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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... protons or heavy ions but is practicable for electrons. The principle was suggested by Vladimir Veksler and Julian Schwinger in 1944, and is illustrated in Fig. 1.11. In 1965, Schwinger was awarded the Nobel Prize; see Table 1.1. The ...
... protons has been obtained. The disadvantage of a synchrocyclotron compared with a cyclotron is the reduced current. Only one bunch at a time is sent through the synchrocyclotron, compared with lots of pulses through the cyclotron ...
... protons and heavy particles , it is not so easy to inject at relativistic speed . Therefore both the RF field and the ... proton synchrotron was the 3 GeV Cosmotron in Brookhaven National Laboratory , completed in 1952. Its ring of ...
... proton - proton colliding - beam accelerator is the CERN Intersecting Storage Rings ( ISR ) , in operation during the period 1972-83 , with two beams of 28 GeV from the CERN proton synchrotron directed into two interlacing storage rings ...
... proton ion neutrons LHC WEST AREA P Ti2 antiproton n - ToF n TT10 ISOLDE AD TT2 р P TT20 NORTH AREA not to scale D AD PS SPS electron Neutrinos Antiproton Decelerator Proton Synchrotron Super Proton Synchrotron EAST AREA p BOOSTER LHC ...
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 |