Jul 21 – 26, 2024
APS Conference Center, Argonne
America/Chicago timezone
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Session

Instrumentation and Techniques

Jul 23, 2024, 10:55 AM
Auditorium (APS Conference Center, Argonne)

Auditorium

APS Conference Center, Argonne

Conveners

Instrumentation and Techniques

  • Yassid Ayyad (University of Santiago de Compostela)

Presentation materials

There are no materials yet.

  1. Daniel Bazin (Facility for Rare Isotope Beams)
    7/23/24, 10:55 AM

    The Active Target Time Projection Chamber (AT-TPC) has been used in experiments aimed at the exploration of structural effects in radioactive nuclei using one step reactions such as transfer or elastic and inelastic scattering. When used as a solenoidal spectrometer by placing it inside a magnetic field, the AT-TPC allows to perform this type of measurement in inverse kinematics with much...

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  2. Fredrik Gustafsson (CERN)
    7/23/24, 11:20 AM

    At CERN's antimatter factory, antiprotons are routinely produced and cooled in bunches utilizing the ELENA/AD decelerators. The low energy antiprotons are distributed to a wide range of trapping experiments primarily aiming at precision tests of fundamental symmetries and interactions [1]. The Antimatter Experiment: Gravity, Interferometry, Spectroscopy (AEGIS) at the antimatter factory has...

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  3. Ian Cox (University of Tennessee, Knoxville)
    7/23/24, 11:40 AM

    Nucleon-nucleon correlaRons lead to changes in shell structure, such as the islands of inversion. The N=28 shell gap has been frequently probed in nuclei south of 48Ca, finding that intruder configuraRons, which correspond to neutron excitaRons across the gap, play an important role in those neutron-rich isotopes at low energy. The locaRon of the states is related to the neutron shell...

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  4. Jin Wu (Brookhaven National Laboratory)
    7/23/24, 12:00 PM

    An abrupt shape change from spherical to deformed ground states has been observed between 98Zr (N = 58) and 100Zr (N = 60) [1]. Monte Carlo shell model (MCSM) cal- culations suggest that the rapid change in the relative excitation energy of spherical and prolate structures fulfills the requirements of a first-order phase transition, and predict an excitation energy of the 0+4 spherical state...

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