Using As2S3 and AsS2 glasses as an example, the principal possibility of using positron annihilation spectroscopy methods for studying the evolution of the free volume of hollow nanoobjects in chalcogenide glassy semiconductors exposed to radiation is shown. The results obtained by measurements of the positron annihilation lifetime and Doppler broadening of the annihilation line in reverse chronological order are in full agreement with the optical spectroscopy data in the region of the fundamental absorption edge, being adequately described within coordination defect-formation and physical-aging models
Positron lifetime and angular correlation of annihilation radiation (ACAR) have been measured on fus...
International audienceSubsequent stages of atomic-deficient nanostructurization finalizing rare-eart...
Positron annihilation techniques, being non-destructive, allowing depth profiling down to a few micr...
Using As2S3 and AsS2 glasses as an example, the principal possibility of using positron annihilation...
Unirradiated and γ-irradiated (average energy E = 1.25 MeV and dose Φ = 2.41 MGy) chalcogenide glass...
The nature of coordination defects in chalcogenide vitreous semiconductors of As-Ge-S system have be...
Chalcogenide glass (ChG) materials are increasingly being utilized in infrared planar photonic devic...
An approach to structural characterization of chalcogenide glasses based on the study of void distri...
International audiencePositron annihilation lifetime spectroscopy combined with Doppler broadening o...
AbstractPositron annihilation lifetime spectroscopy combined with Doppler broadening of annihilation...
The positron annihilation lifetime spectroscopic technique was applied to study nanocrystals formati...
High-energy (2Mev) electron irradiation may produce excess density of valence-alternation pairs (VAP...
The crystal evolution and defect formation in scintillating glasses as a consequence of thermal anne...
International audiencePositron annihilation lifetime (PAL) spectroscopy was applied for the first ti...
Nanovoids in As2S3-based glasses (As 2S3, (As2S3)85Ag 15, and (As2S3)85(AgI) 15), a polymer and a As...
Positron lifetime and angular correlation of annihilation radiation (ACAR) have been measured on fus...
International audienceSubsequent stages of atomic-deficient nanostructurization finalizing rare-eart...
Positron annihilation techniques, being non-destructive, allowing depth profiling down to a few micr...
Using As2S3 and AsS2 glasses as an example, the principal possibility of using positron annihilation...
Unirradiated and γ-irradiated (average energy E = 1.25 MeV and dose Φ = 2.41 MGy) chalcogenide glass...
The nature of coordination defects in chalcogenide vitreous semiconductors of As-Ge-S system have be...
Chalcogenide glass (ChG) materials are increasingly being utilized in infrared planar photonic devic...
An approach to structural characterization of chalcogenide glasses based on the study of void distri...
International audiencePositron annihilation lifetime spectroscopy combined with Doppler broadening o...
AbstractPositron annihilation lifetime spectroscopy combined with Doppler broadening of annihilation...
The positron annihilation lifetime spectroscopic technique was applied to study nanocrystals formati...
High-energy (2Mev) electron irradiation may produce excess density of valence-alternation pairs (VAP...
The crystal evolution and defect formation in scintillating glasses as a consequence of thermal anne...
International audiencePositron annihilation lifetime (PAL) spectroscopy was applied for the first ti...
Nanovoids in As2S3-based glasses (As 2S3, (As2S3)85Ag 15, and (As2S3)85(AgI) 15), a polymer and a As...
Positron lifetime and angular correlation of annihilation radiation (ACAR) have been measured on fus...
International audienceSubsequent stages of atomic-deficient nanostructurization finalizing rare-eart...
Positron annihilation techniques, being non-destructive, allowing depth profiling down to a few micr...