The SPIRAL 2 Project
References (7)
Cited by (22)
ECRIS and EBIS charge state breeders: Present performances, future potentials
2013, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :Despite recent efforts in attempting to reduce beam contamination, this latter issue is the main motivation for ANL [8] and more recently TRIUMF [44] to replace their respective ECRIS by EBIS charge breeders. Yet ECRIS charge breeders still present the advantage of a full continuous operation, and are preferred in the case of the upgrade of the SPIRAL 1 facility [28], and the SPIRAL 2 [45] and SPES [46] projects. In the case of SPIRAL 1 and 2, the CIME cyclotron shall very efficiently suppress contaminants with a relative mass difference beyond a few 10−4 [47].
The orsay universal plunger system
2012, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentDevelopment and test of a cryogenic trap system dedicated to confinement of radioactive volatile isotopes in SPIRAL2 post-accelerator
2011, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :Fission products of different reactions are then scattered out of the target, ionized, separated on line and post-accelerated into the existing CIME cyclotron at GANIL (Fig. 1). Obtained secondary radioactive beams will be used in different experimental areas to perform many experiments in a wide range of neutron and proton rich nuclei far from the line of stability besides various applied and multidisciplinary physics [2]. Produced fission species from target irradiation reactions create strong radiological and environmental constraints that lead to many challenges in accelerator nuclear safety studies [3].
Targets for S3 at SPIRAL2
2010, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentLow-energy and secondary (radioactive) ion-beam profile measurements and optimization using modified Gafchromic® EBT film
2010, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentParticle identification with time-of-flight and pulse-shape discrimination in neutron-transmutation-doped silicon detectors
2009, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :High-quality silicon detectors with good PSD capability may provide a well-priced upgrading, or even alternative, to complex telescope installations, especially in large detector arrays, such as CHIMERA [2,3]. PSD is also an option in the construction of large future experimental instrumentations (e.g. FAZIA [4] and GASPARD [5]) for next generation beam facilities, e.g. SPIRAL2 [6] or EURISOL [7]. Since the early sixties it has been known that, when an energetic charged particle impacts on a solid-state silicon detector, the information on its nuclear charge Z, and partly even mass A, is encoded in the shape of the detector current signal [8–10].
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for the SPIRAL 2 Project Group