50,386 results on '"Applied Physics"'
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2. Technology: Educational Media and Materials for the Handicapped Program. Final Report.
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Johns Hopkins Univ., Laurel, MD. Applied Physics Lab.
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Results are presented of a project that developed 12 social studies (specifically, directionality and geography) and critical thinking computerized instructional modules using multimedia instruction for students with learning disabilities at the upper elementary and lower intermediate school levels. Seven overarching principles were identified as critical to the successful integration of multimedia in the school curricula: establish learning objectives (knowledge); define learning process to be addressed (skills); apply skills in meaningful contextual situations; insure that multimedia provides true 'value added'; provide flexible lesson design tool; capitalize on broad spectrum of multimedia source material; and insure ease of use. The modules provide instruction in 22 thinking skills areas, with emphasis on metacognition and the cross-curricular application of thinking skills. Two additional modules were developed to assist students with mild to moderate disabilities in developing cognitive and organizational skills required for planning and shopping for meals. Information is presented on the lessons, including learning objectives and ways students can use the computer in their studies. Illustrations from the modules are included. Responsibilities undertaken by the project teams are identified, and a list is included of system features and software requirements for use in multimedia educational programs. The evaluation process which resulted in selection of digital video and optical storage for this project is outlined, and use of a multimedia rapid prototyping tool to allow team members to visualize and dynamically run a model of proposed software is described. (SW)
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- 1993
3. Dipolarization Fronts in the Jovian Magnetotail: Statistical Survey of Ion Intensity Variations Using Juno Observations
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Blöcker, A., Kronberg, E. A., Grigorenko, E. E., Roussos, E., Clark, G., 1 Department of Earth and Environmental Sciences Ludwig Maximilian University of Munich Munich Germany, 2 Space Research Institute Russian Academy of Sciences Moscow Russia, 3 Max Planck Institute for Solar System Research Göttingen Germany, and 4 Johns Hopkins University Applied Physics Laboratory Laurel MD USA
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Juno ,Geophysics ,ddc:523 ,Space and Planetary Science ,Jovian magnetotail ,dipolarization fronts ,JEDI ,energetic ions - Abstract
Energetic particle acceleration and energization in planetary magnetotails are often associated with dipolarization fronts characterized by a rapid increase of the meridional component of the magnetic field. Despite many studies of dipolarization events in Earth's magnetotail, Jupiter’s magnetotail provides an almost ideal environment to study high‐energetic ion acceleration by dipolarization fronts because of its large spatial scales and plasma composition of heavy and light ions. In this study, we focus on the response of different high‐energetic ion intensities (H, He, S, and O) to prominent magnetic dipolarization fronts inside the Jovian magnetotail. We investigate if ion energization and acceleration are present in the observations around the identified dipolarization fronts. Therefore, we present a statistical study of 87 dipolarization front signatures, which are identified in the magnetometer data of the Juno spacecraft from July 2016 to July 2021. For the ion intensity analysis, we use the energetic particle observations from the Jupiter Energetic Particle Detector Instrument. Our statistical study reveals that less than half of the identified events are accompanied by an increase of the ion intensities, while most of the other events show no significant change in the ion intensity dynamics. In about 40% of the events located in the dawn sector a significant decrease of the energy spectral index is detected indicating ion acceleration by the dipolarization fronts., Key Points: Eighty‐seven prominent dipolarization front signatures are observed in the MAG data during Juno's prime mission during 21:00–05:30 local time. Less than half of the identified events are accompanied by an increase of the ion intensities. In 40% of the events observed on the dawn side a significant decrease of the energy spectral index indicates ion acceleration by the fronts., Volkswagen Foundation http://dx.doi.org/10.13039/501100001663, Deutsche Forschungsgemeinschaft http://dx.doi.org/10.13039/501100001659, https://doi.org/10.17189/1519711, https://doi.org/10.17189/1519713
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- 2023
4. Modeling and optimization of urban energy systems for large-scale integration of variable renewable energy generation
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Lund, Peter D., Prof. Aalto University, Department of Applied Physics, Finland, Perustieteiden korkeakoulu, School of Science, Teknillisen fysiikan laitos, Department of Applied Physics, Arabzadeh, Vahid, Lund, Peter D., Prof. Aalto University, Department of Applied Physics, Finland, Perustieteiden korkeakoulu, School of Science, Teknillisen fysiikan laitos, Department of Applied Physics, and Arabzadeh, Vahid
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To meet the future emissions goals, the energy systems need to be decarbonized. As much of the energy use originates from urban areas, their role will be of key importance in this context. One strategy for decarbonization is to use large-scale variable renewable electricity schemes, but these include several challenges, notably the issue of supply and demand mismatch. Therefore, a mix of technologies may be needed to achieve ambitious decarbonization targets in cities. The aim of this doctoral thesis is to develop solutions for city-level energy system transition. For this purpose, a dynamic energy system model for Helsinki city is used to ana-lyze a range of scenarios for a low-carbon future. Renewable energy, in particular wind power, was chosen here as the key supply technology. As northern cities are heat-dominated, the heat-ing sector was included in the analysis by using power-to-heat and heat pump schemes in par-allel to power production. To meet short peak heat demand conditions, separate bio-boilers were also considered. Such schemes provided deep decarbonization possibilities. In the Hel-sinki case, the use of fossil fuels could be reduced even up to 70% through the coupling of wind power with curtailment and heat pumps. Though the above type of sectoral coupling to heating helps to integrate large amounts of intermittent renewable power, the role of the exog-enous power market proved to be important for wind power integration. For Helsinki, for ex-ample, with a wind power capacity of 1500 MW corresponding to 62% of the annual electricity demand, 89% of the wind electricity could be used locally in the different sectors, but the rest needs to be coupled to the exogenous market due to the mismatch and plant limitations. In-corporationg demand-side measures, e.g., building energy efficiency, could save 6%-13% in the annual system costs. Other alternatives such as sustainable gas were also investigated. The results of this thesis indicate that there are severa
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- 2021
5. Determining the origin of tidal oscillations in the ionospheric transition region with EISCAT radar and global simulation data
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Günzkofer, F., Pokhotelov, D., Stober, G., Liu, H., Liu, H.‐L., Mitchell, N. J., Tjulin, A., Borries, C., 1 Institute for Solar‐Terrestrial Physics German Aerospace Center (DLR) Neustrelitz Germany, 2 Institute of Applied Physics & Oeschger Center for Climate Change Research, Microwave Physics University of Bern Bern Switzerland, 3 Department of Earth and Planetary Science Kyushu University Fukuoka Japan, 4 High Altitude Observatory National Center for Atmospheric Research Boulder CO USA, 5 British Antarctic Survey Cambridge UK, and 7 EISCAT Scientific Association Kiruna Sweden
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tidal oscillations ,ionsopheric transition region ,Geophysics ,EISCAT radar campaign ,Space and Planetary Science ,Thermosphere-Ionosphere coupling ,Incoherent Scatter Radar ,ddc:538.7 ,Ionospheric tides - Abstract
At high‐latitudes, diurnal and semidiurnal variations of temperature and neutral wind velocity can originate both in the lower atmosphere (UV or infrared absorption) and in the thermosphere‐ionosphere (ion convection, EUV absorption). Determining the relative impact of different forcing mechanisms gives insight to the vertical coupling in the ionosphere. We analyze measurements from the incoherent scatter radar (ISR) facility operated by the EISCAT Scientific Association. They are complemented by meteor radar data and compared to global circulation models. The amplitudes and phases of tidal oscillations are determined by an adaptive spectral filter (ASF). Measurements indicate the existence of strong semidiurnal oscillations in a two‐band structure at altitudes ≲110 and ≳130 km, respectively. Analysis of several model runs with different input settings suggest the upper band to be forced in situ while the lower band corresponds to upward‐propagating tides from the lower atmosphere. This indicates the existence of an unexpectedly strong, in situ forcing mechanism for semidiurnal oscillations in the high‐latitude thermosphere. It is shown that the actual transition of tides in the altitude region between 90 and 150 km is more complex than described so far., Plain Language Summary: Solar and atmospheric variability influence the ionosphere, causing critical impacts on satellite and ground‐based infrastructure. Determining the dominant forcing mechanisms for ionosphere variability is important for prediction and mitigation of these threats. However, this is a challenging task due to the complexity of solar‐terrestrial coupling processes. Tidal oscillations (mostly 12 and 24‐hr periods) allow for a rough estimations of whether forcing from “above” or “below” dominates. The classical understanding is that 12‐hr oscillations propagate upwards from below while 24‐hr oscillations are forced at high altitudes. We analyze data from two radar systems and three global ionosphere models and show that the altitude structure of tidal oscillations is in fact more complex than classically assumed., Key Points: Twenty‐day long EISCAT radar campaign shows a complex mixture of semidiurnal and diurnal tidal oscillations. Three global circulation models show similar tidal structuring and allow to determine the influence of different forcing mechanisms. Adaptive spectral filtering (ASF) technique allows robust fitting of tidal amplitudes and phases., EISCAT, JSPS KAKENHI, DFG, https://doi.org/10.5281/zenodo.6817130, https://doi.org/10.5281/zenodo.7072141
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- 2022
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6. An Empirical Model of the Equatorial Electron Pitch Angle Distributions in Earth's Outer Radiation Belt
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Smirnov, Artem, Shprits, Yuri Y., Allison, Hayley, Aseev, Nikita, Drozdov, Alexander, Kollmann, Peter, Wang, Dedong, Saikin, Anthony, 1 Helmholtz Centre Potsdam GFZ German Research Centre for Geosciences Potsdam Germany, 3 Department of Earth, Planetary and Space Sciences University of California Los Angeles CA USA, and 4 Applied Physics Laboratory Johns Hopkins University Laurel MD USA
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Atmospheric Science ,pitch angle ,model ,van allen probes ,Physics::Space Physics ,magnetosphere ,electrons ,radiation belt ,ddc:538.76 - Abstract
In this study, we present an empirical model of the equatorial electron pitch angle distributions (PADs) in the outer radiation belt based on the full data set collected by the Magnetic Electron Ion Spectrometer (MagEIS) instrument onboard the Van Allen Probes in 2012–2019. The PADs are fitted with a combination of the first, third and fifth sine harmonics. The resulting equation resolves all PAD types found in the outer radiation belt (pancake, flat‐top, butterfly and cap PADs) and can be analytically integrated to derive omnidirectional flux. We introduce a two‐step modeling procedure that for the first time ensures a continuous dependence on L, magnetic local time and activity, parametrized by the solar wind dynamic pressure. We propose two methods to reconstruct equatorial electron flux using the model. The first approach requires two uni‐directional flux observations and is applicable to low‐PA data. The second method can be used to reconstruct the full equatorial PADs from a single uni‐ or omnidirectional measurement at off‐equatorial latitudes. The model can be used for converting the long‐term data sets of electron fluxes to phase space density in terms of adiabatic invariants, for physics‐based modeling in the form of boundary conditions, and for data assimilation purposes., Plain Language Summary: Pitch angle distributions (PADs) are critically important for understanding the dynamics of trapped electrons in Earth's radiation belt region. Specific PAD types are linked to processes acting within the radiation belts which relate to the origins and loss mechanisms of the particle populations, as well as wave activity. In this study we present a polynomial model of the equatorial electron PADs at energies 30 keV–1.6 MeV with a continuous dependence on L‐shell, magnetic local time and activity driven by the solar wind dynamic pressure. The model can be used to reconstruct equatorial electron flux from observations at high latitudes and can be applied for converting the long‐term electron flux data sets to phase space density, driving the boundary conditions for the physics‐based simulations and for data assimilation., Key Points: A sum of the first, third, and fifth sine harmonics is used to approximate equatorial electron Pitch angle distributions (PADs) measured by the MagEIS detector onboard the Van Allen Probes. We present a PAD model with a continuous dependence on L, magnetic local time and activity, driven by the solar wind dynamic pressure. The model allows reconstructions of equatorial PADs from uni‐ and omni‐directional measurements at off‐equatorial latitudes., Deutsche Forschungsgemeinschaft http://dx.doi.org/10.13039/501100001659, Alexander von Humboldt‐Stiftung http://dx.doi.org/10.13039/100005156, https://doi.org/10.5880/GFZ.2.7.2022.001
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- 2022
7. Plasmoids in the Jovian Magnetotail: Statistical Survey of Ion Acceleration Using Juno Observations
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Blöcker, A., Kronberg, E. A., Grigorenko, E. E., Clark, G., Kozak, L., Vogt, M. F., Roussos, E., 1 Department of Earth and Environmental Sciences Ludwig‐Maximilians‐University Munich Germany, 2 Space Research Institute Russian Academy of Sciences Moscow Russia, 3 Johns Hopkins University Applied Physics Laboratory Laurel MD USA, 4 Astronomy and Space Physics Department Kyev Taras Shevchenko University Kyev Ukraine, 5 Center for Space Physics Boston University Boston MA USA, and 6 Max Planck Institute for Solar System Research Göttingen Germany
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Juno ,ddc:523 ,Geophysics ,Space and Planetary Science ,JEDI ,ion acceleration ,plasmoids - Abstract
Transient magnetic reconnection plays an important role in energetic particle acceleration in planetary magnetospheres. Jupiter's magnetosphere provides a unique natural laboratory to study processes of energy transport and transformation. Strong electric fields in spatially confined structures such as plasmoids can be responsible for ion acceleration to high energies. In this study we focus on the effectiveness of ion energization and acceleration in plasmoids. Therefore, we present a statistical study of plasmoid structures in the predawn magnetotail, which were identified in the magnetometer data of the Juno spacecraft from 2016 to 2018. We additionally use the energetic particle observations from the Jupiter Energetic Particle Detector Instrument which discriminates between different ion species. We are particularly interested in the analysis of the acceleration and energization of oxygen, sulfur, helium, and hydrogen ions. We investigate how the event properties, such as the radial distance and the local time of the observed plasmoids in the magnetotail, affect the ion intensities close to the current sheet center. Furthermore, we analyze if ion acceleration is influenced by magnetic field turbulence inside the plasmoids. We find significant heavy ion acceleration in plasmoids close to the current sheet center which is in line with the previous statistical results based on Galileo observations conducted by Kronberg et al. (2019, https://doi.org/10.1029/2019JA026553). The observed effectiveness of the acceleration is dependent on the position of Juno in the magnetotail during the plasmoid event observation. Our results show no correlation between magnetic field turbulence and nonadiabatic acceleration for heavy ions during plasmoids., Key Points: Intensity of heavy ions is strongly increased during plasmoids close to the current sheet center. Significant increase of heavy ion intensities is observed in plasmoids with larger wave power. Acceleration of heavy and light ions in plasmoids due to resonant interaction with the magnetic field fluctuations could not be observed., Volkswagen Foundation (VolkswagenStiftung) http://dx.doi.org/10.13039/501100001663, Deutsche Forschungsgemeinschaft http://dx.doi.org/10.13039/501100001659, NASA, https://pds-ppi.igpp.ucla.edu/
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- 2022
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8. Jovian Auroral Electron Precipitation Budget—A Statistical Analysis of Diffuse, Mono‐Energetic, and Broadband Auroral Electron Distributions
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Salveter, A., Saur, J., Clark, G., Mauk, B. H., 1 Institute of Geophysics and Meteorology University of Cologne Cologne Germany, and 2 The Johns Hopkins University Applied Physics Laboratory Laurel MD USA
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Juno ,ddc:523 ,Geophysics ,Space and Planetary Science ,Jupiter ,particle distribution ,auroral precipitation budget - Abstract
Recent observations by the Juno spacecraft have shown that electrons contributing to Jupiter's main auroral emission appear to be frequently characterized by broadband electron distributions, but also less often mono‐energetic electron distributions are observed as well. In this work, we quantitatively derive the occurrence rates of the various electron distributions contributing to Jupiter's aurora. We perform a statistical analysis of electrons measured by the JEDI‐instrument within 30–1,200 keV from Juno's first 20 orbits. We determine the electron distributions, either pancake, field‐aligned, mono‐energetic, or broadband, through energy and pitch angles to associate various acceleration mechanisms. The statistical analysis shows that field‐aligned accelerated electrons at magnetic latitudes greater than 76° are observed in 87.6% ± 7.2% of the intervals time averaged over the dipole L‐shells according the main oval. Pancake distributions, indicating diffuse aurora, are prominent at smaller magnetic latitudes (, Plain Language Summary: With the Juno spacecraft arriving in the magnetosphere of Jupiter, first flyby particle measurements have changed the knowledge about the developing process of Jupiter's intense aurora. The observations of auroral particles show a stochastic behavior rather than a preference for specific energy. Our statistical analysis of the first 20 flybys at Jupiter compares the occurrence of different particle distributions and highlights the importance of different generation theories for Jupiter's aurora. A generation via stochastic rather than mono‐energetic behavior is deduced and supports previous observations., Key Points: We present a statistical study of Jupiter's auroral electrons within 30–1,200 keV based on Juno's first 20 perijoves. Broadband electron distributions dominates Jupiter's main auroral zone as they are observed in 93% ± 3% of the intervals studied here. Dominance of broadband distributions underlines the importance of a turbulent or stochastic acceleration process., Deutsche Forschungsgemeinschaft http://dx.doi.org/10.13039/501100001659, Universität zu Köln http://dx.doi.org/10.13039/501100008001, https://lasp.colorado.edu/home/mop/files/2015/02/CoOrd_systems7.pdf, https://pds-ppi.igpp.ucla.edu/mission/JUNO/JNO/JEDI, https://lasp.colorado.edu/home/mop/files/2020/04/20190412_Imai_MagFootReader_UIowa_rev.pdf
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- 2022
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9. Evaluation in Chemistry. Report of International Workshop, Ceylon, August 1968.
