• Aucun résultat trouvé

Mixed temperature and radiation effects on fluorine-doped optical fibers

N/A
N/A
Protected

Academic year: 2021

Partager "Mixed temperature and radiation effects on fluorine-doped optical fibers"

Copied!
2
0
0

Texte intégral

(1)

an author's https://oatao.univ-toulouse.fr/23030

Rizzolo, Serena and Girard, Sylvain and Boukenter, Aziz and Ouerdane, Youcef and Boscaino, Roberto and Paillet, Philippe and Marcandella, Claude and Périsse, Jean-Reynald and Cannas, Marco Mixed temperature and radiation effects on fluorine-doped optical fibers. (2016) In: 11th International Symposium on SiO2, Advanced Dielectrics and Related Devices, 13 June 2016 - 15 June 2016 (Nice, France).

(2)

S. Rizzolo

1,2*

, S. Girard

1

, A. Boukenter

1

, Y. Ouerdane

1

, R. Boscaino

2

, P. Paillet

3

,

C. Marcandella

3

, J. Périsse

4

, J-R. Macé

5

, and M. Cannas

2

Mixed temperature and radiation effects

on fluorine-doped optical fibers

AIM

This work is centered on the paramagnetic defects induced by 10keV X-rays exposure at different irradiation temperatures (TI) ranging from 25 °C up to 250 °C in fluorine doped fibers aiming to investigate the influence of TI on the generation mechanisms defects.

* Serena Rizzolo

Ph. Dr

ISAE-SUPAERO

10, Avenue Edouard Belin 31400 Toulouse (France)

serena.rizzolo@isae-supaero.fr

1Laboratoire Hubert Curien, Université Jean Monnet, CNRS UMR 5516, 18 Rue Benoît Lauras, 42000, Saint-Etienne, France 2Dipartimento di Fisica e Chimica, Università di Palermo, Viale delle Scienze Parco d’Orléans II, Ed. 17, 90128 Palermo, Italy

3 CEA, DAM, DIF, F-91297 Arpajon, France, 4Areva NP, 10 Rue Juliette Récamier, 69006, Lyon, France; 5 Areva NP, 1, Place Jean-Millier 92084, Paris-La Défense, France

CONCLUSION

Defects induced in Fluorine-doped single mode fiber by 10keV X-rays have been investigated by EPR experiments up to 1MGy (SiO2) and for TI from 25 °C up to 250 °C. We have identified that several paramagnetic defects related to the silica network, Si- E’, NBOHC and POR are created by irradiation; their concentrations increase and saturate on increasing TI in accordance with an activation energy of 26 meV. x104 x104 (b) (a) (b) 3340 3360 3380 3400 3420 3440 3460 3480

EPR Si

gnal (a.u.)

Magnetic Field (G)

10-1 100 1013 1014 1015 1016 1017 E' NBOH POR Defect Conc entration (cm -3 ) Dose (MGy)

E’ NBOHC POR

CT=0 (cm-3) (10±1)∙10 16 (2.8±0.1)∙1015 (2.8±0.1)∙1015 Ea (meV) 26±1 26±1 26±1 s 7±2 11±2 11±2 20 25 30 35 40 45 50 1015 1016 1017 1014 1015 1016 1014 1015 1016 Experimental Data CE'=CT=0exp[-(Ea/KT)s] (a) Experimental Data CNBOH=CT=0exp[-(Ea/KT)s] (b)

1/KT (eV

-1

)

Defect Concentration (c

m

-3

)

Experimental Data C POR=CT=0exp[-(Ea/KT) s ] (c)

C

T=0 is the defect concentration

at 0K;

s

is a stretching factor.

To estimate the activation energy,

E

a, we fitted the experimental

data with the Arrhenius law:

Table 1. Parameters obtained from the fit

Figure 3: Concentrations of (a) E’,

(b) NBOH and (c) POR centers as a

function of TI for irradiated sample

at 1MGy (SiO2). The dotted lines in

each graph indicate the exponential fits.

EXPERIMENTAL RESULTS

Figure 2: Concentration of E’ centers, NBOHC and POR point defects as a function of the total deposited dose.

All defect concentrations increase with the dose, E’ center

evidences the largest concentration.

We found for the three

generated defects an

activation energy of

26 meV

.

Figure 1: EPR first harmonic spectra for F-doped fiber irradiated at

250°C up to 1MGy(SiO2). The part (a) shows the E’ center line shape

and in (b) is shown the EPR spectrum associated with the NBOH and the POR centers.

 Rad hard single mode optical fiber F-doped in core (0.2 wt.%) and cladding (1.5 wt.%).

 10keV X-ray irradiations with a dose rate of 40Gy/s and a total

dose of 1MGy (SiO2). TI varied from RT~25°C up to 250 °C.

 EPR spectra were recorded at RT to investigate E’ defects and at liquid nitrogen temperature (77K) for NBOH and POR centers.

MATERIALS AND METHODS

The radiation effects in silica have been the object of intensive studies over the last decades. One of the main investigation technique is the electron paramagnetic resonance (EPR), powerful to identify the microscopic structure of paramagnetic defects such as:

The understanding of generation mechanisms and of the influence of important parameters such as the irradiation temperature is relevant to improve the radiation resistance of optical fibers.

INTRODUCTION

E’ center (≡Si•)

Si dangling bond

Non-Brinding Oxygen Hole Center, ≡Si-O•

O dangling bond,.

PerOxy Radical: ≡Si-O-O•

Si atom linked to an oxygen molecule

Références

Documents relatifs

Following tool-use training, participants per- formed a crossmodal congruency task, by responding to tactile vibrations applied to their hands, while ignor- ing visual

The second type of PIGL is produced at a place where the fiber is not translation invariant. We consider two examples : 1) PIGL from the cross section of a cut fiber, 2) PIGL assisted

By the way, BJT degradation involves hole trapping, and dose rate effects are observed… We also remind that comparison between dose rate dependences of the

An ELDRS explanation based on a trap model was proposed in [3]: assuming that degradation results from hole trapping on gap levels, and based on a simple set

Ouerdane, “Combined high dose and temperature radiation effects on multimode silica-based optical fibers ”, IEEE Transactions on Nuclear Science, 60

environments characterized by high doses and high dose-rates. On the basis of the experimental studies we carried out, some further research lines can be suggested.

Figure 4 reports the studied paramagnetic defects induced in the neutron irradiated sample at the highest dose of 10 17 n/cm²: in (a) the axial symmetry lineshape related to

Comme le relève Reif en 2015, « certains États ont mis en place des institutions thématiques indépendantes de défense des droits de l'Homme, qui se consacrent à la