Photoluminescent and Scintillating Performance of Eu3+-Doped Boroaluminosilicate Glass Scintillators

In comparison with single crystal scintillators, glass scintillators are more promising materials for their benefits of easy preparation, low cost, controllable size, and large-scale manufacture. The emission of Eu3+ ion at 612 nm matches well with the photoelectric detector, making it suitable for the activator in glass scintillators. Therefore, the research on Eu3+ doped glass scintillators attract our attention. The photoluminescent and scintillating properties of Eu3+-activated boroaluminosilicate glass scintillators prepared by the conventional melt-quenching method were investigated in this work. The glass samples present good internal quantum yield. Under X-ray radiation, the optimal sample reveals high X-ray excited luminesce (XEL), and its integrated intensity of XEL is 22.7% of that of commercial crystal scintillator Bi4Ge3O12. Furthermore, the optimal specimen possesses a spatial resolution of 14 lp/mm in X-ray imaging. These results suggest that Eu3+-doped boroaluminosilicate glass is expected to be applied in X-ray imaging.


Introduction
X-ray is regarded as an excellent radiation source due to its short wavelength and strong penetration and is widely used in structural analysis, perspective imaging, constituent analysis, and other fields. Perspective imaging technology can be applied in medical diagnosis, industrial nondestructive inspection, national security checks, and so on. Scintillators, an important component in perspective imaging technology, absorb the transmitted X-rays and convert them into visible light, thus recording the structural information of the imaging objects. Currently, scintillator materials used in perspective imaging systems are mostly single crystal scintillators, like Bi 4 Ge 3 O 12 (BGO), (Lu,Y) 2 SiO 5 :Ce, and-CsI:Tl [1][2][3][4][5]. High production cost, complex production process, and limited product size confine the wide application of single crystal scintillators [6,7]. Therefore, many new scintillators have been developed continuously. Among them, glass scintillators stand out because of their high transmittance, strong plasticity, and diverse composition [8][9][10].
Glass scintillators consist of glass hosts and luminescent centers. The glass hosts determine the basic physical properties of glass scintillators and provide an appropriate crystal field environment for luminescent centers. Silicate glasses have high mechanical strength and excellent physical-chemical stability. However, the solubility of rare-earth ions in silicate glasses is not ideal, and the melting point is high. Borosilicate glasses can be obtained by adding the proper amount of boron oxide into silicate glasses. Compared with silicate glasses, the melting point of borosilicate glasses decreases obviously, and the solubility of rare-earth ions increases effectively [11]. The addition of alumina makes the glass structure tighter. The addition of yttrium oxide can improve the density and X-ray absorption capacity of the glasses [12]. Therefore, in this paper, SiO 2 -B 2 O 3 -Al 2 O 3 -Y 2 O 3 glass was selected as a glass host for glass scintillators.
Generally, in glasses, Eu 3+ will occupy an asymmetric crystal field environment. Its strongest emission peak locates at 612 nm ( 5 D 0 to 7 F 2 ), and matches well with the photoelectric detector. Currently, some works of glass scintillators with Eu 3+ doping have been reported [13]. Eu 3+ doped tellurite glass scintillators were reported by Huang et al. [14]. The intergrated intensity of X-ray excited luminesce (XEL) of the optimal sample reached 6% of that of BGO, similarly thereafter. Wantana et al. doped Eu 3+ into borotungstate glasses and borosilicate glasses as luminescent centers, and the XEL intensity was 8.87% and 13% [15,16], respectively. Guo et al. reported Eu 3+ -doped boroaluminate glass scintillators and the maximum XEL intensity was 18.4% [17]. The performance of Eu 3+ -doped glass scintillators needs to be further improved. In addition, there are no reports on Eu 3+ -doped glass scintillators for X-ray perspective imaging technology.
In this work, a series of Eu 3+ doped borosilicate glasses with the addition of aluminium oxide and yttrium oxide was fabricated. Transmittances of samples are about 80% at 600 nm, and the average lifetimes of the 5 D 0 state of Eu 3+ are about 1.7 ms. The optimal sample doped with 8 mol% Eu 3+ exhibited the highest integrated XEL intensity (22.7% of BGO). What is more, for X-ray imaging, its spatial resolution reaches up to 14 lp/mm. Results suggest that boroaluminosilicate glass scintillators doped with Eu 3+ may have potential use in X-ray imaging. with 99.99% purity, were weighed by stoichiometric proportions and mixed uniformly in an agate mortar. The mixture was sintered for 1 h at 1500 • C. Then, the melt was pressed using a heated steel plate after being quickly poured over a stainless-steel plate that had been preheated to 300 • C. After cooling to room temperature, these glass samples were put in the furnace and annealed at 800 • C for 3 h to reduce stress. Ultimately, all glass specimens were cut and polished to 2 mm for the following characterization.

