Antiferromagnetism and superconductivity of the two-dimensional extended t–J model

The mechanism of high-temperature superconductivity (HTS) and the correlation between the antiferromagnetic long-range order (AFLRO) and superconductivity (SC) phases are the central issues of the study of HTS theory. SC and AFLRO of the hole-doped two-dimensional extended t- J model are studied by...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Физика низких температур
Datum:2005
Hauptverfasser: Shih, C.T., Wu, J.J., Chen, Y.C., Mou, C.Y., Chou, C.P., Eder, R., Lee, T.K.
Format: Artikel
Sprache:English
Veröffentlicht: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2005
Schlagworte:
Online Zugang:https://nasplib.isofts.kiev.ua/handle/123456789/121694
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Zitieren:Antiferromagnetism and superconductivity of the two-dimensional extended t–J model / C.T. Shih, J.J. Wu, Y.C. Chen, C.Y. Mou, C.P. Chou, R. Eder, T.K. Lee // Физика низких температур. — 2005. — Т. 31, № 8-9. — С. 995-1001. — Бібліогр.: 39 назв. — англ.

Institution

Digital Library of Periodicals of National Academy of Sciences of Ukraine
Beschreibung
Zusammenfassung:The mechanism of high-temperature superconductivity (HTS) and the correlation between the antiferromagnetic long-range order (AFLRO) and superconductivity (SC) phases are the central issues of the study of HTS theory. SC and AFLRO of the hole-doped two-dimensional extended t- J model are studied by the variational Monte Carlo method. The results show that SC is greatly enhanced by the long-range hopping terms t' and t" for the optimal and overdoped cases. The phase of coexisting SC and AFM in the t-J model disappears when t and t" are included. It is concluded that the extended t-J model provides a more accurate description for HTS than the traditional t-J model does. The momentum distribution function n(k) and the shape of Fermi surface play critical roles for establishing the phase diagram of HTS materials.
ISSN:0132-6414