Properties of Sm-Doped SrCl 2 Crystalline Scintillators

: Sm-doped SrCl 2 crystals were prepared, and the scintillation properties such as emission spectra, decay proﬁles, and pulse height were investigated. Under X-ray irradiation, a broad band can be observed at 680 nm, which indicates that the major origin is due to 5d-4f transitions of Sm 2+ . The decay curve is approximated by one exponential function with a decay time of 10 µ s, and the decay time constant is typical for Sm 2+ . From the pulse height of 137 Cs γ -rays, 0.1% Sm:SrCl 2 shows a light yield of 33,000 photons/MeV.


Introduction
A scintillator is a material that exhibits luminescence when excited by ionizing radiation and is used with a photodetector to convert emitted photons into electrical signals. Scintillators play an important role in radiation measurements such as medicine [1,2], resource exploration [3], security [4], astrophysics [5], and monitoring [6,7]. Conventionally, scintillators that exhibit ultraviolet or visible luminescence, suitable for general Si-based photodiodes or photomultiplier tubes, have mainly been developed [8][9][10]. On the other hand, scintillators with near-infrared (NIR) luminescence have been attracting attention. Wavelengths from 650 to 950 nm, called the first optical window, are transparent to water and blood in the human body [11,12]. Hence, in vivo dosimetry during radiotherapy [13,14] and monitoring of drug delivery [15,16] have been suggested as promising applications. In addition, high-dose monitoring applications have been proposed. When monitoring high-dose environments such as nuclear reactors, radiation damage to semiconductor components hinders stable measurement. Therefore, remote monitoring using optical fiber has been proposed, and NIR photons have an advantage due to their high transmittance for optical fiber [17,18]. In addition, it is easy to distinguish red-NIR photons from Cherenkov light generated in a nuclear reactor because Cherenkov light, characterized by pale light, is known to have high light intensity in the near-ultraviolet to visible regions [19,20]. On the other hand, in high-dose field measurements using conventional ultraviolet-visible scintillators, Cherenkov light inhibits stable measurements.

Materials and Methods
Sm-doped SrCl 2 single crystals were synthesized using a vertical Bridgman furnace (VFK-1800, Crystal Systems, Yamanashi, Japan). The initial concentrations of tested Sm were 0.1, 0.5, and 1%. SrCl 2 ·6H 2 O (99%), SmCl 3 (99.9%), and carbon powders were vacuumed (~10 Pa) in a quartz ampoule and then sealed using a gas burner (KSA-22, Tokyo Koshin Rikagaku Seisakusho, Tokyo, Japan). Here, the carbon powder maintains the reduction conditions to remove residual oxygen contamination and promote the reduction of Sm 3+ → Sm 2+ [36]. Then, crystal growth was performed using the Bridgman furnace with a pulling speed of 10 mm/h. The samples were processed into smaller samples, and the actual concentrations were determined using X-ray fluorescence (XRF) analyses (SEA-1000A, SII, Chiba, Japan). The tested tube voltage and used filters were 50 kV with a Pb filter, 30 kV with a Pb filter, and 15 kV with a Cr filter.
Photoluminescence (PL) properties were evaluated using spectrofluorometers (C11347 and C11367, Hamamatsu Photonics, Shizuoka, Japan). Radioluminescence (RL) spectra under X-ray irradiation, RL decay profiles, and pulse height were measured according to a previously reported setup [37,38]. The photomultiplier tube with a multialkali photoelectric surface used at pulse height covered the sensitivity of 300-900 nm, and the quantum efficiency (QE) was 18% at 520 nm and 10% at 680 nm.

Results and Discussion
The sizes of 0.1, 0.5, and 1% Sm:SrCl 2 synthesized by the Bridgman method were approximately 4-6 mmϕ × 10-15 mm, and they had a few cracks owing to the high pulldown speed. For following characterizations, the samples were cut into small pieces with a size of 2-3 mmϕ × 1 mm, and the surfaces were polished. The actual Sm concentrations of the 0.1, 0.5, and 1% Sm:SrCl 2 samples are 0.043, 0.186, and 0.315%, respectively. In all samples, the selected pieces showed lower Sm concentrations than the initial concentrations because of segregation. Figure 1 shows the appearance of the prepared Sm:SrCl 2 . The appearance of the sample is transparent, and red luminescence is observed when irradiated with an ultraviolet lamp (365 nm). X-ray fluorescence spectra of 0.1% Sm:SrCl 2 sample with a tube voltage of (top) 50 kV, (middle) 30 kV, and (bottom) 15 kV are shown in Figure S1.

