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2 edition of Wave and oscillatory phenomena in electron beams at microwave frequencies found in the catalog.

Wave and oscillatory phenomena in electron beams at microwave frequencies

Vladimir Nikolaevich Shevchik

# Wave and oscillatory phenomena in electron beams at microwave frequencies

• 10 Want to read
• 6 Currently reading

Published by Pergamon Press in Oxford, New York .
Written in English

Subjects:
• Electron beams,
• Microwave tubes

• Edition Notes

Includes bibliographical references.

Classifications The Physical Object Statement [by] V.N. Shevchik, G.N. Shvedov, and A.V. Soboleva. Translated by O.M. Blunn. Translation edited by B. Meltzer. Series International series of monographs in electronics and instrumentation,, vol. 34, International series of monographs on electronics and instrumentation ;, vol. 34. Contributions Shvedov, G. N., joint author., Soboleva, A. V., joint author. LC Classifications TK7835 .S513 1965 Pagination xviii, 362 p. Number of Pages 362 Open Library OL5942295M LC Control Number 65013074 OCLC/WorldCa 9234082

The bounded motion of an electron in an atom is similar to a standing wave, and it must be considered not as the motion of a material point along a trajectory, but as a complex oscillatory process. For a standing wave in a restricted volume, only specific values of wavelength λ (and, consequently, the frequency of oscillations v) are. Since it is relatively simple to generate electron beams with peak powers of 10 10 W, the free-electron laser has the potential for providing high optical power, and since there are no prescribed energy levels, as in the conventional laser, the free-electron laser can operate over a broad spectral range. This article presents an overview of recent advances in the field of electron kinetics in low-temperature plasmas (LTPs). It also provides author's views on where the field is headed and suggests promising strategies for further by: 7. Find an expression for ptx, t) for a sinusoidal sound wave traveling in the positive x-direction in water, given that the wave frequency is I kHz, the velocity of sound in water is krnls, the wave amplitude is 10 N/m2, and p(x, 1) was observed to be at its maximum value at t = 0 and x = m.

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### Wave and oscillatory phenomena in electron beams at microwave frequencies by Vladimir Nikolaevich Shevchik Download PDF EPUB FB2

Wave and oscillatory phenomena in electron beams at microwave frequencies. Oxford, New York, Pergamon Press [] (OCoLC) Document Type: Book: All Authors / Contributors: Vladimir Nikolaevich Shevchik; G N Shvedov; A V Soboleva.

Get this from a library. Wave and oscillatory phenomena in electron beams at microwave frequencies. [Vladimir Nikolaevich Shevchik; G N Shvedov; A V Soboleva].

Leaky-Wave Theory, Techniques, and Applications: From Microwaves to Visible Frequencies Article (PDF Available) in Proceedings of the IEEE (5) May with 5, Reads.

A laser is a device that emits light through a process of optical amplification based on the stimulated emission of electromagnetic term "laser" originated as an acronym for "light amplification by stimulated emission of radiation".

The first laser was built in by Theodore H. Maiman at Hughes Research Laboratories, based on theoretical work by Charles Wave and oscillatory phenomena in electron beams at microwave frequencies book Townes and Arthur.

The one‐dimensional Vlasov equation describes the behavior of an incompressible self‐interacting classical fluid which moves in the (q, p) phase plane. This type of phase fluid occurs in many physical problems and its hydrodynamic properties can be examined from a general point of view.

A characteristic feature with initially unstable spatially homogeneous configurations is the development Cited by: V.

Shevchik, G. Shvedov, and A. Soboleva, Wave and Oscillatory Phenomena in Electron Fluxes at Superhigh Frequencies [in Russian], Saratov State University, Saratov ().

SVCh, Parts 1. Experiments have been carried out on the region of transparency for low-frequency electrostatic waves in the cylindrical plasma column represented by an electron-neutralized ion beam.

The wave frequencies of interest are in the ./sub O/./sub Oe/. /sub O/e,e are. Communications, antenna, radar, and microwave engineers must deal with the generation, transmission, and reception of electromagnetic waves. Device engineers working on ever-smaller integrated circuits and at ever higher frequencies must take into account wave propagation effects at the chip and circuit-board levels.

