Laserand Inc. is a Montreal, Canada based company working in the fields of photonics, robotics and industrial manufacturing & automation. The company supplies photonics components, scientific & industrial equipment and complex systems to customers in North America (USA & Canada) and around the world. Our team of engineers, marketing and technical support specialists with more than 15 years of experience in supplying optics, DPSS lasers, laser diodes, opto-mechanics, automation systems and motion control is ready to assist you in choosing the right product for your application. Contact us when you need integration services.
Laserand股份有限公司是一家总部位于加拿大蒙特利尔的公司，致力于光子、机器人和工业制造及自动化领域。该公司为北美（美国和加拿大）和世界各地的客户提供光子元件、科学和工业设备以及复杂系统。我们的工程师、营销和技术支持专家团队在提供光学、DPSS激光器、激光二极管、光机、自动化系统和运动控制方面拥有超过15年的经验，随时准备帮助您为您的应用选择合适的产品。
产品分类
Optics Laser & Nonlinear Crystals Lasers lmaging Motion control Hexapods
一、OPTICS
1.General Optics 2.Polarization Optics 3.Optical Systems
1.1 Lenses
1.2 Axicons (Conical Lens)
1.3 Dielectric Coated OpticsPrisms
1.4 Uncoated OpticalWindows/SubstratesMetallic Coated Optics
1.5 Filters
1.6 Non Polarizing Beamsplitter Cubes
Lenses
Lens is an optical device, which transmits and refracts light. We offer Plano-convex, Double-Convex, Plano-Concave Lenses, Double-Concave Lenses, Meniscus Lenses, Positive Cylindrical Lenses, Negative Cylindrical Lenses, Achromatic lenses, Aspherical lenses.
Plano-Convex Lenses
Positive focus length lenses have flat surface on one side and spherical surface on the other.
Centration, arcmin | <3 arcmin |
Clear Aperture, % | >90% |
Coatings | Available on request |
Design Wavelength, nm | 632.8 nm |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Focal Length Tolerance, % | ±3 % |
Protective chamfers | <0,25 mm x 45 deg |
Surface Figure | <λ/4@632.8 nm |
Surface Quality, S-D | 40/20 |
Thickness Tolerance, mm | ±0.1 mm |
Plano-Concave Lenses
One surface of a PCV negative focus length lenses is flat, the other is spherical.
Centration, arcmin | <3 arcmin |
Clear Aperture, % | >90% |
Coatings | Available on request |
Design Wavelength, nm | 632.8 nm |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Focal Length Tolerance, % | ±3 % |
Protective chamfers | <0.25 mm x 45° |
Surface Figure | <λ/4@632.8 nm |
Surface Quality, S-D | 40/20 |
Thickness Tolerance, mm | ±0.1 mm |
Double-Convex Lenses
Double convex lenses are symmetrical therefore have equal radius on both sides.
Centration, arcmin | <3 arcmin |
Clear Aperture, % | >90% |
Coatings | Available on request |
Design Wavelength, nm | 632.8 nm |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Focal Length Tolerance, % | ±3 % |
Protective chamfers | <0,25 mm x 45 deg |
Surface Figure | <λ/4@632.8 nm |
Surface Quality, S-D | 40/20 |
Thickness Tolerance, mm | ±0.1 mm |
Double-Concave Lenses
Double concave lenses are symmetrical with equal radius on both sides.
Centration, arcmin | <3 arcmin |
Clear Aperture, % | >90% |
Coatings | Available on request |
Design Wavelength, nm | 632.8 nm |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Focal Length Tolerance, % | ±3 % |
Protective chamfers | <0,25 mm x 45 deg |
Surface Figure | <λ/4@632.8 nm |
Surface Quality, S-D | 40/20 S/D |
Thickness Tolerance, mm | ±0.1 mm |
Meniscus Lenses
These positive and negative focus length lenses have different radii on both sides.
