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Chirped Mirrors

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10 suppliers for chirped mirrors are listed.

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Altechna UAB

Femtosolutions broadband dispersion-compensated and highly dispersive mirrors for ultrafast laser applications

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Ask RP Photonics for working out designs of chirped mirrors to meet special dispersion profiles while avoiding too tight fabrication tolerances. RP Photonics has the powerful RP Coating software for designing optimized chirped mirrors.

Definition: Bragg-type dispersive mirrors with a spatial variation of the Bragg wavelength

German: gechirpte Spiegel

A chirped mirror is a kind of dielectric mirror which is usually used for dispersion compensation in mode-locked lasers. Another interesting feature of chirped mirrors is that they make it possible to achieve a broader reflection bandwidth than ordinary Bragg mirrors.

Principles of Dispersive Chirped Mirrors

The basic idea of chirped mirror designs [1] is that the Bragg wavelength is not constant but varies within the structure, so that light at different wavelengths penetrates to a different extent into the mirror structure and thus experiences a different group delay.

However, a naïve design directly based on this idea would not work: it would exhibit strong oscillations of the group delay and even more so of the group delay dispersion. This disturbing effect can to some extent be mitigated by numerical optimization of the layer structure, but this is difficult because the optimization has to be done in a multi-dimensional space (resulting from the large number of layers) where a huge number of local optima exist, most of which do not correspond to satisfactory designs.

double-chirped mirror

Figure 1: Operation principle of a chirped mirror. Light with a long wavelength penetrates deeper into the mirror structure and thus experiences a larger group delay. This leads to anomalous chromatic dispersion.

Later, it was found [5] that the disturbing oscillations have two origins:

Both problems can be eliminated with a double-chirped design, which has two additional features:

Even without numerical optimization, double-chirped designs can have a dispersion profile which relatively nicely matches the design goal. Further refinement is then achieved with numerical optimization, i.e., with fine tuning of the layer thickness values.

numerically optimized dispersive chirped mirror

Figure 2: Reflection and dispersion properties of a numerically optimized chirped mirror design, developed with the software RP Coating. The dashed curve shows the target dispersion, which is fairly precisely matched in a broad wavelength range. Even broader wavelength ranges are possible, when a larger number of layers is used.

field penetration into dispersive mirror

Figure 3: Field penetration into the chirped mirror of Figure 2. It is apparent that within the wavelength range 1000–1200 nm, the field penetrates more deeply into the structure for longer wavelengths. The larger group delay for longer wavelengths corresponds to anomalous dispersion.

Application in Mode-locked Lasers

For mode-locked lasers with an ultrabroad bandwidth, as required for operation in the few-cycle regime, it is challenging to design mirrors with the corresponding ultrabroad reflection bandwidth, combined with proper chromatic dispersion over the most of that range. The factor limiting the bandwidth achievable is in most cases the difficulty of making anti-reflection structures with very small residual reflectivity over a large bandwidth. This problem can be solved with so-called backside coated (BASIC) chirped mirrors [11]. The key idea of such a design is to interface the chirped mirror structure with a glass substrate rather than with air; the air–glass interface is then at a different location, and the effects of the residual reflectivity of that (also AR-coated) surface can be eliminated by using a wedge shape for that glass piece.

Double-chirped mirrors (DCMs) are often used for dispersion compensation in mode-locked lasers, particularly for those with pulse durations below ≈ 20 fs. They are typically designed not only to compensate a constant group delay dispersion, but also to correct higher-order dispersion. However, there are limits concerning how much dispersion (and in particular higher-order dispersion) can be compensated with a double-chirped mirror. Possible solutions are to use a suitable combination of several mirrors, where the dispersion errors from different mirrors partially cancel each other, and to combine chirped mirrors with a prism pair. Another challenge arises from the tight fabrication tolerances; at least some of the layers typically have to be fabricated with a precision of the thickness of a few nanometers. The remaining wiggles in the group delay versus wavelength can be further reduced by using appropriate combinations of mirrors where the wiggles at least partially cancel each other.

Chirped Semiconductor Mirrors

It has been shown [10] that double-chirped mirror designs can also be used with semiconductor mirrors. Such mirrors can generate a much higher amount of dispersion, although in a much smaller bandwidth. They can be used for compensating the dispersion in a mode-locked laser with a single compact device even when e.g. a long pulse duration requires a high amount of anomalous dispersion for soliton mode locking.

Bibliography

[1]R. Szipöcs et al., “Chirped multilayer coatings for broad-band dispersion control in femtosecond lasers”, Opt. Lett. 19 (3), 201 (1994)
[2]A. Stingl et al., “Sub-10-fs mirror-dispersion-controlled Ti:sapphire laser”, Opt. Lett. 20 (6), 602 (1995)
[3]R. Szipöcs and A. Koházi-Kis, “Theory and design of chirped dielectric mirrors”, Appl. Phys. B 65, 115 (1997)
[4]E. J. Mayer et al., “Ultrabroadband chirped mirrors for femtosecond lasers”, Opt. Lett. 22 (8), 528 (1997)
[5]F. X. Kärtner et al., “Design and fabrication of double-chirped mirrors”, Opt. Lett. 22 (11), 831 (1997)
[6]N. Matuschek et al., “Theory of double-chirped mirrors”, IEEE J. Quantum Electron. 33 (2), 295 ()
[7]G. Tempea et al., “Dispersion control over 150 THz with chirped dielectric mirrors”, IEEE J. Sel. Top. Quantum Electron. 4 (2), 193 (1998)
[8]N. Matuschek et al., “Theory of double-chirped mirrors”, IEEE J. Sel. Top. Quantum Electron. 4, 197 (1998)
[9]N. Matuschek et al., “Analytical design of double-chirped mirrors with custom-tailored dispersion characteristics”, IEEE J. Quantum Electron. 35 (2), 129 (1999)
[10]R. Paschotta et al., “Double-chirped semiconductor mirror for dispersion compensation in femtosecond lasers”, Appl. Phys. Lett. 75 (15), 2166 (1999)
[11]N. Matuschek et al., “Back-side-coated chirped mirrors with ultra-smooth broadband dispersion characteristics”, Appl. Phys. B 71, 509 (2000)
[12]F. X. Kärtner et al., “Ultrabroadband double-chirped mirror pairs for generation of octave spectra”, J. Opt. Soc. Am. B 18 (6), 882 (2001)
[13]G. Tempea et al., “Tilted-front-interface chirped mirrors”, J. Opt. Soc. Am. B 18 (11), 1747 (2001)
[14]V. Pervak et al., “Dispersion control over the ultraviolet–visible–near-infrared spectral range with HfO2/SiO2-chirped dielectric multilayers”, Opt. Lett. 32 (9), 1183 (2007)
[15]V. Pervak et al., “High-dispersive mirrors for femtosecond lasers”, Opt. Express 16 (14), 10220 (2008)

See also: dispersion compensation, dielectric mirrors, anti-reflection coatings

Categories: photonic devices, pulses


Dr. R. Paschotta

This encyclopedia is authored by Dr. Rüdiger Paschotta, the founder and executive of RP Photonics Consulting GmbH. Contact this distinguished expert in laser technology, nonlinear optics and fiber optics, and find out how his technical consulting services (e.g. product designs, problem solving, independent evaluations, or staff training) and software could become very valuable for your business!

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