Hierarchy of simulation approaches for hot carrier transport in deep submicron devices
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[1] K. Jensen,et al. Numerical simulation of transient response and resonant-tunneling characteristics of double-barrier semiconductor structures as a function of experimental parameters , 1989 .
[2] S. Selberherr. Analysis and simulation of semiconductor devices , 1984 .
[3] M. Artaki. Hot‐electron flow in an inhomogeneous field , 1988 .
[4] C. Gardner. Hydrodynamic and Monte Carlo simulation of an electron shock wave in a 1- mu m n/sup +/-n-n/sup +/ diode , 1993 .
[5] Karl Hess,et al. Monte Carlo Device Simulation: Full Band and Beyond , 1991 .
[6] J. Frey,et al. Two-dimensional numerical simulation of energy transport effects in Si and GaAs MESFET's , 1982, IEEE Transactions on Electron Devices.
[7] W. Frensley. Simulation of resonant‐tunneling heterostructure devices , 1985 .
[8] M. Patil,et al. Monte Carlo simulation of real-space transfer transistors: device physics and scaling effects , 1993 .
[9] H. B. Bakoglu,et al. Circuits, interconnections, and packaging for VLSI , 1990 .
[10] M. Claassen,et al. Tunneling and Ionization Phenomena in GaAs Pin Diodes , 1992, ESSDERC '92: 22nd European Solid State Device Research conference.
[11] U. Ravaioli,et al. An improved energy transport model including nonparabolicity and non-Maxwellian distribution effects , 1992, IEEE Electron Device Letters.
[12] Gardner,et al. Smooth quantum potential for the hydrodynamic model. , 1996, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.
[13] W. Frensley,et al. Wigner-function model of a resonant-tunneling semiconductor device. , 1987, Physical review. B, Condensed matter.
[14] Edwin C. Kan,et al. Calculation of velocity overshoot in submicron devices using an augmented drift-diffusion model , 1991 .
[15] T. Ning,et al. Optically induced injection of hot electrons into SiO2 , 1974 .
[16] R. Stratton,et al. Semiconductor current-flow equations (diffusion and degeneracy) , 1972 .
[17] Karl Hess,et al. Theory of hot electron emission from silicon into silicon dioxide , 1983 .
[18] P. A. Childs,et al. Spatially transient hot electron distributions in silicon determined from the chambers path integral solution of the Boltzmann transport equation , 1993 .
[19] C.H. Lee,et al. Simulation of a long term memory device with a full bandstructure Monte Carlo approach , 1995, IEEE Electron Device Letters.
[20] T. H. Ning,et al. Hot-electron emission from silicon into silicon dioxide , 1978 .
[21] Steven E. Laux,et al. Electron states in narrow gate-induced channels in Si , 1986 .
[22] Neil Goldsman,et al. Highly stable and routinely convergent 2-dimensional hydrodynamic device simulation , 1994 .
[23] G. Baccarani,et al. An investigation of steady-state velocity overshoot in silicon , 1985 .
[24] J. F. Verwey,et al. Nonvolatile Semiconductor Memories , 1976 .
[25] Massimo Rudan,et al. MULTI‐DIMENSIONAL DISCRETIZATION SCHEME FOR THE HYDRODYNAMIC MODEL OF SEMICONDUCTOR DEVICES , 1986 .
[26] An analytical formulation of the length coefficient for the augmented drift-diffusion model including velocity overshoot , 1991 .
[27] Numerical simulation of non-homogeneous submicron semiconductor devices by a deterministic particle method , 1993 .
[28] M. Stettler,et al. A critical examination of the assumptions underlying macroscopic transport equations for silicon devices , 1993 .
[29] Y. Kamakura,et al. A Monte Carlo simulation of anisotropic electron transport in silicon including full band structure and anisotropic impact‐ionization model , 1994 .
[30] A. Kriman,et al. Transient Simulation of Ultra-Small GaAs MESFET Using Quantum Moment Equations , 1992, Picosecond Electronics and Optoelectronics.
[31] C. Wang,et al. Metal silicide patterning: a new approach to silicon nanoelectronics , 1996 .
