dc.contributor.author |
Eremin M. |
|
dc.contributor.author |
Shigapov I. |
|
dc.contributor.author |
Eremin I. |
|
dc.date.accessioned |
2018-09-18T20:36:01Z |
|
dc.date.available |
2018-09-18T20:36:01Z |
|
dc.date.issued |
2014 |
|
dc.identifier.uri |
https://dspace.kpfu.ru/xmlui/handle/net/141559 |
|
dc.description.abstract |
© Kazan Federal University (KFU). We derive the dynamical spin susceptibility in the t-J-G model combining the random phase approximation (RPA) and projection operator method, which allows describing the mutual interplay between the local and the itinerant components of susceptibility. Near the antifer- romagnetic wave vector the calculated dispersion of the spin excitations reproduces well the so-called hour-glass dispersion, characteristic for several layered cuprates. It is formed as a result of competition between the original spin-gap in magnon-like excitations spectrum and the superconducting gap, which affects the itinerant component of the susceptibility. Further- more, the calculated collective spin excitations along (0, 0)-(0, π) are in agreement with the positions of the absorption peaks in the inelastic X-ray scattering spectra. They refer to the paramagnon-like modes, characteristic to the itinerant spin system, rather than magnon-like excitations that originate from short range order effect in the system of local spins at Cu sites. |
|
dc.subject |
Collective spin excitations |
|
dc.subject |
Cuprates |
|
dc.subject |
Dynamical spin susceptibility |
|
dc.subject |
HTSC |
|
dc.title |
Spin response in HTSC cuprates: Generalized RPA approach with projection operators method |
|
dc.type |
Article |
|
dc.relation.ispartofseries-volume |
16 |
|
dc.collection |
Публикации сотрудников КФУ |
|
dc.source.id |
SCOPUS-2014-16-SID84925373036 |
|