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HBS11 K9 Broadband Plate Beamsplitters

From $45 USD

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Product description

HBS11 broadband plate beamsplitters use fine-annealed H-K9L glass and are designed for 45° incidence. A beamsplitter coating on S1 divides the incident beam into reflected and transmitted light; an antireflection coating on S2 reduces unwanted reflections and ghost interference.

Choose the size, wavelength range and reflection/transmission ratio from the complete model table. Each model lists its own S1 beamsplitter coating and S2 antireflection coating specifications.

HBS11 plate beamsplitter reference dimensions

Reference drawing only; the source states that actual products may vary and this drawing must not be used for fabrication.
HBS11 K9 circular and rectangular plate beamsplitter dimension diagram. specifies 3 mm thickness.

General specifications

Common specifications apply to the HBS11 series. Model-specific sizes, wavelength ranges, splitting ratios and coatings are listed in the table.

Substrate material
Fine-annealed H-K9L glass
Surface figure
λ/2 per inch @632.8nm
Size tolerance
+0.0/-0.25mm
Thickness
3 mm ±0.2mm
Surface quality
60-40
Clear aperture
>90%
Parallelism
<1arcmin
Edge finish
Protective bevel 0.2–0.5mm×45°
Coating note
45° incidence; S1 beamsplitter coating, S2 antireflection coating
Unverified source standard entry
The source lists “HoSH”; its meaning and supporting standard are not specified.

Available specifications

USD unit prices. Shipping, taxes and dispatch timing are confirmed with your quotation. Select models and quantities to build your quote list.

