Fresnel Rhombs

Fresnel Rhombs

• Rotate polarization, operates over a wide wavelength range • λ/2 rhomb is two optically contacted λ/4 rhombs Due to unequal phase shifts arising in orthogonally polarized components of an incident wave at total… Read more →

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Order

SKU Cementing material or method Material Design Wavelength Range Retardation
481-1210 Optically contacted UVFS 210 nm - 400 nm L/2
3 in stock Ships in: 2–5 calendar days
$707

Specifications

Cementing material or method Optically contacted
Mounted False
Material Type FS
Material UVFS
Design Wavelength Range 210 nm - 400 nm
Retardation L/2

Surface 1

Surface quality, ISO 20-10
Power and Irregularity, fringes @633 nm 0(0.2)

Surface 1, Wavelength 1

Coating AR
Wavelength 210 nm - 400 nm
Reflectivity, % 0 % - 1.5 %
AOI (angle of incidence) 0 deg 0 min 0 sec - 0 deg 0 min 0 sec

Surface 2

Surface quality, ISO 20-10
Power and Irregularity, fringes @633 nm 0(0.2)

Surface 3

Surface quality, ISO 20-10
Power and Irregularity, fringes @633 nm 0(0.2)

Description

  • Rotate polarization, operates over a wide wavelength range
  • λ/2 rhomb is two optically contacted λ/4 rhombs

Due to unequal phase shifts arising in orthogonally polarized components of an incident wave at total internal reflection Fresnel Rhombs are used to alter polarisation type of radiation. They are designed so that two full internal reflections inside a rhomb provide π/2 phase difference between the orthogonally polarized components of radiation. Hence, if there is 45° angle between the polarization of the linearly polarized incident plane, the emerging beam is circularly polarized, i. e. the rhomb effect is similar to that of a quarter-waveplate. Therefore two identical Fresnel rhombs, installed in series, will provide π/2 phase difference similar to that of a half-waveplate, i. e. the device can rotate the beam polarization plane by 90°, leaving the beam direction invariable.