2013
DOI: 10.1016/j.nimb.2013.07.069
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A novel ion cooling trap for multi-reflection time-of-flight mass spectrograph

Abstract: A radiofrequency quadrupole ion trap system for use with a multi-reflection time-of-flight mass spectrograph (MRTOF) for shortlived nuclei has been developed. The trap system consists of two different parts, an asymmetric taper trap and a flat trap. The ions are cooled to a sufficient small bunch for precise mass measurement with MRTOF in only 2 ms cooling time in the flat trap, then orthogonally ejected to the MRTOF for mass analysis. A trapping efficiency of ≈27% for 23 Na + and ≈5.1% for 7 Li + has been ach… Show more

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Cited by 29 publications
(15 citation statements)
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“…As ions left the gas cell via the small exit orifice, they were transported via rf-multipole ion guides to a triplet of rf quadrupole ion traps, similar to that reported in Ref. [20], where they accumulated and cooled. The ions were then orthogonally ejected from the central trap, accelerated by a pulsed drift tube to 1.5 keV, and transported 2.5 m to a second pulsed drift tube and deceleration optics, followed by a second set of rf-quadrupole traps wherein the ions were recaptured.…”
mentioning
confidence: 74%
“…As ions left the gas cell via the small exit orifice, they were transported via rf-multipole ion guides to a triplet of rf quadrupole ion traps, similar to that reported in Ref. [20], where they accumulated and cooled. The ions were then orthogonally ejected from the central trap, accelerated by a pulsed drift tube to 1.5 keV, and transported 2.5 m to a second pulsed drift tube and deceleration optics, followed by a second set of rf-quadrupole traps wherein the ions were recaptured.…”
mentioning
confidence: 74%
“…In these devices cooled short ion bunches are reflected between electrostatic mirrors. Thus, a compact setup can be maintained while providing high mass resolving powers up to about 200 000 for millisecond flight times [36][37][38]. In contrast to conventional ToF-MS where the flight path limits the achievable precision to typically a level of 10 −6 these devices can reach relative mass uncertainties of about 10 −7 or even below [39].…”
Section: Nobel Symposium Ns160 -Chemistry and Physics Of Heavy And Sumentioning
confidence: 99%
“…Hence the beam preparation stages are usually the same involving a buffer gas stopping cell and an RFQ buncher. At RIKEN an MR-ToF-MS setup has been installed behind the new gas-filled recoil separator GARIS II [36]. First on-line measurements have been performed in neutron-deficient Fr isotopes [40].…”
Section: Nobel Symposium Ns160 -Chemistry and Physics Of Heavy And Sumentioning
confidence: 99%
“…The first and second ion trap systems, each consisting of a pair of linear Paul traps on either side of a "flat" ion trap [24], have the same geometry and were filled with helium buffer gas at ∼10 −2 mbar. In the first trap system, the fore and aft linear Paul traps accumulated the continuous ion beams from the gas cell and from a thermal ion source, respectively, in order to precool and prebunch the ion beam prior to transfer to the flat trap.…”
mentioning
confidence: 99%