2 edition of **Transverse oscillations of a relativistic particle beam in a laminated vacuum chamber** found in the catalog.

Transverse oscillations of a relativistic particle beam in a laminated vacuum chamber

Bruno W. Zotter

- 7 Want to read
- 4 Currently reading

Published
**1969**
by CERN in Geneva
.

Written in English

- Particle beams.

**Edition Notes**

Statement | [by] B. Zotter. |

Series | CERN 69-15, CERN (Series) ;, 69-15. |

Classifications | |
---|---|

LC Classifications | QC770 .E82 1969, no. 15 |

The Physical Object | |

Pagination | iii, 41 p. |

Number of Pages | 41 |

ID Numbers | |

Open Library | OL5384367M |

LC Control Number | 72489932 |

Detailed particle-in-cell simulations on the transport of a relativistic electron beam in plasmas Anupam Karmakar,* Naveen Kumar,† and Alexander Pukhov Institut für Theoretische Physik I, Heinrich-Heine-Universität, Düsseldorf , Germany O. Polomarov and Gennady Shvets. Numerical analysis of 10's femtosecond relativistic electron beam generation using single 12TW50fs laser pulse. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, Vol. , Issue. 1, p. Cited by:

As shown in Fig. 4, the betatron functions of the matrix expression are well reproduced in the 3-D tracking and the derived formulae precisely describe the beam envelope of the relativistic beam, for which the space charge can be gh the field strengths of the quadrupole magnets are constant in a conventional FODO lattice, the focusing strengths K F,D in Table 1 are slightly by: 1. An intense charged particle beam can be characterized as an organized charged particle flow for which the effects of beam self-fields are of major importance in describing the evolution of the flow. Research employing such beams is now a rapidly growing field with important applications ranging.

Researchers at the RIKEN Advanced Science Institute (ASI) have developed a theory that provides an understanding of relativistic electron vortex beams. Through the combined consideration of quantum and relativistic properties of the electrons in the beam, the researchers found that spin–orbit inter. Radiative cooling is a natural and effective method of phase-space cooling for stored electron beams. In electron storage rings the average effects of synchrotron radiation from the bending magnets cause the beam emittances in all three degrees of freedom to damp towards equilibria, determined by the fluctuating nature of quantum emissions. In this paper, they show that the radiation damping Cited by: 5.

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KINETIC DESCRIPTION OF COUPLED TRANSVERSE OSCILLATIONS IN AN INTENSE RELATIVISTIC ELECTRON BEAM-PLASMA SYSTEM Han S. Uhm Naval Surface Weapons Center White Oak, Silver Spring, Maryland Ronald C. Davidson Plasma Fusion Center Massachusetts Institute of Technology Cambridge, Massachusetts A relativistic particle is a particle which moves with a relativistic speed; that is, a speed comparable to the speed of is achieved by photons to the extent that effects described by special relativity are able to describe those of such particles themselves.

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the Fundamental and Applied Physics for acceptance a thesis entitled “Self-Modulated Dynamics of Relativistic Charged Particle Beams in Plasmas” by Tahmina Akhter as partial fulﬁllment of the requirements for the degree of Doctor of Philosophy. Dated: Ma Research Supervisor: Professor Renato Fedele Co-Supervisors: Dr.

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A comparison is made between analytic asymptotic forms, linearized “beam break-up” simulations, and particle-in-cell by: The beam profile is measured primarily to find the transverse beam emittance which is the area occupied by the beam in transverse phase space, i.e.

(x, p x). The beam radius at the IPM is equal to the square root of the betatron function, β IPM, times the by: 8. the beam state at the entrance of the cooler is matched with its state at the cathode so that the conditions (4) are satisfied, the beam transverse velocities are finally can-celed.

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The relativistic momentum. p = mv = γm 0 v. departs by 1% from the non-relativistic expression when γ = This occurs for β = or v = c. The kinetic energy at this speed is (γ - 1)m 0 c 2 = m 0 c 1% threshold is then keV for electrons and MeV for protons.Computational Science Laboratory Projects Simulation Studies of Novel Methods for Cooling of Relativistic Particle Beams.

Comparison of simulation and theory of the re-distribution of electron cloud in the vicinity of relativistic beam ions. Simulations are affected by the shot noise.Calculate the phase velocity of a relativistic particle. Solution: Assume a particle of mass m and traveling with a speed of v.

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