Pub Date : 2024-06-10DOI: 10.1149/2162-8777/ad522b
Ami Hitomi, Hiroaki Aizawa, Toru Katsumata
Photoluminescence (PL) spectra, intensities, and image brightness of 0.1–6.0 at% Cr-doped ruby were investigated across temperatures ranging from 24° to 600 °C. PL emissions at λ = 670, 694, 707, and 715 nm were observed in rubies doped with 0.1–1.0 at% Cr. In rubies with higher doping levels of 1.5–6.0 at% Cr, an additional PL emission at λ = 770 nm was detected. PL intensities at λ = 694, 707, 715, and 770 nm decreased with increasing temperatures from 24° to 600 °C, while the PL intensity at λ = 670 nm showed a similar temperature-dependent decrease. The variation in PL image brightness with temperature, particularly the increase observed from 24° to 200 °C, is predominantly influenced by the PL intensity variations at λ = 670 nm. Decay curves and fluorescence lifetimes of PL from ruby with various Cr concentrations were also evaluated at temperatures RT-200 °C.
{"title":"Temperature Variations of Spectra and Images of Photoluminescence from Heavily Cr-Doped Ruby","authors":"Ami Hitomi, Hiroaki Aizawa, Toru Katsumata","doi":"10.1149/2162-8777/ad522b","DOIUrl":"https://doi.org/10.1149/2162-8777/ad522b","url":null,"abstract":"Photoluminescence (PL) spectra, intensities, and image brightness of 0.1–6.0 at% Cr-doped ruby were investigated across temperatures ranging from 24° to 600 °C. PL emissions at <italic toggle=\"yes\">λ</italic> = 670, 694, 707, and 715 nm were observed in rubies doped with 0.1–1.0 at% Cr. In rubies with higher doping levels of 1.5–6.0 at% Cr, an additional PL emission at <italic toggle=\"yes\">λ</italic> = 770 nm was detected. PL intensities at <italic toggle=\"yes\">λ</italic> = 694, 707, 715, and 770 nm decreased with increasing temperatures from 24° to 600 °C, while the PL intensity at <italic toggle=\"yes\">λ</italic> = 670 nm showed a similar temperature-dependent decrease. The variation in PL image brightness with temperature, particularly the increase observed from 24° to 200 °C, is predominantly influenced by the PL intensity variations at <italic toggle=\"yes\">λ</italic> = 670 nm. Decay curves and fluorescence lifetimes of PL from ruby with various Cr concentrations were also evaluated at temperatures RT-200 °C.","PeriodicalId":11496,"journal":{"name":"ECS Journal of Solid State Science and Technology","volume":"13 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-06-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141513605","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-07DOI: 10.1149/2162-8777/ad522a
Sergei P. Stepanoff, Ani Khachatrian, Aman Haque, Fan Ren, Stephen Pearton, Douglas E. Wolfe
Understanding the single event effects (SEE) sensitivity of microelectronic devices and circuits is essential for long-term mission success in ionizing radiation environments. SEEs occur when a single ionizing particle strikes a device with enough energy to cause anomalous malfunction or even a catastrophic failure event. It is conventionally viewed as an electrical phenomenon, whereas this study investigates the possible role of multi-physics. Specifically, we show that localized mechanical stress in electronic devices significantly impacts the degree of SEE sensitivity. We present a technique that indirectly maps both electrical and mechanical field localization to spatially map SEE sensitivity without any need for radiation test sources. It is demonstrated on the operational amplifier LM124 under both pristine and stressed conditions. To validate our hypothesis, our experimental results are compared with those obtained from the well-established pulsed laser SEE technique. Excellent agreement between these results supports our hypothesis that SEE susceptibility may have fundamental roots in both electrical and mechanical fields. Therefore, the ability to map the localizations in these fields may indirectly map the SEE sensitivity of large area electronics, which is very expensive in time and resources.
了解微电子器件和电路的单次事件效应(SEE)灵敏度对于在电离辐射环境中长期成功执行任务至关重要。当单个电离粒子以足够的能量撞击设备,导致异常故障甚至灾难性故障事件时,就会发生 SEE。传统观点认为这是一种电学现象,而本研究则探讨了多物理场的可能作用。具体来说,我们表明电子设备中的局部机械应力会显著影响 SEE 敏感度。我们提出了一种间接映射电场和机械场定位的技术,以空间映射 SEE 灵敏度,而无需辐射测试源。我们在运算放大器 LM124 上演示了该技术在原始和受压条件下的应用。为了验证我们的假设,我们将实验结果与从成熟的脉冲激光 SEE 技术中获得的结果进行了比较。这些结果之间的极佳一致性支持了我们的假设,即 SEE 易感性可能从根本上源于电场和机械场。因此,绘制这些场的定位图的能力可以间接绘制大面积电子设备的 SEE 敏感度图,而这在时间和资源上都是非常昂贵的。
{"title":"Localized Stress Effects on the Single Event Effects Sensitivity of Microelectronics","authors":"Sergei P. Stepanoff, Ani Khachatrian, Aman Haque, Fan Ren, Stephen Pearton, Douglas E. Wolfe","doi":"10.1149/2162-8777/ad522a","DOIUrl":"https://doi.org/10.1149/2162-8777/ad522a","url":null,"abstract":"Understanding the single event effects (SEE) sensitivity of microelectronic devices and circuits is essential for long-term mission success in ionizing radiation environments. SEEs occur when a single ionizing particle strikes a device with enough energy to cause anomalous malfunction or even a catastrophic failure event. It is conventionally viewed as an electrical phenomenon, whereas this study investigates the possible role of multi-physics. Specifically, we show that localized mechanical stress in electronic devices significantly impacts the degree of SEE sensitivity. We present a technique that indirectly maps both electrical and mechanical field localization to spatially map SEE sensitivity without any need for radiation test sources. It is demonstrated on the operational amplifier LM124 under both pristine and stressed conditions. To validate our hypothesis, our experimental results are compared with those obtained from the well-established pulsed laser SEE technique. Excellent agreement between these results supports our hypothesis that SEE susceptibility may have fundamental roots in both electrical and mechanical fields. Therefore, the ability to map the localizations in these fields may indirectly map the SEE sensitivity of large area electronics, which is very expensive in time and resources.","PeriodicalId":11496,"journal":{"name":"ECS Journal of Solid State Science and Technology","volume":"166 1","pages":""},"PeriodicalIF":2.2,"publicationDate":"2024-06-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141513607","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-07DOI: 10.1149/2162-8777/ad522e
B. M. Alotaibi, Haifa A. Alyousef, A. Atta, S. A. Rizk, Abdelfattah T. Elgendy
Novel composite (MC/TiO2) films consisting of titanium dioxide nanoparticles (TiO2NPs) and organic polymer methylcellulose (MC), were synthesized for applied in photocatalysis and industrial sectors. The preparation of the nanocomposites MC/TiO2 films were verified successfully by EDX technique, which demonstrated the uniform distribution of TiO2 in the MC. Moreover, in frequency of 20 Hz to 5.5 MHz, the dielectric properties of MC as a function of TiO2 concentration were determined. The conductivity improved from 5.8 × 10−8 S.cm−1 for MC to 3.8 × 10−6 S.cm−1 for the composite MC/TiO2, and the dielectric constant