English
español
Please use this identifier to cite or link to this item:
http://hdl.handle.net/10261/173715
Share/Impact:
Statistics |
![]() ![]() |
|
|
Visualizar otros formatos: MARC | Dublin Core | RDF | ORE | MODS | METS | DIDL | DATACITE | |||
|
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Brunner, Daniel | es_ES |
dc.contributor.author | Jacquot, Maxime | es_ES |
dc.contributor.author | Larger, Laurent | es_ES |
dc.contributor.author | Fischer, Ingo | es_ES |
dc.date.accessioned | 2019-01-03T09:42:17Z | - |
dc.date.available | 2019-01-03T09:42:17Z | - |
dc.date.issued | 2017 | - |
dc.identifier.citation | 2017 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC) (2017) | es_ES |
dc.identifier.isbn | 978-1-5090-6736-7 | - |
dc.identifier.uri | http://hdl.handle.net/10261/173715 | - |
dc.description | Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC).-- Date of Conference: 25-29 June 2017.-- Conference Location: Munich, Germany. | es_ES |
dc.description.abstract | Networks of photonic elements are a key enabling technology for the realization of multiple next generation photonic systems. Phased beam arrays, coherent beam combining or neuromorphic computing in photonic networks: all these high-impact applications fundamentally require coupling between a large number of photonic components. Recently, a small network of ~20 semiconductor lasers based on coupling via a holographic element was reported [1]. However, the demonstration of large-scale complex photonic networks is lacking.Here, we demonstrate the scalability of holographic coupling, creating a large scale complex network of 1600 opto-electronic oscillators. The network's nonlinear nodes are implemented using a spatial light modulator (SLM) operated in intensity modulation mode. Imaging the SLM-surface through a polarizing beam splitter (PBS) onto a camera and closing the loop between camera and the SLM, we realize a nonlinear iterative map. The state of SLM pixel n is then given by I n (t + 1) = sin 2 (κI n (t) + φ 0 ). Here, I n (t)is the nth pixel intensity at time t, κ the feedback gain and φ 0 a constant phase offset. This equation corresponds to a simplified version of the Ikeda map. Figure 1 (a) schematically illustrates the experimental implementation. An exemplary bifurcation diagram for node (23, 8) is shown in Fig. 1 (b). The route to chaos shown in Fig. 1(b) exhibits the period-doubling behaviour expected from such an Ikeda system. | es_ES |
dc.language.iso | eng | es_ES |
dc.publisher | Institute of Electrical and Electronics Engineers | es_ES |
dc.rights | closedAccess | es_ES |
dc.subject | Photonics | es_ES |
dc.subject | Couplings | es_ES |
dc.subject | Laser beams | es_ES |
dc.subject | Complex networks | es_ES |
dc.subject | Oscillators | es_ES |
dc.subject | Reservoirs | es_ES |
dc.subject | Chaos | es_ES |
dc.title | A complex network of 1600 holographically coupled opto-electronic oscillators: Network dynamics and utilisation for reservoir computing | es_ES |
dc.type | comunicación de congreso | es_ES |
dc.identifier.doi | 10.1109/CLEOE-EQEC.2017.8086462 | - |
dc.description.peerreviewed | Peer reviewed | es_ES |
dc.relation.publisherversion | https://doi.org/10.1109/CLEOE-EQEC.2017.8086462 | es_ES |
dc.relation.csic | Sí | es_ES |
oprm.item.hasRevision | no ko 0 false | * |
Appears in Collections: | (IFISC) Libros y partes de libros |
Files in This Item:
File | Description | Size | Format | |
---|---|---|---|---|
accesoRestringido.pdf | 59,24 kB | Adobe PDF | ![]() View/Open |
Show simple item record
WARNING: Items in Digital.CSIC are protected by copyright, with all rights reserved, unless otherwise indicated.