Characterization
X-ray diffraction (XRD) patterns of samples were gauged by Rigaku MiniFlex/600 XRD (Tokyo, Japan, CuK α1 , λ = 0.154056 nm) equipment. Fourier transforms infrared (FT-IR) spectra was characterized by a NEXUS 670 spectrophotometer (Thermo Nicolet, Waltham, MA, USA). U-3900 spectrophotometer (Hitachi, Tokyo, Japan) was used to test transmission spectra. Excitation and emission spectra, internal quantum efficiency (IQE), and decay curves were investigated with a FS5 spectrofluorometer (Edinburgh Instruments, Livingston, UK) equipped with a 150 W Xe lamp. XEL spectra were accomplished on an OmniFluo960-X-ray scintillator fluorescence spectrometer (Zolix Instruments, Beijing, China). Pictures of X-ray imaging were taken by a Canon camera (EOS600D).  groups [12]. The absorption peak at 985 cm −1 is attributed to the antisymmetric stretching vibration of Si-O in [SiO 4 ] tetrahedra [18]. Furthermore, the asymmetric stretching vibration of B-O of [BO 3 ] units brings on the absorption bands located at 1243 and 1375 cm −1 [20]. The two curves are relatively similar and have the same absorption peak, indicating that the incorporation of Eu 3+ does not impact glasses structures obviously.

Structural Characters
vibration of Si-O in [SiO4] tetrahedra [18]. Furthermore, the asymmetric stretching vibration of B-O of [BO3] units brings on the absorption bands located at 1243 and 1375 cm −1 [20]. The two curves are relatively similar and have the same absorption peak, indicating that the incorporation of Eu 3+ does not impact glasses structures obviously.  Figure 2 demonstrates the transmittance spectra of the SBAY host and SBAY:xEu specimens. Absorption peaks at 362, 378, 395, 414, 465, 531, and 579 nm are observed, which correspond to characteristic transitions from 7 F0 to 5 D4, 5 G3, 5 L6, 5 D3, 5 D2, 5 D1, and 5 D0 of Eu 3+ , respectively. Importantly, transmittances of all Eu 3+ -doped specimens are about 80% at 600 nm. As the concentration of Eu 3+ ions rises, the intensities of all absorption peaks also increase. In addition, the absorption edge also exhibits a significant red shift with increasing Eu 3+ content. Such phenomenon might be attributed to new unoccupied electron states in the gap below the conduction band edge due to the substitution of Y2O3 by Eu2O3 [14,21,22].   Figure 2 demonstrates the transmittance spectra of the SBAY host and SBAY:xEu specimens. Absorption peaks at 362, 378, 395, 414, 465, 531, and 579 nm are observed, which correspond to characteristic transitions from 7 F 0 to 5 D 4 , 5 G 3 , 5 L 6 , 5 D 3 , 5 D 2 , 5 D 1 , and 5 D 0 of Eu 3+ , respectively. Importantly, transmittances of all Eu 3+ -doped specimens are about 80% at 600 nm. As the concentration of Eu 3+ ions rises, the intensities of all absorption peaks also increase. In addition, the absorption edge also exhibits a significant red shift with increasing Eu 3+ content. Such phenomenon might be attributed to new unoccupied electron states in the gap below the conduction band edge due to the substitution of Y 2 O 3 by Eu 2 O 3 [14,21,22].
vibration of Si-O in [SiO4] tetrahedra [18]. Furthermore, the asymmetric stretching vibration of B-O of [BO3] units brings on the absorption bands located at 1243 and 1375 cm −1 [20]. The two curves are relatively similar and have the same absorption peak, indicating that the incorporation of Eu 3+ does not impact glasses structures obviously.  Figure 2 demonstrates the transmittance spectra of the SBAY host and SBAY:xEu specimens. Absorption peaks at 362, 378, 395, 414, 465, 531, and 579 nm are observed, which correspond to characteristic transitions from 7 F0 to 5 D4, 5 G3, 5 L6, 5 D3, 5 D2, 5 D1, and 5 D0 of Eu 3+ , respectively. Importantly, transmittances of all Eu 3+ -doped specimens are about 80% at 600 nm. As the concentration of Eu 3+ ions rises, the intensities of all absorption peaks also increase. In addition, the absorption edge also exhibits a significant red shift with increasing Eu 3+ content. Such phenomenon might be attributed to new unoccupied electron states in the gap below the conduction band edge due to the substitution of Y2O3 by Eu2O3 [14,21,22].  On the basis of Beer-Lambert law (I = I 0 e −αd , here I and I 0 are the intensities of the transmitted light and incident light, respectively, d is the thickness and α is absorption coefficient of samples), the equation of αd = −ln T can be obtained. The equation α 2 = B(hν − E g ) (B is a constant coefficient, hν is the energy of incident photons and E g is band gap energy) is applied for the direct band material [23]. So, E g value of the SBAY host is estimated to be 3.55 eV.

