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J. Santucci

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7 papers
title: RESULTS FROM THE UCLA/FNPL UNDERDENSE PLASMA LENS EXPERIMENT
format: conference procceeding
conference: Erice 2005
year: 2006
11 authors: M. C. Thompson | H. Badakov | J. B. Rosenzweig | G. Travish | H. Edwards | R. Fliller | G. M. Kazakevich | P. Piot | J. Santucci | J. Li | R. Tikhoplav
abstract: A gaussian underdense plasma lens with peak density 5 x 1012 cm−3 and a full width half maximum (FWHM) length of 2.2 cm has been used to focus a relativistic electron beam. This plasma lens is equivalent in strength to a quadrupole magnet with a 150 T/m field gradient. The lens focused a 15 MeV, 16 nC electron beam with initial dimensions σx,y ≈ 650 μm and σz ≈ 6.5 mm onto an optical transition radiation (OTR) screen ∼2 cm downstream of the lens. The average transverse area of the plasma focused electron beam was typically demagnified by a factor of 23. The evolution of the beam envelope in the area near the beam waist was measured for both round beams and asymmetric beams with x:y aspect ratios as large as 1:5. The light from the OTR screen in the round beam case was also imaged into a streak camera in order to directly measure the correlation between z and σ within the beam.
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title: Status of the UCLA/NICADD Plasma Density Transition Trapping Experiment
format: preprint
year: 2004
8 authors: M.C. Thompson | J. B. Rosenzweig | G. Travish | N. Barov | H. Edwards | P. Piot | J. Santucci | R. Tikhoplav
abstract: Plasma density transition trapping is a recently proposed self-injection scheme for plasma wake-field accelerators. This technique uses a sharp downward plasma density transition to trap and accelerate background plasma electrons in a plasma wake-field. This paper recounts the first attempt to demonstrate density transition trapping experimentally. The goal of the experiment is to capture a ∼ 100 pC, 1.5 MeV beam with 4% rms energy spread out of a 2.5x10^13 cm^−3 peak density plasma using a 6nC, 14 MeV drive beam. The first experimental run occurred at the Fermilab NICADD Photoinjector Laboratory (FNPL) between January and May 2004. While several key objectives were achieved, we were unable to achieve the drive beam parameters necessary for the experiment due to technical problems. We are in the process of resolving these problems in preparation for a second experimental run.
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title: Plasma Wakefield Experiments
format: conference procceeding
conference: 10th Advanced Accelerator Concepts Workshop
year: 2002
6 authors: N. Barov | M.C. Thompson | Bishofberger, K. | J. B. Rosenzweig | H. Edwards | Santucci, J.
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title: Ultra high-gradient energy loss by a pulsed electron beam in a plasma
format: conference procceeding
conference: 2001 Particle Accelerator Conference
year: 2001
9 authors: N. Barov | Bishofberger, K. | J. B. Rosenzweig | Carneiro, J. P. | P. Colestock | H. Edwards | Fitch, M. J. | W. Hartung | Santucci, J.
abstract: The plasma wake-field mechanism can be used to couple energy at a high rate from a bunched electron beam into a plasma wave. We will present results from the Fermilab A0 facility where a beam with an initial energy of 14 MeV passes through the plasma to emerge with a much broader energy spread, spanning from a low of 3 MeV to a high of over 20 MeV. Over the 8 cm length of the 10(14) cm(-3) plasma, this implies a 140 MeV/m deceleration and 72 MeV/m acceleration gradient. (12 References).
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title: OBSERVATIONS OF UNDERDENSE PLASMA LENS FOCUSING OF
format: journal article
year: 2007
10 authors: M.C. Thompson | H. Badakov | J.B. Rosenzweig | G. Travish | R. Fliller | G. M. Kazakevich | P. Piot | J. Santucci | J. Li | R. Tikhoplav
abstract: Focusing of a 15 MeV, 19 nC electron bunch by an un- derdense plasma lens operated just beyond the threshold of the underdense condition has been demonstrated in ex- periments at the Fermilab NICADD Photoinjector Labora- tory (FNPL). The strong 1.9 cm focal-length plasma-lens focused both transverse directions simultaneously and re- duced the minimum area of the beam spot by a factor of 23. Analysis of the beam-envelope evolution observed near the beam waist shows that the spherical aberrations of this un- derdense lens are lower than those of an overdense plasma lens, as predicted by theory. Correlations between the beam charge and the properties of the beam focus corroborate this conclusion.
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title: Observations of Underdense Plasma Lens Focusing of Relativistic Electron Beams
format: conference procceeding
conference: PAC07
year: 2007
10 authors: M.C. Thompson | H. Badakov | J.R. Rosenzweig | G. Travish | R. Fliller | G.M. Kazakevich | P. Piot | J. Santucci | J. Li | R. Tikhoplav
abstract: Focusing of a 15 MeV, 19 nC electron bunch by an un- derdense plasma lens operated just beyond the threshold of the underdense condition has been demonstrated in ex- periments at the Fermilab NICADD Photoinjector Labora- tory (FNPL). The strong 1.9 cm focal-length plasma-lens focused both transverse directions simultaneously and re- duced the minimum area of the beam spot by a factor of 23. Analysis of the beam-envelope evolution observed near the beam waist shows that the spherical aberrations of this un- derdense lens are lower than those of an overdense plasma lens, as predicted by theory. Correlations between the beam charge and the properties of the beam focus corroborate this conclusion.
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title: The UCLA/FNPL Time Resolved Underdense Plasma Lens Experiment
format: journal article
year: 2005
11 authors: M.C. Thompsont | H. Badakov | J.B. Rosenzweig | G. Travish | H. Edwards | R. Fliller | G. M. Kazakevich | P. Piot | J. Santucci | J. Li | R. Tikhoplav
abstract: A gaussian underdense plasma lens with peak density 5 × 1012cm-3and a full width half maximum (FWHM) length of 2.2 cm has been used to focus a relativistic electron beam. This plasma lens has a focusing strength equivalent to a quadrupole magnet with a 150 T/m field gradient. The lens focused a 15 MeV, 16 nC electron beam with initial dimensions σr= 500 μm and σz= 5 mm onto an optical transition radiation (OTR) screen 2 cm downstream of the lens. The average transverse area of the plasma focused electron beam was typically demagnified by a factor of 22. The light from the OTR screen was imaged into a streak camera in order to directly measure the correlation between z and σrwithin the beam.
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