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MPE Full Picture
MPE Full Picture
MPE
25X Objective
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FV1000 Multiphoton

The FV1000 MPE allows bright, high-resolution observation deep within specimens without causing damage. By closely adhering to optics principles and designing a microscope that is both compact and easy to use, Olympus has developed the new generation FV1000MPE so that even more researchers can utilize multiphoton capabilities with their samples.

What is a multiphoton laser scanning microscope?

By using femtosecond laser for multiphoton excitation and a complete system's approach to sensitivity, the observation of the deep is more possible than ever before.

The following specimen is the cerebral cortex of M-line, a strain of transgenic mouse (GFP). From the surface in vivo imaging was performed with excitation of 488 nm for single photon and excitation of 920 nm for multiphoton. With single photon, depths to only 400 µm can be observed, whilst with multiphoton depths to about 750 µm can be achieved.

 Neuronal Image single photon v MPE
Kimihiko Kameyama, Tomoyo Ochiishi, Kazuyuki Kiyosue, Tatsuhiko Ebihara Molecular Neurobiology Group, Neuroscience Research Institute, National Institute of Advanced Industrial Science and Technology, Japan.

FV1000MPE Main Visual

 

FV1000MPE enables brighter and deeper imaging with superb resolution

system configuration

 

1. Brighter and deeper imaging with less damage.

By using femtosecond pulsed laser with negative chirp, FV1000MPE enables brighter and deeper imaging with less tissue or cell damage.

2. Custom light adjustment for the exiting laser beam.

During observation of thick specimens, laser intensity can be changed in accordance with specimen depth, enabling consistent image brightness with depth.                                   

 

3. Auto-adjustment of the beam in accordance with the excitation wavelength and objective.

With its auto beam expander, the FV1000MPE achieves auto-adjustment of the beam diameter in accordance with the objective and excitation wavelength, providing the optimal laser beam for multiphoton excitation.

 

4. Correcting for light refraction in the sample and providing deep imaging.

The FV1000MPE’s dedicated objective can allow for the formation of an ideal focal spot deep within a range of sample types without reducing energy density.

5. Widefield design to detect fluorescence with no leakage of scattered light.

With its widefield design, the FV1000MPE can capture the maximum amount of fluorescent signal, along with scattered light, to provide highly efficient fluorescence imaging.

6. Even brighter in-depth observation with transmitted light detection.

A transmitted light fluorescence detector for multiphoton imaging, which detects transmitted fluorescence in addition to fluorescence scattered in the focal spot plane, and a dedicated high N.A. condenser are available for the FV1000MPE.

 

XLPLN25xWMP

Dedicated objective with exceptional brightness and resolution for multiphoton imaging.

This water immersion objective with a high N.A. and widefield design has improved transmittance particularly of near-infrared wavelengths to optimize multiphoton fluorescence microscopy. This unique feature allows for the formation of a precise focal spot without reducing energy density, even for deep tissue observation. Its widefield design, which can detect scattered fluorescence in a specimen, enables extremely bright, high-resolution fluorescence microscopy.

  25x Objective

 

   

 

Special correction collar for spherical aberrations.

Every objective lens is designed for one immersion medium - air, oil, water etc. - creating a perfect focus for the appropriate medium. A change in the refractive index of the medium, for example using a glass cover slip with a water immersion objective, will result in spherical aberration - mainly stretching the focus in z. Correction collars for spherical aberrations are well known in confocal imaging. Olympus has taken this even a step further. As the aim of multiphoton imaging is to image deep within the sample, this means the focussed beam will have to pass through several 100µm of tissue instead of water or oil. Biological tissue has a different refractive index than plain water, leading to spherical aberrations. The XLPLN25xW-MP objective has a correction collar to correct for these aberrations by tissue.

 

focal volume

Figure: fluorescent beads, embedded in high-refractive index medium (n~1.37), imaged in different depth with the excitation wavelength 950nm. With the current state-of-the-art objectives, the focus gets elongated along z, when imaging deeper within the sample. When using the correction collar on the XLPLN25xW-MP objective, the size of the focus stays the same, even at depth of ~1mm.

Optical parameters optimised for multi-photon excitation.

Apart from improving the coating both in the IR as well as the visible light to approximately 90% transmission, the vignetting has been reduced - allowing for a more even illumination in the focal plane.  In MPE everything is about the probability of two or more photons being absorbed simultaneously - the excitation efficiency. As this depends on the density of photons a very small focus is crucial. The XLPLN25xW-MP has a numerical aperture (NA) of 1.05. The field number - which is a measure for the field of view (FOV) - for laser scanning is 18, which fits perfectly to the possibilities of the FV1000MPE, whereas the field number for fluorescence detection is much larger: 27.5. This is important as in multiphoton imaging excitation can only happen in the focus, but the fluorescence emitted from the focal area will be scattered multiple times on its way back out of the sample. The larger the FOV is, the more of these scattered fluorescence photons will be detected.

