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LA-WATAP
LASER-Assisted 3D Atom Probe for Semiconductors and Materials
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The CAMECA LA-WATAP
instrument is the next generation of Tomographic (or 3D) Atom Probe,
providing quantitative atomic scale 3D elemental mapping
of chemical heterogeneities in materials.
The LA-WATAP offers the following advantages:
- Analysis of
semiconductor materials with near-atomic depth resolution. This is possible by using a flexible
(IR/ visible/ UV) ultrafast (400fs) laser setup. The unique hybrid evaporation mode
combines reduced heating of the sample with ultra-fast surface
polarisation promoting ion evaporation under the high DC electrical
field.
- Excellent
mass resolution even on low thermal conductivity materials. This is
obtained by reducing the heating of the sample with ultra-fast laser
pulsing. Conventional picosecond laser based 3DAP work in thermal
evaporation mode leading to thermal effects and peak tails.
- Analysis of thin electrically insulating layers by using
fs-laser pulses of short wavelength (UV).
- Highest analyzer transmission (detected ions/evaporated atoms >60%). Reflectron-based 3DAP instruments reduce this typically to 35% due to the use of grids. Transmission is a key parameter when applying the (destructive) 3DAP technique to the quantification of nanoscale volumes.
- Large analysis area (100nm in diameter) for a better statistics on composition measurements.
- Fast acquisition, up to 1E6 atoms per minute depending on sample strength (flux of at./pulse).
- Best quantitative results with the exclusive Advanced Delay Line Detector (ADLD) and its benchmark multi-hit performance.
- Flexible and
fast dedicated FIM (Field Ion Microscopy) detector for metallurgical
application with highest S/N performance and fast switch between FIM
and 3DAP modes.
A six-page introduction leaflet of the new LA-WATAP 3D Atom Probe can be downloaded.
Flexible Laser setup.
The
response of a material under Laser illumination depends on its nature,
its shape and on the wavelength of the Laser. The LA-WATAP offers
flexible Laser setup,
ensuring optimized analysis conditions for all materials. The operator
can easily select
the most appropriate
wavelength for any given sample: I.R. (1030nm), visible (515nm), or
U.V.
(343nm).
Analysis
of a 12nm thick SiO2 layer. The use of UV facilitates the analysis and
quantification on electrically insulating materials. Using IR the
analysis was not possible. Using green the interfaces were of
unphysical shape and the stoichiometry of the oxide was wrong and with
a loss of mass resolution.
Atomic scale depth resolution in semiconductors.
The interaction of ultrafast
(400fs) pulses of polarized light with a small tip (radius 10-100nm)
results in non-linear effects confining the polarization to the skin of
the tip apex. Combining this with a DC electrical field and a moderate
heating of the tip, the evaporation of ions can take place without
dramatic loss of spatial resolution.
Excellent depth resolution is evidenced
in the 3D AP analysis of a <111> silicon sample.
The
<111> atomic planes are directly visible in the reconstructed
volume (4x4x20nm), without any data treatment. Such data quality is not
available using conventional ps-laser technology.
Improvement of Atom probe mass resolving power with LASER evaporation.
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Mass
spectra of an aluminium-silicon-magnesium alloy obtained with HV pulses (green curve) and
laser pulses (blue curve). On the right, 3D image of the Mg distribution. The
use of femto-second Laser technology and CAMECA design result in a higher mass resolving
power compared to HV pulsing (inducing an energy spread) or pico-second
conventional Laser technology (inducing thermal evaporation effect with longer heating of the tip).
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A larger Field Of View
The
3DAP Field Of View is determined by the instrument geometry
(tip-detector distance and detector size) but also by the tip itself
(radius, cone angle and material evaporation field).
Smaller tip radius and lower evaporation field will result in lower
FoV. Note that the radius increases during the analysis and the DC
voltage is progressively raised in order to regulate the evaporation
flux.
The LA-WATAP typically records volumes of 50-100nm diameter by 100-200nm depth,
resulting in files of several tens of millions ions, in a few hours
(depending on requested evaporation flux that is sample-dependent).

Te: blue, Fe: green, Co: black.
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82 x 82 × 140 nm3 (17 M atoms)
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The Laser evapoartion mode allowed analysis of the above TbFe/Co multilayer,
too fragile to be analyzed in HV mode. Zooming inside the Large Field
Of View reveals atomic plane depth resolution and dissymetric
interfaces (sharp and diffused) linked to layer growth conditions.
Analysis of semiconductors with the Atom Probe:
Drain silicide interface in MOS transistor structure
The concentration profiles of Ni, Si and Pt below clearly reveal the presence of both Ni2Si
and NiSi phases as a consequence of the reactive diffusion between Ni
and Si substrates. Furthermore, Pt enrichment at both Ni/Ni2Si and Ni2Si/NiSi interfaces is clearly evidenced.
This example illustrates the importance of quantification to understand
a physical process. Two NiSi phases are assigned without ambiguity,
mainly thanks to the Advanced Delay Line Detector’s superior multi-hit capabilities and optimized Laser evaporation mode.
Moreover, due to the unique in-depth resolution, boundaries between
phases are clearly revealed without matrix effect as observed in SIMS
with this type of sample.
The CAMECA LA-WATAP is developed through a scientific and technical collaboration with the GPM-University of Rouen-CNRS, France.
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