126 models

DetailsQuote
HBS11-012-20-VISFine-annealed H-K9L glassØ12.5 mm350–700nm20R/80T(20%R/80%T)±10% @350-700nmRavg <1% @350-700nm$45
HBS11-012-30-VISFine-annealed H-K9L glassØ12.5 mm350–700nm30R/70T(30%R/70%T)±10% @350-700nmRavg <1% @350-700nm$45
HBS11-012-40-VISFine-annealed H-K9L glassØ12.5 mm350–700nm40R/60T(40%R/60%T)±10% @350-700nmRavg <1% @350-700nm$45
HBS11-012-50-VISFine-annealed H-K9L glassØ12.5 mm350–700nm50R/50T(50%R/50%T)±10% @350-700nmRavg <1% @350-700nm$45
HBS11-012-60-VISFine-annealed H-K9L glassØ12.5 mm350–700nm60R/40T(60%R/40%T)±10% @350-700nmRavg <1% @350-700nm$45
HBS11-012-70-VISFine-annealed H-K9L glassØ12.5 mm350–700nm70R/30T(70%R/30%T)±10% @350-700nmRavg <1% @350-700nm$45
HBS11-012-80-VISFine-annealed H-K9L glassØ12.5 mm350–700nm80R/20T(80%R/20%T)±10% @350-700nmRavg <1% @350-700nm$45
HBS11-12x17-20-VISFine-annealed H-K9L glass12.5 × 17.5 mm350–700nm20R/80T(20%R/80%T)±10% @350-700nmRavg <1% @350-700nm$47
HBS11-12x17-30-VISFine-annealed H-K9L glass12.5 × 17.5 mm350–700nm30R/70T(30%R/70%T)±10% @350-700nmRavg <1% @350-700nm$47
HBS11-12x17-40-VISFine-annealed H-K9L glass12.5 × 17.5 mm350–700nm40R/60T(40%R/60%T)±10% @350-700nmRavg <1% @350-700nm$47
HBS11-12x17-50-VISFine-annealed H-K9L glass12.5 × 17.5 mm350–700nm50R/50T(50%R/50%T)±10% @350-700nmRavg <1% @350-700nm$47
HBS11-12x17-60-VISFine-annealed H-K9L glass12.5 × 17.5 mm350–700nm60R/40T(60%R/40%T)±10% @350-700nmRavg <1% @350-700nm$47
HBS11-12x17-70-VISFine-annealed H-K9L glass12.5 × 17.5 mm350–700nm70R/30T(70%R/30%T)±10% @350-700nmRavg <1% @350-700nm$47
HBS11-12x17-80-VISFine-annealed H-K9L glass12.5 × 17.5 mm350–700nm80R/20T(80%R/20%T)±10% @350-700nmRavg <1% @350-700nm$47
HBS11-025-20-VISFine-annealed H-K9L glassØ25 mm350–700nm20R/80T(20%R/80%T)±10% @350-700nmRavg <1% @350-700nm$58
HBS11-025-30-VISFine-annealed H-K9L glassØ25 mm350–700nm30R/70T(30%R/70%T)±10% @350-700nmRavg <1% @350-700nm$58
HBS11-025-40-VISFine-annealed H-K9L glassØ25 mm350–700nm40R/60T(40%R/60%T)±10% @350-700nmRavg <1% @350-700nm$58
HBS11-025-50-VISFine-annealed H-K9L glassØ25 mm350–700nm50R/50T(50%R/50%T)±10% @350-700nmRavg <1% @350-700nm$58
HBS11-025-60-VISFine-annealed H-K9L glassØ25 mm350–700nm60R/40T(60%R/40%T)±10% @350-700nmRavg <1% @350-700nm$58
HBS11-025-70-VISFine-annealed H-K9L glassØ25 mm350–700nm70R/30T(70%R/30%T)±10% @350-700nmRavg <1% @350-700nm$58
HBS11-025-80-VISFine-annealed H-K9L glassØ25 mm350–700nm80R/20T(80%R/20%T)±10% @350-700nmRavg <1% @350-700nm$58
HBS11-25x36-20-VISFine-annealed H-K9L glass25 × 36 mm350–700nm20R/80T(20%R/80%T)±10% @350-700nmRavg <1% @350-700nm$66
