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Theoretical Models for Exotic Baryons

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Title: Theoretical Models for Exotic Baryons


1
Theoretical Models for Exotic Baryons
Models of the nucleon chiral soliton vs quark
models The strange spin of the nucleon Interpretat
ion of new exotic baryons
  • John Ellis
  • DESY,
  • Feb. 1st, 2005

2
Models of the Nucleon
Quarks and/or solitons?
3
Models of Nucleon Structure
  • Naïve quark model
  • MQ 300 MeV
  • Wave function QQQ
  • Sea of extra qqbar pairs generated perturbatively
  • Usual SU(3) multiplets
  • Explains OZI rule
  • Proton spin Sum of valence quark spins
  • Sum of quark spins ½
  • Few intrinsic ssbar
  • Chiral soliton model
  • MU,D few MeV,
  • MS 100 MeV
  • Intrinsic qqbar pairs in nucleon wave function
  • Exotic SU(3) multiplets
  • Evasions of OZI rule
  • Proton spin Orbital angular momentum
  • Sum of quark spins 0
  • Many polarized ssbar

4
Baryons in Chiral Soliton Model
  • Baryons clouds of p, K, ?8 mesons
  • ? many ssbar pairs
  • Baryon spin due to rotation of meson cloud
  • ? Spin orbital angular momentum
  • ? no ?0 coupling
  • ? ssbar pairs polarized
  • Exotic baryons ? excitations of meson cloud

5
QCD in Two Dimensions
  • Explicit classical soliton _at_ strong coupling
  • Finite radius
  • Calculable quantum corrections _at_ O(1/Nc)
  • Higher multi-qqbar excited states

JE Frishman, in preparation
6
Exotic Antidecuplet Predicted in Chiral Soliton
Model
7
The Strange Spin of the Nucleon
My personal introduction to chiral soliton models
8
Proton Spin in Chiral-Soliton Model
  • Proton spin sum rule
  • ½ ½(?u ?d ?s) ?G Lz
  • ?SM ? small sum of quark contributions to spin
  • ?u ?d ?s 0 needs ?s lt 0
  • ?SM ? proton spin due to orbital angular
    momentum
  • Lz ½
  • ?SM ? small gluon contribution to spin
  • ?G 0
  • in simple extension of ?SM to include gluons
  • Predictions subject to 1/Nc, ms corrections
    30?

Brodsky JE Karliner, 1988
9
Why Should the Nucleon be Strange?
  • The vacuum is strange
  • chiral symmetry for p, K mesons ?
  • Cannot be expected to disappear when one inserts
    qqq test charge into vacuum
  • Expected to be generated in perturbative QCD
  • s sbar ? gluon ? quark
  • Also, generated by non-perturbative effects
  • instantons, chiral soliton models

10
Pion-Nucleon s Term
  • Measured in low-energy p-N scattering
  • Related to strange scalar density
  • Two recent determinations
  • Maybe y ½ ?

Important later for chiral soliton models of
exotic baryons
11
The Strange Spin of the Nucleon
  • Naïve interpretation of polarized DIS structure
    fns
  • One-particle inclusive particle production
    (HERMES)
  • But beware corrections to independent
    fragmentation, positivity bounds

The strange-quark matrix elements in the nucleon
could be small or large, depending on the quantum
numbers
12
Measurements of Gluon Polarization
Polarized strangeness ?s or gluons ?G ?s ? ?s
(a/p)?G?
HERMES asymmetry in hadron-pair production at
high pT
SMC asymmetry in hadron-pair production at high
pT
13
Most Recent Measurements
PHENIX double helicity asymmetry in pp ?p0 at
high pT
14
Compilation of ?G Measurements
Indirect, using polarized structure function
data BBA ?G 1.026 0.549 BBB ?G 0.031
0.669 AAC ?G 0.533 1.931
Direct, using hadron production
asymmetries HERMES _at_ 0.06 lt xG lt 0.28 ?G
0.41 0.18 0.03 SMC _at_ lt?Ggt 0.07 ?G
0.20 0.28 0.10 COMPASS _at_ ltxGgt 0.13 ?G
0.06 0.31 0.06
15
Estimates of ?G Integral
Use model shapes for ?G, adjust
normalization BB3 ?G 0.42 0.54 BB4 ?G
0.57 0.69 AAC ?G 0.79 0.39 _at_ Q2 5 GeV2
No hint of large ?G
JE Karliner, hep-ph/0501115
16
Comparison with Models for ?G
Need more measurements
JE Karliner, hep-ph/0501115
17
Discovery of Exotic Baryons?
Still needs to be confirmed
18
The Exotic Revolution?
19
Measurements of ? Properties
Stringent upper limits G lt 1(?) MeV from
KN scattering experiments
Inconsistent masses in different experiments?
20
Chiral-Soliton Predictions Revisited
21
Chiral-Soliton Predictions Revisited
J.E., Karliner Praszalowicz hep-ph/0401127
22
Mass Predictions in Chiral Soliton Model
Decuplet-Octet, Antidecuplet-Octet mass
differences where I1, I2 are soliton moments
of inertia. Including corrections of higher order
in Nc and ms where ß, ? related to
soliton moments of inertia Guadagnini
relation

