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1993, Il Nuovo Cimento A
Previous heavy-ion fusion driver system studies suggest that transverse beam combining significantly reduces driver cost. In a combiner, several beams are brought together to a common transport channel which accommodates the increased line charge density. Combining intense beams increases the transverse emittance mainly due to the heating of the beam by space charge forces as the non-uniform original beam configuration becomes more uniform. The combiner itself introduces additional aberrations, which are small for the present design. Those aberrations are due to the reduced available space for the focusing electrodes and reduced clearance from the beamlets to the surrounding electrodes, thereby generating field aberrations and larger image forces. These aberrations can also lead to particle loss. We have studied a particular design of the proposed induction linac system experiment (ILSE) combiner which is a first-order achromat that tolerates a rather large fractional head-to-tail momentum tilt of -+ 10%. Using a 2D particle-in-cell code we have found that -7% of particles are lost in the combiner. The emittance growth after the combiner is large enough so that the emittance growth due to combiner aberrations is unimportant. The scaled projection to a driver shows the growth is small enough to be tolerated. At present, methods of improving combiner design to reduce particle loss and to minimize emittance growth are being studied.
Proceedings of the 1997 Particle Accelerator Conference (Cat. No.97CH36167), 2000
Transverse beam combining is a cost-saving option employed in many designs for induction linac heavy ion fusion drivers. The resultant transverse emittance increase, due predominantly to anharmonic space charge forces, must be kept minimal so that the beam remains focusable at the target. A prototype combining experiment has been built and preliminary results are presented. Four sources each produce up to 4.8 mA Cs + beams at 160 keV. Focusing upstream of the merge consists of four quadrupoles and a final combined-function element (quadrupole & dipole). All lattice elements of the prototype are electrostatic. Due to the small distance between beams near the merge (~ 3-4 mm), the electrodes here are a cage of small rods, each at different voltage.
Conference Record of the 1991 IEEE Particle Accelerator Conference
achieved in practice. These experiments, in which the current Current amplification of heavy ion beams is an integral was amplified from 4x10 mA to 4x90 mA and the energy feature of the induction linac approach to heavy ion fusion. As increased from 200 keV (the injection value) to 900 keV, were part of the Heavy Ion Fusion Accelerator Research program at accompanied by a growth in the normalised emittance by a LBL we have been studying the evolution of die transverse factor of approximately two. This work has been reported emittance of ion beams while they are undergoing current previously and a review can be found elsewhere in these amplification, achieved by longitudinal bunch compression and proceedings'. acceleration. Experiments are conducted on MBE-4, a four beam Cs + induction linac. The space-charge dominated beams 2. EXPERIMENTS of MBE-4 are focused by electrostatic quadrupoles while they are accelerated tram nominally 200 keV up to-1 MeV by 24 We have identified a number of mechanisms which may accelerating gaps. Initially the beams have currents of typically be responsible for emittance growth in MBE-4 including 4 mA to 10 mA per beam. Early experimental results showed matching errors, rapid longitudinal compression (leading to a a growth of the normalized emittance by a factor of 2 while die change in die space-charge electrostatic-field energy), and nonbeam current was amplified by up to 9 times its initial value, linear field effects (self-fields, image-fields, focus fields). The We will discuss me results of recent experiments in which a last of Uiese mechanisms is particularly troublesome for offmild bunch length compression rate, more typical of that axis beams where the edge of the beam may approach the nonrequired by a fusion driver, has shown that the normalized linear field region of the quadrupoles 2. For die experiments emittance can be maintained at its injection value (0.03 mm-discussed here offsets are minimised by the use of steering mr) during acceleration. elements at die entrance to the linac and by careful alignment of the accelerator. Proper matching of the beam phase-space to 1. INTRODUCTION the lattice of die linac is performed by adjustment of ^'matching section" consisting of eight electrostatic The induction Unac approach to heavy ion driven inertial quadrupoles just downstream of thediode. fusion envisages a design in which multiple beams are Recent experiments have involved the application of an employed at the law energy end of the driver with die beam acceleration schedule which results in a smaller increase in die current undergoing amplification as it is accelerated. Current beam line charge density between injection and full energy. In amplification results both from the increase in panicle velocity order to realise this we have reduced the extent of die applied and also from longitudinal bunch compression. This velocity tilt in the early pps of MBE-4 with the majority of compression is achieved by applying a velocity 'tilt' between die acceleration being provided by waveforms in which die die head and tail of the bunch, provided by tailored voltage voltage does