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MOPCC13 |
Beam Energy Measurements With a Optical Transition Radiation for the ELI-NP Compton Gamma Source |
68 |
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- M. Marongiu, D. Cortis
INFN-Roma, Roma, Italy
- E. Chiadroni, F. Cioeta, G. Di Pirro, G. Franzini, V. Shpakov, A. Stella, C. Vaccarezza, A. Variola
INFN/LNF, Frascati (Roma), Italy
- A. Cianchi
Università di Roma II Tor Vergata, Roma, Italy
- A. Giribono, M. Pompili
Sapienza University of Rome, Rome, Italy
- A. Mostacci, L. Palumbo
Rome University La Sapienza, Roma, Italy
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A high brightness electron LINAC is being built in the Compton Gamma Source at the ELI Nuclear Physics facility in Romania. To achieve the design luminosity, a train of 32 bunches, 16 ns spaced, with a nominal charge of 250 pC will collide with the laser beam in the interaction point at two electron beam energies, namely 280 MeV and 720 MeV. Electron beam spot size is measured with optical transition radiation (OTR) profile monitors. The paper deals with the possibility of using the OTR monitors to measure also beam energy along the machine; such measurements may help monitoring the accelerating sections performances, especially when the whole bunch train is being accelerated. We discuss the measurement principle, the expected accuracy and the main characteristic of the optical line to retrieve the angular distribution of the emitted radiation.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IBIC2017-MOPCC13
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TUPCF15 |
S-Band Cavity BPM Readout Electronics for the ELI-NP Gamma Beam Source |
243 |
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- M. Cargnelutti, B.B. Baricevic
I-Tech, Solkan, Slovenia
- G. Franzini, D. Pellegrini, A. Stella, A. Variola
INFN/LNF, Frascati (Roma), Italy
- A. Mostacci
Rome University La Sapienza, Roma, Italy
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The Extreme Light Infrastructure ' Nuclear Physics Gamma Beam Source (ELI-NP GBS) facility will provide an high intensity laser and a very intense gamma beam for verious experiments. The gamma beam is generated through incoherent Compton back-scattering of a laser light off a high brightness electron beam provided by a 720MeV warm LINAC. The electrons are organized in compact trains with up to 32 bunches, each separated by 16ns. To optimize the laser-electron interaction and therefore the generation of the gamma rays, one big challenge is to precisely monitor the trajectory of each electron bunch. To match this requirement, at the interaction point two S-band cavity beam position monitors will be used, and the related readout system should perform bunch-by-bunch position measurements with sub-μm resolution. Using 500MS/s ADC converters and dedicated data processing, the readout system proposes an alternative measurement concept. In this paper the architecture of the system, the implemented signal processing and the results of the first laboratory tests will be presented.
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Poster TUPCF15 [4.303 MB]
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IBIC2017-TUPCF15
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TUPCF16 |
Stripline Beam Position Monitor Modelling and Simulations for Charge Measurements |
247 |
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- G. Castorina
INFN-Roma1, Rome, Italy
- G. Franzini, B. Spataro
INFN/LNF, Frascati (Roma), Italy
- M. Marongiu, A. Mostacci
INFN-Roma, Roma, Italy
- A.A. Nosych
ALBA-CELLS Synchrotron, Cerdanyola del Vallès, Spain
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Strip line Beam Positions Monitors (BPMs) are the main devices used for non-intercepting position measurement for the electron LINAC of ELI-NP (Extreme Light Infrastructure - Nuclear Physics). All the 29 BPMs have the same design, with the exception of the one installed in one of the dump line, which has a much larger acceptance than the others. BPMs will also be used to measure the charge of the beam, by measuring the sum of the pickups signals and calibrating it with beam charge monitors installed along the LINAC. An analytical model has been developed for the proposed BPMs. This model has been checked by means of PIC/wakefield simulations, in order to obtain the pickups signals at the passage of the beam and to study the effects of BPMs non-linearities, particularly on charge measurements. Details of the analytical model, results of the numerical simulations and the correction algorithm proposed for charge measurements are described in this paper.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IBIC2017-TUPCF16
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