J.E., Karliner Praszalowicz hep-ph/0401127
OK experiment
23
Chiral-Soliton Model Parameters
Fix two combinations of a, ß, ? using octet and
decuplet masses Can fix third combination
using p-N S term Using recent range of
values Find
J.E., Karliner Praszalowicz hep-ph/0401127
24
Estimating Antidecuplet Masses
Model range for soliton moment of inertia Find
antidecuplet-octet mass difference Antidecuplet
mass splittings Resulting range for T, ?
masses Overall range
J.E., Karliner Praszalowicz hep-ph/0401127
25
Exotic Baryon Spectrum s Term
Chiral soliton mass formula
numerically
26
Baryon ? Baryon Meson Couplings
Related by generalized Goldberger-Treiman to
axial-current couplings Expressions for
baryon-meson couplings G2 related to
singlet axial-current matrix element
small? Other combinations related to ?, N decay
couplings
J.E., Karliner Praszalowicz hep-ph/0401127
27
O(1/Nc) Corrections to Decay Rates
Need to estimate G0,1,2 Estimate G2 from
spin-dependent structure functions Model
calculations ??pN coupling to estimate
G0,1 Estimate of T?KN coupling in this
approximation Significant suppression of T
decay rate not enough?
J.E., Karliner Praszalowicz hep-ph/0401127
28
SU(3) Corrections to Decay Rates
SU(3) corrections to pNN coupling SU(3)
corrections to ??pN coupling due to
representation mixing SU(3) corrections to
T?KN coupling due to representation
mixing Large suppression of T decay rate
possible not for other antidecuplet baryons
29
Baryon Couplings in Soliton Model
p-Nucleon coupling Consistent with experiment
J.E., Karliner Praszalowicz hep-ph/0401127
30
Predictions for Other Exotic Baryons
Masses of 27-plet states Masses for nominal
parameters Mass difference with T in
27-plet Typical value 63 MeV Similarly for
? in 27-plet Typical value 19 MeV Also
35-plet,
31
Spectrum of Antidecuplet 27 Baryons
Using ? and ?-- masses
J.E., Karliner Praszalowicz hep-ph/0401127
32
Quark Model Approaches
33
Understanding T in Quark Language
34
Diquark-Triquark Structure?
Karliner Lipkin hep-ph/0307243
35
Possible Diquark-Triquark Configurations
Karliner Lipkin hep-ph/0307243
36
Estimating T Mass
Karliner Lipkin hep-ph/0307243
37
Predictions for Heavy-Flavour Exotics
Karliner Lipkin hep-ph/0307243
38
Diquarks
Jaffe Wilczek hep-ph/0307341
39
Diquark Model for T Baryon
Jaffe Wilczek hep-ph/0307341
40
Predictions Postdictions
Jaffe Wilczek hep-ph/0307341
41
Discriminating between Models
also 27 multiplet
42
Summary
  • Complementary models of nucleon structure
  • naïve quark model, chiral soliton
  • Experimental evidence of hidden strangeness
  • p-N s term, polarized DIS
  • Boost for chiral solitons from exotic baryons?
  • Predicted in soliton model,
  • Spectroscopy depends on p-N s term large?
  • New, less naïve quark models
  • Expect more twists in the strange, exotic story!

? solitons
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