jlab hypernuclear workshop 27 th may 2014
DESCRIPTION
Perspectives at Jefferson Lab Medium mass hypernuclei. HKS. HES. JLab Hypernuclear Workshop 27 th May 2014. Satoshi N Nakamura, Tohoku University. L in nuclear medium. Study of hypernuclei. Single particle nature of L in nuclear medium A dependence of L potential - PowerPoint PPT PresentationTRANSCRIPT
JLab Hypernuclear Workshop27th May 2014
Satoshi N Nakamura, Tohoku University
Perspectives at Jefferson LabMedium mass hypernuclei
HKSHES
Study of hypernuclei
High quality medium heavy hypernuclear spectroscopy
Single particle nature of L in nuclear mediumA dependence of L potential
ls force vs. core-config. MixingInputs for mean-field theories
Collective motion of core nucleus
Tri-axial deformation of core nucleus
Modify nature of core Energy level inversion Glue like role of L
L in nuclear medium
L as an impurityL as a probe
Objectives --- Hypernuclear Physics
Medium - Heavy hypernuclei
Light Hypernuclei (s,p shell)
A 1 20 50 200 1057
Elementary ProcessStrangeness electro-production
CSB, LS coupling in large isospin hypernuclei
Hyperonization Softening of EOS ?
Single-particle potentialDistinguishability of a L hyperon
U0(r), mL*(r), VLNN, ...
Neutron/Hyperon star,Strangeness matter
Extend Nuclear Force to Baryon Interaction
Use L as a probe to see deep inside of nucleus
Medium Heavy
Hypernuclei
Precise spectroscopy of HYSingle Particle Model is OK to some extent
Hadron keeps its identities
Baryon Constitute Quark Model
HypernucleiSingle Particle Model
Precise spectroscopy of HY
NucleonValence quarks
QCD vacuumSea quarks, gluons
HypernucleiLambda particle
Nuclear mediumCore’s properties, density
Light HypernucleiBaryon InteractionModification of core
Heavy Hypernuclei Lambda’s behavior in nucleus
Proposed Programs1. Elementary L, S0
Reliable data 1H(e,e’K+)L, S0 in low Q2
2. Few-body 2D(e,e’K+) [LN] Exotic bound state, LN int. 4He(e,e’K+)4
LH LN CSB 3. Medium-heavy
40,44,48Ca(e,e’K+) 40,44,48LK L’s S.E., iso-spin
27Al(e,e’K+) 27LMg Tri-axial deformation
48Ti(e,e’K+) 48LSc Level inv. due to L
4. Heavy208Pb(e,e’K+) 208
LTl L in heaviest nucleus 5. Decay p
Weak decay of light hyper-fragments
6,7Li(e,e’K)6LHe, 7
LHe
3t(e,e’K)[nnL]19F(e,e’K)19
LO
Hypernuclear Chart
K40L K44
L K48L
K40L
[LN]
L
Tl208L
H4L
MgL27
B12L
OL19
1. Ca (e,e’K+) LK
Missing in (e,e’K) dataComplete A dependence of L S.P.Energy
Doubly LS closed 40Ca target
Clean Spectrum
isotope effect of core nuclei: 40Ca, 44Ca , 48Ca targets
P.Bydzovsky et al. NPA881 (2012)199.
2. 27Al (e,e’K+) 27LMg
Tri-axially deformed 26Mg core + L in p-shell
9LBe = a + a + L
Genuine hypernuclear state
Totally new method to search shape of nucleus with L!
M.Isaka Yesterday’s talk
3. 19F target : simplest sd-shell
A’s: p1/2-hole series, B’s: p3/2-hole series
T. Motoba, C2C WS Barcelona (2012)
Study of core-dynamics
Measured hypernuclei & expected A dependence
E05-115L40K
L27Mg
89Y139La 208Pb
L19O
InteractionCharacteristics of Core
L in medium
Few-body physics with strangeness1. 6Li (e,e’K+) 6
LHe
α
Λ
n
r.m.s α-Λ 2.8 fm α-n 5.0 fm
Larger than 6He
Three-layer structure
E.Hiyama : Yesterday’s talk
2. 7Li (e,e’K+) 7LHe
0+
2+
α+n+n0 MeV
6He
-0.98
1.797 MeV
Γ=113 ±20 keV
(2+,1-,0+)?
Γ= 12.1 ±1.1 MeV
Exp.1/2+
3/2+5/2+
5He+n+nΛ
α+Λ+n+n0 MeV
-6.19 MeV
-4.57
neutronhalo states
-3.12
-1.88 Γ=0.7 MeV5/2+
3/2+ -2.04, Γ=0.5 MeV
7HeΛ
2+
Λ
E.Hiyama : Yesterday’s talk
Few-body physics with strangeness
Established lightest hypernyclei = 3LH
Hyp-HI experiment at GSI a structure in d + p- , t + p- invariant mass
T.R.Saito, NUFRA2011
2d(e,e’K+)[nL]Indication of a nL , nnL bound state ?
3. Search of [nL] bound state and study of n-L interaction through FSI.
Direct method to search or set upper limit on this exotic system.
3t(e,e’K+)[nnL]
C.R
appo
ld e
t al.
PR
C88
, 041
001(
R) (
2013
)
Few-body physics with strangeness
2d(e,e’K+) nL
2. Study of n-L interaction through FSI.
2d(e,e’K+) provides also information of n-L interaction through FSI.
R.A.Adelseck & L.E.wrightPRC 39(1989) 580.
Few-body physics with strangeness4. Charge Symmetry Breaking of LN interaction
A=4,iso-doublet hypernuclei
A=7,iso-triplet hypernuclei
JLab E01-011 (HKS)
Recently measured at JLab Hall-C
Phenomenological CSB potential
Introduced to explain A=4.
NOT becessary for A=7.
Re-check of A=4 system
Decay p
4He(e,e’K+) 4LH
E13 @ J-PARC
SummaryMedium heavy hypernuclear study
Ca targets : 40Ca doubly closed, clean, 44Ca 27Al target : 27
LMg tri-axial deformed19F targets: simplest sd-target, excited-core
Other targets : SPE of L with <100 keV accuracy
Few-body hypernuclear study6Li target : 6
LHe n-halo hypernucleus7Li target : 7
LHe unbound states of 6He d target : Exotic nL state, FSI nL study
CTn target : Exotic nnL state
Subtraction of 12C effects and Accidental BG
Expected Yields
>5 times more yield than E94-107Much better S/N than E05-115
Expected Mass Resolution
Calibration for independent K, e’ spectrometers.Established in E94-107.
Absolute missing mass calibration with L,S0 massesEstablished in E05-115.