hypernuclear physics with electromagnetic and hadronic ... · radhey shyam, saha institute of...
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Hypernuclear Physics with Electromagnetic andhadronic Probes
Radhey Shyam, Saha Institute of Nuclear Physics, Kolkata, India
1. Introduction
A brief review and comparison of production reactions
2. Brief sketch of the theoretical model
3. Results, cross sections, spectroscopy
4. Conclusions
Seminar at Jlab, Oct. 27, 2008
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Hypernuclei are systems where one nucleon is replaced by a hyperon
Hypernuclei
Z is a bound state of Z protons (A-Z-1) neutrons and a hyperon
Number of
Baryons
(N+Z+Y)
Element=
Total chargeYXB
Number ofhyperons
Double Hypernuclei, Be, Hypernuclei10
A
Λ
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Good probe for deeply bound single particle states.
Hyperons are free from Pauli principle restrictions
Can occupy quantum states already filled up with nucleons
Y89
New type of nuclear matter, new symmetries, New selection rules. First kind of flavored nuclei.
Why are Hypernuclei interesting!
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Production of Hypernuclei
(+, K+) reaction
MESONIC PROBES
(K-, - ) reaction
Associated strangeness production
Strangeness exchange
Prog. Part. Nucl. Phys. 57, 564 (2006)
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Electromagnetic and baryonic Probes
(,K+) reaction + p + K+
(e,e’ K+) reaction * + p + K+
(p,K+) reaction p + p p + + K+
Heavy Ion reactions p + p p + + K+
H. Yamazaki et al., Phys. Rev. C 52, R1157 (1995)
L. Yuan et al. Phys. Rev. C 73, 044607 (2006)M. Iodice et al, Phys. Rev. Lett. 99, 052501 (2007)F. Cusanno et al., arXiv: 0810:3853
GSI
JLab
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Low momentum transfer
Momentum transfer > pF
(K-,-) reaction
(+,K+) and (,K+) reactions
(p,K+) reaction
Large Momentum transfers
12C KINEMATICS
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Excitation Energy Spectra
(K–,–) substitutional 0+ state dominates
(+,K+) nonsubstitutional 1– and 2+ states dominate
(,K+) unnatural parity states dominate
GS: (p3/2-1,s1/2
Λ ) 1–,2– (p3/2-1,p3/2
Λ ) 11+,21
+,3+ (p3/2-1,p1/2
Λ ) 12
+,22+
(,K+) and (e,e’K+) reactions can also excite unnatural parity stretched states
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Production processes for various reactions
Target emission Projectile emissionA (p,K+)B
A (+,K+)B* A (,K+)B′
N * (1650), N*(1710), N*(1720) baryonic resonances.
+
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A Covarient Description of A(h,K+)B reaction
Effective Lagrangians at various vertices
Bound state nucleon and hyperon spinors
Initial and final state interactions (distorted waves).
Medium modification of N* (also of intermediate mesons in proton induced reactions) self energies.
Coupling constants, form-factors
All calculations in momentum space, so nonlocalities are included.
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A typical amplitude
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pp pK+ reaction
RS, H. Lenske and U. Mosel, Nucl. Phys. 764 (2006) 313
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p (,K+) Λ reaction
RS, K. Tsushima, A.W. Thomas, In prep
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Momentum space Dirac Eq.
Bound state spinors
A mean field approach
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Bound Hypernuclear
spinors
16O (,K+) 16N, 16O (*,K+) 16N ReactionsΛ
Hole states B (p3/2) – B (p1/2) = 6.3 MeV
[ p1/2 -1, sΛ ], [ p3/2
-1, sΛ ], [ p1/2 -1, pΛ ], [ p3/2
-1, pΛ ] 16N spectrumΛ
It is only for q << 1.5 fm-1
|g(q)| << |f(q)|
Jlab, arXiv: 0810.3852
Single particle model
Λ
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12C (,K+) 12B,
Quark meson Coupling model
Single Particle model
12C (*,K+) 12B ReactionsΛ Λ
Saito, Tsushima, Thomas,Prog. Nucl. Part. Phys.58, 1-167 (2007).
