Polarising beamsplitters and extinction ratio

A polarising beamsplitter cube transmits one linear polarisation and reflects the other. Extinction ratio describes how cleanly it does so, and it is almost always much better in transmission than in reflection. Combine one with a half-wave plate and you have a continuously variable power splitter.

Laser opticsExcelitas / LINOS
THE SHORT ANSWER

A polarising beamsplitter cube transmits one linear polarisation and reflects the other. Extinction ratio describes how cleanly it does so, and it is almost always much better in transmission than in reflection. Combine one with a half-wave plate and you have a continuously variable power splitter.

Typical extinction ratio Above 1000:1 in transmission
Transmission Up to 99,9 %
Cube edge 10 to 25,4 mm
Damage threshold 1,5 to 10 J/cm2, per specification
Coating band Designed, per wavelength
Reflected port purity Substantially lower than transmitted

A polarising beamsplitter separates a beam by polarisation state rather than by intensity. Inside the cube, a dielectric coating on the diagonal transmits p-polarised light and reflects s-polarised light.

Reading the extinction ratio

Extinction ratio is the intensity ratio of wanted to unwanted polarisation in a given port. The number quoted on the datasheet, commonly better than 1000:1, is nearly always the transmitted port. The reflected port is typically an order of magnitude worse, because the coating reflects some of the unwanted state as well.

The practical rule follows immediately: if you need a clean polarisation state, take it from the transmitted port and treat the reflected port as a dump or a monitor.

The variable attenuator

Put a half-wave plate in front of the cube. Rotating the plate rotates the incoming polarisation, which changes how the power divides between the two ports. You get a continuously variable, essentially lossless power split with no absorbing elements in the beam, which is why this pair appears in almost every laser laboratory.

Power handling

The cement layer is the limit. For nanosecond pulses at 1064 nm the damage threshold is a real constraint and worth checking against your pulse energy and beam diameter rather than your average power. Where the energy density is too high, a plate polariser removes the cement from the problem.

When to use it

  • Splitting a laser beam with an adjustable ratio, using a wave plate ahead of it
  • Cleaning up the polarisation of a source before a polarisation-sensitive instrument
  • Combining two orthogonally polarised beams into one path
  • Building an optical isolator alongside a Faraday rotator

What to watch out for

  • The reflected beam is far less pure than the transmitted one: take your clean beam out of the transmitted port
  • Cube cement limits damage threshold; for high pulse energy consider a plate polariser instead
  • Extinction is specified at the design wavelength and degrades away from it
  • Cubes introduce a substantial glass path, so account for the optical path length in interferometric work

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