2012
DOI: 10.1109/jphot.2012.2190724
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Photonic Free-Electron Lasers

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Cited by 7 publications
(5 citation statements)
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References 21 publications
(30 reference statements)
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“…Here we demonstrate a very different and much more general approach to photonic crystal Bloch mode lasers where gain and coherent output radiation is provided by free electrons, without relying on any specific gain material. Thereby, the range of output wavelengths is not bound to pre-determined values but can be scaled over orders of magnitude via scaling the spatial period * p.j.m.vanderslot@utwente.nl of the photonic crystal [19]. The work that we present here gives the first complete description and proof of coherent emission from a photonic crystal-based freeelectron laser, by solving self-consistently the coupled Maxwell and Lorentz-Newton equations in three dimensions.…”
Section: Introductionmentioning
confidence: 99%
“…Here we demonstrate a very different and much more general approach to photonic crystal Bloch mode lasers where gain and coherent output radiation is provided by free electrons, without relying on any specific gain material. Thereby, the range of output wavelengths is not bound to pre-determined values but can be scaled over orders of magnitude via scaling the spatial period * p.j.m.vanderslot@utwente.nl of the photonic crystal [19]. The work that we present here gives the first complete description and proof of coherent emission from a photonic crystal-based freeelectron laser, by solving self-consistently the coupled Maxwell and Lorentz-Newton equations in three dimensions.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, while the nanoscale range of low/medium energy electron evanescent fields has provided for the emergence of electron-induced radiation emission (EIRE) and electron energy loss (EELS) spectroscopy techniques for probing and mapping the photonic and plasmonic properties of nanostructures, 18,[21][22][23][24] it places constraints on the experimental geometry in such studies and on the utility of freeelectron pumping in applications such as nanoscale tunable light sourcing. [25][26][27] Here, we report on an experimental platform using a tapered optical fiber geometry ( Fig. 1) akin to those employed for sampling evanescent light fields in near-field optical microscopy, which enables the study of proximity interactions between free electrons and nanophotonic structures mediated by the aforementioned exponentially decaying field at optical frequencies.…”
mentioning
confidence: 99%
“…These codes have been successfully applied in a huge variety of situations. Examples are found in astrophysics, particle acceleration and FELs [69,83,[142][143][144][145][146]. For FELs in particular, these codes allow the investigation of multidimensional effects and highly nonlinear phenomena, which is very complex using other techniques [144].…”
Section: Nonlinear Theory: Particle-in-cell Calculationsmentioning
confidence: 99%
“…Implementing these steps not only in a single spatial dimension, but in three-dimensions, makes PIC methods very powerful tools. For example, three-dimensional PIC methods allow to compute the temporal evolution of the electromagnetic field, particle positions and velocities in a slow-wave FEL [69,83,144,145]. Specifically for the present work, it becomes possible, e.g., to compute the steady-state output power of pFELs or investigate mode competition in pFELs.…”
Section: Nonlinear Theory: Particle-in-cell Calculationsmentioning
confidence: 99%
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