1. Beam tracking with micromegas & wire chambers in secondary electron detection configuration
- Author
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T. Materna, T Chaminade, E Monmarthe, M. A. G. Alvarez, M Riallot, S. Damoy, Begoña Fernández, T. Papaevangelou, C. Spitaels, Diane Doré, H Savajols, M Voštinar, J. Pancin, M Kebbiri, A. Drouart, F. Druillole, G. Frémont, S. Panebianco, Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, and Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
- Subjects
Physics::Instrumentation and Detectors ,Heavy-ion detectors ,Particle tracking detectors (Gaseous detectors) ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,7. Clean energy ,Secondary electrons ,Particle detector ,Micropattern gaseous detectors (MSGC ,Optics ,0103 physical sciences ,drift chambers ,[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] ,29.40.Gx ,29.50.+v 29.40.Wk ,29.30.-h ,010306 general physics ,Instrumentation ,Image resolution ,Mathematical Physics ,drift tubes ,etc) ,Physics ,Wire chamber ,GEM ,Spectrometer ,010308 nuclear & particles physics ,business.industry ,Detector ,Thin-gap chambers ,MicroMegas detector ,InGrid ,3. Good health ,RETHGEM ,Time of flight ,proportional chambers etc) ,MICROMEGAS ,business ,Wire chambers(MWPC ,THGEM - Abstract
Trabajo presentado a la: "3rd International Conference on Micro Pattern Gaseous Detectors (MPGD2013)", celebrada en Zaragoza (España) del 1 al 4 de julio de 2013.-- et al., The focal plane of S3 (Super Separator Spectrometer), a new experimental area of SPIRAL2 at GANIL, will be used for identification of nuclei, and requires the reconstruction of their trajectories and velocities by the Time Of Flight (TOF) method. Classical tracking detectors used in-beam would generate a lot of angular and energy straggling due to their thickness. One solution is the use of a SED (Secondary Electron Detection), which consists of a thin emissive foil in beam coupled to a low pressure gaseous detector out of the beam, for the detection of secondary electrons ejected from the foil. Moreover, this type of detector can be used for classical beam tracking at low energies, or for example at NFS (GANIL) for the FALSTAFF experiment for the reconstruction of fission fragments trajectories. Several low pressure gaseous detectors such as wire chambers and Micromegas have been constructed and tested since 2008. High counting rate capabilities and good time resolution obtained in previous tests motivated the construction of a new real-size 2D prototype wire chamber and a 2D bulk Micromegas at low pressure. For the first time, spatial resolution of the Micromegas at low pressure (below 20 mbar) in the SED configuration was measured. Different tests have been performed in order to characterize time and spatial properties of both prototypes, giving spatial resolution in the horizontal (X) direction of 0.90(0.02) mm FWHM for the real size prototype and 0.72(0.08) mm FWHM for Micromegas, and a time resolution of ~ 110(25) ps for the real size prototype.
- Published
- 2013
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