1999 International Conference on Simulation of Semiconductor Processes and Devices. SISPAD'99 (IEEE Cat. No.99TH8387)
DOI: 10.1109/sispad.1999.799301
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Full-band quantum transport simulation based on tight-binding Green's function method

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Cited by 2 publications
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“…where τ encodes the elements of the coupling Hamiltonian between contact and device, and g B is the surface GF of the semi-infinite reservoir. The problem of the coupling to reservoirs then reduces to the calculation of the contact GF g B , which can be achieved via surface GF methods using decimation techniques [48,49], conformal maps [50] or complex band methods [51][52][53][54]. Similar surface GF approaches can also be used for photons [41,55] or phonons [35,56,57] in systems that are open in the optical or vibrational sense, respectively.…”
Section: Interaction Self-energiesmentioning
confidence: 99%
“…where τ encodes the elements of the coupling Hamiltonian between contact and device, and g B is the surface GF of the semi-infinite reservoir. The problem of the coupling to reservoirs then reduces to the calculation of the contact GF g B , which can be achieved via surface GF methods using decimation techniques [48,49], conformal maps [50] or complex band methods [51][52][53][54]. Similar surface GF approaches can also be used for photons [41,55] or phonons [35,56,57] in systems that are open in the optical or vibrational sense, respectively.…”
Section: Interaction Self-energiesmentioning
confidence: 99%
“…In the case of broken translational invariance caused by the use of nanostructures, the size of the eigenvalue problem in (53) will increase by the dimension of the unit cell in the direction of aperiodicity, while the dimension of the reciprocal space is correspondingly reduced. However, the system is not elastically open in the sense that a scattering problem needs to be solved, i.e., the vibrational state can be described in terms of vibrational eigenmodes in all dimensions.…”
Section: Non-interacting Isolated Subsystemsmentioning
confidence: 99%
“…The whole problem of the coupling to the reservoirs is now reduced to the calculation of the contact GF g R , which in principle is of infinite dimension, but only needs to be known in the close vicinity of the device boundary, owing to the reduced dimensionality of the coupling matrix τ , and can therefore be calculated by surface GF methods using decimation techniques [78,79], conformal maps [80] or complex band methods [81,82,83,53].…”
Section: Contactsmentioning
confidence: 99%
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