Positron Annihilation Spectroscopy (PAS) performed with continuous and pulsed positron beams allows to characterize the size of the intrinsic nano-voids in silica glass, their in depth modification after ion implantation and their decoration by implanted ions. Three complementary PAS techniques, lifetime spectroscopy (LS), Doppler broadening spectroscopy (DBS) and coincidence Doppler broadening spectroscopy (CDBS) will be illustrated by presenting, as a case study, measurements obtained on virgin and gold implanted silica glass
The positron annihilation lifetime spectroscopy was applied to study the porous Vycor glass annealed...
Silver nanoparticles with continuous size distribution from 10 to 20 nm were incorporated into porou...
Nanocrystalline silver particles were grown in a glass medium by ion-exchange and reduction techniqu...
The radiation damage produced in silica glass implanted with Ar+ and Au+ ions at different implantat...
Samples of amorphous silica were implanted with Au ions at an energy of 190 keV and fluences of 1×10...
Resistive Plate Chamber (RPC) detector materials viz., Asahi and Saint Gobain float glasses were exp...
Positron annihilation spectroscopy (PAS) is a technique for measuring the length of time that a posi...
The major aspect of this research is the development of a variable-energy PALS beamline based on a S...
The positronium annihilation of surface modified silica gel particles was discussed. The groups of a...
Silicon implanted thermal SiO{sub 2} layers were studied using depth-resolved positron annihilation ...
Using As2S3 and AsS2 glasses as an example, the principal possibility of using positron annihilation...
The application of positron annihilation spectroscopy for the studies of defects produced by differe...
Positron annihilation techniques, being non-destructive, allowing depth profiling down to a few micr...
We report data on high-quality silicon samples implanted with 4 MeV silicon ions at doses of 1012-10...
Abstract We briefly review the principles of the Doppler Broadening of the positron annihilation ra...
The positron annihilation lifetime spectroscopy was applied to study the porous Vycor glass annealed...
Silver nanoparticles with continuous size distribution from 10 to 20 nm were incorporated into porou...
Nanocrystalline silver particles were grown in a glass medium by ion-exchange and reduction techniqu...
The radiation damage produced in silica glass implanted with Ar+ and Au+ ions at different implantat...
Samples of amorphous silica were implanted with Au ions at an energy of 190 keV and fluences of 1×10...
Resistive Plate Chamber (RPC) detector materials viz., Asahi and Saint Gobain float glasses were exp...
Positron annihilation spectroscopy (PAS) is a technique for measuring the length of time that a posi...
The major aspect of this research is the development of a variable-energy PALS beamline based on a S...
The positronium annihilation of surface modified silica gel particles was discussed. The groups of a...
Silicon implanted thermal SiO{sub 2} layers were studied using depth-resolved positron annihilation ...
Using As2S3 and AsS2 glasses as an example, the principal possibility of using positron annihilation...
The application of positron annihilation spectroscopy for the studies of defects produced by differe...
Positron annihilation techniques, being non-destructive, allowing depth profiling down to a few micr...
We report data on high-quality silicon samples implanted with 4 MeV silicon ions at doses of 1012-10...
Abstract We briefly review the principles of the Doppler Broadening of the positron annihilation ra...
The positron annihilation lifetime spectroscopy was applied to study the porous Vycor glass annealed...
Silver nanoparticles with continuous size distribution from 10 to 20 nm were incorporated into porou...
Nanocrystalline silver particles were grown in a glass medium by ion-exchange and reduction techniqu...