g A biased view Nuclear Physics Applications Detection techniques ions

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Presentation transcript:

g A biased view Nuclear Physics Applications Detection techniques ions Nuclear matter EELS -energy filtered imaging Halo nuclei g Micro dosimetry Environmental radiation Safety analyses

Safety analyses of a repository for nuclear waste Nuclear Physics Safety analyses of a repository for nuclear waste Antonio Pereira, Bruno Mendes, Robert Broed Radiation damage in the biological cell David Liljequist Halo nuclei Katarina Wilhelmsen Rolander, Linda Gerén, Karin Lindh, Per-Erik Tegnér, ChrB

Properties of nuclear matter Nuclear Physics ions Properties of nuclear matter Kjell Fransson Linda Gerén Lennart Holmberg Kalle Lindberg Per-Erik Tegnér Katarina Wilhelmsen Rolander ChrB

Deeply Bound Pionic Atoms Nuclear Physics ions Deeply Bound Pionic Atoms The width and the binding energy of the 1S state give information on the local (s-wave) part of the optical potential, which in turn gives information on pion properties in the nuclear medium.  Partial restoration of chiral symmetry?

HOW: d + 136Xe  135Xep + 3He d + n  p- + 3He Nuclear Physics ions HOW: d + 136Xe  135Xep + 3He d + n  p- + 3He Cluster target of xenon 1013 atoms per cm2

ZERO-degree spectrometer Nuclear Physics ions ZERO-degree spectrometer DE  800 keV for 350MeV 3He

Nuclear Physics Sampled pulses ions E  v  B 15 mm

Detector elements made in Jülich Nuclear Physics ions Detector elements made in Jülich 6636 mm2 position sensitive Three arm spectrometer

Electron Energy Loss Spectroscopy Nuclear Physics e- Electron Energy Loss Spectroscopy Stefan Csillag Susanne Nyquist Esteban Urones Per-Gustaf Åstrand

Nuclear Physics e- Single electron detection

Nuclear Physics e-

Nuclear Physics e-

Nuclear Physics e-

Nuclear Physics e-

Nuclear Physics e-

Nuclear Physics e-

Environmental gamma radiation Nuclear Physics g Environmental gamma radiation Jan Blomquist Kjell Fransson David Liljequist Gilberto Batres Pia Nilsson Per-Erik Tegnér ChrB

g Environmental in situ gamma spectroscopy Nuclear Physics 0.5 g/cm2

CdTe detectors g  Eg=662 keV + - Sampled preamp. pulses (full energy Nuclear Physics CdTe detectors g  Eg=662 keV + - Sampled preamp. pulses (full energy deposited). 2mm For holes: td = 3.6µs  = 2.5µs Pulse-height spectrum

g Interaction depth vs. pulse height (after analysis) Nuclear Physics g Interaction depth vs. pulse height (after analysis) Projection on pulse-height axis. + - Energy spectrum after analysis depth

Nuclear Physics g