
	Where results make sense

Topic: Isochronous cyclotron

	Oak Ridge Isochronous Cyclotron (Site not responding. Last check: 2007-10-23)
		The Oak Ridge Isochronous Cyclotron (ORIC) is a variable energy, multiparticle accelerator which was completed in 1962.
		The isochronous, or azimuthally varying field (AVF), cyclotron concept was first proposed in 1938 by L.H. Thomas.
		Isochronism refers to the constant orbit frequency of circulating ions obtained by radially increasing the magnetic field to compensate for relativistic increases in ion mass.
	www.phy.ornl.gov /hribf/accelerator/oricweb (159 words)

	Cyclotron - Wikipedia, the free encyclopedia
		Cyclotrons can also be configured to strip hydrogen atoms of their electrons, producing a stream of high-energy protons which can be used to bombard other atoms to produce short-lived positron-emitting isotopes suitable for PET imaging.
		The cyclotron is an improvement of the linear accelerator.
		As the beam speed increases, cyclotron radiation is emitted from the side of the beam, because the magnet is turning and slowing, ("braking") the beam.
	en.wikipedia.org /wiki/Cyclotron (1415 words)

	Synchrocyclotron - Wikipedia, the free encyclopedia
		A synchrocyclotron is a cyclotron in which the frequency of the driving RF electric field is varied to compensate for the mass gain of the accelerated particles as their velocity begins to approach the speed of light.
		Isochronous cyclotrons maintain a constant RF driving frequency and compensate for the relativistic mass gain of the accelerated particles by increasing the magnetic field with radius.
		Isochronous cyclotrons are capable of producing much greater beam current than synchrocyclotrons.
	en.wikipedia.org /wiki/Synchrocyclotron (174 words)

	Crocker Nuclear Laboratory...
		The unique capabilities of the 76-inch cyclotron and related facilities at CNL have been utilized by scientists and engineers from private industry, universities and government agencies.
		The Cyclotron is also used to support many of the "in-house" research projects.
		The Cyclotron is the tool used in the analyzing of the samples collected by the Air Quality Group; to make radioisotopes used for medical research; and produces the energy used for the treatment of eye tumors.
	dhcp23.cnl.ucdavis.edu (208 words)

	S.B. Vorozhtsov_abstract (Site not responding. Last check: 2007-10-23)
		The compact isochronous cyclotron is considered as a source of 1.75 MeV protons for the detection of explosives using gamma-ray resonant absorption technique.
		Given the marginal request for the beam intensity and quality H¯ ions were selected for acceleration in the cyclotron aiming at the high efficiency extraction either by stripping at the 1st stage or by Electrostatic Deflector (ESD) attempting to meet the output beam specifications.
		Calculation of the 30 mA CW beam motion through the cyclotron gave axial losses ~66% of the total intensity, radial losses of ~14% and ~20% of particles are accepted in the acceleration regime, corresponding to ~6 mA.
	www.jinr.dubna.su /RuPAC2004/Abstracts/SVorozhtsov_abstract.html (430 words)

	Dzhelepov Laboratory of Nuclear (Site not responding. Last check: 2007-10-23)
		A project of external beam injection in the central region of the accelerator is being developed to increase the intensity of the JINR Phasotron from 5 to 50 µA. Table 1.
		Designing a cyclotron with this mean beam current requires detailed information on the effect of the space charge on particle dynamics.
		The particle dynamics were simulated for a bunch of phase extent 16° RF with particles uniformly distributed within phase ellipses (the xial and radial emittances in injection were 50 π mm mrad).
	nuweb.jinr.ru /~gkaram/science5_eng.htm (757 words)

	Cyclotrons and Synchrotrons: principle of operation
		A cyclotron is not useful for acceleration of electrons since their rotation frequency in a magnetic field slows down quite rapidly even for as low energies as a few MeV due to the small rest mass of an electron.
		A variant of the cyclotron is the microtron in which electrons are accelerated at one gap at the periphery of the orbits.
		The sector-focusing cyclotron is sometimes called continuous wave (CW) cyclotron or isochronous cyclotron, to differentiate it from the frequency modulated (FM) cyclotron or the synchrocyclotron.
	synchrotrons.net /operation.html (1886 words)