Centration, arcmin | <3 arcmin |
Clear Aperture, % | >90% |
Coatings | Available on request |
Design Wavelength, nm | 632.8 nm |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Focal Length Tolerance, % | ±3 % |
Protective chamfers | <0,25 mm x 45 deg |
Surface Figure | <λ/4@632.8 nm |
Surface Flatness | 40/20 S/D |
Thickness Tolerance, mm | ±0.1 mm |
Negative Cylindrical Lenses
A negative focus length cylindrical lens expands light in one dimension only.
Centration, arcmin | <3 arcmin |
Clear Aperture, % | >90% |
Coatings | Available on request |
Design Wavelength, nm | 632.8 nm |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Focal Length Tolerance, % | ±3 % |
Protective chamfers | <0,25 mm x 45 deg |
Surface Figure | <λ/4@632.8 nm |
Surface Flatness | 40/20 S/D |
Thickness Tolerance, mm | ±0.1 mm |
Achromatic lenses
A compound lens system that forms an image free from chromatic aberration.
Centration, arcmin | <3 arcmin |
Clear Aperture, % | >90% |
Coatings | VIS or NIR coated |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Focal Length Tolerance, % | ±3 % |
Material | All type of material are available to design the optimal achromats |
Protective chamfers | <0,25 mm x 45 deg |
Surface Figure | λ/4@632.8nm |
Surface Quality, S-D | 60/40 S/D |
Thickness Tolerance, mm | ±0.1 mm |
Axicons (Conical Lens)
Axicon lenses are conical lenses which, when followed by a conventional lens, can focus laser light to a ring shape. Using an axicon together with a spherical lens will produce an annular focus for hole drilling applications. We offer Plano-Convex , Plano-Concave, Double Convex Axicons
Double Convex Axicon (Conical lens)
Laserand offers Double Convex Axicons of various dimensions and Apex angles.
Material | BK7, UVFS |
Diameter Tolerance, mm | +0.0, -0.15 mm |
Edge Thickness, mm | 9 mm |
Apex Angle, deg | 90 |
Clear Aperture, mm | >90% |
Surface Quality, S-D | 40/20 S/D |
Apex Angle Tolerance, arcmin | +/-0.5 |
Thickness Tolerance, mm | ±0.1 mm |
Design Wavelength, nm | 632.8 nm |
Plano-Convex Axicon (Conical lens)
Axicon lens is a conical lens which, when paired with a conventional lens, can focus laser beam into a ring shaped beam.
Material | UVFS |
Diameter Tolerance, mm | +0.0/-0.15 |
Clear Aperture, % | >90 |
Surface Quality, S-D | 40-20 |
Apex Angle Tolerance, arcmin | ±0.5°. Available down to +/-0.02° |
Thickness Tolerance, mm | ±0.1 |
Protective chamfers | <0.25 mm x 45 deg |
Plano-Concave Axicon (Conical lens)
Laserand offers Plano-Concave Axicons of various dimensions and Apex angles.
Diameter Tolerance, mm | +0.0/-0.15 |
Clear Aperture, % | >90 |
Surface Quality, S-D | 60-40 |
Apex Angle Tolerance, arcmin | ±0.5°. Available down to +/-0.02° |
Thickness Tolerance, mm | ±0.1 |
Protective chamfers | <0.25 mm x 45 deg |
Coatings | Available on request |
Dielectric Coated Optics
Coatings for Dielectric coated optics are provided by Ion Beam Sputtering (IBS) or electron beam evaporation with/without ion assistance coating techniques. We offer HR Laser Line, HR Broad Band, Partial reflecting, Dual Laser Line reflecting mirrors, Wavelength separators, AR coated, Broad Band AR coated and Dual AR coated windows.
Ultra-Broadband Dielectric Mirrors
Ultra-Broadband Dielectric Mirrors high reflect in the range 350 - 1100 nm, AOI - (0°-50°).
Clear Aperture, % | >85 |
Diameter Tolerance, mm | +0/-0.25 |
Laser Damage Threshold, J/cm² | 1 J/cm² @ 355 nm |
Surface Flatness | <λ/4 @ 632.8 nm |
Surface Quality, S-D | 60-40 |
Thickness Tolerance, mm | ±0.2 mm |
HR Laser Line mirrors (HR)
High Reflection (HR) Laser Line mirrors provide an optimized performance at a specific wavelength and a certain angle of incidence (AOI).
