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Instruments:
Laser Scanning
Confocal
Photo-activation
& Conversion
Spinning Disc
Confocal
Fluor.
Emission Fingerprinting
Nuance
Spectral Unmixing System
Total Internal
Reflection Fluor.
Axioskop Fluo. Microscope
Microinjector
Rotary Shadowing System
Ultramicrotomes
Trans. Electron
Microscopes
Software:
MetaMorph 6.0
Volocity
2.0
Zeiss LSM 510
Software
Zeiss Image Examiner
Resources:
Publications
Links
Technical Tips
References and
Books
Web Design: Teng-Leong Chew
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Total Internal Reflection Fluorescent (TIRF) Microscope
A
stringent test for TIRF. A fibroblast co-expressing vinculin and
myosin II regulatory light chain (both tagged with GFP) was imaged
using the TIRF system. Wide field image is pseudo-colored green
while TIRF image is pseudo-colored red. As shown, TIRF is capable
of separating the two green-labeled proteins based solely on their
relative intracellular positions. Picture by Teng-Leong Chew,
NU Cell Imaging Facility.
Olympus
Arc-delivered TIRFM
The facility is equipped with an arc lamp-delivered TIRF microscope
from Olympus. The system is fitted with excitation and emission
filters wheels, allowing users to image red, green, cyan, and
yellow fluorescent emitters. 60X and 100X (N.A. 1.45) lenses are
available for TIRF imaging. Unlike the N.A.1.65 100X objective
lens, our 100X TIRF objective does not require special immersion
oil or special coverslips. The rapid switching between TIRF and
wide field is accomplished by a modified ARCEVA crescent for automated
insertion/removal in the illuminating path. The system is operated
on a MetaMorph-driven platform. To facilitate imaging of extreme
low-light samples under TIRF mode, we have equipped the system
with a Hamamatsu Electron Multiplier C9100 CCD camera. This 14-bit
camera provides a gain factor of up to 2000 and maintain a speed
of 30 frames per second, thus perfectly suited for high speed,
ultra-dim, TIRF imaging.
How does TIRF work?
Various mechanisms are often employed in fluorescence microscopy
applications to restrict the excitation and detection of fluorophores
to a thin region of the specimen. Elimination of background fluorescence
from outside the focal plane can dramatically improve the signal-to-noise
ratio, and consequently, the spatial resolution of the features
or events of interest. A light beam, incident on an interface
with different refractive indexes for the two phases, is totally
reflected if the incident angle exceeds a critical angle qc. While
the light is totally reflected, a portion of the radiation exists
in the distal phase called the evanescent wave. The evanescent
wave will continue to travel into the medium of higher refractive
index, but its strength will decay exponentially.
The TIRF system takes advantage of the evanescent wave to specifically
illuminate only a range of 100-200 nm from the coverslip, thus
serving as an extremely powerful tool to study cell-substrate
contact and adsorption of macromolecules to surfaces. The TIRF
system can focus on an optical section at least 5 times thinner
than any existing confocal microscope, as fluorophores above the
200nm range will not be excited.
In general, total internal reflection illumination
has potential benefits in any application requiring imaging of
minute structures or single molecules in specimens having large
numbers of fluorophores located outside of the optical plane of
interest. Since the excitation light is completely reflected away
from the detection, one can easily discriminate the fluorescence
signal from the excitation light and achieve very low sensitivities
and detection limits. This capability thus allows users to (1)
monitor the interaction between intracellular protein and the
substratum, especially in cases where the intracellular protein
is of very high abundance in the cytoplasm, which will inevitably
generate very high internal noise using conventional epi-illumination.
(2) Another important application of TIRF is in the characterization
of force exerted on the substratum during cell motility. The currently
available fluorescent scopes in the facility do not allow users
to accurately measure the displacement of gel-embedded fluorescent
beads, due to significant light scattering problem. The TIRF system
will completely eliminate this hindrance, thus allowing users
to accurately calculate traction force during cell movement. (3)
By varying the illumination incidence angle, and consequently
the penetration depth of the evanescent wave, fluorophores can
be distinguished by depth on a nanometric scale. By rapid variation
in the evanescent field depth, target vesicles or other structures
can be tracked at different depths and their positions accurately
determined.
It is important to note that TIRF does not work well with fixed
and mounted samples. Most mounting agent seek to generate a refractive
index close to that of the coverslips. While this works for other
fluorescent microscopes, it actually hinders the occurrence of
total internal reflection. The system is designed, therefore,
to work exclusively with aqueous samples.
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