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Some features of creating GRID structure for simulation of nanotransistors. Bolormaa Dalanbayar , Batnyam Battulga. National Universiry of Mongolia School of Information Technology. Outline. About SIT Why parallel computation in SIT curricula? Nanoelectronics development
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Some features of creating GRID structure for simulation of nanotransistors Bolormaa Dalanbayar, Batnyam Battulga National Universiry of Mongolia School of Information Technology
Outline • About SIT • Why parallel computation in SIT curricula? • Nanoelectronics development • Siesta and parallel processing in SIT • Conclusion
Introduction • Presented work – small GRID structure based Unicore software technology • DFT simulation of a bulk silicon using Siesta package
School of Information Technology • 1967 – First Radio-Electronic Engineers • 1990 – Electronics Department • 2002 – School of Information Technology
School of Information Technology Departments: • Electronics • Computer and Information Technology • Communication Technology Research centers: • Research center of NLP • Research center of Mobile and Embedded technology • Animation studio
Why parallel computation in SIT curricula? • Nano electronics in Electronics curricula :
Why parallel computation in SIT curricula? • 2010-2011 Matlab simulation (Landauer-Buttiker formalism, SC Iteration, NEGF,…) • 2011-2012 First ab-initio simulation in Siesta (Linear-scaling DFT )
Nanoelectronics development • Nanotransistor development: - Experimental - Computational • Nanotransistor modeling : - physical process simulation (ab initio,…) - characteristic simulation (NEGF approach,…) - TCAD (Silvaco, Synopsis…)
Simulation and Method Solving the 3D Poisson equation for the electrostatic potential Solving the 2D, 1D Schrodinger equations Solving the coupled or uncoupled nonequilibrium Green function (NEGF) transport equations for the electron charge density. Numerical simulation of ID
Simulation and Method: Matlab • The computed log(ID) vs. VGtransfer characteristics of a ballistic SNWFET with a SiO2 insulator layer (k = 3:9 and 25)
Simulation and Method: Matlab • The computed ID vs. VDcommon source characteristics of ballistic SNWFET with a HfO2 insulator layer (k = 3:9 and 25)
Nanoelectronics development Many electron problem: • Quantum Chemistry (Hartree-Fock, CI…) • Quantum Monte Carlo • Perturbation theory (propagators) • Density Functional Theory (DFT) Very efficient and general BUT implementations are approximate and hard to improve (no systematic improvement)
Siesta and parallel processing in SIT • Nano transistor (device physics) – atomistic models Gabriele Penazzi, PhD dissertation Rome, June 2010.
Siesta and parallel processing in SIT • Nano transistor (device physics) continuous models Gabriele Penazzi, PhD dissertation Rome, June 2010.
Siesta and parallel processing in SIT • Atomistic models: - Siesta - GROMACS - VASP - CASDEP - ABINIT …
Siesta and parallel processing in SIT • Siesta Methods: - Born-Oppenheimer (relaxations, mol.dynamics) - DFT (LDA, GGA) - Pseudopotentials (norm conserving,factorised) - Numerical atomic orbitals as basis (finite range) - Numerical evaluation of matrix elements (3Dgrid)
Siesta and parallel processing in SIT • Pseudopotential of Si:
Siesta and parallel processing in SIT • Carrier charge:
Siesta and parallel processing in SIT • Bulk Si
Siesta and parallel processing in SIT • Used UNICORE 6
Conclusion • Double site configuration
Conclusion Performed calculations in double site UNICORE GRID site: • Matlab code of NEGF • Feature selection Matlab code • DFT Siesta code • Band structure Siesta code
Conclusion Future plan: • Development of cluster • Testing of Torque • Repeating our calculations • Creation of education site map in UB