Mode Cleaners

Figure 1 shows the simple setup, which can be understood relatively easily on the basis of Fourier optics. The (somewhat “spoiled”) beam coming from the left-hand side is focused to a small spot with a lens. In the focal plane, different spatial Fourier components of the original beam are to some extent spatially separated: each spatial Fourier component corresponds to a plane wave with a certain propagation direction, and a component which e.g. propagates slightly upwards will have its focus at a higher position. Therefore, the pinhole in the focal plane can effectively attenuate spatial components related to off-axis components. The second lens recollimates the beam, and the resulting beam has a “cleaned” intensity and phase profile. Of course, the cleanup cannot be perfect, since each spatial component is focused to a spot with finite size. Note that simply focusing more strongly will not necessarily help, since this also reduces the spatial separation of spatial Fourier components in the focal plane. However, a certain degree of focusing is required; a rule of thumb is that the waist size must be a few times smaller than the original beam size. Further, the diameter of the pinhole must of course be appropriate; too small a hole, for example, leads not only to excessive power loss but also to a deterioration of the beam quality.

The beam cleanup can work very well when an originally close to Gaussian beam (with high beam quality) has acquired some spatially “fast” distortions e.g. by reflection on some mirrors with deposited dust particles. Such a beam is very effectively cleaned up without losing a significant amount of the optical power. (Note that one then has a coherent superposition of the Gaussian mode with fairly high-order modes, which can strongly affect the beam quality without carrying significant optical powers.) On the other hand, the method does not work very well on a really spatially multimode beam from a laser with poor beam quality. It is not only that removing the higher-order modes is then really associated with a significant power loss, but also that the separation of modes with similar orders is not perfect.

A practical problem for application with high-power lasers and particularly with Q-switched lasers is that the optical intensities at the pinhole can become fairly large, possibly leading to optical damage.

In comparison with mode cleaner cavities, nonresonant mode cleaners are relatively easy to align and can work with polychromatic radiation, but cannot reach the same amount of beam quality improvement for clearly multimode beams.

Another way to clean up a laser beam is to send the light through a single-mode fiber. If the fiber is sufficiently long to strip off light in the cladding modes (a few centimeters may be sufficient, depending on the cladding), the output will have the nearly Gaussian profile of the fiber mode. Any beam distortions can be removed in this way, at the price of power losses at the fiber's input end. (This is similar to the losses at the above described pinhole apparatus, even though the physical working principles of the devices are different.) A problem may be that the polarization state can be scrambled, unless the fiber is short or a polarization-maintaining fiber is used.

Your question or comment:

Spam check:

  (Please enter the sum of thirteen and three in the form of digits!)

By submitting the information, you give your consent to the potential publication of your inputs on our website according to our rules. (If you later retract your consent, we will delete those inputs.) As your inputs are first reviewed by the author, they may be published with some delay.