t-J model
The t-J model was first derived in 1977 from the Hubbard model by Józef Spałek. The model describes strongly-correlated electron systems. It is used to calculate high temperature superconductivity states in doped antiferromagnets.
The t-J Hamiltonian is:
where
- is the sum over nearest-neighbor sites i and j,
- â†
iσ, â
iσ are the fermionic creation and annihilation operators, - σ is the spin polarization,
- t is the hopping integral,
- J is the coupling constant, J = 4t2/U,
- U is the coulombic repulsion,
- ni = â†
iσâ
iσ is the particle number at site i, and - S→i, S→j are the spins on sites i and j.
Connection to the high-temperature superconductivity
The Hamiltonian of the t1-t2-J model in terms of the CP1 generalized model is:[1]
where the fermionic operators c†
iσ and c
iσ, the spin operators Si and Sj, and the number operators ni and nj all act on restricted Hilbert space and the doubly-occupied states are excluded. The sums in the above mentioned equation are over all sites of a 2-dimensional square lattice, where ⟨…⟩ and ⟨⟨…⟩⟩ denote the nearest and next-nearest neighbors, respectively.
References
- ↑ Karchev, N. (1998). "Generalized CP1 model from the t1-t2-J model". Phys. Rev. B. 57: 10913. doi:10.1103/PhysRevB.57.10913.
- Fazekas, Patrik, Lectures on Correlation and Magnetism, p. 199
- Spałek, Józef (2007). "t-J model then and now: A personal perspective from the pioneering times". Acta Phys. Polon. A. 111: 409–424. arXiv:0706.4236.
This article is issued from Wikipedia - version of the 11/7/2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.