Exotic baryon resonances Exotic baryon resonances in the chiral dynamics in the chiral dynamics Tetsuo Hyodo a a RCNP, Osaka b ECT* c IFIC, Valencia d Barcelona Univ. 2003, December 9th A.Hosaka a , D. Jido b , S.I. Nam a , E. Oset c , A. Ramos d and M. J. Vicente Vacas c
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Exotic baryon resonances in the chiral dynamics Tetsuo Hyodo a a RCNP, Osaka b ECT* c IFIC, Valencia d Barcelona Univ. 2003, December 9th A.Hosaka a, D.
Motivations : Two poles? Cloudy bag model (1990) J. Fink et al. PRC41, 2720 Chiral unitary model (2001~) J. A. Oller et al. PLB500, 263 E. Oset et al. PLB527, 99 D. Jido et al. PRC66, T. Hyodo et al. PRC68, There are two poles of the scattering amplitude around nominal (1405) energy region. (1405) : J P =1/2 , I=0 ChU model, T. Hyodo
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Exotic baryon resonances Exotic baryon resonances in the chiral dynamicsin the chiral dynamics
Tetsuo Hyodoa
a RCNP, Osaka b ECT* c IFIC, Valencia d Barcelona Univ. 2003, December 9th
A. Hosakaa, D. Jidob, S.I. Nama, E. Osetc, A. Ramosd and M. J. Vicente Vacasc
1. Structure of (1405)1. Motivation : Two poles?2. Chiral unitary model3. Pole structure of (1405)4. Photo-production of K*(1405)
2. Quantum numbers of
1. Present status of theoretical studies2. Chiral model for K+p -> +KN3. Results4. Polarization test
Contents
Motivations : Two poles?
• Cloudy bag model (1990) J. Fink et al. PRC41, 2720
• Chiral unitary model (2001~) J. A. Oller et al. PLB500, 263 E. Oset et al. PLB527, 99 D. Jido et al. PRC66, 025203 T. Hyodo et al. PRC68, 018201
There are two poles of the scattering amplitudearound nominal (1405) energy region.
(1405) : JP=1/2, I=0
ChU model, T. Hyodo
Chiral unitary model
Unitarity of S-matrixChiral symmetry
Flavor SU(3) meson-baryon scatterings (s-wave)
Resonances
Low energy behavior
Non-perturbativeresummation
(1405), (1670), N(1535),(1620), (1620)
Dynamicalgeneration
Chiral perturbation theory
Unitarization
Framework of the chiral unitary model
Resonances
Generated resonances areexpressed as poles of the scattering amplitude.
Total cross sections of Kp scatterings
T. Hyodo, et al., Phys. Rev. C 68, 018201 (2003)
200
150
100
50
0300200100
K
70
60
50
40
30
20
10
0300200100
0
200
150
100
50
0300200100
−
60
50
40
30
20
10
0300200100
Plab [MeV/c]
K0n
60
50
40
30
20
10
0300200100
Plab [MeV/c]
0080
60
40
20
0300200100
Plab [MeV/c]
−
(1405) in the chiral unitary model
D. Jido, et al., Nucl. Phys. A 723, 205 (2003)
mass distribution
1390 + 66i (
1426 + 16i (KN)
Example : the p -> K0 reaction
Chiralterm
N(1710)
Chiral unitary model
Results for p -> K0
T. Hyodo, et al., nucl-th/0307005, Phys. Rev. C, in press
Total cross sections [mb]Mass distribution
� There are two mechanisms in the initial stage interaction, which filter each one of the resonances.
Good agreement(1385) effect
Photoproduction of K* (1405)
Only Kp channel appears at the initial stage
Higher pole ??
Effective interactions for meson part
1. VP coupling
2. VPP coupling
Effective interaction for (1385)
3. (1385)MB coupling
4. KP -> (1385) -> MB amplitude
SU(6) symmetry
6
5
4
3
2
1
015001450140013501300
MI [MeV]
00 (~I=0 averae of chared 0 (I=1
invariant mass distribution
Plab = 2.5 GeV/csqrt s ~ 2.35 GeV
Preliminary
1.2
1.0
0.8
0.6
0.4
0.2
0.0300028002600240022002000
sqrt s
π0Σ0 (~I=0) average of charged πΣ
π0Λ (I=1)
ΛK*KππΣ
Result : Total cross section
Preliminary
Summary and conclusions
We study the structure of (1405) using the chiral unitary model.
� There are two poles of the scattering amplitude around nominal (1405).
Pole 1 (1426+16i) : strongly couples to KN statePole 2 (1390+66i) : strongly couples to state
� By observing the mass distribution in the p -> K*(1405) reaction, it could be possible to isolate higher energy pole.
Appendix : other processes
p -> K
Kp -> J.C. Nacher, et al., PLB461, 299(1999)
J.C. Nacher, et al., PLB445, 55(1999)
SPring-8
J-PARC?
baryon : Introduction
+ : 5-quark (4 quark + 1 anti-quark)LEPS, T. Nakano et al., Phys. Rev. Lett. 91 (2003) 012002
Quantum numbers are not yet determinedTheory prediction D. Diakonov et al. (chiral quark soliton) Naive quark model S. Capstick et al. (isotensor formulation) A. Hosaka (chiral potential) R. L. Jaffe et al. (qq-qq-q : 10 + 8) J. Sugiyama et al. (QCD sum rule) F. Csikor et al. (Lattice QCD) S. Sasaki (Lattice QCD)
W. Liu et al. nucl-th/0308034S. I. Nam et al. hep-ph/0308313W. Liu et al. nucl-th/0309023Y. Oh et al. hep-ph/0310117
p -> K0, n -> K
Model (mechanism) dependence
Form factor dependence
Unknown parameters
Initial cm energy ~ 2 GeV (pcm ~ 750 MeV) not low energy -> linear or nonlinear?N* resonances, K* exchange, K1 exchange,…
Monopole, dipole… , value of , …
coupling, K*p coupling, …
Assuming the quantum numbers (spin, parity), we can calculate a reaction
Motivation and advantage
K+p -> ++ -> +K+n(K0p) Low energy model is sufficient (pcm ~ 350 MeV) take decay into account -> background estimation -> Width independent Hadronic process : clear mechanism
We propose
to extract a qualitative behavior which dependson the quantum numbers of .
Determination of quantum numbersNew : pp -> , A. W. Thomas, K. Hicks, and A. Hosaka, hep-ph/0312083
We calculate the Kp -> 0KN reaction usinga chiral model, assuming the possible quantum numbers of + baryon. � If we find the resonance with polarization test, the quantum number of + can be determined as I=0, JP=1/2+
T. Hyodo, et al, nucl-th/0307105, Phys. Lett. B, in pressE. Oset, et al, nucl-th/0312014, Hyp03 proceedings
Future work
� Full calculation of the present reaction without approximation of kinematics -> information from + angular dependence� photo-production of K* and V. Kubarovsky et al., hep-ex/0307088