 

optimised optical parameters

     

Fluorescence detectors for high-sensitivity multiphoton imaging

*Reflected light fluorescence detector.
This detector can capture all fluorescent signals without signal passing through a confocal aperture, so this allows imaging at a high level of sensitivity and minimizes light decay.

 

MPE Config MPE Configuration
MPE Configuration_2

 

Multi-Point Stimulation Software

This software module allows the design of fast optical stimulation experiments. For one single point, several individual points or even a whole field of points (32x32) a time protocol with one or several stimulations can be set up, using all lasers attached to the system. The experiment protocol will be carried out with high temporal precision, minimizing the traveling time from on defined point to the next. The Multi-Point Stimulation software is a very powerful tool, especially in the field of electrophysiology. With its flexibility it will allow the creation of interesting experiments in various fields of research.

 

 

Compact FLIM NDD Upgrade kit for the FV1000MPE

The compact FLIM NDD upgrade kit for the Olympus FluoView FV1000MPE allows deep tissue FLIM imaging at depths beyond 100um. Using up to 4 Olympus NDD PMTs, the upgrade provides a cost effective, highly integrated and compact solution for FLIM imaging.

 

 

What is Second Harmonic Generation Imaging?

SHG is a secondary nonlinear optical phenomenon. In SHG, the energy of 2 photons entering a specimen is combined, producing energy in the form of light. That is, the wavelength of light observed is half of the incident wavelength (the frequency is doubled). An SHG signal is not produced unless molecules in the material are non-centrosymmetric (i.e. a centre of inversion symmetry is absent).The signal is linear, so a transmitted light detector is needed. In addition, SHG signal intensity is proportional to the size of the potential, so changes in membrane potential in the vicinity of lipid bilayers of cells with a regular molecular structure can also be analyzed.

 

SHG

 

A: SHG image of neurons in dissociated culture from the mouse cerebral cortex. After FM4-64 was administered to neurons from outside the cells, the cells were irradiated with a femtosecond laser at 950 nm and the SHG signal at 475 nm was detected with the transmitted light detector.
B: An enlargement (5x) of the portion in the yellow box in image A. As is apparent, spines protruding from dendrites can be observed with SHG.
C: SHG and multiphoton images have been superimposed.
Mutsuo Nuriya, PhD, Masato Yasui, MD, PhD Department of Pharmacology School of Medicine, Keio University.

 

Multiphoton System Line Up from Olympus - from in vivo to live cell imaging

 

 

M (Multiphoton) System

This dedicated multiphoton system is not equipped with a visible light laser. Simple optics optimized for multiphoton microscopy allow a smaller footprint, simple operation, and imaging deep within the sample. The system uses a gold-coated galvanometer scanning mirror.

MPE Config_3

M system

  

B (Basic) System

This system is equipped with an IR laser for multiphoton imaging and single photon laser for visible light imaging. The system is designed for varied imaging including Live Cell and in vivo imaging. Using this system with the double laser combiner enables multiphoton imaging and visible light stimulation.

MPE Config_3

 B System

 

S (Stimulation) System

This system is equipped with an IR laser in the scanner for stimulation. In addition to general multiphoton microscopy, the system allows pinpoint light stimulation by multiphoton excitation during imaging with a visible laser.

MPE Config_3

 S system

 

T (Twin) System

This system synchronizes laser light stimulation and imaging with 2 independent IR lasers. Laser light stimulation is done with a multiphoton laser, allowing pinpoint stimulation of areas deep within a specimen that cannot be reached with single photon. Multiphoton stimulation can be done at a pinpoint, allowing observation of the effect a single dendritic spine has. Laser light stimulation can be performed in 3 dimensions or locally at specific sites.

