中国物理B ›› 2010, Vol. 19 ›› Issue (11): 117401-117402.doi: 10.1088/1674-1056/19/11/117401

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Crossover from a pseudogap state to a superconducting state

曹天德   

  1. Department of Physics, Nanjing University of Information Science and Technology, Nanjing 210044, China
  • 收稿日期:2010-04-25 修回日期:2010-05-29 出版日期:2010-11-15 发布日期:2010-11-15

Crossover from a pseudogap state to a superconducting state

Cao Tian-De(曹天德)   

  1. Department of Physics, Nanjing University of Information Science and Technology, Nanjing 210044, China
  • Received:2010-04-25 Revised:2010-05-29 Online:2010-11-15 Published:2010-11-15

摘要: This paper deduces that the particular electronic structure of cuprate superconductors confines Cooper pairs to be first formed in the antinodal region which is far from the Fermi surface, and these pairs are incoherent and result in the pseudogap state. With the change of doping or temperature, some pairs are formed in the nodal region which locates the Fermi surface, and these pairs are coherent and lead to superconductivity. Thus the coexistence of the pseudogap and the superconducting gap is explained when the two kinds of gaps are not all on the Fermi surface. It also shows that the symmetry of the pseudogap and the superconducting gap are determined by the electronic structure, and non-s wave symmetry gap favours the high-temperature superconductivity. Why the high-temperature superconductivity occurs in the metal region near the Mott metal-insulator transition is also explained.

Abstract: This paper deduces that the particular electronic structure of cuprate superconductors confines Cooper pairs to be first formed in the antinodal region which is far from the Fermi surface, and these pairs are incoherent and result in the pseudogap state. With the change of doping or temperature, some pairs are formed in the nodal region which locates the Fermi surface, and these pairs are coherent and lead to superconductivity. Thus the coexistence of the pseudogap and the superconducting gap is explained when the two kinds of gaps are not all on the Fermi surface. It also shows that the symmetry of the pseudogap and the superconducting gap are determined by the electronic structure, and non-s wave symmetry gap favours the high-temperature superconductivity. Why the high-temperature superconductivity occurs in the metal region near the Mott metal-insulator transition is also explained.

Key words: pseudogap, superconductivity, Fermi surface

中图分类号:  (Pairing symmetries (other than s-wave))

  • 74.20.Rp
74.25.Jb (Electronic structure (photoemission, etc.)) 74.50.+r (Tunneling phenomena; Josephson effects)