Clear Aperture, % | >90 |
Coating Adhesion and Durability | Per MIL-C-675A |
Diameter Tolerance, mm | +0.0/-0.15 |
Laser Damage Threshold, J/cm² | >12 J/cm² for 10 ns pulses @1064nm (for 1047-1064 nm mirrors) |
Parallelism Error, arcsec | <30 |
Protective chamfers | <0.35 mm x 45° |
Surface Flatness | <λ/8 @632.8 nm |
Surface Quality, S-D | 20-10 |
Thickness Tolerance, mm | ±0.2 |
HR Right Angle Retroreflector
HR right angle retroreflector consists of two HR coated mirrors. 90° angle is as precise as ±5 arcsec.
Clear Aperture, % | >80 |
90 deg Angle Tolerance, arcmin | ±30 arcsec |
Dimension Tolerances, mm | +0.0/-0.2 |
Material | UVFS |
Protective chamfers | <0.25 mm x 45 deg |
Pyramidal tolerance, arcmin | <1 arcmin |
Surface Flatness | <λ/8 @ 632.8 nm |
Surface Quality, S-D | 20-10 |
Low Loss HR Mirrors
Low loss HR mirrors are produced by using IBS coating technique, which makes nearly all mirror specification being supreme to the ones provided by other coating technologies. It allows to minimize scatter in dielectric layers, which is a limiting factor, then reflectivity higher than 99.9% is targeted.
Clear Aperture, % | >90 |
Coating Adhesion and Durability | Per MIL-C-675A |
Diameter Tolerance, mm | +0.0/-0.15 mm |
Laser Damage Threshold, J/cm² | >12 J/cm² for 10 ns pulses @ 1064 nm |
Protective chamfers | <0.35 mm x 45 deg |
Surface Flatness | <λ/8 @632.8 nm |
Surface Quality, S-D | 20/10 |
Thickness Tolerance, mm | ±0.2 mm |
HR Broad Band mirrors (BBHR)
HR broad band mirrors (BBHR) provide high reflectance for a broad spectrum.
Clear Aperture, % | >90% |
Coating Adhesion and Durability | Per MIL-C-675A |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Laser Damage Threshold, J/cm² | >2-3 J/cm² for 10 ns pulses @1064 nm |
Measured Reflectivity, % | R>99% @ AOI=0° |
Protective chamfers | <0.35 mm x 45° |
Substrate Material | UVFS (optionally BK7) |
Surface Flatness | <λ/8 @ 632.8 nm |
Surface Quality, S-D | 20/10 |
Thickness Tolerance, mm | ±0.1 mm |
Non-polarizing Plate Beamsplitters
Non-polarizing beamsplitting plates exhibit a polarization insensitve performance.
Clear Aperture, % | >90% |
Coating Adhesion and Durability | Per MIL-C-675A |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Laser Damage Threshold, J/cm² | >6 J/cm2 for 10 ns pulses @1064 nm |
Protective chamfers | <0,25 mm x 45 deg |
(Rs-Rp), % | <5 % |
Surface Flatness | <λ/8 @ 632.8 nm |
Surface Quality, S-D | 20/10 S/D |
Thickness Tolerance, mm | ±0.1 m |
Low GDD Ultrafast Mirrors
Low GDD Ultrafast mirrors are intended for femtosecond Ti:Sapphire, Nd:Glass, Er:Glass, Yb:KYW, Yb:KGW and Yb:CaF2 lasers ant their harmonics.
Clear Aperture, % | >90 |
Coating Adhesion and Durability | Per MIL-C-675A |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Laser Damage Threshold, J/cm² | >100 mJ/cm² for 50 fs pulses @ 800 nm |
Material | UVFS |
Protective chamfers | <0,25 mm x 45 deg |
Surface Flatness | <λ/8 @ 632.8 nm |
Surface Quality, S-D | 20/10 (10/5 on request) |
Thickness Tolerance, mm | ±0.1 mm |
Laser Output Coupler
Output coupler (OC) is a partially reflecting dielectric mirror used in laser cavity.
