|

Electronic
Products Online - November 2010
Improving nanoimaging of
µ-Raman/AFM systems
Negative-stiffness
vibration isolators can easily support the heavy weight of
a combined AFM/micro-Raman system, and isolate it
By Jim McMahon
Zebra Communications
Simi Valley, CA
www.zebracom.net
The need for precise vibration isolation with scanning
probe microscopy (SPM) and nearfield scanning optical microscopy
(NSOM) systems is becoming more critical as resolutions continue
to bridge from micro to nano. Whether used in academic labs
or commercial facilities, SPM and NSOM systems are extremely
susceptible to vibrations from the environment.
When measuring displacements of a very few angstroms or nanometers,
an absolutely stable surface must be established for the instrument.
Any vibration coupled into the instrument's mechanical structure
will cause vertical and/or horizontal noise and thus reduce
the system's ability to measure high resolution features.
And while the vertical axis is the most sensitive for SPMs,
they can also be quite sensitive in the horizontal axis.
Traditional isolation
Traditionally, bungee cords and high-performance air tables
have been the vibration isolators most used for SPM and NSOM
work. The ubiquitous passive-system air tables, adequate until
a decade ago, are now being seriously challenged by the need
for more refined imaging. Benchtop air systems provide limited
vertical and horizontal isolation.
Also at a disadvantage are systems based on active isolation,
known as electronic force cancellation. Such systems use electronics
to sense the motion and then add equal amounts of motion electronically
to compensate and cancel out the motion. Active systems are
somewhat adequate for applications with lasers and optics,
as they can start isolating as low as 0.7 Hz, but because
they run on electricity they can be negatively influenced
by problems of electronic dysfunction and power modulations,
which can interrupt scanning.
Lately, the introduction of integrated microscopy systems
employing multiple microscopes is enabling more complex optical
measurements, but these systems are also much heavier, and
there has been little vibration isolation technology available
for such heavy instrumentation. Air tables, which have been
liberally used for optics applications, are not ideal for
these nanoscale resolution systems because of their inability
to effectively isolate vibrations below 20 Hz. Nor can active
systems be used with these newer combination systems because
of their inability to handle heavy instrumentation.
But now, negative-stiffness mechanism (NSM) vibration isolation
is quickly becoming the choice for SPM and NSOM systems. This
includes applications using atomic force microscopy (AFM)
integrated with micro-Raman spectroscopy, where negative-stiffness
vibration isolation is particularly well adapted. In fact,
it is the application of negative-stiffness isolation that
has enabled AFMs to be truly integrated with micro-Raman into
one combined system. Negative-stiffness isolators can handle
the heavy weight of the combined AFM/micro-Raman system, as
well as isolate the equipment from low frequency vibrations,
a critical set of factors that high-performance air tables
and active systems cannot achieve.
AFM with micro-Raman
The integration of AFM with micro-Raman enables a sizable
improvement in data correlation between the two techniques
and expanded Raman measurement and resolution capabilities.
Micro-Raman is a spectroscopic NSOM technique used in condensed-matter
physics and chemistry to study vibrational, rotational, and
other low-frequency modes in a system. It relies on scattering
of monochromatic light, usually from a laser in the visible,
near-infrared, or near ultraviolet range. The laser light
interacts with phonons or other excitations in the system,
resulting in the energy of the laser photons being shifted
up or down. The shift in energy gives information about the
phonon modes in the system.
Scanning samples in a micro-Raman system, however, suffers
from several problems. As even a very flat sample is scanned,
it is hard to keep the lens-to-sample distance constant. Thus,
as one goes from pixel to pixel under the lens of a Raman,
a mixture of sample and air is sampled in the voxel (volumetric
picture element) that is illuminated. This causes artifactual
intensity variations in the Raman unrelated to the chemical
composition of the sample.
This is even more pronounced with rough samples, and standard
methods of auto-focus are simply not accurate enough for a
host of problems being investigated today. Additionally, the
point-spread function, which determines the resolution of
the Raman image, is significantly broader where there are
contributions from the out-of-focus light, and this reduces
resolution.
The AFM, being a very high-resolution type of scanning-probe
microscope, has demonstrated resolution of fractions of a
nanometer, making it one of the foremost tools for imaging,
measuring, and manipulating matter at the nanoscale. The information
is gathered by "feeling" the surface with a mechanical
probe. Piezoelectric elements that facilitate tiny but accurate
and precise movements on electronic command enable the very
precise scanning.
The AFM consists of a microscale cantilever with a sharp tip
(probe) at its end that is used to scan the specimen surface.
