Oxygen-vacancy donor-electron center in Y3Al5O12 garnet crystals: Electron paramagnetic resonance and dielectric spectroscopy study

The F+ center consisting of an electron trapped at an oxygen vacancy (VO) was investigated in oxygen deficient Y3Al5O12 (YAG) garnet crystals by electron paramagnetic resonance (EPR) techniques. The measurements were performed in the wide temperature interval 5–450 K and the frequency range 9.4–350...

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Veröffentlicht in:Physical review. B 2020-01, Vol.101 (2), p.1
Hauptverfasser: Laguta, V, Buryi, M, Arhipov, P, Sidletskiy, O, Laguta, O, Brik, M G, Nikl, M
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Buryi, M
Arhipov, P
Sidletskiy, O
Laguta, O
Brik, M G
Nikl, M
description The F+ center consisting of an electron trapped at an oxygen vacancy (VO) was investigated in oxygen deficient Y3Al5O12 (YAG) garnet crystals by electron paramagnetic resonance (EPR) techniques. The measurements were performed in the wide temperature interval 5–450 K and the frequency range 9.4–350 GHz using both the conventional continuous-wave and pulse EPR experiments. Pulse electron-nuclear double resonance was applied to resolve the hyperfine interaction of the trapped electron with surrounding nuclei. The measurements show that at low temperatures, T 200 K, we observed delocalization of the F+-center electron into the conduction band with the activation energy about 0.4–0.5 eV that resulted in substantial narrowing of the EPR spectral line with simultaneous change of its shape from Gaussian to Lorentzian due to disappearance of the Fermi contact hyperfine field at Al27 and Y89 nuclei. Such temperature behavior of the F+-center electron in YAG is completely similar to behavior of a donor electron in a semiconductor. Our findings are further supported by measurements of the conductivity and dielectric properties. In particular, these data show that the electrons in the conduction band are not homogeneously distributed in the crystal: There are highly conductive regions separated by poorly conductive dielectric layers. This leads to the so-called Maxwell-Wagner dielectric relaxation with huge apparent dielectric constant at low frequencies. This paper reports an observation of a donorlike behavior of an F+ center in wide band-gap insulating crystals.
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The measurements were performed in the wide temperature interval 5–450 K and the frequency range 9.4–350 GHz using both the conventional continuous-wave and pulse EPR experiments. Pulse electron-nuclear double resonance was applied to resolve the hyperfine interaction of the trapped electron with surrounding nuclei. The measurements show that at low temperatures, T&lt;50 K, the EPR spectrum of the F+ center is anisotropic with g factors in the range 1.999–1.988 and originates from three magnetically inequivalent positions of the center in a garnet lattice. As the temperature increases, the EPR spectrum becomes isotropic suggesting a motional averaging of the anisotropy due to motion of the F+-center electron between neighboring oxygen vacancies. With further increase of temperature up to T &gt; 200 K, we observed delocalization of the F+-center electron into the conduction band with the activation energy about 0.4–0.5 eV that resulted in substantial narrowing of the EPR spectral line with simultaneous change of its shape from Gaussian to Lorentzian due to disappearance of the Fermi contact hyperfine field at Al27 and Y89 nuclei. Such temperature behavior of the F+-center electron in YAG is completely similar to behavior of a donor electron in a semiconductor. Our findings are further supported by measurements of the conductivity and dielectric properties. In particular, these data show that the electrons in the conduction band are not homogeneously distributed in the crystal: There are highly conductive regions separated by poorly conductive dielectric layers. This leads to the so-called Maxwell-Wagner dielectric relaxation with huge apparent dielectric constant at low frequencies. 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With further increase of temperature up to T &gt; 200 K, we observed delocalization of the F+-center electron into the conduction band with the activation energy about 0.4–0.5 eV that resulted in substantial narrowing of the EPR spectral line with simultaneous change of its shape from Gaussian to Lorentzian due to disappearance of the Fermi contact hyperfine field at Al27 and Y89 nuclei. Such temperature behavior of the F+-center electron in YAG is completely similar to behavior of a donor electron in a semiconductor. Our findings are further supported by measurements of the conductivity and dielectric properties. In particular, these data show that the electrons in the conduction band are not homogeneously distributed in the crystal: There are highly conductive regions separated by poorly conductive dielectric layers. This leads to the so-called Maxwell-Wagner dielectric relaxation with huge apparent dielectric constant at low frequencies. 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The measurements were performed in the wide temperature interval 5–450 K and the frequency range 9.4–350 GHz using both the conventional continuous-wave and pulse EPR experiments. Pulse electron-nuclear double resonance was applied to resolve the hyperfine interaction of the trapped electron with surrounding nuclei. The measurements show that at low temperatures, T&lt;50 K, the EPR spectrum of the F+ center is anisotropic with g factors in the range 1.999–1.988 and originates from three magnetically inequivalent positions of the center in a garnet lattice. As the temperature increases, the EPR spectrum becomes isotropic suggesting a motional averaging of the anisotropy due to motion of the F+-center electron between neighboring oxygen vacancies. With further increase of temperature up to T &gt; 200 K, we observed delocalization of the F+-center electron into the conduction band with the activation energy about 0.4–0.5 eV that resulted in substantial narrowing of the EPR spectral line with simultaneous change of its shape from Gaussian to Lorentzian due to disappearance of the Fermi contact hyperfine field at Al27 and Y89 nuclei. Such temperature behavior of the F+-center electron in YAG is completely similar to behavior of a donor electron in a semiconductor. Our findings are further supported by measurements of the conductivity and dielectric properties. In particular, these data show that the electrons in the conduction band are not homogeneously distributed in the crystal: There are highly conductive regions separated by poorly conductive dielectric layers. This leads to the so-called Maxwell-Wagner dielectric relaxation with huge apparent dielectric constant at low frequencies. This paper reports an observation of a donorlike behavior of an F+ center in wide band-gap insulating crystals.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevB.101.024106</doi></addata></record>
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source American Physical Society Journals
subjects Anisotropy
Conduction bands
Conductivity
Continuous radiation
Crystals
Dielectric properties
Dielectric relaxation
Electron paramagnetic resonance
Electrons
Frequency ranges
Hyperfine structure
Lattice vacancies
Line spectra
Low temperature
Nuclei (nuclear physics)
Oxygen
Spectrum analysis
Temperature
Yttrium-aluminum garnet
title Oxygen-vacancy donor-electron center in Y3Al5O12 garnet crystals: Electron paramagnetic resonance and dielectric spectroscopy study
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