MPE Config_3

 Twin system
 B systemS systemT systemM system
Laser unitIR pulsed laser
with negative
chirp for multiphoton excitation
·Mode-locked Ti:sapphire laser
[femtosecond laser (equipped with a group velocity
dispersion correction/control device)],laser power unit,
water-cooled circulating chiller
·MaiTai BB DeepSee-OL or MaiTai HP DeepSee-OL
(Spectra-Physics products)
  MaiTai BB DeepSee-OL: 710 nm – 990 nm
  MaiTai HP DeepSee-OL: 690 nm – 1040 nm
·Chameleon Vision I-OL, Chameleon Vision II-OL
(Coherent products)
  Chameleon Vision I-OL: 690 nm – 1040 nm
  Chameleon Vision II-OL: 680 nm – 1080 nm
Visible light laser
AOTF laser combiner
LD laser: 405nm: 50mW, 440nm: 25mW, 473nm 15mW,
559nm 15mW, 635nm 20mW Multi Ar laser
(458 nm, 488 nm, 515 nm, Total 30 mW),
HeNe (G) laser (543 nm, 1 mW)
Modulation: Continuously adjustable via an AOTF
(0.1 – 100% in 0.1% increments)
·Operating mode: Allows laser turn-off during the retrace
period REX: adjustment of laser power for each region,
and selection of the laser and selection of the laser wavelength
·Visible light laser platform with implemented AOTF system,
ultra-fast intensity with individual laser lines,
additional shutter control,
Connected to scanner via single-mode fiber
·Equipped with laser feedback mechanism to limit changes
in laser light intensity over time
-
Single laser for visible light LD473 laser (15mW) Depending on the type of modulation:
light intensity modulation, shutter control,
corrected to the scanner via single-mode optical fiber
Scanning unitScanning method Light deflection via 2 galvanometer scanning mirrors
Scanning modes ·Pixel size: 64 x 64 – 4096 x 4096 pixels Scanning speed:
(pixel time): 2 µs – 200 µs High-speed scanning mode:
16 frames/s (256 x 256)
·Dimensions: Time, Z, (wavelength) (or any combination thereof)
·Line scan: straight line (includes rotation), free line, point XY scan
Zoom size Observation position zoom with inclination width modification of
galvanometer mirror: 1–50X (adjustable in 0.1X increments
Confocal detector
(The M scanner does not have a confocal detector)
·Detector: 3 channels for fluorescence detection
(photomultipliers),
optional 4CH detector for expansion
·Dichromatic mirrors for excitation, dichromatic mirrors for
multiphoton excitation,
dichromatic mirrors for fluorescence, emission filter
·Infrared cut filter: using a high-performance filter
·A filter or spectral type of fluorescence detector can be
selected
Spectral type: Channels 1 and 2 provided with independent grating and slit
Selectable wavelength range: 1 – 100 nm,
wavelength resolution: 2 nm,
wavelength switching speed: 100 nm/ms
·Pinhole: Single motorized pinhole,
pinhole diameter: ø50 – 800µm (spectral type ø50 – 300µm),
adjustable in 1 µm increments
·Field Number: 18
-
Optics with infrared laser for multiphoton imaging ·Integrates a multiphoton near-infrared pulsed laser
in the scanning unit (Laser safety measures implemented)
·Continuously variable output using AOM
(0.1 – 100%, 0.1% increments)
Component incorporating the laser for multiphoton imaging Main scanner for observation ASU scanner for laser light stimulation, Main scanner for observation: VIS laser Incorporating 2 independent
lasers for laser
light stimulation/
observation
M scanner for observation
Detector for multiphoton imagingReflected light fluorescent detector Photomultiplier (2 or 4 channels),
Fluorescence wavelength can be selected with the dedicated filter cube
(replaceable)
Transmitted light fluorescent detector Photomultiplier (2 channels),
Fluorescence wavelength can be selected with the dedicated filter cube
(replaceable) (not combinable with IX-SVL2)
Exclusive equipment for the BX61WI upright microscope
Transmitted DIC unit ·Integrated transmitted light detector and transmitted illuminator,
Motorized switching Connected to microscope via fiber cable
(IR-DIC observation using an infrared laser is not possible)
Z-drive ·A motorized focus module inside the microscope is used
·Minimum increment: 0.01µm
Microscope Upright microscopes: BX61WI, BX61 Inverted microscope: IX81
System control ·OS: WindowsXP Professional (English version),
WindowsVista (English version)
·CPU: Core2Duo 2.33GHz
·Memory: 2.0GB or larger
·Hard disk: 320GB or larger
·Dedicated I/F board: built-in PC
·Graphics board: Open GL-compliant
·Recording media: Equipped with DVD dual drive
Software FV10-ASW Ver.2.0 or later
Required installation environment Room temperature: 25°C ± 1°C, humidity: 60% or less@25°C,
dust level: Class 10000, requires continuous (24-hour) power supply
Vibration isolation table for microscope and laser installation, size 1500 mm x 1250 mm 1500 mm x
1500 mm
1700 mm x
1700 mm
1500 mm x 1250mm
 
For specific details on clinical applications for this product, please contact your local Olympus Australia/New Zealand representative.
 
 
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