HBS11-25x36-30-VISFine-annealed H-K9L glass25 × 36 mm350–700nm30R/70T(30%R/70%T)±10% @350-700nmRavg <1% @350-700nm$66
HBS11-25x36-40-VISFine-annealed H-K9L glass25 × 36 mm350–700nm40R/60T(40%R/60%T)±10% @350-700nmRavg <1% @350-700nm$66
HBS11-25x36-50-VISFine-annealed H-K9L glass25 × 36 mm350–700nm50R/50T(50%R/50%T)±10% @350-700nmRavg <1% @350-700nm$66
HBS11-25x36-60-VISFine-annealed H-K9L glass25 × 36 mm350–700nm60R/40T(60%R/40%T)±10% @350-700nmRavg <1% @350-700nm$66
HBS11-25x36-70-VISFine-annealed H-K9L glass25 × 36 mm350–700nm70R/30T(70%R/30%T)±10% @350-700nmRavg <1% @350-700nm$66
HBS11-25x36-80-VISFine-annealed H-K9L glass25 × 36 mm350–700nm80R/20T(80%R/20%T)±10% @350-700nmRavg <1% @350-700nm$66
HBS11-050-20-VISFine-annealed H-K9L glassØ50 mm350–700nm20R/80T(20%R/80%T)±10% @350-700nmRavg <1% @350-700nm$108
HBS11-050-30-VISFine-annealed H-K9L glassØ50 mm350–700nm30R/70T(30%R/70%T)±10% @350-700nmRavg <1% @350-700nm$108
HBS11-050-40-VISFine-annealed H-K9L glassØ50 mm350–700nm40R/60T(40%R/60%T)±10% @350-700nmRavg <1% @350-700nm$108
HBS11-050-50-VISFine-annealed H-K9L glassØ50 mm350–700nm50R/50T(50%R/50%T)±10% @350-700nmRavg <1% @350-700nm$108
HBS11-050-60-VISFine-annealed H-K9L glassØ50 mm350–700nm60R/40T(60%R/40%T)±10% @350-700nmRavg <1% @350-700nm$108
HBS11-050-70-VISFine-annealed H-K9L glassØ50 mm350–700nm70R/30T(70%R/30%T)±10% @350-700nmRavg <1% @350-700nm$108
HBS11-050-80-VISFine-annealed H-K9L glassØ50 mm350–700nm80R/20T(80%R/20%T)±10% @350-700nmRavg <1% @350-700nm$108
HBS11-50x72-20-VISFine-annealed H-K9L glass50 × 72 mm350–700nm20R/80T(20%R/80%T)±10% @350-700nmRavg <1% @350-700nm$124
HBS11-50x72-30-VISFine-annealed H-K9L glass50 × 72 mm350–700nm30R/70T(30%R/70%T)±10% @350-700nmRavg <1% @350-700nm$124
HBS11-50x72-40-VISFine-annealed H-K9L glass50 × 72 mm350–700nm40R/60T(40%R/60%T)±10% @350-700nmRavg <1% @350-700nm$124
HBS11-50x72-50-VISFine-annealed H-K9L glass50 × 72 mm350–700nm50R/50T(50%R/50%T)±10% @350-700nmRavg <1% @350-700nm$124
HBS11-50x72-60-VISFine-annealed H-K9L glass50 × 72 mm350–700nm60R/40T(60%R/40%T)±10% @350-700nmRavg <1% @350-700nm$124
HBS11-50x72-70-VISFine-annealed H-K9L glass50 × 72 mm350–700nm70R/30T(70%R/30%T)±10% @350-700nmRavg <1% @350-700nm$124
HBS11-50x72-80-VISFine-annealed H-K9L glass50 × 72 mm350–700nm80R/20T(80%R/20%T)±10% @350-700nmRavg <1% @350-700nm$124
HBS11-012-20-NIRFine-annealed H-K9L glassØ12.5 mm700–1100nm20R/80T(20%R/80%T)±10% @700-1100nmRavg <1% @700-1100nm$45
HBS11-012-30-NIRFine-annealed H-K9L glassØ12.5 mm700–1100nm30R/70T(30%R/70%T)±10% @700-1100nmRavg <1% @700-1100nm$45
HBS11-012-40-NIRFine-annealed H-K9L glassØ12.5 mm700–1100nm40R/60T(40%R/60%T)±10% @700-1100nmRavg <1% @700-1100nm$45
