Difference between revisions of "File:CoherentAddition.jpg"
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| + | Example of the coherent addition (coherent combining) of 4 fiber lasers. |
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| + | There are 100% reflection mirrors (Bragg reflectors) at the left hand side. |
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| + | There are coiled laser amplifiers which can be realized as single-mode double-clad fibers; which are, perhaps, coiled. There is coherent coupler, which provides the splitting of modes of lases. Such a splitter has so many outputs, as inputs. Most of outputs are cleaved providing almost zero reflectivity, and only one provides significant feedback. This channed determines the modes with minimal losses. Such modes are common for all lasers, providing the coherent addition of lasers. |
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| + | This figure has an analogy at http://en.wikipedia.org/wiki/File:CoherentAddition.jpg |
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| + | The free use is allowed, the attribution is required. |
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| + | Description from http://en.wikipedia.org/wiki/Coherent_addition is below |
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| + | ==Coherent addition== |
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| + | Usually, the term '''coherent addition''' applies to [[fiber laser]]s. 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. |
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| + | The coherent addition was demonstrated in [[power scaling]] of [[Raman laser]]s <ref>A. Shirakawa, T. Saitou, T. Sekiguchi and K. Ueda: "[http://www.opticsexpress.org/abstract.cfm?id=70290 Coherent addition of fiber lasers by use of a fiber coupler]" [[Optics Express]] '''10''' (2002) 1167–1172</ref>. |
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| + | [[Image:CoherentAddition.jpg|thumb|right|Fig.1. Example of the coherent addition of 4 fiber lasers with a common coupler.]] |
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| + | == Limits of coherent addition == |
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| + | 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.<ref name="kouz05">D. Kouznetsov, J.F. Bisson. A. Shirakawa, K.Ueda |
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| + | "[http://annex.jsap.or.jp/OSJ/opticalreview/TOC-Lists/vol12/12f0445tx.htm Limits of Coherent Addition of Lasers: Simple Estimate]" [[Optical Review]] Vol. '''12''', No. 6, 445–447 (2005). (Also [http://www.ils.uec.ac.jp/~dima/PAPERS/CoupledOptRev.pdf].)</ref> The future increase of number of combined lasers requires the [[exponential growth]] of the spectral bandwidth of gain and/or length of partial lasers. |
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| + | The same conclusion can be made also on the base of more detailed simulations. |
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| + | <ref name="tony"> |
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| + | A.E.Siegman. Resonant modes of linearly coupled multiple fiber laser structures. |
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| + | Preprint of the Stanford University, 2005, 25 pages; |
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| + | http://www.stanford.edu/~siegman/coupled_fiber_modes.pdf |
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| + | </ref> Practically, the combination of more than ten lasers in such a way should be difficult if at all. |
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| + | == References == |
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| + | <references/> |
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| + | <!-- this link needs to be repaired |
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| + | *A. E. Siegman: "[http://www.stanford.edu/~siegman/Coupled_fiber_modes.pdf Resonant modes of linearly coupled multiple fiber laser structures]", [[Stanford University]] homepage (2004). |
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| + | !--> |
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| + | [[Category:Laser science]] |
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Latest revision as of 09:39, 21 June 2013
Example of the coherent addition (coherent combining) of 4 fiber lasers.
There are 100% reflection mirrors (Bragg reflectors) at the left hand side.
There are coiled laser amplifiers which can be realized as single-mode double-clad fibers; which are, perhaps, coiled. There is coherent coupler, which provides the splitting of modes of lases. Such a splitter has so many outputs, as inputs. Most of outputs are cleaved providing almost zero reflectivity, and only one provides significant feedback. This channed determines the modes with minimal losses. Such modes are common for all lasers, providing the coherent addition of lasers.
This figure has an analogy at http://en.wikipedia.org/wiki/File:CoherentAddition.jpg
The free use is allowed, the attribution is required.
Description from http://en.wikipedia.org/wiki/Coherent_addition is below
Coherent addition
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].
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 in such a way should be difficult if at all.
References
- ↑ 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
- ↑ D. Kouznetsov, J.F. Bisson. A. Shirakawa, K.Ueda "Limits of Coherent Addition of Lasers: Simple Estimate" Optical Review Vol. 12, No. 6, 445–447 (2005). (Also [1].)
- ↑ 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
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