Georgy Vorobjev

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  • W. Barth, M. Bevcic, +30 authors HITRAP LINAC
  • 2007
The heavy ion trap facility (HITRAP), which is shown in fig.1 and is being built in the re-injection channel between ESR and SIS will provide unique beams of highly charged ions up to bare uranium at very low energies for a large variety of experiments. At the HITRAP facility the ions, produced by the GSI accelerator facility, will be decelerated in two(More)
The masses of ten proton-rich nuclides, including the N=Z+1 nuclides ⁸⁵Mo and ⁸⁷Tc, were measured with the Penning trap mass spectrometer SHIPTRAP. Compared to the Atomic Mass Evaluation 2003 a systematic shift of the mass surface by up to 1.6 MeV is observed causing significant abundance changes of the ashes of astrophysical x-ray bursts. Surprisingly low(More)
The heavy ion trap facility (HITRAP), which is being built in the re-injection channel between ESR and SIS will provide unique beams of highly charged ions up to bare uranium at very low energies for a large variety of experiments. At the HITRAP facility it is envisaged to decelerate heavy highly charged ions down to energies of the keV-range where they can(More)
Status of the HITRAP Project The heavy ion trap (HITRAP) will decelerate highly charged ions up to U 92+ , provided by the GSI accelerator complex at 4 MeV/u, down to 6 keV/u [1,2]. The decelerator contains a double drift buncher (DDB), an IH-type structure and a 4-rod Radio Frequency Quadrupole. The basic working frequency is 108 MHz. Until May 2007 the(More)
The heavy ion trap facility (HITRAP) (fig.1) will provide unique beams of highly charged ions up to bare U at very low energies for a large variety of experiments. HITRAP will decelerate ions (e.g. U 91+) produced by the GSI accelerator facility at relativistic energies. The ions are first decelerated the ESR down to 4 MeV/u and further decelerated down to(More)
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