Готові списки джерел за темами / ELECTRIC RESONANCE

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Добірка наукової літератури з теми "ELECTRIC RESONANCE"

Автор: Grafiati
Опубліковано: 11 вересня 2023

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Статті в журналах з теми "ELECTRIC RESONANCE"

1

Bleaney, B. "Magneto-electric resonance." Applied Magnetic Resonance 20, no. 1-2 (February 2001): 203–5. http://dx.doi.org/10.1007/bf03162320.

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2

Tang Ming-Chun, Xiao Shao-Qiu, Deng Tian-Wei, Bai Yan-Ying, Guan Jian, and Wang Bing-Zhong. "Miniaturized electric resonance metamaterial." Acta Physica Sinica 59, no. 7 (2010): 4715. http://dx.doi.org/10.7498/aps.59.4715.

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3

Han, Aoxue, Colm Dineen, Viktoriia E. Babicheva, and Jerome V. Moloney. "Second harmonic generation in metasurfaces with multipole resonant coupling." Nanophotonics 9, no. 11 (July 5, 2020): 3545–56. http://dx.doi.org/10.1515/nanoph-2020-0193.

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AbstractWe report on the numerical demonstration of enhanced second harmonic generation (SHG) originating from collective resonances in plasmonic nanoparticle arrays. The nonlinear optical response of the metal nanoparticles is modeled by employing a hydrodynamic nonlinear Drude model implemented into Finite-Difference Time-Domain (FDTD) simulations, and effective polarizabilities of nanoparticle multipoles in the lattice are analytically calculated at the fundamental wavelength by using a coupled dipole–quadrupole approximation. Excitation of narrow collective resonances in nanoparticle arrays with electric quadrupole (EQ) and magnetic dipole (MD) resonant coupling leads to strong linear resonance enhancement. In this work, we analyze SHG in the vicinity of the lattice resonance corresponding to different nanoparticle multipoles and explore SHG efficiency by varying the lattice periods. Coupling of electric quadrupole and magnetic dipole in the nanoparticle lattice indicates symmetry breaking and the possibility of enhanced SHG under these conditions. By varying the structure parameters, we can change the strength of electric dipole (ED), EQ, and MD polarizabilities, which can be used to control the linewidth and magnitude of SHG emission in plasmonic lattices. Engineering of lattice resonances and associated magnetic dipole resonant excitations can be used for spectrally narrow nonlinear response as the SHG can be enhanced and controlled by higher multipole excitations and their lattice resonances. We show that both ED and EQ–MD lattice coupling contribute to SHG, but the presence of strong EQ–MD coupling is important for spectrally narrow SHG and, in our structure, excitation of narrow higher-order multipole lattice resonances results in five times enhancement.
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4

Shami, Zein Alabidin, Christophe Giraud-Audine, and Olivier Thomas. "A nonlinear piezoelectric shunt absorber with 2:1 internal resonance: experimental proof of concept." Smart Materials and Structures 31, no. 3 (January 28, 2022): 035006. http://dx.doi.org/10.1088/1361-665x/ac4ab5.

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Abstract An experimental proof of concept of a new semi-passive nonlinear piezoelectric shunt absorber, introduced theoretically in a companion article, is presented in this work. This absorber is obtained by connecting, through a piezoelectric transducer, an elastic structure to a resonant circuit that includes a quadratic nonlinearity. This nonlinearity is obtained by including in the circuit a voltage source proportional to the square of the voltage across the piezoelectric transducer, thanks to an analog multiplier circuit. Then, by tuning the electric resonance of the circuit to half the value of one of the resonances of the elastic structure, a two-to-one internal resonance is at hand. As a result, a strong energy transfer occurs from the mechanical mode to be attenuated to the electrical mode of the shunt, leading to two essential features: a nonlinear antiresonance in place of the mechanical resonance and an amplitude saturation. Namely, the amplitude of the elastic structure oscillations at the antiresonance becomes, above a given threshold, independent of the forcing level, contrary to a classical linear resonant shunt. This paper presents the experimental setup, the designed nonlinear shunt circuit and the main experimental results.
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5

Decker, M., T. Pertsch, and I. Staude. "Strong coupling in hybrid metal–dielectric nanoresonators." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 375, no. 2090 (March 28, 2017): 20160312. http://dx.doi.org/10.1098/rsta.2016.0312.

