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| 10.
Glan-Thompson Polarizing Prisms |
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Made from two calcite elements cemented
together in such way that their optical axes are both parallel
to the hypotenuse and to the entrance and exit faces.
When compared to other calcite polarizers they present the advantages
of maximum refractive index difference between ordinary and extraordinary
rays, thus allowing either a larger field angle or a smaller L/A
ratio, with uniform and symmetric polarization over all the field.
There is no lateral shift of the image for axial objects. Glan-Thompsons
present the best extinction coefficient of all polarizers (values
of 3x10-8 have been attained). Due to these advantages
they are the preferred polarizers for use with energy density
up to 1W/cm2, in optical systems such as monochromators,
low-power lasers, light sources and precision polarization instruments.
These prisms have their entrance and exit faces perpendicular
to the prism axis, thus simplifying mounting and alignment. The
figure shows the orientation of optical axes and polarized beam
in this prism. Glan-Thompsons are made with L/A ratios of 3:1
or 2.5:1, with apertures of 10x10, 15x15 and 20x20mm.
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| 11.
Glan-Taylor Polarizing Prisms |
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These
prisms differ from the Glan-Thomson in being air-spaced instead
of cemented and by having their two parts made with optical axes
perpendicular to the hypotenuse. As shown in the figure, the extraordinary,
linearly polarized beam is transmitted without deviation, while
the ordinary beam suffers total internal reflection at the calcite-air
interface, being deviated to a side face, where it is completely
absorbed. By being air-spaced, these prisms show higher ultraviolet
transmission than Glan-Thompsons, with a smaller field. However
their field is larger than other equivalent-sized air-spaced polarizers.
The cut between the two parts is made near the Brewster angle, further
improving transmission. Due to the larger cut angle it is a shorter
prism, allowing better calcite yield and consequent cost reduction.
They can be used with energy densities up to 5W/cm2 (CW)
and 10MW/cm2 (1ns pulses). Glan-Taylors are made with
L/A ratios of 3:1 or 2.5:1, with apertures of 10x10, 15x15 and 20x20mm.
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| 12.
Glan-Laser Polarizing Prisms |
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Glan-Laser polarizers are Glan-Taylor
prisms optimized to be used with medium to high energy lasers and
so are made from scatter-free calcite without any cosmetic defects.
As high energybeams reflected at the calcite-air interface will
heat the mounting medium, causing
degassing and possible damage of the crystal, it is necessary to
send these beams outside the prism, which is done by means of two
polished side faces, as shown in the drawing. The hypotenuse angle
is also optimized to minimize reflection losses and, in order to
prevent multiple reflections in Q-switch applications, the entrance
and exit faces may be made with a 3 angle relative to the prism
mechanical axis, on special request. These prisms may be employed
with laser beams of up to 100W/cm2 (CW) and 300MW/cm2
(pulsed-1ns) in applications such as feedback elimination, pulse
extraction and Q-switching. Glan-Laser prisms are made with apertures
of 10x10 or 20x20mm.
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