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Nonlinear optical Phase matching Frequency doubling SHG THG FHG SPDC β-BaB2O4 BBO Crystal

BBO is a nonlinear optical crystal with combination of number of unique features. Wide transparency and phase matching ranges, large nonlinear coefficient, high damage threshold and excellent optical homogeneity provide attractive possibilities for various nonlinear optical applications.

Nonlinear laser frequency doubling second third harmonic generation lithium triborate SHG THG LBO Crystal

LBO (Lithium triborate or LiB3O5) is a very useful nonlinear optical crystal material, especially for SHG THG of high-intensity laser radiation, intracavity SHG THG, deep-UV SFG and OPO applications.

HGTR-KTP crystal

Nonlinear KTP crystal named Potassium Titanyl Phosphate (KTiOPO4 or KTP) is widely used in both commercial and military lasers including laboratory and medical systems, range-finders, lidar, optical communication and industrial systems.

KDP Crystal

Crystals of KDP (KH2PO4), DKDP or D*KDP (KD2PO4) and ADP (NH4H2PO4) are grown by a water-solution method and can be grown up to very large size. Therefore, they are as low-cost and large-size finished non-linear components available.

Optical nonlinear frequency doubling LiNbO3 crystal

LiNbO3 crystals are the most commonly used material for pockel cells, Q-switches and phase modulators, waveguide substrates, surface acoustic wave (SAW) wafers, etc.

YCOB Crystal （YCa4O(BO3)3 ）

YCa4O (BO3) 3 (YCOB) crystal has superior nonlinear optical properties, high temperature piezoelectric properties and good chemical stability

Nd:YVO4 crystal

Yttrium Vanadate (Nd:YVO4) is one of the most efficient laser host crystal currently existing for diode laser-pumped solid-state lasers.

Nd:YAG crystal

Nd:YAG (neodymium-doped yttrium aluminium garnet; Nd:Y3Al5O12) is a crystal that is used as a lasing medium for solid-state lasers. The dopant, triply ionized neodymium, typically replaces yttrium in the crystal structure of the yttrium aluminium garnet (YAG), since they are of similar size. Generally the crystalline host is doped with around 1% neodymium by atomic percent. Applications: Nd:YAG absorbs mostly in the bands between 730–760 nm and 790–820 nm.At low current densities krypton flashlamps have higher output in those bands than do the more common xenon lamps, which produce more light at around 900 nm. The former are therefore more efficient for pumping Nd:YAG lasers.

For passively Q-switching diode pumped Cr4:YAG Crystal

Passive Q-switching is preferred for simplicity of manufacture and operation, low cost and reduced system size and weight. Cr4+:YAG is an excellent crystal for passively Q-switching diode pumped or lamp-pumped Nd:YAG, Nd:YLF, Yb:YAG or other Nd and Yb doped lasers at wavelength from 1.0 to 1.2um.

promising laser-active materials Yb:YAG crystal

Yb:YAG is one of the most promising laser-active materials and more suitable for diode-pumping than the traditional Nd-doped systems. Compared with the company used Nd:YAG crystal, Yb:YAG crystal has a much larger absorption bandwidth to reduce thermal management requirements for diode lasers, a longer upper-laser level lifetime, three to four times lower thermal loading per unit pump power.

For magneto-optical isolator Terbium Gallium Garnet TGG Crystal

TGG is an excellent magneto-optical crystal used in various Faraday devices(Polarizer and Isolator) in the range of 400nm-1100nm, excluding 475-500nm.

Customized Photonics BK7 Windows

This kind of BK7 Windows is made from SCHOTT N-BK7 Glass, which has transparent range from 330-2100nm.

Customized Photonics Fused Silica Windows

Fused Silica Window is made from the material of fused silica. Fused Silica is a superior optical material possesses excellent optical, chemical and physical properties which is formed by chemical combination of silicon and oxygen.

Custom-made material CaF2 Windows

This kind of windows is made from Custom-made material CaF2.

alpha-BBO & Calcite material Glan Taylor Polarizer

Glan Taylor Polarizer is made of two same birefringence material prisms which are separated by an air space. The polarizer with on side escape window is suitable for low to medium power application. Glan Taylor Polarizer will divide an entering unpolarized beam into beam rays, one is the extraordinary that is transmitted through the other side, and another is the ordinary ray that is totally internally reflected absorbed.

