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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne Deformation in N=40 nuclei G. Duchêne, R. Lozeva, C. Beck, D. Curien, F. Didierjean, Ch. Finck, F. Nowacki, K. Sieja IPHC Strasbourg C. Domingo-Pardo, J. Gerl and the GSI group GSI Darmstadt D. Verney, F.Azaiez, S. Franchoo, F. Ibrahim, F. Le Blanc, I. Matea, M. Niikura, I. Stefan IPN Orsay
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne Deformation in Fe and Cr nuclei E. Caurier et al., Eur. Phys. J A15 (2002) 145 Fe Cr
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne 68 Ni Is 68 Ni a magic nucleus ? Increase of the 2 1 + excitation energy Reduction of the B(E2) value No pronounced irregularity in the 2- neutron separation energy Strong 2p-2h component -> excitation of a neutron pair into g 9/2 orbital Major part of the B(E2) strength around 5 MeV Deformation in 68 Ni 68 Ni gs is spherical ( Gaudefroy et al., Phys. Rev. C80 (2009) 064313 ) Main 0 1 + state configuration is 4p-4h Does not generate much deformation K. Langanke et al., Phys. Rev. C67 (2003) 044314
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne In the vicinity of 68 Ni 67 Co Collective 1p-2h proton intruder First excited ½- state with large quadrupole deformation β ~ 0.25-0.4 D. Pauwels et al., Phys. Rev. C 78, 041307(R) (2009) 69 Cu Measured magnetic moment of 13/2+ state Considerable proton excitations across the Z=28 proton gap Deviate from sphericity G. Georgiev et al., J. Phys. G: Nucl. Part. Phys. 28, 2993 (2002) 70 Zn Given as a γ-soft nucleus ( Gaudefroy et al., Phys. Rev. C80 (2009) 064313 ) Hunt for deformation with np-nh configurations (n=6, 8) at higher excitation energy
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne Shell-model calculations Valence space 40 20 Ca 20 core π: f 7/2 + fp shell υ: f 7/2 frozen + fp shell (p 3/2 frozen)+ g 9/2 + d 5/2 68 Ni: 8p-8h excitations 70 Zn: 6p-6h excitations Huge matrices to diagonalise ~(500 10 6 )² to more than (10 9 )² Several days calculation Results 68 Ni 8p-8h config: B(E2) down ~ 690 e²fm 4 Q 2 = -49 e.fm² β 2 ~ 0.32 E* ~ 13 MeV 6p-6h config: B(E2) down ~ 190 e²fm 4 Less deformation driving E* ~ 10 MeV 70 Zn 6p-6h config: B(E2) down ~ 695 e²fm 4 Q 2 = -48 e.fm² β 2 ~ 0.32 E* ~ 10 MeV All configurations are spread over many states when configuration mixing is allowed ! Mean field calculation in the β-γ plan
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne Angular momentum and particle rates High-angular momentum states feeding Several nucleon knock-out lead to « high-spin » transfers 8+ fed ~10 time less than 2+ state Hypothesis: deformed structure feeding of 10% at 8 ħ Nuclei production rate Primary beam: 76 Ge -> I max = 3 10 8 p/s Primary Be/Nb target of 2.5 g/cm² Al degrader of 1.5 g/cm² Intermediate fragments: 73 Ga or 72 Zn Rates calculations (slits cuts in S1, S3, S4) AGATA Lycca 10 5 Hz/wire 10 4 Hz Primary beam (p/s) Intermediate fragment Trans mission S4 rate (p/s) Reaction Final nucleus Production rate (p/s) 7 10 6 p/s 73 31 Ga30%10 4 fragmentation 68 28 Ni0.3 1p-2n knock- out 70 30 Zn18 3 10 7 p/s 72 30 Zn42%10 4 fragmentation 68 28 Ni2.5 2n knock-out 70 30 Zn35
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne Gamma-ray statistics S’2 geometry Full configuration: 10TC + 5DC -> 17% Min. configuration: 5TC + 3DC -> 9% Intermediate fragment 72 Zn; 1.5 MeV gamma ray Experiment duration: 7 days Projectile Nucleus of interest AGATA config. γ - rate (min -1 ) Total counts singles in 7 days γ γ - rate (min -1 ) Total counts doubles in 7 days 72 Zn 68 Ni 2.5 p/s Full0.1919000.024244 Min0.1010000.006869 70 Zn 35 p/s Full2.66266000.343400 Min1.40140000.095950
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne Ni-Zn-Ge Gaudefroy et al., Phys. Rev. C80 (2009) 064313 J. Van de Walle et al., Phys. Rev. Lett.99 (2007) 142501
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AGATA Physics Workshop Istanbul, Turkey May 4-7, 2010 G. Duchêne Tensor force Attractive between spin-flip orbitals Attractive interaction πf5/2-νd5/2 Relaxed when removing protons from πf5/2 orbital Excitation energy of νs1/2 state apparently decreases vs νd5/2 state π ν f 7/2 p 3/2 f 5/2 p 1/2 g 9/2 d 5/2 s 1/2 g 7/2 j+1/2 j-1/2
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