ISAC and ARIEL: The TRIUMF Radioactive Beam Facilities and the Scientific Program A Laboratory Portrait of ISAC /

The TRIUMF Isotope Separator and Accelerator (ISAC) facility uses the isotope separation on-line (ISOL) technique to produce rare-isotope beams (RIB). The ISOL system consists of a primary production beam, a target/ion source, a mass separator, and beam transport system. The rare isotopes produced d...

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Corporate Author: SpringerLink (Online service)
Other Authors: Dilling, Jens. (Editor, http://id.loc.gov/vocabulary/relators/edt), Krücken, Reiner. (Editor, http://id.loc.gov/vocabulary/relators/edt), Merminga, Lia. (Editor, http://id.loc.gov/vocabulary/relators/edt)
Language:English
Published: Dordrecht : Springer Netherlands : Imprint: Springer, 2014.
Edition:1st ed. 2014.
Subjects:
Online Access:https://doi.org/10.1007/978-94-007-7963-1
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245 1 0 |a ISAC and ARIEL: The TRIUMF Radioactive Beam Facilities and the Scientific Program  |h [electronic resource] :  |b A Laboratory Portrait of ISAC /  |c edited by Jens Dilling, Reiner Krücken, Lia Merminga. 
250 |a 1st ed. 2014. 
264 1 |a Dordrecht :  |b Springer Netherlands :  |b Imprint: Springer,  |c 2014. 
300 |a VII, 284 p. 146 illus.  |b online resource. 
336 |a text  |b txt  |2 rdacontent 
337 |a computer  |b c  |2 rdamedia 
338 |a online resource  |b cr  |2 rdacarrier 
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505 0 |a From the contents: ISAC overview -- The TRIUMF 500 MeV cyclotron: the driver accelerator -- ISAC targets -- Rare isotope beams at ISAC—target & ion source systems -- Off line ion source terminal -- Charge state breeding of radioactive isotopes for ISAC -- ISAC LEBT -- The ISAC post-accelerator -- High energy beam lines -- The experimental facilities at ISAC. 
520 |a The TRIUMF Isotope Separator and Accelerator (ISAC) facility uses the isotope separation on-line (ISOL) technique to produce rare-isotope beams (RIB). The ISOL system consists of a primary production beam, a target/ion source, a mass separator, and beam transport system. The rare isotopes produced during the interaction of the proton beam with the target nucleus are stopped in the bulk of the target material. They diffuse inside the target material matrix to the surface of the grain and then effuse to the ion source where they are ionized to form an ion beam that can be separated by mass and then guided to the experimental facilities. Previously published in the journal Hyperfine Interactions. 
650 0 |a Nuclear physics. 
650 0 |a Particle acceleration. 
650 0 |a Materials science. 
650 1 4 |a Particle and Nuclear Physics.  |0 https://scigraph.springernature.com/ontologies/product-market-codes/P23002 
650 2 4 |a Particle Acceleration and Detection, Beam Physics.  |0 https://scigraph.springernature.com/ontologies/product-market-codes/P23037 
650 2 4 |a Characterization and Evaluation of Materials.  |0 https://scigraph.springernature.com/ontologies/product-market-codes/Z17000 
700 1 |a Dilling, Jens.  |e editor.  |4 edt  |4 http://id.loc.gov/vocabulary/relators/edt 
700 1 |a Krücken, Reiner.  |e editor.  |4 edt  |4 http://id.loc.gov/vocabulary/relators/edt 
700 1 |a Merminga, Lia.  |e editor.  |4 edt  |4 http://id.loc.gov/vocabulary/relators/edt 
710 2 |a SpringerLink (Online service) 
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950 |a Physics and Astronomy (SpringerNature-11651) 
950 |a Physics and Astronomy (R0) (SpringerNature-43715)