Nonlinear LBO Crystal

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.

Inquiry now
products Details
Item: Glan Thompson Polarizer 
Features:
Cemented
Wide Acceptance Angle Field
Suitable for Low Power Application

 

Material:

α-BBO,Calcite

Wavelength Range:

α-BBO:200-1100nm,Calcite:350-2300nm

Extinction Ratio:

α-BBO:<5×10-6,Calcite:<5×10-6

Surface Quality:

10月20日

Beam Deviation:

<3 arc minutes

Wavefornt Distortion:

λ/4@633nm

Damage Threshold:

>200MW/cm2

Coating:

Single Layer MgF2

Holder:

Black Anodized Aluminum

α-BBO Glan Thompson Polarizer

Par. No.

Wavelength Range(nm)

Extinction
Ratio

Angular
Field(°)

C.A.(φa)±0.1
(mm)

O.D.(φd)±0.1
(mm)

L±0.1
(mm)

PGM6006

200-2300nm
(Coating@1300nm)

<5×10-5

>15°

6.0

15.0

18.6

PGM6008

8.0

25.4

21.8

PGM6010

10.0

25.4

25.5

PGM6015

15.0

30.0

34.3

PGM6020

20.0

38.0

43.5

Calcite Glan Thompson Polarizer

Par. No.

Wavelength Range(nm)

Extinction
Ratio

Angular
Field(°)

C.A.(φa)±0.1
(mm)

O.D.(φd)±0.1
(mm)

L±0.1
(mm)

PGM7106

350-2300nm
(Coating@1300nm)

<5×10-6

14-16°

6.0

15.0

23.0

PGM7108

8.0

25.4

28.0

PGM7110

10.0

25.4

33.0

PGM7115

15.0

30.0

45.5

PGM7206

350-2300nm
(Coating@1300nm)

<5×10-6

25-28°

6.0

15.0

26.0

PGM7208

8.0

25.4

32.0

PGM7210

10.0

25.4

38.0

PGM7215

15.0

30.0

53.0

Order based on client requirement, including non-standard product and holder.



