“Canonic” optical fibers for fundamental studies


RADIATION-MATTER INTERACTION MECHANISM

The radiation-induced attenuation and emission in silica fibers or glasses can be explained by the properties of the point defects induced by ionization or atomic displacements [1]. The amplitude and the kinetics of degradation related to these defects depend on very many parameters, in particular the fiber properties: composition, drawing conditions... [1].

To become able to control the radiation response of optical fibers, it is necessary to identify the nature, the optical properties, the generation and bleaching mechanisms of these defects. The ultimate goal of these fundamental studies is to predict, through simulation, the response of an optical fiber for a given application and a specific environment. Such a predictive tool must be multi-scale and multi-physics to account for the complexity of the radiation-matter interactions.

Fig.1. illustrates the theoretical approach chosen for calculating the optical and structural properties of point defects in dielectrics [2]. In order to validate these ab initio tools, the confrontation between theoretical and experimental results remains indispensable. This is made possible thanks to the manufacturing and the characterization of canonical fibers [3-5], designed to correspond to the simulation supercells accessible and based on supercomputers, such as TERA 1000 of the CEA.

Illustration of the coupled simulation/experiment approach implemented for the prediction of the structural and optical properties of radiation induced point defects in optical fibers

Fig.1. Illustration of the coupled simulation/experiment approach implemented for the prediction of the structural and optical properties of radiation induced point defects in optical fibers [2].

COLLABORATIONS

Since 2006, LabH6 has been working with CEA DAM and academic partners: Univ. Palermo, Univ. Nova Gorica, CNR Trieste

This work is partly carried out within the framework of a joint research team (ERC, currently being renewed) between the CEA DAM (Arpajon) and the UJM (LabHC) on the study of the basic mechanisms of radiation interaction - dielectrics.

At the European level, the consortium is simultaneously working on the fabrication of canonical samples (CEA, LabH6), on their experimental characterization (LabH6, Univ., Palermo) as well as on their theoretical characterization at different scales (CEA, Univ.Trieste, Univ. Gorica).

CEA

SPECTROSCOPIC CHARACTERISATION TOOLS

Many spectroscopic techniques can be used for the characterization of point defects. The main ones are absorption spectroscopy, Raman, luminescence and electron paramagnetic resonance. In situ techniques that can be applied during irradiation should be distinguished from those that can only be performed after irradiation. These later can only provide information on stable defects and not on transient, unstable centers.

In the case of optical fibers, it is often useful to be able to carry out spatially-resolved measurements giving accessto the spatial distribution (cartography) of the defects: an example of in situ measurement by cathodo-luminescence is reported in Fig.3 [6]. A recent review paper [2] summarizes the current knowledge of defects related to pure or doped silica fibers and glasses with the following elements: Ge, P, F, Al.

[1] S. Girard et al., TNS, 60 (3) 2015, 2013

[2] S. Girard et al., Reviews in Physics, 2019

[3] S. Girard et al., IEEE TNS 55 (6), 3473, 2008

[4] S. Girard et al., TNS TNS 55 (6), 3508, 2008

[5] N. Richard et al., IEEE TNS 61 (4) 1819, 2014

[6] I. Reghioua, Thèse Doctorat UJM, 2019

 

Since 2006: More than 15 preforms and 30 "canonical" optical fibers have been developed for fundamental studies:

Radiation induced point defects in silica-based optical fibers

Illustration of the first canonical sample made for the study of Ge-doped silica. The simulation cells correspond to the doping levels achieved.

Fig.2.Illustration of the first canonical sample made for the study of Ge-doped silica. The simulation cells correspond to the doping levels achieved.

Fig.3. Illustration of the radial distribution of the GLPC light emitting defect emitting at 400 nm -Cathodoluminescence result in a Ge canonical fiber

Fig.3. Illustration of the radial distribution of the GLPC light emitting defect emitting at 400 nm [2] -Cathodoluminescence result in a Ge canonical fiber [6].