15 research outputs found
Capabilities and performance of the CLEAR facility photo-injector
This paper describes the current functionality and newly implemented capabilities of the CLEAR facility photo-injector laser. The primary focus for CLEAR is general R&D and component studies for existing and future machines at CERN. Accordingly, its photo-injector laser system has been upgraded in order to accommodate for a large range of experimental setups and tests. The systems and performance presented here have been developed with a view on improving the CLEAR injector flexibility, reliability and its systematic optimization
Studies of Cs3Sb cathodes for the CLIC drive beam photo injector option
Within the CLIC (Compact Linear Collider) project, feasibility studies of a photo injector option for the drive beam as an alternative to its baseline design using a thermionic electron gun are on-going. This R&D program covers both the laser and the photocathode side. Whereas the available laser pulse energy in ultra-violet (UV) is currently limited by the optical defects in the 4thharmonics frequency conversion crystal induced by the0.14 ms long pulse trains, recent measurements of Cs3Sbphotocathodes sensitive to green light showed their potential to overcome this limitation. Moreover, using visible laser beams leads to better stability of produced electron bunches and one can take advantages of the availability of higher quality optics. The studied Cs3Sbphotocathodes have been produced in the CERN photo emission laboratory using the co-deposition technique and tested in a DC gun set-up. The analysis of data acquired during the cathode production process will be presented in this paper, as well as the results of lifetime measurements in the DC gu
Further development of GALS setup at JINR
The aim of this paper is to report on the present status of the GAs cell based Laser ionization and separation Setup (GALS project) that is under construction at the Flerov Laboratory of Nuclear Reactions (FLNR) of JINR, Dubna. This project is directed on production of neutron-rich isotopes in the region of the magic â=â126 neutron number using multi-nucleon transfer reactions. The laser laboratory extension based on new TiSa lasers was performed, options of using a straight sextupole (SPIG) or an S-shaped quadrupole ion guides in the setup were compared based on the computer simulations, and the work on the rest of the GALS subsystems is being continued
Production of long bunch trains with 4.5ââÎŒC total charge using a photoinjector
A photoinjector, PHIN (PHotoINjector), has been realized at CERN by a joint effort of several institutes within the European Coordinated Accelerator Research in Europe program. The test facility has been installed and commissioned at CERN with the aim to demonstrate the beam parameters needed for the CLIC Test Facility 3 (CTF3). This beam is unique with respect to its long bunch train and high average charge per bunch requirements. The nominal beam for CTF3 consists of 1908 bunches each having a 2.33 nC charge and a bunch frequency of 1.5 GHz. Thus, a total charge of âŒ4.4ââÎŒC has to be extracted and accelerated. The stability of the intensity and the beam parameters along this exceptionally high average current train is crucial for the correct functioning of the CLIC drive beam scheme. Consequently, extensive time-resolved measurements of the transverse and longitudinal beam parameters have been developed, optimized, and performed. The shot-to-shot intensity stability has been studied in detail for the electron and the laser beams, simultaneously. The PHIN photoinjector has been commissioned between 2008 and 2010 during intermittent operations. This paper reports on the obtained results in order to demonstrate the feasibility and the stability of the required beam parameters
In-source laser spectroscopy of dysprosium isotopes at the ISOLDE-RILIS
A number of radiogenically produced dysprosium isotopes have been studied by in-source laser spectroscopy at ISOLDE using the Resonance Ionization Laser Ion Source (RILIS). Isotope shifts were measured relative to Dy in the 4 f6s I (gs) 4 f6s6p (8,1) (418.8 nm) resonance transition. The electronic factor, F, and mass shift factor, M, were extracted and used for determining the changes in mean-squared charge radii for Dy and Dy for the ïŹrst time.A number of radiogenically produced dysprosium isotopes have been studied by in-source laser spectroscopy at ISOLDE using the Resonance Ionization Laser Ion Source (RILIS). Isotope shifts were measured relative to Dy in the 46 I (gs)â 466(8,1) (418.8nm) resonance transition. The electronic factor, , and mass shift factor, , were extracted and used for determining the changes in mean-squared charge radii for Dy and Dy for the first time
MELISSA: Laser ion source setup at CERN-MEDICIS facility. Blueprint
The Resonance Ionization Laser Ion Source (RILIS) has become an essential feature of many radioactive ion beam facilities worldwide since it offers an unmatched combination of efficiency and selectivity in the production of ion beams of many different chemical elements. In 2019, the laser ion source setup MELISSA is going to be established at the CERN-MEDICIS facility, based on the experience of the workgroup LARISSA of the University Mainz and CERN ISOLDE RILIS team. The purpose is to enhance the capability of the radioactive ion beam supply for end users by optimizing the yield and the purity of the final product. In this article, the blueprint of the laser ion source, as well as the key aspects of its development and operation are presented.The Resonance Ionization Laser Ion Source (RILIS) has become an essential feature of many radioactive ion beamfacilities worldwide since it offers an unmatched combination of efficiency and selectivity in the production ofion beams of many different chemical elements. In 2019, the laser ion source setup MELISSA is going to beestablished at the CERN-MEDICIS facility, based on the experience of the workgroup LARISSA of the UniversityMainz and CERN ISOLDE RILIS team. The purpose is to enhance the capability of the radioactive ion beamsupply for end users by optimizing the yield and the purity of the final product. In this article, the blueprint ofthe laser ion source, as well as the key aspects of its development and operation are presented