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Exotic baryon resonances in the chiral dynamics. Tetsuo Hyodo a. Hosaka a , D. Jido b , S.I. Nam a , E. Oset c , A. Ramos d and M. J. Vicente Vacas c. a RCNP , Osaka b ECT* c IFIC, Valencia d Barcelona Univ. 2003, December 9th. Contents. Structure of L (1405) - PowerPoint PPT Presentation
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Exotic baryon resonances Exotic baryon resonances in the chiral dynamicsin the chiral dynamics
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
ContentsContents
Motivations : Two poles?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 modelChiral 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 modelFramework of the chiral unitary model
Resonances
Generated resonances areexpressed as poles of the scattering amplitude.
Total cross sections of Kp scatteringsTotal cross sections of Kp scatterings
T. Hyodo, et al., Phys. Rev. C 68, 018201 (2003)
200
150
100
50
0300200100
K-p
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(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 reactionExample : the p -> K0 reaction
Chiralterm
N(1710)
Chiral unitary model
Results for p -> K0Results 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)Photoproduction of K* (1405)
Only Kp channel appears at the initial stage
Higher pole ??
Effective interactions for meson partEffective interactions for meson part
1. VP coupling
2. VPP coupling
Effective interaction for (1385)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 (~ =0)I average of charged 0 ( =1)I
invariant mass distribution 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 sectionResult : Total cross section
Preliminary
Summary and conclusionsSummary 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 processesAppendix : other processes
p -> K
p -> J.C. Nacher, et al., PLB461, 299(1999)
J.C. Nacher, et al., PLB445, 55(1999)
SPring-8
J-PARC?
baryon : Introduction 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)
: 1/2+, I=0: 1/2
: 1/2, 3/2, 5/2, I=2: 1/2+ (strong ): 1/2+, I=0: 1/2, I=0: 1/2+ -> 1/2
: 1/2
S = +1, M ~ 1540 MeV, < 25 MeV
Photo-production processPhoto-production process
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, 1 exchange,…
Monopole, dipole… , value of , …
coupling, K*p coupling, …
Assuming the quantum numbers (spin, parity), we can calculate a reaction
Motivation and advantageMotivation 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
A model for p -> +K+n A model for p -> +K+n
E. Oset and M. J. Vicente Vacas, PLB386, 39(1996)
Vertices are derived from the chiral Lagrangian
Proportional to vanishes
Assume final + is almost at rest
Dominant
DiagramsDiagrams
Tree level(background)
One loop
Possibilities of spin & parityPossibilities of spin & parity
1/2 (KN s-wave resonance)1/2 , 3/2 (KN p-wave resonance)
MR = 1540 MeV = 20 MeV
Resonance termResonance term
Amplitude of resonance term for K+p -> +K+n :
Angular dependenceAngular dependence
total resonance background
10
8
6
4
2
01.00.50.0-0.5-1.0
cosθ
10
8
6
4
2
01.00.50.0-0.5-1.0
cosθ5
4
3
2
1
01.00.50.0-0.5-1.0
cosθ
,I JP=0,1/2- ,I JP=0,1/2+
,I JP=0,3/2+
Mass distributionsMass distributions
8
6
4
2
015801560154015201500
MI
,I JP=0,1/2-
,I JP=0,1/2+
,I JP=0,3/2+kin( ) = 850 /Lab MeV cθ = 90 deg
1.4
1.2
1.0
0.8
0.6
0.4
0.2
0.015801560154015201500
MI
Polarization testPolarization test
# Same result is obtained for final pK0
Angular dependence : polarization testAngular dependence : polarization test
total resonance background
5
4
3
2
1
01.00.50.0-0.5-1.0
cosθ
20
15
10
5
01.00.50.0-0.5-1.0
cosθ5
4
3
2
1
01.00.50.0-0.5-1.0
cosθ
,I JP=0,1/2- ,I JP=0,1/2+
,I JP=0,3/2+
Polarization test
Mass distributions : polarization testMass distributions : polarization test
14
12
10
8
6
4
2
015801560154015201500
MI
,I JP=0,1/2-
,I JP=0,1/2+
,I JP=0,3/2+kin( ) = 850 /Lab MeV cθ = 90 deg
1.4
1.2
1.0
0.8
0.6
0.4
0.2
0.015801560154015201500
MI
Polarization test
Incomplete polarizationIncomplete polarization
14
12
10
8
6
4
2
015801560154015201500
MI
,I JP=0,1/2-
,I JP=0,1/2+ kin( ) = 850 /Lab MeV cθ = 90 deg
Polarization
100 %80 % 0 %
ConclusionConclusion
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 workFuture 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