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International Union of Pure and Applied Physics. and United Nations Educational, Scientific, and Cultural Organization, Paris (France).
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Included are the proceedings and conclusions of an international workshop held in Ceylon in August, 1968, which was convened by the International Union of Pure and Applied Chemistry (IUPAC). The report is concerned not only with the design, construction and administration of chemistry examinations and evaluation of chemistry curricula but with the whole interrelated problem of curriculum change within an educational system. The first part of the report considers: (1) Aims and Objectives of Education through Chemistry, (2) The Functions of Chemistry Examinations in an Educational System, (3) Administrative and Teaching Action Necessary to Achieve Objectives, (4) Planning an Examination Scheme, (5) Administration and Execution of Chemistry Examinations, and (6) Strategy and Tactics for Curriculum Reform. The rest of the report consists of supporting evidence and background papers from actual developments in Ceylon, India, United Kingdom, and the Soviet Union. (Author/TS)
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- 1968
10. Electrical conductivity of functionalised carbon nanotube networks
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Havu, Ville, Dr., Aalto University, Department of Applied Physics, Finland, Perustieteiden korkeakoulu, School of Science, Teknillisen fysiikan laitos, Department of Applied Physics, Puska, Martti, Prof., Aalto University, Department of Applied Physics, Finland, Electronic Properties of Materials, Ketolainen, Tomi, Havu, Ville, Dr., Aalto University, Department of Applied Physics, Finland, Perustieteiden korkeakoulu, School of Science, Teknillisen fysiikan laitos, Department of Applied Physics, Puska, Martti, Prof., Aalto University, Department of Applied Physics, Finland, Electronic Properties of Materials, and Ketolainen, Tomi
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The fabrication of novel electronic devices requires new kinds of materials. The use of carbon nanotubes (CNTs) in various applications has already been demonstrated and therefore the CNTs are also important carbon materials in addition to graphene and fullerenes. Because the electronic properties of individual CNTs depend on their atomic structures, the individual CNTs are not possibly the best choice for building new electronics. Instead, the new devices could be made using thin films or networks of CNTs. The CNT thin films are transparent, flexible, and conduct electricity. Hence, the CNT thin films are expected to be utilised in a remarkable amount of applications including transistors, touch screens, and solar cells. However, a significant challenge related to the CNT thin films is making a film with both high conductivity and transparency simultaneously. Several methods to improve the conductivity of CNT networks have been studied experimentally. The goal of this thesis is to investigate a few methods to increase the conductivity of CNT networks by using density functional theory combined with the standard Green's function electron transport calculations. In particular, the conductance of junctions of CNTs is examined since the CNT junctions mainly determine the conductivity of the whole network. Two different approaches to improve the electrical conductivity of CNT networks are studied. The conductivity can be enhanced by depositing group 6 transition metal (TM) atoms on the CNT networks because the TM atoms are able to link the CNTs. The four-terminal electron transport calculations show that Cr, Mo, and W linker atoms enhance the conductances of the CNT junctions in a similar way. The increase in the conductance is related to the strong hybridisation between the carbon and TM atom orbitals. The second approach is based on functionalising the CNTs with molecules. The interaction of AuCl4 molecules with CNTs leads to a p-type doping effect. In addition, the d, Uusien elektronisten laitteiden valmistus vaatii uudenlaisia materiaaleja. Hiilinanoputkien käyttäminen useissa sovelluksissa on jo demonstroitu, ja siksi hiilinanoputket ovat myös tärkeitä hiilimateriaaleja grafeenin ja fulleriinien lisäksi. Koska yksittäisten hiilinanoputkien elektroniset ominaisuudet riippuvat hiilinanoputkien atomirakenteesta, yksittäiset hiilinanoputket eivät mahdollisesti ole paras valinta uuden elektroniikan rakentamista varten. Sen sijaan uusia laitteita voitaisiin valmistaa käyttäen hiilinanoputkiohutkalvoja tai -verkkoja. Hiilinanoputkiohutkalvot ovat läpinäkyviä, taipuisia ja johtavat sähköä. Siksi hiilinanoputkiohutkalvoja odotetaan hyödynnettävän merkittävässä määrässä sovelluksia mm. transistoreissa, kosketusnäytöissä ja aurinkokennoissa. Merkittävä hiilinanoputkiohutkalvoihin liittyvä haaste on kuitenkin valmistaa kalvo, jolla on samanaikaisesti sekä suuri johtavuus että läpinäkyvyys. Useita menetelmiä hiilinanoputkiverkkojen johtavuuden parantamiseen on tutkittu kokeellisesti. Tämän tutkielman tavoite on selvittää muutamaa menetelmää hiilinanoputkiverkkojen johtavuuden parantamista varten käyttäen tiheysfunktionaaliteoriaa yhdistettynä tavallisiin Greenin funktio -elektronikuljetuslaskuihin. Erityisesti hiilinanoputkiliitosten johtavuutta tutkitaan, koska hiilinanoputkiliitokset pääasiassa määrittävät koko verkon johtavuuden. Kahta erilaista lähestymistapaa hiilinanoputkiverkkojen sähkönjohtavuuden parantamiseksi tutkitaan. Johtavuutta voidaan kasvattaa pinnoittamalla hiilinanoputkiverkot ryhmän 6 transitiometalliatomeilla, koska transitiometalliatomit pystyvät yhdistämään hiilinanoputket. Neljän terminaalin elektronikuljetuslaskut osoittavat, että Cr-, Mo- ja W-linkkeriatomit voimistavat hiilinanoputkiliitosten johtavuutta samalla tavalla. Johtavuuden kasvu liittyy vahvaan hybridisaatioon hiili- ja transitiometalliatomien orbitaalien välillä. Toinen lähestymistapa perustuu hiilinanoputkien funktionalisoimiseen molekyyleillä. Vuorova
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- 2019
11. Photoluminescence properties of CdSe/ZnS/TOPO nanocrystals in full- and half-microcavity structures
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Division of Advanced Applied Physics, Institute of Engineering, Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Kogane-i, Tokyo 184-8588, Japan, Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Kogane-i, Tokyo 184-8588, Japan, Oda, Masaru, Kazita, Hiroyuki, Obara, Yuki, Tani, Toshiro, Division of Advanced Applied Physics, Institute of Engineering, Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Kogane-i, Tokyo 184-8588, Japan, Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Kogane-i, Tokyo 184-8588, Japan, Oda, Masaru, Kazita, Hiroyuki, Obara, Yuki, and Tani, Toshiro
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type:Journal Article, We report a recent study on photoluminescence (PL) properties of CdSe/ZnS/TOPO nanocrystals (NCs) in a planar full microcavity composed of top and bottom two metal (Ag) mirrors, and also in a similar structure but without top mirror, i.e. half-microcavity, respectively. Angular-dependencies of PL spectra and PL decay curves have been measured to investigate PL modifications due to light-matter coupling in the microcavities. Obtained results indicate that PL dynamics are drastically changed depending on the microcavity structures. In the full-microcavity, PL emission is directed at particular angles and its decay-time is shortened, both of which can be described in terms of so-called Purcell effect, i.e. the interaction between photon-modes and confined excitons in the NCs. As for the half-microcavity, anomalous PL band appears at low energy side of a main PL band associated with the confined excitons. The origin of the anomalous PL will be interpreted as due to the interaction between specific photon-modes in the half-microcavity structure and excitons associated with surface states., source:https://doi.org/10.1002/pssc.201000526
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- 2018
12. Synthesis, characterization, and its PL dynamics of colloidal type II CdTe/CdSe nanocrystals
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Institute of Symbiotic Science and Technology, Division of Advanced Applied Physics, Tokyo University of Agriculture and Technology (TAT), Department of Applied Physics, TAT, Oda, Masaru, Nishiyama, Akira, Marumo, Gi-ichi, Yamada, Shuhei, Tanaka, Erina, Tani, Toshiro, Institute of Symbiotic Science and Technology, Division of Advanced Applied Physics, Tokyo University of Agriculture and Technology (TAT), Department of Applied Physics, TAT, Oda, Masaru, Nishiyama, Akira, Marumo, Gi-ichi, Yamada, Shuhei, Tanaka, Erina, and Tani, Toshiro
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type:Journal Article, We describe our improved synthesis and optical properties of high quality type II CdTe/CdSe nanocrystals (NCs). Specifically, clear shell-thickness dependences have been observed in the absorption and photoluminescence (PL) spectra and PL decay profiles as well. The magnitude of the lowest absorption band decreases drastically with large redshift as the shell thickness increases. The origin will be discussed on the bases of the model where the spatial configuration of the lowest electron-hole pair in the NCs changes from that of type I to type II as the shell thickness increases. As for the PL lifetime of the lowest electron-hole excitations, substantial increase is observed with increasing shell thickness. This can also be understood by considering the spatial configuration; spatial overlap between electron and hole wavefunctions decreases with increasing shell thickness, thus the lifetime increases. As for the NCs with extremely thin shell (∼1 ML; 1 ML = 0.35 nm), the PL lifetime seems much longer than expected. This suggests that the thin shells seem imperfect and work rather a kind of trap sites than layers., source:https://doi.org/10.1002/pssc.200879878
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- 2018
13. Single-molecule detection of chaperonin dynamics through polarization rotation modulation of CdSe QD luminescence imaging
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Division of Advanced Applied Physics, Tokyo University of Agriculture and Technology, Institute of Technology, Division of Advanced Applied Physics, Tokyo University of Agriculture and Technology, Institute of Technology, Department of Basic Sciences, Faculty of Engineering, Kyushu Institute of Technology, Department of Applied Physics, Tokyo University of Agriculture and Technology, Institute of Technology, Department of Biotechnology and Life Science, Tokyo University of Agriculture and Technology, Institute of Technology, Division of Biotechnology and Life Science, Tokyo University of Agriculture and Technology, Institute of Technology, Tani, Toshiro, Oda, Masaru, Araki, Daisuke, Miyashita, Tatsuki, Nakajima, Koudai, Arita, Mayuno, Yohda, Masafumi, Division of Advanced Applied Physics, Tokyo University of Agriculture and Technology, Institute of Technology, Division of Advanced Applied Physics, Tokyo University of Agriculture and Technology, Institute of Technology, Department of Basic Sciences, Faculty of Engineering, Kyushu Institute of Technology, Department of Applied Physics, Tokyo University of Agriculture and Technology, Institute of Technology, Department of Biotechnology and Life Science, Tokyo University of Agriculture and Technology, Institute of Technology, Division of Biotechnology and Life Science, Tokyo University of Agriculture and Technology, Institute of Technology, Tani, Toshiro, Oda, Masaru, Araki, Daisuke, Miyashita, Tatsuki, Nakajima, Koudai, Arita, Mayuno, and Yohda, Masafumi
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type:Conference Paper, We report our recent trials examining the single-molecule three-dimensional (3D) detection of protein conformational dynamics at room temperature. Using molecular chaperones as model proteins and cadmium selenide (CdSe) semiconductor quantum dots (QDs) as nanometer-scale probes, we monitored the temporal evolution of ATP-induced conformation changes with a total internal reflection fluorescence (TIRF) microscopy imaging technique in buffer solutions. The two-dimensional (2D) degenerate nature of the emission dipoles of the QDs, due to the uniaxial wurtzite crystal structure, made it possible to capture the 3D orientation using a polarization modulation technique in real time. The temporal resolution was half the period of analyzer rotation. Although still insufficient, the obtained signals suggest possible 3D detection of specific motions, which supports the two-step conformational changes triggered by ATP attachment., 18th International Conference on Dynamical Processes in Excited States of Solids (DPC2013), August 4-9,2013, Fuzhou, China, source:https://doi.org/10.1016/j.jlumin.2014.01.059
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- 2018
14. Dynamics of photoexcited carriers sinking into an enlarged well in a GaAs/AlAs short-period superlattice
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Department of Applied Physics, Faculty of Engineering, Nagoya University, Chikusa-ku, Nagoya 464, Japan, Central Research Laboratory, Mitsubishi Electric Corporation, Amagasaki, Hyogo 661, Japan, Department of Applied Physics, Faculty of Engineering, Tohoku University, Sendai 980, Japan, Nakamura, A, Fujiwara, K, Tokuda, Y, Nakayama, T, Hirai, M, Department of Applied Physics, Faculty of Engineering, Nagoya University, Chikusa-ku, Nagoya 464, Japan, Central Research Laboratory, Mitsubishi Electric Corporation, Amagasaki, Hyogo 661, Japan, Department of Applied Physics, Faculty of Engineering, Tohoku University, Sendai 980, Japan, Nakamura, A, Fujiwara, K, Tokuda, Y, Nakayama, T, and Hirai, M
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type:Journal Article, We report on the dynamics of photoexcited carriers using picosecond luminescence measurements of GaAs/AlAs superlattices with a barrier width of 1.2 nm and a well width of 3.4 nm. The observed decay kinetics allow us to observe the tunneling-assisted radiative recombination of electrons and holes in different wells. Furthermore, introducing an enlarged well in the superlattice, we investigate the dynamics of photoexcited carriers sinking into the deeper well via vertical transport., source:http://www.aps.org, source:https://doi.org/10.1103/PhysRevB.34.9019
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- 2017
15. Improved recombination lifetime of photoexcited carriers in GaAs single quantum-well heterostructures confined by GaAs/AlAs short-period superlattices
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Central Research Laboratory, Mitsubishi Electric Corporation, Amagasaki, Hyogo 661, Japan, Department of Applied Physics, Faculty of Engineering, Nagoya University, Nagoya 464, Japan, Department of Applied Physics, Faculty of Engineering, Tohoku University, Sendai 980, Japan, Fujiwara, K, Nakamura, A, Tokuda, Y, Nakayama, T, Hirai, M, Central Research Laboratory, Mitsubishi Electric Corporation, Amagasaki, Hyogo 661, Japan, Department of Applied Physics, Faculty of Engineering, Nagoya University, Nagoya 464, Japan, Department of Applied Physics, Faculty of Engineering, Tohoku University, Sendai 980, Japan, Fujiwara, K, Nakamura, A, Tokuda, Y, Nakayama, T, and Hirai, M
- Abstract
type:Journal Article, Photoluminescence (PL) decay time measurements at 77 and 300 K are reported from 6.1 nm GaAs single quantum well heterostructures (SQWH’s) confined by GaAs/AlAs short‐period superlattices (SPS’s) or ternary AlGaAs alloys with similar Al content, prepared by molecular beam epitaxy. The SQW PL intensity exhibits a single exponential decay with a time constant of 1.6 ns for SQWH’s confined by SPS’s and 0.3 ns for SQWH’s confined by AlGaAs alloys at 77 K. From comparison of the decay rates in both types of the sample, it is found that the radiative recombination efficiency is improved by a factor of about 6 in SPS confined SQWH’s. This higher efficiency is attributed to the improved heterointerfaces in addition to the enhanced radiative recombination rate due to the increased overlap of electron and hole wave functions in the narrow SQW., source:http://www.aip.org
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- 2017
16. Room-Temperature Fluorescence Lifetime of Pseudoisocyanine (PIC) J Excitons with Various Aggregate Morphologies in Relation to Microcavity Polariton Formation
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Graduate School of Engineering, Department of Applied Physics, Tokyo University of Agriculture and Technology, Graduate School of Engineering, Department of Applied Physics, Tokyo University of Agriculture and Technology, Division of Advanced Applied Physics, Institute of Technology, Tokyo University of Agriculture and Technology, Obara, Yuki, Saitoh, Keita, Oda, Masaru, Tani, Toshiro, Graduate School of Engineering, Department of Applied Physics, Tokyo University of Agriculture and Technology, Graduate School of Engineering, Department of Applied Physics, Tokyo University of Agriculture and Technology, Division of Advanced Applied Physics, Institute of Technology, Tokyo University of Agriculture and Technology, Obara, Yuki, Saitoh, Keita, Oda, Masaru, and Tani, Toshiro
- Abstract
type:Journal Article, The results of room-temperature fluorescence lifetime measurements are reported for the excitation of J aggregates (Js) of pseudoisocyanine chloride (PIC-Cl) prepared in potassium polyvinyl sulfate (PVS) polymer thin films, their aqueous solutions, and NaCl aqueous solutions. Variations of the microscopic morphologies of the aggregates were investigated. The results show that fluorescence decay features correlated to the morphology change. The observed fluorescence lifetime and quantum efficiency of PIC J aggregates (PIC-Js) in a NaCl aqueous solution were 310 ps and 28%, respectively. The lifetime of the fibril-shaped macroaggregates prepared in PVS thin films was below the instrumental time resolution of 5 ps, and the efficiency decreased to below 3%. The results indicate that PIC-Js prepared with PVS polymers have an increased nonradiative contribution to the excitation deactivation process. In particular, macro-Js with isolated fibril-shaped structures revealed nonradiative pathway(s) that are closely associated to the specific packaging morphology of the constituent meso-Js. The possibility of a destructive effect on the formation of cavity-polaritons is also discussed., source:https://doi.org/10.3390/ijms13055851
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- 2017
17. Fabrication, characterization and its local reflection properties of a metal-mirror microcavity with high concentrated PIC J-aggregates
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Institute of Symbiotic Science and Technology, Tokyo University of Agriculture and Technology, Department of Applied Physics, Tokyo University of Agriculture and Technology, Department of Applied Physics, Tokyo University of Agriculture and Technology, Oda, M., Obara, Y., Saito, K., Higashi, K., Tani, T., Institute of Symbiotic Science and Technology, Tokyo University of Agriculture and Technology, Department of Applied Physics, Tokyo University of Agriculture and Technology, Department of Applied Physics, Tokyo University of Agriculture and Technology, Oda, M., Obara, Y., Saito, K., Higashi, K., and Tani, T.