@article{osti_, title = {THz electromagnetic radiation driven by intense relativistic electron beam based on ion focus regime}, author = {Zhou, Qing and Xu, Jin and Zhang, Wenchao and Duan, Zhaoyun and Wave and oscillatory phenomena in electron beams at microwave frequencies book, Yubin and Yang, Shengpeng and Tang, Changjian}, abstractNote = {The simulation study finds that the relativistic electron beam propagating through the plasma background can produce.

A laser with parameters modulated at a Wave and oscillatory phenomena in electron beams at microwave frequencies book f may respond not only at f and its harmonics, but also at is sub-harmonic frequencies f/ laser behaviour can become irregular though remaining deterministic.

A gain modulation has been applied on the Super-ACO Free Electron Laser close to its natural frequency, via a change of the synchronization between the electron bunch and the optical. This banner text can have markup. web; books; video; audio; software; images; Toggle navigation.

De Broglie formalized this wave nature of matter in the following equation (chapter ): where l is the effective wavelength, h is Plank’s constant and p is the momentum of the particle of matter.

The wave-like nature of matter and light gives rise to another phenomena that is closely related to the argument above. About this page. Dislocations in Solids. R.W. Armstrong, W.L. Elban, in Dislocations in Solids, Electromagnetic Radiation and Radio Waves (Natural and Man-Made Miracles) Television signals at microwave frequencies beamed down by satellites The spectrum above shows that the individual photons in visible light have energies of a few electron Volts while the particles in cosmic rays with an equivalent frequency of around 10 25 Hertz.

Overview. Resonance occurs when a system is able to store and easily transfer energy between Wave and oscillatory phenomena in electron beams at microwave frequencies book or more different storage modes (such as kinetic energy and potential energy in the case of a simple pendulum).

However, there are some losses from cycle to cycle, called damping is small, the resonant frequency is approximately equal to the natural frequency of the system, which is a. These will make many calculations a little easier. All EM radiation is composed of photons. Figure 1 shows various divisions of the EM spectrum plotted against wavelength, frequency, and photon energy.

Previously in this book, photon characteristics were alluded to in the discussion of some of the characteristics of UV, x rays, and ${\gamma}$ rays, the first of which start with Author: OpenStax.

Page 1 Electronic, Optical, and Magnetic Materials and Phenomena: The Science of Modern Technology. Important and unexpected discoveries have been made in all areas of condensed-matter and materials physics in the decade since the Brinkman report.

1 Although these scientific discoveries are impressive, perhaps equally impressive are technological advances during the same decade. From the perspective of engineering, microwave technologies are based on electric transients and electromagnetic waves in the millimeter range.

For many years, a frequency of 1 THz, which corresponds to a vacuum wavelength of μm, has been considered the borderline between electric phenomena at lower frequencies and optics at higher. Mesyats' Pulsed Power provides in-depth coverage of the generation of pulsed electric power, electron and ion beams, and various types of pulsed electromagnetic radiation.

The electric power that can be produced by the methods described ranges from to W for pulse durations of s. Another important electron based radiation source is the backward wave oscillator (BWO) which, as discussed for the TWT, is based on the slow-wave structure geometry.

We have already mentioned, among the properties of the Brillouin diagram of figurethat in a slow-wave we can set the parameters in a way in which we can have a positive. The separated oscillatory fields method first used in this experiment has been used in many subsequent experiments at radio and microwave frequencies and has been extended to laser frequencies, as discussed in Paper The first part of the book describes the fundamentals of this research area, starting with a review of Maxwell’s equations in a form suited to the description of metals.

Subsequent chapters introduce the two major ingredients of plasmonics, surface plasmon polaritons at metallic interfaces and localized plasmons in nanostructures. Perpetual wave propagation, independent of wave-generating source velocity, has to be sustained by a tension field when excited within its linear restoration limit.