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We study resonant photonic–plasmonic coupling between a gold dipole nanoantenna and a silicon nanodisc supporting electric and magnetic dipolar Mie-type resonances. Specifically, we consider two different cases for the mode structure of the silicon nanodisc, namely spectrally separate and spectrally matching electric and magnetic dipolar Mie-type resonances. In the latter case, the dielectric nanoparticle scatters the far fields of a unidirectional Huygens’ source. Our results reveal an anticrossing of the plasmonic dipole resonance and the magnetic Mie-type dipole resonance of the silicon nanodisc, accompanied by a clear signature of photonic–plasmonic mode hybridization in the corresponding mode profiles. These characteristics show that strong coupling is established between the two different resonant systems in the hybrid nanostructure. Furthermore, our results demonstrate that in comparison with purely metallic or dielectric nanostructures, hybrid metal–dielectric nanoresonators offer higher flexibility in tailoring the fractions of light which are transmitted, absorbed and reflected by the nanostructure over a broad range of parameters without changing its material composition. As a special case, highly asymmetric reflection and absorption properties can be achieved. This article is part of the themed issue ‘New horizons for nanophotonics’.
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6

Nguyen Thi, Thuy, Ngoc Tran Minh, Tu Vu Minh, and Dung Pham Thi. "STUDY ELECTROMAGNETIC WAVE INTERACTION OF ACTIVE-MATRIX THIN FILM TRANSISTORS." Journal of Science Natural Science 65, no. 10 (October 2020): 24–28. http://dx.doi.org/10.18173/2354-1059.2020-0044.

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Active-matrix thin film transistors (TFTs) on glass substrates with a metal backplane, that are applied for flat panel displays, can be considered as a metamaterial absorber. In this study, TFT structures using doped silicon at source, drain, and channel terminals are investigated. These terminals are unchanged in size of 75 µm square and thickness of 5.3 µm. The electric conductivity is varied at the channel. The simulation results show that the structures with 500 S\m electric conductivity channels absorb incident electromagnetic waves with appropriately 100% at 758 GHz and a wide bandwidth of 20 GHz. As the electrical conductivity increases, the absorption and bandwidth are smaller at the main resonance peak. As the electrical conductivity decreases, the absorption falls at the resonance frequency, but the bandwidth is broadened. In addition, the electric field in the channel may influence the electron in the semiconductor and the electrical current between the source and drain terminals. By observing the electric field at the resonance frequency, we found that it is focused on the sides of channel terminals.
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7

Thornton, Jack. "Pulling Power from the Road." Mechanical Engineering 136, no. 04 (April 1, 2014): 44–49. http://dx.doi.org/10.1115/1.2014-apr-3.

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This article presents an overview of charging technology called Shaped Magnetic Field in Resonance (SMFIR). It has been developed by a team of engineers and technologists at the Korea Advanced Institute for Science and Technology. An all-electric bus developed in Korea recharges its battery when it travels over electric coils buried at intervals along its route. The concept is called on-line electric vehicles, and the heart of OLEV technology is the transfer of enough electricity across gaps of up to 10 inches to power a fully loaded bus. Specifically, underground cables transfer power from the electrical grid to drive motors and on-board batteries via pickups beneath the OLEV bus bodies. The OLEV system wirelessly charges a bus, stopped or in motion, for continuous operation. SMFIR transfers rely on electromagnetic field resonance rather than inductive coupling. In SMFIR technology, the sending unit and the vehicle receiver resonate at 20,000 hertz.
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8

Nakayama, S., H. Akimune, Y. Arimoto, I. Daito, H. Fujimura, Y. Fujita, M. Fujiwara, et al. "Isovector Electric Monopole Resonance in60Ni." Physical Review Letters 83, no. 4 (July 26, 1999): 690–93. http://dx.doi.org/10.1103/physrevlett.83.690.

