CM112 Compact 1/8米单色仪

CM112是两个单独的单色仪串联在一起，第一个单色仪的出射狭缝就是第二个单色仪的入射狭缝。在抑制杂散光方面，两个单色仪如同一个双重滤波片，其能力相当于单个单色仪的平方。

CM112在出厂时可以配置成增强或者降低色散的双单色仪。增强色散型的第一个光栅将光谱以一定角度范围色散展开，第二个光栅则将这个色散加倍，从而获得比单个1/8米单色仪高一倍的分辨能力。降低色散型的第一个单色仪选定一个带宽，第二个单色仪则消除第一个单色仪光谱角色散所产生的时域和角度色差。

CM112 Compact 1/8 Meter Monochromator

• Compact size - Only 5-1/4"x6-1/4"x3-1/4"
• Connects to any computer via RS232.
• Scans in both directions. Programmable in angstroms, nanometers, microns, wavenumbers, or eV.
• Dual double-grating turrets with automatic grating change allows for broad spectral range coverage.
• Subtractive dispersion mode minimizes image distortion and pulse spread, with sub-picosecond residual broadening versus nanosecond pulse broadening of regular monochromators.
• Additive mode gives increased dispersion and low stray light for Raman and fluorescence studies.
• May be configured as a monochromator or a spectrograph.
• Monochromator may be factory configured for right angle or straight through beam path.

  The Digikröm CM112: Much More than a Monochromator

  The CM112 is two single monochromators in series. The exit slit of the first monochromator is the entrance slit of the second. The two monochromators act as a double filter with the rejection of stray light being almost the square of the single monochromator value.

  The CM112 may be factory configured as an additive or subtractive dispersion double monochromator. As an additive instrument, the first grating spreads the spectrum over an angular range; the second grating then doubles this dispersion. The result is twice the resolution of a single 1/8 meter monochromator. As a subtractive instrument, the first monochromator selects a bandpass, the second monochromator then removes the temporal and angular aberrations introduced by the angular spectral dispersion in the first monochromator.

  The CM112 offers a solution to practical problems in monochromatic imaging. Selecting a monochromatic image with an ordinary monochromator fails because multiple wavelengths in the bandpass create multiple, overlapping images. In the CM112, the second subtractive monochromator recombines these multiple images, creating a clear image.

  Finally, the CM112 is a unique solution to practical problems in the spectroscopy of pulsed sources. An ordinary monochromator has a spread in the internal optical path lengths that will introduce a 25 to 100 picosecond broadening in light pulses that are passed through the monochromator. In the subtractive dispersion CM112, the second monochromator equalizes the optical path lengths so that broadening is reduced to a minimum.

  Feature	Value
  Design:	Double cascaded Czerny-Turner. Double-grating turrets standard in each section.
  Focal Length:	110mm each section.
  f/#:	3.9 overall
  Beam Path:	Right angle or straight through
  Wavelength Drive:	Dual worm and wheel with electronic synchronization and computer control. Programable in additive or subtractive dispersion with positive or negative grating orders.
  Wavelength Precision:	0.1nm (additive)    0.2nm (subtractive)
  Wavelength Accuracy:	± 0.3nm (additive)    ± 0.6nm (subtractive)
  Max Resolution:	<0.5nm (additive)    <1nm (subtractive)
  Bandpass: with standard slits	0.25nm (additive)    0.50nm (subtractive)
  Slewing Speed:	>100nm/second
  Stray Light:	<10-9
  Slits:	Standard Set includes: 0.125mm, 0.15mm, 0.30mm, 0.6mm, 1.2mm and 2.4mm x 4.0mm. For other sizes, consult SP.
  Gratings:	Two or four gratings (30 x 30mm) must be purchased. See Appendix A for options
  Software:	Demonstration control program and LabView driver included.
  Power:	UL listed 110/220V power pack
  Warranty:	One year
  Options:	Hand-held control module with function keys and display for local control IEEE-488 interface See options and accessories

  If you need more information about this item, please call (505)343-9700 x100 or email sales@spectralproducts.com