The cantilever is typically silicon or silicon nitride with
a tip radius of curvature on the order of nanometers. When
the tip is brought into proximity of a sample surface, forces
between the tip and the sample lead to a deflection of the
cantilever. Resultant characteristics, such as mechanical,
electrostatic, magnetic, chemical and other forces are then
measured by the AFM using, typically, a laser spot reflected
from the top surface of the cantilever into an array of photodiodes.
Most systems employing AFM in concert with Raman perform separately,
executing either an AFM scan or a Raman scan independently.
The recently developed direct integration of Raman spectroscopy
with AFM technique, however, has opened the door to significantly
improved technique and sample analyses.
Micro-Raman is a microtechnique, but when AFM is added, it
becomes a nanotechnique. It allows the AFM structural data
to be recorded online and improves the resolution of the Raman
information when the nanometric feedback of the system adjusts,
with unprecedented precision, the position of each pixel of
the sample relative to the lens. Also the small movements
of the AFM stage provide oversampling, which is a well-known
technique for resolution improvement.
One integrated AFM-Raman system developed by Nanonics Imaging
in association with major Raman manufacturers such as Renishaw
plc, Horiba JY and others provides simultaneous and, very
importantly, on-line data from both modalities (see Fig. 1).
Most systems employing AFM in concert with Raman perform separately,
executing either an AFM scan or a Raman scan independently.
The recently developed direct integration of Raman spectroscopy
with AFM technique, however, has opened the door to significantly
improved technique and sample analyses.
Micro-Raman is a microtechnique, but when AFM is added, it
becomes a nanotechnique. It allows the AFM structural data
to be recorded online and improves the resolution of the Raman
information when the nanometric feedback of the system adjusts,
with unprecedented precision, the position of each pixel of
the sample relative to the lens. Also the small movements
of the AFM stage provide oversampling, which is a well-known
technique for resolution improvement.
One integrated AFM-Raman system developed by Nanonics Imaging
in association with major Raman manufacturers such as Renishaw
plc, Horiba JY and others provides simultaneous and, very
importantly, on-line data from both modalities (see Fig. 1).
|
|
|
Fig. 1. The
MicroView4000 platform from Nanonics Imaging is the
basis for AFM-Raman integration.
|
This advantage addresses critical problems in Raman including
resolution and intensity comparisons in Raman images while permitting
on-line functional characterization such as thermal conductivity,
elasticity and adhesion, electrical and other properties. It
also provides for new avenues of improved resolution including
AFM functioning without optical obstruction, parallel recording
with Raman in a wide variety of scanned probe imaging modalities
enabling direct and simultaneous image comparison and analysis,
and high-resolution Raman mapping.
The Nanonics platform can be used for structural and photonic
characterization, as well as the structural and chemical characterization
that is available with AFM and Raman integration. For these
applications, Nanonics Imaging is the innovator of AFM and NSOM
systems, including dual tip/sample scanning AFM systems, the
industry's first NSOM-AFM cryogenic systems, integrated Raman-AFM
systems, multiprobe AFM and SEM-AFM systems.
The Nanonics MultiView AFM-NSOM microscope, with its free optical
axis on a standard micro-Raman, now makes it possible to truly
integrate the separate worlds of Raman and AFM/NSOM nanocharacterization,
which has led to a new era in high-resolution Raman spectroscopy.
NSVI enables integration
Underlying this pioneering integration of AFM with micro-Raman
is negative-stiffness vibration isolation, developed my Minus
K Technology. What negative-stiffness isolators provide is really
quite unique to SPM-Raman and other NSOM systems. In particular,
improved transmissibility of a negative-stiffness isolator -
that is the vibrations that transmit through the isolator relative
to the input floor vibrations. Transmissibility with negative-stiffness
is substantially improved over air systems and over active isolation
systems.
Negative-stiffness isolators employ a unique, completely mechanical
concept for low-frequency vibration isolation. Vertical-motion
isolation is provided by a stiff spring that supports a weight
load, combined with a negative-stiffness mechanism (see Fig.
2). The net vertical stiffness is made very low without affecting
the static load-supporting capability of the spring. Beam-columns
connected in series with the vertical-motion isolator provide
horizontal-motion isolation.
|
|
|
Fig. 2.
The negative-stiffness isolator concept developed by
Minus K Technology makes it possible for a heavy AFM-Raman
system to be immune to shocks that would make nanoprecision
impossible.
|
The horizontal stiffness of the beam-columns is reduced by the
"beam-column" effect (A beam-column behaves as a spring
combined with a negative-stiffness mechanism).
The result is a compact passive isolator capable of very low
vertical and horizontal natural frequencies and very high internal
structural frequencies. The isolators (adjusted to 1/2 Hz) achieve
93% isolation efficiency at 2 Hz; 99% at 5 Hz; and 99.7% at
10 Hz.
PDF
version of this article
Top
|