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000465228 088__ $$2arXiv$$aarXiv:2012.10680
000465228 1001_ $$0K.Sjoebaek.1$$aSjobak, K. N.$$b0$$eCorresponding author
000465228 245__ $$aStrong focusing gradient in a linear active plasma lens
000465228 260__ $$aCollege Park, MD$$bAmerican Physical Society$$c2021
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000465228 500__ $$aarXiv title: Multi-kT/m Focusing Gradient in a Linear Active Plasma Lens8 pages, 6 figures. Submitted to Physical Review Applied
000465228 520__ $$aActive plasma lenses are compact devices developed as a promising beam-focusing alternative for charged particle beams, capable of short focal lengths for high-energy beams. We have previously shown that linear magnetic fields with gradients of around 0.3 kT/m can be achieved in argon-filled plasma lenses that preserve beam emittance [C.A. Lindstrøm et al., Phys. Rev. Lett. 121, 194801 (2018)]. Here we show that with argon in a 500 μm diameter capillary, the fields are still linear with a focusing gradient of 3.6 kT/m, which is an order of magnitude higher than the gradients of quadrupole magnets. The current pulses that generate the magnetic field are provided by compact Marx banks, and are highly repeatable. The demonstrated operation with simultaneously high-gradient, linear fields and good repeatability establish active plasma lenses as an ideal device for pulsed particle beam applications requiring very high focusing gradients that are uniform throughout the lens aperture.
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000465228 536__ $$0G:(DE-HGF)2015_IFV-VH-VI-503$$aVH-VI-503 - Plasma wakefield acceleration of highly relativistic electrons with FLASH (2015_IFV-VH-VI-503)$$c2015_IFV-VH-VI-503$$x1
000465228 536__ $$0G:(DE-HGF)2018_ZT-0009$$aZT-0009 - Plasma Accelerators (2018_ZT-0009)$$c2018_ZT-0009$$x2
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000465228 650_7 $$2INSPIRE$$acharged particle: beam
000465228 650_7 $$2INSPIRE$$abeam: width
000465228 650_7 $$2INSPIRE$$amagnetic field: gradient
000465228 650_7 $$2INSPIRE$$abeam emittance
000465228 650_7 $$2INSPIRE$$abeam focusing
000465228 650_7 $$2INSPIRE$$abeam: pulsed
000465228 650_7 $$2INSPIRE$$aargon
000465228 650_7 $$2INSPIRE$$aaccelerator: plasma
000465228 650_7 $$2INSPIRE$$acurrent: time dependence
000465228 693__ $$0EXP:(DE-MLZ)External-20140101$$5EXP:(DE-MLZ)External-20140101$$eMeasurement at external facility$$x0
000465228 7001_ $$0E.Adli.1$$aAdli, E.$$b1
000465228 7001_ $$0R.Corsini.1$$aCorsini, R.$$b2
000465228 7001_ $$0W.Farabolini.1$$aFarabolini, W.$$b3
000465228 7001_ $$0P:(DE-H253)PIP1083196$$aBoyle, Gregory James$$b4$$udesy
000465228 7001_ $$0P:(DE-H253)PIP1086874$$aLindstroem, Carl Andreas$$b5$$udesy
000465228 7001_ $$0P:(DE-H253)PIP1027730$$aMeisel, Martin$$b6$$udesy
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000465228 7001_ $$0P:(DE-H253)PIP1016832$$aRöckemann, Jan-Hendrik$$b8
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000465228 7001_ $$0A.E.Dyson.1$$aDyson, A. E.$$b10
000465228 773__ $$0PERI:(DE-600)2844143-6$$a10.1103/PhysRevAccelBeams.24.121306$$gVol. 24, no. 12, p. 121306$$n12$$p121306$$tPhysical review accelerators and beams$$v24$$x1098-4402$$y2021
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