GLAN THOMPSON BEAM SPLITTING

The Beam Splitting Glan Thompson polarizer is made of two cemented prisms of calcite. It is a modification of the Glan Thompson polarizer in the sense that the totally reflected ordinary polarization is made to exit the polarizer. For an input beam at normal incidence, the two orthogonally polarized output beams exit at normal incidence to their respective output faces. Therefore, the beam separation angle of 37 degrees and 45 degrees in the two available versions is independent of wavelength. Their length to aperture ratio is 3.0:1 and 2.5:1, respectively. There is a slight mismatch of the refractive index of straight through the extraordinary beam and the cement. Due to this, some extraordinary polarization is reflected, which results in an unequal extinction ratio of the two output beams. These polarizers can be used from 350 nm to 2300 nm. The table shown lists A-grade polarizers. Polarizers made of B or S-grade of calcite are also available upon request.

A drawing of a piece of metal with a hole in it.
A graph of the polarization field of msbt-4 5.
A graph of the polarization field of msbt-3 7

Specifications:

B grade calcite: greater than one wave wavefront deformation @ 633 nm due to striae only

A grade calcite: quarter to one wave wavefront deformation @ 633 nm due to striae only

S grade calcite: quarter wave wavefront deformation @ 633 nm due to striae only

Surface flatness: at least quarter wave @ 633 nm over the clear aperture

Surface quality: 40-20 scratch dig

Transmission (uncoated): 35-40% at 350 nm, 65-70% at 400 nm, 80-88% at > 500 nm
please visit Anti Reflection Coating page for reflectivity plots of available coatings

Calcite is a natural mined crystal. Defects in bulk calcite are characterized by bubbles (presence of randomly scattered bubbles vary from relatively large to small sizes and fine bubble lines), striae (streaks of sudden variation of refractive index which can be detected interferometrically), optical inhomogeneity (gradual variation of refractive index in bulk material) and stress birefringence (variation of birefringence in bulk material due to defective growth of the crystal). These defects cause degradation of polarization and transmission loss due to scattering and absorption.

BEAM SPLITTING GLAN THOMPSON

Catalog Number

Clear Aperture

Diameter (mm)

Mount Dimensions

(Inches)

Remarks

Height

Maximum

Width

+/- .0025

Length

+/- .005

MSBTB- 8-45 8 .875 .622 1.125

Grade B

Extinction - Reflected Beam 1*10^-4

Extinction - Straight Through Beam 5*10^-5

MSBTB-10-45 10 1.000 .872 1.375
MSBTB-12-45 12 1.125 .996 1.500
MSBTA- 8-45 8 .875 .622 1.125

Grade A

Extinction - Reflected Beam 5*10^-5

Extinction - Straight Through Beam 1*10^-5

MSBTA-10-45 10 1.000 .872 1.375
MSBTA-12-45 12 1.125 .996 1.500
MSBTS- 8-45 8 .875 .622 1.125

Grade S

Extinction - Reflected Beam 1*10^-5

Extinction - Straight Through Beam 5*10^-6

MSBTS-10-45 10 1.000 .872 1.375
MSBTS-12-45 12 1.125 .996 1.500
MSBTB- 8-37 8 .875 .622 1.500

Grade B

Extinction - Reflected Beam 1*10^-4

Extinction - Straight Through Beam 5*10^-5

MSBTB-10-37 10 1.000 .872 1.625
MSBTB-12-37 12 1.125 .996 1.875
MSBTA- 8-37 8 .875 .622 1.500

Grade A

Extinction - Reflected Beam 5*10^-5

Extinction - Straight Through Beam 1*10^-5

MSBTA-10-37 10 1.000 .872 1.625
MSBTS-12-37 12 1.125 .996 1.875
MSBTS- 8-37 8 .875 .622 1.500

Grade S

Extinction - Reflected Beam 1*10^-5

Extinction - Straight Through Beam 5*10^-6

MSBTS-10-37 10 1.000 .872 1.625
MSBTS-12-37 12 1.125 .996 1.875