Clear Aperture, % | >90% |
Coating Adhesion and Durability | Per MIL-C-675A |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Laser Damage Threshold, J/cm² | >10J/cm² for 10 ns pulses @ 1064 nm |
Protective chamfers | <0.25 mm x 45 deg |
Surface Flatness | <λ/8 @ 632.8 nm |
Surface Quality, S-D | 20-10 |
Thickness Tolerance, mm | ±0.1 mm |
Prisms
Prism is an optical element, which refracts light. We offer: Dispersing, Right-Angle, Penta, Dove, Anamorphic, Wedge, Littrow, Beamsplitter Penta Prisms, Corner Cube Retroreflectors and Right-Angle Prism-Retroreflectors
Dispersing Prisms
Dispersing prisms are used for wavelength separation applications.
Angle Tolerance, arcmin | ±2 arcmin |
Clear Aperture, % | >80% |
Dimension Tolerances, mm | +0.0/-0,2 mm |
Protective chamfers | <0,25 mm x 45 deg |
Pyramidal tolerance, arcmin | ±1 arcmin |
Surface Flatness | λ/4 @ 632.8 nm |
Surface Quality, S-D | 40/20 S/D |
Brewster Angle Dispersing Prisms For Ultrashort Pulses
High quality dispersing prisms for intra and extra cavity use in ultrashort pulse laser systems.
Angle Tolerance, arcmin | ±3 arcmin |
Clear Aperture, % | >80% |
Dimension Tolerances, mm | +0.0/-0.2 mm |
Protective chamfers | <0.25 mm x 45° |
Right-Angle Prism
These prisms are used to direct beams at 90 degrees by using hypotenuse face in total internal reflection (TIR).
Clear Aperture, % | >80% |
90 deg Angle Tolerance, arcmin | ±2 (general type); |
Dimension Tolerances, mm | +0/-0.2 |
Protective chamfers | <0.25 mm x 45° |
Pyramidal tolerance, arcmin | ±1 (general type); |
Surface Flatness | λ/4 @ 633 nm |
Surface Quality, S-D | 40/20 S/D |
Right-Angle Prism-Retroreflectors
Clear Aperture, % | >80% |
90 deg Angle Tolerance, arcmin | ±2 (general type); ±0.12 (precision type) |
Dimension Tolerances, mm | +0/-0,2 |
Protective chamfers | <0,25 mm x 45 deg |
Pyramidal tolerance, arcmin | ±1 (general type); ±0.5 (precision type) |
Surface Flatness | λ/4 @ 633 nm |
Surface Quality, S-D | 40/20 S/D |
Corner Cube Retroreflectors
BK7 or UVFS Corner cube retroreflectors designed to deviate incident light by 180 degrees independently of an angle of incidence.
Angular Deviation, arcsec | ±5 arcsec |
Beam Deviation | 180° ± 30 arcsec |
Clear Aperture, % | >80% |
Dimension Tolerances, mm | +0.0/-0.2 mm |
Protective chamfers | <0.25 mm x 45° |
Surface Flatness | λ/10 @ 632.8 nm |
Surface Quality, S-D | 40/20 S/D |
Beamsplitter Penta Prism
Beamsplitter penta prism assembly combines the transmitting/reflecting function of a beamsplitter with the 90 deg path bend associated with a penta prism (no inversion or reversion).
Penta Prism
Penta prism's function is to deviate the direction of the light beam by 90 degrees.
Clear Aperture, % | >80% |
Coatings | Available on request |
90 deg Angle Tolerance, arcmin | <30 arcsec |
Dimension Tolerances, mm | +0.0/-0,2 mm |
Protective chamfers | <0,25 mm x 45 deg |
Surface Flatness | λ/4 @ 632.8 nm |
Surface Quality, S-D | 40/20 S/D |
Dove Prisms
A Dove prism is a type of reflective prism which is used to invert an image.
