'Round beam' presentation slideshows

The 4 n =1 resonance of a high intensity linac

The 4 n =1 resonance of a high intensity linac. D. Jeon (SNS) I. Hofmann, L. Groening, G. Franchetti (GSI) HB 2008 August 25-29, 2008. This work is the result of the collaboration between GSI and SNS. Thanks to J. Galambos, S. Henderson for the support. History of halo formation mechanisms.

418 views • 41 slides

Summary: Observations of Lepton Colliders

Summary: Observations of Lepton Colliders. [ ICFA Mini-Workshop on Beam-Beam Effects in Hadron Colliders]. John Seeman March 22, 2013. Topics. Yoshihiro Funakoshi: KEKB Crab Cavities Experience Mikhail Zobov : DAFNE Large Piwinski Angle and Crab Waist

449 views • 32 slides

Hong Qin and Ronald C. Davidson Plasma Physics Laboratory, Princeton University

Non-Abelian Courant-Snyder Theory for Coupled Transverse Dynamics. Hong Qin and Ronald C. Davidson Plasma Physics Laboratory, Princeton University US Heavy Ion Fusion Science Virtual National Laboratory www.princeton.edu/~hongqin/. How to make a smooth round beam?. Solenoid

455 views • 31 slides

Prospective for Flat Beam Optics

S. Fartoukh AB/ABP, LHC MAC no. 19, 15-17 June 2006 Acknowledgment for technical support and fruitful discussions: W. Herr, B. Jeanneret, E. McIntosh, F. Schmidt, F. Zimmermann. Prospective for Flat Beam Optics. Potential of flat beam optics :

263 views • 20 slides

CCR Status, 1/31/2012

268 views • 18 slides

Electron Beam Disruption Simulations

Electron Beam Disruption Simulations. Yue Hao C-AD, BNL. Beam-Beam Model. For an exactly round beam with transverse Gaussian distribution, the electric field is expressed as:. The field amplitude increase linear with r at small r, decrease as 1/r at large r. The maximum occur at r= 1.585 ?.

226 views • 10 slides

X-Ray SASE FEL

e + e - Linear Colliders. X-Ray SASE FEL . Flat Beam Production.

200 views • 7 slides