27 June 2022 to 1 July 2022
Prague, Czech Republic
Europe/Zurich timezone

Session

4; Thu-IIb

30 Jun 2022, 11:00
Prague, Czech Republic

Prague, Czech Republic

Prague, Czech Republic

Conveners

4; Thu-IIb

  • Petr Bydzovsky (Nuclear Physics Institute AS CR)

Presentation materials

There are no materials yet.

  1. Dr Atsushi Umeya (Nippon Institute of Technology)
    30/06/2022, 11:00
    online talk

    The $(e, e'K^+)$ reaction experiments with several nuclear targets performed recently at the Jefferson Lab have provided high-resolution spectroscopic data. They are very fruitful in disclosing hypernuclear structure details and also in understanding hyperon-nucleon fundamental interaction properties.

    Among others, the $^{10}$B $(e, e'K^+)$ $_{\,\Lambda}^{10}$Be reaction data are quite...

    Go to contribution page
  2. Hiroyuki Fujioka (Tokyo Institute of Technology)
    30/06/2022, 11:15
    online talk

    Intense $K^-$ beam at J-PARC will enable us to investigate strangeness $-2$ systems, namely $\Xi$-hypernuclei and double-$\Lambda$ hypernuclei. In particular, the high-resolution S-2S spectromter will be a key ingredient for a systematic study of these systems by means of $(K^-,K^+)$ reactions.

    The J-PARC E75 experiment plans to produce $^5_{\Lambda\Lambda}{\mathrm{H}}$ as a decay product...

    Go to contribution page
  3. Takuya Nanamura (Kyoto University and JAEA)
    30/06/2022, 11:30
    online talk

    Hyperon-proton scattering experiment is one of the most direct methods to study the $YN$ interaction, as in the case of the $NN$ interaction. Although it was experimentally difficult due to short lifetime of hyperons for a long time, we successfully performed novel high-statistics $\Sigma p$ scattering experiment at J-PARC (J-PARC E40 experiment). One of the physics motivations was...

    Go to contribution page
  4. Yudai Ichikawa (JAEA)
    30/06/2022, 11:45
    online talk

    Recently, we have proposed a new experiment (J-PARC P90 experiment) to measure the missing-mass spectrum around the $\Sigma N$ threshold in the $d(K^-, \pi^-)$ reaction at 1.4 GeV/$c$. A clear enhancement was observed near the $\Sigma N$ threshold, so called "$\Sigma N$ cusp", for a long time ago. However, the dynamical origin of this enhancement remains unclear as yet. Especially, whether...

    Go to contribution page
  5. Atsushi Tokiyasu
    30/06/2022, 12:00
    online talk

    The $\Xi$particle-nucleon interaction is the last piece of the nuclear force study that has been extended to the strange quark, and the $\Xi$ hypernuclear spectroscopy experiment will provide us the rich information. We are planning a series of $\Xi$ hypernuclear spectroscopy experiments using $(K^-, K^+)$ reactions at the Japan Proton Accelerator Re-search Complex (J-PARC), K1.8...

    Go to contribution page
  6. Dalibor Skoupil (Nuclear Physics Institute CAS, Rez)
    30/06/2022, 12:15
    talk

    We have used an isobar model to study the $K^+\Sigma^-$ photoproduction reaction on a neutron target with focus on the resonance region. In order to achieve a reasonable agreement with the data, we included spin-3/2 and spin-5/2 nucleon resonances in the consistent formalism [1,2], where spurious lower-spin modes vanish in the amplitude, together with a $\Delta$ resonance and two kaon...

    Go to contribution page
  7. Dr Franco Garibaldi (INFN Roma1)
    30/06/2022, 12:30
    talk

    The recent observation of two-solar-mass neutron stars rules out most of the current models of hyperonic matter equation of state, which favour the appearance of hyperons in the neutron star interior but predict maximum masses (Mmax) incompatible with data. This issue, referred to as “hyperon puzzle”, strongly suggests that the present understanding of nuclear interactions involving hyperons...

    Go to contribution page
Building timetable...