Novel γ- and X-ray scintillator research: on the emission wavelength, light yield and time response of Ce3+doped halide scintillators

2009 ◽  
Vol 206 (1) ◽  
pp. 9-20 ◽  
Author(s):  
M. D. Birowosuto ◽  
P. Dorenbos
2020 ◽  
Vol 10 (6) ◽  
pp. 2111
Author(s):  
Yoshihiro Momose ◽  
Takao Sakurai ◽  
Keiji Nakayama

Little is known about the temperature dependence of electron transfer occurring at real metal surfaces. For iron surfaces scratched in seven environments, we report Arrhenius activation energies obtained from the data of photoelectron emission (PE) and X-ray photoelectron spectroscopy (XPS). The environments were air, benzene, cyclohexane, water, methanol, ethanol, and acetone. PE was measured using a modified Geiger counter during repeated temperature scans in the 25–339 °C range under 210-nm-wavelength light irradiation and during light wavelength scans in the range 300 to 200 nm at 25, 200, and 339 °C. The standard XPS measurement of Fe 2p, Fe 3p, O 1s, and C 1s spectra was conducted after wavelength scan. The total number of electrons counted in the XPS measurement of the core spectra, which was called XPS intensity, strongly depended on the environments. The PE quantum yields during the temperature scan increased with temperature, and its activation energies (ΔEaUp1) strongly depended on the environment, being in the range of 0.212 to 0.035 eV. The electron photoemission probability (αA) obtained from the PE during the wavelength scan increased with temperature, and its activation energies (ΔEαA) were almost independent of the environments, being in the range of 0.113–0.074 eV. The environment dependence of the PE behavior obtained from temperature and wavelength scans was closely related to that of the XPS characteristics, in particular, the XPS intensities of O 1s and the O2− component of the O 1s spectrum, the acid–base interaction between the environment molecule and Fe–OH, and the growth of non-stoichiometric FexO. Furthermore, the origin of the αA was attributed to the escape depth of hot electrons across the overlayer.


Crystals ◽  
2020 ◽  
Vol 10 (7) ◽  
pp. 584 ◽  
Author(s):  
Kyoung Jin Kim ◽  
Yuki Furuya ◽  
Kei Kamada ◽  
Rikito Murakami ◽  
Vladimir V. Kochurikhin ◽  
...  

Ce-doped LaBr3/AEBr2 (AE = Mg, Ca, Sr, Ba) eutectics were grown using the Bridgman–Stockbarger (BS) method in quartz ampoules. The eutectics (AE = Mg and Ca) showed optical transparency like optical fiber bundles. A grown Ce-doped LaBr3/MgBr2 eutectic shows a 355 nm emission ascribed to Ce3+ 4f-5d transition under X-ray excitation. The smaller the ionic size of AE, the higher the light yield of the sample was. The light yield of Ce:LaBr3/MgBr2 was 34,300 photon/MeV, which is higher than Ce:LYSO standard. Scintillation decay time under 662 keV gamma-ray excitation was 18.8 ns.


2020 ◽  
Vol 1 (1) ◽  
pp. 71-76 ◽  
Author(s):  
Drew R. Onken ◽  
Federico Moretti ◽  
Javier Caravaca ◽  
Minfang Yeh ◽  
Gabriel D. Orebi Gann ◽  
...  

The impact of PPO concentration in LAB micelles on the luminescence decay time is determined.


2002 ◽  
Vol 47 (19) ◽  
pp. 3057-3064 ◽  
Author(s):  
J.E. DeVilbiss ◽  
J.X. Wang ◽  
B.M. Ocko ◽  
K. Tamura ◽  
R.R. Adzic ◽  
...  

2019 ◽  
Vol 215 ◽  
pp. 116613 ◽  
Author(s):  
R.M. Turtos ◽  
S. Gundacker ◽  
S. Omelkov ◽  
E. Auffray ◽  
P. Lecoq

Nanoscale ◽  
2021 ◽  
Author(s):  
Zhu Meng ◽  
Benoit Mahler ◽  
Julien Houel ◽  
Florian Kulzer ◽  
Gilles Ledoux ◽  
...  

We explore the effect of the shell thickness on the time response of CdS/CdSe/CdS spherical quantum wells (SQWs) nanoscintillators under X-ray excitation. We first compare the spectral and timing properties...


2020 ◽  
Author(s):  
Haibo Zeng ◽  
Xiaoming Li ◽  
Jiaxin Chen ◽  
Dandan Yang ◽  
Xi Chen ◽  
...  

Abstract Fluorescent type nuclear battery (NB) consisting of scintillator and photovoltaic device (PVD) enables semipermanent power source for both small and large devices working under harsh circumstances without instant energy supply. In spite of the progress of device structure design, the development of scintillators with high light yield (LY) and longer emission wavelength catering to PVDs is far behind. Here, a novel Cs3Cu2I5: Mn scintillator, which exhibits an ultrahigh LY of ~ 67000 ph/MeV at an emission wavelength of 564 nm is presented, and this is the highest value at such a long wavelength based on low cost precursors. Besides, doping and intrinsic features endow Cs3Cu2I5: Mn with robust thermal stability and irradiation hardness that 71% or > 90% of the initial radioluminescence (RL) intensity can be maintained in an ultra-broad temperature range of 77 K-433 K or after a total irradiation dose of 38.7 Gy at 333 K, respectively. These superiorities allow the fabrication of an efficient and stable NB, which showed an output improvement of 337% respect to that without scintillator. Luminescence mechanisms including self-trapped exciton, energy transfer, and impact excitation are proposed for the dramatic RL improvement. It is expected that such a new and robust scintillator will open a window for the fields of NBs and radiography.


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