KnE Materials Science | Sino-Russian ASRTU Conference Alternative Energy: Materials, Technologies, and Devices | pages: 98-108

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1. Introduction

Nowadays, study of aluminum–magnesium spinel (AMS) is carried out by many laboratories due to the fact that spinel is of practical interest for fiber optic temperature sensors, tunable solid-state lasers, matrices, manufacturing optical nanodevices, matrices for carrying out transmutation transformations, and filler material for disposal of radioactive waste [1–4]. Transparent ceramics of aluminum–magnesium spinel doped with ions of transition metals and rare earths can be used as radiation energy converters [5–7]. The polycrystalline structure of the magnesia spinel is optically isotropic. AMS undergoes no polymorphic transformations and, hence, is devoid of any thermally induced phase changes. Such ceramics have wide optical window (0.2–5.5 μm), high radiation and corrosion resistance, as well as mechanical strength, which is of great interest for many practical applications including alternative energy [8,9].

AMS belongs to the class of binary AB 2 O 4 oxides (A-bivalent, B-trivalent cation) having cubic system. Single cubic unit cell contains 64 tetra- and 32 octahedral cationic positions. An important characteristic of spinel structure is cations positions distribution. Normal and inverse spinel structures are distinguished based on ions distribution in the cation sublattice [10]. An intermediate case is also distinguished, characterized by a partial inversion of the structure [11,12]. It is known that degree of reversal in AMS structure increases together with rising of synthesis temperature and heat treatment at 1000 K [13]. Synthetic AMS always has replacement defects (so called anti-site defects – ADs) due to having low energy of formation and harsh conditions of synthesis (high temperature and pressure) [14,15].

Impact of fast neutrons and gamma radiation on AMS leads to changes in cations structural positions. Such defects are characterized by an aluminum ion in the tetrahedral position of magnesium [Al 3+ ] Mg and vice versa [16,17]. Anion vacancies are formed together with cation defects in MgAl 2 O 4 . The presence of the F and F + type centers was confirmed by the studies of thermochemically sintered polycrystalline MgAl 2 O 4 [18] and investigation of single crystalline AMS irradiated by neutrons [19]. Activation of AMS and ceramics by ions of such transition 3d elements as Mn, Ti, Cr, Fe, etc. results in wide spectral range luminescence. At the same time, it should be noted that effect of radiation-induced substitution defects on spinel optical properties has not been sufficiently studied.

The aim of this work is to study formation and features of radiation-induced anti-site defects, as well as impurity ions Mn 2+ and Cr 3+ as factors influenced on the optical properties of AMS transparent ceramics.

2. Methods

Nanopowder of MgAl 2 O 4 synthesized by Pechini method with additional heat treatment in liquid melt of inactive salt matrix with addition of 1 wt. % LiF was subjected to uniaxial hot pressing at 35 MPa with 1550 C soaking temperature for 1 h. Obtained ceramics were polished to decrease dispersion at the surface.

Optical absorbance spectrum was registered using Perkin Elmer Lambda 35 spectrophotometer. Absorbance centers concentration was calculated by means of Smakula–Dexter formula n = 0.87*10 17 (a 0 /(a 20 +2) 2 ) ( Δ E/f)*k 0 , here n is amount of absorbance centers, a 0 is refractivity index around absorbance maximum (1.72 of single crystalline AMS), Δ E is full width at half maximum, f is oscillator power (taken as 1), k 0 is absorption constant at the maximum position.

Photoluminescence (PL) and Raman scattering spectra (Raman spectra) were recorded on a LabRam HR 800 Evolution spectrometer with an Olympus BX–FM microscope (50x and 100x lenses) with excitation by laser radiation with an energy of 2.54 eV (Ar-laser, radiation power on the sample 1.5 mW) and recording the Peltier-cooled CCD detector using a diffraction grating 600 ppm/mm at room temperature. The spectral resolution in the Raman scattering region of the spinel was 6–8 cm -1 , in the region of registration of the PL of chromium ions, 0.01 nm. Position of the RNC peaks is determined after adjusting the baseline by approximating the spectral profile with Voigt functions using LabspecⓇ software. A sample of natural spinel (KOS-II) was used as an object for comparing the spectra of Raman and PL of transparent ceramics.

