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Bulk Lasers

Definition: lasers based on bulk crystals as gain media

More general term: solid-state lasers

More specific terms: end-pumped lasers, side-pumped lasers, rod lasers, slab lasers, thin-disk lasers

German: Bulk-Laser

Category: article belongs to category laser devices and laser physics laser devices and laser physics


Cite the article using its DOI: https://doi.org/10.61835/0zh

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Q-switched bulk laser
Figure 1: Setup of a Q-switched bulk laser. The used bulk components used are two mirrors, a laser crystal, and the Q switch.

The term bulk laser refers to a solid-state laser with a bulk piece of doped crystal or glass as the gain medium – not something containing a waveguide. Apart from the laser crystal (or glass), the laser resonator contains some laser mirrors and possibly some other optical elements such as a polarizer, a birefringent tuner, a prism, a Q switch or a saturable absorber for mode locking.

The term bulk lasers is used to distinguish such lasers from waveguide lasers and in particular from fiber lasers (= lasers based on fiber optics). In most cases, the laser gain medium is doped either with rare earth ions or transition metal ions, but bulk lasers also include color center lasers.

bulk laser setup
Figure 2: Setup of a bulk laser, containing a diode-pumped laser head (box with blue label), a frequency doubler in a crystal oven and various other optical elements. Source: Cutting Edge Optronics.

Free-space Beam Propagation

As there is no waveguide structure, so that the beam propagates in free space between optical components, the beam radius in the gain medium is essentially determined not by the gain medium, but by the design of the laser resonator. That has important implications:

Air Spaces

The laser resonator of a bulk laser is in most cases formed with discrete laser mirrors placed around the crystal (or glass), with an air space in between. The use of air spaces between mirrors, crystal and possibly other elements also has important implications:

  • It allows the simple insertion of additional optical elements, such as a birefringent tuner or other kind of optical filter, a Q switch for nanosecond pulse generation, or a nonlinear crystal for intracavity frequency doubling.
  • By optimizing the length of such air gaps, in addition to selecting mirrors with certain curvature radii, one can tailor the mode properties of the resonator.
  • Optical elements, particularly laser mirrors, have to be precisely aligned, and that alignment may be lost e.g. due to thermal drifts or mechanical vibrations.
  • Dust particles or organic matter in the air may be deposited on laser mirrors and other components, particularly when high optical intensities and/or short wavelengths are involved. For long-term reliable operation, the laser housing may therefore have to be sealed.

In many cases, the mirrors and other optical components are attached to adjustable mounts, where two or three micrometer screws allow for precise angular adjustments. In many industrial lasers and certain mass-produced OEM laser modules, these adjustable mounts are replaced with fixed mounts, which can be more robust (also less sensitive to temperature drifts) and cost-effective. Optical components can be soldered to their mounts, leading to very stable setups.

It is also possible to use a laser crystal with a highly reflecting dielectric mirror coating on one side, which serves as a resonator end mirror. There are also monolithic solid-state lasers where the beam path is entirely inside the crystal.

Comparison with Other Laser Types

Tentatively, bulk lasers and amplifiers are preferable for devices operating with high peak power, whereas low-threshold and high-gain operation is more easily achieved with waveguide lasers and waveguide amplifiers. Also, bulk lasers are more flexible e.g. in laboratory setups, as it is comparatively easy to add or exchange optical elements, whereas waveguide-type lasers are possibly cheaper to manufacture.

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