Influence of external β-irradiation in oxide glasses

https://doi.org/10.1016/S0022-3093(03)00307-7Get rights and content

Abstract

Radiation effects in oxide glass as external β-irradiation has been investigated by Raman spectroscopy, Cr3+ luminescence and EPR spectroscopy to analyze microstructure evolution. Comparison between simplified and complex glasses (high-level nuclear waste glass analogue) was undertaken. Migration and segregation of sodium have been confirmed on simplified irradiated glasses by a polymerization increase and dissolved oxygen presence. Densification under irradiation has also been demonstrated with the increase of three-membered silicate rings in silicate glass and the decrease of the average Si–O–Si angle in the borosilicate glass. In both glasses, Cr3+ crystal field was increased, suggesting a Cr–O length decrease. The complex borosilicate glass responds differently: densification effect and Na segregation were not detected. Under β-irradiation, electron-trapping processes on Cr6+ occurred, forming Cr4+ and Cr5+ species.

Introduction

Radiations from beta and alpha decay can produce structural changes in glasses. In particular, some changes occur in high-level waste glasses submitted to radiation [1], [2]. Therefore, understanding the glass structure change under irradiation is important to predicting the long-term behaviour of this material. Even if radiation effects on SiO2 structure have been extensively studied [3], [4] and external beta irradiation on six oxides glasses have been recently studied by Boizot et al. [5], [6], to our knowledge, mechanisms in complex glasses are limited. To simulate the β dose irradiation accumulated during nuclear waste storage, external electron irradiation has been performed with a Van de Graaff accelerator.

This paper aims to compare the changes in a complex borosilicate glass having a composition very close to the French nuclear SON68 borosilicate glass with those of simplified borosilicate and silicate glasses. Raman, Cr3+ photoluminescence and EPR spectra were investigated. Raman spectroscopy can reveal glasses microstructure changes under radiation [5]. Cr3+ plays the role of a local luminescent probe in order to follow the Cr3+ crystal field change under radiation. Radiation-induced valence state changes in the glass network are also studied by EPR technique.

Section snippets

Experimental

Two borosilicate (BS1) and (S) silicate glasses were synthesized and doped with chromium while a complex borosilicate glass (BS2) with a composition close to the SON68 glass (Table 1) was fused. Compounds were melted at 1200 °C in a platinum crucible (excepted for S glass where fusion temperature is 1400 °C) then annealed at 520 °C during 1 h in a graphite crucible (this temperature corresponds to Tg+20 °C). Chromium solubility was checked in 1.5% of Cr2O3 doped glasses. Small crystals of Cr2O3

Raman spectra of β irradiated samples

The spectrum of the irradiated silicate glass (S; 4.6 × 109 Gy) on Fig. 1 shows that bands near 850 and 910 cm−1 disappear after irradiation. These bands are respectively assigned to the Si–O symmetric bond stretching motion of Q0 and Q1 species [7] (Qn species correspond to SiO4 units with n bridging oxygen [7]). Moreover, the lower frequency spectrum of the irradiated S glass shows an increase of a peak near 600 cm−1 similar to the D2 ‘defect’ peak of pure silica, corresponding to the

Discussion

Raman experiments indicate that: the average Si–O–Si angle decreases in irradiated BS1 and D2 species increase in irradiated S glasses. We interpret theses results as indicating a possible densification of simplified irradiated glasses. The increase of D2 species was previously observed by Bates et al. [4] in SiO2 irradiated with neutrons, known to be compacted.

Concerning the local luminescent probe Cr3+, absorption peak positions ν1 (4A2  4T2) and ν2 (4A2  4T1) are in relation to the ligand

Conclusion

This study has shown different changes in simplified and complex glasses under irradiation. Segregation and migration of sodium was confirmed on irradiated simplified silicate and borosilicate glasses. Densification on simplified samples is also attested with the production of three-membered silicate rings in the 4.6 × 109 Gy silicate glass, the decrease of Si–O–Si average angle in the borosilicate glass as well as the Cr–O length bond in both glasses. Actually, Cr3+ crystal field increases with

Acknowledgements

The authors thank P. Jollivet (CEA Marcoule) for the synthesis of glasses. The authors are also indebted to the LSI laboratory for the runs at the Van de Graaff accelerator and to T. Pouthier and S. Guillous of the LSI for preparing β-irradiation experiments.

References (17)

  • W.J. Weber

    Nucl. Instrum. and Meth. B

    (1988)
  • R.C. Ewing et al.

    Prog. Nucl. Energy

    (1995)
  • R.A.B. Devine

    Nucl. Instrum. and Meth. B

    (1994)
  • B. Boizot et al.

    J. Non-Cryst. Solids

    (1999)
  • B. Boizot et al.

    Nucl. Instrum. and Meth. B

    (2000)
  • F.L. Galeener

    Solid State Commun.

    (1982)
  • Cz. Koepke et al.

    J. Alloys Compd.

    (2002)
  • U. Hommerich et al.

    J. Lumin.

    (1994)
There are more references available in the full text version of this article.

Cited by (39)

  • Creation of glass-characteristic point defects in crystalline SiO<inf>2</inf> by 2.5 MeV electrons and by fast neutrons

    2019, Journal of Non-Crystalline Solids
    Citation Excerpt :

    In contrast to these studies, interstitial O2 was calculated to be the main diffusing species both in cristobalite and α-quartz structures [49]. However, the presence of interstitial O2 in undamaged α-quartz has never been experimentally demonstrated, while there is ample Raman [19–21,23], PL[17,18,22, 24], EPR [9] or diffusion-based evidence for O2 in silica and silica-based glasses. The present data further confirm the results of the previous study [3], performed at ≈140× lower dose (0.051 GGy γ-rays), that the POL configuration rather than interstitial O2 may be the preferable way of incorporation of excess oxygen in undamaged α-quartz lattice, and that creation of larger voids than available in an intact α-quartz structure is required for interstitial O2 configuration to exist.

View all citing articles on Scopus
View full text