Coherent addition

Coherent addition (or coherent combining) of lasers is one of methods of the power scaling. It allows a to increase the output power and brightness of single-transversal mode laser.

Usually, the term coherent addition applies to fiber lasers. As the ability of pumping and/or cooling of a single laser is saturated, several similar lasers can be forced to oscillate in phase with common coupler. The coherent addition was demonstrated in power scaling of Raman lasers.[1]

Fig.1. Example of the coherent addition of 4 fiber lasers with a common coupler.

Limits of coherent addition

The addition of lasers reduces the number of longitudinal modes in the output beam; the more lasers are combined, the smaller is the number of longitudinal modes in the output. The simple estimates show that the number of output modes reduces exponentially with number of lasers combined. Of order of eight lasers can be combined in such a way.[2] The future increase of number of combined lasers requires the exponential growth of the spectral bandwidth of gain and/or length of partial lasers. The same conclusion can be made also on the base of more detailed simulations. [3] Practically, the combination of more than ten lasers with a passive combining arrangement appears to be difficult. However, active coherent combining of lasers has the potential to scale to very large numbers of channels.[4]

Nonlinear coherent addition of lasers

Nonlinear interactions of light waves are used widely to synchronize the laser beams in multichannel optical systems. Self-adjusting of phases may be robustly achievable in binary-tree array of beam-splitters and degenerate four-wave mixing Kerr Phase conjugation[5] in Chirped pulse amplification extreme light facilities.[6] This phase-conjugating Michelson interferometer increases the brightness as ${\displaystyle N^{2}}$,[7] where ${\displaystyle N}$ is the number of phase-locked channels.

Talbot coherent addition

Constructive interference due to Talbot self-imaging forces the lasers in the array to transverse mode lock. The Fresnel number ${\displaystyle F}$ of the one-dimensional ${\displaystyle N-}$ element laser array phase-locked by Talbot cavity is given by[8] ${\displaystyle F=N^{2}.}$ For the two-dimensional ${\displaystyle N^{2}-}$ element laser array phase-locked by Talbot cavity Fresnel number ${\displaystyle F}$ scales as ${\displaystyle F=N^{2}}$ as well. Talbot phase-locking techniques are applicable to thin disk diode-pumped solid-state laser arrays.[9]

See also

• List of laser articles

References

1. A. Shirakawa, T. Saitou, T. Sekiguchi and K. Ueda: "Coherent addition of fiber lasers by use of a fiber coupler" Optics Express 10 (2002) 1167–1172
2. D. Kouznetsov, J.F. Bisson. A. Shirakawa, K.Ueda "Limits of Coherent Addition of Lasers: Simple Estimate Archived 2007-09-27 at the Wayback Machine" Optical Review Vol. 12, No. 6, 445–447 (2005). (Also .)
3. A.E.Siegman. Resonant modes of linearly coupled multiple fiber laser structures. Preprint of the Stanford University, 2005, 25 pages; http://www.stanford.edu/~siegman/coupled_fiber_modes.pdf
4. Leo A. Siiman, Wei-zung Chang, Tong Zhou, and Almantas Galvanauskas, "Coherent femtosecond pulse combining of multiple parallel chirped pulse fiber amplifiers" Optics Express 20 (2012) 18097-18116
5. Okulov, A Yu (2014). "Coherent chirped pulse laser network with Mickelson phase conjugator". Applied Optics. 53 (11): 2302–2311. arXiv:1311.6703. doi:10.1364/AO.53.002302.
6. "The Nobel Prize in Physics 2018". Nobel Foundation. Retrieved 2 October 2018.
7. Basov, N G; Zubarev, I G; Mironov, A B; Michailov, S I; Okulov, A Yu (1980). "Laser interferometer with wavefront reversing mirrors". Sov. Phys. JETP. 52 (5): 847. Bibcode:1980ZhETF..79.1678B.
8. Okulov, A Yu (1990). "Two-dimensional periodic structures in nonlinear resonator". JOSA B. 7 (6): 1045–1050. doi:10.1364/JOSAB.7.001045.
9. Okulov, A Yu (1993). "Scaling of diode-array-pumped solid-state lasers via self-imaging". Opt. Comm. 99 (5–6): 350–354. doi:10.1016/0030-4018(93)90342-3.