	Dzhelepov Laboratory of Nuclear (Site not responding. Last check: 2007-10-23)
		CYTRACK is an isochronous cyclotron with azimuthally varying field (four pairs of sector shims) axial injection, radio-frequency accelerating system and electrostatic deflectors for extracting ions from the accelerator.
		A general plan of the cyclotron with 4 sector shims S, 2 dees of RF system D1 and D2, electrostatic deflectors ESD1, ESD2 followed by magnetic focusing channel FD is shown in Fig.
		The spiral inflector for ion bending from axial to median plane is used There is a possibility of inflector rotation by ±8° to assure fitting of ion trajectories from inflector to central region trajectories in radius, radial and azimuth.
	nuweb.jinr.ru /~gkaram/science2_eng.htm (723 words)

	Institute of Nuclear Physics NNC RK
		The cyclotron was designed at the D.V.Efremov's institute (St.-Petersburg, Russia) and put into operation at the "classic made" in 1965 with fixed energy of ac celerated particles (p, d, aa) of 10 MeV/nucleon.
		In 1972 the cyclotron was transformed to the isochronous mode with adjustable energies of ions.
		The cyclotron is provided with the He gas recycling system, the system for external beam transportation, the beam scanning system over a solid target, the system of the beam contactless diagnostics, etc. The cyclotron is used for radioisotope production, nuclear investigations, radiation material science.
	www.inp.kz /indexeng.php?part=3 (327 words)

	1105-1113 (Site not responding. Last check: 2007-10-23)
		An electron model of an axially-symmetric isochronous cyclotron was constructed and the beam properties were investigated for the purpose of studying, experimentally, an accelerator using electric and magnetic fields in combination as a guide field.
		As a model cyclotron of those which accelerate proton beams up to ∼100 MeV, a maximum energy of electrons of 50 KeV (γ\cong1.1) was chosen.
		The isochronous field of the cyclotron was composed of electric and magnetic fields -- the electric field having a radial component and the magnetic field having an axial component on the median plane.
	jjap.ipap.jp /link?JJAP/7/1105 (180 words)

	Design Studies for an Ultra High Field K80 Cyclotron (Site not responding. Last check: 2007-10-23)
		We are investigating the use of a wide-bore, 8 T magnet as a component of an ultra high field cyclotron.
		The K80 `Eight Tesla Cyclotron' would have roughly the same magnetic rigidity (B\rho) as the Oak Ridge Isochronous Cyclotron in a package of only one fourth the radius, with a corresponding reduction in cost.
		This cyclotron could accelerate particles with a charge state Q/A = \frac14 to a final energy of between 5 and 6 MeV/nucleon, the energy range currently being used to study superdeformed, high angular momentum nuclei that result from glancing collisions.
	flux.aps.org /meetings/BAPSMAY96/abs/S1530008.html (168 words)

	Accelerator facilities
		The major improvement in the performance of the K130 cyclotron was achieved by building a new 14.5 GHz ECR ion source.
		The intensities of heavy-ion beams from the cyclotron will increase by a factor of 10 for the medium heavy ions and it is possible to accelerate heavier elements (e.g.
		Negative ions can be extracted with 100 percent efficiency from the cyclotron by shooting them in the end of the acceleration trough a thin carbon foil, which will strip electrons from the hydrogen atoms, and the positively charged protons will immediately bend out from the magnetic field of the cyclotron.
	www.phys.jyu.fi /research/accelerator/facilities/facilities.html (738 words)

	INCT Home Page
		This paper is a description of the automatic isochronous cyclotron, AIC-144, designed and built with the author in charge, at the Institute of Nuclear Physics, Krakow in cooperation with Polish industrial firms.
		The cyclotron was designed for applications in various areas of science and technology.
		The AIC-144 cyclotron was intended to accelerate in an adjustable energy range a wide variety of ions with the ratio of charge to atomic mass Z/A = 0.285
	www.ichtj.waw.pl /ichtj/nukleon/back/abstract/vol42_1997/v42n3p727.htm (182 words)

	Forschungszentrum Jülich GmbH - Institute for Nuclear Physics
		The internal experiments which are an integral part of the COSY accelerator ring and external experiments set up in separate areas are predominantly used for fundamental research in medium-energy hadron physics.
		In parallel to the operation of COSY the cyclotron beam alone may be also used for irradiation and nuclide production.
		Isochronous cyclotron with proton beams of about 300 MeV/c momentum and deuteron beams with a momentum of 550 MeV/c
	www.fz-juelich.de /ikp/en/ikp_gg.shtml (292 words)

	Crocker Nuclear Laboratory...
		Crocker Nuclear Laboratory houses a medium-energy particle accelerator, the Davis 76-inch isochronous cyclotron, with associated facilities and scientific and technical personnel.
		The unique capabilities of the 76-inch cyclotron and related facilities at CNL have been utilized by scientists and engineers from private industry, universities and government agencies.
		The Cyclotron is the tool used in the analyzing of the samples collected by the Air Quality Group; to make radioisotopes used for medical research; and produces the energy used for the treatment of eye tumors.
	media.cnl.ucdavis.edu /Crocker/WebSite/default.php (208 words)

