Extracting density information from finite Hamiltonian matrices - PowerPoint PPT Presentation

About This Presentation
Title:

Extracting density information from finite Hamiltonian matrices

Description:

Extracting density information from finite Hamiltonian matrices We demonstrate how to extract approximate, yet highly accurate, density-of-state information over a ... – PowerPoint PPT presentation

Number of Views:84
Avg rating:3.0/5.0
Slides: 27
Provided by: AD57
Category:

less

Transcript and Presenter's Notes

Title: Extracting density information from finite Hamiltonian matrices


1
Extracting density information from finite
Hamiltonian matrices
  • We demonstrate how to extract approximate, yet
    highly accurate, density-of-state information
    over a continuous range of energies from a finite
    Hamiltonian matrix. The approximation schemes
    which we present make use of the theory of
    orthogonal polynomials associated with
    tridiagonal matrices. However, the methods work
    as well with non-tridiagonal matrices. We
    demonstrate the merits of the methods by applying
    them to problems with single, double, and
    multiple density bands, as well as to a problem
    with infinite spectrum.

2
  • With every Hamiltonian (hermitian matrix), there
    is an associated positive definite density of
    states function (in energy space).
  • Simple arguments could easily be under-stood when
    the Hamiltonian matrix is tridiagonal.
  • We exploit the intimate connection and interplay
    between tridiagonal matrices and the theory of
    orthogonal polynomials.

3
(No Transcript)
4
  • Solutions of the three-term recursion relation
    are orthogonal polynomials.
  • Regular pn(x) and irregular qn(x) solutions.
  • Homogeneous and inhomogeneous initial relations,
    respectively.

5
  • pn(x) is a polynomial of the first kind of
    degree n in x.
  • qn(x) is a polynomial of the second kind of
    degree (n?1) in x.
  • The set of n zeros of pn(x) are the
    eigenvalues of the finite n?n matrix H.
  • The set of (n?1) zeros of qn(x) are the
    eigenvalues of the abbreviated version of this
    matrix obtained by deleting the first raw and
    first column.

6
  • They satisfy the Wronskian-like relation
  • The density (weight) function associated with
    these polynomials
  • The density function associated with the
    Hamiltonian H

7
y
G00(xiy)
x
?
?
?
?
Discrete spectrum of H
Continuous band spectrum of H
8
Connection
9
For a single limit The density is single-band
with no gaps and with the boundary
For some large enough integer N
10
Note the reality limit of the root and its
relation to the boundary of the density band
11
One-band density example
12
Two-Band Density
giving again a quadratic equation for T(z)
The boundaries of the two bands are obtained from
the reality of T as
13
Two-band density example
Three-band density example
Infinite-band density example
14
Asymptotic limits not known?
  • Analytic continuation method
  • Dispersion correction method
  • Stieltjes Imaging method

15
Non-tridiagonal Hamiltonian matrices?
Solution will be formulated in terms of the
matrix eigenvalues instead of the
coefficients .
16
Analytic Continuation
?
?
?
?
?
?
?
?
?
17
(No Transcript)
18
One-Band Density
Two-Band Density
Infinite-Band Density
19
Dispersion Correction
Gauss quadrature
Numerical weights
20
(No Transcript)
21
n
4
?
?(?)
3
?
2
?
?
1
?
?
0
?1
?2
?3
?4
?0
22
One-Band Density
Two-Band Density
Infinite-Band Density
23
Stieltjes Imaging
24
Stieltjes Imaging
25
One-Band Density
Two-Band Density
Infinite-Band Density
26
????? ??? ??????? ??????? ??? ???? ???????????
????? ????? ???? ???????
Thank you
Write a Comment
User Comments (0)
About PowerShow.com