spatial hole burning (original) (raw)

Author: the photonics expert

Acronym: SHB

Definition: a distortion of the gain shape in a laser medium (or the loss spectrum in a saturable absorber medium), caused by saturation effects of a standing wave

Categories: article belongs to category laser devices and laser physics laser devices and laser physics, article belongs to category physical foundations physical foundations

DOI: 10.61835/cln [Cite the article](encyclopedia%5Fcite.html?article=spatial hole burning&doi=10.61835/cln): BibTex plain textHTML Link to this page LinkedIn

When two counterpropagating quasi-monochromatic light waves are superimposed, they form a so-called standing-wave interference pattern, the period of which is half the wavelength. When that happens with laser light in a laser gain medium, that has two effects:

This can lead to a deformation of the spectral shape of the gain, i.e., a kind of inhomogeneous gain saturation.

spatial hole burning

Figure 1: Illustration of spatial hole burning in a laser crystal. A strong beam with the blue standing-wave intensity pattern saturates the gain (red curve). It experiences a more strongly reduced gain than a weaker beam with slightly longer wavelength, indicated by the green curve.

Similarly, the loss spectrum of a saturable absorber medium can obtain a dip due to spatial hole burning. That can occur e.g. in a rare-earth-doped fiber and is the basis for, e.g., the construction of an automatic tracking filter, as is sometimes used in the context of single-frequency fiber lasers.

Spatial hole burning can have various consequences for the operation of lasers:

Note that lasers with ring resonators (ring lasers) often use unidirectional operation, i.e., not avoiding counterpropagating waves in the laser medium, so that spatial hole burning is eliminated.

Even in standing-wave (linear) resonators, spatial hole burning can be suppressed by the use of special polarization states (→ twisted-mode technique).

The hole burning effect is effectively suppressed for lasing with a sufficiently large bandwidth, where interference patterns are largely washed out. This is also often the case in mode-locked lasers; here it is obvious already in the time domain that a circulating pulse cannot overlap (interfere) with itself in the gain medium, unless the time for traveling from the gain medium to an end mirror and back again is comparable to or shorter than the pulse duration.

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Bibliography

[1] C. L. Tang et al., “Spectral output and spiking behavior of solid-state lasers”, J. Appl. Phys. 34 (8), 2289 (1963) (first mention of spatial hole burning)
[2] T. Kimura et al., “Spatial hole-burning effects in a Nd3+:YAG laser”, IEEE J. Quantum Electron. 7 (6), 225 (1971); https://doi.org/10.1109/JQE.1971.1076746
[3] W. S. Rabinovich and B. J. Feldman, “Spatial hole burning effects in distributed feedback lasers”, IEEE J. Quantum Electron. 25 (1), 20 (1989); https://doi.org/10.1109/3.16236
[4] J. J. Zayhowski, “Limits imposed by spatial hole burning on the single-mode operation of standing-wave laser cavities”, Opt. Lett. 15 (8), 431 (1990); https://doi.org/10.1364/OL.15.000431
[5] B. Braun et al., “Continuous-wave mode-locked solid-state lasers with enhanced spatial hole burning, part I: experiments”, Appl. Phys. B 61 (5), 429 (1995); https://doi.org/10.1007/BF01081271
[6] F. X. Kärtner et al., “Continuous-wave-mode-locked solid-state lasers with enhanced spatial hole-burning, part II: theory”, Appl. Phys. B 61, 569 (1995); https://doi.org/10.1007/BF01091215
[7] R. Paschotta et al., “Single-frequency ytterbium-doped fiber laser stabilized by spatial hole burning”, Opt. Lett. 22 (1), 40 (1997); https://doi.org/10.1364/OL.22.000040
[8] J. Y. Law and G. P. Agrawal, “Effects of spatial hole burning on gain switching in vertical-cavity surface-emitting lasers”, IEEE J. Quantum Electron. 33 (3), 462 (1997); https://doi.org/10.1109/3.556016
[9] R. Paschotta et al., “Passive mode locking of thin-disk lasers: effects of spatial hole burning”, Appl. Phys. B 72 (3), 267 (2001); https://doi.org/10.1007/s003400100486
[10] C. Schäfer et al., “Effects of spatial hole burning in 888 nm pumped, passively mode-locked high-power Nd:YVO4 lasers”, Appl. Phys. B 102, 523 (2011); https://doi.org/10.1007/s00340-011-4409-3
[11] C. Shi et al., “1.2 W single-frequency Tm3+/Ho3+ co-doped fiber oscillator at 2050 nm”, Opt. Lett. 48 (23), 6144 (2023); https://doi.org/10.1364/OL.502554

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