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Dive into the research topics where J. Santucci is active.

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Featured researches published by J. Santucci.


Physical Review Special Topics-accelerators and Beams | 2011

Ugrades of beam diagnostics in support of emittance-exchange experiments at the Fermilab A0 photoinjector

Alex H. Lumpkin; A. S. Johnson; J. Ruan; J. Santucci; Y.-E. Sun; R. Thurman-Keup; H. Edwards

The possibility of using electron beam phase space manipulations to support a free-electron laser accelerator design optimization has motivated our research. An ongoing program demonstrating the exchange of transverse horizontal and longitudinal emittances at the Fermilab A0 photoinjector has benefited recently from the upgrade of several of the key diagnostics stations. Accurate measurements of these properties upstream and downstream of the exchanger beamline are needed. Improvements in the screen resolution term and reduced impact of the optical systems depth-of-focus by using YAG:Ce single crystals normal to the beam direction will be described. The requirement to measure small energy spreads (<10 keV) in the spectrometer and the exchange process which resulted in bunch lengths less than 500 fs led to other diagnostics performance adjustments and upgrades as well. A longitudinal to transverse exchange example is also reported.


bipolar/bicmos circuits and technology meeting | 2003

Angular momentum measurement of the FNPL electron beam

Y.-E. Sun; K.-J. Kim; Ph Piot; K. Desler; D. Edwards; H. Edwards; M. Huening; J. Santucci; N. Barov; D. Mihalcea; R. Tikhoplav; Steven M. Lidia; S.-H. Wang

In the flat beam experiment at Fermilab/NICADD Photoinjector Laboratory(FNPL), it is essential to have a nonvanishing longitudinal magnetic field on the photocathode. The canonical angular momentum of the electron beam generated by this magnetic field is an important parameter in understanding the round to flat beam transformation. In this paper, we report our measurements of the canonical angular momentum, which is directly related to the skew diagonal elements of the beam matrix before beam is made flat. The measurements of the other elements of the beam matrix are also reported.


Physics of Plasmas | 2016

Longitudinal bunch shaping of picosecond high-charge MeV electron beams

B. Beaudoin; J.C.T. Thangaraj; Dean Edstrom; J. Ruan; A. H. Lumpkin; Daniel Broemmelsiek; K. A. Carlson; Darren Crawford; Alexander Romanov; J. Santucci; G. Stancari; R. Thurman-Keup; A. Warner

With ever increasing demands for intensities in modern accelerators, the understanding of space-charge effects becomes crucial. Herein are presented measurements of optically shaped picosecond-long electron beams in a superconducting L-band linac over a wide range of charges, from 0.2 nC to 3.4 nC. At low charges, the shape of the electron beam is preserved, while at higher charge densities, modulations on the beam convert to energy modulations. Energy profile measurements using a spectrometer and time profile measurements using a streak camera reveal the dynamics of longitudinal space-charge on MeV-scale electron beams.


Physics of Plasmas | 2010

Observations of low-aberration plasma lens focusing of relativistic electron beams at the underdense threshold

M.C. Thompson; H. Badakov; J. B. Rosenzweig; G. Travish; N. Barov; P. Piot; R. Fliller; G. M. Kazakevich; J. Santucci; J. Li; R. Tikhoplav

Focusing of a 15 MeV electron bunch by a plasma lens operated at the threshold of the underdense regime has been demonstrated. The strong, 1.7 cm focal length, plasma lens focused both transverse directions simultaneously and reduced the minimum area of the beam spot by a factor of 23. It is shown through analytic analysis and simulation that the observed spherical aberration of this underdense lens, when expressed as the fractional departure of the focusing strength from its linear expectation, is ΔK/K=0.08±0.04. This is significantly lower than the minimum theoretical value for the spherical aberration of an overdense plasma lens. Parameter scans showing the dependence of focusing performance on beam charge, as well as time resolved measurements of the focused electron bunch, are reported.


Archive | 2018

Commissioning and Operation of FAST Electron Linac at Fermilab

Alexander Romanov; Nathan B. Eddy; Curtis Baffes; Kermit Carlson; Darren Crawford; Alexander Valishev; G. Stancari; Michael Kucera; A. Warner; Elvin Harms; J. Ruan; R. Thurman-Keup; Vladimir Shiltsev; Jerry Leibfritz; J. Santucci; Igor Rakhno; Daniel Broemmelsiek; Dean Edstrom; Joseph Hurd; John Reid

We report results of the beam commissioning and first operation of the 1.3 GHz superconducting RF electron linear accelerator at Fermilab Accelerator Science and Technology (FAST) facility. Construction of the linac was completed and the machine was commissioned with beam in 2017. The maximum total beam energy of about 300 MeV was achieved with the record energy gain of 250 MeV in the ILC-type SRF cryomodule. The photoinjector was tuned to produce trains of 200 pC bunches with a frequency of 3 MHz at a repetition rate of 1 Hz. This report describes the aspects of machine commissioning such as tuning of the SRF cryomodule and beam optics optimization. We also present highlights of an experimental program carried out parasitically during the two-month run, including studies of wake-fields, and advanced beam phase space manipulation.


Archive | 2017

Notes on the design of experiments and beam diagnostics with synchrotron light detected by a gated photomultiplier for the Fermilab superconducting electron linac and for the Integrable Optics Test Accelerator (IOTA)

G. Stancari; Aleksandr Romanov; J. Ruan; J. Santucci; R. Thurman-Keup; Alexander Valishev

We outline the design of beam experiments for the electron linac at the Fermilab Accelerator Science and Technology (FAST) facility and for the Integrable Optics Test Accelerator (IOTA), based on synchrotron light emitted by the electrons in bend dipoles, detected with gated microchannel-plate photomultipliers (MCP-PMTs). The system can be used both for beam diagnostics (e.g., beam intensity with full dynamic range, turn-by-turn beam vibrations, etc.) and for scientific experiments, such as the direct observation of the time structure of the radiation emitted by single electrons in a storage ring. The similarity between photon pulses and spectrum at the downstream end of the electron linac and in the IOTA ring allows one to test the apparatus during commissioning of the linac.


arXiv: Accelerator Physics | 2016

Microlens Array Laser Transverse Shaping Technique for Photoemission Electron Source

A. Halavanau; Gwanghui Ha; J. Santucci; J. G. Power; Eric Wisniewski; Dean Edstrom; G. Qiang; P. Piot; J. Ruan; W. Gai

A common issue encountered in photoemission electron sources used in electron accelerators is distortion of the laser spot due to non ideal conditions at all stages of the amplification. Such a laser spot at the cathode may produce asymmetric charged beams that will result in degradation of the beam quality due to space charge at early stages of acceleration and fail to optimally utilize the cathode surface. In this note we study the possibility of using microlens arrays to dramatically improve the transverse uniformity of the drive laser pulse on UV photocathodes at both Fermilab Accelerator Science \& Technology (FAST) facility and Argonne Wakefield Accelerator (AWA). In particular, we discuss the experimental characterization of the homogeneity and periodic patterned formation at the photocathode. Finally, we compare the experimental results with the paraxial analysis, ray tracing and wavefront propagation software.


International Journal of Modern Physics A | 2007

RESULTS FROM THE UCLA/FNPL UNDERDENSE PLASMA LENS EXPERIMENT

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

A gaussian underdense plasma lens with peak density 5 x 10{sup 12} cm{sup -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 {sigma}{sub x,y} {approx} 650 {micro}m and {sigma}{sub z} {approx} 6.5 mm onto an optical transition radiation (OTR) screen {approx}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 {sigma}{sub r} within the beam.


Journal Name: AIP Conf.Proc.877:561-567,2006; Conference: Prepared for 12th Advanced Accelerator Concepts Workshop (AAC 2006), Lake Geneva, Wisconsin, 10-15 Jul 2006 | 2006

UCLA/FNPL Underdense Plasma Lens Experiment: Results and Analysis

M. C. Thompson; H. Badakov; J. B. Rosenzweig; G. Travish; R. Fliller; G. M. Kazakevich; P. Piot; J. Santucci; J. Li; R. Tikhoplav

Focusing of a 15 MeV, 16 nC electron bunch by a gaussian underdense plasma lens operated just beyond the threshold of the underdense condition has been demonstrated. The strong 1.9 cm focal length plasma lens focused both transverse directions simultaneously and reduced 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 underdense lens are lower than those of an overdense plasma lens, as predicted by theory. Time resolved measurements of the focused electron bunch are also reported and compared to simulations.


international conference on plasma science | 2005

The UCLA/FNPL Underdense Plasma Lens Experiment

M.C. Thompson; J. B. Rosenzweig; G. Travish; H. Edwards; G. M. Kazakevich; P. Piot; J. Santucci; J. Li; R. Tikhoplav

Summary form only given. An underdense plasma lens experiment is underway as a collaboration between UCLA and the Fermilab NICADD Photoinjector Laboratory (FNPL). The experiment will focus on measuring the variation of the plasma focusing along the longitudinal beam axis and comparing these results with theory and simulation. The experiment utilizes a thin Gaussian underdense plasma lens with peak density 5times1012 cm-3 and a FWHM length of 2.2 cm. This plasma lens will have a focusing strength equivalent to a quadrupole magnet with about 180 T/m field gradient. A 15 MeV, 8-12 nC electron beam with nominal dimensions sigmar = 600 mum and sigmaz= 2.1 mm will be focused by this plasma lens onto an OTR screen approximately 2 cm downstream of the lens. The light from the OTR screen will be imaged into a streak camera in order to directly measure the correlation between z and sigmar within the beam. Status and progress on the experiment are reported

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P. Piot

Northern Illinois University

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N. Barov

Northern Illinois University

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R. Tikhoplav

University of Rochester

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G. Travish

University of California

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Alex H. Lumpkin

Argonne National Laboratory

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