Laser Beam Characterization

For the measurement of the optical power of a laser beam, there are various types of power meters, which may be based on photodiodes or on some kind of thermal detector. For permanent monitoring, there are optical power monitors.

A full characterization of a monochromatic laser beam could in principle lead to the complete complex amplitude profile in one plane perpendicular to the beam, from which the further evolution (propagation) of the beam could be calculated with a suitable beam propagation software, for example. Such a characterization can be done with a Shack–Hartmann wavefront sensor, for example. Although this measures field amplitudes and wavefront directions only on some grid of spots, the amplitudes at intermediate points can be interpolated, if the spatial resolution is good enough. Alternative measurement methods may be based on interferometry, for example.

For non-monochromatic laser beams, one often assumes that the amplitude pattern is not frequency-dependent. That assumption may be completely wrong, however; for example, different resonator modes of a solid-state laser generally have different optical frequencies, so that different frequency components of the generated beam can have entirely different beam profiles. For lasers with operation on a single transverse mode, however, the mentioned assumption can be fairly accurately fulfilled.

There are also various kinds of beam profilers which measure only the intensity distribution, but not the optical phase. They can be based on cameras, for example. A comprehensive assessment of beam quality (quantified e.g. with the beam parameter product or the M² factor) is nevertheless possible, if such intensity profiles are taken at different positions along the laser beam.

Some laser beams exhibit “hot spots”, i.e., regions with higher intensity, which may play role in damage phenomena. There can also be satellite structures, halos and other deviations from beam uniformity. Note that the shape of the beam intensity profile may change during propagation, and is also not always stable over time.

Some devices do not measure the whole beam profile, but only a beam radius or diameter. Note that the beam radius is usually not defined as a half width at half maximum (HWHM) value, but as the radial position where the intensity falls to 1/e² times the peak intensity. This comes from the context of Gaussian beams.

A laser beam may exhibit beam pointing fluctuations, which can be measured by monitoring the position (center of gravity of the intensity distribution) at a suitable location.

The polarization state may be roughly characterized based on the power transmission of a polarizer for different orientations, or more completely with various techniques for polarimetry.

For pulsed lasers, measurements of the pulse energy, pulse duration and peak power are often required. In case of Q-switched lasers, optical energy meters and fast photodiodes can be suitable. For mode-locked lasers, generating much shorter pulses, one uses instruments like autocorrelators all those for more advanced methods like FROG and SPIDER.

The optical spectrum of a laser beam can be measured with some kind of spectrograph or another kind of spectrometer.

For various methods of laser beam characterization, for example with cameras, it is necessary to more or less attenuate a laser beam without e.g. affecting its beam profile. Straight-forward approaches like using some absorbing neutral density filters often do not work at high power levels. Therefore, advanced types of optical attenuators may be needed.

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