People | Locations | Statistics |
---|---|---|
Naji, M. |
| |
Motta, Antonella |
| |
Aletan, Dirar |
| |
Mohamed, Tarek |
| |
Ertürk, Emre |
| |
Taccardi, Nicola |
| |
Kononenko, Denys |
| |
Petrov, R. H. | Madrid |
|
Alshaaer, Mazen | Brussels |
|
Bih, L. |
| |
Casati, R. |
| |
Muller, Hermance |
| |
Kočí, Jan | Prague |
|
Šuljagić, Marija |
| |
Kalteremidou, Kalliopi-Artemi | Brussels |
|
Azam, Siraj |
| |
Ospanova, Alyiya |
| |
Blanpain, Bart |
| |
Ali, M. A. |
| |
Popa, V. |
| |
Rančić, M. |
| |
Ollier, Nadège |
| |
Azevedo, Nuno Monteiro |
| |
Landes, Michael |
| |
Rignanese, Gian-Marco |
|
Min, Rui
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (25/25 displayed)
- 2023Correction: Savović et al. Power Flow in Multimode Graded-Index Microstructured Polymer Optical Fibers. Polymers 2023, 15, 1474
- 2023Power Flow in Multimode Graded-Index Microstructured Polymer Optical Fiberscitations
- 2023Bragg Gratings in ZEONEX Microstructured Polymer Optical Fiber With 266 nm Nd:YAG Lasercitations
- 2022Mode Coupling and Steady-State Distribution in Multimode Step-Index Organic Glass-Clad PMMA Fiberscitations
- 2022Treatment of Mode Coupling in Step-Index Multimode Microstructured Polymer Optical Fibers by the Langevin Equationcitations
- 2022Influence of the Width of Launch Beam Distribution on the Transmission Performance of Seven-Core Polymer-Clad Silica Fiberscitations
- 2022Transmission performance of multimode W-type microstructured polymer optical fiberscitations
- 2022Interrogation Method with Temperature Compensation Using Ultra-Short Fiber Bragg Gratings in Silica and Polymer Optical Fibers as Edge Filterscitations
- 2021Compact dual-strain sensitivity polymer optical fiber grating for multi-parameter sensingcitations
- 2021Chirped POF Bragg grating production utilizing UV cure adhesive coating for multiparameter sensingcitations
- 2020Bragg gratings inscribed in solid-core microstructured single-mode polymer optical fiber drawn from a 3D-printed polycarbonate preformcitations
- 2020Bragg gratings inscribed in solid-core microstructured single-mode polymer optical fiber drawn from a 3D-printed polycarbonate preform
- 2019Inscription of Bragg gratings in undoped PMMA mPOF with Nd:YAG laser at 266 nm wavelengthcitations
- 2019Toward Commercial Polymer Fiber Bragg Grating Sensors: Review and Applicationscitations
- 2018Hot water-assisted fabrication of chirped polymer optical fiber Bragg gratingscitations
- 2018Bragg Grating Inscription With Low Pulse Energy in Doped Microstructured Polymer Optical Fiberscitations
- 2018Influence of the Cladding Structure in PMMA mPOFs Mechanical Properties for Strain Sensors Applicationscitations
- 2018Fast Inscription of Long Period Gratings in Microstructured Polymer Optical Fiberscitations
- 2018Thermal stability of fiber Bragg gratings inscribed in microstructured polymer optical fibers with a single UV laser pulse
- 2018Largely tunable dispersion chirped polymer FBGcitations
- 2018Microstructured PMMA POF chirped Bragg gratings for strain sensingcitations
- 2018LPG inscription in mPOF for optical sensingcitations
- 2018Chirped mPOF Bragg grating for strain sensing
- 2017Bandpass transmission filters based on phase shifted fiber Bragg gratings in microstructured polymer optical fiberscitations
- 2016Passive and Portable Polymer Optical Fiber Cleavercitations
Places of action
Organizations | Location | People |
---|
article
Influence of the Width of Launch Beam Distribution on the Transmission Performance of Seven-Core Polymer-Clad Silica Fibers
Abstract
<jats:p>We propose a space division multiplexing (SDM) in a newly constructed multicore polymer-clad silica fiber (PCSF) with seven cores arrayed in a hexagonal array, each carrying a centrally launched beam. This enables a higher SDM capacity at longer fiber lengths in the proposed seven-core PCSF if compared with previously proposed angular division multiplexing (ADM) in single-core (SC) PCSF. As a result, the SDM is not limited to short fiber lengths in the proposed seven-core PCSF, as it is in the case of the ADM channels due to mode coupling in the SC PCSF. In addition, the time-independent power flow equation (TI PFE) is used to analyze the effect of the width of the launch beam distribution on the equilibrium mode distribution (EMD) and steady state distribution (SSD) in each of the seven cores of the investigated PCSF. The width of the launch beam distribution has a considerable impact on the fiber length at which the EMD and SSD are attained, according to our numerical results. Thus, by decreasing the full width at half maximum (FWHM) of the launch beam distribution from 20 to 2°, the length at which EMD is established increases from Lc = 1020 to 1250 m, and the length at which SSD is attained increases from zs = 2650 to 3250 m. A narrow launch beam distribution leads to higher bandwidth at small and intermediate fiber lengths. On the other hand, at shorter fiber lengths, a wider launch beam distribution induces a bandwidth change from 1/z proportional to 1/z1/2 proportional curve, e.g., a slower bandwidth reduction. When building a multicore optical fiber transmission system for SDM, such characterization of multicore PCSFs under various launch conditions should be taken into account.</jats:p>