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DMLP900R - 25 mm x 36 mm Longpass Dichroic Mirror, 50% Trans./Refl. at 900 nm 
DMLP900R - 25 mm x 36 mm Longpass Dichroic Mirror, 50% Trans./Refl. at 900 nm
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DMLP900R
25 mm x 36 mm Longpass Dichroic Mirror, 50% Trans./Refl. at 900 nm
Part Number: DMLP900R - Ask a technical question Ask a technical question.
Weight: 0.07 lbs / Each
Available / Ships: Today
RoHS: RoHS Compliant
Price: $360.00
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DMLP900R Support Documentation
 
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Product Summary:

Features

  • Longpass Dichroic Mirror with Minimal Absorption Losses
  • 25 mm x 36 mm Filter
  • Hard Coating Allows Easy Handling and Cleaning
  • Resistant to Damage from UV Light and Chemicals

A dichroic mirror/beamsplitter functions as a 50:50 beamsplitter at its design wavelength, known as the cutoff wavelength. Thorlabs' DMLP900R Longpass Dichroic Mirror/Beamsplitter has a 900 nm cutoff wavelength and provides >90% average reflection from 400 - 872 nm and >90% average transmission from 932 - 1300 nm. It has a 25 mm x 36 mm size and is designed for use at a 45° incident angle.

Our dichroic mirrors/beamsplitters feature a dichroic coating on one surface and an antireflection coating on the opposing surface. The surface with the dichroic coating is engraved with the part number.

Dichroic mirrors/beamsplitters can be used to combine a beam that has a wavelength (or wavelength range) shorter than the design wavelength with a beam that has a wavelength (or wavelength range) longer than the design wavelength while minimizing intensity losses. Alternatively, spatially overlapping beams of different colors can be split with a single optic. This feature is commonly used in fluorescence microscopy to prevent light of the excitation wavelength from reaching the imaging detector.

Specifications

  • Cutoff Wavelength: 900 nm
  • Reflection Band: 400 - 872 nm
  • Transmission Band: 932 - 1300 nm
  • AR Coating Range: 932 - 1300 nm
  • Damage Threshold at 532 nm: 1.21 J/cm2 (10 Hz, 10 ns, Ø250 µm)
  • Damage Threshold at 1064 nm: 6.78 J/cm2 (10 Hz, 12 ns, Ø250 µm)

Applications

  • Fluorescence Microscopy
  • Splitting or Combining Two Beams of Different Wavelengths
  • Filtering of Spectral Components
  • Laser Applications that Require Minimal Wavefront Distortion

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