1 study of n* excitations in 2-pion production. 2 analysis of + - p single differential...
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![Page 1: 1 Study of N* excitations in 2-pion production. 2 Analysis of + - p single differential cross-sections. p - ++ p+0p+0 pppp](https://reader036.vdocuments.net/reader036/viewer/2022062304/56649d2b5503460f94a00871/html5/thumbnails/1.jpg)
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Study of N* excitations in 2-pion production
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Analysis of +-p single differential cross-sections.
p-++
p+0
pp
p-P++33(1600)
p+F015(1685)
direct 2production
p+D13(1520)
Isobar Model JM05
JM06
V. Mokeev
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Test of JM05 program on well known states.
D13(1520)
ep → ep (A1/22+S1/2
2)1/2, GeV-1/2 A3/2, GeV-1/2
Q2 GeV2Q2 GeV2
→ JM05 works well for states with significant N couplings.
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P11(1440) and D13(1520) electrocouplings from N and pπ+π-
from analysis of CLAS 2data within JM06
from analysis of 1 CLAS data
combined analysis of 1 CLAS data
• 2 data show clear evidence for sign flip of P11(1440) A1/2
electrocoupling. • Electrocouplings obtained in two independent analyses of 1 and 2 channels are in reasonable agreement.
D13(1520)P11(1440)
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First consistent amplitudes for A1/2(Q2), A3/2(Q2) of D33(1700)
D33(1700)ep → ep State has dominant coupling to N : PDG:80-90%Np
Many of the higher mass states have significant coupling to Nππ.
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Search for New Baryon States
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|q3>
|q2q>
Possible reason: they have small coupling to N-channel.
Possible solutions: 1. States don’t exist, e.g. di-quark model predicts fewer states, with different underlying symmetry group
2. States exist but have not been found.
Model expectations: Hadronic couplings to N(, N) much larger, while photocouplings are more comparable to those for observed states. Other channels that may be sensitive to “missing” states are: K, K, p
“Missing” Baryon States
Quark models with underlying SU(6)xO(3) symmetry predict many states, not observed in either hadronic experiments or in meson photo- and electro-production.
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- Is the P33(1600)*** is really there?
- One more 3/2+(1720) state ?
- New resonances in KY ?
Evidence for new baryon states?
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Search for Baryon States in p p
Two methods:
Isobar models (similar approach as in single pion analysis): energy-dependences of amplitudes are parameterized. fits to several (or all) one-dimensional projections.
Event-by event analysis: fit partial-wave content independently for every energy bin. makes maximum use of all correlations in the multi-dimensional phase space. ambiguities can give multiple solutions.
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SU(6)xO(3) Classification of Baryons
P(1600)
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Evidence for P33(1600) *** state
W=1.59 GeV
no P33(1600)
with P33(1600)
Fit to high statistics photoproduction datarequires inclusion ofP33(1600) state.
Sample datap p
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P33(1600) state parameters
Mass, MeV 1686 ± 10 1550 - 1700 PDG1687 ± 44 Dytman1706 ± 10 Manley
Total decaywidth, MeV
338 ± 100 250 - 450 PDG493 ± 75 Dytman430 ± 75 Manley
BF ( 65 ± 6 40 -70 PDG59 ± 10 Dytman67 ± 5 Manley
A1/2 -30 ± 10 - 29 ± 20 PDG
A3/2 -17 ± 10 -19 ± 20 PDG
this analysis world
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A new 3/2+(1720) baryon state?
M.Ripani et. al. Phys. Rev. Lett.91, 022002 (2003)
Difference between curves due to signal from possible 3/2+(1720) state
Fit with new 3/2+(1720) state
Contributions from conventional states only
JM03 Isobar Model Analysis
→ epep
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Photo- and electroproduction comparsion
photoproductionelectroproductionp
Q2=0
W(GeV) W(GeV)
Q2=0
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Total p p cross-section off protons.
Signal from 3/2+(1720) state present, but masked by large background and destructive N*/background interference.
Hadronic couplings and mass derived from the fit of virtual photon data, and 3/2+(1720) photocouplings fitted to the real photon data.
Background
Resonances
Interference
full calculation
no 3/2+
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Parameters derived from combined analysis
Mass,MeV
Total width,MeV
BF(),%
BF(P),%
“New 3/2+
State” 1722 92 50 11
PDGP13(1720)
1650-1750 100-200 not observed
70 – 85
Mass and decays
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– To reduce ambiguities, the search for new excited states aims at “complete” or nearly complete measurements in γp→πN, ηN, K+Y and γn→πN, K0Y and using combinations of beam, target, and recoil polarizations:
• differential cross sections with unpolarized, circularly polarized, and linearly polarized photon beams,
• recoil polarizations for hyperons,
• longitudinally or transversely polarized proton and neutron (deuteron) targets.
