In-line Faraday Rotator, ILF 1310nm, 1440nm, 1550nm

Center wavelength: 2000 nm Operating bandwidth: ±30 nm Insertion loss [Option2/Option3: Insertion Loss +3.0dB when launching circular polarized light; each connector added: IL +0.3dB; default connector key aligned to slow axis]: ≤1.0 dB

The 2000nm In-line Polarizer is a Micro Optics device can be used to convert un-polarized light into polarized light with high extinction ratio. It can also be used to enhance the extinction ratio of signals. The In-line polarizer offers low insertion loss, high extinction ratio, high return loss and excellent environmental stability and reliability. It is ideal for high speed communication systems and test instrumentation applications.

Dimension Tolerance: ±0.2mm Flatness [@ 632.8nm]: λ/6 @ 632.8nm Surface Quality: 60/40

PBS cube split randomly polarized beams into two orthogonal,linearly,polarized beams. S-polarized light is reflected at 90deg angle while P-polarized light is transmitted. Each PBS cube consists of a pair of high precision tolerance right angle prisms which cemented together with a dielectric coating on the hypotenuse of one of the prisms.

wavelength: 450nm wavelength: 520nm wavelength: 638nm

Extinction ratio [High-Contrast Glass Linear Pol]: 10000:1 Extinction ratio [Visible Polarizer]: 100:1 Extinction ratio [Visible-NIR Band Polarizer]: 4300:1

Fuzhou Jingzhi offers a full range of polarizing optics, including glass linear polarizers, plastic linear polarizers, metal wire-grid polarizers, near-infrared polarizers and high-damage-threshold nanoparticle polarizers. Operating bands span ultraviolet, visible, near-infrared and mid/far-infrared wavelengths over 250–5000 nm.

Material: H-ZF3 Glass 、 Fused silica Dimensions: 8*8*8 10*10*10mm 12.7*12.7*12.7mm 25.4*25.4*25.4mm 38.1*38.1*38.1mm 50.8*50.8*50.8mm 100*100*100mm Dimensional tolerance 。: +0.00/-0.2

The polarizing prism splits incident unpolarized light into two orthogonal components. P-polarized light is fully transmitted, while S-polarized light is reflected at 45° and exits at 90° to the P beam. It consists of two high-precision right-angle prisms, with a polarizing dielectric coating on one hypotenuse.