	[No title] (Site not responding. Last check: 2007-10-23)
		A contract was signed with Philips to build an isochronous cyclotron, which was completed in 1970.
		The cyclotron is equipped with three external ion sources: a cusp source for the production of intense beams of protons, deuterons and alpha particles, an ECR ion source for the prodution of light and heavy ions and a polarized-ion source for protons and deuterons.
		Since 1998, the operation, improvement and development of the AGOR cyclotron is accomodated in a so-called FOM programme.
	www.kvi.nl /~secreta/pr/wwwhist.txt (719 words)

	CERN Courier - Silver celebration for Swiss - IOP Publishing - article
		The then director, Jean-Pierre Blaser, and the late Hans Willax, the designer of the ring cyclotron concept, were seen with "silent glows" on their faces.
		The opening address was given by deputy director Ralph Eichler, who set the scene and outlined the present range of experiments at the Ring Accelerator, with the continuing trend towards larger and longer types of precision measurements.
		Then it was the turn of Claude Joseph (Lausanne), a long-standing experimenter at the facility, and Florian Scheck (Mainz), former head of the SIN Theory Group, to summarize physics milestones in the strong interaction and electroweak sectors respectively.
	www.cerncourier.com /main/article/39/10/18 (919 words)

	Centre de Recherches du Cyclotron - CRC
		(CYClotron de LOuvain-la-NEuve) was built in the early seventies by Thompson CSF in collaboration with ACEC.
		CYCLONE is a multiparticle, variable energy, isochronous cyclotron capable of accelerating protons up to 80 MeV, deuterons up to 55 MeV, alpha particles up to 110 MeV and heavier ions up to an energy of 110 Q
		It is a fixed field fixed frequency cyclotron, capable of accelerating H
	www.cyc.ucl.ac.be /Facility (292 words)

	Crocker Nuclear Laboratory...
		The accelerator, an isochronous cyclotron, is one of the few of this design remaining in productive operation.
		The Crocker Nuclear Labortory's Isochronous Cyclotron began operating in 1965, accelerating protons, alpha particles, and other light ions into various targets to study nuclear structure.
		Instead of the uniform magnetic fields used in the earlier cyclotrons, the isochronous design employed tailored sectors with a varying magnetic field.
	media.cnl.ucdavis.edu /Crocker/Website/b_Information/index.php (203 words)

	THEME05-2-1038-2001/2006
		Improvement of the parameters of the isochronous cyclotron AIC-144, Krakow, Poland.
		Improvement of the parameters of the cyclotron U-115T, Tashkent.
		Consideration of the cyclotron variants in order to determine the type of particles and their energy; computer simulation of the beam dynamics and choice of the magnetic and accelerating field parameters; computation of the magnet and the resonator.
	www.jinr.ru /~golosk/ptp-2004/e421038.htm (367 words)

	Cyclic Accelerator R&D Division (Site not responding. Last check: 2007-10-23)
		The investigations concerning the improvement of the operation parameters of cyclotrons that are at present operating in the world are one of the main subjects of our interest.
		Basic parameters of conventional isochronous cyclotrons as well as sector ring Isochronous Cyclotron with separated magnets.
		Full analysis of the effect of resonance excitations in the beam accelerated on the isochronous cyclotrons.
	chall.ifj.edu.pl /cyklo.html (336 words)

	Simulation of Space-Charge Dominated Beam Dynamics in an Isochronous AVF Cyclotron (ResearchIndex) (Site not responding. Last check: 2007-10-23)
		If your firewall is blocking outgoing connections to port 3125, you can use these links to download local copies.
		Abstract: This paper describes a beam dynamics code `PICN' for simulation of high current proton beams in an isochronous azimuthally-varying-field cyclotron.
		It is assumed that the median plane and vertical motions are decoupled, so that the internal space-charge forces can be calculated by a particle-in-cell method applied to the median plane charge distribution.
	citeseer.ist.psu.edu /208813.html (273 words)

