RP Photonics logo
VL logo part of the
Virtual
Library

The Photonics Spotlight

Strength of Thermal Lensing Effects

It may seem quite trivial: if you are dealing with some lensing effect – e.g. with thermal lensing in a laser gain medium – you can quantify this with an effective focal length. The smaller that is, the stronger the lensing effect.

However, consider a Nd:YAG laser, where the laser rod has a certain focal length for a given pump power. It turns out that in a simplified situation, where the thermal lensing results only from the temperature dependence of the refractive index, the effective focal length depends only on the pump power density (more precisely on the dissipated power per unit of pumped area), but not on the total pump power. So you might expect that you could easily double the pump power together with the mode area, and lensing effects would not become stronger, right? If this were true, we would be dealing with a power-scalable laser architecture.

The caveat is that a larger cavity mode becomes more sensitive to lensing effects. In particular, the width of the stability zones of the laser cavity, quantified with respect to the inverse effective focal length, scales in inverse proportion to the mode area. So it becomes more and more delicate to operate the laser within such a stability zone, as the mode area is increased.

Apparently, the focal length is not sufficient to judge how strong a lensing effect really is. To understand this, consider the radially varying phase changes related to the lensing effect. There is a term proportional to the radius squared in the phase expression, with the coefficient being inversely related to the focal length. Now, the larger the laser beam, the stronger are the corresponding phase changes within the beam area.

In conclusion, in some situations it is more appropriate to quantify a lensing effect based on the maximum phase change within the mode area. May one test this e.g. in the context of a thin-disk laser, where the maximum phase change via thermal lensing depends only on the pump intensity (again with certain simplifying assumptions), so that in this case power scaling is indeed possible. This advice also applies to higher-order phase distortions, as are related e.g. to aberrations of the thermal lens: you can always remove the quadratic distortions by applying an appropriate correction lens, but the higher-order distortions remain.

This article is a posting of the Photonics Spotlight. You may send comments and suggestions to RP Photonics Consulting GmbH. You may also link to this page, because its location is permanent. See also the Encyclopedia of Laser Physics and Technology.

This encyclopedia is provided by
RP Photonics Consulting GmbH.

Utilize the expertise of the author, Dr. Rüdiger Paschotta, also in the form of technical consulting services!

Onefive logo

Onefive

Low-noise
femtosecond,
picosecond,
and tunable single-frequency lasers for OEM and R&D applications.

A.L.S. logo

A.L.S. GmbH

Picosecond laser diodes
<30 ps, 375 – 1600 nm, >1 Wp, single shot – 120 MHz

RP Fiber Power

This software helps to design and analyze fiber amplifiers and lasers.

RP Q-switch

A powerful software tool for designing
Q-switched lasers. See the details.

TRUMPF logo

TRUMPF-Laser

a leading supplier of industrial diode pumped solid state lasers,
CO2 lasers, and laser systems for material processing.

Field Guide to Lasers

This new book by Dr. Paschotta explains principles and types of lasers.

Your Advertisement at This Place

will be seen by many thousands of visitors per month. These banners receive far over 100'000 page hits per month. Check the details.