Response of the Pixel Detector TimePix to Heavy Ions
- NázevTitle
- Response of the Pixel Detector TimePix to Heavy IonsResponse of the Pixel Detector TimePix to Heavy Ions
- Druh výsledkuResult type
- Článek v časopiseJournal article
- AutořiAuthors
- C. Granja, J. Jakůbek, U. Koester, M. Platkevič, S. Pospíšil
- DOIDOI
- 10.1016/j.nima.2010.06.166
- Časopis / citaceJournal / citation
- Nuclear Instruments and Methods in Physics Research, Section A, Accelerators, Spectrometers, Detectors and Associated Equipment. 2011, 2011(633), 198-202. ISSN 0168-9002.
- RokYear
- 2011
- JazykLanguage
- eng
- WoSWoS
- 000292782400060
- ScopusScopus
- 2-s2.0-79959820531
- RIVRIV
- RIV/68407700:21670/11:00165658!RIV12-MSM-21670___
- ProjektProject
- Experimentální studium exotických kanálů štěpení, prostorová a časová detekce radioaktivních iontůExperimental study of exotic fission decay modes and spatial and time coincidence detection of radioactive ions; Centrum experimentální jaderné astrofyziky a jaderné fyzikyCenter of Experimental Nuclear Astrophysics and Nuclear Physics; Fundamentální experimenty ve fyzice mikrosvětaFundamental Experiments in Physics of Microworld
AbstraktAbstract
The response of the pixel detector TimePix to ions in the 4-110 MeV kinetic energy range and A=1-136 mass range has been studied using the fission-fragment separator Lohengrin of the Institute Laue Langevin in Grenoble. For heavy charged particles TimePix can measure their (i) location and spatial distribution, (ii) kinetic energy, and (iii) time of arrival. Pixel signal distortion and saturation arise when large charge is locally deposited and can be minimized by suitable detector settings of baseline and threshold together with suitable low bias voltage.
The response of the pixel detector TimePix to ions in the 4-110 MeV kinetic energy range and A=1-136 mass range has been studied using the fission-fragment separator Lohengrin of the Institute Laue Langevin in Grenoble. For heavy charged particles TimePix can measure their (i) location and spatial distribution, (ii) kinetic energy, and (iii) time of arrival. Pixel signal distortion and saturation arise when large charge is locally deposited and can be minimized by suitable detector settings of baseline and threshold together with suitable low bias voltage.