not vary greatly during die passage of die beam waveforms applied at die accelerating gaps. MBE-4 is a four pulse. The reduction in bunch compression in these beam Cs* linac built to investigate longitudinal dynamics experiments means that the beam pulse length is not issues related to this concept. The linac is comprised of a 30 sufficiently short for the final accelerating waveforms to period, electrostatic, AG focusing lattice. Each doublet is completely straddle the beam pulse. Consequently die current followed by an accelerating gap with die exception of every waveforms observed in diese experiments are poorer dian those fifth doublet where the gap is reserved for diagnostic access and obtained in earlier studies, however me focus of these vacuum pumping. Each lattice period (l.p.) is 45.7 cm long experiments is transverse beam dynamics, resulting in a linac of 13.7 metres. Early experiments on MBE-4 concentrated on a In attempting to maintain a matched beam during demonstration of current amplification while maintaining acceleration we scale the strengths of die quadrupoie focusing control of die current profile and correcting for inevitable voltages, Vq, such as to keep diem proportional to die beam acceleration errors', which arose from the difference between lfae-charge density, X, i.e. V Q-\-1 / v, where I and v are ideal accelerating pulser waveforms and those waveforms Ae
2003
The U.S. Heavy Ion Fusion Virtual National Laboratory is proposing as its next experiment the Integrated Beam Experiment (IBX). All experiments in the U.S. Heavy Ion Fusion (HIF) program up to this time have been of modest scale and have studied the physics of selected parts of a heavy ion driver. The mission of the IBX, a proof-of-principle experiment, is
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2001
An overview of experiments is presented, in which the physical dimensions, emittance and perveance are scaled to explore driver-relevant beam dynamics. Among these are beam merging, focusing to a small spot, and bending and recirculating beams. The Virtual National Laboratory for Heavy Ion Fusion (VNL) is also developing two driver-scale beam experiments involving heavy-ion beams with I(sub beam) ~; 1 Ampere to provide guidance for the design of an Integrated Research Experiment (IRE) for driver system studies within the next 5 years. Multiple-beam sources and injectors are being designed and a one-beam module will be built and tested. Another experimental effort will be the transport of such a beam through ~;100 magnetic quadrupoles. The experiment will determine transport limits at high aperture fill factors, beam halo formation, and the influence on beam properties of secondary electron Research into driver technology will be briefly presented, including the development of ferromagnetic core materials, induction core pulsers, multiple-beam quadrupole arrays and plasma channel formation experiments for pinched transport in reactor chambers.
2005
Significant experimental and theoretical progress has been made in the US heavy-ion fusion program on high-current sources, injectors, transport, final focusing, chambers and targets for high-energy density physics (HEDP) and inertial fusion energy (IFE) driven by induction linac accelerators. One focus of present research is the beam physics associated with quadrupole focusing of intense, space-charge dominated heavy-ion beams, including gas and electron cloud effects at high currents, and the study of long-distance-propagation effects such as emittance growth due to field errors in scaled experiments. A second area of emphasis in present research is the introduction of background plasma to neutralize the space charge of intense heavy-ion beams and assist in focusing the beams to a small spot size. In the near future, research will continue in the above areas, and a new area of emphasis will be to explore the physics of neutralized beam compression and focusing to high intensities required to heat targets to high-energy density conditions as well as for inertial fusion energy. r
1998
Transverse beam combining is a cost-saving option em- ployed in many designs for heavy-ion inertial fusion en- ergy 1 drivers. A major area of interest, both theoretically and experimentally, is the resultant transverse phase space dilution during the beam merging process. Currently, a pro- totype combining experiment is underway at LBNL and we have employed a variety of numerical descriptions
Nuclear Fusion
Significant experimental and theoretical progress has been made in the U.S. heavy ion fusion program on high-current sources, injectors, transport, final focusing, chambers and targets for high energy density physics (HEDP) and inertial fusion energy (IFE) driven by induction linac accelerators. One focus of present research is the beam physics associated with quadrupole focusing of intense, space-charge dominated heavy-ion beams, including gas and electron cloud effects at high currents, and the study of long-distance-propagation effects such as emittance growth due to field errors in scaled experiments. A second area of emphasis in present research is the introduction of background plasma to neutralize the space charge of intense heavy ion beams and assist in focusing the beams to a small spot size. In the near future, research will continue in the above areas, and a new area of emphasis will be to explore the physics of neutralized beam compression and focusing to high intensities required to heat targets to high energy density conditions as well as for inertial fusion energy.