For high power laser Glan Laser Polarizer

Glan Laser Polarizer is designed specifically for high energy laser. It is made of two same birefringence material prisms that are assembled with an air space. The polarizer with two escape windows allows the rejected beam to escape out of the polarizer which makes it suitable for high power laser.

alpha-BBO & Calcite Glan Thompson Polarizer

Glan Thompson Polarizer is made of two α-BBO or calcite prisms cemented together. It has a wavelength from 200nm to 2300nm. α-BBO polarizer can be used from about 200nm to 1100nm, and calcite polarizer can be used from 350nm to 2300nm. This type polarizer has higher extinction ratio than air spaced polarizer. And it has the widest field angle of any design. For example, α-BBO Glan Thompson Polarizer has an angular field lager than 15 degree.

High Performance Optical Wollaston Polarizer

Wollaston Polarizer is made of birefringence material prisms that are cemented together. The ordinary ray in the first half of the prism becomes the extraordinary ray in the second half. The Wollaston Polarizing beam splitter has approximately twice the deviation for the Rochon Polarizer.

Optical alpha-BBO & YVO4 Rochon Polarizer

Rochon Polarizer is the earliest polarizer, which is made of two birefringence material prisms that are cemented together. This type polarizer separates incident beam into ordinary ray and extra-ordinary ray like Wollaston Polarizer, but the extra-ordinary ray is straight transmitted through, while ordinary is transmitted with a deviation angle.

Right Angle Prism as a mirror and a retroreflector

Right Angle Prism is used as a mirror to deviate light through 90 degree, and also as a retroreflector to deflect light through 180 degree by total internal reflection.

Aluminum Coated Penta Prisms

Penta Prism is a five-sided prism containing two reflecting surfaces at 45° to each other, and two refracting faces perpendicular to the entering and emerging beams. The standard Penta Prism reflecting surfaces are coated with aluminum or enhanced aluminum.

Retroreflector Optics Corner Cube

Corner Cube Retroreflector has three mutually perpendicular surfaces and a hypotenuse face.

Plano-concave Cylindrical Lenses

Cylindrical lenses are mainly used to change the size of imaging per design requirements. Plano concave cylindrical lenses are mostly used in laser scanners, spectroscopy, dye lasers, acousto-optics, optical processors and other optical applications.

Plano-convex Cylindrical Lenses

Cylindrical lenses are mainly used to change the size of imaging per design requirements. Plano convex cylindrical lenses are used to focus light to a thin line in the applications like laser scanners, spectroscopy, dye lasers, acousto-optics, optical processors and etc.

Plano-Convex Lenses for optical systems

Plano-convex Lenses present a curvecd interface and a planar interface. Thay are for instance the microlenses situated on top of a wafer, and also encountered in macroscopic optical systems.

Expand lights Plano-Concave Lenses

Plano-concave Lenses have one concave surface. It has negative focal length. It is often used to expand light or to increase focal length in existing systems.

Positive Focal Length Double-Convex Lenses

Double-convex Lenses are manufactured with an identical convex surface on both sides of the lens. This kind of lenses has positive focal length and form both real and vitrual images.

For diverging light Double-Concave Lenses

Double concave lens is the most common form of Negative lens. Negative lens is most suited to producing diverging light or a virtual image, where the input light is converging.

High Precision Positive-Meniscus Lenses

Positive meniscus lenses may be used to increase the numerical aperture of apositive lens assembly, without an undue increase in the aberrations.

Achromatic Negative-Meniscus Lenses

Negative meniscus lens is a convex-concave lens and is with thinner at the center than at the edges.

Infrared reflectors and windows' material 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.

For high performance infrared imaging systems Germanium(Ge)

Germanium (Ge) is the preferred lens and window material for high performance infrared imaging systems in the 8–12 μm wavelength bands.

Infrared optics CVD ZnS windows for full band of 0.4-12μm

ZnS is grown by chemical vapor deposition (CVD) method, for windows,domes and lenses for thermal-imaging system.

Infrared applications ZnSe for IR lasers

ZnSe (Zinc Selenide) is the most popular material for infrared applications. It can transmit from 0.6 μm to 20 μm.

Superior infrared material sapphire crystal

Sapphire is a superior optical material possesses excellent optical, chemical and physical properties.

High Reflection Mirror for scientific apparatus

High reflection mirror is an object with a surface that has high reflection. It is smooth enough to form an image.

High Performance Fused Silica Multi-Coated Filter

Multi-Coated Filter is made of optical materials such as Bk7, Fused Silica, Colored Glass, Sapphire and so on. Hundreds Optics offers Multi-Coated Filters include bandpass filters, dichroic filters, short-pass filters and long-pass filters.

Colored Glass Filter for your customization

Colored Glass Filter is widely used in the field of display, CCD, microscopy, photometry, radiometry, imaging, astronomy, instrumentation, aerospace etc. We can supply a variety of different Schott, Hoya, and Chinese colored glasses covering the UV, visible, and near-infrared wavelength regions.

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