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Confotec MR150

It is a multifunction and compact confocal microscope.

MR150Àº ºÐ±¤ ºÐ¼®, ½ºÆåÆ®·³ º¸Á¤ Á¤È®µµ, º¸Æí¼º ¹× ´Ù¾çÇÑ ¶ó¸¸ ÃøÁ¤À» ¼öÇà ÇÒ ¼öÀÖ´Â ´É·ÂÀ¸·Î ÀÎÇØ °¡°Ý / Ç°Áú ±âÁØÀÇ ÃÖ´ë Á¡¼ö¸¦¹ÞÀ» ¼öÀÖ´Â µ¿±Þ ÃÖ°íÀÇ ¶ó¸¸ Çö¹Ì°æÀÔ´Ï´Ù.



³× °¡Áö ±¸¼º º¯ÇüÀ» ÅëÇØ »ç¿ëÀÚÀÇ ¿ä±¸¿¡ °¡Àå ÀûÇÕÇÑ ½Ã½ºÅÛ ¼Ö·ç¼ÇÀ» ¼±ÅÃÇÒ ¼ö ÀÖ½À´Ï´Ù.

 

MR150 is the best Raman microscope in its class that deserves the maximum score for the price/quality criterion due to its spectral resolution, spectral calibration accuracy, universality, and ability to perform a variety of Raman measurements.

 

Four configuration variants allow to choose the best system solution for your needs:


MR150-SMR, MR150-SR, MR150-S and MR150.

 

Features

  • Fully integrated with a standard optical microscope
  • Rigid design, no preadjustment is needed
  • Compact spectrograph with a fixed position of Grating provides high thermal and temporal stability of spectral measurements
  • Nondestructive analysis, no special requirements for sample preparations
  • Two automatic switchable lasers with different wavelengths allow to measure the Raman spectra of the various samples without influence of fluorescence background
  • Two independent imaging spectrometers allow to optimize the spectral range for each of the two installed lasers or achieve an extremely high spectral resolution using Echelle grating in a spectrometer
  • Only some sample areas are located in focus due to limited confocal depth of field. A high-speed reflected unit allows you to quickly find a sample focus areas and to use them for Raman measurements. This provides a significant gain in time and allows you to immediately apply a high numerical aperture objective to record high spatial resolution Raman maps
  • High speed and high spatial resolution panoramic Rayleigh scattering imaging using a galvano-mirror scanner and an automated microscope stage
  • Automatic spectral calibration
  • The whole spectral range at once may be recorded, without the need for scanning and spectrometer tuning

 

  • Compact spectrograph with a fixed position of Grating provides high thermal and temporal stability of spectral measurements
  • Nondestructive analysis, no special requirements for sample preparations
  • Two automatic switchable lasers with different wavelengths allow to measure the Raman spectra of the various samples without influence of fluorescence background
  • Two independent imaging spectrometers allow to optimize the spectral range for each of the two installed lasers or achieve an extremely high spectral resolution using Echelle grating in a spectrometer
  • Only some sample areas are located in focus due to limited confocal depth of field. A high-speed reflected unit allows you to quickly find a sample focus areas and to use them for Raman measurements. This provides a significant gain in time and allows you to immediately apply a high numerical aperture objective to record high spatial resolution Raman maps
  • High speed and high spatial resolution panoramic Rayleigh scattering imaging using a galvano-mirror scanner and an automated microscope stage
  • Automatic spectral calibration
  • The whole spectral range at once may be recorded, without the need for scanning and spectrometer tuning

Configuration

The most complete configuration corresponds to the model MR150-SMR, consisting

  • Microscope with an automated stage
  • Two automatic switchable lasers: one laser is integrated into the Raman system (473 nm or 532 nm), another one is external (633 nm or 785 nm)
  • Two independent imaging spectrometers in one housing, each of which has a diffraction grating in the fixed position and a CCD detector cooled by the Peltier element
  • X-Y galvanometer scanner
  • Z- piezoscanner
  • Reflected Unit for high speed imaging using Rayleigh scattering from a sample (3 sec / frame, 1001 x 1001 points)

Spatil resolution

 

Laser

Objective lens:

magnification and numerical aperture NA

Lateral resolution (XY)

Axial resolution (Z)

473 nm

 

100x, NA = 0.95

 

430 nm

585 nm

532 nm

 

100x, NA = 0.95

 

525 nm

705nm

633 nm

 

100x, NA = 0.95

 

570 nm

780 nm

785 nm

100x, NA = 0.95

 

995 nm

1280 nm

 

Spectral charecteristics

Spectral range for Raman spectra detection:

from 60 cm-1 to 11600 cm-1

(depends on the laser excitation wavelength)

Spectral resolution:

0.9 cm-1 (Echelle, 75 l/mm)

 

 

Scanning

 

Model

 

Scanning modes

 

Confotec

MR150-SMR

 

  • 2D / 3D Raman mapping of a sample with full spectra saving at each point using a high speed digital CCD and XY galvano-mirror / Z-piezo scanners
  • high speed 2D / 3D Rayleigh imaging (3 sec / frame, 1001 x 1001 points) using a Reflected unit and XY galvano-mirror / Z-piezo scanners
  • high speed and high spatial resolution panoramic Rayleigh scattering imaging using a Reflected unit, XY galvano-mirrors and an automated mi-croscope stage

 

 

 

Confotec MR150-SR

 

 

  • 2D / 3D Raman mapping of a sample with full spectra saving at each point using a high speed digital CCD and XY galvano-mirror / Z-piezo scanners
  • high speed 2D / 3D Rayleigh imaging (3 sec / frame, 1001 x 1001 points) using a Reflected unit and XY galvano-mirror / Z-piezo scanners

 

Confotec MR150-S

 

 

  • 2D / 3D Raman mapping of a sample with full spectra saving at each point using a high speed digital CCD and XY galvano-mirror / Z-piezo scanners

 

Confotec

MR150

 

  • One point Raman spectra measurement with a digital CCD camera

 

 

 

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