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Morrell Instruments Imaging
Department
 

Advanced
Imaging Techniques
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Multi-Dimensional
Acquisition 6D
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Ex
Multi Dimensional set: D-F-TR, 30 image z stacks,
acquired in just over 3 seconds
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Physiology
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FRET
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FLIM
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FRAP
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Bioluminescence
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Chemiluminescence
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Laser
Microdissection
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IR
Dissection Systems
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Real-Time
Ratiometric Systems
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Calcium
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Deconvolution
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IVF
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High
Speed Slide Scanning- capture up to 10 frames a
second with focus and tiling
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Automated
Counting/ Measuring
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3D
Visualization/ Voxel Measurements
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Wafer
Inspection
Digital
Cameras

Nikon Digital Cameras
Photometrics
Digital Cameras
QImaging Digital Cameras
Fluorescence
Filter Guide
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Nikon LiveScan Swept
Field Confocal
Microscope

Whether you're doing
multi-dimensional
imaging of cells (X,Y,Z,T
or even X,Y,Z,T at
multiple coordinates),
observing fast neural
events, or looking to
capture live-motion
images of cells, the
Nikon LiveScan SFC
(Swept Field Confocal)
microscope offers
advance technology for
your advanced research.
The key to the image
quality is Nikon's
patent-pending swept
field technology.
Unlike confocal
systems with pinhole
apertures embedded in a
spinning disc, the Nikon
LiveScan SFC's 32
pinhole array remains
stationary.
Galvonometric and piezo
controlled mirrors sweep
the image of the
pinholes across the
sample. The emission
photons are de-scanned
and focused through a
complementary set of
pinholes onto a CCD
camera

This swept field
technology overcomes
some limitations of
systems with spinning
discs such as a lack of
synchronization between
the moving pinholes and
the CCD camera,
crosstalk between
pinholes, and true
confocality with a very
limited selection of
objective lenses.
Another common problem
with spinning disc
systems is that banding
occurs at rapid frame
rates. The Nikon
LiveScan SFC has the
fastest rates of data
acquisition of any
commercially available
confocal system.
Also, in contrast to
systems with spinning
discs, where the pinhole
diameter is set, Nikon
LiveScan SFC offers four
selectable confocal
pinhole diameters (from
30 microns to 90
microns), along with a
slit scanning (35 and 70
microns) mode- so you
can choose to optimize
sensitivity, resolution,
or speed.
The LiveScan SFC
offers you:
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Speed: the
fastest data
acquisition speeds
of any commercially
available confocal
system
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Maximum
acquisition
frame rate
exceeding
1000frames/second
inslit scan mode
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up to 120
frames/second in
pinhole mode for
high resolution
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High Efficiency
Optical System:
Swept field
technology and
state-of-the art
optics yield a high
rate of photon
capture, in the
range of 440-700nm
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Multiple Laser
Configuration
Options
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Multiple
Wavelength Scanning:
possibility of up to
6 wavelengths in one
fiber and single or
dual fiber outputs
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Compatible with
TIRF Illumination
Why settle for
spinning disk when you
can have Swept Field?
Seeing is believing.
Click here
to request a
demonstration.
To find out more
about how the Nikon
LiveScan SFC is bringing
live-cell image capture
to a new level, or to
discuss what
configuration is best
suited for your
research, call
1-800-570-4277 |
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Nikon Confocal Systems
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The innovative technology of the
C1si gives you a level of
flexibility, speed, and spectral
capability not available in
conventional confocal systems,
including: One-pass,
high-resolution, wide-band
spectral imaging
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One-Pass:
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High Resolution:
Select 2nm, 5nm, or 10nm
channel width.
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Wide-Band
Acquisition:
Spectra over a full range of
320nm (400nm-750nm) can be
obtained in a single pass,
at 10nm.
Spectral imaging focusing on
brightness
The uncompromised optical design
and signal processing of the
C1si places it among the most
efficient spectral detectors
available. Signal loss has been
minimized by the use of:
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Proprietary optics (patent
pending) that very
efficiently capture
fluorescence emission
photons.
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Signal-processing circuitry
(patent pending) that
digitizes for the full pixel
period, eliminating dead
time.
True Spectral Imaging
Innovative technology
(patent-pending) allows:
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True fluorescence colors
across spectrum.
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Accurate fluorescence
spectrum even at highest
resolution (2 nm).
Unmixing of Fluorescent
Signals Without Crosstalk
The C1si software allows you to
cleanly separate the signals of
fluorescent probes, including
those with closely overlapping
spectra, such as CFP, RFP, YFP,
and Alexa488. This is
particularly useful for:
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Observing multistained
specimens
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FRET experiments
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Separating the signal from
autofluorescence
Fluorescence
spectra of GFP
and Alexa 488

Spectra
displayed at 2.5
nm wavelength
resolution per
channel of the
fluorescence
detector in the
493-570.5 nm
range.
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Separation of
GFP and Alexa 488
spectra
GFP expressed in
HeLa cell nuclei and
actin stained with Alexa
488. Excitation
wavelength 488 nm.]
Combined
channel
True
Color
image.obtained
with 2.5
nm
wavelength
resolution
in
493-570.5
nm
range.
Image
with
separated
spectra
after
using
unmixing
software. |
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Even overlapping red
fluorochromes are easily
unmixed!
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Unmixing red
fluorochromes
Red
flourochromes,which
had previously
posed a
challenge, are
now simple to
unmix as well.

Rhodamine's
fluorescence
spectral peak is
at approximately
579 nm, while
that for RFP is
approximately
600 nm. RFP's
fluorescence is
weaker than
Rhodamine's, but
their spectra
are cleanly
unmixed.
RFP
expressed in
HeLa cell nuclei
and actin
stained with
Rhodamine. True
Color image
overlay of 32
images in the
550-630 nm range
at 2.5 nm
wavelength
resolution.
After
fluorescence
unmixing.
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Compatible with TIRF
Illumination
Easy To Operate. Easy to Modify.
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Switch easily:
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from the
high-resolution, 32
channel detector to a
standard 3 channel
confocal detector with
all the optical advances
of the C1 Plus.
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from eyepiece
observation to laser
scanning mode.
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Variable Color Filtering:
Wavelength information from
the entire range can be
gathered in one pass.
Afterward, you can easily
digitally filter in any
desired wavelength range.
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Intuitive Software: Most
parameters can be modified
with a single click of the
mouse.
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Nikon TIRF
Systems

Nikon's Evanescent Wave Imaging System utilizes an
evanescent wave to excite single molecules in the thin
section in contact with the coverglass
Extendable "stratum structure". This unique design
permits simultaneous mounting of both TIRF and epi-fluorescence
illumination systems, with no restriction on their
individual capabilities. It also allows their dedicated
filters to be used independently.
Multi-mode imaging observation: By doing both TIRF and
Confocal laser imaging, you can investigate dynamic
events in cells because this method produces both
extremely high signal-to-noise image at the cell's
membrane and 3D images of the whole cell.
TIRF objective is adjustable to correct for
temperature-induced changes in refractive index. We've
developed a dedicated Plan Apo 60x NA 1.45 oil immersion
TIRF objective with correction collar, the first lens in
the world to correct for spherical aberration induced by
temperature changes in the refractive index of immersion
oil.
SRIC (Surface Reflective Interference Contrast) method
can reveal focal contacts prior to switching to TIRF.
Laser illumination is safe and easy-to-use. To comply
with laser safety standards, the laser's shutter
features an interlocking mechanism. The laser shutter
will not operate when the optical path to the binocular
is open, preventing laser illumination from entering the
user's eyes through the eyepieces.
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