2009
DOI: 10.1016/j.jcp.2009.08.001
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Optimal block-tridiagonalization of matrices for coherent charge transport

Abstract: Numerical quantum transport calculations are commonly based on a tight-binding formulation. A wide class of quantum transport algorithms requires the tight-binding Hamiltonian to be in the form of a block-tridiagonal matrix. Here, we develop a matrix reordering algorithm based on graph partitioning techniques that yields the optimal block-tridiagonal form for quantum transport. The reordered Hamiltonian can lead to significant performance gains in transport calculations, and allows to apply conventional two-te… Show more

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Cited by 59 publications
(59 citation statements)
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“…12 Moreover, we compare the results to the LandauZener approximation for ballistic systems. The electron mean free path l e is estimated from the disorder strength.…”
Section: A Numerical Methodsmentioning
confidence: 99%
“…12 Moreover, we compare the results to the LandauZener approximation for ballistic systems. The electron mean free path l e is estimated from the disorder strength.…”
Section: A Numerical Methodsmentioning
confidence: 99%
“…Alternative approaches have been developed to treat arbitrarily shaped regions with multiple leads [12,13,30]. These so-called knitting algorithms add single sites at a time.…”
Section: Adaptive Recursion For Device Regionmentioning
confidence: 99%
“…Although variants of the method can be used for arbitrary geometries and multiple leads [12][13][14], the method remains limited * mikse@nanotech.dtu.dk to finite-width or periodic systems. Consequently, it cannot describe local and nonperiodic perturbations, or pointlike probes similar to those considered experimentally [15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…More recent work on the contact-block reduction method 16 divides a generic device into smaller blocks which are pieced together like a jig-saw puzzle. In addition, graph theory has been used to develop a relatively elaborate system permitting the use of LRGF with generic boundary conditions 28 . These results, along with others 21 , suggest the approach we explore in depth in this article, however we argue that the formalism of the "virtual lead" is not necessary.…”
Section: The Outward Wave Methodsmentioning
confidence: 99%
“…To understand how each method contributed to the optimization function, we also plot the size of each matrix that must be inverted for the LRGF and Outward Wave methods for stadia of system size parameter 10 and 40 in Figure 5 as in Wimmer and Richter 28 . The area underneath each function is the same and adds to the total number of orbitals in each system.…”
Section: B Relativistic Stadiums Of Various Sizesmentioning
confidence: 99%