Materials and Methods
Sm-doped SrCl2 single crystals were synthesized using a vertical Bridgman furnace (VFK-1800, Crystal Systems, Yamanashi, Japan). The initial concentrations of tested Sm were 0.1, 0.5, and 1%. SrCl2·6H2O (99%), SmCl3 (99.9%), and carbon powders were vacuumed (~10 Pa) in a quartz ampoule and then sealed using a gas burner (KSA-22, Tokyo Koshin Rikagaku Seisakusho, Tokyo, Japan). Here, the carbon powder maintains the reduction conditions to remove residual oxygen contamination and promote the reduction of Sm 3+ → Sm 2+ [36]. Then, crystal growth was performed using the Bridgman furnace with a pulling speed of 10 mm/h. The samples were processed into smaller samples, and the actual concentrations were determined using X-ray fluorescence (XRF) analyses (SEA-1000A, SII, Chiba, Japan). The tested tube voltage and used filters were 50 kV with a Pb filter, 30 kV with a Pb filter, and 15 kV with a Cr filter.
Photoluminescence (PL) properties were evaluated using spectrofluorometers (C11347 and C11367, Hamamatsu Photonics, Shizuoka, Japan). Radioluminescence (RL) spectra under X-ray irradiation, RL decay profiles, and pulse height were measured according to a previously reported setup [37,38]. The photomultiplier tube with a multialkali photoelectric surface used at pulse height covered the sensitivity of 300-900 nm, and the quantum efficiency (QE) was 18% at 520 nm and 10% at 680 nm.

