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Solution of the dispersion relations for the πN-scattering amplitudes by the method of Padé approximants
The [1, 1] Padé approximant is used in order to obtain a solution of the dispersion relations for the πN-scattering amplitude. The dispersion relations are constructed with one subtraction for the amplitude A (+) and without subtraction for all the other amplitudes. There is one free parameter (β) o...
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Published in: | Nuclear physics. B 1972-06, Vol.42, p.541-557 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The [1, 1] Padé approximant is used in order to obtain a solution of the dispersion relations for the
πN-scattering amplitude. The dispersion relations are constructed with one subtraction for the amplitude
A
(+) and without subtraction for all the other amplitudes. There is one free parameter (β) only, connected with the
t-channel contribution. The results obtained for s, p and d waves with isospin
T=
1
2
and T=
3
2
are in satisfactory agreement with experiment in quite a large energy region (except the P
13 wave). The results of the calculations do not change very much if one neglects the contribution of the
t-channel (
β=0). The partial
S
l±
(2
t)
matrix analysis in the region below the threshold of
πN-scattering indicates the existence of antibound states in the P
33 wave with effective masses of 900 and 955 MeV and in the P
11 wave with an effective mass of1010 MeV. |
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ISSN: | 0550-3213 1873-1562 |
DOI: | 10.1016/0550-3213(72)90497-X |