- Abstract
type:Journal Article, We have investigated reflection properties of light-matter strong coupling in a planar metal-mirror microcavity with highly concentrated PIC J-aggregates. Large vacuum Rabi-splitting ranging from 100 to 250 meV is obtained depending on the concentration of the J-aggregates. The factors for providing these large Rabi-splitting will be discussed based on its concentration dependence. We also present our recent study focused on microscopic reflection properties of the microcavity. We have improved microscope optics which enables us to measure local reflection spectra within 0.3-m-diameter area. Observation of incident-light-angle dependence becomes possible. We found existence of micrometer-scale inhomogeneity in the Rabi-splitting (e.g. ±10% in a region), which will be interpreted mainly by the spatial distribution of J’s in the active layer., source:https://doi.org/10.1016/j.phpro.2010.01.229
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- 2017
18. Synthesis, characterization and its photoluminescence properties of group I-III-VI2 CuInS2 nanocrystals
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Division of Advanced Applied Physics, Institute of Engineering/Department of Applied Physics, Graduate School of Engineering, Tokyo University of Agriculture and Technology, Department of Applied Physics, Graduate School of Engineering, Tokyo University of Agriculture and Technology, Oda, Masaru, Miyaoka, Tomotari, Yamada, Shuhei, Tani, Toshiro, Division of Advanced Applied Physics, Institute of Engineering/Department of Applied Physics, Graduate School of Engineering, Tokyo University of Agriculture and Technology, Department of Applied Physics, Graduate School of Engineering, Tokyo University of Agriculture and Technology, Oda, Masaru, Miyaoka, Tomotari, Yamada, Shuhei, and Tani, Toshiro
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type:Journal Article, We report the synthesis, characterization, and photoluminescence (PL) properties of colloidal I-III-VI2 CuInS2 and CuInS2/ZnS nanocrystals (NCs). Absorption shoulder and PL bands of the NCs are located at higher energy than those of band gap energy of bulk crystals due to a quantum-confinement effect. The PL band has a relatively large Stokes-shift, broad linewidth, and long decay-time, which suggests that the PL originates from a recombination of confined-excitions associated with donor(s) and/or acceptor(s). We found that quantum yield of the PL depends strongly on the photon-energy of excitation light and that it is up to 40-50% in resonant excitation at the energy positions corresponding to the absorption shoulder. Detailed properties and possible dynamics will be described. We also present preliminary results of PL properties focused on single NCs. There exist highluminescent NCs exhibiting so-called PL blinking as similar with II-VI NCs, while the others are dark NCs. 73.21.La, 78.47.jd, 78.67.Bf, 78.67.Hc
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- 2017
19. Measurement of the Core Human Body Temperature by Means of Passive Acoustic Thermometry
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Работа поддержана «Проектом повышения конкурентоспособности ведущих российских университетов среди ведущих мировых научно-образовательных центров» (5-100), частично в рамках Госзадания Института прикладной физики РАН № 0035-2014-0008, а также поддержана РФФИ, грант № 18-29-02052 мк. Благодарим проф. А. М. Черныша за плодотворное обсуждение работы., A. Anosov A.; I. M. Sechenov First Moscow State Medical University, Ministry of Health of Russia, I. Balashov S.; V. I. Kulakov Research Center for Obstetrics, Gynecology and Perinatology, Ministry of Health of Russia, A. Erofeev V.; I. M. Sechenov First Moscow State Medical University, Ministry of Health of Russia, Yu. Zhdankina S.; I. M. Sechenov First Moscow State Medical University, Ministry of Health of Russia, A. Sharakshane A.; V. A. Kotel’nikov Institute of Radio-Engeneering and Electronics, RAS, A. Mansfel’d D.; Federal Research Center Institute of Applied Physics, RAS, А. Аносов А.; Первый Московский государственный медицинский университет им. И. М. Сеченова Минздрава России, И. Балашов С.; Национальный медицинский исследовательский центр акушерства, гинекологии и перинатологии им. В. И. Кулакова Минздрава России, А. Ерофеев В.; Первый Московский государственный медицинский университет им. И. М. Сеченова Минздрава России, Ю. Жданкина С.; Первый Московский государственный медицинский университет им. И. М. Сеченова Минздрава России, А. Шаракшанэ А.; Институт радиотехники и электроники им. В. А. Котельникова РАН, А. Мансфельд Д.; Федеральный исследовательский центр Институт прикладной физики РАН, Работа поддержана «Проектом повышения конкурентоспособности ведущих российских университетов среди ведущих мировых научно-образовательных центров» (5-100), частично в рамках Госзадания Института прикладной физики РАН № 0035-2014-0008, а также поддержана РФФИ, грант № 18-29-02052 мк. Благодарим проф. А. М. Черныша за плодотворное обсуждение работы., A. Anosov A.; I. M. Sechenov First Moscow State Medical University, Ministry of Health of Russia, I. Balashov S.; V. I. Kulakov Research Center for Obstetrics, Gynecology and Perinatology, Ministry of Health of Russia, A. Erofeev V.; I. M. Sechenov First Moscow State Medical University, Ministry of Health of Russia, Yu. Zhdankina S.; I. M. Sechenov First Moscow State Medical University, Ministry of Health of Russia, A. Sharakshane A.; V. A. Kotel’nikov Institute of Radio-Engeneering and Electronics, RAS, A. Mansfel’d D.; Federal Research Center Institute of Applied Physics, RAS, А. Аносов А.; Первый Московский государственный медицинский университет им. И. М. Сеченова Минздрава России, И. Балашов С.; Национальный медицинский исследовательский центр акушерства, гинекологии и перинатологии им. В. И. Кулакова Минздрава России, А. Ерофеев В.; Первый Московский государственный медицинский университет им. И. М. Сеченова Минздрава России, Ю. Жданкина С.; Первый Московский государственный медицинский университет им. И. М. Сеченова Минздрава России, А. Шаракшанэ А.; Институт радиотехники и электроники им. В. А. Котельникова РАН, and А. Мансфельд Д.; Федеральный исследовательский центр Институт прикладной физики РАН
- Abstract
The purpose of the study. To determine whether it is possible to use passive acoustic thermometry to measure the core temperature of human body regions. Materials and methods. Thermal acoustic radiation was measured by a multichannel acoustic thermograph with a threshold sensitivity of 0.3°С at an integration time of 10 s. A portable computer infrared thermograph with a sensitivity of 0.1°С was used to measure the superficial temperature. Results. Measurements of thermal acoustic radiation of the right hypochondrium of the study subject were carried out to obtain an integral temperature of the liver after intake of sugar. At the same time, blood glucose concentrations were measured. The glucose level increased from 4 to 8 mmol/l within an hour and a half; then it began to decline. The acoustic radiation temperature increased by 2°С with a half an hour delay after the increase in the glucose level. Model calculation showed that the liver temperature increased from 37 to 38°С. Conclusion. It was shown that passive acoustic thermometry can be used to measure the core temperature of different regions of the human body. The proposed method may be useful in the emergency medicine., Цель исследования. Установить возможность использования пассивной акустической термометрии для измерения глубинной температуры участков тела человека. Материалы и методы. Тепловое акустическое излучение измеряли многоканальным акустотермографом с пороговой чувствительностью 0,3°С при времени интегрирования 10 с. Для измерения поверхностной температуры использовали портативный компьютерный инфракрасный термограф с чувствительностью 0,1°С. Результаты исследования. Измерения теплового акустического излучения правого подреберья испытуемого провели, чтобы получить интегральную температуру печени после приема испытуемым сахара. Одновременно проводили измерения концентрации глюкозы в крови. В течение полутора часов содержание глюкозы выросло от 4 до 8 ммоль/л, после чего начало снижаться. С задержкой в полчаса после увеличения концентрации глюкозы измеряемая акустояркостная температура увеличилась на 2°С. Модельный расчет показал, что температура печени при этом увеличилась с 37 до 38°С. Заключение. Показали, что пассивную акустическую термометрию можно использовать для измерения глубинной температуры участков тела человека. Предложенный метод может быть востребован в медицине критических состояний.
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- 2019
20. Lightning-driven electric fields measured in the lower ionosphere: Implications for transient luminous events
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Department of Earth and Space Sciences, University of Washington, Seattle, Washington, USA., Geomagnetism Program, USGS, Denver, Colorado, USA., Applied Physics Laboratory, Johns Hopkins University, Laurel, Maryland, USA., Department of Earth and Space Sciences, University of Washington, Seattle, Washington, USA., Department of Electrical Engineering, Kyushu Institute of Technology, Kitakyushu, Japan., Department of Electrical Engineering, Cornell University, Ithaca, New York, USA., Thomas, Jeremy N., Barnum, Benjamin H., Lay, Erin, Holzworth, Robert H., Cho, Mengu, Kelley, Michael C., Department of Earth and Space Sciences, University of Washington, Seattle, Washington, USA., Geomagnetism Program, USGS, Denver, Colorado, USA., Applied Physics Laboratory, Johns Hopkins University, Laurel, Maryland, USA., Department of Earth and Space Sciences, University of Washington, Seattle, Washington, USA., Department of Electrical Engineering, Kyushu Institute of Technology, Kitakyushu, Japan., Department of Electrical Engineering, Cornell University, Ithaca, New York, USA., Thomas, Jeremy N., Barnum, Benjamin H., Lay, Erin, Holzworth, Robert H., Cho, Mengu, and Kelley, Michael C.
- Abstract
type:Journal Article, Transient luminous events above thunderstorms such as sprites, halos, and elves require large electric fields in the lower ionosphere. Yet very few in situ measurements in this region have been successfully accomplished, since it is typically too low in altitude for rockets and satellites and too high for balloons. In this article, we present some rare examples of lightning‐driven electric field changes obtained at 75–130 km altitude during a sounding rocket flight from Wallops Island, Virginia, in 1995. We summarize these electric field changes and present a few detailed case studies. Our measurements are compared directly to a 2D numerical model of lightning‐driven electromagnetic fields in the middle and upper atmosphere. We find that the in situ electric field changes are smaller than predicted by the model, and the amplitudes of these fields are insufficient for elve production when extrapolated to a 100 kA peak current stroke. This disagreement could be due to lightning‐induced ionospheric conductivity enhancement, or it might be evidence of flaws in the electromagnetic pulse mechanism for elves.
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- 2019
21. Giant resonance in electronic stopping power of carbon for MeV-per-atom C60 fullerene ions
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Toshiaki, Kaneko and Department of Applied Physics, Faculty of Science, Okayama University of Science
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- 2018
22. Rainfall variability and trends over East Africa
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E. Cattani, A. Merino, V. Levizzani 1National Research Council of Italy - Institute of Atmospheric Sciences, Climate (CNR-ISAC), Bologna, Italy 2Dept. of Applied Physics, University of León, León, and Spain
- Subjects
Satellite precipitation ,trend analysis ,East Africa - Abstract
The Africa Rainfall Climatology (ARC) v2, Climate Hazards Group InfraRed Precipitation with Stations (CHIRPS) v2, and Tropical Applications of Meteorology using SATellite (TAMSAT) African Rainfall Climatology And Time Series (TARCAT) v3 satellite rainfall products are exploited to study the spatial and temporal variability of East Africa (EA) rainfall between 1983 and 2017 through the time series of selected rainfall indices from the joint CCl/CLIVAR/JCOMM Expert Team on Climate Change Detection and Indices (ETCCDI). The indexes total rainfall amount (PRCPTOT), Simple Daily Intensity (SDII), number of precipitating days (R1), number of consecutive dry and wet days (CDD and CWD), and number of very heavy precipitating days (R20) were analyzed. The scope of the work is to draw the attention on the rainfall trend and variability identifying significant trend patterns regardless of the single satellite product, and also estimating the trend rate variability stemming from the multiplicity of the satellite products. The trend spatial patterns are recognized through the Mann-Kendall technique, considering the time series of the ensemble mean of the three satellite products and the corresponding time series of the standard deviations, which were interpreted as error bars associated with the ensemble mean time series. Indications on rainfall trends were extracted at annual and seasonal scales and the regions that more frequently exhibit statistically significant trends are located in eastern Kenya, Somalia at the border with western Ethiopia, northern Tanzania, and limited areas of South Sudan. At the seasonal scale increasing trends were identified for the October-November-December PRCPTOT, SDII, and R20 indices over eastern EA, with the exception of central Kenya, where rising trends with limited areas of significance stand out for R1 and CWD, distinguishable also at the yearly scale. In March-April-May rainfall decline is perceivable only through R1 and CWD in particular over the eastern EA region, whereas PRCPTOT, even though associated with negative trends, does not present any high confidence areas.
