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Title: Collisionless shock acceleration of narrow energy spread ion beams from mixed species plasmas using 1 μ m lasers

Authors:
; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ;
Publication Date:
Research Org.:
SLAC National Accelerator Lab., Menlo Park, CA (United States); Univ. of California, Los Angeles, CA (United States)
Sponsoring Org.:
USDOE Office of Science (SC), Fusion Energy Sciences (FES) (SC-24); USDOE National Nuclear Security Administration (NNSA)
OSTI Identifier:
1479144
Alternate Identifier(s):
OSTI ID: 1490380; OSTI ID: 1525470
Grant/Contract Number:  
AC52-07NA27344; AC02-76SF00515; SC0010064; NA0001944; 15-LW-095; FWP 100237; FWP 100182; FWP 100331; SCW1575-1; NA0002950; NA0003873; 1734315; RGPIN-2014-05736
Resource Type:
Published Article
Journal Name:
Physical Review Accelerators and Beams
Additional Journal Information:
Journal Name: Physical Review Accelerators and Beams Journal Volume: 21 Journal Issue: 10; Journal ID: ISSN 2469-9888
Publisher:
American Physical Society
Country of Publication:
United States
Language:
English
Subject:
43 PARTICLE ACCELERATORS

Citation Formats

Pak, A., Kerr, S., Lemos, N., Link, A., Patel, P., Albert, F., Divol, L., Pollock, B. B., Haberberger, D., Froula, D., Gauthier, M., Glenzer, S. H., Longman, A., Manzoor, L., Fedosejevs, R., Tochitsky, S., Joshi, C., and Fiuza, F. Collisionless shock acceleration of narrow energy spread ion beams from mixed species plasmas using 1     μ m lasers. United States: N. p., 2018. Web. doi:10.1103/PhysRevAccelBeams.21.103401.
Pak, A., Kerr, S., Lemos, N., Link, A., Patel, P., Albert, F., Divol, L., Pollock, B. B., Haberberger, D., Froula, D., Gauthier, M., Glenzer, S. H., Longman, A., Manzoor, L., Fedosejevs, R., Tochitsky, S., Joshi, C., & Fiuza, F. Collisionless shock acceleration of narrow energy spread ion beams from mixed species plasmas using 1     μ m lasers. United States. doi:10.1103/PhysRevAccelBeams.21.103401.
Pak, A., Kerr, S., Lemos, N., Link, A., Patel, P., Albert, F., Divol, L., Pollock, B. B., Haberberger, D., Froula, D., Gauthier, M., Glenzer, S. H., Longman, A., Manzoor, L., Fedosejevs, R., Tochitsky, S., Joshi, C., and Fiuza, F. Thu . "Collisionless shock acceleration of narrow energy spread ion beams from mixed species plasmas using 1     μ m lasers". United States. doi:10.1103/PhysRevAccelBeams.21.103401.
@article{osti_1479144,
title = {Collisionless shock acceleration of narrow energy spread ion beams from mixed species plasmas using 1     μ m lasers},
author = {Pak, A. and Kerr, S. and Lemos, N. and Link, A. and Patel, P. and Albert, F. and Divol, L. and Pollock, B. B. and Haberberger, D. and Froula, D. and Gauthier, M. and Glenzer, S. H. and Longman, A. and Manzoor, L. and Fedosejevs, R. and Tochitsky, S. and Joshi, C. and Fiuza, F.},
abstractNote = {},
doi = {10.1103/PhysRevAccelBeams.21.103401},
journal = {Physical Review Accelerators and Beams},
number = 10,
volume = 21,
place = {United States},
year = {2018},
month = {10}
}

Journal Article:
Free Publicly Available Full Text
Publisher's Version of Record
DOI: 10.1103/PhysRevAccelBeams.21.103401

Citation Metrics:
Cited by: 9 works
Citation information provided by
Web of Science

Figures / Tables:

FIG. 1 FIG. 1: (Color online) a)Experimental setup. A near-critical density target is created by first irradiating a Mylar foil with an ablation laser. After the target has expanded for a time $\tau$ , a high-intensity ps duration laser pulse is focused onto the target to produce the electrostatic shock wave. Acceleratedmore » ions are measured by the imaging magnetic spectrometer (IMS) and Thomson parabola (TP). TP measurements indicate the majority of accelerated ions are C6+/O8+. Accelerated electrons are measured by a permanent magnet electron spectrometer. Radiochromic film (RCF) was used to measure a portion of the spatial beam profile. Orthogonal to the target, a probe laser was used to measure the target expansion. Accelerated proton spectra shown for b) an unablated foil, and c-e) at different time delays from consecutive shots. The inferred peak ne of the target and laser a0 are also denoted. Only signal > 4× the background variation is shown.« less

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