HBS11-012-50-NIRFine-annealed H-K9L glassØ12.5 mm700–1100nm50R/50T(50%R/50%T)±10% @700-1100nmRavg <1% @700-1100nm$45
HBS11-012-60-NIRFine-annealed H-K9L glassØ12.5 mm700–1100nm60R/40T(60%R/40%T)±10% @700-1100nmRavg <1% @700-1100nm$45
HBS11-012-70-NIRFine-annealed H-K9L glassØ12.5 mm700–1100nm70R/30T(70%R/30%T)±10% @700-1100nmRavg <1% @700-1100nm$45
HBS11-012-80-NIRFine-annealed H-K9L glassØ12.5 mm700–1100nm80R/20T(80%R/20%T)±10% @700-1100nmRavg <1% @700-1100nm$45
HBS11-12x17-20-NIRFine-annealed H-K9L glass12.5 × 17.5 mm700–1100nm20R/80T(20%R/80%T)±10% @700-1100nmRavg <1% @700-1100nm$47
HBS11-12x17-30-NIRFine-annealed H-K9L glass12.5 × 17.5 mm700–1100nm30R/70T(30%R/70%T)±10% @700-1100nmRavg <1% @700-1100nm$47
HBS11-12x17-40-NIRFine-annealed H-K9L glass12.5 × 17.5 mm700–1100nm40R/60T(40%R/60%T)±10% @700-1100nmRavg <1% @700-1100nm$47
HBS11-12x17-50-NIRFine-annealed H-K9L glass12.5 × 17.5 mm700–1100nm50R/50T(50%R/50%T)±10% @700-1100nmRavg <1% @700-1100nm$47
HBS11-12x17-60-NIRFine-annealed H-K9L glass12.5 × 17.5 mm700–1100nm60R/40T(60%R/40%T)±10% @700-1100nmRavg <1% @700-1100nm$47
HBS11-12x17-70-NIRFine-annealed H-K9L glass12.5 × 17.5 mm700–1100nm70R/30T(70%R/30%T)±10% @700-1100nmRavg <1% @700-1100nm$47
HBS11-12x17-80-NIRFine-annealed H-K9L glass12.5 × 17.5 mm700–1100nm80R/20T(80%R/20%T)±10% @700-1100nmRavg <1% @700-1100nm$47
HBS11-025-20-NIRFine-annealed H-K9L glassØ25 mm700–1100nm20R/80T(20%R/80%T)±10% @700-1100nmRavg <1% @700-1100nm$58
HBS11-025-30-NIRFine-annealed H-K9L glassØ25 mm700–1100nm30R/70T(30%R/70%T)±10% @700-1100nmRavg <1% @700-1100nm$58
HBS11-025-40-NIRFine-annealed H-K9L glassØ25 mm700–1100nm40R/60T(40%R/60%T)±10% @700-1100nmRavg <1% @700-1100nm$58
HBS11-025-50-NIRFine-annealed H-K9L glassØ25 mm700–1100nm50R/50T(50%R/50%T)±10% @700-1100nmRavg <1% @700-1100nm$58
HBS11-025-60-NIRFine-annealed H-K9L glassØ25 mm700–1100nm60R/40T(60%R/40%T)±10% @700-1100nmRavg <1% @700-1100nm$58
HBS11-025-70-NIRFine-annealed H-K9L glassØ25 mm700–1100nm70R/30T(70%R/30%T)±10% @700-1100nmRavg <1% @700-1100nm$58
HBS11-025-80-NIRFine-annealed H-K9L glassØ25 mm700–1100nm80R/20T(80%R/20%T)±10% @700-1100nmRavg <1% @700-1100nm$58
HBS11-25x36-20-NIRFine-annealed H-K9L glass25 × 36 mm700–1100nm20R/80T(20%R/80%T)±10% @700-1100nmRavg <1% @700-1100nm$66
HBS11-25x36-30-NIRFine-annealed H-K9L glass25 × 36 mm700–1100nm30R/70T(30%R/70%T)±10% @700-1100nmRavg <1% @700-1100nm$66
HBS11-25x36-40-NIRFine-annealed H-K9L glass25 × 36 mm700–1100nm40R/60T(40%R/60%T)±10% @700-1100nmRavg <1% @700-1100nm$66