Laser and Particle Beams, 2003
We describe the next set of experiments proposed in the U.S. Heavy Ion Fusion Virtual National Laboratory, the so-called Integrated Beam Experiment~IBX!. The purpose of IBX is to investigate in an integrated manner the processes and manipulations necessary for a heavy ion fusion induction accelerator. The IBX experiment will demonstrate injection, acceleration, compression, bending, and final focus of a heavy ion beam at significant line charge density. Preliminary conceptual designs are presented and issues and trade-offs are discussed. Plans are also described for the step after IBX, the Integrated Research Experiment~IRE!, which will carry out significant target experiments.
2009
The Heavy-Ion Fusion Sciences Virtual National Laboratory is pursuing an approach to target heating experiments in the Warm Dense Matter regime, using space-charge-dominated ion beams that are simultaneously longitudinally bunched and transversely focused. Longitudinal beam compression by large factors has been demonstrated in the LBNL Neutralized Drift Compression Experiment (NDCX) experiment with controlled ramps and forced neutralization. The achieved peak beam current and energy can be used in experiments to heat targets and create warm dense matter. Using an injected 30 mA K + ion beam with initial kinetic energy 0.3 MeV, axial compression leading to !50x current amplification and simultaneous radial focusing to beam radii of a few mm have led to encouraging energy deposition approaching the intensities required for eVrange target heating experiments. We discuss experiments that are under development to reach the necessary higher beam intensities and the associated beam diagnostics.
2004
Significant experimental and theoretical progress has been made in the U.S. heavy ion fusion program on high-current sources, injectors, transport, final focusing, chambers and targets for high energy density physics (HEDP) and inertial fusion energy (IFE) driven by induction linac accelerators. One focus of present research is the beam physics associated with quadrupole focusing of intense, space-charge dominated heavy-ion beams, including gas and electron cloud effects at high currents, and the study of long-distance-propagation effects such as emittance growth due to field errors in scaled experiments. A second area of emphasis in present research is the introduction of background plasma to neutralize the space charge of intense heavy ion beams and assist in focusing the beams to a small spot size. In the near future, research will continue in the above areas, and a new area of emphasis will be to explore the physics of neutralized beam compression and focusing to high intensitie...
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1998
The approach to heavy-ion-driven inertial fusion studied most extensively in the US uses induction modulators and cores to accelerate and confine the beam longitudinally. The intrinsic peak-current capabilities of induction machines, together with their flexible pulse formats, provide a suitable match to the high peak-power requirement of a heavy-ion fusion target. However, as in the RF case, where combinations of linacs, synchrotrons, and storage rings offer a number of choices to be examined in designing an optimal system, the induction approach also allows a number of architectures, from which choices must be made.
The Review of Laser Engineering, 1977
A review of Sandia Laboratories' program to investigate the feasibility of achieving inertial confinement fusion using pulsed power technology to produce focused electron and ion beams is presented. Recent results are discussed, including beam focusing, target interaction studies, and accelerator development.
Physics of Plasmas, 2003
The U.S. Heavy Ion Fusion program has recently commissioned several new experiments. In the High Current Experiment ͓P. A. Seidl et al., Laser Part. Beams 20, 435 ͑2003͔͒, a single low-energy beam with driver-scale charge-per-unit-length and space-charge potential is being used to study the limits to transportable current posed by nonlinear fields and secondary atoms, ions, and electrons. The Neutralized Transport Experiment similarly employs a low-energy beam with driver-scale perveance to study final focus of high perveance beams and neutralization for transport in the target chamber. Other scaled experiments-the University of Maryland Electron Ring ͓P. G. O'Shea et al., accepted for publication in Laser Part. Beams͔ and the Paul Trap Simulator Experiment ͓R. C. Davidson, H. Qin, and G. Shvets, Phys. Plasmas 7, 1020 ͑2000͔͒-will provide fundamental physics results on processes with longer scale lengths. An experiment to test a new injector concept is also in the design stage. This paper will describe the goals and status of these experiments, as well as progress in theory and simulation. A proposed future proof-of-principle experiment, the Integrated Beam Experiment, will also be described.
Proceedings of International Conference on Particle Accelerators
Longitudinal space-charge waves develop on a heavyion inertial-fusion pulse from initial mismatches or from inappropriately timed or shaped accelerating voltages. Without correction, waves moving backward along the beamcan grow due to the interaction with their resistively retarded image fields, eventually degrading the longitudinal emittance. A simple correction algorithm is presented here that uses a time-dependent axial electric field to reverse the direction of backward-moving waves. The image fields then damp these forward-moving waves. The method is demonstrated by fluid simulations of an idealized inertialfusion driver, and practical problems in implementing the algorithm are discussed.
