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HBE Economy Plate Beamsplitters

From $20 USD

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Product description

HBE economy plate beamsplitters divide incident light into reflected and transmitted beams. The front S1 surface carries the beamsplitter coating; the rear S2 surface carries an antireflection coating to reduce interference and ghost reflections.

The 126 listed models use fine-annealed H-K9L glass at 45° angle of incidence. Circular and rectangular sizes are listed with their complete dimensions and 1.1 mm nominal thickness. Select each model by size, wavelength band and reflection/transmission ratio.

Listed R/T ratios are 30R/70T, 50R/50T and 70R/30T. The S1 splitting-ratio condition is ±10% average over the model band; the S2 AR condition is Ravg <1% over that band. VIS covers 400–700 nm, NIR 600–1100 nm and SWIR 900–1700 nm. These conditions do not imply performance outside the stated band.

Dimensional reference

Source generic circular and rectangular plate reference: 1.1 mm nominal thickness and S1/S2 surfaces. Reference only; not a manufacturing drawing. Individual model sizes and current H-K9L material are listed below.
Circular and rectangular plate beamsplitter reference with diameter, length, width, S1/S2 labels and 1.1 mm thickness.

The source states that B270 markings in product drawings refer to older batches; current material has been updated to H-K9L optical glass. Drawings are reference only, may contain discrepancies and must not be used for manufacturing. Model material remains H-K9L.

General specifications

Eight category common references remain separate from the seven fields in each actual model. Band-specific coating conditions are listed per model.

Substrate material
Fine-annealed H-K9L glass
Surface figure
4–8λ per inch
Size tolerance
+0.0/-0.25 mm
Thickness
1.1 mm ±0.2 mm
Surface quality
80-50
Clear aperture
90%
Parallelism
<3 arcmin
Edge finish
Cut edges

