Photoelastic Modulators (PEMs)

Photoelastic modulators (PEMs) are key components in a diverse range of photonics applications. Hinds Instruments are the world leader based on the principles of polarisation modulation. Measuring the polarisation of light is enabled thanks to a wide range of photoelastic modulators developed for a variety of applications across a wide spectral region, UV to TeraHertz.

Hinds Instruments PEMs are made of isotropic optical materials and operate at a resonant frequency and are used across a variety of applications including chopping a light beam (20 – 84kHz), birefringence measurements, stokes polarimetry, optical rotation polarimetry, linear and circular dichroism in UV-Vis and IR, magnetic circular dichroism, FTIR double modulation spectroscopy (VCD, VLD, IRRAS), ellipsometry, fluorescence polarisation, and waveplate measurement.

Photoelastic Modulators (PEMs)

Range features

A high level overview of what this range offers

  • Wide range of products for different spectral regions, from vacuum UV to Terahertz
  • Aperture: up to 56mm
  • Nominal Frequency: several values available between 20kHz and 84kHz
  • Large acceptance angle
  • Polarisation purity and high-power handling capability – up to 5 GW/cm2 for some devices
  • Retardation: quarter-wave or half-wave
  • Assemblies: one PEM or dual PEM
  • Delay stability, renowned for stable, trouble-free performance
  • Options: anti-reflective coating, magnetic field compatible, vacuum compatible
  • Durability – (some PEMs are still in use from 1977)

Downloads

for Photoelastic Modulators (PEMs)

pdf
Hinds PEM technical overview
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What’s in this range?

All the variants in the range and a comparison of what they offer

ModelNominal frequencyQuarter wave retardation rangeHalf-wave retardation rangeUseful aperture

I/FS50

50kHz

170nm – 2µm

170nm – 1µm

16mm

I/FS20

20kHz

170nm – 2µm

170nm – 1µm

22mm

I/CF50

50kHz

130nm – 1µm

130nm – 500nm

16mm

II/FS20

20kHz

170nm – 2.6µm

170nm – 2.5µm

56mm

II/FS42

42kHz

170nm – 2.6µm

170nm – 2.5µm

27mm

II/FS47

47kHz

170nm – 2.6µm

170nm – 2.5µm

24mm

II/FS50

50kHz

170nm – 2.6µm

170nm – 2.5µm

22mm

II/FS84

84kHz

200nm – 2.5µm

200nm – 2.5µm

13mm

II/IS42

42kHz

300nm – 3.5µm

300nm – 3µm

27mm

II/IS84

84kHz

300nm – 3.5µm

300nm – 3µm

13mm

II/CF57

57kHz

2µm – 8.5µm

2µm – 5.5µm

23mm

II/ZS37

37kHz

2µm – 18µm

1µm – 9µm

19mm

II/ZS42

42kHz

2µm – 18µm

1µm – 10µm

17mm

II/ZS50

50kHz

2µm – 18µm

1µm – 10µm

14mm

II/SI40

40kHz

28µm – 57µm

36mm

II/SI50

50kHz

28µm – 57µm

29mm

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FAQs

for Photoelastic Modulators (PEMs)

A Photoelastic Modulator (PEM) is an optical device that modulates the polarisation of light to gain information about mechanical stresses in materials. This is achieved by using photoelastic material that changes its optical properties due to mechanical stress. The PEM by Hinds Instruments utilises this effect to provide precise information about the stress distribution in an examined object.

The basic operating principle of the PEM is based on the photoelastic effect. A mechanically stressed sample exhibits birefringence proportional to the strain caused by the induced stress. Therefore, the PEM can be considered a birefringence modulator. The optics’ resonance results in birefringence along an axis that is either compressed or stretched, causing the light to travel faster or slower along this axis. For instance, in quartz glass, the light moves faster along the horizontal component when compressed and slower along the horizontal axis (parallel to the modulation) when stretched.

PEMs have several unique features, including a broad spectral range, large aperture, wide acceptance angle, and precise phase modulation. They are typically used for fast and highly sensitive measurements. Unlike Pockels cells and electro-optical modulators, optical elements made of quartz glass are isotropic when no stress is applied. This gives the PEM an expanded acceptance angle.

Hinds produces over a dozen standard PEM models that collectively cover the range from 130 nm to 57 µm.

Integrating Hinds Instruments’ PEM into existing measurement systems is generally straightforward. The modulator can be incorporated into optical setups and works well with common light sources and detectors. Hinds Instruments often provides software and interfaces that facilitate seamless integration into various measurement systems. This ensures easy adaptation to the specific requirements of the users.