By D. A. Edwards

ISBN-10: 0471551635

ISBN-13: 9780471551638

ISBN-10: 3527617280

ISBN-13: 9783527617289

The 1st part offers with the movement of a unmarried particle lower than the impression of digital and magnetic fields. the fundamental language of linear and round accelerators is constructed. the primary of section balance is brought besides part oscillations in linear accelerators and synchrotrons. offers a remedy of betatron oscillations by way of an expedition into nonlinear dynamics and its software to accelerators. the second one part discusses depth based results, fairly area cost and coherent instabilities. contains tables of parameters for a range of accelerators that are utilized in the varied difficulties supplied on the finish of every bankruptcy.

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**Extra info for An introduction to the physics of high energy accelerators**

**Sample text**

A model-insulator theory [Tung, Ritchie, Ashley and Anderson (1976)] - already used in previous calculations - was employed to describe the response of the valence electrons. 2 of [Thompson et al. (2001)]. 1 Collision Losses and the Most Probable Energy-Loss The treatment - assuming that interactions occur on quasi-free atomic electrons and neglecting the shell correction term - of the energy loss by collisions for incoming electrons and positrons follows the same lines as for massive charged particles.

Further calculations and comparisons are reported in Sects. 3 of [ICRUM (1984)]. 2195 ρZ [MeV/cm]. 56) shows that the energy loss is larger for electrons than for massive charged particles. 6% higher than the one for a massive charged particle at the ionization-loss minimum. In addition, the restricted energy-loss equation for electrons (and positrons) is expressed by the one [see Eq. 23)] for massive and z = 1 particles, but neglecting the shell-correction term. As for massive charged particles, the energy-loss process of electrons and positrons undergoes statistical ﬂuctuations.

5in Interactions of Charged Particles and Photons ws-book975x65˙SSRD 27 the stopping powers obtained from Eq. F. D. 6) % for α-particles (lead ions) in silicon down to about 50 keV/nucleon. With respect to the tabulated values reported in [ICRUM (1993)], the agreement for α-particles is usually better than 4% at low energy down to 50 keV/nucleon. 9) %. In Fig. 7, the nuclear stopping powers in a silicon medium for α-particles and a few heavy-ions are shown as function of the kinetic energy of incoming ions in units of MeV/amu† .

### An introduction to the physics of high energy accelerators by D. A. Edwards

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