Get Accelerator physics PDF

By S. Y. Lee

ISBN-10: 9812567739

ISBN-13: 9789812567734

Study and improvement of excessive power accelerators all started in 1911.
(1) improvement of excessive gradient dc and rf accelerators,
(2) success of excessive box magnets with very good box quality,
(3) discovery of transverse and longitudinal beam focusing principles,
(4) invention of excessive strength rf sources,
(5) development of ultra-high vacuum technology,
(6) attainment of excessive brightness (polarized/unpolarized) electron/ionsources,
(7) development of beam dynamics and beam manipulation schemes, comparable to beam injection, accumulation, sluggish and quick extraction, beam damping and beam cooling, instability suggestions, laser-beam interplay and harvesting instability for top brilliance coherent photon source.

The affects of the accelerator improvement are evidenced by means of the numerous ground-breaking discoveries in particle and nuclear physics, atomic and molecular physics, condensed topic physics, biology, biomedical physics, nuclear drugs, clinical treatment, and commercial processing. This ebook is meant for use as a graduate or senior undergraduate textbook in accelerator physics and technology. it may be used as preparatory direction fabric in graduate accelerator physics thesis study. The textual content covers ancient accelerator improvement, transverse betatron movement, synchrotron movement, an advent to linear accelerators, and synchrotron radiation phenomena in low emittance electron garage jewelry, creation to big themes equivalent to the unfastened electron laser and the beam-beam interplay. realization is paid to derivation of the action-angle variables of the section area, as the transformation is necessary for figuring out complicated themes similar to the collective instability and nonlinear beam dynamics. every one part is by means of workouts, that are designed to augment ideas and to resolve sensible accelerator layout difficulties.

Readership: Accelerator, high-energy, nuclear, plasma and utilized physicists.

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Maxwell's equations are V-(eE) = 0, VxE = on - ~ , where the external charge and current are zero. Let x, z and s form the basis of an orthonormal coordinate system. For a transverse guided field propagating in the +s direction, we assume E{r,t) = Ex{x,z)e-^ks-ut\ H(f, t) = Hx(x, z)e-^ks-ut\ B± = tfj_, where fields are all transverse with phase velocity up = u/k. (a) Show that the frequency ui and the wave number k of the electromagnetic wave satisfy the dispersion relation UJ — fc/^/e/J. Show that the transverse electromagnetic fields satisfy the static electromagnetic field equation, and the transverse plane wave obeys the relation H = ^ sxEj_, where Z = \fJTjl is the intrinsic impedance of the medium.

At the Continuous Electron Beam Accelerator Facility (CEBAF) at the Thomas Jefferson National Accelerator Laboratory in Virginia, about 160 m of superconducting cavity was installed for attaining a beam energy up to 4 GeV in 5 paths using 338 five-kW CW klystrons. During the LEP-II upgrade more than 300 m of superconducting rf cavity was installed for attaining an almost 100-GeV beam energy. S. and DESY in Germany, are collaborating in the effort to achieve a high-gradient superconducting cavity for a linear collider design called the TeV Superconducting Linear Accelerator (TESLA).

The beam can be accelerated by a DC accelerator or RFQ to attain the proper velocity needed for a drift-tube linac. The beams can be injected into a chain of synchrotrons to reach high energy. Some basic accelerator components are described in the following subsections. II. 40 The DC acceleration column is usually used in low energy accelerators such as the Cockcroft-Walton, Van de Graaff, etc. The rf acceleration cavity provides a longitudinal electric field at an rf frequency that ranges from a few hundred kHz to 10-30 GHz.

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Accelerator physics by S. Y. Lee

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