– Other reactions include γp → ρN, ωp, ππN with linearly polarized beams, and with polarized beam and polarized targets.
Search for CQM predicted states.CLAS
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New Results in γp→pπ0CLASFA06 solutionof SAID analysis
A1/2 from Nπ analysis for S11(1535) now agrees with Nη results as was found earlier in electro-production.
Strong excitation of P13(1720) is consistent with earlier analysis of pπ+π- electro-couplings.
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Photoproduction of K+Λ, K+Σ0
Fit: Bonn-Gatchina group, Anisovich et al., 2007
CLAS
P13
P13P11 K exchange
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Photoproduction of K+Λ/Σ0
Fit: Bonn-Gatchina group, Anisovich et al., 2007
KΛ KΣ
Fit with P13(1900)
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γp—>K+Λ Polarization transfer
w/o P13(1900) with P13(1900)
CLAS
Fit shows strong preference for second P13 state. Existence of this state would be evidence against the quark-diquark model.
Includes *** / **** states
(E. Santopinto, 2005)
Quark-Diquark Model
Coupled channel fit: Bonn-Gatchina group, Anisovich et al, 2007
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Excited Cascades Ξ*
• Advantage over search for N*’s and Y*’s is narrow widths of Ξ’s• Possible production mechanism through decay of excited
hyperons – requires large acceptance and high luminosity experiments
CLAS
Ξ(1320)
Ξ(1530)
Missing mass MM(K+K+) works for narrow states, but higher energy and higher statistics are needed.
Possible production mechanism
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Search in γp―>π-K+K+Ξ*CLAS
A Ξ state at 1.62GeV and 50 MeV width could be the 1* candidate in PDG. Such a state would be consistent with a dynamically generated Ξπ state. It would contradict quark models. Requires more statistics and PWA.
Ξ(1530)
New high statististics run in 2008!
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Reaction Diffcrs
Lin. beam
Circ. beam
Long.Target
Trans. Target
Recoil Group Publication/Status/Schedule
γp→pπ0 x G1 arXiv:0705.0816
γp→nπ+ x G1 analysis
γp→pη x G1, G10 PRL89, 222002, 2002
γp→pη’ x G1, G10 PRL96, 062001, 2006
γp→K+Λ, K+Σ x x x G1, G10 PRC69 042201, 2004; PRC73, 035202, 2006; PRC75 035205, 2007
γp→K0*Σ+ x G1 PRC75 042201, 2007
γp→pπ-π+ x x G1 PRL95 162003, 2006, analysis
γp→pω, pρ0, nρ+ x x G8 2005 / Analysis
γn→ K0Λ, K0Σ, K+Σ-, K-Σ+
x x x x G13 2007 / Analysis
γp→pπ0, nπ+, pη x x x x G9-FROST 2007/2009
γp→K+Λ, K+Σ x x x x x G9-FROST 2007/2009
γp→pπ-π+ x x x x G9-FROST 2007/2009
γn→ K0Λ, K0Σ, K+Σ-, K-Σ+
x x x x x G14-HD 2010
γn→pπ-,nπ+π- x x x x G14-HD 2010
Experiment Status & Plans of Search for New N* StatesCLAS
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CLAS γd→K0Λ, π-p, (ps)
Eγ=1.5 – 1.7
Online beam asymmetry for γn→π-p
Photons produced coherently from aligned diamond crystals are linearly polarized.
Identify: Ks →π+π- Λ→pπ-
Eγ=1.1-1.3 GeVAll polar angles
< 0.1% of all data
Ks
M(π+π-), GeV
Λ
M(pπ-), GeV
• Plots show a 5 GeV run with the coherent edge at 1.9 GeV
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γp →K+ΛProjected Accuracy of Data (4 of over 100 bins)
→→ →
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γn →K0Λ Projected Accuracy of Data (4 of over 100 bins)
→→ →
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Conclusions
• The study of N* excitations in photo- and electroproduction of mesons from nucleons is key for the understanding of the strong force that confines the quarks into nucleons.
• The experimental and theoretical analysis we are all engaged in will make gigantic contributions towards that goal.
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N*’s ARE FUN !
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Fit of CLAS 2 data on 3 invariant masses and - angular distributions within the framework of JM05.
, mcbn
W, GeV
Q2=0.65 Gev2
Q2=0.95 Gev2
Q2=1.30 Gev2
Reasonable description of invariant mass and p- angular distributions was achieved in entire kinematics area covered by CLAS data.
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Diquark-Quark Model
Includes all observed *** & **** states
(E. Santopinto, 2005)
Spectrum predicted for masses below 2 GeV.