Abstract

Ion beams (including protons) with low emittance and high space-charge intensity can be propagated with normal incidence through a sequence of thin metallic foils separated by vacuum gaps of order the characteristic transverse beam extent to transport/collimate the beam or to focus it to a small transverse spot. Energetic ions have sufficient range to pass through a significant number of thin foils with little energy loss or scattering. The foils reduce the (defocusing) radial electric self-field of the beam while not altering the (focusing) azimuthal magnetic self-field of the beam, thereby allowing passive self-beam focusing if the magnetic field is sufficiently strong relative to the residual electric field. Here we present an envelope model developed to predict the strength of this passive (beam generated) focusing effect under a number of simplifying assumptions including relatively long pulse duration. The envelope model provides a simple criterion for the necessary foil spacing for net focusing and clearly illustrates system focusing properties for either beam collimation (such as injecting a laser-produced proton beam into an accelerator) or for magnetic pinch focusing to a small transverse spot (for beam driven heating of materials). An illustrative example is worked for an idealization of a recently performed laser-produced proton-beam experiment to provide guidance on possible beam focusing and collimation systems. It is found that foils spaced on the order of the characteristic transverse beam size desired can be employed and that envelope divergence of the initial beam entering the foil lens must be suppressed to limit the total number of foils required to practical values for pinch focusing. Relatively modest proton-beam current at 10 MeV kinetic energy can clearly demonstrate strong magnetic pinch focusing achieving a transverse rms extent similar to the foil spacing ($20--50\text{ }\text{ }\ensuremath{\mu}\mathrm{m}$ gaps) in beam propagation distances of tens of mm. This is a surprisingly optimistic result since placing many foils per characteristic beam radius, which one might expect to be necessary to strongly attenuate the self-electric field, would likely result in excessive scattering and loss of focusing from the current neutralization due to the beam propagating too far through solid metal. Results from the envelope model are compared with particle-in-cell simulations to help clarify limits related to envelope-model idealizations. Possible degradations of focusing in situations where strong halo can be generated and where pulse duration is short are clarified.

Highlights

  • Focusing of space-charge dominated proton and ion beams is required in various applications, including intense beam injectors derived from short pulse laser-illuminated foils via target normal sheath acceleration (TNSA), radiography, generation of beam-heated warm dense matter, proton and ion-based fast ignition concepts, and medical therapies [1,2,3,4,5,6]

  • We provide estimates based on an idealized TNSA protonbeam experiment analyzed in later sections with $400 A of protons in a 4 ps pulse window about 10 MeV and a broad energy spectrum and $50 m spaced Al foils that are $0:5 m thick [10]

  • The boundary conditions on the electric field are conducting at the ends and the radial edge of the grid, and for the magnetic field, periodic at the ends and ‘‘conducting’’ at the radial edge. We refer to these simulations as ‘‘infinite beam.’’ For infinite-beam simulations, we calculate the rms-transverse beam extent hx2i1?=2 averaged over the full axial domain in z

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Summary

Introduction

Focusing of space-charge dominated proton and ion beams is required in various applications, including intense beam injectors derived from short pulse laser-illuminated foils via target normal sheath acceleration (TNSA), radiography, generation of beam-heated warm dense matter, proton and ion-based fast ignition concepts, and medical therapies [1,2,3,4,5,6]. Comoving electrons which must be stripped while focusing is provided if the beam is injected into a conventional beam transport lattice for further acceleration and phase-space manipulations. Such ‘‘collimation’’ procedures should be simple and compact to enable future TNSA injectors for a wide range of applications. These classes of focusing and collimation applications are a substantial challenge due to strong space-charge forces in the intense beams. Such applied-focusing based systems have critical disadvantages including high beam losses due to chromatic aberrations; often, small focal spot radii (& 50 m) are desired, requiring large and expensive magnet systems

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