[32] N. Goldsman,et al. Device modeling by deterministic self-consistent solution of Poisson and Boltzmann transport equations , 1992 .
[33] A. Tasch,et al. Simulation program suitable for hot carrier studies: An efficient multiband Monte Carlo model using both full and analytic band structure description for silicon , 1993 .
[34] P. Lugli,et al. A comparison of Monte Carlo and cellular automata approaches for semiconductor device simulation , 1993, IEEE Electron Device Letters.
[35] J. P. Kreskovsky,et al. Transport via the Liouville equation and moments of quantum distribution functions , 1993 .
[36] Karl Hess,et al. Calculation of hot electron distributions in silicon by means of an evolutionary algorithm , 1996 .
[37] K. Blotekjaer. Transport equations for electrons in two-valley semiconductors , 1970 .
[38] Richard M. Martin,et al. Ab initio analysis of the electron-phonon interaction in silicon , 1993 .
[39] Kenji Taniguchi,et al. Analytical device model for submicrometer MOSFET's , 1991 .
[40] R. Stratton,et al. Diffusion of Hot and Cold Electrons in Semiconductor Barriers , 1962 .
[41] L. Register,et al. Numerical simulation of mesoscopic systems with open boundaries using the multidimensional time‐dependent Schrödinger equation , 1991 .
[42] Ferry,et al. Self-consistent study of the resonant-tunneling diode. , 1989, Physical review. B, Condensed matter.
[43] S. Luryi,et al. Novel real-space hot-electron transfer devices , 1983, IEEE Electron Device Letters.
[44] W. Pötz. Self‐consistent model of transport in quantum well tunneling structures , 1989 .
[45] M. Stettler,et al. Formulation of the Boltzmann equation in terms of scattering matrices , 1993 .
[46] M. Fischetti. Monte Carlo simulation of transport in technologically significant semiconductors of the diamond and zinc-blende structures. I. Homogeneous transport , 1991 .
[47] Chi-Wang Shu,et al. The Response of the Hydrodynamic Model to Heat Conduction, Mobility, and Relaxation Expressions , 1995 .
[48] W. Fawcett,et al. Monte Carlo determination of electron transport properties in gallium arsenide , 1970 .
[49] Karl Hess,et al. Negative differential resistance through real‐space electron transfer , 1979 .
[50] Multidimensional augmented current equation including velocity overshoot , 1991, IEEE Electron Device Letters.
[51] Varani,et al. Generalization of Thermal Conductivity and Lorenz Number to Hot-Carrier Conditions in Nondegenerate Semiconductors. , 1996, Physical review letters.
[52] K. Thornber,et al. Current equations for velocity overshoot , 1982, IEEE Electron Device Letters.
[53] C. Jacoboni,et al. The Monte Carlo method for the solution of charge transport in semiconductors with applications to covalent materials , 1983 .
[54] Macucci,et al. Quasi-three-dimensional Green's-function simulation of coupled electron waveguides. , 1995, Physical review. B, Condensed matter.
[55] N. Goldsman,et al. A physics-based analytical/numerical solution to the Boltzmann transport equation for use in device simulation , 1991 .
[56] A. Gnudi,et al. Two-dimensional NOSFET Simulation by means of Multidimensional Spherical Harmonics Expansion of the Boltzmann Transport Equation , 1992, ESSDERC '92: 22nd European Solid State Device Research conference.
[57] T. Tang,et al. Transport coefficients for a silicon hydrodynamic model extracted from inhomogeneous Monte-Carlo calculations , 1992 .
[58] Zhiping Yu,et al. Formulation of Macroscopic Transport Models for Numerical Simulation of Semiconductor Devices , 1995 .
[59] P. J. Price,et al. Monte Carlo calculations on hot electron energy tails , 1977 .
[60] P. Lugli,et al. The Monte Carlo Method for Semiconductor Device Simulation , 1990 .
[61] J. P. Kreskovsky,et al. Electron diffraction through an aperture in a potential wall , 1989 .
[62] A. T. Galick,et al. Efficient numerical simulation of electron states in quantum wires , 1990 .