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Collaboration LPC-CHARISSA-DEMON H Al Falou, FM Marqués, JL Lecouey, NA Orr, … Spectroscopy Beyond the Neutron Dripline: 9 He & 10 Li
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“ I have come 500 miles just to see a halo … ” Who wrote and sang …
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MotivationExperimentalApproach Selection “Rules” Backgrounds N=7 : 10 Li & 9 He N=7 : 10 Li & 9 He Conclusions Conclusions Spectroscopy Beyond the Neutron Dripline: 9 He & 10 Li
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The Light Neutron-Rich Nuclei … 10 Li Structure =core+xn … driplines and beyond experimentally accessible, extreme test of models (shell model, shell model in continuum, “ab initio”, cluster, etc) 9 He
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Light Unbound Neutron-Rich Systems input for 3-body models input for 3-body models 3-body systems n-n and core-n interactions 11 Li : 9 Li-n interaction spectroscopy of 10 Li 10 He : 8 He-n interaction spectroscopy of 9 He
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N=7 1/2 + – 1/2 - Level Inversion … PG Hansen et al. PG Hansen et al. … 10 Li & 9 He ??
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Experimental Approach … “knockout” or breakup + inflight decay projectile structure known VfVf VnVn V f -V n target Proj. A Z A-1 Z + n
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DEMON 90 modules ( NE213 ) ToF & position n ~ 10% Kinematically “Complete” Measurement
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Resolution Experimental Response Function Efficiency FWHM ~ 0.3 E d 1/2 nnnn JL Lecouey LPCC 04-03 JL Lecouey LPCC 04-03 model distributions must be “ filtered ” through the simulation model distributions must be “ filtered ” through the simulation
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Selection “Rules” - Sudden Approximation (i) 1 & 2-proton knockout l n =0 proj. valence neutron config. C( 11 Be, 10 Li)X,C( 11 Be, 9 He)X s 1/2 [ 11 Be C 2 S ( s 1/2 ) 0.8 ] (ii) fragmentation (-xp,-xn) valence neutron config. + others C( 14 B, 10 Li)X, C( 14 B, 9 He)X s 1/2 + p 1/2 + … C( 12 Be, 9 He)X s 1/2 + p 1/2 + d 5/2 + … NB: E d lineshape dependent on initial state (esp. for broad final states)
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“background” ≡ non-resonant continuum event-mixed distribution * * ie., uncorrelated fragment-neutron pairs E r = 85 15 keV sp << 100 keV uncorrelated 15 B+n distribution BACKGROUND : C( 17 C, 15 B+n)X – single-proton knockout JL Lecouey et al, nucl-ex/0802.4225 JL Lecouey et al, nucl-ex/0802.4225
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“background” ≡ neutrons evaporated from PLF + continuum BACKGROUND : C( 14 B, 6 He+n)X – fragmentation JL Lecouey, LPCC T 04-03. JL Lecouey, LPCC T 04-03.
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Scattering/Virtual s-wave States a s = 0 fm no FSI ; a s << 0 fm stronger FSI
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10 Li : Low-Lying Level Scheme * * “ Partial ” – also d( 9 Li,p) etc s- virtual E r ~ ћ 2 / 2a s
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10 Li : C( 11 Be, 9 Li+n) @ 35 MeV/nucleon H Al Falou LPCC 07-03 uncorrelated / event-mixed distribution * * normalised for comparison at high E d
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10 Li : C( 11 Be, 9 Li+n) @ 35 MeV/nucleon s-wave [a s = -14±2 fm] + non-resonant continuum H Al Falou LPCC 07-03
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10 Li : C( 14 B, 9 Li+n) @ 35 MeV/nucleon s-wave virtual state + p-wave [E r = 0.51, = 0.50 MeV] + background H Al Falou LPCC 07-03
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9 He : Low-Lying Level Scheme * * 9 Li IAS expts not shown ; [Set87, Boh88, Oer95] assignments tentative
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9 He : C( 11 Be, 8 He+n) @ 35 MeV/nucleon uncorrelated distribution/event mixed distribution H Al Falou LPCC 07-03
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9 He : C( 11 Be, 8 He+n) @ 35 MeV/nucleon s-wave [a s = -3 ~ 0 fm (3 )] + non-resonant continuum H Al Falou LPCC 07-03
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9 He : C( 14 B, 8 He+n) @ 35 MeV/nucleon uncorrelated distribution/event mixed distribution H Al Falou LPCC 07-03
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9 He : C( 14 B, 8 He+n) @ 35 MeV/nucleon s-wave [a s = -3 ~ 0 fm] + p-wave [E r = 1.2, = 1.0 MeV] + background H Al Falou LPCC 07-03
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9 He : C( 12 Be, 8 He+n) @ 41 MeV/nucleon s-wave [a s = -10 fm] + p 1/2 [E r = 1.2 MeV] + (d 5/2 ) [E r = 2.4 MeV] + background G Normand LPCC 04-03
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Conclusions & Perspectives spectroscopy beyond the dripline using breakup/knockout of RNB … 10 Li : low-lying s-wave strength (a s = -14±2 fm) low-lying p-wave resonance (E r = 0.5 MeV) N= 7 inversion confirmed [ but … p 3/2 s 1/2, p 1/2, d 5/2 ] 9 He : low-lying s-wave strength (a s 0 fm) + E x 1.2 & 2.4 MeV (l>0) N= 7 inversion … ?? [ FSI 0) N= 7 inversion … ?? [ FSI << 9 Li+n ?? ] validity of s-wave virtual states (eg., deformed 9 Li core) ?? more realistic structure + reaction modelling needed … … including non-resonant continuum + other backgrounds
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