| HAL : in2p3-00656422, version 1 |
| DOI : 10.1016/j.nima.2011.10.061 |
| Fiche détaillée | Récupérer au format |
|
|
| Nuclear Instruments and Methods in Physics Research Research: Accelerators, Spectrometers, Detectors and Associated Equipment 664 (2012) 251-263 |
|
|
|
|
| Particle identification using the (DELTA)E-E technique and pulse shape discrimination with the silicon detectors of the FAZIA project |
|
|
|
|
| FAZIA Collaboration(s) |
|
|
| (2012) |
|
|
| The response of silicon-silicon-CsI(Tl) and silicon-CsI(Tl) telescopes to fragments produced in nuclear interactions has been studied. The telescopes were developed within the FAZIA collaboration. The capabilities of two methods are compared: (a) the standard ΔE-E technique and (b) the digital Pulse Shape Analysis technique (for identification of nuclear fragments stopped in a single Si-layer). In a test setup, nuclear fragments covering a large range in nuclear charge, mass and energy were detected. They were produced in nuclear reactions induced by a 35A MeV beam of 129Xe impinging on various targets. It was found that the ΔE-E correlations allow the identification of all isotopes up to Z∼25. With the digital Pulse Shape Analysis it is possible to fully distinguish the charge of stopped nuclei up to the maximum available Z (slightly over that of the beam, Z=54). |
|
|
|
|
|
|
|
|
|
|
| 1 : | LPCC - Laboratoire de Physique Corpusculaire de Caen |
| 2 : | IPNO - Institut de Physique Nucléaire d'Orsay |
| 3 : | GANIL - Grand Accélérateur National d'Ions Lourds |
|
|
|
|
|
|
|
|
| Physique théorique Dynamique et thermodynamique nucléaire |
|
|
|
|
| Thème(s) | : | Physique/Physique Nucléaire Expérimentale |
|
|
| Pulse shape discrimination – ΔE-E – Silicon detector – Charge signal – Current signal |
| in2p3-00656422, version 1 | |
| http://hal.in2p3.fr/in2p3-00656422 | |
| oai:hal.in2p3.fr:in2p3-00656422 | |
| Contributeur : Sandrine Guesnon | |
| Soumis le : Mercredi 4 Janvier 2012, 11:42:49 | |
| Dernière modification le : Mercredi 4 Janvier 2012, 15:43:08 | |