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9

Andrianov, B. A. "Electric analog of magnetic resonance." Technical Physics Letters 26, no. 3 (March 2000): 228–30. http://dx.doi.org/10.1134/1.1262800.

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10

Mori, N., N. Nakamura, K. Taniguchi, and C. Hamaguchi. "Electric field-induced magnetophonon resonance." Solid-State Electronics 31, no. 3-4 (March 1988): 777–80. http://dx.doi.org/10.1016/0038-1101(88)90387-5.

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Дисертації з теми "ELECTRIC RESONANCE"

1

Neff, Joseph Daniel. "Controlled stochastic resonance and nonlinear electronic circuits." Diss., Georgia Institute of Technology, 2000. http://hdl.handle.net/1853/30476.

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ARDUINO, ALESSANDRO. "Mathematical methods for magnetic resonance based electric properties tomography." Doctoral thesis, Politecnico di Torino, 2018. http://hdl.handle.net/11583/2698325.

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Magnetic resonance-based electric properties tomography (MREPT) is a recent quantitative imaging technique that could provide useful additional information to the results of magnetic resonance imaging (MRI) examinations. Precisely, MREPT is a collective name that gathers all the techniques that elaborate the radiofrequency (RF) magnetic field B1 generated and measured by a MRI scanner in order to map the electric properties inside a human body. The range of uses of MREPT in clinical oncology, patient-specific treatment planning and MRI safety motivates the increasing scientific interest in its development. The main advantage of MREPT with respect to other techniques for electric properties imaging is the knowledge of the input field inside the examined body, which guarantees the possibility of achieving high-resolution. On the other hand, MREPT techniques rely on just the incomplete information that MRI scanners can measure of the RF magnetic field, typically limited to the transmit sensitivity B1+. In this thesis, the state of art is described in detail by analysing the whole bibliography of MREPT, started few years ago but already rich of contents. With reference to the advantages and drawbacks of each technique proposed for MREPT, the particular implementation based on the contrast source inversion method is selected as the most promising approach for MRI safety applications and is denoted by the symbol csiEPT. Motivated by this observation, a substantial part of the thesis is devoted to a thoroughly study of csiEPT. Precisely, a generalised framework based on a functional point of view is proposed for its implementation. In this way, it is possible to adapt csiEPT to various physical situations. In particular, an original formulation, specifically developed to take into account the effects of the conductive shield always employed in RF coils, shows how an accurate modelling of the measurement system leads to more precise estimations of the electric properties. In addition, a preliminary study for the uncertainty assessment of csiEPT, an imperative requirement in order to make the method reliable for in vivo applications, is performed. The uncertainty propagation through csiEPT is studied using the Monte Carlo method as prescribed by the Supplement 1 to GUM (Guide to the expression of Uncertainty in Measurement). The robustness of the method when measurements are performed by multi-channel TEM coils for parallel transmission confirms the eligibility of csiEPT for MRI safety applications.
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3

Aydin, Ahmet. "Application of electric potential sensors in nuclear Magnetic resonance signal acquisition." Thesis, University of Sussex, 2006. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.536554.

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Hsu, Fang-Chi. "Electric field effect in "metallic" polymers." Connect to resource, 2005. http://rave.ohiolink.edu/etdc/view?acc%5Fnum=osu1127229727.

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Thesis (Ph. D.)--Ohio State University, 2005.
Title from first page of PDF file. Document formatted into pages; contains xxi, 177 p.; also includes graphics (some col.). Includes bibliographical references (p. 167-177). Available online via OhioLINK's ETD Center
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5

Cheng, Mao-Sen. "Molecular beam electric resonance spectroscopy of CO-SO₂ and Kr-SO₂ complexes /." view abstract or download file of text, 2000. http://wwwlib.umi.com/cr/uoregon/fullcit?p9998027.

