001709392 001__ 1709392
001709392 005__ 20170213104504.0
001709392 0247_ $$2DOI$$a10.1016/j.nima.2012.12.090
001709392 0248_ $$aoai:cds.cern.ch:1709392$$pcerncds:CERN
001709392 035__ $$9Inspire$$a1224399
001709392 041__ $$aeng
001709392 100__ $$aRajabali, M.M$$uLeuven U.
001709392 245__ $$aA dedicated decay-spectroscopy station for the collinear resonance ionization experiment at ISOLDE
001709392 260__ $$c2013
001709392 300__ $$a5 p
001709392 520__ $$9Elsevier$$aA new decay-spectroscopy station (DSS) has been developed to be coupled to the collinear resonance ionization spectroscopy (CRIS) beam line at CERN-ISOLDE. The system uses a rotatable wheel with ten 20@mg/cm^2 carbon foils as beam implantation sites for the efficient measurement of charged decay products. Silicon detectors are placed on either side of the carbon foil in an optimal geometry to cover a large solid angle for detecting these charged particles. In addition to the silicon detectors at the on-beam axis position, a second pair of off-beam axis detectors are placed at the wheel position 108^o away, allowing longer-lived species to be studied. Up to three high purity germanium detectors can be placed around the chamber for particle-gamma correlated measurement. The radioactive beam is transported through the CRIS beam line before implantation into a carbon foil at the DSS. All materials used in the DSS are UHV-compatible to maintain high vacuum conditions required by the CRIS beam line. This paper describes the DSS and presents the first data collected at the setup during the commissioning run with ^2^2^1Fr.
001709392 595__ $$aINSPIRE-PUBL-2013-06
001709392 65017 $$2SzGeCERN$$aDetectors and Experimental Techniques
001709392 690C_ $$aCERN
001709392 693__ $$aCERN ISOLDE
001709392 700__ $$aBillowes, J$$uManchester U.
001709392 700__ $$aBissell, M.L$$uLeuven U.
001709392 700__ $$aCocolios, T.E$$uCERN
001709392 700__ $$aDe Schepper, S$$uLeuven U.
001709392 700__ $$aDewolf, K$$uLeuven U.
001709392 700__ $$aFlanagan, K.T$$uManchester U.
001709392 700__ $$aLe Blanc, F$$uOrsay, IPN$$uOrsay, LPT
001709392 700__ $$aLynch, K.M$$uManchester U$$uCERN
001709392 700__ $$aMarsh, B.A$$uCERN
001709392 700__ $$aMason, P.J.R$$uSurrey U.
001709392 700__ $$aMatea, I$$uOrsay, LPT$$uOrsay, IPN
001709392 700__ $$aNeyens, G$$uLeuven U.
001709392 700__ $$aPapuga, J$$uLeuven U.
001709392 700__ $$aProcter, T.J$$uManchester U.
001709392 700__ $$aRothe, S$$uCERN$$uMainz U., Inst. Phys.
001709392 700__ $$aSimpson, G.S$$uLPSC, Grenoble
001709392 700__ $$aSmith, A.J$$uManchester U.
001709392 700__ $$aStroke, H.H$$uNew York U.
001709392 700__ $$aVerney, D$$uOrsay, IPN$$uOrsay, LPT
001709392 700__ $$aWalker, P.M$$uSurrey U.
001709392 700__ $$aWendt, K$$uMainz U., Inst. Phys.
001709392 700__ $$aWood, R.T$$uSurrey U.
001709392 773__ $$c35-39$$pNucl. Instrum. Methods Phys. Res., A$$v707$$y2013
001709392 916__ $$sn$$w201425$$ya2013
001709392 960__ $$a13
001709392 980__ $$aARTICLE