We are re-naming this field as the Cosmic Tension Field, or CTF [6, Ch in 3]. This is to differentiate the name CTF from the old ether that was rejected based on Michelson-Morley Cited by: 1. Now the question is, whether the light emitted by such a quasi-elastic electron is ideally monochromatic, i.e.

whether it will be characterized by an infinitely lasting sine wave with fixed values of the amplitude a and frequen- * Radiation is also possible in oscillations of a magnetic dipole, as well as of an electric or magnetic quadrupole.

electron A subatomic particle.(See Wikipedia.)electron gas See Lorentz gas electrostatic induction A m odification in the distribution of electric charge on one material under the influence of an electric charge on a nearby object. It occurs whenever any object is placed in an electric a negatively charged object is brought near a neutral object, it induces a positive charge on the.

Superconductivity at millimeter wave frequencies. Tien Chi Chen: PhD () H. Sponer: A generalised united-atom approach for the evaluation of molecular electronic energy levels and the mechanization by means of an electronic ditital computer.

Perry W. Morton:. We study Gaussian wave beam and wave packet types of solutions to the linearized cold plasma system in a toroidal domain (tokamak). Such solutions are constructed with help of Maslov’s complex germ theory (short-wave or semi-classical asymptotics with complex phases).

The term “semi-classical” asymptotics is understood in a broad sense: asymptotic solutions of evolutionary and stationary Author: Anatoly Yu. Anikin, Sergey Yu. Dobrokhotov, Alexander I. Klevin, Brunello Tirozzi. Quantum Mechanics: Classical Results, Modern Systems, and Visualized Examples is a comprehensive introduction to non-relativistic quantum mechanics for advanced.

Vacuum electronic sources range from relatively small units, such as backward-wave oscillators [,], to facilities that take up a whole room or building, such as free-electron lasers [, ] and synchrotrons. These yield the highest power of all present terahertz sources, but are accompanied by limitations related to Author: Roger Lewis.

At low frequencies, the term s=. is the largest term in Z m and the impedance is said to be stiffness controlled. At high frequencies!m is the dominant term and the impedance is mass controlled.

At a frequency. 0 where. 0 m ¼ s=. 0, the impedance has its minimum value Z m ¼ r and is a real quantity with zero reactance. A primary objective is to give students of Fourier optics the capability of programming their own basic wave optic beam propagations and imaging simulations.

The book will also be of interest to professional engineers and physicists learning Fourier optics simulation techniques-either as a self-study text or a text for a short course.

We develop energy efficient, continuous microwave schemes to couple electron and nuclear spins, using phase or amplitude modulation to bridge their frequency difference. These controls have promising applications in biological systems, where microwave power should be limited, as well as in situations with high Larmor frequencies due to large.

Interaction between optical lasers and the electron beam can be used to manipulate the phase space of the electron bunch to produce desirable shapes in the x-ray emission. After the x-ray photons have been generated, optical lasers are used in synchronization with the x-ray pulse to study dynamics in atomic and molecular systems.

De Broglie formalized this wave nature of matter in the following equation (chapter ): where is the effective wavelength, h is Plank’s constant and p is the momentum of the particle of matter. The wave-like nature of matter and light gives rise to another phenomena that is closely related to the argument above.

Cambridge Core - Atomic Physics, Molecular Physics and Chemical Physics - Dissociative Recombination of Molecular Ions - by Mats LarssonCited by: Eng Aik Chan, Giorgio Adamo, Syed Abdullah Aljunid, Athanasios Laliotis, Martial Ducloy, Nikolay Zheludev, David Wilkowski Proc.

SPIE.Optical, Opto-Atomic, and Entanglement-Enhanced Precision Metrology. 'Nonlinear Optical Systems achieves an unmatched coverage in a field that has grown into many sub-disciplines in a very clear and coherent manner. This is a beautiful and self-contained book that starts with the fundamentals and goes on to cover the dynamical phenomena and optical pattern formation in quantum optical by: The most important mechanism for the production of free ion-electron pairs is the electron impact ionization, where an electron with sufﬁcient kinetic energy E kin hits an atom A and releases another electron e− (E kin) + A → A+ + e− (E 1) + e− (E 2).

Within the framework of microwave spin chemistry, the effects of “microwave catalysis” in a large number of cases are reduced to the phenomena of the so-called “spin catalysis”: microwave pumping of radical pairs induces electron-spin transitions, and when the frequency coincides with the frequencies of magnetic resonance transitions Author: Oleg V.

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