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Thesis (Ph. D.)--University of Oregon, 2000.
Typescript. Includes vita and abstract. Includes bibliographical references (leaves 110-113). Also available for download via the World Wide Web; free to University of Oregon users.
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6

Bolton, David Robert. "Circuits and systems for CW and pulsed high-field electron spin resonance." Thesis, University of St Andrews, 2006. http://hdl.handle.net/10023/7104.

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This thesis is concerned with the design and realisation of components for a new state of the art 94GHz Electron Spin Resonance (ESR) spectrometer capable of operating in both pulsed and CW modes. The complete spectrometer is designed to provide phase coherent 1kW peak power sub-nanosecond π/2 pulses having variable duration and repetition rate. The mm-wave response of a paramagnetic sample to these pulses is detected with a superheterodyne detector. Such a system would offer a step change in performance, promising unprecedented resolution and sensitivity. These aims should be compared with the performance of commercial (Bruker) instruments capable of delivering 200mW 30ns π/2 pulses. For this type of system, both the long term (thermal) and short term (phase) stability of oscillators and sources employed are extremely important. Consideration of phase noise, frequency, tunability and power output shows that multiplied sources offer substantial benefits compared to fundamental sources. A delay line discriminator method of phase noise measurement, suitable for use with the low frequency oscillators is described and implemented. This is extended to 94GHz using a down convertor with a quasi-optically stabilised Gunn oscillator. These tools are used to select an optimum oscillator-multiplier combination to produce a low noise 94GHz source. Anew method of pulse generation, which has produced +23dBm peak power 250ps rectangular and 115ps Gaussian envelope phase coherent pulses, is described. These are believed to be the shortest phase coherent pulses at 94GHz available. This system will be used to provide ns pulses suitable for amplification to 1kW using a Klystron amplifier. A heterodyne detector has been constructed which employs the same oscillator/multiplier techniques identified above to produce the required local oscillator signal. It is demonstrated that by careful consideration of multiplication factors a system employing one variable and one fixed oscillator allows all the signals required in the spectrometer to maintain phase coherence. It is demonstrated that the complete demodulator responds to pulses on a ns time scale and has a noise temperature of 737K.
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7

Goulding, Philip. "The use of electric potential sensors in nuclear magnetic resonance and particle detection applications." Thesis, University of Sussex, 2015. http://sro.sussex.ac.uk/id/eprint/57919/.

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The work in this thesis extends the applications of the Electric Potential Sensor (EPS) designed by the Sensor Research Technology Centre. Combined is work undertaken in two areas related by their application in security systems: low-field nuclear magnetic resonance with electric-field acquisition, and particle detection for alpha, beta and neutron radiation. In both these areas the EPS is used as to acquire signals. The first half of the thesis consists of the work undertaken to design a low-field Nuclear Magnetic Resonance spectrometer to detect drugs and explosives. In doing so, the use of the electric field detection technique - patented by Sussex University - is extended to low-field NMR work. The eventual negative results in this field lead first to the design of a simpler proton magnetometer apparatus, a design which would confirm the use of the EPS at low frequencies, and eventually to a change in direction of the research: particle detection. Detailed in this first section are a theoretical explanation of NMR in chapter 2, and a chapter covering the design and testing of the equipment in chapter 3. The particle detection part of the thesis covers modifications made to the EPS in order to detect particles and experiments conducted to confirm their operation. As in the NMR section, the work is split into a theory chapter which underpins the work, providing context for the experiments chapter. Chapter 5 covers the detection of alpha, beta and neutron radiation and the use of feedback to control the RC time constant of the front end of the sensor. The work in this thesis concludes negative results in the NMR area, but proves the EPS particle detector as a viable, cost effective alternative to conventional detectors.
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Mukherjee, Shrijit. "Broadband electric field sensing and its application to material characterisation and nuclear quadrupole resonance." Thesis, University of Sussex, 2012. http://sro.sussex.ac.uk/id/eprint/7666/.

