Raman Filters

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Product Description
  • Outer diameter 25.0 mm, with mechanical retaining ring
  • High environmental resistance, long service life
  • FWHM: 3 nm, 4 nm, 5 nm, 6 nm, 7 nm
  • Center wavelength: 266 nm-1064 nm
  • Optical density in stop band: OD5, OD6
LBTEK offers CHROMA Raman Filters with a diameter of 25 mm and mechanical retaining rings. Raman Filters are bandpass filters with a bandwidth of less than 10 nm, used in instruments such as Raman spectrometers. Raman filters fully transmit only the central wavelength, with optical densities in the stop band reaching as high as OD5 and OD6. LBTEK's CHROMA Raman filters utilize a magnetron sputtering coating process, resulting in high transmittance, a high cutoff depth, and a high steepness. In Raman spectroscopy applications, they effectively reduce stray light interference, improve spectral signal quality, and enhance detection sensitivity and accuracy.
Attribute
Base materialUV fused silica
Transmitted Wavefront Error (TWE) (@633 nm)λ
Surface finish (scratches/pits)60/40
Raman long-pass filter
  • Longpass Filter
  • Cut-On Wavelength: 270 nm-1072 nm
  • Outer Diameter 25.0 mm, with Mechanical Retaining Ring
  • Angle of Incidence: 0°

LBTEK Raman long-pass filters include two types: low wavenumber Raman long-pass filters and conventional Raman long-pass filters. They are optical filters that allow light with wavelengths longer than a specific wavelength to pass through. They exhibit high transmittance (Tavg > 90%) for light longer than the starting (cut-off) wavelength and high blocking depth (ODavg > 6) for light shorter than the starting (cut-off) wavelength. The filters are pre-installed in Ø25.0 mm black anodized aluminum rings, with the light propagation direction marked by an arrow on the housing for easy installation and use. Raman long-pass filters are recommended for use at an incident angle of 0°. When used at incident angles deviating from the design angle, the starting (cut-off) wavelength may shift.

Raman long-pass filter installed on the coaxial mounting plate

Product Model
Start (Stop) Wavelength
Wave Number
Diameter
Unit Price
Curve
Compare
Lead Time
RET1072LP New1072 nm~96 cm-1Ø25.0 mm$717.25
7 weeks
RET837LP New837 nm~132 cm-1Ø25.0 mm$717.25
7 weeks
RET792LP New792 nm~160 cm-1Ø25.0 mm$717.25
7 weeks
RET638LP New638 nm~177 cm-1Ø25.0 mm$717.25
7 weeks
RET493LP New493 nm~228 cm-1Ø25.0 mm$717.25
7 weeks
RET359LP New359 nm~368 cm-1Ø25.0 mm$717.25
7 weeks
RET270LP New270 nm~271 cm-1Ø25.0 mm$717.25
7 weeks
RET787LP-X New787 nm~72 cm-1Ø25.0 mm$1074.95
7 weeks
RET634LP-X New634 nm~79 cm-1Ø25.0 mm$1074.95
7 weeks
RET533LP-X New533 nm~94 cm-1Ø25.0 mm$1074.95
7 weeks
RET489LP-X New489 nm~125 cm-1Ø25.0 mm$1074.95
7 weeks
RET537LP New537 nm~209 cm-1Ø25.0 mm$717.25
7 weeks
Raman Dichroic Mirror
  • Longpass Dichroic Mirror
  • Reflection Cutoff & Transmission Start Wavelength: 266 nm-785 nm
  • Ø25.0 mm (Mounted), Ø25.0 mm (Unmounted), 36 mm x 25.5 mm
  • Incidence Angle: 45°

LBTEK Raman long-pass dichroic mirrors are filters that allow long wavelengths to pass through while reflecting or absorbing short wavelengths. They exhibit high transmittance (Tavg > 90%) for light with wavelengths longer than the cut-on (cut-off) wavelength and high reflectance (Ravg > 90%) for light with wavelengths shorter than the cut-on (cut-off) wavelength. Raman long-pass dichroic mirrors are available in two types: mounted (Ø25.0 mm) and unmounted (Ø25.0 mm & 36 mm x 25.5 mm). For the mounted version, an arrow (↑) engraved on the housing indicates the direction of light propagation, while for the unmounted version, an arrow (>) on the side indicates the direction of the coated surface, facilitating installation and use. Raman long-pass dichroic mirrors are recommended for use at an incident angle of 45°. If the incident angle deviates from the design angle, the cut-on (cut-off) wavelength will shift.

The Raman dichroic mirror is installed on the coaxial mounting plate.

Product Model
Start (Stop) Wavelength
Wave Number
Size
Unit Price
Curve
Compare
Lead Time
RT633RDC New633 nm158 cm-1Ø25.0 mm (with mounting)$764.44
7 weeks
RT532RDC New532 nm209 cm-1Ø25.0 mm (with mounting)$764.44
7 weeks
RT785RDC-R New785 nm120 cm-136.0×25.5 mm (L×W)$764.44
7 weeks
RT633RDC-R New633 nm158 cm-136.0×25.5 mm (L×W)$764.44
7 weeks
RT532RDC-R New532 nm209 cm-136.0×25.5 mm (L×W)$764.44
7 weeks
RT488RDC-R New488 nm187 cm-136.0×25.5 mm (L×W)$764.44
7 weeks
RT355RDC-R New355 nm468 cm-136.0×25.5 mm (L×W)$764.44
7 weeks
RT266RDC-R New266 nm271 cm-136.0×25.5 mm (L×W)$764.44
7 weeks
RT785RDC-UM New785 nm120 cm-1Ø25.0 mm (Not Installed)$764.44
7 weeks
RT532RDC-UM New532 nm209 cm-1Ø25.0 mm (Not Installed)$764.44
7 weeks
RT266RDC-UM New266 nm271 cm-1Ø25.0 mm (Not Installed)$764.44
7 weeks
Raman Filters
  • Center Wavelength: 266 nm-1064 nm
  • FWHM: 3 nm, 4 nm, 5 nm, 6 nm, 7 nm
  • Stopband Optical Density: OD5, OD6

LBTEK offers CHROMA Raman Filters with a diameter of 25 mm and mechanical retaining rings. The mechanical retaining rings are marked with arrows indicating the incident direction, with light coming along the arrow direction for easy installation and use. When the incident angle deviates from the designed angle, the center wavelength may shift. It is recommended to use at the designed angle.

The Raman filter is mounted on the coaxial mounting plate.
Product Model
Center wavelength
Full Width at Half Maximum (FWHM)
Passband transmittance
Unit Price
Curve
Compare
Lead Time
RET785/3x New785 nm3 nmTabs>90%@785 nm$717.25
7 weeks
RET633/3x New633 nm3 nmTabs>90%@632.8 nm$717.25
7 weeks
RET532/2x New532 nm2 nmTabs>90%@532 nm$717.25
7 weeks
RET1064/7x 1064 nm7 nmTabs>90%@1064 nm;$717.25
today
RET830/6x 830 nm6 nmTabs>93%@830 nm;$717.25
today
RET785/6x 784.5 nm6 nmTabs>93%@785 nm;$717.25
today
RET633/5x 632.3 nm5 nmTabs>93%@632.8 nm;$717.25
8 weeks
RET532/4x 532 nm4.5 nmTabs>93%@532 nm;$717.25
today
RET488/4x 487.7 nm4.2 nmTabs>93%@488 nm;$717.25
today
RET355/3x 355 nm3 nmTabs>88%@355 nm;$717.25
today
RET266/3x 266 nm3 nmTabs>55%@266 nm;$717.25
today
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