Electrostatic Accelerators: Fundamentals and ApplicationsRagnar Hellborg Springer Science & Business Media, 2005/11/02 - 620 ページ Electrostatic accelerators are an important and widespread subgroup within the broad spectrum of modern, large particle acceleration devices. They are specifically designed for applications that require high-quality ion beams in terms of energy stability and emittance at comparatively low energies (a few MeV). Their ability to accelerate virtually any kind of ion over a continuously tunable range of energies makes them a highly versatile tool for investigations in many research fields including, but not limited to, atomic and nuclear spectroscopy, heavy ion reactions, accelerator mass spectroscopy as well as ion-beam analysis and modification. The book is divided into three parts. The first part concisely introduces the field of accelerator technology and techniques that emphasize their major modern applications. The second part treats the electrostatic accelerator per se: its construction and operational principles as well as its maintenance. The third part covers all relevant applications in which electrostatic accelerators are the preferred tool for accelerator-based investigations. Since some topics are common to all types of accelerators, Electrostatic Accelerators will also be of value for those more familiar with other types of accelerators. |
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... proton accelerator, and with a beam of 400 keV they induced the reaction Li + p → 2He (1.2) In 1951, Cockcroft and Walton obtained the Nobel Prize; see Table 1.1. The years around 1930 can be taken as the starting point of the accelera ...
... Proton storage SPS ring colliders et - e storage ring colliders 100 Proton synchrotrons GeV 10 Electron synchrotrons 1 -Synchrocyclotrons 100 Sector focused cyclotrons Cyclotrons MeV 10 Electrostatic accelerators 1930 Cascade ...
... electrons and 800 MeV for protons . In 1947 , Luis Alvarez built beam drift tubes RF source vacuum enclosure Fig . 1.6 . Principle of a linear accelerator a machine [8] with a structure which differed significantly from. 12 R. Hellborg.
... protons of 1.2 MeV . The two dees are connected to the RF source ( usually within the range of 10-30 MHz ) so that an alternating voltage appears across the gap separating the dees . An ion source , located at the center of the chamber ...
... protons are up to 20–30MeV, cor- responding to a magnet diameter of little more than 1 m. As the beam in a cyclotron travels outwards towards the edge of the magnet, the magnetic field lines are diverted somewhat from true straight ...
目次
3 | |
43 | |
Electrostatics | 64 |
Calculation Technique for HighVoltage Equipment | 84 |
Development of Charging Belts in Russia | 101 |
Voltage Distribution Systems Resistors | 110 |
Accelerator Tubes | 123 |
Development of Tubes | 147 |
Nonradiation Hazards and Safety Considerations | 365 |
ElectrostaticAccelerator FreeElectron Lasers | 378 |
Introduction to Part III Research Fields | 392 |
Roberts T E Barnhart R J Nickles 395 | 413 |
Corradi | 429 |
Detection of Explosives and Other Threats | 445 |
Accelerator Mass Spectrometry | 461 |
Atomic Collisions in Matter | 486 |
Stripper Systems | 166 |
Charge Exchange and Electron Stripping | 181 |
NegativeIon Formation Processes | 222 |
Tandem Terminal Ion Source | 274 |
Beam Envelope Techniques for IonOptical Calculations | 299 |
Equipment for Beam Diagnostics | 317 |
Radiation Protection at an Accelerator Laboratory | 337 |
Modification of Materials | 508 |
Ion Beam Analysis | 530 |
Atomic Structure | 560 |
Industrial Electron Accelerators | 581 |
Electrostatic Accelerators Production | 595 |
Index | 608 |