Results and Discussion
The sizes of 0.1, 0.5, and 1% Sm:SrCl2 synthesized by the Bridgman method were approximately 4-6 mmφ × 10-15 mm, and they had a few cracks owing to the high pulldown speed. For following characterizations, the samples were cut into small pieces with a size of 2-3 mmφ × 1 mm, and the surfaces were polished. The actual Sm concentrations of the 0.1, 0.5, and 1% Sm:SrCl2 samples are 0.043, 0.186, and 0.315%, respectively. In all samples, the selected pieces showed lower Sm concentrations than the initial concentrations because of segregation. Figure 1 shows the appearance of the prepared Sm:SrCl2. The appearance of the sample is transparent, and red luminescence is observed when irradiated with an ultraviolet lamp (365 nm). X-ray fluorescence spectra of 0.1% Sm:SrCl2 sample with a tube voltage of (top) 50 kV, (middle) 30 kV, and (bottom) 15 kV are shown in Figure S1.    Figure 2 shows the PL 3D spectrum of the 0.1% Sm-doped sample, and the 0.1, 0.5, and 1% doped samples show QYs of 85.9%, 65.7%, and 39.4%, respectively. Under excitation from 290 to 680 nm, a broad emission band is observed at 680 nm The spectral features are almost the same as those in Sm:SrBr 2 [28]. Figure 3 shows the PL decay profiles monitored at 680 nm when excited at 280 nm. The obtained curves are fitted with an exponential function, which indicates the emission has the decay time constants of 9-11 µs. The origin is the 5d-4f transitions of Sm 2+ because the decay time constants are close to those reported in previous studies [28]. The decrease in QY indicates concentration quenching, while the decay does not change. The results suggest that the radiative transition rate decreases, and the nonradiative transition rate increases as the Sm-concentration increases.
Crystals 2022, 12, x FOR PEER REVIEW 3 of 7 are almost the same as those in Sm:SrBr2 [28]. Figure 3 shows the PL decay profiles monitored at 680 nm when excited at 280 nm. The obtained curves are fitted with an exponential function, which indicates the emission has the decay time constants of 9-11 μs. The origin is the 5d-4f transitions of Sm 2+ because the decay time constants are close to those reported in previous studies [28]. The decrease in QY indicates concentration quenching, while the decay does not change. The results suggest that the radiative transition rate decreases, and the nonradiative transition rate increases as the Sm-concentration increases.   Figure 4 shows the RL spectra of Sm:SrCl2 crystals. The samples dominantly exhibit an emission band at 680 nm due to Sm 2+ . In addition, a broad emission band is observed at 430 nm, which is due to self-trapped excitons [39]. The emission decreases with the concentration of doped Sm. According to PL analyses, the wavelength of STE luminescence overlaps with the absorption wavelength of Sm 2+ , and the absorption decreases STE luminescence. In addition, all samples exhibit a few sharp peaks in the range from 550 to 610 nm, and the origin is the 4f-4f transitions of Sm 3+ . Figure 5 shows the RL decay curves of the Sm:SrCl2 crystals. The obtained curves are approximated with one exponential function, which indicates that the decay times are about 9 μs. The values are shorter than PL decay, and this trend was also observed in other materials. One reason is thought to be the interaction of numerous excited secondary electrons leading to quenching. are almost the same as those in Sm:SrBr2 [28]. Figure 3 shows the PL decay profiles monitored at 680 nm when excited at 280 nm. The obtained curves are fitted with an exponential function, which indicates the emission has the decay time constants of 9-11 μs. The origin is the 5d-4f transitions of Sm 2+ because the decay time constants are close to those reported in previous studies [28]. The decrease in QY indicates concentration quenching, while the decay does not change. The results suggest that the radiative transition rate decreases, and the nonradiative transition rate increases as the Sm-concentration increases.   Figure 4 shows the RL spectra of Sm:SrCl2 crystals. The samples dominantly exhibit an emission band at 680 nm due to Sm 2+ . In addition, a broad emission band is observed at 430 nm, which is due to self-trapped excitons [39]. The emission decreases with the concentration of doped Sm. According to PL analyses, the wavelength of STE luminescence overlaps with the absorption wavelength of Sm 2+ , and the absorption decreases STE luminescence. In addition, all samples exhibit a few sharp peaks in the range from 550 to 610 nm, and the origin is the 4f-4f transitions of Sm 3+ . Figure 5 shows the RL decay curves of the Sm:SrCl2 crystals. The obtained curves are approximated with one exponential function, which indicates that the decay times are about 9 μs. The values are shorter than PL decay, and this trend was also observed in other materials. One reason is thought to be the interaction of numerous excited secondary electrons leading to quenching.  