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The aim of this project is to address the challenges associated with extending the radio frequency capability of Electric Potential Sensors to greater than 10 MHz. This has culminated in a single broadband sensor, with a frequency range of 200 Hz to greater than 200 MHz. The use of Electric Potential Sensors for the measurement of electric field with minimal perturbation has already been demonstrated at Sussex. These high impedance sensors have been successfully employed in measuring signals with frequencies in the range 1 mHz to 2 MHz. Many different versions of these sensors have been produced to cater for specific measurement requirements in a wide variety of experimental situations. From the point of view of this project, the relevant prior work is the acquisition of a 2 MHz electric field nuclear magnetic resonance signal, and the non-destructive testing of composite materials at audio frequency. Two very distinct electric field measurement scenarios are described which illustrate the diverse capabilities of the broadband sensor. Firstly, an electric field readout system for nuclear quadrupole resonance is demonstrated for the first time, with a sodium chlorate sample at a frequency of 30 MHz. Nuclear quadrupole resonance is an important technique with applications in the detection of explosives and narcotics. Unlike nuclear magnetic resonance a large magnet is not required, opening up the possibility of portable equipment. The electric field readout system is shown to be simpler than the conventional magnetic readout and may therefore contribute to the development of portable devices. Secondly, a broadband, high spatial resolution microscope system for materials characterisation with four different imaging modes is described. This includes; the surface topography of a conducting sample; the dielectric constant variation in glass/epoxy composite; the conductivity variation in a carbon fibre composite; and the electrode pixels inside a solid state CMOS fingerprint sensor.
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9

Adamov, Minja Gemisic. "Measurements of local electric fields by doppler-free laser spectroscopy of hydrogen resonance lines." Doctoral thesis, Humboldt-Universität zu Berlin, Mathematisch-Naturwissenschaftliche Fakultät I, 2007. http://dx.doi.org/10.18452/15576.

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In dieser Arbeit wurde eine einfache laserspektroskopische Messmethode für lokale elektrische Feldstärken im Hinblick auf ihre Messmöglichkeiten und -grenzen untersucht. Als empfindliche optische Feldsensoren dienen dabei Wasserstoffatome, für die die Stark-Aufspaltung der Spektrallinien im elektrischen Feld wohl bekannt und exakt berechenbar ist. Die experimentellen Untersuchungen wurden an einer Niederdruck-Gaszelle durchgeführt, in der ein elektrisch geheizter Wolframdraht für thermische Dissoziation von Wasserstoffmolekülen sorgte. Die Wasserstoffatome wurden durch zwei gegenläufige Laserstrahlen Doppler-frei angeregt. Die Durchstimmung der schmalbandigen Laserstrahlung über den Wellenlängenbereich der Zwei-Photonen-Resonanz lieferte direkt das vom elektrischen Feld hervorgerufene Stark-Spektrum des angeregten Zustands. Weil die Methode im Gegensatz zu ähnlichen, erheblich aufwendigeren Verfahren nur die niedrigsten Wasserstoff-Energieniveaus benutzt, die mit Zwei-Photonen-Anregung direkt aus dem Grundzustand erreichbar sind, kommt sie mit einem einzigen Laser aus. Für das erste angeregte Niveau mit n = 2 wird Strahlung bei 243 nm benötigt, das nächsthöhere Niveau mit n = 3 erfordert 205 nm. Für n = 2 wurden Untersuchungen an Wasserstoff und Deuterium durchgeführt und Stark-Spektren mittels optogalvanischer Detektion gemessen. Schwerpunkt der Arbeit waren aber die Messungen an Wasserstoff für n = 3, bei denen zusätzlich Balmer-alpha-Fluoreszenz im Sichtbaren zur Detektion eingesetzt werden konnte. Bei elektrischen Feldern bis 200 V/cm wurden Stark-Spektren für drei verschiedene Polarisationszustände der Laserstrahlung aufgenommen. Als Ergebnis konnte jeweils ein Paar isolierter Stark-Komponenten in den Spektren identifiziert werden, dessen gut messbarer Frequenzabstand durch Vergleich mit theoretischen Werten die Bestimmung der elektrischen Feldstärke ermöglicht.
A method for electric field measurements that observes the Stark spectra of the low excited levels n = 2 and n = 3 of atomic hydrogen has been explored in this work. As advantage these levels can be excited Doppler-free from the ground state by a single laser and the highly resolved Stark spectra are easy to understand and to be calculated. Good sensitivity of electric field measurements is achieved with specially designed solid state laser systems, which provide tuneable pulsed UV radiation with a high pulse peak-power and a narrow bandwidth needed for Doppler-free two-photon excitation. Using hydrogen and deuterium the Stark spectra of the n = 2 level are detected as optogalvanic signal. For three different cases of laser polarization the n = 3 spectra of hydrogen are measured simultaneously with optogalvanic and laser induced Balmer alpha fluorescence detection. Electric fields down to 200 V/cm can be determined from the Stark spectra of n = 2 level, while the spectra of n = 3 level enable measurements of electric fields as small as 50 V/cm in each of the three cases of laser polarization.
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10

