Semi-Inclusive Reactions: N, Z, Nucleon momenta, and Pairing - - PowerPoint PPT Presentation
Semi-Inclusive Reactions: N, Z, Nucleon momenta, and Pairing - - PowerPoint PPT Presentation
Semi-Inclusive Reactions: N, Z, Nucleon momenta, and Pairing Lawrence Weinstein Old Dominion University N, Z and high momentum nucleons: 54-40 or Fight aka The CaFe Experiment Goal: understand pairing mechanisms in symmetric and
N, Z and high momentum nucleons:
“54-40 or Fight” aka “The CaFe Experiment”
- Goal: understand pairing mechanisms in symmetric and
asymmetric nuclei
– Neutron skins – Connection to EMC effect
- Method: Measure A(e,e’p) at low and hi missing momentum
at kinematics sensitive to n(k)
- Targets: D, 12C, 40Ca, 48Ca, 54Fe
– Add p, n symmetrically from D to 12C to 40Ca – Add 8 neutrons from 40Ca to 48Ca – Add 6 protons from 48Ca to 54Fe
- L. Weinstein, EMC SRC MIT 2016
2
N, Z and high momentum nucleons:
“54-40 or Fight” aka “The CaFe Experiment”
- Goal: understand pairing mechanisms in symmetric and
asymmetric nuclei
– Neutron skins – Connection to EMC effect
- Method: Measure A(e,e’p) at low and hi missing momentum
at kinematics sensitive to n(k)
- Targets: D, 12C, 40Ca, 48Ca, 54Fe
– Add p, n symmetrically from D to 12C to 40Ca – Add 8 neutrons from 40Ca to 48Ca – Add 6 protons from 48Ca to 54Fe
- L. Weinstein, EMC SRC MIT 2016
3
40Ca 54Fe
48Ca
- 8 Neutrons
+ 6 Protons
Adding neutrons to 40Ca
Two models:
- More neutrons, similar volume larger pn
- More neutrons, more np pairs larger pp
- L. Weinstein, EMC SRC MIT 2016
4
No Correlations With Correlations
48Ca
+8%
- 12%
40Ca
- M. Vanhalst, et al., J. Phys. G 42, 055104 (2015)
Adding neutrons to 40Ca
Two models:
- More neutrons, similar volume larger pn
- More neutrons, more np pairs larger pp
- L. Weinstein, EMC SRC MIT 2016
5
0.00E+00 2.00E-01 4.00E-01 6.00E-01 8.00E-01 1.00E+00 1.20E+00
0.00E+00 2.00E-01 4.00E-01 6.00E-01 8.00E-01 1.00E+00 1.20E+00 1.40E+00 1.60E+00 1.80E+00 2.00E+00
Integrated momentum density
sum p sum n
2.0 1.0 0.0 0.5 1.5
neutrons protons Larger pn
Hagen et al, Nature Phys 12, p186 (2015)
N2LO saturation
Focusing on 48Ca
0.15 – 0.3 fm
Coordinate space:
[CREX]
Momentum space:
[CaFe]
Adding correlations:
- Reduce the radius.
- Inverts the momentum
skin?
- M. Vanhalst, et al., J. Phys. G 42, 055104 (2015)
Neutron Proton No SRC + np-SRC + nn-SRC Neutron Proton Neutron Proton
- L. Weinstein, EMC SRC MIT 2016
6
Focusing on 48Ca
0.15 – 0.3 fm
Coordinate space:
[CREX]
Momentum space:
[CaFe]
Adding correlations:
- Reduce the radius.
- Inverts the momentum
skin?
- M. Vanhalst, et al., J. Phys. G 42, 055104 (2015)
Neutron Proton No SRC + np-SRC + nn-SRC Neutron Proton Neutron Proton
16
Depends on pairing mechanisms in asymmetric nuclei!
7
8
40Ca 48Ca 54Fe
48Ca has a
40% neutron excess!!
The CaFe Triplet: A Lab for Asymmetric Nuclei
- L. Weinstein, EMC SRC MIT 2016
Nucleus Z N
40Ca
20 20 Symmetric double magic
48Ca
20 28 + Full neutron shell (1f7/2)
54Fe
26 28 Almost symmetric double magic
How do the neutrons from the
- uter 1f7/2 shell correlate with
the 40Ca core?