Irradiation by fast electrons was performed by means of UERL-10C linear electron accelerator at Ural Federal University (E = 10 MeV, fluence 10 17 e/cm 2 ). Samples were placed in a chamber with water cooling. Temperature of samples during irradiation did not exceed 70 C.

3. Results and Discussion

Optical absorbance

Initial AMS ceramics has high degree of transparency in wide spectral range. Great increase in optical absorption (OA) at photon energies above 6 eV is due to absorption in fundamental absorption edge range of material – E g = 7.8 eV for single crystal (Figure 1(a)). Irradiation of ceramics by 10 MeV electron beam results in absorption growth in wide spectral range from 1.5 to 6 eV. It is known that 4.75 and 5.3 eV maxima can be attributed to F + and F-centers in aluminum magnesium spinel [18,19]. Ones in 2.7 and 3.2 are due to extrinsic cation defects present in sample [20]. It is to be noted that there is no consensus about nature of 3.5–4.2 band in literature. According to researchers [20,21], in the range from 3.5 to 4.2 eV, the absorption is caused by the formation of ADs with subsequent localization of charge carriers. However, there are works that connect the latter with anion dimers, that is, two closely situated oxygen vacancies – F 2 -centers. [22]. Correlation of observed OA and Raman spectra supports ADs hypothesis. Origin of intensive band 6.2 eV requires additional investigations.

Figure 1

Optical absorption spectra of initial and irradiated AMS sample (a). The difference between optical absorption spectra (b). Solid line – resulting curve, dash line – Gaussians.

fig-1.jpg

Concentrations of indicated defects were calculated using Smakula–Dexter formula according to experimental spectra (Table 1). Centers of F + , F-type and unknown band have the highest concentration. The formation of V-type centers upon irradiation with accelerated electrons is caused by the formation of Frenkel defects of the cation sublattice by the mechanism of shock displacement with the formation of Al 3+ and Mg 2+ interstitials. Electron and hole centers can exist in ADs as a result of electron or hole localization at [Al] +Mg or [Mg] -Al , accordingly with charge compensation. Centers of F + and F-type are formed due to dislodging of oxygen atom from its sublattice followed by capture of one or two electrons, respectively.

Table 1

The concentration of defects obtained by Smakula–Dexter formula.


Location, eV 2.15 2.7 3.1 3.75 4.7 5.3 6.2
n*10 16 1,2 1,4 1,9 2,45 5,9 6,5 8,7
Type of centrums V V V Electron or hole at ADs F + F ?

Raman spectra

Raman spectra of initial and irradiated ceramics, as well as single crystalline of natural spinel are shown in Figure 2. In synthesized ceramics, as in natural spinel, four of the five vibrational modes (A 1g , E g , F 2g (3), F 2g (1)) are observed, which are active according to the group theoretical analysis in Raman scattering of spinel with a normal cation distribution over the positions. Energy values of vibrational modes (Table 2) in synthesized and natural spinel are close to each other and consistent with literature data for MgAl 2 O 4 [23]. Mode with E g 407–408 cm -1 has the highest intensity. Low-intensity peak F 2g (2) at 562 cm -1 is not stationary.

Figure 2

Raman scattering spectra of initial ceramics, irradiated one, and natural spinel. Dash lines – modes characteristic for natural spinel with normal structure.

fig-2.jpg
Table 2

Vibrational modes in the Raman spectra of irradiated and initial ceramics of AMS, natural spinel. Comparison of the obtained results with the literature data for a synthetic single crystal MgAl 2 O 4 (sh – shoulder; l/i – low intensity maxima; * – modes, associated in the literature with the inversion of the spinel structure).


