5 results on '"Jeffrey C. McCallum"'
Search Results
2. Spectral Broadening of a Single Er3+ Ion in a Si Nanotransistor
- Author
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Jiliang Yang, Jian Wang, Wenda Fan, Yangbo Zhang, Changkui Duan, Guangchong Hu, Gabriele G. de Boo, Brett C. Johnson, Jeffrey C. McCallum, Sven Rogge, Chunming Yin, and Jiangfeng Du
- Subjects
General Physics and Astronomy - Published
- 2022
3. Piezoresistance in Defect-Engineered Silicon
- Author
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C. T.-K. Lew, Brett C. Johnson, Steve Arscott, A. Thayil, Marcel Filoche, Alistair Rowe, Jeffrey C. McCallum, H. Li, Laboratoire de physique de la matière condensée (LPMC), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), University of Melbourne, Institut d’Électronique, de Microélectronique et de Nanotechnologie - UMR 8520 (IEMN), Centrale Lille-Université de Lille-Centre National de la Recherche Scientifique (CNRS)-Université Polytechnique Hauts-de-France (UPHF)-JUNIA (JUNIA), Nano and Microsystems - IEMN (NAM6 - IEMN), Centrale Lille-Institut supérieur de l'électronique et du numérique (ISEN)-Université de Valenciennes et du Hainaut-Cambrésis (UVHC)-Université de Lille-Centre National de la Recherche Scientifique (CNRS)-Université Polytechnique Hauts-de-France (UPHF)-Centrale Lille-Institut supérieur de l'électronique et du numérique (ISEN)-Université de Valenciennes et du Hainaut-Cambrésis (UVHC)-Université de Lille-Centre National de la Recherche Scientifique (CNRS)-Université Polytechnique Hauts-de-France (UPHF), ANR-17-CE24-0005,TRAMP,Propriétés électromécaniques nouvelles des nanostructures de silicium induites par des pièges électroniques(2017), Université catholique de Lille (UCL)-Université catholique de Lille (UCL), Université catholique de Lille (UCL)-Université catholique de Lille (UCL)-Centrale Lille-Université de Lille-Centre National de la Recherche Scientifique (CNRS)-Université Polytechnique Hauts-de-France (UPHF)-JUNIA (JUNIA), financial support from the French Agence Nationale de la Recherche (ANR-17-CE24-0005), and M.F. and A.T. are funded by a grant from the Simons Foundation (601944, MF)
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Electron mobility ,Silicon ,Dimension (graph theory) ,FOS: Physical sciences ,General Physics and Astronomy ,chemistry.chemical_element ,Applied Physics (physics.app-ph) ,02 engineering and technology ,01 natural sciences ,0103 physical sciences ,[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics ,010306 general physics ,Electronic band structure ,Physics ,Condensed Matter - Materials Science ,Condensed matter physics ,Materials Science (cond-mat.mtrl-sci) ,Defect engineering ,Physics - Applied Physics ,Disordered Systems and Neural Networks (cond-mat.dis-nn) ,Condensed Matter - Disordered Systems and Neural Networks ,021001 nanoscience & nanotechnology ,chemistry ,[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci] ,0210 nano-technology ,Energy (signal processing) - Abstract
The steady-state, space-charge-limited piezoresistance (PZR) of defect-engineered, silicon-on-insulator device layers containing silicon divacancy defects changes sign as a function of applied bias. Above a punch-through voltage ($V_t$) corresponding to the onset of a space-charge-limited hole current, the longitudinal $\langle 110 \rangle$ PZR $\pi$-coefficient is $\pi \approx 65 \times 10^{-11}$~Pa$^{-1}$, similar to the value obtained in charge-neutral, p-type silicon. Below $V_t$, the mechanical stress dependence of the Shockley-Read-Hall (SRH) recombination parameters, specifically the divacancy trap energy $E_T$ which is estimated to vary by $\approx 30$~$\mu$V/MPa, yields $\pi \approx -25 \times 10^{-11}$~Pa$^{-1}$. The combination of space-charge-limited transport and defect engineering which significantly reduces SRH recombination lifetimes makes this work directly relevant to discussions of giant or anomalous PZR at small strains in nano-silicon whose characteristic dimension is larger than a few nanometers. In this limit the reduced electrostatic dimensionality lowers $V_t$ and amplifies space-charge-limited currents and efficient SRH recombination occurs via surface defects. The results reinforce the growing evidence that in steady state, electro-mechanically active defects can result in anomalous, but not giant, PZR., Comment: 9 pages, 8 figures