HBS11-25x36-50-NIRFine-annealed H-K9L glass25 × 36 mm700–1100nm50R/50T(50%R/50%T)±10% @700-1100nmRavg <1% @700-1100nm$66
HBS11-25x36-60-NIRFine-annealed H-K9L glass25 × 36 mm700–1100nm60R/40T(60%R/40%T)±10% @700-1100nmRavg <1% @700-1100nm$66
HBS11-25x36-70-NIRFine-annealed H-K9L glass25 × 36 mm700–1100nm70R/30T(70%R/30%T)±10% @700-1100nmRavg <1% @700-1100nm$66
HBS11-25x36-80-NIRFine-annealed H-K9L glass25 × 36 mm700–1100nm80R/20T(80%R/20%T)±10% @700-1100nmRavg <1% @700-1100nm$66
HBS11-050-20-NIRFine-annealed H-K9L glassØ50 mm700–1100nm20R/80T(20%R/80%T)±10% @700-1100nmRavg <1% @700-1100nm$108
HBS11-050-30-NIRFine-annealed H-K9L glassØ50 mm700–1100nm30R/70T(30%R/70%T)±10% @700-1100nmRavg <1% @700-1100nm$108
HBS11-050-40-NIRFine-annealed H-K9L glassØ50 mm700–1100nm40R/60T(40%R/60%T)±10% @700-1100nmRavg <1% @700-1100nm$108
HBS11-050-50-NIRFine-annealed H-K9L glassØ50 mm700–1100nm50R/50T(50%R/50%T)±10% @700-1100nmRavg <1% @700-1100nm$108
HBS11-050-60-NIRFine-annealed H-K9L glassØ50 mm700–1100nm60R/40T(60%R/40%T)±10% @700-1100nmRavg <1% @700-1100nm$108
HBS11-050-70-NIRFine-annealed H-K9L glassØ50 mm700–1100nm70R/30T(70%R/30%T)±10% @700-1100nmRavg <1% @700-1100nm$108
HBS11-050-80-NIRFine-annealed H-K9L glassØ50 mm700–1100nm80R/20T(80%R/20%T)±10% @700-1100nmRavg <1% @700-1100nm$108
HBS11-50x72-20-NIRFine-annealed H-K9L glass50 × 72 mm700–1100nm20R/80T(20%R/80%T)±10% @700-1100nmRavg <1% @700-1100nm$124
HBS11-50x72-30-NIRFine-annealed H-K9L glass50 × 72 mm700–1100nm30R/70T(30%R/70%T)±10% @700-1100nmRavg <1% @700-1100nm$124
HBS11-50x72-40-NIRFine-annealed H-K9L glass50 × 72 mm700–1100nm40R/60T(40%R/60%T)±10% @700-1100nmRavg <1% @700-1100nm$124
HBS11-50x72-50-NIRFine-annealed H-K9L glass50 × 72 mm700–1100nm50R/50T(50%R/50%T)±10% @700-1100nmRavg <1% @700-1100nm$124
HBS11-50x72-60-NIRFine-annealed H-K9L glass50 × 72 mm700–1100nm60R/40T(60%R/40%T)±10% @700-1100nmRavg <1% @700-1100nm$124
HBS11-50x72-70-NIRFine-annealed H-K9L glass50 × 72 mm700–1100nm70R/30T(70%R/30%T)±10% @700-1100nmRavg <1% @700-1100nm$124
HBS11-50x72-80-NIRFine-annealed H-K9L glass50 × 72 mm700–1100nm80R/20T(80%R/20%T)±10% @700-1100nmRavg <1% @700-1100nm$124
HBS11-012-20-SWIRFine-annealed H-K9L glassØ12.5 mm900–1700nm20R/80T(20%R/80%T)±10% @900-1700nmRavg <1% @900-1700nm$47
HBS11-012-30-SWIRFine-annealed H-K9L glassØ12.5 mm900–1700nm30R/70T(30%R/70%T)±10% @900-1700nmRavg <1% @900-1700nm$47
HBS11-012-40-SWIRFine-annealed H-K9L glassØ12.5 mm900–1700nm40R/60T(40%R/60%T)±10% @900-1700nmRavg <1% @900-1700nm$47
HBS11-012-50-SWIRFine-annealed H-K9L glassØ12.5 mm900–1700nm50R/50T(50%R/50%T)±10% @900-1700nmRavg <1% @900-1700nm$47