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- 2018
23. Investigation of Pore Structures in Shallow Longmaxi Shale, South China, via Large-Area Electron Imaging and Neutron Scattering Techniques.
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Yu WangKey Laboratory of Interfacial Physics and Technology,Shanghai Institute of Applied Physics, Chinese Academy ofSciences, Shanghai, 201800, China;University of Chinese Academy of Sciences, Beijing,100049, China, Hanqiu Jiang, Yubin Ke, Shengkai Zhang, Lihua Wang, Yanfei Wang, Chunyong He, Linjuan Zhang, and Jian-Qiang WangKey Laboratory of Interfacial Physics and Technology,Shanghai Institute of Applied Physics, Chinese Academy ofSciences, Shanghai, 201800, China;University of Chinese Academy of Sciences, Beijing,100049, China
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- 2020
- Full Text
- View/download PDF
24. Enhanced Biocatalytic Esterification with Lipase-Immobilized Chitosan/Graphene Oxide Beads
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Department of Chemistry, Faculty of Science, Universiti Putra Malaysia, Department of Chemistry, Faculty of Science, Universiti Putra Malaysia, Serdang, Selangor, Malaysia, Institute of Advanced Technology, University Putra Malaysia, Serdang, Selangor, Malaysia, Department of Chemistry, Faculty of Science, Universiti Putra Malaysia, Serdang, Selangor, Malaysia, Laboratory of Molecular Biomedicine, Institute of Bioscience, Universiti Putra Malaysia, Department of Chemistry, Faculty of Science, Universiti Putra Malaysia, Serdang, Faculty of Biotechnology and Biomolecular Sciences, Universiti Putra Malaysia, Low Dimensional Materials Research Centre, Department of Physics, Faculty of Science, University of Malaya, School of Applied Physics, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, Eco-Town Collaborative Research and Development Center for the Environment and Recycling, Kyushu Institute of Technology, Lau, Siaw Cheng, Lim , Hong Ngee, Basri, Mahiran, Masoumi, Hamid Reza Fard, Tajudin, Asilah Ahmad, Huang, Nay Ming, Pandikumar, Alagarsamy, Chia, Chi Hua, Andou, Yoshito, Department of Chemistry, Faculty of Science, Universiti Putra Malaysia, Department of Chemistry, Faculty of Science, Universiti Putra Malaysia, Serdang, Selangor, Malaysia, Institute of Advanced Technology, University Putra Malaysia, Serdang, Selangor, Malaysia, Department of Chemistry, Faculty of Science, Universiti Putra Malaysia, Serdang, Selangor, Malaysia, Laboratory of Molecular Biomedicine, Institute of Bioscience, Universiti Putra Malaysia, Department of Chemistry, Faculty of Science, Universiti Putra Malaysia, Serdang, Faculty of Biotechnology and Biomolecular Sciences, Universiti Putra Malaysia, Low Dimensional Materials Research Centre, Department of Physics, Faculty of Science, University of Malaya, School of Applied Physics, Faculty of Science and Technology, Universiti Kebangsaan Malaysia, Eco-Town Collaborative Research and Development Center for the Environment and Recycling, Kyushu Institute of Technology, Lau, Siaw Cheng, Lim , Hong Ngee, Basri, Mahiran, Masoumi, Hamid Reza Fard, Tajudin, Asilah Ahmad, Huang, Nay Ming, Pandikumar, Alagarsamy, Chia, Chi Hua, and Andou, Yoshito
- Abstract
type:Journal Article, In this work, lipase from Candida rugosa was immobilized onto chitosan/graphene oxide beads. This was to provide an enzyme-immobilizing carrier with excellent enzyme immobilization activity for an enzyme group requiring hydrophilicity on the immobilizing carrier. In addition, this work involved a process for the preparation of an enzymatically active product insoluble in a reaction medium consisting of lauric acid and oleyl alcohol as reactants and hexane as a solvent. This product enabled the stability of the enzyme under the working conditions and allowed the enzyme to be readily isolated from the support. In particular, this meant that an enzymatic reaction could be stopped by the simple mechanical separation of the “insoluble” enzyme from the reaction medium. Chitosan was incorporated with graphene oxide because the latter was able to enhance the physical strength of the chitosan beads by its superior mechanical integrity and low thermal conductivity. The X-ray diffraction pattern showed that the graphene oxide was successfully embedded within the structure of the chitosan. Further, the lipase incorporation on the beads was confirmed by a thermo-gravimetric analysis. The lipase immobilization on the beads involved the functionalization with coupling agents, N-hydroxysulfosuccinimide sodium (NHS) and 1-ethyl-(3-dimethylaminopropyl) carbodiimide (EDC), and it possessed a high enzyme activity of 64 U. The overall esterification conversion of the prepared product was 78% at 60°C, and it attained conversions of 98% and 88% with commercially available lipozyme and novozyme, respectively, under similar experimental conditions.
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- 2018
25. Strong exciton‐photon coupling and its polarization dependence in a metal‐mirror microcavity with oriented PIC J‐aggregates
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Strategic Research Initiative for Future Nano-Science and Technology, Tokyo University of Agriculture and Technology, Department of Applied Physics, Tokyo University of Agriculture and Technology, Oda, Masaru, Hirata, Kazuyuki, Inoue, Tokiko, Obara, Yuki, Fujimura, Tomoko, Tani, Toshiro, Strategic Research Initiative for Future Nano-Science and Technology, Tokyo University of Agriculture and Technology, Department of Applied Physics, Tokyo University of Agriculture and Technology, Oda, Masaru, Hirata, Kazuyuki, Inoue, Tokiko, Obara, Yuki, Fujimura, Tomoko, and Tani, Toshiro
- Abstract
type:Journal Article, We present a study of strong exciton-photon coupling and its dependence on incident light polarization in a metal-metal mirror microcavity containing PIC J-aggregates. Rabi-splitting energies between upper and lower polariton branches are estimated as 94 meV and 69 meV for s- and p-polarized incident light, respectively. These large values are due to large oscillator strength of Frenkel excitons in the PIC J-aggregates and strong confinement of light attributed to the metallic microcavity as well. As for the effective thickness of the active layer for s-polarized light, a good agreement is obtained between Lfiteff = 201 nm deduced from the experimental data and Lcalceff = 207 nm calculated from the summation of the measured thickness of active layer with the estimated penetration depths into silver mirrors. We also discuss the difference in the polarization dependences of Rabi-splitting energy, quantitatively. It is concluded that the polarization dependence is mainly due to an alignment of the J-aggregates in the active layer and is not affected so much by anisotropy of the penetration depths into the silver mirrors., source:https://doi.org/10.1002/pssc.200879879
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- 2018
26. Body Armor | Capt Morley [video]
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Naval Postgraduate School, Applied Physics, Morley, Joseph, Naval Postgraduate School, Applied Physics, and Morley, Joseph
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- 2018
27. Measurement of charge-exchange between Na and Ca+ in a hybrid trap
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Naval Postgraduate School, Applied Physics, Kwolek, J.M., Goodman, D.S., Slayton, B., Blümel, R., Wells, J.E., Narducci, F.A., Smith, W.W., Naval Postgraduate School, Applied Physics, Kwolek, J.M., Goodman, D.S., Slayton, B., Blümel, R., Wells, J.E., Narducci, F.A., and Smith, W.W.
- Abstract
We present measurements of the charge-exchange reaction rate between neutral sodium (Na) and ionized calcium (Ca+) in a hybrid atom-ion trap, which is comprised of a Na magneto-optical trap concentric with a linear Paul trap. Once the Na and Ca+ are co-trapped, the reaction rate is measured by continuously quenching the reaction product Na+ from the ion trap, and then destructively measuring the decay of the remaining ion population. The reactants’ electronic state and temperature are experimentally controlled, allowing us to determine the four individual reaction- rates between Na[S or P] and Ca+[S or D] at different collision energies. With the exception of the largest reaction-rate channel (Na[S] + Ca+[D]), our rates agree with classical Langevin rate limit. We have also found evidence of reactant collision-energy thresholds associated with two of the four entrance-channels.
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- 2018
28. Formation of the first portions of є- and а ' deformationinduced martensite in chromium-nickel steels of the austenitic class
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Snizhnoi, G. V.; Department of micro- and nanoelectronics, State Higher Education Establishment “Zaporizhzhya National Technical University”, 64, Zhukovskogo str., Zaporizhzhya, 69063, Mishchenko, V. G.; Department of Applied Physics, State Higher Education Establishment “Zaporizhzhya National University”, 66, Zhukovskogo str., Zaporizhzhya, 69600, Snizhnoi, V. L.; Department of Applied Physics, State Higher Education Establishment “Zaporizhzhya National University”, 66, Zhukovskogo str., Zaporizhzhya, 69600, Snizhnoi, G. V.; Department of micro- and nanoelectronics, State Higher Education Establishment “Zaporizhzhya National Technical University”, 64, Zhukovskogo str., Zaporizhzhya, 69063, Mishchenko, V. G.; Department of Applied Physics, State Higher Education Establishment “Zaporizhzhya National University”, 66, Zhukovskogo str., Zaporizhzhya, 69600, and Snizhnoi, V. L.; Department of Applied Physics, State Higher Education Establishment “Zaporizhzhya National University”, 66, Zhukovskogo str., Zaporizhzhya, 69600
- Abstract
Purpose. The first portions of the emerging є- paramagnetic and а '- ferromagnetic martensite under uniaxial compression plastic deformation moderately unstable austenite chromium-nickel X12CrNi15-16 steel experimentally fix. Methodology. Dependence of the magnetic susceptibility of the steel from the degree of deformation K and amount of а '- martensite deformation sensitive magnetometric method is found. This method influence of the magnetization of paramagnetic austenite into account. Neglecting the magnetization of paramagnetic austenite leads to significant errors in determining the very low number of а- phase, for example, the error is more than 1000 % when the content of а -phase 0.005 %, 80 % - at 0.1 %, and only in the presence of 2.5 ... 3.0 % error reaches about 3 %. Findings. In X14CrNi17-18 steel (stable austenite) during plastic deformation by compression (K = 0...67 %) the paramagnetic susceptibility increased by 4 % revealed. In this steel transformation у ^ а ' is not found. In X12CrNi15-16 steel with unstable austenite moderately depending on the degree of deformation three regions of phase transformations found. The first region of deformation: while increasing the plastic deformation (K = 0 ... 26 %) increase in the magnetic state of the austenite у ^ у ' and increase the paramagnetic susceptibility of austenite by 8 % to maximum value z ' / aX takes place. The second region: with increasing deformation (K = 26.5 ... 44 %) in the paramagnetic austenite matrix formed the first portions of the paramagnetic є- and ferromagnetic а ’ martensite deformation (у/тх ^ є + у' + а '). In this region, the amount of deformation occurring а'-martensite Ра = 0.01 ... 0.025 % is found. The third region: with increasing deformation (K = 49 ... 70 %) is transformed paramagnetic phase є and у' to maximum paramagnetic state у 'max austenite (є + у '^ у 'max, у 'max а ' ). Further accumulation of the amount of а -martensite (Ра = 0.03 ... 0.11 %) takes place. Origina, Цель. Экспериментально зафиксировать первые порции зарождающихся парамагнитного є- и ферромагнитного а - мартенситов при одноосной пластической деформации сжатием умеренно нестабильного аустенита хромоникелевой стали 12Х15Н16. Методика. Для нахождения зависимости магнитной восприимчивости аустенизированной исследуемой стали от степени деформации К и определения весьма низких содержаний зарождающегося а - мартенсита деформации использовался чувствительный магнитометрический метод, учитывающий влияние намагниченности парамагнитного аустенита. Неучет намагниченности парамагнитного аустенита приводит к значительным погрешностям определения весьма низкого количества а-фазы, например, ошибка составляет более 1000 % при содержании а-фазы 0.005 %, 80 % - при 0.1 % и лишь при наличии 2.5 ... 3.0 % ошибка достигает ~3 %. Результаты. Установлено, что в стали 14Х17Н18 со стабильным аустенитом при пластической деформации сжатием (К= 0 .6 7 %) парамагнитная восприимчивость увеличилась на 4 % и при этом не обнаружено у-^а' превращение. В стали 12Х15Н16 с умеренно нестабильным аустенитом выявлено в зависимости от степени относительной деформации К три области: 1 - в процессе увеличения пластической деформации (К = 0 .2 6 %) возрастает магнитное состояние аустенита у -^ у ', которое описывается увеличением парамагнитной восприимчивости аустенита на 8 % до постоянного максимального значения %max ; 2 - при последующем увеличении деформации (К= 26.5 ... 44 %) в полученной парамагнитной аустенитной матрице зарождаются первые порции парамагнитного є- и ферромагнитного а-мартенситов деформации (у'max ^ є + у' + а '), в этой области количество возникающего o'-мартенсита зафиксировано Ра = 0.01 ... 0.025 %; 3 - при дальнейшей деформации (К= 4 9 .7 0 %) происходит превращение парамагнитных фаз єи у в исходное максимальное парамагнитное состояние у' max аустенита (є+ у '^ у ' max, у/тах ^ а ') и дальнейшее накопление количества а - мартенсита (Ра = 0.03 ... 0.11 %). Научная новизна. Предложен, Мета. Експериментально зафіксувати перші порції парамагнітного є- і феромагнітного а - мартенситів, які зароджуються при одновісній пластичній деформації стисненням помірно нестабільного аустеніту хромонікелевої сталі 12Х15Н16. Методика. Для знаходження залежності магнітної сприйнятливості аустенізованої досліджуваної сталі від ступеня деформації К і визначення дуже низьких вмістів а - мартенситу деформації, який зароджується, використовувався чутливий магнітометричний метод, що враховує вплив намагніченості парамагнітного аустеніту. Неврахування намагніченості парамагнітного аустеніту призводить до значних похибок визначення низької кількості а-фази, наприклад, похибка складає більше 1000 % при вмісті а-фази 0.005 %, 80 % - при 0.1 % і лише за наявності 2.5 ... 3.0 % похибка досягає ~ 3 %. Результати. Встановлено, що в сталі 14Х17Н18 зі стабільним аустенітом при пластичній деформації стисненням (К= 0...67 %) парамагнітна сприйнятливість збільшилась на 4 % і при цьому не виявлено у ^ а ' перетворення. У сталі 12Х15Н16 з помірно нестабільним аустенітом виявлено залежно від ступеня відносної деформації К три області: 1 - в процесі збільшення пластичної деформації (К = 0 ... 26%) зростає магнітний стан аустеніту у - ^ у \ який описується збільшенням парамагнітної сприйнятливості аустеніту на 8 % до постійного максимального значення ; 2 - при подальшому збільшенні деформації (К =26.5 ...44 %) в отриманій парамагнітній аустенітній матриці зароджуються перші порції парамагнітного є- і феромагнітного а'- мартенситів деформації (у/шах^ £ + у /+ а /), у цій області зафіксовано кількість а'-мартенситу Р а = 0.01 ... 0.025% що виникає; 3 - при подальшій деформації (К= 49...70 %) відбувається перетворення парамагнітних фаз є і у' у вихідний максимальний парамагнітний стан у/шах аустеніту (є +у'-^у/шах, у/тах ^ а ') і подальше накопичення кількості а '- мартенситу (Ра = 0.03 ... 0.11%). Наукова новизна. Запропоновано фізичну модель зародження перших порцій є- і а '- мартенситів
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- 2015
29. The effect of the surface quality of the material on the operational properties of the heating elements
- Author
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Mishchenko, V. G.; Department of applied physics, Zaporizhia National University, Zhukovskogo str., 66, 69600, Zaporizhia, Ukraine., Tutyk, V. A.; Department of physics, National Metallurgical Academy of Ukraine, Gagarina avenue, 4, 49600, Dnepropetrovsk, Ukraine., Grechka, A. V.; Department of applied physics, Zaporizhia National University, Zhukovskogo str., 66, 69600, Zaporizhia, Ukraine., Mishchenko, V. G.; Department of applied physics, Zaporizhia National University, Zhukovskogo str., 66, 69600, Zaporizhia, Ukraine., Tutyk, V. A.; Department of physics, National Metallurgical Academy of Ukraine, Gagarina avenue, 4, 49600, Dnepropetrovsk, Ukraine., and Grechka, A. V.; Department of applied physics, Zaporizhia National University, Zhukovskogo str., 66, 69600, Zaporizhia, Ukraine.
