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Plano-Convex Rectangular Cylindrical Lenses

Plano-convex rectangular cylindrical lenses are useful for line imaging or uni-axial magnification in a wide range of applications. These lenses may be combined with other lenses to form complex imaging systems.
  • product origin:

    China
  • shipping port:

    Fuzhou China
  • lead time:

    4 working weeks
  • payment:

    T/T Payment, Western Union
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  • description

Why are Plano-conves Retangular Cylindrical lenses used?


Plano-convex rectangular cylindrical lenses are available with positive or negative focal lengths, ideal for laser line generation or anamorphic beam shaping uni-axial magnification in a wide range of applications to circularize laser outputs.These lenses may be combined with other lenses to form complex imaging systems.


Plano-convex rectangular Cylindrical Lenses  Plano-convex rectangular Cylindrical Lenses


Specifications: 


Material: Optical glass, Fused silica
Design wavelength: 546.1nm
Diameter tolerance: +0/-0.05mm
Focal tolerance: +/-2%
surface quality : 40-20 S/D
Centration: 3 arcmin
Surface flatness: N=5 △N=0.5
Clear aperture: 90%
Bevel: Protective
Coating Optional



Part NO. Material W x H F(mm) R(mm) Tc(mm) Te(mm) Fb(mm)
ULYPX1010127 BK7 10.0x10.0 12.7 6.54 4.3 2 9.8
ULYPX1010020 BK7 10.0x10.0 20.0 10.29 3.3 2 17.8
ULYPX1010025 BK7 10.0x10.0 25.0 12.87 3.0 2 23
ULYPX1210010 BK7 12.0x10.0 10.0 5.2 5.9 2 6.17
ULYPX1210015 BK7 12.0x10.0 15.0 7.8 3.8 2 12.6
ULYPX1210020 BK7 12.0x10.0 20.0 10.34 3.3 2 17.8
ULYPX2010127 BK7 20.0x10.0 12.7 6.54 , 4.3 2 9.8
ULYPX2010020 BK7 20.0x10.0 20.0 10.29 3.3 2 17.8
ULYPX2010025 BK7 20.0x10.0 25.0 12.87 3.0 2 23
ULYPX2020050 BK7 20.0x20.0 50.0 25.73 4.0 2 47.3
ULYPX2020075 BK7 20.0x20.0 75.0 38.6 3.3 2 72.8
ULYPX2020100 BK7 20.0x20.0 100.0 51.47 4.0 2 97.3
ULYPX2020150 BK7 20.0x20.0 150.0 77.2 3.7 3 147.5
ULYPX2020200 BK7 20.0x20.0 200.0 102.93 3.5 3 197.7
ULYPX2020250 BK7 20.0x20.0 250.0 128.67 3.3 3 247.7
ULYPX2020300 BK7 20.0x20.0 300.0 154.4 3.2 3 297.8
ULYPX2020500 BK7 20.0x20.0 500.0 257.33 4.0 3 497.9
ULYPX4020050 BK7 40.0x20.0 50.0 25.73 3.3 3 47.3
ULYPX4020075 BK7 40.0x20.0 75.0 38.6 3.3 2 72.8
ULYPX4020100 BK7 40.0x20.0 100.0 51.47 4.0 2 97.3
ULYPX4020150 BK7 40.0x20.0 150.0 77.2 3.7 3 147.5
ULYPX4020200 BK7 40.0x20.0 200.0 102.93 3.5 3 197.7
ULYPX4020250 BK7 40.0x20.0 250.0 128.67 3.4 3 247.7
ULYPX4020300 BK7 40.0x20.0 300.0 154.4 3.3 3 297.8
ULYPX4020500 BK7 40.0x20.0 500.0 257.33 3.2 3 497.9

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Custom Truncated Doublet and Singlet Lenses
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Custom Truncated Doublet and Singlet Lenses from UNI Optics


We offer an extensive custom truncated doublet lens service. With our 30 year heritage of experience in the industry means we can always find the right product and specification for you, whether you require exotic materials, or exceptionally tight tolerances, we are confident in our ability to supply to your complete satisfaction. The table below is a brief overview of our doublet lens  and is not an exhaustive list. If your individual requirements are not met, then please contact our technical sales team who will be happy to advise.es and is n’t an exhaustive list. If your individual requirements are not met, then please contact our technical sales team who will be happy to advise.


Typical Specifications:


Typical materials: Flint (N/F2) and Crown (BK7)
                             Flint (SF6) and Crown (N-LAK22)
                             UV & IR materials on request
Diameter: 3mm to 200mm+
Focal length: 3mm to 1000mm+
Centration: < 3 arcseconds
Surface figure: < 0.1 fringe
Surface quality: < 10/5 Scratch/dig
Coating options: Single layer and BBAR coatings for UV/VIS/NIR with R.avg.<0.25%

More information on the achievable specifications for your individual application can be found by contacting our technical sales team. 

IR Optics material
Infrared Optics Material

1.  Germanium (Ge)


Germanium (Ge) is the preferred lens and window material for high performance infrared imaging systems in the 8–12 μm wavelength band. Its high refractive index makes Ge ideal for low power imaging systems because of minimum surface curvature. Chromatic aberration is small, often eliminating the need for correction.

