Titlebook: Measurement and Control of Charged Particle Beams; Michiko G. Minty,Frank Zimmermann Textbook‘‘‘‘‘‘‘‘ 20031st edition The Editor(s) (if ap

Flange

書目名稱Measurement and Control of Charged Particle Beams影響因子(影響力)




書目名稱Measurement and Control of Charged Particle Beams影響因子(影響力)學(xué)科排名




書目名稱Measurement and Control of Charged Particle Beams網(wǎng)絡(luò)公開度




書目名稱Measurement and Control of Charged Particle Beams網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Measurement and Control of Charged Particle Beams被引頻次




書目名稱Measurement and Control of Charged Particle Beams被引頻次學(xué)科排名




書目名稱Measurement and Control of Charged Particle Beams年度引用




書目名稱Measurement and Control of Charged Particle Beams年度引用學(xué)科排名




書目名稱Measurement and Control of Charged Particle Beams讀者反饋




書目名稱Measurement and Control of Charged Particle Beams讀者反饋學(xué)科排名

Meander

Transverse Optics Measurement and Correction,tribution of a beam injected into a storage ring is not matched to the ring optics, the emittance will grow due to filamentation. Or, if there is a significant optics error, e.g., induced by a strength error in a quadrupole magnet, the beam envelope may vary strongly. The resulting reduction in dyna

開始發(fā)作

Orbit Measurement and Correction,Such uncertainties include the variations in the electronic and/or mechanical centers of the beam position monitors (BPMs), in the magnetic center of the quadrupoles (inside which the position monitors are often mounted), or in the electromagnetic center of accelerating structures. Consider the case

聰明

Transverse Beam Emittance Measurement and Control,se positions, . and . are the transverse angles, . is the time-like variable representing the relative phase of the beam, and . is the relative beam momentum error. Using the notation of the beam matrix .. introduced in Chap. 1, the 6-dimensional emittance is . Considering now only the horizontal pl

placebo

Collimation,since they produce a background in the particle-physics detector. The background arises either when the halo particles are lost at aperture restrictions in the vicinity of the detector, producing electro-magentic shower or muons, or when they emit synchrotron radiation that is not shielded and may h

輕而薄

Longitudinal Optics Measurement and Correction,tage. Usually one employs a smooth approximation, i.e., one ignores the discrete locations of the rf cavities, in describing the particle motion. The longitudinal motion can then be modelled by second order differential equations. For small oscillation amplitudes these equations simplify to those of

Synovial-Fluid

Longitudinal Phase Space Manipulation, second moments of the longitudinal distribution; that is, on the bunch length and energy spread. As will be shown, the bunch length can be varied using accelerating cavities to compress, coalesce, split, and lengthen stored bunches. The energy spread of the beam can also be adjusted (usually to be

VICT

Spinous-Process

Polarization Issues, beam energies. A selection of reviews of the dynamics of polarized beams may be found in [1]–[9]. In this chapter, we focus on experimental data and describe spin transport in circular accelerators and transport lines. Except where explicitly mentioned, radiative effects in electron accelerators or

稀釋前