Accelerator Physics by S. Y. Lee

By S. Y. Lee

Learn and improvement of excessive strength 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 energy 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, reminiscent of beam injection, accumulation, sluggish and quick extraction, beam damping and beam cooling, instability suggestions, laser-beam interplay and harvesting instability for prime brilliance coherent photon source.

The affects of the accelerator improvement are evidenced by means of the various ground-breaking discoveries in particle and nuclear physics, atomic and molecular physics, condensed topic physics, biology, biomedical physics, nuclear drugs, clinical remedy, and commercial processing. This ebook is meant for use as a graduate or senior undergraduate textbook in accelerator physics and technological know-how. it may be used as preparatory direction fabric in graduate accelerator physics thesis learn. The textual content covers old accelerator improvement, transverse betatron movement, synchrotron movement, an creation to linear accelerators, and synchrotron radiation phenomena in low emittance electron garage earrings, advent to important themes equivalent to the loose electron laser and the beam-beam interplay. awareness is paid to derivation of the action-angle variables of the part house, as the transformation is necessary for figuring out complex subject matters comparable to the collective instability and nonlinear beam dynamics. every one part is through workouts, that are designed to enhance options and to unravel lifelike accelerator layout difficulties.

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

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For superconducting magnets, the superconducting coils are arranged to simulate the cosine-theta like distribution. 17) where B1 = aB,/dx evaluated at the center of the quadrupole, and P , i , and i are the unit vectors in the horizontal, azimuthal, and vertical directions. For a charged particle passing through the center of a quadrupole, the magnetic field and the Lorentz force are zero. At a displacement (z, z ) from the center, the Lorentz force for a particle with charge e and velocity u along the B direction is given by + F = euBli x (22 + x i ) = - e v B l z i -k evBlxP.

Particle beams are produced from ion sources, where charged ions are extracted by a high-voltage source to form a beam. Before injection into various types of accelertttors, the beam pulse is usually prebunched and chopped into appropriate sizes. 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 t o reach high energy. Some basic accelerator components are described in the following subsections.

46) This implies that the transfer matrix of a periodic section has identical eigenvalues. The transfer matrix for passing through P superperiods is M ( s PLls) = [M(s)]', and for passing through m revolutions becomes (M(s)]"'. The necessary and sufficient condition for stable orbital motion is that all matrix elements of the matrix [M(s)]"' remain bounded as m increases. Let X I , X2 be the eigenvalues and v l , v2 be the corresponding eigenvectors of the matrix M. e. XI = 1/&, and X i Xz = Trace(M).

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