Particle Accelerator, IEEE Conference, 2001
The High Current Experiment (HCX) is being built to explore heavy-ion beam transport at a scale appropriate to the low-energy end of a driver for fusion energy production. The primary mission of this experiment is to investigate aperture fill factors acceptable for the transport of space-charge dominated heavy-ion beams at high space-charge intensity (line-charge density ~0.2 μC/m) over long pulse durations (3-10 μsec). A single beam transport channel will be used to evaluate scientific and technological issues resulting from the transport of an intense beam subject to applied field nonlinearities, envelope mismatch, misalignment-induced centroid excursions, imperfect vacuum, halo, background gas and electron effects resulting from lost beam ions. Emphasis will be on the influence of these effects on beam control and limiting degradations in beam quality (emittance growth). Electrostatic (Phase I) and magnetic (Phase II) quadrupole focusing lattices have been designed and future phases of the experiment may involve acceleration and/or pulse compression. The Phase I lattice is presently under construction and simulations to better predict machine performance are being carried out. Here we overview: the scientific objectives of the overall project, processes that will be explored, and transport lattices developed
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2001
For heavy ion fusion (HIF) induction linac drivers, a typical injector requires total beam current of 50-100 A and is comprised of many individual beams of 0.5-1.0 A each. As a step towards developing a full ion driver for inertial fusion energy (IFE) power plants, an Integrated Research Experiment (IRE) will be proposed within a few years . The IRE will have a linac of more than 150 MeV and beam current about 18 A (ion mass 39). At present, a compact multiple-beam injector is being developed to meet the IRE specifications. In our design, about 100 miniature beamlets (of a few mA each) will be merged to form each 0.5 A beam at the matching section. The beamlets have current density up to 100 mA/cm2 at the ion source (as opposed to 3.5 mA/cm2 used in previous low current density large beam designs). With optimized positioning and aiming, the miniature beamlets can quickly merge and match into an ESQ channel thus minimizing the matching section size requirement. Simulation results have shown that when the beamlet current is small and the number of beamlets are large, the emittance of a 1.6 MeV, 0.5 A beam (after merging) at the end of the injector is 1.0 π mm-mrad.
2002
Significant experimental and theoretical progress in the U.S heavy-ion fusion (HIF) program is reported in modeling and measurements of intense space-charge-dominated heavy ion and electron beams. Measurements of the transport of a well-matched and aligned high current (0.2A) 1.0 MeV potassium ion beam through 10 electric quadrupoles, with a fill factor of 60%, shows no emittance growth within experimental measurement uncertainty, as expected from the simulations. Another experiment shows that passing a beam through an aperture can reduce emittance to near the theoretical limits, and that plasma neutralization of the beam's space-charge can greatly reduce the focal spot radius. Measurements of intense beamlet current density, emittance, charge-state purity, and energy spread from a new, high-brightness, Argon plasma source for HIF experiments are described. New theory and simulations of neutralization of intense beam space charge with plasma in various focusing chamber configurations indicate that near-emittance-limited beam focal spot sizes can be obtained even with beam perveance an order of magnitude higher than in earlier HIF focusing experiments.
Proceedings of International Conference on Particle Accelerators, 1993
The longitudinal wall impedance instability is of potential importance for a heavy ion fusion (HIF) driver because complete stabilization of this mode via momentum spread is impractical due to the requirement of focusing the beam ont,u thp inertial confinement fusion target. This instability is being studied with the WARPrz particle-in-cell code. The impedance of the induction linac modules is modeled as a wall impedance corresponding to a continuum of resist,ors and capacitors in parallel. We discuss simulations of the this instability, including reflection of perturbations off the beam end, the effect of finite temperature on the growth rate, and errors in intermittently-applied axial confining fields as a seed for this instability. We also present very long simulations in which we study the approach to ~quilibriurn.
Il Nuovo Cimento A, 1993
A two-year study of recirculating induction heavy ion accelerators as low-cost driver for inertial-fusion energy applications was recently completed. The projected cost of a 4 MJ accelerator was estimated to be about $500 M (million) and the efficiency was estimated to be 35%. The principal technology issues include energy recovery of the ramped dipole magnets, which is achieved through use of ringing inductive/capacitive circuits, and high repetition rates of the induction cell pulsers, which is accomplished through arrays of field effect transistor (FET) switches. Principal physics issues identified include minimization of particle loss from interactions with the background gas, and more demanding emittance growth and centroid control requirements associated with the propagation of space-charge-dominated beams around bends and over large path lengths. In addition, instabilities such as the longitudinal resistive instability, beam-breakup instability and betatron-orbit instability were found to be controllable with careful design.
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