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Booster (particle accelerator)

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Article Genealogy
Parent: CERN LHC Hop 5
Expansion Funnel Raw 83 → Dedup 0 → NER 0 → Enqueued 0
1. Extracted83
2. After dedup0 (None)
3. After NER0 ()
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Booster (particle accelerator)
NameBooster (particle accelerator)
TypeSynchrotron/Booster ring
LocationVarious laboratories
EstablishedEarly 20th century developments
OperatorNational laboratories and universities
EnergyInjection and intermediate energies

Booster (particle accelerator) is a circular intermediate accelerator used to increase the energy of charged particles between an injector and a main accelerator such as a synchrotron, collider, or storage ring. Boosters appear at facilities like Brookhaven National Laboratory, CERN, Fermilab, SLAC National Accelerator Laboratory, and DESY, where they link injectors such as cyclotrons, linacs, and ion sources to higher-energy stages. They underpin programs at institutions including Argonne National Laboratory, Lawrence Berkeley National Laboratory, KEK, and TRIUMF and are integral to projects like Large Hadron Collider, Relativistic Heavy Ion Collider, Spallation Neutron Source, European XFEL, and ISIS Neutron and Muon Source.

Overview

Boosters function within accelerator complexes involving components from Van de Graaff generators, Cockcroft–Walton systems, and linear accelerators to rings like the Proton Synchrotron and Super Proton Synchrotron. They occupy a niche between devices such as ion sources, radio-frequency quadrupoles, and main rings exemplified by Main Injector and Tevatron in historical contexts. Prominent booster designs derive heritage from pioneers including Ernest Lawrence, Rolf Widerøe, Luis Alvarez, and institutions like CERN Accelerator School and Brookhaven National Laboratory training programs. Accelerator collaborations such as FAIR, ITER (for neutral beam injectors), and ITER Neutral Beam Test Facility influence booster development.

Design and Components

Typical booster rings integrate magnets, radio-frequency (RF) cavities, vacuum systems, diagnostics, and power supplies similar to those in Superconducting Super Collider proposals and modernized by technology from National Ignition Facility engineering efforts. Magnet systems include dipoles, quadrupoles, and sextupoles comparable to arrays used at Diamond Light Source and PETRA III; superconducting options draw on advances at SNS superconducting linac programs and DESY superconducting R&D. RF systems reference concepts from Stanford Linear Accelerator Center and TRIUMF RF groups, while vacuum and beam instrumentation reflect heritage from Los Alamos National Laboratory, Rutherford Appleton Laboratory, and Oak Ridge National Laboratory. Control systems often use standards developed at CERN Control Centre and software from EPICS collaborations involving SLAC and Fermilab.

Operation and Beam Dynamics

Beam capture, acceleration, and extraction in booster machines involve synchrotron motion, betatron oscillations, and space-charge effects studied by teams at Institute of High Energy Physics (China), National Institute for Nuclear Physics (Italy), Institute for Nuclear Research (Russia), and KEK Theory Center. Emittance control and lattice design employ techniques from MAD-X and simulation tools developed at GSI Helmholtz Centre for Heavy Ion Research and Cockcroft Institute. Resonance correction schemes and chromaticity compensation build on methods proven at SLAC National Accelerator Laboratory and CERN test facilities; injection painting and multiturn injection draw on experiments at GANIL and RIKEN. Beam loss mitigation leverages diagnostics from RIA proposals and collimation strategies seen at LHC and RHIC.

Types and Notable Examples

Booster varieties include proton boosters, electron boosters, ion boosters, and synchrotron booster concepts used in light sources and colliders. Notable installations: the Brookhaven Booster, the Fermilab Booster, the CERN Proton Synchrotron Booster, and the booster ring at TRIUMF. Synchrotron light source boosters serve facilities such as SPring-8, Advanced Photon Source, ESRF, Max IV Laboratory, and SOLEIL. Heavy-ion boosters appear at GSI, FRIB, and FAIR pre-accelerators. Examples of upgrade campaigns reference projects at Spallation Neutron Source, Diamond Light Source and modernization programs at KEK PF and APS Upgrade.

Applications

Boosters support research programs in high-energy physics at ATLAS (particle detector), CMS (particle detector), and ALICE (A Large Ion Collider Experiment) by supplying beams to colliders and storage rings. They feed synchrotron light sources used by scientists from CERN, DESY, Argonne National Laboratory, and Diamond Light Source for experiments in materials science, biology, and chemistry. Medical isotope production and proton therapy rely on booster-fed systems in hospitals partnered with Paul Scherrer Institute and MD Anderson Cancer Center initiatives. Neutron spallation and muon facilities such as ISIS Neutron and Muon Source and J-PARC use booster rings for target irradiation, while accelerator-driven systems draw on booster technologies explored at Department of Energy laboratories and international consortia.

Challenges and Upgrades

Common challenges include managing space-charge limits, mitigating beam loss, and extending component lifetimes amid radiation damage studied at CERN Radiation Protection programs and Oak Ridge materials science groups. Upgrades employ superconducting RF from European XFEL developments, new magnet designs inspired by High Luminosity LHC research, and digital control advances from CERN and SLAC collaborations. Funding and policy decisions from entities like Department of Energy (United States), European Commission, Japanese Ministry of Education, Culture, Sports, Science and Technology, and national research councils shape upgrade timelines alongside multinational projects such as ITER and FAIR. Future booster concepts interface with proposals for compact accelerators at Lawrence Livermore National Laboratory and novel injector chains under investigation at CERN and KEK.

Category:Particle accelerators