- Abstract
Purpose. To improve durability and trouble-free operation of electric furnaces it is required to ensure reliable operation of their most important element - heater. As a material for heating elements heat-resistant steels and alloys shall be used. Extensive application among them find Fe-Cr-Al alloys. To increase durability of the heaters it is required to improve surface quality of the heaters and, consequently, technological and service properties. Methodology. The article describes the main factors which affect the process of formation of dense oxide films, analyzed defects that are observed on the surface of the wire, used for manufacture of heating elements of electric resistance furnaces. It shows that ensuring formation of dense and adherent scale of protective oxide films such as spinels FeO-(AhO3, &2O3) on metal surface, plays an important role in improvement of corrosion resistance. Findings. During the study of the surface layer of wires Х15Ю5, Х20Н80 it was found that on the surface of the metal there were defects formed during the factory production of the wires. The article presents a comparative analysis of the surface of steel wire 03Х23Ю5Т before vapor-plasma discharge treatment and after the treatment which lasted for 30 seconds and 6 minutes. Originality. Researchers have extensively studied the effect of reactive alloying elements Ca, Ce, La, Y, on the properties of protective oxide films: adhesive capasity of the oxide layer, its plasticity and growth rate. However, the relation between quality of the surface of the wire for the heaters and technological, operational properties has not been established. Practical significance. Service life of a furnace before the overhaul is directly connected with the service life of heating elements. Consequently, increasing the service life of the heater is an important issue, both from technical and economical points of view. Necessity for use of joint integrated modification with additional vapor-plasma, Цель. Для повышения долговечности и безотказной работы электрических печей сопротивления требуется обеспечить надежную работу его наиболее важного элемента - нагревателя. В качестве материала для элементов сопротивления используются жаростойкие стали и сплавы, широкое применение среди них находят железохромалюминиевые сплавы: фехрали и хромали. Для повышения срока службы нагревателей необходимо повышение качества поверхности нагревателей и, следовательно, технологических и служебных свойств. Методика. В статье рассмотрены основные факторы, влияющие на процесс образования плотных окисных пленок, проанализированы дефекты, которые наблюдаются на поверхности проволоки, применяемой для изготовления нагревательных элементов электрических печей сопротивления. Показано, что обеспечение образования плотного, прочно сцепленного слоя защитных окисных пленок типа шпинелей FeO-(AhO3, СГ2О3) на поверхности металла, играет большую роль в повышении коррозионной стойкости. Результаты. При исследовании поверхностного слоя проволоки марок Х15Ю5, Х20Н80 установлено, что на поверхности металла присутствуют дефекты, образовавшиеся в процессе производства проволоки в заводских условиях. В статье проводится сравнительный анализ поверхности проволоки из стали 03Х23Ю5Т до обработки пароплазменным разрядом и после обработки в течение 30 секунд и 6 минут. Научная новизна. Исследователями широко изучалось влияние реактивных легирующих элементов Ca, Ce, La, Y, на свойства защитных оксидных пленок: адгезионную способность оксидного слоя, его пластичность и скорость роста. Однако взаимосвязь между качеством поверхности проволоки для нагревателей и технологическими, эксплуатационными свойства не была установлена. Практическая значимость. Срок службы печи до капитального ремонта напрямую связан со сроком службы нагревательных элементов, следовательно, увеличение срока службы нагревателя является важной задачей, как с технической, так и с экономической точки зрения. Выявлена и обоснована необходимост, Мета. Для підвищення довговічності і безвідмовної роботи електричних печей опору потрібно забезпечити надійну роботу його найбільш важливого елемента - нагрівача. В якості матеріалу для елементів опору використовуються жаростійкі сталі і сплави, широке застосування серед них знаходять залізохромалюмінієві сплави: фехралі і хромалі. Для підвищення терміну служби нагрівачів необхідно підвищення якості поверхні нагрівачів і, отже, технологічних і службових властивостей. Методика. У статті розглянуті основні фактори, що впливають на процес утворення щільних окисних плівок, проаналізовано дефекти, які спостерігаються на поверхні дроту, що застосовується для виготовлення нагрівальних елементів електричних печей опору. Показано, що забезпечення утворення щільного, міцно зчепленого шару захисних окисних плівок типу шпінелей FeO-(AhO3, &2O3) на поверхні металу, грає велику роль у підвищенні корозійної стійкості. Результати. При дослідженні поверхневого шару дроту марок Х15Ю5, Х20Н80 встановлено, що на поверхні металу присутні дефекти, що утворилися в процесі виробництва дроту в заводських умовах. У статті проводиться порівняльний аналіз поверхні дроту зі сталі 03Х23Ю5Т до обробки пароплазмовим розрядом і після обробки протягом 30 секунд і 6 хвилин. Наукова новизна. Науковцями широко вивчався вплив реактивних легуючих елементів Ca, Ce, La, Y, на властивості захисних оксидних плівок: адгезійну здатність оксидного шару, його пластичність і швидкість росту. Однак взаємозв'язок між якістю поверхні дроту для нагрівачів і технологічними, експлуатаційними властивостями не був встановлений. Практична значимість. Термін служби печі до капітального ремонту безпосередньо пов'язаний з терміном служби нагрівальних елементів, отже, збільшення терміну служби нагрівача є важливим завданням, як з технічної, так і з економічної точки зору. Виявлено та обґрунтовано необхідність використання спільного комплексне модифікування з додатковою обробкою ППР для підвищення технологічних та експлуат
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- 2015
30. Parameters control of steel diffusion layer in the process of thermochemical treatment
- Author
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Meniailo, О. І.; Department of Applied Physics, State Higher Education Establishment "Zaporizhzhya National University", 66, Zhukovsky str., Zaporizhzhya 69600, Ukraine, Mishchenko, V. G.; Department of Applied Physics, State Higher Education Establishment "Zaporizhzhya National University", 66, Zhukovsky str.,Zaporizhzhya 69600, Ukraine, Meniailo, О. І.; Department of Applied Physics, State Higher Education Establishment "Zaporizhzhya National University", 66, Zhukovsky str., Zaporizhzhya 69600, Ukraine, and Mishchenko, V. G.; Department of Applied Physics, State Higher Education Establishment "Zaporizhzhya National University", 66, Zhukovsky str.,Zaporizhzhya 69600, Ukraine
- Abstract
Purpose. The aim of this study is to develop and to test management system TCT, which allows to get the required parameters of the diffusion layer - saturating concentration of the element C and the gradient of its distribution, as well as the thickness of the layer B to products of critical appointment. Methodology. As the material for research is selected the steel of the type 14ХГСН2МА which was influenced bu carburizing in solid carburizer at 1300 K. In order to study the kinetics of diffusion saturation (cementation) was used differential dilatometer. Findings. The laws of change of the linear dimensions of the sample tube differential dilatometer during the entire cycle of carburizing steel 14ХГСН2МА. The use of standard hollow instead of a solid, greatly improving the accuracy of fixing the beginning of diffusion saturation, which can be explained by more rapid heating of the hollow standard. This shown that the constructed dilatometric curves allow to identify and prevent saturation directly in the process of such undesirable processes as decarburization and sudden cessation of diffusion saturation with insufficient activity saturating the atmosphere. After reaching the temperature of carburizing steel 14ХГСН2МА (1300 K) there was an increase over time elongated tubular sample. These results confirmed the theoretical calculations of the length of the tubular sample based on the data dependence of the lattice parameter of austenite on the content of carbon in it. Also, using the results of chemical analysis and metallographic analysis supersaturation prototypes carbon steel 14ХГСН2МА and ways saturation mode to obtain the required parameters of cemented layer. Originality. For the first time to monitor and control the process suggested the use of steel TCT differential dilatometer. We give the design features, the operating principle of the device and its proper use as an example of carburizing steel 14ХГСН2МА. Practical value. It is shown that by using diffe, Цель. Целью данной работы была разработка и испытание системы управления ХТО, которая позволяет гарантированно получать необходимые параметры диффузионного слоя - концентрацию насыщающего элемента С и градиент его распределения, а также толщину слоя B для изделий ответственного назначения. Методика. Материалом для исследований выбрана сталь марки 14ХГСН2МА, которую подвергали цементации в твёрдом карбюризаторе при температуре 1300 К. Для исследования кинетики диффузионного насыщения (цементации) был использован дифференциальный дилатометр. Результаты. Установлены закономерности изменения линейных размеров трубчатого образца дифференциального дилатометра в процессе всего периода цементации стали 14ХГСН2МА. Использование пустотелого эталона вместо сплошного позволило значительно повысить точность фиксации начала процесса диффузионного насыщения, что можно объяснить более ускоренным прогревом пустотелого эталона. В работе показано, что построенные дилатометричекие кривые дают возможность определить и предотвратить непосредственно в процессе насыщения такие нежелательные процессы, как обезуглероживание и внезапное прекращение диффузионного насыщения при недостаточной активности насыщающей атмосферы. После выхода на температуру цементации стали 14ХГСН2МА (1300 К) наблюдалось удлинение трубчатого образца. Указанные результаты подтверждены теоретическими расчетами длины трубчатого образца на основании данных зависимости параметра решетки аустенита от содержания в нём углерода. Также, с помощью результатов метоллографического и химического анализа установлено пересыщение опытных образцов стали 14ХГСН2МА углеродом и предложены режимы насыщения для получения требуемых параметров цементированного слоя. Научная новизна. Впервые для контроля и управления процесса ХТО стали предложено использование дифференциального дилатометра. В работе указаны особенности конструкции, принцип работы прибора и правила его эксплуатации на примере цементации стали 14ХГСН2МА. Практическая значимост, Мета. Метою даної роботи була розробка та випробування системи керування ХТО, яка дозволяє гарантовано отримувати необхідні параметри дифузійного шару - концентрацію насичуваного елементу С і градієнт його розподілу, а також товщину шару B для виробів відповідального призначення. Методика. Матеріалом для досліджень вибрана сталь марки 14ХГСН2МА, яку піддавали цементації у твердому карбюризаторі при температурі 1300 К. Для дослідження кінетики дифузійного насичення (цементації) був використаний диференційний дилатометр. Результати Встановлено закономірності зміни лінійних розмірів трубчастого зразка диференційного дилатометру в процесі всього періоду цементації сталі 14ХГСН2МА. Використання пустотілого еталону замість суцільного дозволило значно підвищити точність фіксації початку процесу дифузійного насичення, що можна пояснити більш прискореним перегріванням пустотілого еталону. У роботі показано, що побудовані дилатометричні криві дають можливість визначити і запобігти безпосередньо в процесі насичення таким небажаним процесам, як зневуглецювання і раптове припинення дифузійного насичення при недостатній активності насичуючої атмосфери. Після виходу на температуру цементації сталі 14ХГСН2МА (1300 К) спостерігалося видовження трубчастого зразка. Зазначені результати підтверджені теоретичними розрахунками довжини трубчастого зразка на підставі даних залежності параметра гратки аустеніту від вмісту в ньому вуглецю. Також, за допомогою результатів металографічного та хімічного аналізу встановлено пересичення дослідних зразків сталі 14ХГСН2МА вуглецем та запропоновано режими насичення для отримання необхідних параметрів цементованого шару. Наукова новизна. Вперше для контролю та керування процесу ХТО сталі запропоновано використання диференціального дилатометру. У роботі вказані особливості конструкції, принцип роботи приладу та правила його експлуатації на прикладі цементації сталі 14ХГСН2МА. Практична значимість. Показано, що за допомогою диференційного дилатометру і
- Published
- 2015
31. Large-array beamforming and gain in random multimode channels: Basic physical aspects and performance estimations
- Author
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This research was supported in part by the Russian Government under the Agreement with Lobachevsky University of Nizhny Novgorod (No. 11.G34.31.0048) and by the RAS under the Program “Fundamentals of Acoustic Diagnostics of Artificial and Natural Media”., Malekhanov, Alexander I.; Institute of Applied Physics, Russian Academy of Sciences, Smirnov, A. V.; Institute of Applied Physics, Russian Academy of Sciences, This research was supported in part by the Russian Government under the Agreement with Lobachevsky University of Nizhny Novgorod (No. 11.G34.31.0048) and by the RAS under the Program “Fundamentals of Acoustic Diagnostics of Artificial and Natural Media”., Malekhanov, Alexander I.; Institute of Applied Physics, Russian Academy of Sciences, and Smirnov, A. V.; Institute of Applied Physics, Russian Academy of Sciences
- Abstract
An intrinsic issue of large-array beamforming and signal processing in random-inhomogeneous environments is known to be considerable degradation of signal coherence in space domain. Such a scenario arises in many applications, and array operations in underwater sound channels with emphasis on long-range sound propagation is one of the most typical cases. Another key issue is here the multimode propagation of the desired signal (and, generally, noise interference) so the spatial spectrum of the received field consists of numerous harmonics even for a single point source. In this paper, our focus is to demonstrate numerically the multimode signal coherence degradation at the large-array input, both for horizontal and vertical arrays in an underwater channel, and to predict the coherence effects on the output performance, array beampattern and gain included. The vertical array operation is emphasized to be the most interesting problem here due to the specific features of ambient noise in real oceanic channels. An essential conclusion concerns the fact that not only the signal coherence but signal localization in mode domain as is compared with the ambient noise affect together the array output performance.