Angle Tolerance, arcmin | < 3 arcmin |
Clear Aperture, % | >80% |
Dimension Tolerances, mm | +0.0/-0,2 mm |
Protective chamfers | <0,25 mm x 45 deg |
Surface Flatness | λ/4 @ 632.8 nm |
Surface Quality, S-D | 40/20 S/D |
Uncoated Optical Windows/Substrates
Various dimensions substrates made from BK7, UVFS, IRFS, CaF2, ZnSe, Sapphire, MgF2. Standard substrates are laser grade polished on both surfaces. These substrates are ideal for beamsplitters, windows, partial reflecting mirrors etc.
Uncoated Optical Windows/Substrates
Substrates of various sizes and dimensions are made of BK7, UVFS, FS, CaF2, ZnSe, Sapphire, MgF2.
Clear Aperture, % | >90% |
Coatings | uncoated |
Diameter, mm | +0.0/-0.1 mm |
Protective chamfers | <0.25 mm x 45° |
Surface Flatness | <λ/10 - λ/8@632.8 nm (BK7, UVFS) |
Surface Quality, S-D | 20/10 S/D (BK7, UVFS) |
Thickness Tolerance, mm | ±0.1 mm |
Precision Uncoated Optical Windows/Substrates
High performance uncoated optical windows/substrates for demanding applications
Clear Aperture, % | >90 % |
Coatings | uncoated |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Parallelism, arcsec | < 5 arcsec |
Protective chamfers | <0.25 mm x 45° |
Surface Quality, S-D | 10/5 S/D |
Thickness Tolerance, mm | ±0.1 mm |
Transmitted Wavefront Distortion | <λ/10@632.8 nm |
Metallic Coated Optics
Metallic coatings can be used at any angle of incidence because they have extremely broadband reflectance. We offer Gold, Silver and Aluminum high reflection coatings formed by vacuum deposition. All metallic reflectors can be over-coated with dielectric film of MgF2 or SiO2 in order to prevent oxidation of the metallic surface and provide abrasion resistance.
Metallic Coated Round Optics
Metallic mirrors and partial reflectors
Clear Aperture, % | >90% |
Laser Damage Threshold, J/cm² | Protected Aluminum: >0.25 J/cm² for 11 ns pulses @1064 nm |
Substrate Dimension Tolerance, mm | +0.0/-0.1 mm |
Substrate Material | BK7, UVFS for UV enhanced mirrors |
Surface Flatness (After Coating) | L/4 |
Surface Quality ( After Coating), Scratch &Dig | 40/20 S/D |
Right Angle Prism Mirror
Right angle mirrors are used for simplifying alignment and increasing the rigidity of an optical system.
Clear Aperture, % | >80% of the face size |
90 deg Angle Tolerance, arcmin | ±2 arcmin |
Dimension Tolerances, mm | +0.0/-0.2 mm |
Laser Damage Threshold, J/cm² | Protected Aluminum: >0.25 J/cm² for 11 ns pulses @1064 nm |
Pyramidal tolerance, arcmin | ±1 arcmin |
Surface Accuracy | λ/4 @ 632.8 nm |
Surface Quality, S-D | 40/20 S/D |
Elliptical Flat Mirrors
Elliptical flat aluminum, silver and gold coated mirrors.
Clear Aperture, % | >90% |
Diameter Tolerance, mm | +0.0/-0.1 mm |
Laser Damage Threshold, J/cm² | Protected Aluminum: >0.25 J/cm² for 11 ns pulses @1064 nm |
Material | BK7, UVFS for UV enhanced mirrors |
Parallelism, arcsec | <30 arcsec |
Protective chamfers | <0,25 mm x 45 deg |
Protective Coating | SiO2 |
Surface Flatness | <λ/8 @ 633 nm |
Surface Quality, S-D | 40/20 S/D |
Thickness Tolerance, mm | +/-0.1 mm |
Cylindrical Concave Metallic Coated Mirrors
Cylindrical concave metallic coated mirrors focus a light to a thin line in one dimention only.