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
HBE-012-30-VISFine-annealed H-K9L glassØ12.5 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-025-30-VISFine-annealed H-K9L glassØ25.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$24
HBE-050-30-VISFine-annealed H-K9L glassØ50.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$41
HBE-12x12-30-VISFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-12x17-30-VISFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-20x30-30-VISFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$24
HBE-25x36-30-VISFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-30x30-30-VISFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-30x45-30-VISFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-35x35-30-VISFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-35x50-30-VISFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$39
HBE-50x50-30-VISFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$41
HBE-50x72-30-VISFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$54
HBE-75x75-30-VISFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm400–700 nm30R/70T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$85
HBE-012-50-VISFine-annealed H-K9L glassØ12.5 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-025-50-VISFine-annealed H-K9L glassØ25.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$24
HBE-050-50-VISFine-annealed H-K9L glassØ50.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$41
HBE-12x12-50-VISFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-12x17-50-VISFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-20x30-50-VISFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$24
HBE-25x36-50-VISFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-30x30-50-VISFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-30x45-50-VISFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-35x35-50-VISFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-35x50-50-VISFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$39
HBE-50x50-50-VISFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$41
HBE-50x72-50-VISFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$54
HBE-75x75-50-VISFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm400–700 nm50R/50T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$85
HBE-012-70-VISFine-annealed H-K9L glassØ12.5 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-025-70-VISFine-annealed H-K9L glassØ25.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$24
HBE-050-70-VISFine-annealed H-K9L glassØ50.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$41
HBE-12x12-70-VISFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-12x17-70-VISFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$20
HBE-20x30-70-VISFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$24
HBE-25x36-70-VISFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-30x30-70-VISFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-30x45-70-VISFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-35x35-70-VISFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$33
HBE-35x50-70-VISFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$39
HBE-50x50-70-VISFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$41
HBE-50x72-70-VISFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$54
HBE-75x75-70-VISFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm400–700 nm70R/30T45°VIS: splitting ratio (R/T), ±10% average @ 400–700 nmVIS: Ravg <1% @ 400–700 nm$85
HBE-012-30-NIRFine-annealed H-K9L glassØ12.5 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-025-30-NIRFine-annealed H-K9L glassØ25.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$29
HBE-050-30-NIRFine-annealed H-K9L glassØ50.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$45
HBE-12x12-30-NIRFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-12x17-30-NIRFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-20x30-30-NIRFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$29
HBE-25x36-30-NIRFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-30x30-30-NIRFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-30x45-30-NIRFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-35x35-30-NIRFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-35x50-30-NIRFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$43
HBE-50x50-30-NIRFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$45
HBE-50x72-30-NIRFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$58
HBE-75x75-30-NIRFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm600–1100 nm30R/70T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$93
HBE-012-50-NIRFine-annealed H-K9L glassØ12.5 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-025-50-NIRFine-annealed H-K9L glassØ25.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$29
HBE-050-50-NIRFine-annealed H-K9L glassØ50.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$45
HBE-12x12-50-NIRFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-12x17-50-NIRFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-20x30-50-NIRFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$29
HBE-25x36-50-NIRFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-30x30-50-NIRFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-30x45-50-NIRFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-35x35-50-NIRFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-35x50-50-NIRFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$43
HBE-50x50-50-NIRFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$45
HBE-50x72-50-NIRFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$58
HBE-75x75-50-NIRFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm600–1100 nm50R/50T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$93
HBE-012-70-NIRFine-annealed H-K9L glassØ12.5 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-025-70-NIRFine-annealed H-K9L glassØ25.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$29
HBE-050-70-NIRFine-annealed H-K9L glassØ50.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$45
HBE-12x12-70-NIRFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-12x17-70-NIRFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$24
HBE-20x30-70-NIRFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$29
HBE-25x36-70-NIRFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-30x30-70-NIRFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-30x45-70-NIRFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-35x35-70-NIRFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$37
HBE-35x50-70-NIRFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$43
HBE-50x50-70-NIRFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$45
HBE-50x72-70-NIRFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$58
HBE-75x75-70-NIRFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm600–1100 nm70R/30T45°NIR: splitting ratio (R/T), ±10% average @ 600–1100 nmNIR: Ravg <1% @ 600–1100 nm$93
HBE-012-30-SWIRFine-annealed H-K9L glassØ12.5 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-025-30-SWIRFine-annealed H-K9L glassØ25.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$31
HBE-050-30-SWIRFine-annealed H-K9L glassØ50.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-12x12-30-SWIRFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-12x17-30-SWIRFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-20x30-30-SWIRFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$31
HBE-25x36-30-SWIRFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-30x30-30-SWIRFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-30x45-30-SWIRFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-35x35-30-SWIRFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-35x50-30-SWIRFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-50x50-30-SWIRFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-50x72-30-SWIRFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$62
HBE-75x75-30-SWIRFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm900–1700 nm30R/70T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$97
HBE-012-50-SWIRFine-annealed H-K9L glassØ12.5 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-025-50-SWIRFine-annealed H-K9L glassØ25.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$31
HBE-050-50-SWIRFine-annealed H-K9L glassØ50.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-12x12-50-SWIRFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-12x17-50-SWIRFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-20x30-50-SWIRFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$31
HBE-25x36-50-SWIRFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-30x30-50-SWIRFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-30x45-50-SWIRFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-35x35-50-SWIRFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-35x50-50-SWIRFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-50x50-50-SWIRFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-50x72-50-SWIRFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$62
HBE-75x75-50-SWIRFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm900–1700 nm50R/50T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$97
HBE-012-70-SWIRFine-annealed H-K9L glassØ12.5 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-025-70-SWIRFine-annealed H-K9L glassØ25.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$31
HBE-050-70-SWIRFine-annealed H-K9L glassØ50.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-12x12-70-SWIRFine-annealed H-K9L glass12.5 × 12.5 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-12x17-70-SWIRFine-annealed H-K9L glass12.5 × 17.5 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$27
HBE-20x30-70-SWIRFine-annealed H-K9L glass20.0 × 30.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$31
HBE-25x36-70-SWIRFine-annealed H-K9L glass25.0 × 36.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-30x30-70-SWIRFine-annealed H-K9L glass30.0 × 30.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-30x45-70-SWIRFine-annealed H-K9L glass30.0 × 45.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-35x35-70-SWIRFine-annealed H-K9L glass35.0 × 35.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$41
HBE-35x50-70-SWIRFine-annealed H-K9L glass35.0 × 50.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-50x50-70-SWIRFine-annealed H-K9L glass50.0 × 50.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$47
HBE-50x72-70-SWIRFine-annealed H-K9L glass50.0 × 72.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$62
HBE-75x75-70-SWIRFine-annealed H-K9L glass75.0 × 75.0 × 1.1 mm900–1700 nm70R/30T45°SWIR: splitting ratio (R/T), ±10% average @ 900–1700 nmSWIR: Ravg <1% @ 900–1700 nm$97

Curves

Nine complete HBE transmission curves: VIS, NIR and SWIR, each with 30R/70T, 50R/50T and 70R/30T.
Nine complete source transmission plots: VIS 400–700 nm, NIR 600–1100 nm and SWIR 900–1700 nm, each in 30R/70T, 50R/50T and 70R/30T source order. The NIR gallery heading says700–1100 nm while its plotted range and listed models start at600 nm; the original source chart pixels are preserved. Typical reference curves; use the selected model specifications.

Technical notes

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