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By Martin Reiser
So much complex accelerator functions require beams with high-power and excessive brightness, that are decided by means of space-charge results at low strength. Examples are the enormous excessive power Physics huge Hadron Collider (LHC) at CERN, to be introduced in 2008, and the foreign Linear Collider (ILC) being thought of to persist with the LHC. different examples are Spallation Neutron resources, the proposed Heavy Ion Inertial Fusion motive force for strength creation, loose Electron Lasers, and Muon Colliders.This revised and up to date monograph bargains a wide synoptic description of beams in accelerators and different units with negligible to powerful house cost results. The publication develops fabric in a scientific approach and discusses the underlying physics and validity of theoretical relationships, layout formulation and scaling legislation. Assumptions and approximations are truly indicated throughout.The re-creation of conception and layout of Charged Particle Beams has major extra content material, which covers experiments, idea, and simulation in beam physics learn on the grounds that 1993, while the 1st version used to be released. It contains the college of Maryland Electron Ring for learning space-charge ruled beams in earrings and re-circulators.From the Contents:Review of Charged Particle DynamicsBeam Optics and Focusing structures with no area ChargeLinear Beam Optics with area ChargeSelf-Consistent conception of BeamsEmittance VariationBeam Physics study from 1999 to 2007
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Extra resources for Theory and Design of Charged Particle Beams
Sample text
1 eV, the brightness has an upper limit of Bn = 8 × 1010 A/(m-rad)2 . 12b) In practice, the brightness of the electron beam in the system downstream from the electron gun will always be less than this ideal value. The preceding discussion was intended to provide an introductory overview of basic design principles of charged particle sources and of the fundamental performance limits of high-intensity beams due to constraints imposed by the physics and technology of source operation. 23 listed in the bibliography, and in the 13 14 1 Introduction proceedings of accelerator conferences or topical meetings on low-energy beams and sources.
2964, ed. Wurtele, J. S. 3 Fraser, J. , Sheffield, R. , Gray, E. , Rodenz, G. , IEEE Trans. Nucl. Sci. NS-32, 1791 (1985); Fraser, J. , Sheffield, R. , IEEE J. Quantum Electron. 23, 1489 (1987). , “High Current, High Brightness, and High Duty Factor Ion Injectors,” AIP Conf. Proc. 139, 1 (1986), ed. , Kuo, Y. , Wangler, T. P. 1 The Lorentz Force and the Equation of Motion In this chapter we present a brief review of the methods of relativistic classical dynamics for determining the motion of charged particles in electromagnetic fields.
This appears to be a reasonable compromise between the two extreme cases of α = 1 and α = 2. It should be pointed out, however, that such simple scaling laws have to be used with some caution. In practice, electrical breakdown is a very complicated phenomenon that depends on many details (other than gap spacing and voltage), such as gas flow from the source, geometry of the electrode structures, and surface cleanliness. Another important constraint influencing the output characteristics (perveance and emittance) of high-current, low-emittance charged particle sources is imposed by considerations of beam optics.