- Published
- 2015
32. Affinity of Polyclonal IgG and F(ab')2 Fragments for Different Polymeric Surfaces
- Author
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Ortega Vinuesa, J. L.; Biocolloid and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071, Jose Galvez Ruiz, M.; Biocolloid and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071, Hidalgo Alvarez, R.; Biocolloid and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071, Ortega Vinuesa, J. L.; Biocolloid and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071, Jose Galvez Ruiz, M.; Biocolloid and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071, and Hidalgo Alvarez, R.; Biocolloid and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071
- Abstract
In this paper we show experimental data of antibody adsorption isotherms onto polystyrene surfaces. These values corroborate the important role played by both the electrostatic and the hydrophobic interactions in protein adsorption processes. To do that, we have worked with a well-known protein (IgG) and its F(ab')2 fragment. Both macromolecules differ in isoelectric points and molecular weights. The first factor allows us to study the influence of the electrostatic forces that come into play if the adsorption isotherms are carried out at different pHs in low ionic strength media. In addition, we have used four different colloidal polymer particles (latex) in order to analyze the importance of the hydrophobic driving force for protein adsorption. Our results clearly indicate that: (i) the most hydrophobic latex adsorbs the maximum amounts of both antibody molecules, and (ii) the highest affinity shown by antibodies for sorbent surfaces is found when both have opposite sign of charge, that is, under favourable electrostatic interaction conditions. On the other hand, when adsorbing IgG and F(ab')2 as a function of pH at low ionic strength media, a maximum amount of adsorbed antibodies is observed near the isoelectric point of the protein-latex complex. Finally, we have also quantified the adsorption affinity using a thermodynamic equation that allows us to calculate the standard free energy for the transfer of one mole of protein from bulk water to the surface.
- Published
- 2015
33. Use of n-Octyl-b-D-Thioglucopyranoside in the Isolation of a Bacterial Membrane Protein: An Improved Method for Immunological Applications
- Author
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Peula-Garcia, J. M.; Amphiphilic Systems and Structured Fluids Group, Deparatment of Applied Physics II, Campus de Teatinos, University of Malaga, 29071, Malaga, Rojas, J.; VIRCELL SL, Pol. Industrial “Dos de Octubreâ€, 18320, Santa Fe, Granada, Camacho, A. G.; VIRCELL SL, Pol. Industrial “Dos de Octubreâ€, 18320, Santa Fe, Granada, Molina-Bolivar, J. A.; Amphiphilic Systems and Structured Fluids Group, Deparatment of Applied Physics II, Campus de Teatinos, University of Malaga, 29071, Malaga, Aguiar, J.; Amphiphilic Systems and Structured Fluids Group, Deparatment of Applied Physics II, Campus de Teatinos, University of Malaga, 29071, Malaga, Carnero Ruiz, C.; Amphiphilic Systems and Structured Fluids Group, Deparatment of Applied Physics II, Campus de Teatinos, University of Malaga, 29071, Malaga, Peula-Garcia, J. M.; Amphiphilic Systems and Structured Fluids Group, Deparatment of Applied Physics II, Campus de Teatinos, University of Malaga, 29071, Malaga, Rojas, J.; VIRCELL SL, Pol. Industrial “Dos de Octubreâ€, 18320, Santa Fe, Granada, Camacho, A. G.; VIRCELL SL, Pol. Industrial “Dos de Octubreâ€, 18320, Santa Fe, Granada, Molina-Bolivar, J. A.; Amphiphilic Systems and Structured Fluids Group, Deparatment of Applied Physics II, Campus de Teatinos, University of Malaga, 29071, Malaga, Aguiar, J.; Amphiphilic Systems and Structured Fluids Group, Deparatment of Applied Physics II, Campus de Teatinos, University of Malaga, 29071, Malaga, and Carnero Ruiz, C.; Amphiphilic Systems and Structured Fluids Group, Deparatment of Applied Physics II, Campus de Teatinos, University of Malaga, 29071, Malaga
- Abstract
Surfactants are essential in the isolation of integral membrane biomolecules from biological membranes of different microorganisms. Our objective is the isolation of the major outer membrane protein (MOMP) of Chlamydia trachomatis, to use it in the preferential and specific detection of immunoglobulins. We have improved a method using an alkylglycoside surfactant, n-Octyl-b-D-thioglucoside (OTG), which is a non-ionic detergent used in membrane solubilization due to its "weak" action preserving the biological and functional properties of solubilized biomolecules. Different solubilization conditions, such as surfactant and salt concentrations, temperature and the presence of additive (di-thiothreitol (DTT)), were tested. To know the influence of the parameters previously indicated on the micellar properties and the solubilizing ability of the surfactant, we have studied the micellization process of OTG under several conditions by using static fluorescence measurements. MOMP was isolated by a simplified method consisting of a two-step extraction using OTG and DTT with an optimization of the experimental conditions. In this way, MOMP turns out to be separated from other biomolecules (i.e., lipopolysaccharides) in order to avoid immunological cross-reactions among the different chlamydial species. Furthermore, gel electrophoresis experiments showed monomeric MOMP without multi-aggregation, even after removing DTT and OTG molecules by dialysis of the OTG-DTT soluble fraction. The isolated protein (MOMP) is used to coat microplate wells to develop immunoenzymatic assays (ELISA). The preliminary immunological study shows the detection of specific IgG of Chlamydia trachomatis, with adequate values of the immunological parameters: sensibility and specificity. Moreover, these results show the role of surfactant molecules in the binding process of proteins to solid-liquid interface.
- Published
- 2015
34. Electrokinetic Analysis of the Influence of Additives on Calcium Oxalate Crystallization
- Author
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Callejas, J.; Biocolloids and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071 Granada, Martinez, R.; Biocolloids and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071 Granada, De Las Nieves, F. J.; Biocolloids and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071 Granada, Hidalgo-Alvarez, R.; Biocolloids and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071 Granada, Callejas, J.; Biocolloids and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071 Granada, Martinez, R.; Biocolloids and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071 Granada, De Las Nieves, F. J.; Biocolloids and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071 Granada, and Hidalgo-Alvarez, R.; Biocolloids and Fluid Physics Group, Department of Applied Physics, University of Granada, 18071 Granada
- Abstract
The Calcium Oxalate crystallization is of special interest because of its wide-spread occurrence in biomineralization processes [I-51. The formation of renal stones involves very often the precipitation of calcium oxalates. Calcium oxalate inonohydrate (COM) and calcium oxalate dihydrate (COD) are the crystalline fomls of calcium oxalate (CaOx) most commonly found in kidney stones [S]. Although thermodynamically unstable with respect to the monohydrate the COD is more commonly seen in urine [6].
- Published
- 2015
35. ESTIMATION OF PARTIAL DISCHARGE PARAMETERS IN GIS USING ACOUSTIC EMISSION TECHNIQUES
- Author
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GUPTA, N. and RAMU, T.S.
- Published
- 2001
- Full Text
- View/download PDF
36. Seasonal Noise Versus Subseasonal Signal: Forecasts of California Precipitation During the Unusual Winters of 2015–2016 and 2016–2017
- Author
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Wang, Shuguang, Anichowski, Alek J., Tippett, Michael K., Sobel, Adam H., and Columbia University. Applied Physics And Applied Mathematics
- Subjects
Environmental sciences ,Precipitation variability ,Atmospherics ,Atmospheric physics ,Weather forecasting - Abstract
Subseasonal forecasts of California precipitation during the unusual winters of 2015–2016 and 2016–2017 are examined in this study. It is shown that two different ensemble forecast systems were able to predict monthly precipitation anomalies in California during these periods with some skill in forecasts initialized near or at the start of the month. The unexpected anomalies in February 2016, as well as in January and February 2017, were associated with shifts in the position of the jet stream over the northeast Pacific in a manner broadly consistent with associations found in larger ensembles of forecasts. These results support the broader notion that what is unpredictable atmospheric noise at the seasonal time scale can become predictable signal at the subseasonal time scale, despite that the lead times and verification averaging times associated with these forecasts are outside the predictability horizons of canonical midrange weather forecasting.
- Published
- 2017
- Full Text
- View/download PDF
37. Long-range pseudorapidity dihadron correlations in d+Au collisions at sNN=200 GeV
- Author
-
Adamczyk, L.AGH University of Science and Technology, Cracow, 30-059, Poland, Adkins, J.K.(University of Kentucky, Lexington, KY, 40506-0055, USA), Agakishiev, G.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Aggarwal, M.M.(Panjab University, Chandigarh, 160014, India), Ahammed, Z.(Variable Energy Cyclotron Centre, Kolkata, 700064, India), Alekseev, I.(Alikhanov Institute for Theoretical and Experimental Physics, Moscow, 117218, Russia), Alford, J.(Kent State University, Kent, OH, 44242, USA), Aparin, A.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Arkhipkin, D.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Aschenauer, E.C.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Averichev, G.S.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Banerjee, A.(Variable Energy Cyclotron Centre, Kolkata, 700064, India), Bellwied, R.(University of Houston, Houston, TX, 77204, USA), Bhasin, A.(University of Jammu, Jammu, 180001, India), Bhati, A.K.(Panjab University, Chandigarh, 160014, India), Bhattarai, P.(University of Texas, Austin, TX, 78712, USA), Bielcik, J.(Czech Technical University in Prague, FNSPE, Prague, 115 19, Czech Republic), Bielcikova, J.(Nuclear Physics Institute AS CR, Řež/Prague, 250 68, Czech Republic), Bland, L.C.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Bordyuzhin, I.G.(Alikhanov Institute for Theoretical and Experimental Physics, Moscow, 117218, Russia), Bouchet, J.(Kent State University, Kent, OH, 44242, USA), Brandin, A.V.(Moscow Engineering Physics Institute, Moscow, 115409, Russia), Bunzarov, I.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Burton, T.P.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Butterworth, J.(Rice University, Houston, TX, 77251, USA), Caines, H.(Yale University, New Haven, CT, 06520, USA), Calder'on de la Barca S'anchez, M.(University of California, Davis, CA, 95616, USA), Campbell, J.M.(Ohio State University, Columbus, OH, 43210, USA), Cebra, D.(University of California, Davis, CA, 95616, USA), Cervantes, M.C.(Texas A&M University, College Station, TX, 77843, USA), Chakaberia, I.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Chaloupka, P.(Czech Technical University in Prague, FNSPE, Prague, 115 19, Czech Republic), Chang, Z.(Texas A&M University, College Station, TX, 77843, USA), Chattopadhyay, S.(Variable Energy Cyclotron Centre, Kolkata, 700064, India), Chen, J.H.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Chen, X.(Institute of Modern Physics, Lanzhou, 730000, China), Cheng, J.(Tsinghua University, Beijing, 100084, China), Cherney, M.(Creighton University, Omaha, NE, 68178, USA), Christie, W.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Codrington, M.J.M.(University of Texas, Austin, TX, 78712, USA), Contin, G.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Crawford, H.J.(University of California, Berkeley, CA, 94720, USA), Das, S.(Institute of Physics, Bhubaneswar, 751005, India), De Silva, L.C.(Creighton University, Omaha, NE, 68178, USA), Debbe, R.R.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Dedovich, T.G.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Deng, J.(Shandong University, Jinan, Shandong, 250100, China), Derevschikov, A.A.(Institute of High Energy Physics, Protvino, 142281, Russia), di Ruzza, B.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Didenko, L.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Dilks, C.(Pennsylvania State University, University Park, PA, 16802, USA), Dong, X.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Drachenberg, J.L.(Valparaiso University, Valparaiso, IN, 46383, USA), Draper, J.E.(University of California, Davis, CA, 95616, USA), Du, C.M.(Institute of Modern Physics, Lanzhou, 730000, China), Dunkelberger, L.E.(University of California, Los Angeles, CA, 90095, USA), Dunlop, J.C.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Efimov, L.G.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Engelage, J.(University of California, Berkeley, CA, 94720, USA), Eppley, G.(Rice University, Houston, TX, 77251, USA), Esha, R.(University of California, Los Angeles, CA, 90095, USA), Evdokimov, O.(University of Illinois at Chicago, Chicago, IL, 60607, USA), Eyser, O.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Fatemi, R.(University of Kentucky, Lexington, KY, 40506-0055, USA), Fazio, S.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Federic, P.(Nuclear Physics Institute AS CR, Řež/Prague, 250 68, Czech Republic), Fedorisin, J.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Feng, None(Central China Normal University (HZNU), Wuhan, 430079, China), Filip, P.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Fisyak, Y.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Flores, C.E.(University of California, Davis, CA, 95616, USA), Fulek, L.(AGH University of Science and Technology, Cracow, 30-059, Poland), Gagliardi, C.A.(Texas A&M University, College Station, TX, 77843, USA), Garand, D.(Purdue University, West Lafayette, IN, 47907, USA), Geurts, F.(Rice University, Houston, TX, 77251, USA), Gibson, A.(Valparaiso University, Valparaiso, IN, 46383, USA), Girard, M.(Warsaw University of Technology, Warsaw, 00-661, Poland), Greiner, L.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Grosnick, D.(Valparaiso University, Valparaiso, IN, 46383, USA), Gunarathne, D.S.(Temple University, Philadelphia, PA, 19122, USA), Guo, Y.(University of Science and Technology of China, Hefei, 230026, China), Gupta, S.(University of Jammu, Jammu, 180001, India), Gupta, A.(University of Jammu, Jammu, 180001, India), Guryn, W.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Hamad, A.(Kent State University, Kent, OH, 44242, USA), Hamed, A.(Texas A&M University, College Station, TX, 77843, USA), Haque, R.(National Institute of Science Education and Research, Bhubaneswar, 751005, India), Harris, J.W.(Yale University, New Haven, CT, 06520, USA), He, L.(Purdue University, West Lafayette, IN, 47907, USA), Heppelmann, S.(Pennsylvania State University, University Park, PA, 16802, USA), Hirsch, A.(Purdue University, West Lafayette, IN, 47907, USA), Hoffmann, G.W.(University of Texas, Austin, TX, 78712, USA), Hofman, D.J.(University of Illinois at Chicago, Chicago, IL, 60607, USA), Horvat, S.(Yale University, New Haven, CT, 06520, USA), Huang, H.Z.(University of California, Los Angeles, CA, 90095, USA), Huang, X.(Tsinghua University, Beijing, 100084, China), Huang, B.(University of Illinois at Chicago, Chicago, IL, 60607, USA), Huck, P.(Central China Normal University (HZNU), Wuhan, 430079, China), Humanic, T.J.(Ohio State University, Columbus, OH, 43210, USA), Igo, G.(University of California, Los Angeles, CA, 90095, USA), Jacobs, W.W.(Indiana University, Bloomington, IN, 47408, USA), Jang, H.(Korea Institute of Science and Technology Information, Daejeon, 305-701, Republic of Korea), Jiang, K.(University of Science and Technology of China, Hefei, 230026, China), Judd, E.G.(University of California, Berkeley, CA, 94720, USA), Kabana, S.(Kent State University, Kent, OH, 44242, USA), Kalinkin, D.(Alikhanov Institute for Theoretical and Experimental Physics, Moscow, 117218, Russia), Kang, K.(Tsinghua University, Beijing, 100084, China), Kauder, K.