Title: Isospin Symmetry test on the semimagic 44Cr
1Isospin Symmetry test on the semimagic 44Cr
- Toward the dripline
- in the f7/2 shell
244Cr
- N20, 40Ca 4 protons
- Mid mass, Tz-2
- 36Ca_at_RISING
NZ
3T1 and T2 mirror nuclei
- Shell evolution
- Gaps Z14 and N14
- No cross shell excitations
f7/2
f7/2
N,Z20
N,Z20
d3/2
d3/2
s1/2
s1/2
d5/2
d5/2
p
p
?
?
36S
36Ca
4Cross conjugate nuclei
f7/2
f7/2
N,Z20
N,Z20
d3/2
d3/2
s1/2
s1/2
d5/2
d5/2
p
p
?
?
44Ca
44Cr
f7/2
f7/2
N,Z20
N,Z20
d3/2
d3/2
s1/2
s1/2
d5/2
d5/2
p
p
?
?
36S
36Ca
544Cr
f5/2
f5/2
p1/2
p1/2
p3/2
p3/2
f7/2
f7/2
N,Z20
N,Z20
p
p
?
?
44Cr
44Ca
1360
2
1248
2
1157
2
0
0
0
44Ca
Exp
kb3g
gxpf1a
104
9.8
10.3
B(E2)e2fm4
644Cr
p3/2
p3/2
f7/2
f7/2
N,Z20
N,Z20
d3/2
d3/2
s1/2
s1/2
p
p
?
?
44Cr
44Ca
2
1571
1360
2
1248
2
1157
2
0
0
0
0
44Ca
Exp
kb3g
gxpf1a
sdfp
104
9.8
10.3
105.6
B(E2)e2fm4
7Particle-hole cross-shell excitations
2
1571
1360
2
1248
2
1157
2
0
0
0
0
44Ca
Exp
kb3g
gxpf1a
sdfp
104
9.8
10.3
105.6
B(E2)e2fm4
844Cr
3307
3-
3285
6
Sp 2800 keV (SY)
2283
4
2
1157
0
0
44Ca
44Cr
9f7/2 shell and INC nuclear forces
VCm,
VCM
VB
From the MED we extract information of nuclear
structure properties
- How the nucleus generates its angular momentum
- Evolution of the deformation along a rotational
band - Isospin non-conserving terms in the nuclear
interaction - Learn about the configuration of the states
1036Ca from 40Ca
Fragmentation 40Ca ? 37Ca 38
µbarn Knock-out37Ca ? 36Ca 2 mbarn
1144Cr from 50Cr
Fragmentation 50Cr ? 45Cr 1.5
µbarn Knock-out45Cr ? 44Cr 2 mbarn
1244Cr from 58Ni
Fragmentation 58Ni ? 45Cr 0.6
µbarn Knock-out45Cr ? 44Cr 2 mbarn
13Feasibility fragmentation knock-out
- Comparison to 36Ca
- Cross section /50
- AGATA efficiency x5
- AGATA resolution x2
- Energy of the gamma (3.0? 1.2 MeV) x3
- Beam current x30 (3108?1010)
- 44Cr now is a factor 20 easier!
P. Doornenbal et al. Physics Letters B 647
(2007) 237242
14Feasibility fragmentation coulex
- Directly produced 44Cr 24 nbarn
- More than an order of magnitude lost
- Coulex on secondary target
- 2 predicted collective (2p2h, 4p4h)
- Enhanced B(E2)
- Good excitation cross section (200 mbarn)
- Factor of 10 in statistics for the 2
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18B(E1) in T2
- Janecke
- EC (A,T,TZ) EC0(A,T) - Tz EC1(A,T)
(3Tz2-T(T1))EC2(A,T) - Warburton
- Corresponding E1 transition in conjugate nuclei
have equal strength - T2 Tz-2
- EC EC0 2 EC1(A,2) 6EC2(A,T)
- T2 Tz-1
- EC EC0 1 EC1(A,2) - 3EC2(A,T)
- T2 Tz0
- EC EC0 - 6EC2(A,T)
- T2 Tz1
- EC EC0 1 EC1(A,2) - 3EC2(A,T)
- T2 Tz2
- EC EC0 - 2 EC1(A,2) 6EC2(A,T)
WILKINSON - ISOSPIN IN NUCLEAR PHYSICS