Kurimura, Tomo. "Driving micro-scale object by a dc electric field." 京都大学 (Kyoto University), 2016. http://hdl.handle.net/2433/215288.

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Книги з теми "ELECTRIC RESONANCE"

1

Magnetic and electric resonance. Newcastle upon Tyne, UK: Cambridge Scholars Publishing, 2018.

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2

Anderson, P. M. Subsynchronous resonance in power systems. New York: IEEE Press, 1990.

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3

Padiyar, K. R. Analysis of subsynchronous resonance in power systems. Boston: Kluwer Academic Publishers, 1999.

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4

J, Speth, ed. Electric and magnetic giant resonances in nuclei. Singapore: World Scientific, 1991.

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5

Dylla, Thorsten. Electron spin resonance and transient photocurrent measurements on microcrystalline silicon. Jülich: Forschungszentrum, Zentralbibliothek, 2005.

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6

Kinnen, Edwin. Resonance: Electrical engineering at the University of Rochester. Rochester, NY, USA: University of Rochester Press, 2003.

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7

1969-, Cao Yijia, and Jiang Quanyuan 1975-, eds. Dian li xi tong ci tong bu zhen dang de li lun yu fang fa. Beijing: Ke xue chu ban she, 2009.

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8

P, Shestopalov V., and Instytut radiofizyky i elektroniky (Akademii͡a︡ nauk Ukraïnsʹkoï RSR), eds. Rezonansnoe rassei͡a︡nie voln. Kiev: Nauk. dumka, 1986.

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9

Long, Edward R. Spectroscopic comparison of effects of electron radiation on mechanical properties of two polyimides. [Washington, DC]: National Aeronautics and Space Administration, Scientific and Technical Information Branch, 1987.

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10

Shestopalov, V. P. Spektralʹnai͡a︡ teorii͡a︡ i vozbuzhdenie otkrytykh struktur. Kiev: Nauk. dumka, 1987.

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Частини книг з теми "ELECTRIC RESONANCE"

1

Morris, Noel M., and Frank W. Senior. "Resonance." In Electric Circuits, 121–41. London: Macmillan Education UK, 1991. http://dx.doi.org/10.1007/978-1-349-11232-6_6.

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2

Asaad, Serwan. "Nuclear Electric Resonance." In Electrical Control and Quantum Chaos with a High-Spin Nucleus in Silicon, 83–108. Cham: Springer International Publishing, 2021. http://dx.doi.org/10.1007/978-3-030-83473-9_6.

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3

Slichter, Charles P. "Electric Quadrupole Effects." In Principles of Magnetic Resonance, 485–502. Berlin, Heidelberg: Springer Berlin Heidelberg, 1990. http://dx.doi.org/10.1007/978-3-662-09441-9_10.