(University of Illinois at Chicago, Chicago, IL, 60607, USA), Ke, H.W.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Keane, D.(Kent State University, Kent, OH, 44242, USA), Kechechyan, A.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Khan, Z.H.(University of Illinois at Chicago, Chicago, IL, 60607, USA), Kikola, D.P.(Warsaw University of Technology, Warsaw, 00-661, Poland), Kisel, I.(Frankfurt Institute for Advanced Studies FIAS, Frankfurt, 60438, Germany), Kisiel, A.(Warsaw University of Technology, Warsaw, 00-661, Poland), Koetke, D.D.(Valparaiso University, Valparaiso, IN, 46383, USA), Kollegger, T.(Frankfurt Institute for Advanced Studies FIAS, Frankfurt, 60438, Germany), Kosarzewski, L.K.(Warsaw University of Technology, Warsaw, 00-661, Poland), Kotchenda, L.(Moscow Engineering Physics Institute, Moscow, 115409, Russia), Kraishan, A.F.(Temple University, Philadelphia, PA, 19122, USA), Kravtsov, P.(Moscow Engineering Physics Institute, Moscow, 115409, Russia), Krueger, K.(Argonne National Laboratory, Argonne, IL, 60439, USA), Kulakov, I.(Frankfurt Institute for Advanced Studies FIAS, Frankfurt, 60438, Germany), Kumar, L.(Panjab University, Chandigarh, 160014, India), Kycia, R.A.(Institute of Nuclear Physics PAN, Cracow, 31-342, Poland), Lamont, M.A.C.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Landgraf, J.M.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Landry, K.D.(University of California, Los Angeles, CA, 90095, USA), Lauret, J.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Lebedev, A.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Lednicky, R.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Lee, J.H.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Li, X.(Temple University, Philadelphia, PA, 19122, USA), Li, X.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Li, W.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Li, Z.M.(Central China Normal University (HZNU), Wuhan, 430079, China), Li, Y.(Tsinghua University, Beijing, 100084, China), Li, C.(University of Science and Technology of China, Hefei, 230026, China), Lisa, M.A.(Ohio State University, Columbus, OH, 43210, USA), Liu, F.(Central China Normal University (HZNU), Wuhan, 430079, China), Ljubicic, T.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Llope, W.J.(Wayne State University, Detroit, MI, 48201, USA), Lomnitz, M.(Kent State University, Kent, OH, 44242, USA), Longacre, R.S.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Luo, X.(Central China Normal University (HZNU), Wuhan, 430079, China), Ma, L.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Ma, R.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Ma, G.L.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Ma, Y.G.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Magdy, N.(World Laboratory for Cosmology and Particle Physics (WLCAPP), Cairo, 11571, Egypt), Majka, R.(Yale University, New Haven, CT, 06520, USA), Manion, A.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Margetis, S.(Kent State University, Kent, OH, 44242, USA), Markert, C.(University of Texas, Austin, TX, 78712, USA), Masui, H.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Matis, H.S.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), McDonald, D.(University of Houston, Houston, TX, 77204, USA), Meehan, K.(University of California, Davis, CA, 95616, USA), Minaev, N.G.(Institute of High Energy Physics, Protvino, 142281, Russia), Mioduszewski, S.(Texas A&M University, College Station, TX, 77843, USA), Mohanty, B.(National Institute of Science Education and Research, Bhubaneswar, 751005, India), Mondal, M.M.(Texas A&M University, College Station, TX, 77843, USA), Morozov, D.A.(Institute of High Energy Physics, Protvino, 142281, Russia), Mustafa, M.K.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Nandi, B.K.(Indian Institute of Technology, Mumbai, 400076, India), Nasim, Md.(University of California, Los Angeles, CA, 90095, USA), Nayak, T.K.(Variable Energy Cyclotron Centre, Kolkata, 700064, India), Nigmatkulov, G.(Moscow Engineering Physics Institute, Moscow, 115409, Russia), Nogach, L.V.(Institute of High Energy Physics, Protvino, 142281, Russia), Noh, S.Y.(Korea Institute of Science and Technology Information, Daejeon, 305-701, Republic of Korea), Novak, J.(Michigan State University, East Lansing, MI, 48824, USA), Nurushev, S.B.(Institute of High Energy Physics, Protvino, 142281, Russia), Odyniec, G.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Ogawa, A.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Oh, K.(Pusan National University, Pusan, 609735, Republic of Korea), Okorokov, V.(Moscow Engineering Physics Institute, Moscow, 115409, Russia), Olvitt, D.L.(Temple University, Philadelphia, PA, 19122, USA), Page, B.S.(Indiana University, Bloomington, IN, 47408, USA), Pan, Y.X.(University of California, Los Angeles, CA, 90095, USA), Pandit, Y.(University of Illinois at Chicago, Chicago, IL, 60607, USA), Panebratsev, Y.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Pawlak, T.(Warsaw University of Technology, Warsaw, 00-661, Poland), Pawlik, B.(Institute of Nuclear Physics PAN, Cracow, 31-342, Poland), Pei, H.(Central China Normal University (HZNU), Wuhan, 430079, China), Perkins, C.(University of California, Berkeley, CA, 94720, USA), Peterson, A.(Ohio State University, Columbus, OH, 43210, USA), Pile, P.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Planinic, M.(University of Zagreb, Zagreb, HR-10002, Croatia), Pluta, J.(Warsaw University of Technology, Warsaw, 00-661, Poland), Poljak, N.(University of Zagreb, Zagreb, HR-10002, Croatia), Poniatowska, K.(Warsaw University of Technology, Warsaw, 00-661, Poland), Porter, J.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Posik, M.(Temple University, Philadelphia, PA, 19122, USA), Poskanzer, A.M.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Pruthi, N.K.(Panjab University, Chandigarh, 160014, India), Putschke, J.(Wayne State University, Detroit, MI, 48201, USA), Qiu, H.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Quintero, A.(Kent State University, Kent, OH, 44242, USA), Ramachandran, S.(University of Kentucky, Lexington, KY, 40506-0055, USA), Raniwala, R.(University of Rajasthan, Jaipur, 302004, India), Raniwala, S.(University of Rajasthan, Jaipur, 302004, India), Ray, R.L.(University of Texas, Austin, TX, 78712, USA), Ritter, H.G.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Roberts, J.B.(Rice University, Houston, TX, 77251, USA), Rogachevskiy, O.V.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Romero, J.L.(University of California, Davis, CA, 95616, USA), Roy, A.(Variable Energy Cyclotron Centre, Kolkata, 700064, India), Ruan, L.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Rusnak, J.(Nuclear Physics Institute AS CR, Řež/Prague, 250 68, Czech Republic), Rusnakova, O.(Czech Technical University in Prague, FNSPE, Prague, 115 19, Czech Republic), Sahoo, N.R.(Texas A&M University, College Station, TX, 77843, USA), Sahu, P.K.(Institute of Physics, Bhubaneswar, 751005, India), Sakrejda, I.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Salur, S.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Sandacz, A.(Warsaw University of Technology, Warsaw, 00-661, Poland), Sandweiss, J.(Yale University, New Haven, CT, 06520, USA), Sarkar, A.(Indian Institute of Technology, Mumbai, 400076, India), Schambach, J.(University of Texas, Austin, TX, 78712, USA), Scharenberg, R.P.(Purdue University, West Lafayette, IN, 47907, USA), Schmah, A.M.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Schmidke, W.B.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Schmitz, N.(Max-Planck-Institut fur Physik, Munich, 80805, Germany), Seger, J.(Creighton University, Omaha, NE, 68178, USA), Seyboth, P.(Max-Planck-Institut fur Physik, Munich, 80805, Germany), Shah, N.(University of California, Los Angeles, CA, 90095, USA), Shahaliev, E.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Shanmuganathan, P.V.(Kent State University, Kent, OH, 44242, USA), Shao, M.(University of Science and Technology of China, Hefei, 230026, China), Sharma, M.K.(University of Jammu, Jammu, 180001, India), Sharma, B.(Panjab University, Chandigarh, 160014, India), Shen, W.Q.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Shi, S.S.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Shou, Q.Y.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Sichtermann, E.P.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Sikora, R.(AGH University of Science and Technology, Cracow, 30-059, Poland), Simko, M.(Nuclear Physics Institute AS CR, Řež/Prague, 250 68, Czech Republic), Skoby, M.J.(Indiana University, Bloomington, IN, 47408, USA), Smirnov, N.(Yale University, New Haven, CT, 06520, USA), Smirnov, D.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Solanki, D.(University of Rajasthan, Jaipur, 302004, India), Song, L.(University of Houston, Houston, TX, 77204, USA), Sorensen, P.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Spinka, H.M.(Argonne National Laboratory, Argonne, IL, 60439, USA), Srivastava, B.(Purdue University, West Lafayette, IN, 47907, USA), Stanislaus, T.D.S.(Valparaiso University, Valparaiso, IN, 46383, USA), Stock, R.(Frankfurt Institute for Advanced Studies FIAS, Frankfurt, 60438, Germany), Strikhanov, M.(Moscow Engineering Physics Institute, Moscow, 115409, Russia), Stringfellow, B.(Purdue University, West Lafayette, IN, 47907, USA), Sumbera, M.(Nuclear Physics Institute AS CR, Řež/Prague, 250 68, Czech Republic), Summa, B.J.(Pennsylvania State University, University Park, PA, 16802, USA), Sun, Y.(University of Science and Technology of China, Hefei, 230026, China), Sun, Z.(Institute of Modern Physics, Lanzhou, 730000, China), Sun, X.M.(Central China Normal University (HZNU), Wuhan, 430079, China), Sun, X.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Surrow, B.(Temple University, Philadelphia, PA, 19122, USA), Svirida, D.N.(Alikhanov Institute for Theoretical and Experimental Physics, Moscow, 117218, Russia), Szelezniak, M.A.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Takahashi, J.(Universidade Estadual de Campinas, Sao Paulo, 13131, Brazil), Tang, A.H.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Tang, Z.(University of Science and Technology of China, Hefei, 230026, China), Tarnowsky, T.(Michigan State University, East Lansing, MI, 48824, USA), Tawfik, A.N.(World Laboratory for Cosmology and Particle Physics (WLCAPP), Cairo, 11571, Egypt), Thomas, J.H.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Timmins, A.R.(University of Houston, Houston, TX, 77204, USA), Tlusty, D.(Nuclear Physics Institute AS CR, Řež/Prague, 250 68, Czech Republic), Tokarev, M.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Trentalange, S.(University of California, Los Angeles, CA, 90095, USA), Tribble, R.E.(Texas A&M University, College Station, TX, 77843, USA), Tribedy, P.(Variable Energy Cyclotron Centre, Kolkata, 700064, India), Tripathy, S.K.(Institute of Physics, Bhubaneswar, 751005, India), Trzeciak, B.A.(Czech Technical University in Prague, FNSPE, Prague, 115 19, Czech Republic), Tsai, O.D.(University of California, Los Angeles, CA, 90095, USA), Ullrich, T.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Underwood, D.G.(Argonne National Laboratory, Argonne, IL, 60439, USA), Upsal, I.(Ohio State University, Columbus, OH, 43210, USA), Van Buren, G.(Brookhaven National Laboratory, Upton, NY, 11973, USA), van Nieuwenhuizen, G.(Massachusetts Institute of Technology, Cambridge, MA, 02139-4307, USA), Vandenbroucke, M.(Temple University, Philadelphia, PA, 19122, USA), Varma, R.(Indian Institute of Technology, Mumbai, 400076, India), Vasiliev, A.N.(Institute of High Energy Physics, Protvino, 142281, Russia), Vertesi, R.(Nuclear Physics Institute AS CR, Řež/Prague, 250 68, Czech Republic), Videbaek, F.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Viyogi, Y.P.(Variable Energy Cyclotron Centre, Kolkata, 700064, India), Vokal, S.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), Voloshin, S.A.(Wayne State University, Detroit, MI, 48201, USA), Vossen, A.(Indiana University, Bloomington, IN, 47408, USA), Wang, Y.(Central China Normal University (HZNU), Wuhan, 430079, China), Wang, F.(Purdue University, West Lafayette, IN, 47907, USA), Wang, H.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Wang, J.S.(Institute of Modern Physics, Lanzhou, 730000, China), Wang, G.(University of California, Los Angeles, CA, 90095, USA), Wang, Y.(Tsinghua University, Beijing, 100084, China), Webb, J.C.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Webb, G.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Wen, L.(University of California, Los Angeles, CA, 90095, USA), Westfall, G.D.(Michigan State University, East Lansing, MI, 48824, USA), Wieman, H.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Wissink, S.W.(Indiana University, Bloomington, IN, 47408, USA), Witt, R.(United States Naval Academy, Annapolis, MD, 21402, USA), Wu, Y.F.(Central China Normal University (HZNU), Wuhan, 430079, China), Xiao, Z.(Tsinghua University, Beijing, 100084, China), Xie, W.(Purdue University, West Lafayette, IN, 47907, USA), Xin, K.(Rice University, Houston, TX, 77251, USA), Xu, Z.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Xu, Q.H.(Shandong University, Jinan, Shandong, 250100, China), Xu, N.(Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA), Xu, H.(Institute of Modern Physics, Lanzhou, 730000, China), Xu, Y.F.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Yang, Y.(Central China Normal University (HZNU), Wuhan, 430079, China), Yang, C.(University of Science and Technology of China, Hefei, 230026, China), Yang, S.(University of Science and Technology of China, Hefei, 230026, China), Yang, Q.(University of Science and Technology of China, Hefei, 230026, China), Yang, Y.(Institute of Modern Physics, Lanzhou, 730000, China), Ye, Z.(University of Illinois at Chicago, Chicago, IL, 60607, USA), Yepes, P.(Rice University, Houston, TX, 77251, USA), Yi, L.(Purdue University, West Lafayette, IN, 47907, USA), Yip, K.(Brookhaven National Laboratory, Upton, NY, 11973, USA), Yoo, I.-K.(Pusan National University, Pusan, 609735, Republic of Korea), Yu, N.(Central China Normal University (HZNU), Wuhan, 430079, China), Zbroszczyk, H.(Warsaw University of Technology, Warsaw, 00-661, Poland), Zha, W.(University of Science and Technology of China, Hefei, 230026, China), Zhang, J.B.(Central China Normal University (HZNU), Wuhan, 430079, China), Zhang, X.P.(Tsinghua University, Beijing, 100084, China), Zhang, S.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Zhang, J.(Institute of Modern Physics, Lanzhou, 730000, China), Zhang, Z.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Zhang, Y.(University of Science and Technology of China, Hefei, 230026, China), Zhang, J.L.(Shandong University, Jinan, Shandong, 250100, China), Zhao, F.(University of California, Los Angeles, CA, 90095, USA), Zhao, J.(Central China Normal University (HZNU), Wuhan, 430079, China), Zhong, C.(Shanghai Institute of Applied Physics, Shanghai, 201800, China), Zhou, L.(University of Science and Technology of China, Hefei, 230026, China), Zhu, X.(Tsinghua University, Beijing, 100084, China), Zoulkarneeva, Y.(Joint Institute for Nuclear Research, Dubna, 141 980, Russia), and Zyzak, M.(Frankfurt Institute for Advanced Studies FIAS, Frankfurt, 60438, Germany)
- Subjects
Nuclear Experiment ,lcsh:Physics ,lcsh:QC1-999 - Abstract
Dihadron angular correlations in d+Au collisions at sNN=200 GeV are reported as a function of the measured zero-degree calorimeter neutral energy and the forward charged hadron multiplicity in the Au-beam direction. A finite correlated yield is observed at large relative pseudorapidity (Δ η ) on the near side (i.e. relative azimuth Δϕ∼0 ). This correlated yield as a function of Δ η appears to scale with the dominant, primarily jet-related, away-side ( Δϕ∼π ) yield. The Fourier coefficients of the Δ ϕ correlation, Vn=〈cosnΔϕ〉 , have a strong Δ η dependence. In addition, it is found that V1 is approximately inversely proportional to the mid-rapidity event multiplicity, while V2 is independent of it with similar magnitude in the forward ( d -going) and backward (Au-going) directions.
- Published
- 2015
38. Proceedings of the International Conference on Physics Education. (Nanjing, The People's Republic of China, August 31-September 5, 1986).
- Author
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International Union of Pure and Applied Physics.