Photoluminescent Properties
The photoluminescent emission (PL) and photoluminescent excitation (PLE) spectra of SBAY:xEu specimens are displayed in Figure 3a,b, respectively. Excited by 464 nm, five characteristic emission peaks of Eu 3+ at 579, 593, 612, 653, and 700 nm correspond to transitions from 5 D 0 to 7 F J (J = 0-4) [17,24], respectively. Thereinto, the 5 D 0 → 7 F 1 (593 nm) transition of Eu 3+ is a magnetic dipole transition. It is not affected by the environment of Eu 3+ because of the selection rule (∆J = 1). Furthermore, the transition of 5 D 0 → 7 F 2 of Eu 3+ at 612 nm is an electric dipole transition [16], which is strongly dependent on the symmetry of the environmental structure of Eu 3+ . As demonstrated in Figure 3, the intensity of the emission peak at 612 nm is the strongest. Therefore, Eu 3+ ions located at an asymmetric crystal field environment. In order to intuitively get the symmetry of the environment of Eu 3+ , the integral intensity ratio (R) is calculated by the following formula [25], where I ED is luminescent intensity of electric dipole transition, and I MD is luminescent intensity of magnetic dipole transition. The values of R of SBAY:xEu are listed in Table 1.
The values of R decrease slightly with increasing Eu 3+ concentration, indicating that environmental structure of Eu 3+ becomes more ordered slightly.
Materials 2023, 16, x FOR PEER REVIEW 4 of 11 energy) is applied for the direct band material [23]. So, Eg value of the SBAY host is estimated to be 3.55 eV.

Photoluminescent Properties
The photoluminescent emission (PL) and photoluminescent excitation (PLE) spectra of SBAY:xEu specimens are displayed in Figure 3a,b, respectively. Excited by 464 nm, five characteristic emission peaks of Eu 3+ at 579, 593, 612, 653, and 700 nm correspond to transitions from 5 D0 to 7 FJ (J = 0-4) [17,24], respectively. Thereinto, the 5 D0→ 7 F1 (593 nm) transition of Eu 3+ is a magnetic dipole transition. It is not affected by the environment of Eu 3+ because of the selection rule (J = 1). Furthermore, the transition of 5 D0→ 7 F2 of Eu 3+ at 612 nm is an electric dipole transition [16], which is strongly dependent on the symmetry of the environmental structure of Eu 3+ . As demonstrated in Figure 3, the intensity of the emission peak at 612 nm is the strongest. Therefore, Eu 3+ ions located at an asymmetric crystal field environment. In order to intuitively get the symmetry of the environment of Eu 3+ , the integral intensity ratio (R) is calculated by the following formula [25], where IED is luminescent intensity of electric dipole transition, and IMD is luminescent intensity of magnetic dipole transition. The values of R of SBAY:xEu are listed in Table 1.
Both PL and PLE spectra show that the luminescent intensity of Eu 3+ increases first and then decrease with increasing Eu 3+ concentration, and the optimal sample is SBAY:6Eu. The reason is that with increasing concentration of Eu 3+ , the concentration quenching phenomenon occurs because the possibility of non-radiation transition is promoted. The values of IQE were measured to evaluate the optical performance of glass samples and computed by the equation followed [28], where L specimen is the emission intensity of specimen, E reference and E specimen are excitation intensities with BaSO 4 and specimen, respectively. The corresponding spectra are demonstrated in Figure 4 and the maximum IQE value is 81.5% for SBAY:2Eu, which is higher than most Eu 3+ -doped glasses [26]. Furthermore, the IQE value of SBAY:6Eu sample is 67.5%, as listed in Table 1.
where Lspecimen is the emission intensity of specimen, Ereference and Especimen are excitation intensities with BaSO4 and specimen, respectively. The corresponding spectra are demonstrated in Figure 4 and the maximum IQE value is 81.5% for SBAY:2Eu, which is higher than most Eu 3+ -doped glasses [26]. Furthermore, the IQE value of SBAY:6Eu sample is 67.5%, as listed in Table 1.
where It stands for the emission intensity of SBAY:xEu samples at t time. As shown in Table 1, as the content of Eu 3+ increases, the average lifetimes are 1.71, 1.64, 1.71, and 1.43 ms, respectively.   [17,27], where I t stands for the emission intensity of SBAY:xEu samples at t time. As shown in

