PPT-Mass measurements on very neutron-rich isotopes with a new Penning trap phase detection

Author : olivia-moreira | Published Date : 2019-12-09

Mass measurements on very neutronrich isotopes with a new Penning trap phase detection technique Guy Savard Argonne National Laboratory amp University of Chicago

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Mass measurements on very neutron-rich isotopes with a new Penning trap phase detection: Transcript


Mass measurements on very neutronrich isotopes with a new Penning trap phase detection technique Guy Savard Argonne National Laboratory amp University of Chicago Nuclear Structure 2016 Knoxville Tennessee July 2529 2016. Wolfram KORTEN. CEA . Saclay. DSM/IRFU/. SPhN. Shapes and shells in exotic nuclei. Prolate. Oblate. Quadrupole . deformation. . of. the nuclear ground states. M. Girod, CEA Bruy. ères-le-Châtel. Dominance of . Visit our Exhibitors:. Special Canberra demonstration during poster session Tuesday evening. Session M1. Session M1 (Chair: . Petr. . Navrátil. ).  . 08:45 Jonathan Bagger, . Director of . TRIUMF. . mass. . measurements. of . n-rich. . nuclei. . between. N=50 and 82.. Short overview on the experimental approach. Penning trap mass measurements on n-rich nuclei. Impact of improved knowledge of masses. Tommi Eronen. Max-Planck-Institut für Kernphysik. Heidelberg, Germany. Outline. Penning trap mass spectrometry. Q. = . m. parent. – . m. daughter. . Masses for CKM unitarity tests.... Superallowed beta decay. Stars: . Insights . into their Formation. , Evolution & . Structure from their. Masses and Radii. Feryal Ozel. University of Arizona. In collaboration with T. . Guver. , M. . Baubock. , L. . Camarota. AME2003, G. Audi et al., Nucl. Phys. A 729 (2003) 3Accuracyrequiredfor fundamentalphysicsMassaccuracy obsionTRNRcmm X c qBc AND FFT Contents. Breakup reactions. of . 14. Be on a proton target. Inelastic scattering (. 14. Be). One-neutron removal reaction (. 13. Be). Y. Kondo. RIKEN . Nishina. Center. 2. Collaborators. Y. Kondo. Farrukh. J. . Fattoyev. My TAMUC collaborators: . B.-A. Li, W. G. Newton . My outside collaborators: . C. J. Horowitz, J. . Piekarewicz. , G. . Shen. , J. . Xu. Texas A&M University-Commerce. International Workshop on Nuclear Dynamics and Thermodynamics. 2015. D. Lascar | Postdoctoral Fellow | TRIUMF. How do you relate time to mass?. How do you trap ions?. What is going on in a Penning trap?. Time of Flight conversion. Outline. Oct 9, 2015. SFU Nuclear Chemistry - Mass 2. III. How atoms differ. . A. Atomic Number. Equal to the number of protons – never changes; equals the number of electrons if AND ONLY IF the atom is . neutral. ; Moseley discovered . each atom has a unique number of protons in the nucleus. fMass MeasurementsConclusions and Future WorkAcknowledgementsMass Measurements ofNa and Beamline Upgrades to TAMUTRAP FacilityMartin A Fisher School of Physics Brandeis University Waltham MaCyclotron M. Scott Dewey. National Institute of Standards and Technology. Workshop on Next Generation Neutron Lifetime Measurements in the U.S.. How to Measure . τ. n. … .  . “Bottle” Experiments:. Direct Observation of Exponential Decay:. in neutron . star mergers through . mass measurements . with . the CPT. July 16-27. , . 2018. Jason . clark. FRIB and the GW170817 . kilonova. outline. 2. Role of mass measurements in r-process calculations. Alexander Saunders. Los Alamos National Lab. LA-UR-14-26812. 2. Outline. Why study weak interactions via the neutron beta decay lifetime?. Because of the scientific reach. Because of the impact across nuclear and particle physics.

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