Performance of GRETINA for in-beam spectroscopy at NSCL

ORAL

Abstract

In early summer 2012, the Gamma-Ray Energy TRAcking In-beam Nuclear Array GRETINA was installed in front of the S800 Magnetic Spectrograph for in-flight gamma-ray spectroscopy campaign with fast beams of rare isotopes. In this type of experiments rare-isotopes beams provided by the Coupled Cyclotron Facility of the National Superconducting Cyclotron Laboratory (NSLC) are delivered onto a reaction target placed at the center of GRETINA. Reaction residues are detected in the spectrograph in coincidence with gamma rays in GRETINA. The high spatial resolution of GRETINA allows for accurate Doppler-shift reconstruction, while GRETINA's tracking capability provides gamma-ray data of high spectral quality. The performance of this powerful setup will be summarized.

Authors

  • Dirk Weisshaar

    • National Superconducting Cyclotron Laboratory, Michigan State University
    • NSCL
    • Michigan State University/NSCL
    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Vincent Bader

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Travis Baugher

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Daniel Bazin

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Jill Berryman

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Alexandra Gade

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Christoph Langer

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Antoine Lemasson

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Eric Lunderberg

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Shumpei Noji

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Francesco Recchia

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Ragnar Stroberg

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Christopher Walz

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Kathrin Wimmer

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA
  • Chris M. Campbell

    • Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
  • Heather L. Crawford

    • Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
  • Mario Cromaz

    • Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
  • Paul Fallon

    • Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
  • I-Yang Lee

    • Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
  • Augusto Macchiavelli

    • Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
  • Andreas Wiens

    • Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
  • Mike P. Carpenter

    • Physics Division, Argonne National Laboratory, Argonne, IL 60439, USA
  • Shaofei Zhu

    • Physics Division, Argonne National Laboratory, Argonne, IL 60439, USA
  • David Radford

    • Oak Ridge National Laboratory, Oak Ridge, Tennessee
  • Mike Scott

    • National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824, USA