𝔖 Bobbio Scriptorium
✦   LIBER   ✦

On the origin of the unconventional two-hole bound state in the t-J model

✍ Scribed by Piotr Wróbel; Robert Eder


Publisher
Elsevier Science
Year
1994
Tongue
English
Weight
184 KB
Volume
199-200
Category
Article
ISSN
0921-4526

No coin nor oath required. For personal study only.

✦ Synopsis


We present a description of the ground state and low-lying excited states of two holes in the 4 x 4 cluster t-J model in terms of a simple model for the motion of a single bipolaron. The existence of short-range antiferromagnetic correlations has been assumed. According to the suggested scenario, the formation of the bipolaron is mediated by the reduction of the magnetic energy in the case of two holes occupying nearest neighbor sites. The relevant part of the Hilbert space consists of wave functions corresponding to holes oscillating around pairs of nearest neighbor sites and trapped in a potential well due to strings of spin defects. Virtual processes which connect these states involve both the kinetic term and the transverse part of the Heisenberg Hamiltonian. Many properties of energy level schemes obtained by numerical diagonalizations such as the sequence of the lowest states for each irreducible representation of the k vector point groups can be reproduced satisfactorily. In agreement with numerical methods the ground state has nontriviai dx2_y2 symmetry.


📜 SIMILAR VOLUMES


Bound states of holes in the two-dimensi
✍ A. Mishima 📂 Article 📅 1994 🏛 Elsevier Science 🌐 English ⚖ 138 KB

The bound states of p holes are studied within the two-dimensional two-band model with the antiferromagnetic exchange interaction between d and p spins, J. The binding energies of p holes are computed as a function of the Cu-O transfer and one of J within the mean-field theory with the periodic boun

Dynamics of one hole in the polarized t−
✍ K. Hallberg; A.G. Rojo; C.A. Balseiro 📂 Article 📅 1991 🏛 Elsevier Science 🌐 English ⚖ 506 KB

We calculate the one-hole spectral function for the polarized t-J model using exact diagonalization for a finite size cluster. A well-defined quasiparticle peak appears at the bottom of the spectrum for intermediate values of J. The momentum of the quasiparticle corresponding to the bottom of the ba