	[No title] (Site not responding. Last check: 2007-10-23)
		At the Karlsruhe Isochronous Cyclotron a beam of about 3 ?A of 40-MeV deuterons impinged on a saturation thick target of natural lithium.
		Any deuteron beam energy lower than 52 MeV would have been available at this cyclotron only by positioning the target some way inside the cyclotron magnet gap, so that it cuts into the spiralling beam trajectory, which means that the beam will hit the target only near one of its edges.
		With the full energy, however, the `lifted' beam could be used, i.e., the beam was deflected away from its preceding turn by several millimeters using an electrostatic septum, as if it were to be extracted to a beam line.
	www.ubka.uni-karlsruhe.de /vvv/fzk/6764/6764.text (3504 words)

	The Gustaf Werner cyclotron (Site not responding. Last check: 2007-10-23)
		Possible to use between 12.25 and 24.5 MHz (on the orbit frequency of the ions and on harmonics 2, 3 and 4).
		Principle in isochronous mode is precessional extraction and in synchrocyclotron mode regenerative extraction.
		An ECR source is used for a wide variety of ions (from alfa particles to Xenon), and a polarized source is available for protons and deuterons.
	www3.tsl.uu.se /~bengtl/webcyc/cycl.html (278 words)

	Operation, Development and Construction of Large Scale Nuclear Physics Instruments (Site not responding. Last check: 2007-10-23)
		Operation and development of the accelerator facility comprising the cooler-synchrotron COSY-Jülich, the injector isochronous cyclotron JULIC and various experimental facilities.
		Parallel to the operation of COSY the cyclotron beam is utilized for irradiation and nuclide production.
		Isochronous Cyclotron with proton beams between 22.5 - 45 MeV
	www.fz-juelich.de /ikp/cosy/maier_e.html (307 words)

	History
		This allowed for the acceleration of heavy ions in the cyclotron and was
		The cyclotron is equipped with three external ion sources: a cusp source
		In addition to fundamental nuclear-physics experiments, the AGOR accelerator is also used for radiobiology experiments with proton beams and for experiments dedicated to applications, e.g., irradiation of electronic components and measuring cross sections needed in the simulation of accelerator-driven systems for waste transmutation and energy amplification.
	www.kvi.nl /LB/about/history.htm (620 words)

	LavaCUBED \Science\Physics\Nuclear\Facilities (Site not responding. Last check: 2007-10-23)
		Radioactive ions are produced by the K=105 Oak Ridge Isochronous Cyclotron (ORIC).
		The radioactive elements are injected into the 25 MV Tandem Accelerator producing beams of 0.1-10 MeV per nucleon for light nuclei and up to 5 MeV per nucleon for mass 80.
		National Superconducting Cyclotron Laboratory - National user facility located at Michigan State University, operating two coupled cyclotrons for basic research in nuclear science as well as accelerator and instrumentation research and development.
	www.lavacubed.com /new.cats.php?path=/Science/Physics/Nuclear/Facilities (489 words)

	Beam Dynamics
		The former Beam Dynamics Group, now integrated in the High Intensity Accelerator Section is responsible for providing the theoretical background in accelerator theory and for designing and maintaining control computer programs for beam diagnostics and beam optimisation in order to support the successful operation of the PSI accelerator complex.
		With an intensive study that has started towards the end of 1997 we plan to substantially increase our knowledge on space charge effects in cyclotrons.
		Proceedings of the 13th Cyclotron Conference, Vancouver, 1992.
	abe.web.psi.ch /hsb/bdynhome.php (360 words)

	What is the TESLA Accelerator Installation? (Site not responding. Last check: 2007-10-23)
		The TESLA Accelerator Installation is an ion accelerator facility consisting of a compact isochronous cyclotron - the VINCY Cyclotron, an electron cyclotron resonance heavy ion source - the mVINIS Ion Source, a volume light ion source - the pVINIS Ion Source, and a number of low energy and high energy experimental channels.
		The construction of this facility has been going on the Vinca Institute of Nuclear Sciences, in Belgrade, Yugoslavia.
		The VINCY Cyclotron will be able to deliver, e.g., 4 µA of 27 MeV per nucleon N
	tesla.rcub.bg.ac.yu /~vincy/vincy2.html (235 words)

	shtursa (Site not responding. Last check: 2007-10-23)
		The isochronous cyclotron U-120M (in operation since 1977) was designed in Dubna (the former USSR) as an accelerator of light positively charged particles (A/Z = 1 - 2.8, K = 40).
		Due to its low extraction efficiency (several mA), solely the internal targets have been routinely used for effective radionuclide production where the internal beam currents reach several hundreds of mA.
		The effective method of extracted beam increase is the acceleration of negative H-/D- ions and their extraction by means of the charge exchange on the thin stripping carbon foil.
	uc.jinr.ru /SummerSchool/shtursa.html (272 words)

Try your search on: Qwika (all wikis)