Abstract:Herein, the optical absorption, X‐ray diffraction (XRD) analysis data, and mechanical properties along the ion path are analyzed for gadolinium gallium garnet (Gd3Ga5O12 or GGG) single crystals irradiated with fast 84Kr ions to fluences of 1013–1014 ion cm−2. It is found that the optical absorption spectra of Czochralski‐grown unirradiated GGG crystal consist of relatively narrow lines in the UV spectral range associated with the 4f–4f transitions in Gd3+ ions. Transitions from the 6S7/2 ground state to the 6P… Show more
“…It is also known that when ZrO 2 is irradiated with ions with an energy above the threshold, an intense generation of anion vacancies occurs in it, which can also contribute to the formation of complex defects [ 40 , 53 , 54 ]. In the past few years, a large number of such complex defects have been studied in detail in MgO, Al 2 O 3 , and Gd 3 Ga 5 O 12 crystals [ 55 , 56 , 57 , 58 , 59 , 60 ].…”
The ESR spectra of nanostructured samples of monoclinic ZrO2 irradiated by electrons with energies of 130 keV, 10 MeV, and by a beam of Xe ions (220 MeV) have been studied. It has been established that irradiation of samples with electrons (10 MeV) and ions leads to the formation of radiation-induced F+ centers in them. Thermal destruction of these centers is observed in the temperature range of 375–550 K for electron-irradiated and 500–700 K for ion-irradiated samples. It is shown that the decrease in the concentration of F+ centers is associated with the emptying of traps responsible for thermoluminescence (TL) peaks in the specified temperature range. In the samples irradiated with an ion beam, previously unidentified paramagnetic centers with g = 1.963 and 1.986 were found, the formation of which is likely to involve Zr3+ ions and oxygen vacancies. Thermal destruction of these centers occurs in the temperature range from 500 to 873 K.
“…It is also known that when ZrO 2 is irradiated with ions with an energy above the threshold, an intense generation of anion vacancies occurs in it, which can also contribute to the formation of complex defects [ 40 , 53 , 54 ]. In the past few years, a large number of such complex defects have been studied in detail in MgO, Al 2 O 3 , and Gd 3 Ga 5 O 12 crystals [ 55 , 56 , 57 , 58 , 59 , 60 ].…”
The ESR spectra of nanostructured samples of monoclinic ZrO2 irradiated by electrons with energies of 130 keV, 10 MeV, and by a beam of Xe ions (220 MeV) have been studied. It has been established that irradiation of samples with electrons (10 MeV) and ions leads to the formation of radiation-induced F+ centers in them. Thermal destruction of these centers is observed in the temperature range of 375–550 K for electron-irradiated and 500–700 K for ion-irradiated samples. It is shown that the decrease in the concentration of F+ centers is associated with the emptying of traps responsible for thermoluminescence (TL) peaks in the specified temperature range. In the samples irradiated with an ion beam, previously unidentified paramagnetic centers with g = 1.963 and 1.986 were found, the formation of which is likely to involve Zr3+ ions and oxygen vacancies. Thermal destruction of these centers occurs in the temperature range from 500 to 873 K.
“…Karipbayev et al presented a study of the optical, structural, and mechanical properties of Gd 3 Ga 5 O 12 single crystals irradiated by 84 Kr þ ions. [6] The observed changes are ascribed to structural disturbances caused by depletion of the surface layer and an increase in the number of displaced atoms, accompanied by an increase in the crystal lattice parameter. C. Barone et al combined measurements of broadband optical spectroscopy (10 meV to 6 eV), electrical resistivity and Hall effect to study the effects of gamma irradiation on electronic and optical properties of Ga-doped ZnO thin films.…”
“…Focusing on GGG samples that possess a very strong ability to resist color center formation, a series of absorption bands at 275, 306, and 313 nm in the UV region below 400 nm associated with electronic transitions in Gd 3+ are assigned to 8 S 7/2 → 6 D j , 8 S 7/2 → 6 I j , and 8 S 7/2 → 6 P j , respectively. [66] In addition to an overall increase in absorbance, the fundamental absorption edge red-shifts by 20-35 nm to the long-wavelength part of the spectra (UV-vis) after Xe 35+ irradiation with increasing fluence, which is caused by an irradiation-induced structural disorder in the surface layer. Utilizing the Kubelka-Munk function to fit (αhυ) 2 versus the photon energy (hυ) extracted from the absorption band spectrum (αhv = A(hv − E g ) 1/2 ), [67][68][69][70] it is evidenced that the bandgap width has been reduced by extrapolating this linear region onto the x-axis, which is dependent on increasing fluences of Xe 35+ onto both garnets.…”
Section: Bandgap Adjustment and Photoluminescence Emissionmentioning
The susceptibility to irradiation-induced damage, the fundamental mechanism of the relaxation kinetics, and the corresponding recrystallization effect related to the cation radius ratio are comprehensively investigated for Y 3 Al 5 O 12 and Gd 3 Ga 5 O 12 garnet crystals under 645 MeV Xe 35+ irradiation with different fluences of 5 × 10 11 -3 × 10 12 ions cm −2 . Regarding different lattice distortion and swelling levels, the observed microstructure transformations to disordered and amorphous phases, and corresponding hillock dimensions, consistently confirm that Gd 3 Ga 5 O 12 has a higher susceptibility to radiation damage than Y 3 Al 5 O 12 . Combined with iTS model calculations, although Y 3 Al 5 O 12 has higher atomic temperature and energy deposition than Gd 3 Ga 5 O 12 under the same ion velocity and electronic energy loss, the relatively high thermal conductivity and specific heat coefficient of Y 3 Al 5 O 12 crystals enhance the conduction and dissipation of deposition energy, and Gd 3 Ga 5 O 12 , with a higher cation-radius-ratio (r A /r B ), is more easily damaged to amorphous phase due to the less favorable kinetics of ordering and recovery of a melted track region to the crystalline phase. Additionally, the significant bandgap modification in spectral ranges of 5.88-6.75 eV for Y 3 Al 5 O 12 and 4.83-5.41 eV for Gd 3 Ga 5 O 12 , and the enhancement of defect-assisted-related luminescence are achieved, providing a basis to design novel optoelectronic devices in microelectronics fields.
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