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    Á¦Ç°ÄÚµå MR150
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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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