مشخصات محصول
3D Scanning Laser Spectrometer RAMOS CARS
Spatial XYZ resolution of CARS signals (Objective lens: 60х, NA=1.2, watter immersion): |
< 0.7 μm |
Spatial resolution of Raman signals (excitation wavelength 633 nm; objective lens: 60х, NA=1.2, watter immersion): |
XY: < 300 nm Z: < 700 nm |
Spectral detectable range: | CARS signals: 985 – 5000 cm-1 Raman signals: 75 – 6000 cm-1 |
Spectral resolution: | CARS signals: 7-8 cm-1 Raman signals: 0.25 cm-1(grating 75 l/mm Echelle); 0.6 cm-1 (grating 1800 g/mm) |
Scanning range (fast scanning mode, 60x lens) | XY: 225 х 225 μm Z: 80 μm |
Control and automation: | Fully motorized |
Optical microscope
Type: | inverted |
Model: | Nikon Ti-U |
Stage: | motorized |
– travel range: | 114 х 75 mm |
– accuracy (for 1 mm traveling): | 0.06 μm |
– XY repeatability: | ± 1 μm |
– minimal step: | 0.02 μm |
Micro- objective lens: | 60 х NA-1.2 water immersion 20 x NA-0.45 |
Z-scanner: | |
– type: | piezo scanner |
– lens movement range: | 80 μm |
– minimal step: | 50 nm |
– Reapetability: | < 6 nm |
Illuminator for reflection mode: | Halogen lamp 100 W |
Illuminator for transmission mode: | LED |
Laser input port: | motorized triple turret |
High resolution digital video camera: | |
– type: | digital color CCD camera |
– sensor: | 1/2″, 2048 x 1536 pixeles |
– ADC: | 10 bit, 12 frames per min |
CARS excitation laser system
Single module optical parametric laser system consisting of: | |
Picosecond solit state Nd:YVO4 laser | |
Output wavelength: | 1064 nm |
Pulse duration: | 6.5 ps |
Output power: | 6 W |
Pulse repetition rate: | 85 MHz |
Mode composition: | TEM00 |
Beam quality (М2): | < 1.5 |
Beam diameter: | 2 mm |
Tunable SOPO (Synchronously pumped Optical Parametrical Oscillator) |
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Wavelength tuning range: | 690 – 990 nm |
Output power: | > 400 mW (at 800 nm) |
Pulse duration: | 5 – 6 ps |
Pulse repetition rate: | 85 MHz |
Polarization: | horizontal |
Mode composition: | TEM00 |
Beam quality (М2): | < 1.2 |
Beam diameter: | 2 mm |
Built-in delay tuning optical line |
Laser for Raman spectroscopy
Laser type: | cw HeNe |
Wavelength: | 632.8 nm |
Average output power: | > 10 mW |
Polarization: | linear |
Beam diameter: | 0.65 mm |
Beam divergence: | < 1.24 mrad |
Laser beam convergence and appointment unit
Laser shutter: | 3 pieces (Nd:YVO4 laser, SOPO and HeNe laser) |
Polarizer: | 2 pieces (Nd:YVO4 laser and SOPO) |
Wavelength plate λ/2 | 2 pieces (Nd:YVO4 laser and HeNe laser) |
Variable telescope: | 3 pices (Nd:YVO4 laser, SOPO and HeNe laser) |
Main optical unit
Optimized optics for spectral range: | 400 – 1100 nm |
Polarization analyzer: | Glan-Teylor prism |
Laser beam attenuator: | veriable neutral density filter 0 – 3D |
Pinhole lens positioner: | three-axis (X, Y, Z) |
CARS, Raman, fluorescence filters positioner: | five- position |
Posotioner of dihroic mirrors: | six- position |
Imaging monochromator / spectrograph MS5004i
Focal length: | 520 mm |
F number (input): | 9.8 |
Horizontal magnification: | 1.0 |
Vertical magnification: | 1.0 |
Vertical spatial resolution: | < 20 μm |
Flat field size: | 28 х 5 mm |
Stray light ( 20 nm from 633 nm laser line) |
1 х 10-5 |
Difraction gratings unit: | 4-position motorized grating turret |
Spectral resolution (wavelength 633 nm, CCD pixel size: 12×12 μm) |
0.01 nm (Echelle grating 75 l/mm) 0.025 nm (grating 1800 l/mm) |
Entrance spectral slit | motorized confocal pinhole, continuously adjustable from 0 to 1.5 mm |
Output spectral slit: | motorized, width from 0 to 2 mm (continuously adjustable) |
Ports: | 1 input, 2 output |
Detector (Raman, E-CARS, fast measurements) | Hamamatsu Photosensor module H7844 (with TE cooling) |
Monochromator for fluorescence measurements (integrated with MS5004i)
Focal length: | 100 mm |
Input spectral slit: | motorized confocal pinhole |
Output spectral slit: | fixed, width 4.2 mm |
Difraction grating: | 600 l/mm |
Spectral range: | 400 – 920 nm |
Linear reciprocal dispersion: | 13 nm/mm |
Detector | Hamamatsu Photosensor module H7844 (with TE cooling) |
Spectral CCD camera (Raman, E-CARS)
Type: | digital CCD camera |
Photosensor: | back-thinned CCD sensor 2048 х 122 pixels |
Pixel size: | 12 х 12 μm |
Photosensitive area: | 24.576 х 1.464 mm (length х heigh) |
Spectral sensitivity range: | from 200 to 1100 nm |
Cooling with temperature stabilization: | two-stage Peltier (TE) cooling down to – 45 °С |
ADC digitization: | 16 bit |
Sensitivity: | 1 photon for 1 ADC count (at 650 nm) |
Dinamic range: | at least 10 000 |
Fast scanning unit (X, Y)
