wavelengths
 

Dispersive coatings

The phase velocity of a light wave travelling through optical materials depends on the wa­velength. This phenomenon is called chroma­tic dispersion.

As a critical requirement for the generation of ultrashort pulses (e.g. in femtosecond lasers) and for controlling the pulse shape, dispersive dielectric optics are needed to compensate the group-­delay dispersion (GDD) which is introdu­ced by other components such as the laser crystal.

The GDD is defined as the derivative of the group delay with respect to the angular frequency, or the second-order derivative of the phase.

Of course all dispersive elements inside the  re­­­sonator have to be taken into account for ­op­­timizing the total GDD (see also the Group Velocity Dispersion of standard substra­tes). Otherwise the different delays of various frequency components within a short pulse result in
–     pulse broadening
–     generation of satellites in the time-domain and
–     loss of peak power.

Mirrors may have either low (i.e. close to zero) GDD or a tailored non-zero GDD. As shown in the following sections, there are different types of coating designs. LASEROPTIK offers:

•    mirrors with low or optimized GDD
•    highly dispersive narrow bandwidth mirrors, so-called GTI mirrors
•    chirped mirrors and matched pairs
•    octave-spanning broadband chirped mirrors with moderate GDD
•    partial reflectors
•    coatings used with an OPO

For example, these coatings compensate the dispersion introduced by other components like the laser crystal in a laser cavity. Or they serve as compressors in chirped pulse amplification systems (CPA).

In general, various spectral requirements can be combined with a GDD value as target for coating design and production, e.g. for OPO optics or partial reflectors. The dispersion management is highly depen­ding on the coating design and a sub-nanometer manufacturing accuracy for GDD optimized optics. At LASEROPTIK, this precision is ensu­red by the sophisticated method of Ion Beam Sputtering (IBS).

With the help of an optical in-situ process control based on the calculated design, the deposition of complex, custom tailored stacks of many (n > 70) non­­­quar­terwave layers is performed. The results are verified ex-situ by in-house GDD measurements and are used for reengineering of the coating design.

LASEROPTIK uses both custom-built and commercial GDD measurement setups ranging from 350 nm to 2400 nm (see measuring methods), whereas dispersive mirrors can be produced up to 4 µm, optimized and characterized for GDD by retrograde analysis of the coating thickness data.

Frequently asked questions

Can LASEROPTIK offer optics and dispersive coatings for ultrashort pulses?

As a critical requirement for the generation of ultrashort pulses (e.g. in femtosecond lasers) and for controlling the pulse shape, dispersive dielectric optics are needed.

LASEROPTIK offers a wide range of dispersive coatings with optimized group delay dispersion (GDD), such as low GDD mirrors, GTI mirrors, chirped mirrors and matched pairs.

For an overview see chapter https://www.laseroptik.com/en/coatings/dispersive-coatings

How can I compensate for the dispersion introduced by other components like the laser crystal in a laser cavity?

With the high accuracy of the IBS coating technique, LASEROPTIK produces GTI mirrors which are optimized for the GDD but also compensate for the dispersion of other optics within the beam path. GDD targets can be set precisely for every material and specific thickness. 

What is the difference between ultrafast and ultrashort laser? Do I need different optics?

There is no difference between ultrafast and ultrashort lasers or optics; both mean the same.

You have short pulses (ps/fs) with high peak power and need dispersive coatings to prevent pulse broadening, such as chirped mirrors or low dispersion mirrors.

https://www.laseroptik.com/en/coatings/dispersive-coatings