HBS11-012-60-SWIRFine-annealed H-K9L glassØ12.5 mm900–1700nm60R/40T(60%R/40%T)±10% @900-1700nmRavg <1% @900-1700nm$47
HBS11-012-70-SWIRFine-annealed H-K9L glassØ12.5 mm900–1700nm70R/30T(70%R/30%T)±10% @900-1700nmRavg <1% @900-1700nm$47
HBS11-012-80-SWIRFine-annealed H-K9L glassØ12.5 mm900–1700nm80R/20T(80%R/20%T)±10% @900-1700nmRavg <1% @900-1700nm$47
HBS11-12x17-20-SWIRFine-annealed H-K9L glass12.5 × 17.5 mm900–1700nm20R/80T(20%R/80%T)±10% @900-1700nmRavg <1% @900-1700nm$49
HBS11-12x17-30-SWIRFine-annealed H-K9L glass12.5 × 17.5 mm900–1700nm30R/70T(30%R/70%T)±10% @900-1700nmRavg <1% @900-1700nm$49
HBS11-12x17-40-SWIRFine-annealed H-K9L glass12.5 × 17.5 mm900–1700nm40R/60T(40%R/60%T)±10% @900-1700nmRavg <1% @900-1700nm$49
HBS11-12x17-50-SWIRFine-annealed H-K9L glass12.5 × 17.5 mm900–1700nm50R/50T(50%R/50%T)±10% @900-1700nmRavg <1% @900-1700nm$49
HBS11-12x17-60-SWIRFine-annealed H-K9L glass12.5 × 17.5 mm900–1700nm60R/40T(60%R/40%T)±10% @900-1700nmRavg <1% @900-1700nm$49
HBS11-12x17-70-SWIRFine-annealed H-K9L glass12.5 × 17.5 mm900–1700nm70R/30T(70%R/30%T)±10% @900-1700nmRavg <1% @900-1700nm$49
HBS11-12x17-80-SWIRFine-annealed H-K9L glass12.5 × 17.5 mm900–1700nm80R/20T(80%R/20%T)±10% @900-1700nmRavg <1% @900-1700nm$49
HBS11-025-20-SWIRFine-annealed H-K9L glassØ25 mm900–1700nm20R/80T(20%R/80%T)±10% @900-1700nmRavg <1% @900-1700nm$62
HBS11-025-30-SWIRFine-annealed H-K9L glassØ25 mm900–1700nm30R/70T(30%R/70%T)±10% @900-1700nmRavg <1% @900-1700nm$62
HBS11-025-40-SWIRFine-annealed H-K9L glassØ25 mm900–1700nm40R/60T(40%R/60%T)±10% @900-1700nmRavg <1% @900-1700nm$62
HBS11-025-50-SWIRFine-annealed H-K9L glassØ25 mm900–1700nm50R/50T(50%R/50%T)±10% @900-1700nmRavg <1% @900-1700nm$62
HBS11-025-60-SWIRFine-annealed H-K9L glassØ25 mm900–1700nm60R/40T(60%R/40%T)±10% @900-1700nmRavg <1% @900-1700nm$62
HBS11-025-70-SWIRFine-annealed H-K9L glassØ25 mm900–1700nm70R/30T(70%R/30%T)±10% @900-1700nmRavg <1% @900-1700nm$62
HBS11-025-80-SWIRFine-annealed H-K9L glassØ25 mm900–1700nm80R/20T(80%R/20%T)±10% @900-1700nmRavg <1% @900-1700nm$62
HBS11-25x36-20-SWIRFine-annealed H-K9L glass25 × 36 mm900–1700nm20R/80T(20%R/80%T)±10% @900-1700nmRavg <1% @900-1700nm$69
HBS11-25x36-30-SWIRFine-annealed H-K9L glass25 × 36 mm900–1700nm30R/70T(30%R/70%T)±10% @900-1700nmRavg <1% @900-1700nm$69
HBS11-25x36-40-SWIRFine-annealed H-K9L glass25 × 36 mm900–1700nm40R/60T(40%R/60%T)±10% @900-1700nmRavg <1% @900-1700nm$69
HBS11-25x36-50-SWIRFine-annealed H-K9L glass25 × 36 mm900–1700nm50R/50T(50%R/50%T)±10% @900-1700nmRavg <1% @900-1700nm$69
HBS11-25x36-60-SWIRFine-annealed H-K9L glass25 × 36 mm900–1700nm60R/40T(60%R/40%T)±10% @900-1700nmRavg <1% @900-1700nm$69