Clear Aperture, % | >90% |
Edge Thickness, mm | 5 mm |
Focal Length Tolerance, % | +/- 1% |
Laser Damage Threshold, J/cm² | Protected Aluminum: >0.25 J/cm² for 11 ns pulses @1064 nm |
Surface Accuracy | λ/4 @ 632.8 nm |
Surface Quality, S-D | 40/20 S/D |
Off-Axis Parabolic Metal Mirrors
Laserand provides standard and special metal mirrors with parabolic surface contours for off-axis beam focusing performance.
Diameter Tolerance, mm | +0.00/-0.40 mm |
Focal Length Tolerance, % | +/- 1% |
Material | Aluminium |
Surface Figure | 1/4λ - 1λ RMS (depends on size) |
Surface Roughness, RMS | < 100-175 Å RMS |
Filters
Optical glass filters are widely used in safety glasses, industrial measurement, environment protection and many other applications. We offer: Color Glass, Interference, Neutral Density, Circular Variable Neutral Density and Linear Variable Density Filters.
Non Polarizing Beamsplitter Cubes
Non Polarizing Beamsplitter Cubes are constructed by cementing two precision right angle prisms together with metallic-dielectric coating on the hypotenuse surface. Absorption loss due to coating is around 10%, moreover these cubes do not affect the polarization of the beam!
2.Polarization Optics
2.1 Glan Type and Other Polarizers
2.2 Polarizing Cubes
2.3 Waveplates (Phase Retardation Plates)
2.4 Other Products
Glan Type and Other Polarizers
We offer: High Power Laser Glan, Glan Taylor, Glan Thompson, Wollaston, Rochon Polarizers and Beamdisplacer.
Polarizing Cubes
Polarizing cubes for specified wavelength (250-2200 nm) AR coated on four input and output working surfaces. Polarizing Beamsplitter Cubes split randomly polarized beams into two orthogonal, linearly polarized components: s polarized light is reflected at a 90 degrees angle while p-polarized light is transmitted.
Waveplates (Phase Retardation Plates)
Waveplates are made from materials which exhibit birefringence. The velocity of the extraordinary and ordinary rays through the birefringent material varies inversely with their refractive indices. This difference in velocities gives a rise to phase difference. At any specific wavelength the phase difference is governed by the thickness of the retarder - waveplate. We offer: Crystalline quartz, Achromatic (Broadband), Mid-IR and High Power Waveplates.
Other Products
3.Optical Systems
3.1 Montorized Polarization Rotators
3.2 Beam Expanders
3.3 Laser Power Attenuators
3.4 Flat-Top Converter
Glan Type and Other Polarizers
We offer: High Power Laser Glan, Glan Taylor, Glan Thompson, Wollaston, Rochon Polarizers and Beamdisplacer.
Beam Expanders
Laser Power Attenuators
Flat-Top Converter
二、Laser & Nonlinear Crystals
1.Nonlinear Crystals 2.Laser Crystals 3.Passive Q-Switch Crystals 4.Photorefractive Crystals 5.Birefringent Crystals 6.Raman Crystals
1.Nonlinear Crystals
Nonlinear Optics section is for optical elements, which dielectric polarization responds nonlinearity to the electric field. Nonlinear Optics includes: Nonlinear, Photorefractive, Birefringent and Raman crystals.
2.Laser Crystals
3. Passive Q-Switch Crystals
4.Photorefractive Crystals
Photorefractive crystals can be used in various applications: Pockels Readout Optical Memory (PROM), as thin film optical waveguides, Photorefraction, Holographic Recording, Wave Mixing and Phase Conjugation. We offer: SBN, BSO, Fe:LiNbO3, BGO, BSO, BTO, Fe:Ti:Ce:LiNbO3 crystals
5. Birefringent Crystals
The refractive index of Birefringent crystal depends on the polarization and direction of light. These crystals are widely used in production of polarizing devices. We Offer: YVO4 Crystal and CaCO3.