Scanners: | Galvano-mirror scanners (X, Y) |
Scanning model: | raster high speed and start-stop mode |
Positioning accuracy: | < 30 μm |
Scanning area: | 225 μm х 225 μm (objective lens 60Х) |
Full frame scanning speed: | 4 s/frame: 1000 х 1000 points |
Laser confocal microscope unit (Reflected)
Prepinhole lens positioner: | three -axis (X, Y, Z) |
Confocal pinhole: | motorized confocal pinhole, continuously adjustable from 0 to 1.5 mm |
Detector: | Hamamatsu Photosensor module H6780-01 |
F-CARS and transmitted signal registration system
Polarization alanyzer: | Glan-Teylor prism |
F-CARS filters positioner: | 4-position, motorized |
F-CARS signal registration detector: | Hamamatsu Photosensor module H7844 (with TE cooling) |
Transmitted signal registration detector: | Hamamatsu Photosensor module H6780-01 |
Registration and processing control unit
Number of registration channels: | 5 |
Number of simultaneously registered channels: | up to 5 |
PC connection interface: | Ethernet 100 Base-T (TCP/IP protocol) |
Multifunctional – RAMOS CARS combines:
Multi-channel – five channels for simultaneous high-speed measurements:
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Polysterene balls of various diameter (F-CARS, 3045 cm-1) |
Advantages of CARS method
- high sensitivity: CARS generates more intensive and directed signals in comparison to spontaneous Raman microscopy;
- anti-Stokes CARS signal has frequency exceeding pumping waves frequencies and is detected in a spectral range free from the stray light of Stokes luminescence;
- CARS signal is registrated only in a focus where excitation intensity is the highest. It allows imaging with a high spatial resolution using non-confocal pinholes and also performs 3D layer-by-layer scanning with minimal neighboring layers influence on measuring results;
- spectral resolution of CARS signal is defined only by the width of pumping lasers lines, what simplifies spectral measurements, as detection of CARS signals can be performed without any spectral instrument;
- CARS signal is proportional to the squared molecule concentration, it allows using CARS (along with the selectivity and noninvasivity of the method) for quantitative measurements of chemical substance concentration in a sample;
- minimal invasive (nondestructive) CARS method for biological samples. Due to the high sensitivity of CARS method molecules in living cells can be detected without fluorescent markers.
FeaturesHigh spatial resolution:
Wide spectral range:
High spectral resolution:
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3D CARS image of liquid crystal 8CB structure on resonant frequency 2236 cm-1
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Simultaneous / multifunctional analysis:
Three types of CARS measurements:
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Multimodal CARS/TPEF image of growing cancer cells HeLa: DNA/RNA/Proteins/Lipids colored |
Five independent speed channels for simultaneous detection up to four 2D and 3D images:
- F-CARS: CARS signal in forward direction
- E-CARS & Raman: CARS signal in backward (EPI) direction/ Raman signal
- Reflected: reflected laser radiation signal
- Transmitted: transmitted laser radiation signal
- Luminescent: transmitted laser radiation signal
- Polarization control over the excitation and detection
- Mono-block laser system for CARS signal excitation
- Additional laser 633nm for excitation of a conventional one-photon fluorescence and spontaneous Raman scattering
- PC-controlled: switching of modes of measurement is performed by automatic switching of the components inside the system
Three scanning modes:
- Laser beam scanning over fixed sample surface with XY scanner
- Sample transfer by means of XY automated stage relative to the fixed laser beam
- Multiplexed mode for panorama imaging with a high speed and high spatial resolution: XY scanner + automated stage
Highly-precise calibration over the wavelengths: better than ±0,002nm due to an embedded calibration lamp as a source of reference lines for automated operative calibration of the monochromator-spectrograph. Block, rigid framing provides a high temporal and thermal stability.
Intuitive software NanoSP®:
Application
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Selective imaging of MIA-PaCa pancreatic human cancer cell for resonance 2845 cm -1 C-H bound (C-H aliphatic stretch). Selective lipids visualization. 3D image of a cell References: Dr. A. V. Kachynski, The Institute for Lasers, Photonics, and Bio-photonics, State University of New York at Buffalo |
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