Sample The energy of vibrational modes of different type symmetry, cm -1
F 2g (1) E g E g F 2g (2) F 2g (2) F 2g (3) A 1g A 1g
Initial 305 366(sh) *381(sh) 406 669 *722 766
e-beam (exposed by 10MeV electrons) 304 358(sh) *380(sh) 408 669 *721 766
KOS-II 312 * 385(sh) 407 554(l/i) 666 * 715(l/i) 767
MgAl 2 O 4[23] 308 *375(sh) 408 *493 562 670 *720 768

Several additional maxima in Raman spectra of synthesized transparent ceramics are observed as well as broadening and intensity decrease of fundamental vibrational modes most explicitly expressed for the E g mode. Measured width of this peak changes from 8 cm -1 in natural spinel to 35 cm -1 in synthesized ceramics. These spectral features of transparent ceramics are associated with reversal of the structure (presence of ADs) [23,24].

Shape of Raman basic mode (E g ) in irradiated ceramics caused by formation of additional ADs is observed. Electrons with 10 MeV energy colliding with cation knock it out of sublattice to interstice or an adjacent cation position. Thus, the results of synthesized AMS ceramics Raman analysis allow concluding that there is a substantial disorder associated with reversal of the structure. Irradiation by accelerated electrons leads to structural changes caused by formation of additional ADs.

Photoluminescence

Luminescence of natural spinel and AMS ceramics under 2.54 eV excitation is presented in Figure 3. Zero-phonon lines of chromium (R 1 , R 2 ) radiative 2 E 4 A 2 transitions, phonon wing in Stokes region (R-PSB), and region of zero-phonon N-lines associated with disorder of chromium environment are observed in luminescence spectrum of natural spinel (KOS-II) [25,16].

Figure 3

Luminescence spectra of initial ceramics, irradiated one, and natural spinel, RT.

fig-3.jpg

Synthesized ceramics have broadened bands associated with luminescence of Cr ions in spinel matrix. A halo in 1.6–2 eV range is observed in spectra of spinel ceramics irradiated by electrons in addition to indicated luminescence. Irradiation by high-energy electrons leads to formation of ADs as it was shown in OA and Raman spectra. Growth of cation disordering leads to change of crystalline field local strength around Cr ion impurity. Such local distortions of matrix near chromium ion result in the luminescence bands broadening. It is noted that nonstoichiometry of AMS can have a significant effect on optical properties along with inversion of the structure [18].

On the luminescence spectra, an additional maximum of 2.4 eV caused by the presence of impurity Mn 2+ in the tetrahedral position of Mg 2+ is observed. There were no obvious changes in shape or intensity of the observed signal after irradiation.

Synthesized spinel has increased ADs concentration compared to natural crystals. On the other hand, irradiation by accelerated electrons also results in increase of ADs concentration. Thus, observed correlation between OA spectra (rise of absorption band in 3.7 eV), RS (decrease of main oscillation mode intensity in irradiated ceramics and redistribution of intensities of oscillation modes derived from deconvolution), and PL (widening of Cr 3+ spectral lines) is due to effect of ADs on Cr 3+ ions in octahedral aluminum cation position. Therefore, extrinsic cation center in transparent ceramics of aluminum magnesium spinel can act as indicator of ADs presence in cation sublattice.

4. Conclusion

Transparent MgAl 2 O 4 ceramics were synthesized. Characterization of the samples was performed by optical absorption, Raman scattering, and photoluminescence methods. Relatively high stability to electron beams allows using transparent AMS ceramics as a functional material in alternative energy devices operating under extreme conditions.

Irradiation of aluminum magnesium spinel transparent ceramic by 10 MeV electrons results in formation of optically active defects in wide spectral range. Analysis of absorption, Raman scattering, and luminescence spectra allowed finding that irradiated samples have F + , F-, and V-type anion defects. These defects in spinel are identified by the methods of OA and Raman scattering by the presence and broadening of characteristic bands.