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4

Blanchard, John W., Alexander O. Sushkov, and Arne Wickenbrock. "Magnetic Resonance Searches." In The Search for Ultralight Bosonic Dark Matter, 173–200. Cham: Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-030-95852-7_6.

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AbstractUltralight bosonic dark matter (UBDM), such as axions and axionlike particles (ALPs), can interact with Standard Model particles via a variety of portals. One type of portal induces electric dipole moments (EDMs) of nuclei and electrons and another type generates torques on nuclear and electronic spins. Several experiments search for interactions of spins with the galactic dark matter background via these portals, comprising a new class of dark matter haloscopes based on magnetic resonance.
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5

Padiyar, K. R. "Modelling of the Electric Network." In Analysis of Subsynchronous Resonance in Power Systems, 63–81. Boston, MA: Springer US, 1999. http://dx.doi.org/10.1007/978-1-4615-5633-6_3.

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6

Imura, Takehiro. "Basic Characteristics of Electric Field Resonance." In Wireless Power Transfer, 361–84. Singapore: Springer Singapore, 2020. http://dx.doi.org/10.1007/978-981-15-4580-1_11.

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7

Yoon, Uooyeol. "Magnetic Energy Pickup Using Resonance." In The On-line Electric Vehicle, 115–28. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-51183-2_7.

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8

van der Woude, A. "Excitation and decay of electric giant resonances — especially the isoscalar giant monopole resonance." In Symmetries and Semiclassical Features of Nuclear Dynamics, 213–29. Berlin, Heidelberg: Springer Berlin Heidelberg, 1987. http://dx.doi.org/10.1007/3-540-17926-7_53.

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9

Le Dour, Olivier, Markus Vester, Peter Henninger, and Wolfgang Renz. "Finite Element Computation of the Electromagnetic Fields Produced in the Body by Magnetic Resonance Imaging Surface Coils." In Electric and Magnetic Fields, 257–60. Boston, MA: Springer US, 1995. http://dx.doi.org/10.1007/978-1-4615-1961-4_58.

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10

Merkt, U. "Cyclotron Resonance in InSb in Crossed Electric and Magnetic Fields." In Springer Series in Solid-State Sciences, 256–65. Berlin, Heidelberg: Springer Berlin Heidelberg, 1987. http://dx.doi.org/10.1007/978-3-642-83114-0_37.

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Тези доповідей конференцій з теми "ELECTRIC RESONANCE"

1

Reisz, Aloysius I. "High-Density Electron Cyclotron Resonance Electric Propulsion." In 51st AIAA/SAE/ASEE Joint Propulsion Conference. Reston, Virginia: American Institute of Aeronautics and Astronautics, 2015. http://dx.doi.org/10.2514/6.2015-3725.

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2

Belan, A., Z. Eleschova, and M. Smola. "Resonance overvoltages in electric power networks." In 2005 IEEE Russia Power Tech. IEEE, 2005. http://dx.doi.org/10.1109/ptc.2005.4524609.

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3

Matveev, O. I., W. L. Clevenger, L. S. Mordoh, B. W. Smith, and J. D. Winefordner. "Plasma emission in a pulsed electric field after resonance ionization of atoms." In Resonance ionization spectroscopy 1996: Eighth international symposium. AIP, 1997. http://dx.doi.org/10.1063/1.52179.

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4

Nasrullah, K. "Voltage surge resonance on electric power network." In 1999 IEEE Transmission and Distribution Conference (Cat. No. 99CH36333). IEEE, 1999. http://dx.doi.org/10.1109/tdc.1999.756134.

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5

Tokura, Yasuhiro, Toshihiro Kubo, and William John Munro. "Power Dependence of Electric Dipole Spin Resonance." In Proceedings of the 12th Asia Pacific Physics Conference (APPC12). Journal of the Physical Society of Japan, 2014. http://dx.doi.org/10.7566/jpscp.1.012022.

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6

Aseyev, S. A., Yu A. Kudryavtsev, and V. V. Petrunin. "Ionization of fast Rydberg atoms in longitudinal and transverse electric fields." In The 7th international symposium: Resonance ionization spectroscopy 1994. AIP, 1995. http://dx.doi.org/10.1063/1.47570.

