In stock
SKU
ATL - NADL
Visible spectrum achromats are air spaced achromatic triplets or doublets for lasers in the visible spectrum or white light applications. The elements are made of crown glass of low dispersion and flint glass of high dispersion.
Customize product
Filters
Enabled filters :
Remove all filters
| Name | Focal length | Delivery | Price | Add to cart | |||||||||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
|
i
Visible Spectrum Achromat 40.2mm Focal Length
ATL-30-40PY2 |
40.2mm |
in stock
|
$832.00
|
|
|
||||||||||||||||||
|
i
Visible Spectrum Achromat 80.1mm Focal Length
NADL-30-80PY2 |
80.1mm |
6-12 weeks
|
$696.00
|
|
|
||||||||||||||||||
|
i
Visible Spectrum Achromat 199.8mm Focal Length
NADL-30-200PY2 |
199.8mm |
6-12 weeks
|
$696.00
|
|
|
||||||||||||||||||
|
i
Visible Spectrum Achromat 49.4mm Focal Length
ATL-30-50PY2 |
49.4mm |
6-12 weeks
|
$832.00
|
|
|
||||||||||||||||||
|
i
Visible Spectrum Achromat 99.8mm Focal Length
NADL-30-100PY2 |
99.8mm |
6-12 weeks
|
$696.00
|
|
|
||||||||||||||||||
|
i
Visible Spectrum Achromat 58.9mm Focal Length
ATL-30-60PY2 |
58.9mm |
in stock
|
$832.00
|
|
|
||||||||||||||||||
|
i
Visible Spectrum Achromat 150.0mm Focal Length
NADL-30-150PY2 |
150mm |
6-12 weeks
|
$696.00
|
|
|
You must be logged in to ask questions
◦These lenses have been optimized for achromatic and spherical aberrations and coma for the 3 wavelengths; blue (486.1nm), green (546.1nm) and red (656.3nm). They are coated with a broadband multi-layer anti-reflection coating for 400 − 700nm.
◦Air spaced design allows high power laser applications which includes YAG second harmonic wavelength (532nm).
◦The triplets with F-numbers ≧2 and doublets with F-numbers ≧3 are designed to have each spot size equal to the diffraction limited spot size and very ideal for a Gaussian input beam.
◦Air spaced design allows high power laser applications which includes YAG second harmonic wavelength (532nm).
◦The triplets with F-numbers ≧2 and doublets with F-numbers ≧3 are designed to have each spot size equal to the diffraction limited spot size and very ideal for a Gaussian input beam.