PRL 99, 052501 (2007)
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Bound Hypernuclear wave spinors
In the region of the momentum transfer of interest, the lower component of the spinor is not negligible.
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scattering states
pf (pK) = (pK0 – EK) ℓ m (-) ℓ Yℓm (pf ) Y*ℓm (pK ) Fℓ (pK )
Fℓ (pK) = jℓ (pK r) ƒℓ (pf ,r) r2 dr
800 MeV/c
2EVK(r) = -Ab0k2 (r)+Ab1.
b0 and b1 are parameters of the potential
Kaon optical potential
This provides ƒℓ (pf ,r)
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Fℓ (pK) = 0 jℓ (pK r) ƒℓ (pf ,r) r2 dr
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Fℓ (pK) = 0 jℓ (pK r) ƒℓ (pf ,r) r2 dr
= 0 jℓ (pK r) ƒℓ (pf ,r) r2 dr + Rmax jℓ (pK r) ƒℓ (pf ,r) r2 dr
Rmax
h (pKr) + h (pKr)1 2
H (pf r) - S H (pf r)- +
y= Im (r)
I2 = exp [ ±i(pK pf )r ]
Z=x+iy
Z=x-iy
C0
Z = x + iy
Z = x - iy
Scattering wave function in momentum space
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ƒℓ (pf ,r)
Fℓ (pK)
= 15
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(,K+) reaction on Nuclei
• K+ is weakly absorbing so reactionoccurs deep in the nuclear interior.
• Unnatural parity states strongly excited
• p→ΛK+ reaction well understood within an effective Lagrangian picture
• A proton is converted into a Λ, produces neutron rich hypernuclei.
Excitations of N*(1650), N*(1710), N*(1720) resonances.
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Relative Contribution of Various resonances
N*(1720) weaker by 3-4 orders of magnitude
Different J excitation
Largest J state is dominant
RS, H. Lenske and U. Mosel, PRC77, 052201 (2008)Jlab results from (*,K+)
16O (,K+) 16N Reaction
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Excitation spectrum of 4 groups of (p-1,Λ) states
In each group highest J is most strong.
Unnatural Parity states dominate.
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12C (,K+) 12B ReactionΛ
RS, K. Tsushima and A.W. Thomas, In preparation
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Contributions of Various Meson Exchange Processes
Π exchange dominates, and exchange more important at back angles due to large momentum transfers.
A (p,K+)B
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Binding energy selectivity
B (C)
0p1/2 0.708 MeV0p3/2 0.860 0s1/2 11.690
B ( Ca)4113
0d3/2 0.753 0d5/2 1.544 0p1/2 9.140 0s1/2 17.882
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Results for 4He target
For momentum transfers of interest, Dirac spinors smoothly varying, and are devoid of structures.
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Relative Contribution of Various resonances
RS, H. Lenske and U. Mosel, Phys. Rev.C 69 (2004) 065205
Role of pion self energy
A(p,K+)B
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(+, K+) reaction
N*(1710) dominates in his case too. S. Bender
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SUMMARY AND OUTLOOK
A(h,K+)B reactions provide mutually complimentary information about the hypernuclear spectrum.
A fully covariant description of these reactions is desirable
and is possible.
Hypernuclear states with largest angular momentum are dominant, typical of large momentum trasfer reactions.
(,K +), (*,K +) strongly excites also the unnatural parity states.
Tighter constraints on the models of Λ-N interaction
In-medium Chiral Dynamics, orxiv:0709.2298 (Weise)
Quark Meson Coupling Model (Tsushima, A.W. Thomas, Saito, Guichon)
Coll: H. Lenske, U. Mosel, K. Tsushima and A.W. Thomas