dc.contributor.author |
Ershov, S.N.
|
|
dc.contributor.author |
Rakityansky, Sergei Anatoljevich
|
|
dc.date.accessioned |
2022-03-03T06:33:51Z |
|
dc.date.available |
2022-03-03T06:33:51Z |
|
dc.date.issued |
2021-02 |
|
dc.description.abstract |
A family of analytically solvable potential models for the one- and two-channel problems is considered within
the Jost matrix approach. The potentials are chosen to be constant in the interior region and to have different
asymptotic behavior (tails) at large distances. The migration of the S-matrix poles on the Riemann surface of the
energy, caused by variations of the potential strength, is studied. It is demonstrated that the long-range (∼1/r2)
tails and Coulomb potential (∼1/r) cause an unusual behavior of the S-matrix poles. It is found that in the
two-channel problem with the long-range potentials the S-matrix poles may appear at complex energies on the
physical Riemann sheet. The Coulomb tail not only changes the topology of the Riemann surface, but also breaks
down the so-called mirror symmetry of the poles in both the single-channel and the two-channel problems. |
en_ZA |
dc.description.department |
Physics |
en_ZA |
dc.description.librarian |
pm2022 |
en_ZA |
dc.description.uri |
http://prc.aps.org |
en_ZA |
dc.identifier.citation |
Ershov, S.N. & Rakityansky, S.A. 2021, 'Jost matrices for some analytically solvable potential models', Physical Review C, vol. 103, no. 2, art. 24612, pp. 1-16. |
en_ZA |
dc.identifier.issn |
2469-9985 (print) |
|
dc.identifier.issn |
2469-9993 (online) |
|
dc.identifier.other |
10.1103/PhysRevC.103.024612 |
|
dc.identifier.uri |
http://hdl.handle.net/2263/84315 |
|
dc.language.iso |
en |
en_ZA |
dc.publisher |
American Physical Society |
en_ZA |
dc.rights |
© 2021 American Physical Society |
en_ZA |
dc.subject |
Jost matrices |
en_ZA |
dc.subject |
Analytical solutions |
en_ZA |
dc.subject |
Solvable potential models |
en_ZA |
dc.title |
Jost matrices for some analytically solvable potential models |
en_ZA |
dc.type |
Article |
en_ZA |