“…Those characteristics are very similar to ones evidenced by Bates et al in neutron-irradiated quartz and amorphous silica [5]. This metamict phase could be considered as a "Medium Density Amorphous" (density = 2.26 g/cm 3 ) phase in addition to the Low Density Amorphous and High Density Amorphous Phases. Hence, it presents interesting aspects regarding the still open question of polyamorphism in silica glass [6].…”
Section: Introductionsupporting
confidence: 86%
“…The densi cation of silica glass under high pressure (HP) [1], by shock waves or irradiation (laser [2], ions, electrons, neutrons) has been extensively studied. Compression of silica gives rise to permanent densi cation with a densi cation ratio of 20% (for HP > 15 GPa) while irradiation does not lead to values exceeding 3-4% [3]. We recently showed the convergence to a common "metamict-like" silica phase after irradiating with 2.5 MeV high-energy electrons amorphous silica samples having different initial densities, up to 11 GGy [4].…”
Section: Introductionmentioning
confidence: 99%
“…We recently showed the convergence to a common "metamict-like" silica phase after irradiating with 2.5 MeV high-energy electrons amorphous silica samples having different initial densities, up to 11 GGy [4]. The metamict densi ed silica phase has density of 2.26 g/cm 3 , and its structure shows a large amount of 3-membered rings, as indicated by the intense 606 cm − 1 ("D 2 ") band in the Raman spectrum [4]. Those characteristics are very similar to ones evidenced by Bates et al in neutron-irradiated quartz and amorphous silica [5].…”
Section: Introductionmentioning
confidence: 99%
“…If the interstitial voids are su ciently large, they can accommodate oxygen molecules O 2 , formed in irradiated silica glass by dimerization of two interstitial oxygen atoms created in Frenkel process [….]. Whether this process is energetically feasible, it is determined by the size of voids: O 2 easily forms by 13 MGy γirradiation in glassy silica (density 2.20 g/cm 3 ) and, in contrast, is completely absent in similarly irradiated α-quartz (density 2.65 g/cm 3 ) [9]. There is no measurable O 2 concentration in α-quartz, even after much higher (7 GGy) dose of MeV electrons [10].…”
The aim of the paper was to learn more about the structure of densified silica, in particular about the metamict-like silica phase (density = 2.26g/cm3) by examining the radiation-induced formation of E’ point defects and interstitial molecular oxygen. The large amount of the molecular oxygen produced after 11 GGy integrated dose irradiation in the metamict-like phase is destroyed when this one is submitted to electron irradiation. It infers a particular behavior to this silica phase compared to the other densified silica where the amount of O2 is reduced compared to silica. The position and shape of the O2 emission line support the idea that the void configuration of metamict phase is close to silica. A strong correlation exists between the formation of 3-membered rings of Si-O bonds and E’-centers in the densification process between 2.20-and 2.26 density.
“…Those characteristics are very similar to ones evidenced by Bates et al in neutron-irradiated quartz and amorphous silica [5]. This metamict phase could be considered as a "Medium Density Amorphous" (density = 2.26 g/cm 3 ) phase in addition to the Low Density Amorphous and High Density Amorphous Phases. Hence, it presents interesting aspects regarding the still open question of polyamorphism in silica glass [6].…”
Section: Introductionsupporting
confidence: 86%
“…The densi cation of silica glass under high pressure (HP) [1], by shock waves or irradiation (laser [2], ions, electrons, neutrons) has been extensively studied. Compression of silica gives rise to permanent densi cation with a densi cation ratio of 20% (for HP > 15 GPa) while irradiation does not lead to values exceeding 3-4% [3]. We recently showed the convergence to a common "metamict-like" silica phase after irradiating with 2.5 MeV high-energy electrons amorphous silica samples having different initial densities, up to 11 GGy [4].…”
Section: Introductionmentioning
confidence: 99%
“…We recently showed the convergence to a common "metamict-like" silica phase after irradiating with 2.5 MeV high-energy electrons amorphous silica samples having different initial densities, up to 11 GGy [4]. The metamict densi ed silica phase has density of 2.26 g/cm 3 , and its structure shows a large amount of 3-membered rings, as indicated by the intense 606 cm − 1 ("D 2 ") band in the Raman spectrum [4]. Those characteristics are very similar to ones evidenced by Bates et al in neutron-irradiated quartz and amorphous silica [5].…”
Section: Introductionmentioning
confidence: 99%
“…If the interstitial voids are su ciently large, they can accommodate oxygen molecules O 2 , formed in irradiated silica glass by dimerization of two interstitial oxygen atoms created in Frenkel process [….]. Whether this process is energetically feasible, it is determined by the size of voids: O 2 easily forms by 13 MGy γirradiation in glassy silica (density 2.20 g/cm 3 ) and, in contrast, is completely absent in similarly irradiated α-quartz (density 2.65 g/cm 3 ) [9]. There is no measurable O 2 concentration in α-quartz, even after much higher (7 GGy) dose of MeV electrons [10].…”
The aim of the paper was to learn more about the structure of densified silica, in particular about the metamict-like silica phase (density = 2.26g/cm3) by examining the radiation-induced formation of E’ point defects and interstitial molecular oxygen. The large amount of the molecular oxygen produced after 11 GGy integrated dose irradiation in the metamict-like phase is destroyed when this one is submitted to electron irradiation. It infers a particular behavior to this silica phase compared to the other densified silica where the amount of O2 is reduced compared to silica. The position and shape of the O2 emission line support the idea that the void configuration of metamict phase is close to silica. A strong correlation exists between the formation of 3-membered rings of Si-O bonds and E’-centers in the densification process between 2.20-and 2.26 density.
“…The integration of silica glasses in optical and electronic devices are, at present, limited by the effects of high-energy radiation on the transmission and reflection properties of the material. As reported in a large number of studies [1][2][3][4][5][6][7][8][9][10][11], the irradiation of silica with either photons or energetic particles (neutrons, electrons, protons, heavy ions) activates a wide range of damage processes that result in the formation of point defects. These localized irregularities of the network are characterized by one or more energy levels lying in the band gap of the dielectric and are responsible for the shift in the optical absorption edge of the glass to lower energies.…”
Due to its unique properties, amorphous silicon dioxide (a-SiO2) or silica is a key material in many technological fields, such as high-power laser systems, telecommunications, and fiber optics. In recent years, major efforts have been made in the development of highly transparent glasses, able to resist ionizing and non-ionizing radiation. However the widespread application of many silica-based technologies, particularly silica optical fibers, is still limited by the radiation-induced formation of point defects, which decrease their durability and transmission efficiency. Although this aspect has been widely investigated, the optical properties of certain defects and the correlation between their formation dynamics and the structure of the pristine glass remains an open issue. For this reason, it is of paramount importance to gain a deeper understanding of the structure–reactivity relationship in a-SiO2 for the prediction of the optical properties of a glass based on its manufacturing parameters, and the realization of more efficient devices. To this end, we here report on the state of the most important intrinsic point defects in pure silica, with a particular emphasis on their main spectroscopic features, their atomic structure, and the effects of their presence on the transmission properties of optical fibers.
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