1 / 17

g -ray spectroscopy of the sd -shell hypernuclei

g -ray spectroscopy of the sd -shell hypernuclei. Graduate school of Science, Tohoku University T. Koike Hyperball-J collaboration. Survey of sd-shell hypernuclear cores g -ray spectroscopy of well deformed hypernuclei 25 L Mg Summary. E13. Z=20.

satin
Télécharger la présentation

g -ray spectroscopy of the sd -shell hypernuclei

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. g-ray spectroscopy of the sd-shell hypernuclei Graduate school of Science, Tohoku University T. Koike Hyperball-J collaboration • Survey of sd-shell hypernuclear cores • g-ray spectroscopy of well deformed hypernuclei • 25LMg • Summary

  2. E13 Z=20 Possible sd-shell L hypernuclei via g-ray spectroscopy with (K-,p-) & (p+,K+) reactions 39Ca 40Ca 38K 39K 38Ar 39Ar 40Ar 37Cl 34Cl 35Cl 36Cl 39Cl 31S 34S 36S 32S Z 30P 31P 28Si 30Si 27Si 26Al 27Al Most abundant isotopes (target) 26Mg 23Mg 24Mg 25Mg ~10% abundance 23Na 24Na 25Na 22Na proton decay 20Ne 22Ne 19Ne 21Ne neutron decay 18F 19F 21F N Z=9

  3. Bound states of sd-shell nuclei and hypernuclei • Co-existence of shell (mean field) and cluster-like structures • More valence nucleons • higher level densities (especially odd-odd) • Collective (rotational) excitation spectrum → low-lying energy • pLstates also bound • Shell model • Cluster model • Self-consistent calculations (12/4 Hagino) • RMF • Hatree-Fcok+BCS • AMD (12/4 Kimura) D. J. Millener et al., Phys. Rev. C, 38 2700 (1988)

  4. Bn Bp Ex(pL) Target A -1ZXn-1

  5. 28LSi dL pL sL A-1LZ-1 g SKSMinus? A-1LZ g-g coincidence with Hyperball-J (p+,K+) T.Hasegawa et al., Phys. Rev. C 53, 1210 (1996) g g ALZ Weak decay (mostly via non-mesonic in the sd-shell hypernuclei)

  6. even-even mirror E13 Z=20 Possible sd-shell L hypernuclei via g-ray spectroscopy with (K-,p-) & (p+,K+) reactions 39Ca 40Ca 38K 39K 38Ar 39Ar 40Ar 37Cl 34Cl 35Cl 36Cl 39Cl 31S 34S 36S 32S Z 30P 31P 28Si 30Si 27Si 26Al 27Al Most abundant isotopes (target) 26Mg 23Mg 24Mg 25Mg ~10% abundance 23Na 24Na 25Na 22Na proton decay 20Ne 22Ne 19Ne 21Ne neutron decay 18F 19F 21F N Z=9

  7. Non collective oblate (b, g=60°) triaxial g spherical b Collective prolate (0,0) (b, g=0°)

  8. Skyrme Hartree-Fock +BCS Myaing Thi Win et al., submitted to PRC • self-consistent mean field • Skyrme-type LN interaction • PES of L hypernuclei with triaxial deformation: E(b,g) • Angular momentum not good quantum number 24Mg, 24Mg+L +L

  9. 42+ E(41+)/E(21+) 31+ 43+ 22+ 23+ g-band 02+ b-band Spectra of a deformed even-even nucleus (collective excitation mode) 41+ g 21+ vibrational v.s. rotational 0+ K=0, nb=1, ng=0 b2, J K=2, nb=0, ng=1 K=0, nb=0, ng=0

  10. 18(▲) ,20Ne 22(▲) ,24Mg 30S 38Ar 38Ca 26Si 21+, 22+, and 02+

  11. Rotational 24Mg 38Ca 20Ne 26Si 38Ar 22Mg Vibrational 18Ne Rotational v.s. Vibrational

  12. g-ray spectroscopy of 25LMg • Well deformed & even-even core hypernuclei • low and simple (regular) energy level • direct observation of core polarization effect of L • Nuclear density saturation at the g.s. with little change in size, but a shape can change in (b,g) plane • A few 100 keV change • Observation of spin averaged 21+, 22+, 02+→(b,g) • Observation of 41+ • pL-bound-states particle stable (Bp=11693keV Bn=16532 keV) • Observation of pL splitting in the sd-shell • Hyperball-J with LaBr, CsI detectors (?) • Use of a natural target • possibility of increasing the number of accessible hypernuclei • a test case for heavier hypernucley beyond sd-shell

  13. 24Mg level scheme pL pL pL T=0 T=0 12C 13LC 24Mg 25LMg

  14. Use of a natural Mg target even-even odd-A odd-odd

  15. Mg even-even core: 22,24Mg T=0 T=0 2212Mg10(2) 2412Mg12(4)

  16. 26LMg 25LMg 24LMg 23LMg 11% 10% 79% 23LNa 24LNa Use of natural Mg target and identification of six L hypernuclei (1) Natural Mg (2) 27Al (3) 23Na sL, dL sL ,pL sL dL 27Al(K-,p-) → p+26LMg (pL gate) ←dL 23Na(K-,p-)→23LNa (sL gate)

  17. Summary • The sd-shell region more vast than the p-shell • Importance of coupling of L to nuclear collectivity (non-spherical vacuum) in the sd-shell • Core polarization effect of L in the 2D (b,g) plane • Measurement oftheinter shell (pL→sL) g ray • g-ray spectroscopy of 25LMg with a use of natural target (Hyperball-J, SKSMinus, LaBr3/CsI detectors?) • Essential role of g-g coincidence technique in the sd-shell

More Related