It was found that effect of `ionic mixing' in cation sublattice took place under 10 MeV electron beam irradiation. This effect is associated with the formation of point anti-site defects [Al] Mg and [Mg] Al . There were no significant changes in the characteristic luminescence band of extrinsic Mn 2+ ions according to spectroscopy data. It was shown that radiation-stimulated anti-site defects led to the formation of the halo induced by the growth of disordering in cation sublattice near the Cr 3+ ions in the luminescence range 1.6–2 eV. Optical properties of Cr 3+ ions can be utilized as indicators of cation disordering in the transparent ceramics structure.

Acknowledgement

Author Yu. V. S. would like to thank the RFBR for supporting (project No. 18-05-01153).

Funding

The work has been done as a part of the government task (№3.1485.2017/4.6) of the Ministry of Education and Science of the Russian Federation.

References

1 

Aizawa H., Ohishi N., Ogawa S., Watanabe E., Katsumata T., Komuro S., Morikawa T., Toba E., Characteristics of chromium doped spinel crystals for a fiber-optic thermometer application, Review of Scientific Instruments, Year: 2002, Volume: 73, Issue: 8, Page: 3089 DOI: 10.1063/1.1491998

2 

Jouini A., Yoshikawa A., Brenier A., Fukuda T., Boulon G., Optical properties of transition metal ion-doped MgAl2O 4 spinel for laser application, Physica Status Solidi (c) – Current Topics in Solid State Physics, Year: 2007, Volume: 4, Issue: 3, Page: 1380-1383.

3 

Kishimoto N., Takeda Y., Umeda N., Gritsyna V. T., Lee C. G., Saito T., Metal nanocrystal formation in magnesium aluminate spinel and silicon dioxide with high-flux Cu- ions, Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, Year: 2000, Volume: 166, Page: 840-844.

4 

Konings R. J. M., Conrad R., Dassel G., Pijlgroms B. J., Somers J., Toscano E., The EFTTRA-T4 experiment on americium transmutation, Journal of Nuclear Materials, Year: 2000, Volume: 282, Issue: 2-3, Page: 159-170. DOI: 10.1016/S0022-3115(00)00411-6

5 

Nakagawa H., Ebisu K., Zhang M., Kitaura M., Luminescence properties and afterglow in spinel crystals doped with trivalent Tb ions, Journal of Luminescence, Year: 2003, Volume: 102-103, Page: 590-596. DOI: 10.1016/S0022-2313(02)00593-8

6 

Chen X. Y., Ma C., Zhang Z. J., Li X. X., Structure and photoluminescence study of porous red-emitting MgAl2O4:Eu3+ phosphor, Microporous and Mesoporous Materials, Year: 2009, Volume: 123, Issue: 1-3, Page: 202-208. DOI: 10.1016/j.micromeso.2009.04.002

7 

Hanamura E., Kawabe Y., Takashima H., Sato T., Tomita A., Optical properties of transition-metal doped spinels, Journal of Nonlinear Optical Physics & Materials, Year: 2003, Volume: 12, Issue: 4, Page: 467-473. DOI: 10.1142/S0218863503001584

8 

Rubat Du Merac M., Kleebe H.-J., Müller M. M., Reimanis I. E., Fifty years of research and development coming to fruition; Unraveling the complex interactions during processing of transparent magnesium aluminate (MgAl 2 O 4) spinel, Journal of the American Ceramic Society, Year: 2013, Volume: 96, Issue: 11, Page: 3341-3365. DOI: 10.1111/jace.12637

9 

Clinard F. W.Jr., Ceramics for fusion applications, Ceramics International, Year: 1987, Volume: 13, Issue: 2, Page: 69-75. DOI: 10.1016/0272-8842(87)90041-1

10 

Vest A., Solid State Chemistry. Theory and applications. Part 2, Year: 1988, MoscowMir. (in Russian

11 

Krupichka S., Pohomov A. S., Physics of Ferrites and Related Magnetic Oxides, Year: 1976, MoscowMir. (in Russian

12 

Chaschukhin I. P., Votyakov S. L., Shchapova Yu. U., Crystallochemistry of Chrome-spinels and Oxy-thermobarometry of Ultramafites of Folded Regions., Yekaterinburg, Institute of Geology and Geochemistry, Year: 2007, in Russian