The CaFe Triplet: A Lab for Asymmetric Nuclei
24
- L. Weinstein, EMC SRC MIT 2016
9
10
What do we already know?
(e,e’) cross-section ratios at xB>1 are sensitive to the TOTAL NUMBER OF SRC PAIRS:
=> 48Ca: + 20% nucleons, +20% SRC pairs!
- Z. Ye Ph.D. Thesis, UVA. arXiv: 1408.5861
1.44 1.2
0.96
- Z. Ye, JLab Users Group Meeting Talk (2016)
~5% norm uncertainty not shown
- Z. Ye Ph.D. Thesis, UVA. arXiv: 1408.5861
- Z. Ye, JLab Users Group Meeting Talk (2016)
1.44 1.2 0.96
What do we already know?
The neutrons in the outer 1f7/2 shell (i.e. in the skin) are equally correlated as the nucleons in the 40Ca core!
(e,e’) cross-section ratios at xB>1 are sensitive to the TOTAL NUMBER OF SRC PAIRS:
Due to the extra 8 neutrons
26
11
- Z. Ye Ph.D. Thesis, UVA. arXiv: 1408.5861
- Z. Ye, JLab Users Group Meeting Talk (2016)
1.4 1.2 1.0
What do we already know?
The neutrons in the outer 1f7/2 shell (i.e. in the skin) are equally correlated as the nucleons in the 40Ca core!
(e,e’) cross-section ratios at xB>1 are sensitive to the TOTAL NUMBER OF SRC PAIRS:
Due to the extra 8 neutrons
The crust neutrons form MANY SRC pairs!
[What types? What’s their impact?]
27
12
13
Cross section factorizes (in PWIA):
detect the proton (e,e’p)
- L. Weinstein, EMC SRC MIT 2016
dσ dEedΩedTpdΩ p = KS( ! pmiss,Emiss) dσ free dΩ
Emiss = ν −Tp −TA−1 ! pmiss = ! q − ! pp = − ! pinitial Complications:
- Rescattering of the outgoing proton.
- Off-shell proton cross-section.
- Meson Exchange Currents (MEC).
- Delta production (i.e. IC).
=> Spectral function is not an observable! Compare cross sections for high (SRC) and low (MF) missing momentum protons in various nuclei
S D( ! pmiss,Emiss) = dσ dEedΩedTpdΩ p
/ K dσ free
dΩ
Minimizing FSI
- L. Weinstein, EMC SRC MIT 2016
14
Pmiss (GeV/c) θnq= 35o θnq= 75o
PWIA Full 0.1 0.1 0.5 0.5 R = σFull / σPWIA
200 MeV/c
400 MeV/c 500 MeV/c
3He e,e' p
( )
θrq
20 40 100 120 60 80
d(e,e’p)
Boeglin et al., PRL 107 (2011) 262501
Sargsian Full = PWIA + FSI Θrq = angle between q and recoil
Avoid rescaaering peak at θrq ≈ 70o
Optimizing (e,e’p) kinematics
- L. Weinstein, EMC SRC MIT 2016
15
- Ebeam = 11 GeV @ 40 uA to maximize rates.
- 1H, 2H, 12C, 40Ca, 48Ca, and 54Fe targets.
- Q2 ≈ 3.5 GeV2
– Reduces non-nucleonic currents (MEC, IC). – Proton energies high enough for Glauber FSI calculahons.
- xB = Q2/2mω > 1.2 to minimize non-nucleonic currents.
- θrq < 50o to minimize FSI.
- Two Kinemahcs:
– 350 < pmiss < 600 MeV/c (“SRC”) – pmiss < 250 MeV/c (“Mean-Field”)
“Observables”
- Distorted spectral funchons (i.e., reduced σ)
– Need theory support to interpret
- Double rahos of
– extra SRC p from A1 to A2
- e.g.: from 40 to 48Ca np pairs created by 8 more n
– Reduced transparency (FSI) correchons – Compare symmetric and asymmetric nuclei
- 40 and 48Ca; 6 and 7Li
- d, C, Ca, Fe
- L. Weinstein, EMC SRC MIT 2016
16