Our 1064 nm antireflection coated UV grade fused silica plano-concave lenses are designed to meet the demanding requirements of laser beam expansion applications. These lenses are polished to tight tolerances using master test plates to ensure minimum wavefront distortion. Tight surface quality tolerances minimize scatter and unwanted diffraction effects.
| Compare | Model | Drawings, CAD & Specs | Availability | Price | |||
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SPC010AR.33 Plano-Concave Lens, Fused Silica, 6.35 mm, -12.5 mm EFL, 1064 nm | $194 |
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SPC013AR.33 Plano-Concave Lens, Fused Silica, 12.7 mm, -25 mm EFL, 1064 nm |
2 Weeks
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$194 |
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SPC016AR.33 Plano-Concave Lens, Fused Silica, 25.4 mm, -1000 mm EFL, 1064 nm |
In Stock
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$161 |
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SPC019AR.33 Plano-Concave Lens, Fused Silica, 25.4 mm, -250 mm EFL, 1064 nm |
In Stock
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$160 |
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SPC022AR.33 Plano-Concave Lens, Fused Silica, 25.4 mm, -200 mm EFL, 1064 nm |
In Stock
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$165 |
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SPC025AR.33 Plano-Concave Lens, Fused Silica, 25.4 mm, -150 mm EFL, 1064 nm |
In Stock
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$165 |
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SPC028AR.33 Plano-Concave Lens, Fused Silica, 25.4 mm, -100 mm EFL, 1064 nm |
In Stock
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$165 |
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SPC031AR.33 Plano-Concave Lens, Fused Silica, 25.4 mm, -75 mm EFL, 1064 nm |
In Stock
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$165 |
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SPC034AR.33 Plano-Concave Lens, Fused Silica, 25.4 mm, -50 mm EFL, 1064 nm |
In Stock
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$165 |
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SPC037AR.33 Plano-Concave Lens, Fused Silica, 50.8 mm, -1000 mm EFL, 1064 nm |
In Stock
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$465 |
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SPC040AR.33 Plano-Concave Lens, Fused Silica, 50.8 mm, -500 mm EFL, 1064 nm | $445 |
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SPC043AR.33 Plano-Concave Lens, Fused Silica, 50.8 mm, -250 mm EFL, 1064 nm |
In Stock
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$494 |
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SPC046AR.33 Plano-Concave Lens, Fused Silica, 50.8 mm, -200 mm EFL, 1064 nm |
In Stock
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$582 |
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SPC049AR.33 Plano-Concave Lens, Fused Silica, 50.8 mm, -150 mm EFL, 1064 nm |
In Stock
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$641 |
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SPC052AR.33 Plano-Concave Lens, Fused Silica, 50.8 mm, -100 mm EFL, 1064 nm |
4 Weeks
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$680 |
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UV Grade Fused Silica is synthetic amorphous silicon dioxide of extremely high purity providing maximum transmission from 195 to 2100 nm. This non-crystalline, colorless silica glass combines a very low thermal expansion coefficient with good optical qualities, and excellent transmittance in the ultraviolet region. Transmission and homogeneity exceed those of crystalline quartz without the problems of orientation and temperature instability inherent in the crystalline form. It will not fluoresce under UV light and is resistant to radiation. For high-energy applications, the extreme purity of fused silica eliminates microscopic defect sites that could lead to laser damage. For more information, refer to our optical materials Technical Note
Our precision UV Fused Silica plano-convex lenses are polished to tight tolerances minimizing wavefront distortion. Tight surface quality tolerances minimize scatter and unwanted diffraction effects. These lenses have a 20-10 scratch-dig surface quality, and a λ/4 surface irregularity. For more information, refer to the optical surfaces technical note.
Our AR.33 laser line V-coating offers the lowest reflectance at 1064 nm for maximum transmission while maintaining high durability and high damage resistance. Valuable laser energy is efficiently transmitted through the plano-convex lens rather than lost to surface reflection and scattering. The trade off to its superior performance is the minimal laser line wavelength range.
Standard effective focal lengths on our plano-concave lenses provide a systematic approach allowing for lenses of different sizes and materials to be interchanged without requiring other changes to your optical system.
The lenses can be mounted in LT series lens tube for constructing a complex optical system or quickly connecting to other threaded lens mounts: A-Line™ series fixed lens mount, or adjustable lens positioner (with thread adapter). Use LT-WR series spanner wrench for easy lens installation.
As an application example, consider a Newport R-31005 HeNe Laser with beam diameter 0.63 mm and a divergence of 1.3 mrad. Note that these are beam diameter and full divergence, so in the notation of our figure, y1 = 0.315 mm and θ1= 0.65 mrad. To expand this beam ten times while reducing the divergence by a factor of ten, we could select a plano-concave lens KPC043 with f1 = -25 mm and a plano-convex lens KPX109 with f2 = 250 mm. Since real lenses differ in some degree from thin lenses, the spacing between the pair of lenses is actually the sum of the back focal lengths BFL1 + BFL2 = -26.64 mm + 247.61 mm = 220.97 mm.
The expanded beam diameter is: 2y3 = 2y1f2/|-f1| = 2(0.315 mm)(250 mm)/|-25 mm|= 6.3 mm.
The divergence angle is: θ3 = θ1|-f1|/f2 = (0.65 mrad)|-25 mm|/250 mm = 0.065 mrad.
For minimal aberrations, it is best to use a plano-concave lens for the negative lens and a plano-convex lens for the positive lens with the plano surfaces facing each other. To further reduce aberrations, only the central portion of the lens should be illuminated, so choosing oversized lenses is often a good idea. This style of beam expander is called Galilean.
We offer a full range of optical lens mounts to meet various experimental requirements. Below lists the recommended mounts for spherical lenses of standard sizes. Please see our Lens Mount Guide for additional information.
Note: besides the diameter, please check the Edge Thickness (Te) specification of the lens and the lens mount to ensure compatibility before purchasing.
| Lens Diameter |  A-Line™ Lens Mounts |
 LT Series Lens Tubes |
 LP Series Lens Positioners |
 Optics Cage Plus Series |
|---|---|---|---|---|
| 76.2 mm | ( |
N/A | N/A | N/A |
| 50.8 mm | ( |
N/A | ||
| 38.1 mm | ( |
LT20 lens tube with |
LP-2 lens positioner with |
N/A |
| 25.4 mm | ( |
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| 12.7 mm | ( |
N/A | ||
| 6.35 mm | LT05 lens tube with |
LP-05 lens positioner with |
N/A |
For non-standard sizes not listed above, check out our variable size lens mounts.
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