14
Resolution assessment in NanoRaman on Cu-TCNQ
TOPOGRAPHY
ELASTIC SCATTERING
RAMAN 1445 cm -1
  • Scan width 2.5 2.5 ?m2
  • Simultaneous maps of topography, Elastic and
    Raman scattering show correlated features.
  • Raman imaging confirms the spectral information
    on the chemical nature of the bumps.
  • A resolution of 240 nm can be assessed.

15
Difficulties in Illumination-mode SNOM NanoRaman
experiments
Metal-Phosphorus trichalcogenides NanoRaman
TCNQ NanoRaman Spectrum
  • Raman emission of the SNOM fiber probe in the
    100 500 cm-1 region.
  • High efficiency materials are a must.
  • Limited Spectral Resolution 25 cm-1
  • Image acquisition times of 1h
  • Variations of the baseline.

16
during the last year
  • A very sensitive, versatile and performant SNOM
    setup was developed for spectroscopy
    applications.
  • NanoRaman imaging has been demonstrated on
    organic materials, within reasonable acquisition
    times.
  • Sub-diffraction resolution has been achieved.
  • Topography, Elastic and Raman scattering signals
    can be acquired simultaneously.
  • Critical points and limits of illumination mode
    Near-Field Raman experiments have been
    identified.
  • A class of materials suitable for NanoRaman
    investigations has been identified.

17
Whats next ?
  • Materials Calchogenides, Nanotubes, Silicon.
  • Tecnhiques SERS.
  • Instrumentation Apertureless SNOM, Transmission
    mode, Different collection angles.
  • Upgrades Better spectral resolution (5 cm-1),
    better spatial (10 nm) resolutions.

18
The New Concept
  • Different Probes
  • Aperture SNOM
  • Scattering SNOM
  • AFM, STM
  • Olympus Microscope
  • Localization
  • Light Collection
  • Micrometer screws
  • Coarse positioning

Thanks for the kind attention !
  • Clearence
  • Transmission Mode
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