Figure 4 shows the RL spectra of Sm:SrCl 2 crystals. The samples dominantly exhibit an emission band at 680 nm due to Sm 2+ . In addition, a broad emission band is observed at 430 nm, which is due to self-trapped excitons [39]. The emission decreases with the concentration of doped Sm. According to PL analyses, the wavelength of STE luminescence overlaps with the absorption wavelength of Sm 2+ , and the absorption decreases STE luminescence. In addition, all samples exhibit a few sharp peaks in the range from 550 to 610 nm, and the origin is the 4f-4f transitions of Sm 3+ . Figure 5 shows the RL decay curves of the Sm:SrCl 2 crystals. The obtained curves are approximated with one exponential function, which indicates that the decay times are about 9 µs. The values are shorter than PL decay, and this trend was also observed in other materials. One reason is thought to be the interaction of numerous excited secondary electrons leading to quenching.    Figure 6 shows the pulse height spectra of Sm:SrCl2 under 137 Cs (662 keV γ-rays) exposure. Ce:Y3Al5O12 was selected as a reference sample showing an RL peak at 520 nm with an LY of 20,000 photons/MeV [40]. The light yields (LYs) of the samples were calculated as follows: LY = 20,000 × (channelsample/channelref) × (18%/10%), calculated considering the photoabsorption peak channel and spectral sensitivity of the used photomultiplier tube. The LYs are 33,000 for 0.1%, 28,000 for 0.5%, and 24,000 photons/MeV for 1% Sm:SrCl2 crystals. Among the samples, the 0.1% doped sample shows the highest LY. This value is higher than Sm:Ba0.3Sr0.7Cl2 (22,000), Sm:SrBr2 (32,000) and Eu:SrBr2 (25,000), while it is lower than Sm, Eu:SrI2 (~40,000), Eu:SrI2 (80,000) and Yb:SrX2 (~50,000) [22,23,31,34,41]. The LYs increase with increasing QYs, and the LYs are dependent on the QYs. The trend of the results are consistent with the Robbins and Lempicki models [42,43].    Figure 6 shows the pulse height spectra of Sm:SrCl2 under 137 Cs (662 keV γ-rays) exposure. Ce:Y3Al5O12 was selected as a reference sample showing an RL peak at 520 nm with an LY of 20,000 photons/MeV [40]. The light yields (LYs) of the samples were calculated as follows: LY = 20,000 × (channelsample/channelref) × (18%/10%), calculated considering the photoabsorption peak channel and spectral sensitivity of the used photomultiplier tube. The LYs are 33,000 for 0.1%, 28,000 for 0.5%, and 24,000 photons/MeV for 1% Sm:SrCl2 crystals. Among the samples, the 0.1% doped sample shows the highest LY. This value is higher than Sm:Ba0.3Sr0.7Cl2 (22,000), Sm:SrBr2 (32,000) and Eu:SrBr2 (25,000), while it is lower than Sm, Eu:SrI2 (~40,000), Eu:SrI2 (80,000) and Yb:SrX2 (~50,000) [22,23,31,34,41]. The LYs increase with increasing QYs, and the LYs are dependent on the QYs. The trend of the results are consistent with the Robbins and Lempicki models [42,43].  Figure 6 shows the pulse height spectra of Sm:SrCl 2 under 137 Cs (662 keV γ-rays) exposure. Ce:Y 3 Al 5 O 12 was selected as a reference sample showing an RL peak at 520 nm with an LY of 20,000 photons/MeV [40]. The light yields (LYs) of the samples were calculated as follows: LY = 20,000 × (channel sample /channel ref ) × (18%/10%), calculated considering the photoabsorption peak channel and spectral sensitivity of the used photomultiplier tube. The LYs are 33,000 for 0.1%, 28,000 for 0.5%, and 24,000 photons/MeV for 1% Sm:SrCl 2 crystals. Among the samples, the 0.1% doped sample shows the highest LY. This value is higher than Sm:Ba 0.3 Sr 0.7 Cl 2 (22,000), Sm:SrBr 2 (32,000) and Eu:SrBr 2 (25,000), while it is lower than Sm, Eu:SrI 2 (~40,000), Eu:SrI 2 (80,000) and Yb:SrX 2 (~50,000) [22,23,31,34,41]. The LYs increase with increasing QYs, and the LYs are dependent on the QYs. The trend of the results are consistent with the Robbins and Lempicki models [42,43].

Conclusions
Sm-doped SrCl2 crystals were prepared to investigate the properties for scintillator applications. Sm:SrCl2 shows a broad peak at 680 nm due to Sm 2+ . The decay curves are approximated with an exponential function, and the decay time constant is typical of Sm 2+ . The PL QY and LY of the 0.1% SmSrCl2 sample are higher than the other presented samples. Sm:SrCl2 exhibits a comparable LY (33,000 photons/MeV) in comparison with conventional scintillators such as Tl:NaI and Ce:Lu2SiO5, and the LYs are high enough to measure γ-rays.

Conclusions
Sm-doped SrCl 2 crystals were prepared to investigate the properties for scintillator applications. Sm:SrCl 2 shows a broad peak at 680 nm due to Sm 2+ . The decay curves are approximated with an exponential function, and the decay time constant is typical of Sm 2+ . The PL QY and LY of the 0.1% SmSrCl 2 sample are higher than the other presented samples. Sm:SrCl 2 exhibits a comparable LY (33,000 photons/MeV) in comparison with conventional scintillators such as Tl:NaI and Ce:Lu 2 SiO 5 , and the LYs are high enough to measure γ-rays.