Scintillating Properties
The outstanding transparency, high IQE, pure red emission, and suitable lifetime indicate that Eu 3+ -doped boroaluminosilicate glasses are promising scintillators for X-ray imaging. XEL spectra of SBAY:xEu and BGO are measured to excavate the scintillating performance, as displayed in Figure 6. Peaks at 579, 593, 612, 653, and 701 nm are assigned 5 7 3+

Scintillating Properties
The outstanding transparency, high IQE, pure red emission, and suitable lifetime indicate that Eu 3+ -doped boroaluminosilicate glasses are promising scintillators for X-ray imaging. XEL spectra of SBAY:xEu and BGO are measured to excavate the scintillating performance, as displayed in Figure 6. Peaks at 579, 593, 612, 653, and 701 nm are assigned to transitions of 5 D 0 → 7 F J (J = 0-4) of Eu 3+ , which are similar to PL spectra. Integrated XEL intensities of samples enhance as increasing concentration of Eu 3+ . The highest integrated XEL intensity is 22.7% (from SBAY:8Eu) of that of BGO. It is higher than other Eu 3+ -doped borate and germanate glass scintillators listed in Table 2.

Scintillating Properties
The outstanding transparency, high IQE, pure red emission, and suitable lifetime indicate that Eu 3+ -doped boroaluminosilicate glasses are promising scintillators for X-ray imaging. XEL spectra of SBAY:xEu and BGO are measured to excavate the scintillating performance, as displayed in Figure 6. Peaks at 579, 593, 612, 653, and 701 nm are assigned to transitions of 5 D0→ 7 FJ (J = 0-4) of Eu 3+ , which are similar to PL spectra. Integrated XEL intensities of samples enhance as increasing concentration of Eu 3+ . The highest integrated XEL intensity is 22.7% (from SBAY:8Eu) of that of BGO. It is higher than other Eu 3+ -doped borate and germanate glass scintillators listed in Table 2.    Relating scintillating mechanism is shown in Figure 7 and described as follows [31,32]. At the first conversion stage, heavy atoms in the host interaction with X-ray irradiation, and, therefore, many electrons and holes are created by the photoelectric effect or Compton scattering. Subsequently, electrons and holes are thermalized to secondary electrons and deep holes [33]. At the second transport stage, secondary electrons and low energy holes are gradually migrated to the bottom of the conduction band and the top of the valence band with the production of phonons, respectively. After that, the luminescent centers (Eu 3+ ions) absorb the energy of electron-hole pairs and jump to an excited state from the ground state. At the last luminescence stage, Eu 3+ ions in excited state return to the ground state with the desired scintillation light.
trons and deep holes [33]. At the second transport stage, secondary electrons and low energy holes are gradually migrated to the bottom of the conduction band and the top of the valence band with the production of phonons, respectively. After that, the luminescent centers (Eu 3+ ions) absorb the energy of electron-hole pairs and jump to an excited state from the ground state. At the last luminescence stage, Eu 3+ ions in excited state return to the ground state with the desired scintillation light. To investigate the radiation tolerance, the optimal SBAY:8Eu specimen was radiated continuously for 60 min by X-ray (6 W). The XEL spectra were measured at five-minute intervals and are given in Figure 8a. Because of some fluctuations in X-ray, the line of integrated XEL intensity is not a straight line (Figure 8b). But, the magnitude of the changes can be almost negligible. Therefore, the specimen has competent radiation tolerance [34]. To investigate the radiation tolerance, the optimal SBAY:8Eu specimen was radiated continuously for 60 min by X-ray (6 W). The XEL spectra were measured at five-minute intervals and are given in Figure 8a. Because of some fluctuations in X-ray, the line of integrated XEL intensity is not a straight line (Figure 8b). But, the magnitude of the changes can be almost negligible. Therefore, the specimen has competent radiation tolerance [34].
