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45-824 9 mm Dia. N-LAK22/N-SF6 Achromatic Doublet; EFL=15mm NIR II 750-1550nm

45-824 9 mm Dia. N-LAK22/N-SF6 Achromatic Doublet; EFL=15mm NIR II 750-1550nm

Type
Lens
Subtype
Multiplets
Brand
Edmund Optics
Product webpage
Edmund Optics products in the 3DOptix catalog

Properties

Shape
Circular
Diameter
9 mm
EFL
15 mm
R1
9.68 mm
R2
-7.91 mm

Material 1

Name
N-LAK22
Dispersion Equation
Sellmeier
n (λ)
1.6536179449828925
λ
550 nm
B1
1.14229781
C1
0.00585778594 μm2
B2
0.535138441
C2
0.0198546147 μm2
B3
1.04088385
C3
100.834017 μm2

Material 2

Name
N-SF6
Dispersion Equation
Sellmeier
n (λ)
1.811866267147773
λ
550 nm
B1
1.77931763
C1
0.0133714182 μm2
B2
0.338149866
C2
0.0617533621 μm2
B3
2.08734474
C3
174.01759 μm2

45-824 9 mm Dia. N-LAK22/N-SF6 Achromatic Doublet; EFL=15mm NIR II 750-1550nm

The 45-824 is a high-performance achromatic doublet lens, boasting a 9 mm diameter and a focal length of 15 mm, specifically designed for use in the near-infrared spectrum, spanning from 750 to 1550 nm. This lens is sourced from the esteemed optical vendor, Edmund Optics, and is a multiplet type, ensuring superior image quality and minimal chromatic aberration.

The lens is crafted from two distinct materials, N-LAK22 and N-SF6, both from the reputable Schott glass catalog. These materials are carefully selected for their excellent optical properties in the NIR II range. The lens is coated with Edmund Optics' standard NIR-II coating on both the front and back surfaces, further enhancing its performance in the infrared spectrum.

The geometry of the lens is meticulously designed, with an inner radius of 0 mm, an outer radius of 0 mm, and a central thickness of 4.2 mm. The edge thickness measures 4.84 mm, while the first and second radii of curvature are 9.68 mm and -7.91 mm, respectively. The third radius of curvature is -39.89 mm, contributing to the lens's achromatic properties.

This lens is a versatile and high-quality option for applications that require superior performance in the NIR II spectrum. Its robust construction, precise geometry, and high-quality materials make it an ideal choice for a wide range of optical systems.

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