- Published
- 2021
4. Optically Active Defects at the SiC/SiO2 Interface
- Author
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Massimo Camarda, Benjamin Pingault, Brett C. Johnson, S. Dimitrijev, C. T.-K. Lew, Judith Woerle, R. A. Parker, Mete Atatüre, Adam Gali, Jeffrey C. McCallum, D. Haasmann, and Helena S. Knowles
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Materials science ,Passivation ,business.industry ,Interface (computing) ,General Physics and Astronomy ,02 engineering and technology ,Optically active ,021001 nanoscience & nanotechnology ,01 natural sciences ,Capacitance ,Characterization (materials science) ,chemistry.chemical_compound ,Reliability (semiconductor) ,stomatognathic system ,chemistry ,0103 physical sciences ,Silicon carbide ,Optoelectronics ,Electronics ,010306 general physics ,0210 nano-technology ,business - Abstract
The SiC/SiO2 interface is a central component of many SiC electronic devices. Defects intrinsic to this interface can have a profound effect on their operation and reliability. It is therefore crucial to both understand the nature of these defects and develop characterization methods to enable optimized SiC-based devices. Here we make use of confocal microscopy to address single SiC/SiO2-related defects and show the technique to be a noncontact, nondestructive, spatially resolved and rapid means of assessing thequality of the SiC/SiO2 interface. This is achieved by a systematic investigation of the defect density of the SiC/SiO2 interface by varying the parameters of a nitric oxide passivation anneal after oxidation. Standard capacitance-based characterization techniques are used to benchmark optical emission rates and densities of the optically active SiC/SiO2-related defects. Further insight into the nature of these defects is provided by low-temperature optical measurements on single defects.
- Published
- 2019
5. Irradiation-Induced Modification of the Superconducting Properties of Heavily-Boron-Doped Diamond
- Author
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Jeffrey C. McCallum, Brett C. Johnson, Hiroshi Kawarada, Taisuke Kageura, Steven Prawer, Yi Jiang, Daniel L. Creedon, Kumaravelu Ganesan, Alastair Stacey, and David N. Jamieson
- Subjects
inorganic chemicals ,Superconductivity ,Annealing (metallurgy) ,business.industry ,Doping ,Analytical chemistry ,General Physics and Astronomy ,chemistry.chemical_element ,Diamond ,02 engineering and technology ,Chemical vapor deposition ,engineering.material ,021001 nanoscience & nanotechnology ,01 natural sciences ,Condensed Matter::Materials Science ,Semiconductor ,chemistry ,Condensed Matter::Superconductivity ,0103 physical sciences ,engineering ,Irradiation ,010306 general physics ,0210 nano-technology ,Boron ,business - Abstract
Diamond, a wide band-gap semiconductor, can be engineered to exhibit superconductivity when doped heavily with boron. The phenomena has been demonstrated in samples grown by chemical vapor deposition where the boron concentration exceeds the critical concentration for the metal-to-insulator transition of nMIT4×1020/cm3. While the threshold carrier concentration for superconductivity is generally well established in the literature, it is unclear how well correlated higher critical temperatures are with increased boron concentration. Previous studies have generally compared several samples grown under different plasma conditions, or on substrates having different crystallographic orientations, in order to vary the incorporation of boron into the lattice. Here, we present a study of a single sample with unchanging boron concentration, and instead modify the charge-carrier concentration by introducing compensating defects via high-energy ion irradiation. Superconductivity is completely suppressed when the number of defects is sufficient to compensate the hole concentration to below threshold. Furthermore, we show it is possible to recover the superconductivity by annealing the sample in vacuum to remove the compensating defects.
- Published
- 2018
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