0000000000023485

AUTHOR

N. Braun

showing 4 related works from this author

The Performance of Belle II Data Acquisition System in the First Physics Run

2019

The Belle II experiment is a new generation B-factory experiment at KEK in Japan aiming at the search for New Physics in a huge sample of B-meson dacays. The commissioning of the SuperKEKB accelerator was started in 2017 (Phase 1), and then a pilot run with outer detectors was performed in 2018 (Phase 2). From March this year, an operation with the full detector has been started for the physics data taking (Phase 3). The Belle II data acquisiton system (DAQ) is now fully working in the Phase 3 run. The system consists of the trigger timing distribution system, the common readout modules (COPPER) with the unified optical data link to the detector front end, the readout PCs and the network sw…

Physicsbusiness.product_categoryPhysics::Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industrymedia_common.quotation_subjectDetector01 natural sciencesSample (graphics)Front and back endsData acquisitionDebugging0103 physical sciencesComputer data storageNetwork switch010306 general physicsbusinessComputer hardwareData reductionmedia_common2019 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC)
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Isospin symmetry in thesdshell: Transition strengths in the neutron-deficientsdshell nucleusAr33

2014

Reduced transition strengths of the deexciting transitions from the first two excited states in 33Ar were measured in a relativistic Coulomb excitation experiment at the GSI Helmholtz center. The radioactive ion beam was produced by fragmentation of a primary 36Ar beam on a 9Be target followed by the selection of the reaction product of interest via the GSI Fragment Separator. The 33Ar beam hit a secondary 197Au target with an energy of approximately 145 MeV/nucleon. An array of high-purity germanium cluster detectors and large-volume BaF2 scintillator detectors were employed for γ -ray spectroscopy at the secondary target position. The Lund-York-Cologne Calorimeter was used to track the ou…

Nuclear reactionPhysicsNuclear and High Energy PhysicsIon beamNuclear TheoryCoulomb excitationIonNuclear physicsExcited stateGamma spectroscopyNeutronAtomic physicsNuclear ExperimentNucleonPhysical Review C
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Superallowed Gamow-Teller decay of the doubly magic nucleus $^{100}$Sn

2012

Expérience au GSI; The shell structure of atomic nuclei is associated with 'magic numbers' and originates in the nearly independent motion of neutrons and protons in a mean potential generated by all nucleons. During b1-decay, a proton transforms into a neutron in a previously not fully occupied orbital, emitting a positron-neutrino pair with either parallel or antiparallel spins, in a Gamow-Teller or Fermi transition, respectively. The transition probability, or strength, of a Gamow-Teller transition depends sensitively on the underlying shell structure and is usually distributed among many states in the neighbouring nucleus. Here we report measurements of the half-life and decay energy fo…

PhysicsMultidisciplinaryProton010308 nuclear & particles physicsProton decayNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBeta decayNuclear physicsDecay energy0103 physical sciencesAtomic nucleusPhysical SciencesFysikNeutronAtomic physics010306 general physicsNucleonNuclear ExperimentRadioactive decay
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Relativistic Coulomb excitation of Kr 88

2016

International audience; To investigate the systematics of mixed-symmetry states in N=52 isotones, a relativistic Coulomb excitation experiment was performed during the PreSPEC campaign at the GSI Helmholtzzentrum für Schwerionenforschung to determine E2 transition strengths to 2+ states of the radioactive nucleus $^{88}$Kr. Absolute transition rates could be measured towards the first and third 2+ states. For the latter a mixed-symmetry character is suggested on the basis of the indication for a strong M1 transition to the fully symmetric 21+ state, extending the knowledge of the N=52 isotones below Z=40. A comparison with the proton-neutron interacting boson model and shell-model predictio…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryNuclear structureState (functional analysis)Coulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsgamma-ray spectroscopySubatomic Physicsrelativistic Coulomb excitationnuclear structure0103 physical sciencesGamma spectroscopyAtomic physicsInteracting boson modelNuclear Experiment010306 general physics
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