13 

Andreozzi G. B., Princivalle F., Kinetics of cation ordering in synthetic MgAl2O4 spinel, American Mineralogist, Year: 2002, Volume: 87, Issue: 7, Page: 838-844. DOI: 10.2138/am-2002-0705

14 

White G. S., Jones R. V., Crawford J. H.Jr., Optical spectra of MgAl2O4 crystals exposed to ionizing radiation, Journal of Applied Physics, Year: 1982, Volume: 53, Issue: 1, Page: 265-270. DOI: 10.1063/1.331603

15 

Gilbert C. A., Smith R., Kenny S. D., Murphy S. T., Grimes R. W., Ball J. A., A theoretical study of intrinsic point defects and defect clusters in magnesium aluminate spinel, Journal of Physics: Condensed Matter, Year: 2009, Volume: 21, Issue: 27, Page: 275406 DOI: 10.1088/0953-8984/21/27/275406

16 

Skvortsova V., Mironova-Ulmane N., Ulmanis U., Neutron irradiation influence on magnesium aluminium spinel inversion, Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, Year: 2002, Volume: 191, Issue: 1-4, Page: 256-260. DOI: 10.1016/S0168-583X(02)00571-2

17 

White G. S., Jones R. V., Crawford J. H.Jr., Optical spectra of MgAl2O4 crystals exposed to ionizing radiation, Journal of Applied Physics, Year: 1982, Volume: 53, Issue: 1, Page: 265-270. DOI: 10.1063/1.331603

18 

Sawai S., Uchino T., Visible photoluminescence from MgAl2O4 spinel with cation disorder and oxygen vacancy, Journal of Applied Physics, Year: 2012, Volume: 112, Issue: 10,

19 

Ibarra A., Bravo D., Garcia M. A., Llopis J., Lopez F. J., Garner F. A., Dose dependence of neutron irradiation effects on MgAl2O4 spinels, Journal of Nuclear Materials, Year: 1998, Volume: 258-263, Page: 1902-1907. DOI: 10.1016/S0022-3115(98)00130-5

20 

Kazarinov Y., Kvatchadze V., Gritsyna V., Abramishvili M., Akhvlediani Z., Galustashvili M., Dekanozishvili G., Kalabegishvili T., Tavkhelidze V., Spectroscopic studies of defects in gamma- and neutron-irradiated magnesium aluminates spinel ceramics, Problems of Atomic Science and Technology, Year: 2017, Volume: 111, Issue: 5, Page: 8-13.

21 

Tyutyunik O. K., Moskvitin A. O., Kazarinov Y. G., Gritsyna V. T., Radioluminescence mechanism of magnesium aluminate spinel transparent ceramics, Functional Materials, Year: 2010, Volume: 17, Issue: 1, Page: 41-45.

22 

Costantini J.-M., Lelong G., Guillaumet M., Weber W. J., Takaki S., Yasuda K., Color-center production and recovery in electron-irradiated magnesium aluminate spinel and ceria, Journal of Physics: Condensed Matter, Year: 2016, Volume: 28, Issue: 32,

23 

D'Ippolito V., Andreozzi G. B., Bersani D., Lottici P. P., Raman fingerprint of chromate, aluminate and ferrite spinels, Journal of Raman Spectroscopy, Year: 2015, Volume: 46, Issue: 12, Page: 1255-1264. DOI: 10.1002/jrs.4764

24 

Cynn H., Anderson O. L., Nicol M., Effects of cation disordering in a natural MgAl2O4 spinel observed by rectangular parallelepiped ultrasonic resonance and Raman measurements, Pure and Applied Geophysics ( PAGEOPH ), Year: 1993, Volume: 141, Issue: 2-4, Page: 415-444. DOI: 10.1007/BF00998338

25 

Mikenda W., Preisinger A., N-lines in the luminescence spectra of Cr3+ -doped spinels (II) origins of N-lines, Journal of Luminescence, Year: 1981, Volume: 26, Issue: 1-2, Page: 67-83. DOI: 10.1016/0022-2313(81)90170-8

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