related Applications
Glan Taylor Polarizer alpha-BBO & Calcite material Glan Taylor Polarizer
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.
Read More
Glan Laser Polarizer For high power laser Glan Laser Polarizer
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.
Read More
Wollaston Polarizer High Performance Optical Wollaston Polarizer
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.
Read More
Rochon Polarizer Optical alpha-BBO & YVO4 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.
Read More
Waveplate Waveplate
Waveplate
Waveplates (retardation plates or phase shifters) are made from materials which exhibit birefringence. The velocities of the extraordinary and ordinary rays through the birefringent materials vary inversely with their refractive indices. The difference in velocities gives rise to a phase difference when the two beams recombine. In the case of an incident linearly polarized beam this is given by a=2pi*d(ne-no)/l (a-phase difference; d-thickness of waveplate; ne,no-refractive indices of extraordinary and ordinary rays respectively; l-wavelength). At any specific wavelength the phase difference is governed by the thickness of the retarder. Transmission range:330nm-2100nm Thermal Expansion Coefficient:7.5x10-6/K .Density:2.51g/cm3  Half Waveplate The thickness of a half waveplate is such that the phase difference is l/2-wavelength (true-zero order) or some multiple of l/2-wavelength (multiple order).  A linearly polarized beam incident on a half waveplate emerges as a linearly polarized beam but rotates such that its angle to the optical axis is twice that of the incident beam. Therefore, half waveplates can be used as continuously adjustable polarization rotators. Half waveplates are used in rotating the plane of polarization, electro-optic modulation and as a variable ratio beamsplitter when used in conjunction with a polarization cube. Quarter Waveplate The thickness of the quarter waveplate is such that the phase difference is l/4 wavelength (true-zero order) or some multiple of l/4 wavelength (multiple order). If the angle q (between the electric field vector of the incident linearly polarized beam and the retarder principal plane) of the quarter waveplate is 45, the emergent beam is circularly polarized. When a quarter waveplate is double passed, i.e. by mirror reflection, it acts as a half waveplate and rotates the plane of polarization to a certain angle. Quarter waveplates are used in creating circular polarization from linear or linear polarization from circular, ellipsometry, optical pumping, suppressing unwanted reflection and optical isolation. Optically Contacted Zero-Order Waveplate   • Optically Contacted • Thickness 1.5~2mm • Double Retardation Plates • Broad Spectral Bandwidth • Wide Temp. bandwidth Specifications: Material: Optical grade Crystal Quartz Dimension Tolerance: +0.0,-0.2mm Wavefront Distortion: <l/8@633nm Retardation Tolerance: <l/300 Surface Quality: 20/10 Scratch and Dig AR Coating: R<0.2% at center wavelength Standard wavelength: 532nm, 632.8nm, 800nm, 850nm, 980nm, 1064nm, 1310nm, 1550nm Cemented Zero-Order Waveplate Cemented by Epoxy Better Temperature Bandwidth Wide Wavelength Bandwidth AR Coated, R<0.2% Specifications: Material: Optical grade Crystal Quartz Dimension Tolerance: +0.0,-0.2mm Wavefront Distortion: <l/8@633nm Retardation Tolerance: <l/500 Surface Quality: 20/10 Scratch and Dig AR Coating: R<0.2% at center wavelength Standard wavelength: 266nm, 355nm, 532nm, 632.8nm, 800nm, 850nm, 980nm, 1064nm, 1310nm, 1550nm Air Spaced Zero-Order Waveplate Double Retardation Plates AR Coated,R<0.2% and Mounted High Damage Threshold Better Temperature Bandwidth Wide Wavelength Bandwidth Specifications: Material: Optical grade Crystal Quartz Dimension Tolerance: +0.0,-0.2mm Wavefront Distortion: <l/8@633nm Retardation Tolerance: <l/300 Surface Quality: 20/10 Scratch and Dig AR Coating: R<0.2% at center wavelength Standard wavelength: 266nm, 355nm, 532nm, 632.8nm, 800nm, 850nm, 980nm, 1064nm, 1310nm, 1550nm Single Plate Ture Zero-order Waveplate 1.Broad Spectral Bandwidth 2.Wide Temperature .Bandwidth 3.Wide Angle Bandwidth 4.High Damage Threshold Specifications: Material: Optical grade Crystal Quartz Dimension Tolerance: +0.0,-0.2mm Wavefront Distortion: <l/8@633nm Retardation Tolerance: <l/500 Surface Quality: 20/10 Scratch and Dig AR Coating: R<0.2% at center wavelength Standard wavelength: 1310nm, 1550nm   Cemented Ture Zero-Order Waveplate Cemented by Epoxy Wide Angle Acceptance Better Temperature Bandwidth Wide Wavelength Bandwidth   Specifications: Material: Optical grade Crystal Quartz Dimension Tolerance: +0.0,-0.2mm Wavefront Distortion: <l/8@633nm Retardation Tolerance: <l/500 Surface Quality: 20/10 Scratch and Dig AR Coating: R<0.2% at center wavelength Standard wavelength: 532nm, 632.8nm, 800nm, 850nm, 980nm, 1064nm, 1310nm, 1550nm Cemented Achromatic: Achromatic waveplate is similar to Zero-order waveplate except that the two plates are made from different materials, such as crystal quartz and magnesium fluoride. Since the dispersion of the birefringence can be different for the two materials, it is possible to specify the retardation values at a wavelength range. Material: Optical grade Crystal Quartz and MgF2 Dimension Tolerance: +0.0, -0.2mm Wavefront Distortion: < l/ 8@633nm Retardation Tolerance: <l/ 100 Surface Quality: 20/10 Scratch and Dig AR Coating: R<0.2% at center wavele...
Read More
Beamsplitter Beamsplitter
Beamsplitter
Beamsplitters are optical components used to split input light into two separate parts,mainly include cube polarization beamsplitter, plate polarization beamsplitter and cube non-polarization beamsplitter.
Read More
Plano Concave Lenses Expand lights Plano-Concave Lenses
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.
Read More
Penta Prisms Aluminum Coated Penta Prisms
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.
Read More
Nonlinear KTP crystal HGTR-KTP crystal
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.
Read More
Sapphire crystal Superior infrared material sapphire crystal
Superior infrared material sapphire crystal
Sapphire is a superior optical material possesses excellent optical, chemical and physical properties.
Read More
Electro-optical crystals KDP KDP Crystal
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.
Read More
SF10 Cylindrical Lenses Plano-convex Cylindrical Lenses
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.
Read More
Send a Message
If you have questions or suggestions,please leave us a message,we will reply you as soon as we can!
Get In Touch
  • Tel : +86-591-22857792
  • Email : sales@100optics.com
  • Add : 3th Floor, Building 1, No 39 Jinlin Road, Cangshan District, Fuzhou Fujian,P.R.China.
Leave Message welcome to Hundreds Optics
If you have questions or suggestions,please leave us a message,we will reply you as soon as we can!

Home

Products

News

contact