- Abstract
This document contains 65 papers presented at the International Conference on Physics Education. Included are papers dealing with: (1) physics education in China; (2) the evaluation of physics courses in engineering colleges; (3) climate and weather; (4) the implications of physics education research for the classroom; (5) university physics teaching; (6) teacher training in developing countries; (7) community-based physics education; (8) microcomputer-aided physics teaching; (9) standardized examinations; (10) general physics experiments; (11) the application of video techniques in physics teaching; (12) training graduate students in the field of college physics education; (13) light, lasers, and holograms; (14) the reform of general physics courses; (15) scientific inquiry in computer-assisted laboratory experiments; (16) the physics of daily life; (17) the function of physics history on physics education; (18) the apparatus of the Franck-Hertz experiment; and (19) graduate courses on science teaching. (TW)
- Published
- 1986
39. Multifrequency diagnostics of inhomogeneous media
- Author
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Gaikovich, K. P.; Institute for Physics of Microstructures RAS, Maksimovitch, Ye. S.; Institute of Applied Physics National Academy of Sciences of Belarus, Badeev, V. A.; Institute of Applied Physics National Academy of Sciences of Belarus, Gaikovich, K. P.; Institute for Physics of Microstructures RAS, Maksimovitch, Ye. S.; Institute of Applied Physics National Academy of Sciences of Belarus, and Badeev, V. A.; Institute of Applied Physics National Academy of Sciences of Belarus
- Abstract
Method of electromagnetic scanning tomography and holography of subsurface objects based on the solution of inverse scattering problem for the pseudopulse synthesized by multifrequency measurements of the scattered field is studied. Results of its applications to diagnostics of various subsurface inhomogeneities are demonstrated.
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- 2014
40. Development of UWB planar dipole for near surface applications
- Author
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Maksimovitch, Ye. S.; Institute of Applied Physics National Academy of Sciences of Belarus, Badeev, V. A.; Institute of Applied Physics National Academy of Sciences of Belarus, Gaikovich, K. P.; Institute for Physics of Microstructures RAS, Petrukhin, Yu. V.; Research Institute of Modern Telecommunication Technologies, Maksimovitch, Ye. S.; Institute of Applied Physics National Academy of Sciences of Belarus, Badeev, V. A.; Institute of Applied Physics National Academy of Sciences of Belarus, Gaikovich, K. P.; Institute for Physics of Microstructures RAS, and Petrukhin, Yu. V.; Research Institute of Modern Telecommunication Technologies
- Abstract
In the article the results of numerical and experimental studies of ultra-wideband dipole radiator and optimized CPW-to-CPS transformer (balun) are presented. Such dipole is used in GPR scanning system based on the Agilent E5071B VNA, and is located in direct proximity to object surface. Different theoretical models were developed to optimize and analyze the 50 to 100 Ohms balun with passband 1-7 GHz. The special attention was paid to matching antennas open with properties of the media under test. All numerical results were performed using CST Microwave Studio software.
- Published
- 2014
41. Signal coherence and coherence-induced effects on array output in multimode transmission channels
- Author
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Malekhanov, Alexander I.; Institute of Applied Physics, Russian Academy of Sciences, Smirnov, A. V.; Institute of Applied Physics, Russian Academy of Sciences, Malekhanov, Alexander I.; Institute of Applied Physics, Russian Academy of Sciences, and Smirnov, A. V.; Institute of Applied Physics, Russian Academy of Sciences
- Abstract
It is well known that the statistical effects of long-range signal propagation in random channels generally lead to considerable degradation of both the signal coherence and the array output. In random-inhomogeneous underwater sound channels, these effects are of a primary importance if a large horizontal array is used for high-resolution operation in spatial domain. The key physical effect in such a scenario is known to be the range-dependent cross-modal coherence loss caused by multiple sound scattering by random channel inhomogeneities, both volume and windy surface ones. In this pa-per, we demonstrate numerically how and why the horizontal array output dramatically degrades if the received signal consists of a large number of partially-correlated normal modes. From the point of view of general statistical antenna theory, the results present-ed are considered to be a further development, with application to the multimode transmission channels.
- Published
- 2014
42. On the Convergence of Waveform Relaxation Methods for Differential-Functional Systems of Equations
- Author
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Bartoszewski, Z and Kwapisz, Marian
- Published
- 1999
- Full Text
- View/download PDF
43. Exact Treatment of the Pauli Exclusion Operator in Nuclear Matter Calculation
- Author
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Department of Physics, Kyushu Institute of Technology, Kitakyushu 804-8550, Japan, Physics Division, Kyushu Dental College, Kitakyushu 803-8580, Japan, Department of Applied Physics, Faculty of Engineering, Miyazaki University, Miyazaki 889-2192, Japan, Suzuki, K, Okamoto, Ryoji, Kohno, M, Nagata, S, Department of Physics, Kyushu Institute of Technology, Kitakyushu 804-8550, Japan, Physics Division, Kyushu Dental College, Kitakyushu 803-8580, Japan, Department of Applied Physics, Faculty of Engineering, Miyazaki University, Miyazaki 889-2192, Japan, Suzuki, K, Okamoto, Ryoji, Kohno, M, and Nagata, S
- Abstract
type:Journal Article, Exact expressions of the Pauli exclusion operator Q in the nuclear matter calculationare presented in detail. Exact formulae are also given for the calculations of thesingle-particle-potential energy and the binding energy per nucleon with the exactQ operator. Numerical calculations of the G matrix in the lowest-order Bruecknertheory are carried out to check the reliability of the standard angle-average approximationfor the Q operator by employing the Bonn B and C NN potentials. It isobserved that the exact treatment of the operator Q brings about non-negligibleand attractive contributions to the binding energy., source:http://www.sciencedirect.com/science/journal/03759474
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- 2017
44. Electroconvection in nematic liquid crystals in Hele-Shaw cells
- Author
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Department of Mechanical Systems Engineering, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Fukuoka 820-8502, Japan, Department of Applied Physics and Graduate School of Systems Life Science, Faculty of Engineering, Kyushu University, Fukuoka 812-8581, Japan, Huh, Jong-Hoon, Kai, Shoichi, Department of Mechanical Systems Engineering, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Fukuoka 820-8502, Japan, Department of Applied Physics and Graduate School of Systems Life Science, Faculty of Engineering, Kyushu University, Fukuoka 812-8581, Japan, Huh, Jong-Hoon, and Kai, Shoichi
- Abstract
type:Journal Article, We report electrohydrodynamic instability in nematic liquid crystals found in Hele-Shaw cells. Due to the present cell geometry, the convective structures could be directly visualized as surface or bulk flows. An unexpected structure is observed, which is completely different from the well-known patterns in the standard cells. By using the voltage-frequency jump method, the stability of a convective structure in Hele-Shaw cells is discussed in terms of the Busse diagram., source:https://doi.org/10.1103/PhysRevE.68.042702, source:http://www.aps.org
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- 2017
45. Prewavy instability of nematic liquid crystals in a high-frequency electric field
- Author
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Department of Mechanical Systems Engineering, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Fukuoka 820-8502, Japan, Department of Applied Physics, Faculty of Engineering, Kyushu University, Fukuoka 812-8581, Japan, Huh, Jong-Hoon, Yusuf, Yusril, Hidaka, Yoshiki, Kai, Shoichi, Department of Mechanical Systems Engineering, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Fukuoka 820-8502, Japan, Department of Applied Physics, Faculty of Engineering, Kyushu University, Fukuoka 812-8581, Japan, Huh, Jong-Hoon, Yusuf, Yusril, Hidaka, Yoshiki, and Kai, Shoichi
- Abstract
type:Journal Article, A kind of electrohydrodynamic instability, the prewavy instability, in nematic liquid crystals is reported. The characteristic of the instability was optically investigated and discussed in comparison with some similar instabilities. Obviously the instability partially shows an isotropic feature around the nematic-isotropic transition temperature. Owing to the characteristic properties of the flow and the spatial periodicity, it should be distinguished from a previously proposed isotropic instability., source:https://doi.org/10.1103/PhysRevE.66.031705, source:http://www.aps.org
- Published
- 2017
46. Condensation energy density properties of Ba-122 pnictide superconductor with columnar defects introduced by heavy-ion irradiation
- Author
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Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technolog, JST-TRIP, 5 Sanbancho, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technolog, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Department of Life, Environment and Materials Science, Department of Life, Environment and Materials Science, JST-TRIP, 5 Sanbancho, Department of Applied Physics, The University of Tokyo, JST-TRIP, 5 Sanbancho, Otabe, E. S., Myose, K., Murakami, K., Kiuchi, M., Matsushita, T., Ge, J., Ni, B., Nakajima, Y., Tamegai, T., Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technolog, JST-TRIP, 5 Sanbancho, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technolog, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Department of Life, Environment and Materials Science, Department of Life, Environment and Materials Science, JST-TRIP, 5 Sanbancho, Department of Applied Physics, The University of Tokyo, JST-TRIP, 5 Sanbancho, Otabe, E. S., Myose, K., Murakami, K., Kiuchi, M., Matsushita, T., Ge, J., Ni, B., Nakajima, Y., and Tamegai, T.
- Abstract
type:Journal Article, It is important to investigate condensation energy density of superconducting material, since it determines its pinning property. According to the heavy-ion irradiation, the columnar defects are introduced to the superconductor which act as the strong pinning centers, and the critical current density is enhanced by the new pinning centers. Since the number density and the size of the columnar defects can be observed, the condensation energy density is estimated by using the pinning summation theory. In the present study, we prepared Ba(Fe0.93Co0.07)2As2 (Ba-122) pnictide superconductors by self-flux method. 200 MeV Au ions were irradiated into the specimens along c-axis and the matching field was 2 T. After the irradiation, the critical current density was 6 times larger than that before the irradiation. The estimated condensation energy density is in the order of 104 J/m3 and is slightly smaller than those of cuprate superconductors. The temperature dependence is similar to that of YBa2Cu3Ox oxide superconductors, since the anisotropy parameter is small in Ba-122. Therefore, it is expected to use Ba-122 at high temperatures near the critical temperature., Superconductivity Centennial Conference 2011 - EUCAS–ISEC–ICMC, Sep 18 - 23, 2011, Hague, Netherlands, source:https://doi.org/10.1016/j.phpro.2012.06.269
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- 2017
47. Observation and determination of abnormal rolls and abnormal zigzag rolls in electroconvection in homeotropic liquid crystals
- Author
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Department of Applied Physics, Faculty of Engineering, Kyushu University, Fukuoka 812-8581, Japan, Huh, Jong-Hoon, Hidaka, Yoshiki, Kai, Shoichi, Department of Applied Physics, Faculty of Engineering, Kyushu University, Fukuoka 812-8581, Japan, Huh, Jong-Hoon, Hidaka, Yoshiki, and Kai, Shoichi
- Abstract
type:Journal Article, Direct evidence for two different types of normal rolls and of zigzag rolls in homeotropically aligned nematic liquid crystals in a magnetic field is reported. The conventional normal rolls have the reflection symmetry in the xy plane. The instability, however, breaks the reflection symmetry y→-y on the director and then the abnormal rolls are expected to be observed. We have investigated the instability experimentally and discussed it in terms of the recent numerical results by Plaut et al. [Phys. Rev. Lett. 79, 2367 (1997)]. Due to the new instability, the abnormal zigzag rolls are also found below the Lifshitz frequency., source:http://link.aps.org/abstract/PRE/v58/p7355, source:http://www.aps.org
- Published
- 2017
48. Evaluation of Critical Current Density of FeAs-based Superconductors
- Author
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Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Department of Information Electronics, Fukuoka Institute of Technology, Institute of Electrical Engineering, Chinese Academy of Science, Department Applied Physics, The University of Tokyo, TRIP-JST, Japan Science and Technology Agency, Otabe, Edmund S., Kiuchi, Masaru, Matsushita, Teruo, Ni, Baorong, Qi, Yanpeng, Wang, Lei, Gao, Zhaoshun, Wang, Dongliang, Zhang, Xianping, Ma, Yanwei, Nakajima, Yasuyuki, Tamegai, Tsuyoshi, Faculty of Computer Science and Systems Engineering, Kyushu Institute of Technology, Department of Information Electronics, Fukuoka Institute of Technology, Institute of Electrical Engineering, Chinese Academy of Science, Department Applied Physics, The University of Tokyo, TRIP-JST, Japan Science and Technology Agency, Otabe, Edmund S., Kiuchi, Masaru, Matsushita, Teruo, Ni, Baorong, Qi, Yanpeng, Wang, Lei, Gao, Zhaoshun, Wang, Dongliang, Zhang, Xianping, Ma, Yanwei, Nakajima, Yasuyuki, and Tamegai, Tsuyoshi
- Abstract
type:Journal Article, In this review paper, we report the characteristics of the critical current density in FeAs based superconductors which is newly discovered by Hosono group of Tokyo Institute of Technology on 2008. Since the many specimens in present stage are not single crystals, there are two kinds of critical current density observed in the specimens which are so-called local and global critical current densities. Therefore, it is necessary to evaluate both kinds of critical current densities. The history effect in which the global critical current density shows different values in increasing and decreasing magnetic field is also observed when the specimens have the local and the global critical current densities. The wire which critical current is 180 A is successfully developed with using the knowledge of abovementioned characteristics of two kinds of critical current densities and the history effect., source:https://doi.org/10.9714/psac.2012.14.2.001
- Published
- 2017
49. Single molecule and single quantum dot photodynamics by polarization-rotating modulation microscopy
- Author
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Institute of Symbiotic Science and Technology, Department of Applied Physics, Graduate School of Engineering, Tokyo University of Agriculture and Technology, Tani, T., Sakai, H., Usukura, E., Suzuki, T., Oda, M., Institute of Symbiotic Science and Technology, Department of Applied Physics, Graduate School of Engineering, Tokyo University of Agriculture and Technology, Tani, T., Sakai, H., Usukura, E., Suzuki, T., and Oda, M.
- Abstract
type:Journal Article, We present our recent study of polarization modulating fluorescence imaging microscopy on single CdSe colloidal quantum dots (QDs) and quantum rods (QRs) adsorbed on silica glass substrates at room temperatures. Simple optical setup is introduced to provide detection of emission profiles projected on to the sample plane as well as detection of rotating excitation polarization effect. While most studies so far in structural changes in biological or amorphous systems rely on extrinsic fluorophores with linear transition dipoles, those with twofold degenerate dipoles are noteworthy due to the intrinsic advantage for 3D orientation information. Performance of modulations is also evaluated in combination with tetramethylrodamine moieties as typical linear emitters. CdSe QDs with aspect ratio of 1.3 actually reveal plane-polarized emission at room temperature and, based on maximum-likelihood analysis, are exceptionally highly oriented on silica glass substrates., source:https://doi.org/10.1016/j.phpro.2010.01.228
- Published
- 2017
50. Versatile implementation in angle-resolved optical microscopy: its application to local spectrometry of microcavities with PIC-J-aggregates
- Author
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Department of Applied Physics Graduate School of Engineering, Tokyo University of Agriculture and Technology, Obara, Y., K., Saitoh, Oda, M., Tani, T., Department of Applied Physics Graduate School of Engineering, Tokyo University of Agriculture and Technology, Obara, Y., K., Saitoh, Oda, M., and Tani, T.
- Abstract
type:Journal Article, Versatile novel implementations in microspectroscopy are developed, which can provide angle-resolved optical spectroscopy at local sample areas almost in diffraction limit. By selecting focus position of light flux incident within the back focal plane of the objective lens radially from the position of the optical axis of the microscope with employing off-centered pinhole, we can obtain parallel beam with oblique incidence and its angle tuning at the sample surface. In this paper, we describe our specific optical setup and its practical working principle in detail. We report, as a demonstration of its performance, our latest studies on optical properties of cavity polariton states in the so-called quantum microcavity structures, which contain molecular J-aggregates of pseudoisocyanine (PIC) dye as active working materials. By using the microscope technique, we obtain a fair amount of improvement in the linewidth observation of cavity polariton spectra., source:https://doi.org/10.1155/2011/523017
- Published
- 2017
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