HBS11-25x36-70-SWIRFine-annealed H-K9L glass25 × 36 mm900–1700nm70R/30T(70%R/30%T)±10% @900-1700nmRavg <1% @900-1700nm$69
HBS11-25x36-80-SWIRFine-annealed H-K9L glass25 × 36 mm900–1700nm80R/20T(80%R/20%T)±10% @900-1700nmRavg <1% @900-1700nm$69
HBS11-050-20-SWIRFine-annealed H-K9L glassØ50 mm900–1700nm20R/80T(20%R/80%T)±10% @900-1700nmRavg <1% @900-1700nm$115
HBS11-050-30-SWIRFine-annealed H-K9L glassØ50 mm900–1700nm30R/70T(30%R/70%T)±10% @900-1700nmRavg <1% @900-1700nm$115
HBS11-050-40-SWIRFine-annealed H-K9L glassØ50 mm900–1700nm40R/60T(40%R/60%T)±10% @900-1700nmRavg <1% @900-1700nm$115
HBS11-050-50-SWIRFine-annealed H-K9L glassØ50 mm900–1700nm50R/50T(50%R/50%T)±10% @900-1700nmRavg <1% @900-1700nm$115
HBS11-050-60-SWIRFine-annealed H-K9L glassØ50 mm900–1700nm60R/40T(60%R/40%T)±10% @900-1700nmRavg <1% @900-1700nm$115
HBS11-050-70-SWIRFine-annealed H-K9L glassØ50 mm900–1700nm70R/30T(70%R/30%T)±10% @900-1700nmRavg <1% @900-1700nm$115
HBS11-050-80-SWIRFine-annealed H-K9L glassØ50 mm900–1700nm80R/20T(80%R/20%T)±10% @900-1700nmRavg <1% @900-1700nm$115
HBS11-50x72-20-SWIRFine-annealed H-K9L glass50 × 72 mm900–1700nm20R/80T(20%R/80%T)±10% @900-1700nmRavg <1% @900-1700nm$131
HBS11-50x72-30-SWIRFine-annealed H-K9L glass50 × 72 mm900–1700nm30R/70T(30%R/70%T)±10% @900-1700nmRavg <1% @900-1700nm$131
HBS11-50x72-40-SWIRFine-annealed H-K9L glass50 × 72 mm900–1700nm40R/60T(40%R/60%T)±10% @900-1700nmRavg <1% @900-1700nm$131
HBS11-50x72-50-SWIRFine-annealed H-K9L glass50 × 72 mm900–1700nm50R/50T(50%R/50%T)±10% @900-1700nmRavg <1% @900-1700nm$131
HBS11-50x72-60-SWIRFine-annealed H-K9L glass50 × 72 mm900–1700nm60R/40T(60%R/40%T)±10% @900-1700nmRavg <1% @900-1700nm$131
HBS11-50x72-70-SWIRFine-annealed H-K9L glass50 × 72 mm900–1700nm70R/30T(70%R/30%T)±10% @900-1700nmRavg <1% @900-1700nm$131
HBS11-50x72-80-SWIRFine-annealed H-K9L glass50 × 72 mm900–1700nm80R/20T(80%R/20%T)±10% @900-1700nmRavg <1% @900-1700nm$131

Curves

All 21 HBS11 K9 VIS, NIR and SWIR transmission curve frames, with complete axes and data.
Twenty-one complete source transmission curves: VIS 350–700 nm, NIR 700–1100 nm and SWIR 900–1700 nm, each with 20R/80T, 30R/70T, 40R/60T, 50R/50T, 60R/40T, 70R/30T and 80R/20T in source order. Typical reference curves; use the selected model specifications.

Technical notes

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Illustrations and printable specification summaries are reference information, not manufacturing drawings. Confirm technical suitability and final requirements with your quotation.

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