6.Raman Crystals
We offer large variety of nonlinear materials for a high efficiency Stimulated Raman Scattering (SRS) conversion with low thresholds for nanosecond and picosecond laser pulses. These materials provide SRS conversion to a wide range of wavelengths.
三、Lasers
1.Single Frequency CW DPSS Lasers 2.Laser Accessories
Single Frequency CW DPSS Lasers
We supply a wide range of high performance Continuous Wave Single Frequency DPSS lasers. We focus on SLM DPSS lasers in mid to high powers.Our products have excellent output beam parameters and performance characteristics. We offer many wavelengths, some of them unattainable elsewhere and others have the highest output power on the market.
Laser Accessories
四、Imaging
1.THz lmaging 2.CCD Cameras 3.Optical Spectroscopy Systems
THz lmaging
4.1NIR VIS UV cameras 4.2 WUV EUV X-ray cameras 4.3 VUV EUV X-ray in-vacuum cameras
NIR VIS UV cameras
Based on a unique platform concept, greateyes offers a portfolio of scientific cameras for imaging and spectroscopy in the UV, VIS and NIR range. The deep-cooled, high-performance CCD detectors are very compact. They combine highly sensitive sensors with ultra-low noise 16-bit electronics for optimal detection of weak signals. Select among different pixel formats, several sensor technologies and various sensor coatings to find the best solution for your imaging or spectroscopic application. The full-frame CCD sensors are integrated in hermetically sealed vacuum chambers with multi-stage Peltier elements. The cameras provide a rich set of functionalities including flexible binning operation, various trigger and synchronization modes, software switchable gain as well as temperature monitoring of the sensor and the Peltier hot side.
VUV EUV X-ray cameras
Based on a unique platform concept, greateyes offers a portfolio of scientific cameras with vacuum interface for imaging and spectroscopy in the VUV, EUV, soft and hard X-ray range. Incoming photons are directly detected by the CCD sensor. Beside the precise measurement of high energy radiation, the detectors exhibit a high sensitivity in the ranges NIR, VIS and UV as well. All our offered cameras combine scientific CCD sensors with ultra-low noise electronics for optimal detection of weak signals. Select among different spectral sensitivities and flange types to find the best solution for your imaging or spectroscopic application. The full frame CCD sensors are cooled by multi-stage Peltier elements. The cameras provide a rich set of functionalities including flexible binning operation, various trigger and synchronization modes, software switchable gain as well as temperature monitoring of the sensor and the Peltier hot side.
VUV EUV X-ray in-vacuum cameras
Based on a unique platform concept, greateyes offers a portfolio of scientific in-vacuum cameras for imaging and spectroscopy in the VUV, EUV, soft and hard X-ray range up to 20 keV. They are fabricated in stainless steel or aluminium providing excellent vacuum compatibility. A single additional flange integrates electrical and water cooling feedthroughs. Incoming photons are directly detected by the CCD sensor. No external controller is required to operate the detectors.
All our offered cameras combine scientific CCD sensors with ultra-low noise electronics for optimal detection of weak signals. Select among different spectral sensitivities and sensor technologies to find the best solution for your imaging or spectroscopic application. The full-frame in-vacuum CCD cameras are cooled by multi-stage Peltier elements. The cameras provide a rich set of functionalities including flexible binning operation, various trigger and synchronization modes, software switchable gain as well as temperature monitoring of the CCD sensor and the Peltier hot side.
Optical Spectroscopy Systems
五. Motion control
Linear Stages
5.1 XN Serie Linear Stages 5.2 XS Series Linear Stages
XN Serie Linear Stages
XS Series Linear Stages
六、Hexapods
1.Positioning Hexapods 2.Motion Hexapods
Positioning Hexapods
Discover our wide range of precision positioning hexapods for loads from a few grams to several tons and resolutions from 10 nm to a few tenths of a micron!
Motion Hexapods
We help you succeed in your dynamic motion projects, allowing you to test objects weighing from a few kg to several tons with up to 2m/s speed and 1g acceleration.