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7

Beterov, Igor M., Igor I. Ryabtsev, and Nicolai V. Fateev. "Ionization probing of static electric fields by double stark resonance in Rydberg atoms." In The 7th international symposium: Resonance ionization spectroscopy 1994. AIP, 1995. http://dx.doi.org/10.1063/1.47540.

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8

Tarnev, Khristo. "Numerical method for determination of resonance electron velocities in periodic electric fields." In APPLICATIONS OF MATHEMATICS IN ENGINEERING AND ECONOMICS (AMEE'14). AIP Publishing LLC, 2014. http://dx.doi.org/10.1063/1.4902472.

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9

Hu, Hao, and Stavros V. Georgakopoulos. "Wireless power transfer through strongly Coupled Electric Resonance." In 2013 IEEE International Symposium on Antennas and Propagation & USNC/URSI National Radio Science Meeting. IEEE, 2013. http://dx.doi.org/10.1109/aps.2013.6711077.

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10

Mohr, P., T. Hartmann, K. Vogt, S. Volz, and A. Zilges. "Electric dipole strength below the giant dipole resonance." In NUCLEAR PHYSICS IN THE 21st CENTURY:International Nuclear Physics Conference INPC 2001. AIP, 2002. http://dx.doi.org/10.1063/1.1470052.

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Звіти організацій з теми "ELECTRIC RESONANCE"

1

ORLOV, Y. F., W. M. MORSE, and Y. K. SEMERTZIDIS. RESONANCE METHOD OF ELECTRIC-DIPOLE-MOMENT MEASUREMENTS IN STORAGE RINGS. Office of Scientific and Technical Information (OSTI), May 2006. http://dx.doi.org/10.2172/884642.

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2

Choe, W., M. Ono, and C. S. Chang. Temperature anisotropy in a cyclotron resonance heated tokamak plasma and the generation of poloidal electric field. Office of Scientific and Technical Information (OSTI), November 1994. http://dx.doi.org/10.2172/10196164.

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3

Iselin, L. H. Using nitrogen-14 nuclear quadrupole resonance and electric field gradient information for the study of radiation effects. Office of Scientific and Technical Information (OSTI), December 1995. http://dx.doi.org/10.2172/527440.

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4

Cohen, S. Response of the /sup 1/P/sup 0/ resonance near n = 3 in the H/sup -/ continuum to external electric fields. Office of Scientific and Technical Information (OSTI), May 1986. http://dx.doi.org/10.2172/5842274.

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5

Ranjbar, Vahid H., M. Blaskiewicz, F. Meot, C. Montag, and S. Tepikian. Spin Resonance Free Electron Ring Injector. Office of Scientific and Technical Information (OSTI), January 2017. http://dx.doi.org/10.2172/1436273.

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6

Williams, G. M. Resonance electronic Raman scattering in rare earth crystals. Office of Scientific and Technical Information (OSTI), November 1988. http://dx.doi.org/10.2172/6343820.

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7

Peter Damiano and J.R. Johnson. Electro Acceleration in a Geomagnetic Field Line Resonance. Office of Scientific and Technical Information (OSTI), August 2012. http://dx.doi.org/10.2172/1062556.

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Van Willigen, H. Magnetic resonance studies of photo-induced electron transfer reactions. Office of Scientific and Technical Information (OSTI), January 1992. http://dx.doi.org/10.2172/5710499.

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9

van Willigen, H. Magnetic resonance studies of photo-induced electron transfer reactions. Office of Scientific and Technical Information (OSTI), November 1992. http://dx.doi.org/10.2172/6889113.

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10

Sambe, Hideo, and David E. Ramaker. Resonance Electron Scattering by O2 Monolayers on Graphites: Reinterpreted. Fort Belvoir, VA: Defense Technical Information Center, January 1993. http://dx.doi.org/10.21236/ada261851.

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