Radionuclides containment in nuclear glasses: an overview

S Gin, P Jollivet, M Tribet, S Peuget, S Schuller - Radiochimica Acta, 2017 - degruyter.com
… The major species integrated in vitreous conditioning matrices are anionic (S 2− , SO 4 2−
). However, their incorporation rate do not exceed 0.1 wt% in the case of metal sulfur [26] and …

Inhibition of p53 inhibitors: progress, challenges and perspectives

G Sanz, M Singh, S Peuget… - Journal of molecular cell …, 2019 - academic.oup.com
p53 is the major tumor suppressor and the most frequently inactivated gene in cancer. p53
could be disabled either by mutations or by upstream negative regulators, including, but not …

Translating p53-based therapies for cancer into the clinic

S Peuget, X Zhou, G Selivanova - Nature Reviews Cancer, 2024 - nature.com
… As p53 is a key regulator of the G1/S cell cycle checkpoint, loss of p53 function leads to
dependence on the intra-S checkpoint and the G2/M checkpoint to detect and initiate repair of …

Effect of chemical composition on borosilicate glass behavior under irradiation

…, S Peuget, G Panczer, D De Ligny, S Henry… - Journal of Non …, 2010 - Elsevier
Assessing the behavior under irradiation of oxide glasses used for nuclear waste immobilization
is essential for qualifying the long-term behavior of the wasteform. This study focuses on …

[HTML][HTML] TP53INP1, a tumor suppressor, interacts with LC3 and ATG8-family proteins through the LC3-interacting region (LIR) and promotes autophagy-dependent cell …

M Seillier, S Peuget, O Gayet, C Gauthier… - Cell Death & …, 2012 - nature.com
TP53INP1 (tumor protein 53-induced nuclear protein 1) is a tumor suppressor, whose
expression is downregulated in cancers from different organs. It was described as a p53 target …

Irradiation stability of R7T7-type borosilicate glass

S Peuget, JN Cachia, C Jégou, X Deschanels… - Journal of nuclear …, 2006 - Elsevier
… ’s modulus of … s modulus was determined from the force applied and the sample deflection
by using Eq. (2).(2) E ( 1 - υ 2 ) = α × r 2 × F D × e 3 , where E is Young’s modulus, υ Poisson’s

Specific outcomes of the research on the radiation stability of the French nuclear glass towards alpha decay accumulation

S Peuget, JM Delaye, C Jégou - Journal of Nuclear Materials, 2014 - Elsevier
This paper presents an overview of the main results of the French research on the long-term
behavior of SON68 nuclear glass towards alpha decay accumulation. The effect of the …

Effects of deposited nuclear and electronic energy on the hardness of R7T7-type containment glass

S Peuget, PY Noël, JL Loubet, S Pavan, P Nivet… - Nuclear Instruments and …, 2006 - Elsevier
The effects of elastic and inelastic interactions induced by cumulative alpha decay on the
hardness of R7T7-type nuclear containment glass were investigated on actinide-doped glass …

Molecular dynamics simulation of radiation damage in glasses

JM Delaye, S Peuget, G Bureau, G Calas - Journal of non-crystalline solids, 2011 - Elsevier
Molecular dynamics simulations of the ballistic effects arising from displacement cascades
in glasses have been investigated in silica and in a SiO 2 –B 2 O 3 –Na 2 O glass. In both …

Raman spectroscopy characterization of actinide oxides (U1− yPuy) O2: Resistance to oxidation by the laser beam and examination of defects

C Jégou, R Caraballo, S Peuget, D Roudil… - Journal of Nuclear …, 2010 - Elsevier
s intervals with a total acquisition time of 30 min. Without the attenuation filter (red curves in
Fig. 5), the 1150 cm −1 peak intensity diminished rapidly for 180 s… intensity after 180 s can be …