 

Crystallographic properties
Syngony Cubic
Crystal Form Poly or Single Crystal
Lattice Constant 5.66
Cleavability <111>, non-perfect
Molecular Weight 72.6
Physical properties
Density, at 20 °C 5.33
Hardness, Mohs 6.3
Dielectric Constant for 9.37 × 109 Hz at 300 K 16.6
Melting 937
Thermal Conductivity, W/m·K at at 293 K 59
Thermal Expansion, 1/K at 298 K 6.1 × 10-6
Specific Heat Capacity, J/(kgK) at 273-373 K 0.074
Bandgap, eV 0.67
Knoop Hardness, kg/mm2 800
Youngs Modulus, Gpa 102.66
Shear Modulus, GPa 67.04
Bulk Modulus, GPa 77.86
Debye Temperature, K 370
Poissons Ratio 0.278
Elastic Coefficient C11=129, C12=48.3, C44=67.1
Apparent Elastic Limit 89.6 MPa (13000psi)
Chemical properties
Solubility in water None
Solubility in acids Soluble
Molecular Weight 72.59

2. Silicon (Si) 


Silicon (Si) is grown by Czochralski pulling techniques (CZ) and contains some oxygen that causes an absorption band at 9 microns.To avoid this, material can be prepared by a Float-Zone (FZ) process. Optical silicon is generally lightly doped (5 to 40 ohm cm) for best transmission above 10 microns, and doping is usually boron (P-type) and phosphorus (N-type). After doping silicon has a further pass band: 30 to 100 microns which is effective only in very high resistivity uncompensated material.
 
CZ Silicon is commonly used as substrate material for infrared reflectors and windows in the 1.5-8 micron region. The strong absorption band at 9 microns makes it unsuitable for CO2 laser transmission applications, but it is frequently used for laser mirrors because of its high thermal conductivity and low density. Application as window, lens in the 1.5 - 8 um region; Mirror for CO2 laser and spectrometer applications.
 

Crystallographic properties
Syngony Cubic
Lattice Constant, A 5.43
Physical properties
Density 2.33g/cm3
Hardness, Mohs 7
Dielectric Constant for 9.37 x 109 Hz 13
Melting point, оС 1414
Thermal Conductivity, W/m·K at 313 K 163
Thermal Expansion, 1/K at 293 K 2.6x10-6
Specific Heat Capacity, J/(kg°C) 712.8
Bandgap, eV 1.1
Knoop Hardness, kg/mm2 1100
Youngs Modulus, Gpa 130.91
Shear Modulus, GPan 79.92
Bulk Modulus, GPa 101.97
Debye Temperature, K 640
Poissons Ratio 0.28
Chemical properties
Solubility in water None
Molecular Weight 28.09

3、ZnS material:


ZnS MultiSpectral Under intense heat and pressure, defects within the crystalline lattice are virtually eliminated, leaving a water-clear material with minimal scatter and high transmission characteristics from 0.4 to 12 microns. This material is particularly well suited for high-performance common aperture systems that must perform across a broad wavelength spectrum.

Specifications:

Material: ZnS MultiSpectral
Diameter Tolerance: --------------------- +0.0, -0.1mm
Thickness Tolerance: -------------------- ±0.1mm
Clear Aperture: ---------------------------->85%
Parallelism: -----------------------------------3 arc minute
Surface Quality: ----------------------------80-50 scratch and dig
Wavefront Distortion: -------------------- λ /2 per 25mm @633mm
Bevel: -----------------------------------------Protective  (<0.2mm x 45° )
Coating: -------------------------------------- Optional (Uncoated, AR Coating, etc.)


4. ZnSe material


ZnSe is a preferred material for lenses, windows, output couplers and beam expanders for its low absorptivity at infrared wavelengths and its visible transmission. For high-power applications, it’s critical that the material bulk absorption and internal defect structure be carefully controlled, that minimum-damage polishing technology be employed, and the highest quality optical thin-film coatings are used. The material absorption is verified by CO2 laser vacuum calorimetry. Our quality assurance department provides testing and specific optics certification on request.

ZnSe is non-hygroscopic and chemically stable, unless treated with strong acids. It’s safe to use in most industrial field, and laboratory environments.



Optical color less glass
Optical Grade Glass
Optical glass can change the direction of light, as well as relative spectral distribution of ultraviolet, visible or infrared light.Optical glass material is the most common type because of its excellent optical properties such as high light transmission and environmental stability.
UN-GSWIR5014C
UN-GSWIR5014C
· Developed for 1" image format
· Wavelength: 900-1700nm
· Large Aperture, upto F1.4
· Compact and lightweight design
Laser Lenses
Laser beam collimation Lens

Laser Lenses are used to focus collimated light from laser beams in a variety of laser applications. Laser Lenses include a range of lens types including PCX Lenses, Cylinder Lenses, or Laser Generator Lenses. Laser Lenseare designed to focus light in several different ways depending on the lens type, such as focusing down to a point,  a line, or a ring. Many different lens types are available in a range of wavelengths.

UN-TFA1620X-12MP
UN-TFA1620X-12MP

Taurus Series 4/3Format FA Lens(12MP)

Model

UN-TFA1620X-12MP

Focal length

16mm

 


Aperture

F2.0-F22

Image Format

4/3(23mm)

Mount

C

 

Field Angle

D x H x V (°)

 

4/3

1

1/2"

D

73.0°

54.2°

28.3°

H

61.0°

44.3°

22.7°

V

47.3°

33.6°

17.1°

Optical Distortion

-1.93%@

y=11.5mm

-1.82%@

y=8.0mm

-0.55%@

y=4.0mm

M. O. D.

0.1m

Dimension

Φ60.2*85.9mm

Back Focal Length

21mm

Design Wavelength

420~1000nm

Operation

Manual  Iris

Manual  Focus

Filter Thread

M58.0×P0.75

Weight

339g

Work Temperature

-20℃+60℃

 


Beamsplitters Plates
Visible and NIR Plate Beamsplitters
Our beamsplitter plates can be used in high power laser system. When using beamsplitter plates, it is important to make it in mind that the two partial beams travel in different optical paths. The optical paths depend on the incident angle and the thickness of plates.
Plano-Convex Circular Cylindrical Lenses
Optical glass Plano Convex Circular Cylindrical Lenses
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