valence band with the production of phonons, respectively. After that, the luminescent centers (Eu 3+ ions) absorb the energy of electron-hole pairs and jump to an excited state from the ground state. At the last luminescence stage, Eu 3+ ions in excited state return to the ground state with the desired scintillation light. To investigate the radiation tolerance, the optimal SBAY:8Eu specimen was radiated continuously for 60 min by X-ray (6 W). The XEL spectra were measured at five-minute intervals and are given in Figure 8a. Because of some fluctuations in X-ray, the line of integrated XEL intensity is not a straight line (Figure 8b). But, the magnitude of the changes can be almost negligible. Therefore, the specimen has competent radiation tolerance [34]. Furthermore, the resistance under X-ray radiation of the SBAY:8Eu sample is assessed with different input power likewise. As demonstrated in Figure 9a, the XEL intensity of the SBAY:8Eu sample increases with the growth of input X-ray power. Firstly, the transmittance of the SBAY:8Eu sample is higher than 80%. Even though the input power of the X-ray increases from 4 W to 12 W, the transmittance of the SBAY:8Eu sample is steady (Figure 9b). The above results illustrate that Eu 3+ -doped boroaluminosilicate glass possesses pretty good radiation resistance [29]. Figure 8. (a) The XEL spectra (measured at five-minute interval) of SBAY:8Eu specimen radiated continuously for 60 min by X-ray (6 W), and (b) time-dependent integrated XEL intensities for SBAY:8Eu specimen. Furthermore, the resistance under X-ray radiation of the SBAY:8Eu sample is assessed with different input power likewise. As demonstrated in Figure 9a, the XEL intensity of the SBAY:8Eu sample increases with the growth of input X-ray power. Firstly, the transmittance of the SBAY:8Eu sample is higher than 80%. Even though the input power of the X-ray increases from 4 W to 12 W, the transmittance of the SBAY:8Eu sample is steady (Figure 9b). The above results illustrate that Eu 3+ -doped boroaluminosilicate glass possesses pretty good radiation resistance [29]. X-ray imaging ability of Eu 3+ -doped glass scintillators was first reported in this paper (SBAY:8Eu sample). To appraise the practicality of SBAY:8Eu glass for X-ray imaging, the bright field photos of chip, metallic spring in capsule, and standard X-ray imaging testpattern plate are exhibited in Figure 10a,c,e, respectively. Their X-ray images with high resolution are displayed in Figure 10b,d,f, respectively. And the internal structures of the electronic chip and encapsulated metallic spring can be clearly visualized using an X-ray imaging instrument. As demonstrated in Figure 10f, the spatial resolution of 14 lp/mm can be achieved for the SBAY:8Eu sample. Therefore, the SBAY:8Eu sample with high integrated XEL intensity and excellent spatial resolution (14 lp/mm) might have potential application for X-ray imaging [35]. X-ray imaging ability of Eu 3+ -doped glass scintillators was first reported in this paper (SBAY:8Eu sample). To appraise the practicality of SBAY:8Eu glass for X-ray imaging, the bright field photos of chip, metallic spring in capsule, and standard X-ray imaging test-pattern plate are exhibited in Figure 10a,c,e, respectively. Their X-ray images with high resolution are displayed in Figure 10b,d,f, respectively. And the internal structures of the electronic chip and encapsulated metallic spring can be clearly visualized using an X-ray imaging instrument. As demonstrated in Figure 10f, the spatial resolution of 14 lp/mm can be achieved for the SBAY:8Eu sample. Therefore, the SBAY:8Eu sample with high integrated XEL intensity and excellent spatial resolution (14 lp/mm) might have potential application for X-ray imaging [35].

Conclusions
A series of Eu 3+ -doped SiO2-B2O3-Al2O3-Y2O3 glasses were manufactured by the melt quenching method. All specimens present good optical transmittance and good internal quantum yield. The optimal SBAY:8Eu sample reveals a fine X-ray conversion ability (integrated intensity of XEL is 22.7% of that of BGO crystals), excellent radiation tolerance, and good spatial resolution of 14 lp/mm. Such results suggest that Eu 3+ -doped boroaluminosilicate might be utilized in X-ray imaging.

Data Availability Statement:
The data presented in this study are available on request from the corresponding author.

Conflicts of Interest:
The authors declare no conflict of interest.

Conclusions
A series of Eu 3+ -doped SiO 2 -B 2 O 3 -Al 2 O 3 -Y 2 O 3 glasses were manufactured by the melt quenching method. All specimens present good optical transmittance and good internal quantum yield. The optimal SBAY:8Eu sample reveals a fine X-ray conversion ability (integrated intensity of XEL is 22.7% of that of BGO crystals), excellent radiation tolerance, and good spatial resolution of 14 lp/mm. Such results suggest that Eu 3+ -doped boroaluminosilicate might be utilized in X-ray imaging.

Data Availability Statement:
The data presented in this study are available on request from the corresponding author.