Analysis of pion photoproduction and the quark model

Moorhouse, R.G.; Oberlack, H.

doi:10.1016/0370-2693(73)90540-6

Analysis of pion photoproduction and the quark model

R.G. Moorhouse
(
- Glasgow U.
)
,
H. Oberlack
(
- LBL, Berkeley
)

1973

5 pages

Published in:

Phys.Lett.B 43 (1973) 44-48

Published: 1973

DOI:

10.1016/0370-2693(73)90540-6

View in:

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Abstract: (Elsevier)

(N ∗ Nγ) couplings for resonances in the first, second, and third resonance region are determined in a continuous-energy partial wave analysis of single-pion photoproduction off protons and neutrons using fixed- t dispersion relations. Several couplings are determined for the first time. Most results, especially for the principal resonances, agree well with the predictions of the quark model, but the P 11 (1470), on its present unmixed multiplet assignment, disagrees.

photon p: interaction
interaction: photon p
final state
photon n: interaction
interaction: photon n
pi: photoproduction
photoproduction: pi
quark
partial-wave analysis
coupling constant: photon-nucleon-baryon resonance

References(19)

Figures(0)

[1]

Phenomenological analysis of single pion photoproduction

R.L. Walker
(
- Caltech
)

- Phys.Rev. 182 (1969) 1729-1748
•
DOI:
- 10.1103/PhysRev.182.1729

[2]

Proc. Daresbury Conf. on Electron and photon interactions at high energy

D. Braben
,
R.L. Walker

[3]

Analysis of pion photoproduction in the second resonance region

- Phys.Rev. 163 (1967) 1632-1645
•
DOI:
- 10.1103/PhysRev.163.1632

[3]

An analysis of single pion photoproduction in the second resonance region

R.G. Moorhouse
(
- Glasgow U.
)
,
W.A. Rankin
(
- Glasgow U.
)

- Nucl.Phys.B 23 (1970) 181-217
•
DOI:
- 10.1016/0550-3213(70)90187-2

[4]

Photoproduction and electroproduction of pions. 1. Dispersion relation theory

- Nucl.Phys.B 4 (1967) 1-53
•
DOI:
- 10.1016/0550-3213(67)90196-4

[5]

R.C.E. Devenish
,
D.H. Lyth
,
W.A. Rankin

[6]

A Collection of pion photoproduction data. 1. From the threshold to 1.5-GeV

[7]

to be published

R.C. Moorhouse
,
H. Oberlack
,
A.H. Rosenfeld

[8]

Vanishing of the E2 part of the N $^∗_{33}$ → N + γ amplitude in the non-relativistic quark model of “elementary” particles

C. Becchi
(
- Genoa U. and
- INFN, Genoa
)
,
G. Morpurgo
(
- Genoa U. and
- INFN, Genoa
)

- Phys.Lett. 17 (1965) 352-354
•
DOI:
- 10.1016/0031-9163(65)90563-9

[8]

R.G. Moorhouse

- Phys.Rev.Lett. 16 (1966) 771

[8]

Backward single pion photoproduction and the symmetric quark model

- Phys.Lett.B 29 (1969) 117-120
•
DOI:
- 10.1016/0370-2693(69)90261-5

[8]

Single pion photoproduction in the quark model

- Nucl.Phys.B 13 (1969) 303-319
•
DOI:
- 10.1016/0550-3213(69)90237-5

[9]

R.P. Feynman
,
M. Kislinger
,
F. Ravndal

- Phys.Rev.D 3 (1971) 1706

[10]

Harmonic oscillator model for baryons

- Phys.Rev. 173 (1968) 1720-1729,
- In *Lichtenberg, D. B. ( Ed.), Rosen, S. P. ( Ed.): Developments In The Quark Theory Of Hadrons, Vol. 1*, 337-346
•
DOI:
- 10.1103/PhysRev.173.1720

[10]

Electromagnetic decays of baryon resonances in the harmonic-oscillator model

D. Faiman
(
- Illinois U., Urbana
)
,
A.W. Hendry
(
- Illinois U., Urbana
)

- Phys.Rev. 180 (1969) 1572-1577
•
DOI:
- 10.1103/PhysRev.180.1572

[10]

Harmonic-oscillator model for baryons

D. Faiman
(
- Illinois U., Urbana
)
,
A.W. Hendry
(
- Illinois U., Urbana
)

- Phys.Rev. 180 (1969) 1609-1610
•
DOI:
- 10.1103/PhysRev.180.1609

[11]

R. Ayed
,
P. Bareyre
,
Y. Lemoigne

[12]

D.J. Herndon

[13]

Stanford Linear Accelerator Center Report -EXP BC 47

M. Bogdanski