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Phys 498CQM Lecture Notes 24
Exact Diagonalization for Many-Body Problems
Lanczos Methods

Wednesday, April 18, 2001
Lecturer: Richard Martin
Thijssen, Ch. 11, 12
Koonin, p. 119
Other references given in lecture

Thijssen Ch. 11 discusses "Transfer Matrix methods"; Need Lanczos (sec. 11.3) or QMC methods (12.6) for solution of complex cases

Other cases discussed in notes and in the references given

  1. Examples of many-body problems
    • Hubbard Model
      • Review by Dagotto for problems in HiTc related systems
      • Setting up Hamiltonian in convenient basis (see Lin and Gubernatis)
      • Example from Class project, 1996, by Sengupta
    • Spin systems, Heisenberg Model - Derived in limit of Hubbard Model
      • Magnetic order?
      • Finite size scaling
    • Spin systems, the Ising model - See review by Kogut
      • Real model for classical, quantum spins
      • Isomorphic to Lattice gauge theories
        See review by Kogut; Thijssen, Ch. 13
      • Transfer matrix method
        • Large eigenvalue gives free energy
        • Simple 1d spin 1/2 case (Thijssen Ch. 11)
        • Approach to 2d - very complex (Thijssen Ch. 11)
        • Solution by Lanczos (Thijssen Ch. 11) or QMC (Thijssen Ch. 12)
      • The 1d Ising model in a transverse field
        • Maps onto model for quantum double-well tunneling model for ferroelectrics
        • Hamiltonian for intracting quantum Ising spins
        • Perturbation theory analysis - shows the key points of ground state energy and correlation functons
        • Phase transition at critical coupling constant
        • Duality of Ising model shows analytically where transition is expected
        • A gap vanishes at this point (gap between ground state and lowest excited state.)
    • Solution by Lanczos methods
      • Consider finite systems with a finite (but large basis)
      • The hamiltonian operator as a sparse matrix
      • Generation of the basis in which H is tridiagonal
        (This is the tricky part for a many body system, because the basis is so large one must order the computations carefully)
      • Examples of solutions
        • Ising model from Roomany
        • Hubbard Model from Sengupta
      • Finite size scaling and the phase transition at infinite size
    • References
      • E. Dagotto, Rev. Mod. Phys. 66, 763 (1994).
      • J. Kogut, Rev. Mod. Phys. 51, 651 (1979).
      • H. Roomany, H. W. Wyld, and L. Holloway, Phys. Rev. D21, 1557 (1980), and thesis, U of I, 1980.
      • H. Q. Lin and J. E. Gubernatis, Computers in Physics 7, 400 (1993).
      • E. R. Gagliano, et. al., Phys. Rev. B34, 1677 (1986).
      • B. Bernu, C. Lhuillier, and L. Pierre, Phys. Rev. Letters 69, 2590 (1992).


Last Modified April 18
Email question/comments/corrections to rmartin@uiuc.edu .