Download Accelerator Physics, Second Edition by S. Y. Lee PDF

By S. Y. Lee

The advance of excessive strength accelerators all started in 1911, while Rutherford chanced on the atomic nuclei contained in the atom. when you consider that then, growth has been made within the following: (1) improvement of excessive voltage dc and rf accelerators, (2) success of excessive box magnets with first-class box caliber, (3) discovery of transverse and longitudinal beam focusing ideas, (4) invention of excessive strength rf resources, (5) development of excessive vacuum expertise, (6) attainment of excessive brightness (polarized/unpolarized) electron/ion assets, (7) development of beam dynamics and beam manipulation schemes, reminiscent of beam injection, accumulation, sluggish and speedy extraction, beam damping and beam cooling, instability suggestions, and so forth. 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 subject physics, biomedical physics, drugs, biology, and commercial processing. This e-book is meant for use as a graduate or senior undergraduate textbook in accelerator physics and technology. it may be used as preparatory path fabric for graduate accelerator physics scholars doing thesis learn. The textual content covers old accelerator improvement, transverse betatron movement, synchrotron movement, an advent to linear accelerators, and synchrotron radiation phenomena in low emittance electron garage earrings, creation to important issues corresponding to the loose electron laser and the beam-beam interplay. consciousness is paid to derivation of the action-angle variables of the part area, as the transformation is necessary for realizing complex issues akin to the collective instability and nonlinear beam dynamics. every one part is via workouts, that are designed to augment the idea that mentioned and to resolve a pragmatic accelerator layout challenge.

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B) For an ideal solenoid, show that the inductance is L = non2(S = non2 x volume of the solenoid, where S is the cross-section area of the solenoid. Note that the total energy stored in the magnet is given by the magnetic energy. 9. From elementary physics, the field at a distance r from a long straight wire carrying current / is B = ^oI/2-nr along a direction tangential to a circle with radius r around the wire. 47 (b) If the current per unit area of an infinitely long circular current sheet is X(r, ) = ( / i / 2 o ) cos 5{r - a), where I\ is the total dipole current and (r, ) are the cylindrical coordinates with x = r cos and z = r sin , show that the magnetic field inside the current sheet is Bz = -ti0Ii/4a, Bx = 0.

Bert M. Coursey and R. Nath, Phys. Today, p. 25, April 2000. 6 T (SSC), what is the total length of dipoles needed in each accelerator? 2. The resonance frequency of a LC circuit is / r = l/2-Ky/LC. Assuming that you can build a capacitor with a minimum capacitance of C = 1 pF, what value of inductance L is needed to attain 3 GHz resonance frequency? What is your conclusion from this exercise? Can you use a conventional LC circuit for microwave tuning? 44 3. r o 6 2 2r , r - a r> a ( 2^607" 7 where 7 = l / \ / l - / 3 2 and e is the charge of the beam particle.

2In principle, the method discussed in this chapter can also be applied to a linac or a transport line, where the betatron motion is equivalent to an initial value problem. 35 36 CHAPTER 2. TRANSVERSE MOTION beam emittance, and properties of the envelope function. In Sec. Ill, we study the effects of linear magnetic imperfections (dipole and quadrupole field errors) and their application in beam manipulation. Section IV deals with the off-momentum closed orbit and its implications for longitudinal synchrotron motion, and also with the lattice design strategies for variable 7T and minimum dispersion action.

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