RP Photonics logo
RP Photonics
Technical consulting services on lasers, nonlinear optics, fiber optics etc.
Profit from the knowledge and experience of a top expert!
Powerful simulation and design software.
Make computer models in order to get a comprehensive understanding of your devices!
Success comes from understanding – be it in science or in industrial development.
The famous Encyclopedia of Laser Physics and Technology – available online for free!
The ideal place for finding suppliers for many photonics products.
Advertisers: Make sure to have your products displayed here!
… combined with a great Buyer's Guide!
VLib part of the

The Photonics Spotlight

Quantifying the Chirp of Ultrashort Pulses

Dr. Rüdiger Paschotta

Ref.: encyclopedia articles on chirp and ultrashort pulses

The chirp of an ultrashort pulse is a concept which is relatively easy to grasp. Nevertheless, rather surprising issues arise when one tries to quantify such chirp. It turns out that different definitions of chirp lead to quantities which can not simply be converted into each other. Furthermore, such quantities may not even agree on the question whether the magnitude of chirp increases or decreases in certain situations!

The article on chirp gives two examples, which are discussed in some more detail here:

Effect of Chromatic Dispersion

Consider a situation where an initially unchirped (transform-limited) pulse experiences normal dispersion when propagating in a medium. Of course, one would expect this to lead to an increasing amount of chirp. It obviously does so, when the magnitude of chirp is considered to be the amount of anomalous dispersion required to recompress the pulse.

However, this is not the case for the rate of change of the instantaneous frequency, which is actually a rather natural definition for the magnitude of chirp. That kind of chirp first rises with increasing amount of dispersion, but then it decreases again. Why is that? Because the instantaneous frequency goes through an interval of finite width, and as the pulse becomes longer and longer, the rate of change (in Hz/s) decreases.

Effect of Kerr Nonlinearity

Here we consider an initially unchirped pulse which is subject to self-phase modulation (SPM) via a Kerr nonlinearity of some medium. SPM creates a chirp, and the rate of change of the instantaneous frequency will increase with increasing propagation length. However, the amount of dispersion as required for maximum compression will initially increase, but then decrease. The reason for that is that the pulse bandwidth is increasing, and broadband pulses are more sensitive to dispersive effects.


The conclusion of this insight is clear: be careful when considering the magnitude of chirp, as different definitions have very different meanings, and can not even be considered to quantify the same physical property.

This article is a posting of the Photonics Spotlight, authored by Dr. Rüdiger Paschotta. You may link to this page, because its location is permanent. See also the Encyclopedia of Laser Physics and Technology.

Note that you can also receive the articles in the form of a newsletter or with an RSS feed.

If you like this article, share it with your friends and colleagues, e.g. via social media: