A. Biagioni
Istituto Nazionale di Fisica Nucleare
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Featured researches published by A. Biagioni.
Applied Physics Letters | 2017
R. Pompili; M. P. Anania; M. Bellaveglia; A. Biagioni; S. Bini; F. Bisesto; E. Brentegani; G. Castorina; E. Chiadroni; A. Cianchi; M. Croia; D. Di Giovenale; M. Ferrario; Francesco Filippi; A. Giribono; V. Lollo; A. Marocchino; Marco Marongiu; A. Mostacci; G. Di Pirro; S. Romeo; A. R. Rossi; J. Scifo; V. Shpakov; C. Vaccarezza; F. Villa; A. Zigler
The active plasma lens represents a compact and affordable tool with radially symmetric focusing and field gradients up to several kT/m. In order to be used as a focusing device, its effects on the particle beam distribution must be well characterized. Here, we present the experimental results obtained by focusing an high-brightness electron beam by means of a 3 cm-long discharge-capillary pre-filled with Hydrogen gas. We achieved minimum spot sizes of 24 μ m (rms) showing that, during plasma lensing, the beam emittance increases due to nonlinearities in the focusing field. The results have been cross-checked with numerical simulations, showing an excellent agreement.
Applied Physics Letters | 2017
A. Marocchino; M. P. Anania; M. Bellaveglia; A. Biagioni; S. Bini; F. Bisesto; E. Brentegani; E. Chiadroni; A. Cianchi; M. Croia; D. Di Giovenale; M. Ferrario; Francesco Filippi; A. Giribono; V. Lollo; Marco Marongiu; A. Mostacci; G. Di Pirro; R. Pompili; S. Romeo; A. R. Rossi; J. Scifo; V. Shpakov; C. Vaccarezza; F. Villa; A. Zigler
We report on the experimental characterization of the effect that a passive plasma lens in the overdense regime has on high-brightness bunch quality by means of 6D phase-space analysis. The passive lens is generated by confining hydrogen gas with a capillary tube pre-ionized with a high-voltage discharge. We observed that the optimum condition is retrieved at the end of the overdense regime with almost no effect on bunch brightness. The presence of gas jets, leaking from the hollow capillary end-points, extends the lens effects also outside of the capillary, resulting in longer focusing channels. Experimental results are supported with numerical simulations of the complete accelerator line together with the plasma channel section.
New Journal of Physics | 2016
R. Pompili; M. P. Anania; M. Bellaveglia; A. Biagioni; G. Castorina; E. Chiadroni; A. Cianchi; M. Croia; D. Di Giovenale; M. Ferrario; Francesco Filippi; A. Gallo; G. Gatti; F. Giorgianni; A. Giribono; Wei-Xue Li; S. Lupi; A. Mostacci; M. Petrarca; L. Piersanti; G. Di Pirro; S. Romeo; J. Scifo; V. Shpakov; C. Vaccarezza; F. Villa
The generation of ultra-short electron bunches with ultra-low timing-jitter relative to the photo-cathode (PC) laser has been experimentally proved for the first time at the SPARC_LAB test-facility (INFN-LNF, Frascati) exploiting a two-stage hybrid compression scheme. The first stage employs RF-based compression (velocity-bunching), which shortens the bunch and imprints an energy chirp on it. The second stage is performed in a non-isochronous dogleg line, where the compression is completed resulting in a final bunch duration below 90 fs (rms). At the same time, the beam arrival timing-jitter with respect to the PC laser has been measured to be lower than 20 fs (rms). The reported results have been validated with numerical simulations.
Journal of Instrumentation | 2016
Francesco Filippi; M. P. Anania; A. Biagioni; E. Chiadroni; A. Cianchi; M. Ferrario; A. Mostacci; L. Palumbo; A. Zigler
Advanced particle accelerators are based on the excitation of large amplitude plasma waves driven by either electron or laser beams. Future experiments scheduled at the SPARC_LAB test facility aim to demonstrate the acceleration of high brightness electron beams through the so-called resonant Plasma Wakefield Acceleration scheme in which a train of electron bunches (drivers) resonantly excites wakefields into a preformed hydrogen plasma; the last bunch (witness) injected at the proper accelerating phase gains energy from the wake. The quality of the accelerated beam depends strongly on plasma density and its distribution along the acceleration length. The measurements of plasma density of the order of 1016–1017 cm−3 can be performed with spectroscopic measurements of the plasma-emitted light. The measured density distribution for hydrogen filled capillary discharge with both Balmer alpha and Balmer beta lines and shot-to-shot variation are here reported.
Journal of Physics: Conference Series | 2017
Francesco Filippi; M. P. Anania; E. Brentegani; A. Biagioni; A. Cianchi; E. Chiadroni; M. Ferrario; R. Pompili; S. Romeo; A. Zigler
Plasma Wakefield Accelerators are based on the excitation of large amplitude plasma waves excited by either a laser or a particle driver beam. The amplitude of the waves, as well as their spatial dimensions and the consequent accelerating gradient depend strongly on the background electron density along the path of the accelerated particles. The process needs stable and reliable plasma sources, whose density profile must be controlled and properly engineered to ensure the appropriate accelerating mechanism. Plasma confinement inside gas filled capillaries have been studied in the past since this technique allows to control the evolution of the plasma, ensuring a stable and repeatable plasma density distribution during the interaction with the drivers. Moreover, in a gas filled capillary plasma can be pre-ionized by a current discharge to avoid ionization losses. Different capillary geometries have been studied to allow the proper temporal and spatial evolution of the plasma along the acceleration length. Results of this analysis obtained by varying the length and the number of gas inlets will be presented.
Journal of Instrumentation | 2016
A. Biagioni; M. P. Anania; M. Bellaveglia; E. Chiadroni; A. Cianchi; D. Di Giovenale; G. Di Pirro; M. Ferrario; Francesco Filippi; A. Mostacci; R. Pompili; V. Shpakov; C. Vaccarezza; F. Villa; A. Zigler
Plasma density represents a very important parameter for both laser wakefield and plasma wakefield acceleration, which use a gas-filled capillary plasma source. Several techniques can be used to measure the plasma density within a capillary discharge, which are mainly based on optical diagnostic methods, as for example the well-known spectroscopic method using the Stark broadening effect. In this work, we introduce a preliminary study on an alternative way to detect the plasma density, based on the shock waves produced by gas discharge in a capillary. Firstly, the measurements of the acoustic spectral content relative to the laser-induced plasmas by a solid target allowed us to understand the main properties of the acoustic waves produced during this kind of plasma generation; afterwards, we have extended such acoustic technique to the capillary plasma source in order to calibrate it by comparison with the stark broadening method.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
R. Pompili; M. P. Anania; M. Bellaveglia; A. Biagioni; S. Bini; F. Bisesto; E. Chiadroni; A. Cianchi; G. Costa; D. Di Giovenale; M. Ferrario; Francesco Filippi; A. Gallo; A. Giribono; V. Lollo; A. Marocchino; V. Martinelli; A. Mostacci; G. Di Pirro; S. Romeo; J. Scifo; V. Shpakov; C. Vaccarezza; F. Villa; A. Zigler
Abstract The current activity of the SPARC_LAB test-facility is focused on the realization of plasma-based acceleration experiments with the aim to provide accelerating field of the order of several GV/m while maintaining the overall quality (in terms of energy spread and emittance) of the accelerated electron bunch. In the following, the current status of such an activity is presented. We also show results related to the usability of plasmas as focusing lenses in view of a complete plasma-based focusing and accelerating system.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
E. Chiadroni; M. P. Anania; M. Bellaveglia; A. Biagioni; F. Bisesto; E. Brentegani; F. Cardelli; A. Cianchi; G. Costa; D. Di Giovenale; G. Di Pirro; M. Ferrario; Francesco Filippi; A. Gallo; A. Giribono; A. Marocchino; A. Mostacci; L. Piersanti; R. Pompili; J. B. Rosenzweig; Andrea Rossi; J. Scifo; V. Shpakov; C. Vaccarezza; F. Villa; A. Zigler
Abstract Beam injection and extraction from a plasma module is still one of the crucial aspects to solve in order to produce high quality electron beams with a plasma accelerator. Proper matching conditions require to focus the incoming high brightness beam down to few microns size and to capture a high divergent beam at the exit without loss of beam quality. Plasma-based lenses have proven to provide focusing gradients of the order of kT/m with radially symmetric focusing thus promising compact and affordable alternative to permanent magnets in the design of transport lines. In this paper an overview of recent experiments and future perspectives of plasma lenses is reported.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
J. Scifo; D. Alesini; M. P. Anania; M. Bellaveglia; S. Bellucci; A. Biagioni; F. Bisesto; F. Cardelli; E. Chiadroni; A. Cianchi; G. Costa; D. Di Giovenale; G. Di Pirro; R. Di Raddo; D. H. Dowell; M. Ferrario; A. Giribono; A. Lorusso; F. Micciulla; A. Mostacci; D. Passeri; A. Perrone; L. Piersanti; R. Pompili; V. Shpakov; A. Stella; M. Trovò; F. Villa
Abstract R&D activity on Cu photocathodes is under development at the SPARC_LAB test facility to fully characterize each stage of the photocathode “life” and to have a complete overview of the photoemission properties in high brightness photo-injectors. The nano(n)-machining process presented here consists in diamond milling, and blowing with dry nitrogen. This procedure reduces the roughness of the cathode surface and prevents surface contamination introduced by other techniques, such as polishing with diamond paste or the machining with oil. Both high roughness and surface contamination cause an increase of intrinsic emittance and consequently a reduction of the overall electron beam brightness. To quantify these effects, we have characterized the photocathode surface in terms of roughness measurement, and morphology and chemical composition analysis by means of Scanning Electron Microscopy (SEM), Energy Dispersive Spectroscopy (EDS), and Atomic Force Microscopy (AFM) techniques. The effects of n -machining on the electron beam quality have been also investigated through emittance measurements before and after the surface processing technique. Finally, we present preliminary emittance studies of yttrium thin film on Cu photocathodes.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
A. Biagioni; M. P. Anania; M. Bellaveglia; E. Brentegani; G. Castorina; E. Chiadroni; A. Cianchi; D. Di Giovenale; G. Di Pirro; Hesham Fares; L. Ficcadenti; Francesco Filippi; M. Ferrario; A. Mostacci; R. Pompili; J. Scifo; B. Spataro; C. Vaccarezza; F. Villa; A. Zigler
Abstract Plasma wake-field acceleration experiments are performed at the SPARC_LAB test facility by using a gas-filled capillary plasma source composed of a dielectric capillary. The electron can reach GeV energy in a few centimeters, with an accelerating gradient orders of magnitude larger than provided by conventional techniques. In this acceleration scheme, wake fields produced by passing electron beams through dielectric structures can determine a strong beam instability that represents an important hurdle towards the capability to focus high-current electron beams in the transverse plane. For these reasons, the estimation of the transverse wake-field amplitudes assumes a fundamental role in the implementation of the plasma wake-field acceleration. In this work, it presented a study to investigate which parameters affect the wake-field formation inside a cylindrical dielectric structure, both the capillary dimensions and the beam parameters, and it is introduced a quantitative evaluation of the longitudinal and transverse electric fields.