Semiconductor Switch Simulations Texas Tech U. & Sandia National Labs

Slides:



Advertisements
Similar presentations
1 M. Zarcone Istituto Nazionale per la Fisica della Materia and Dipartimento di Fisica e Tecnologie Relative, Viale delle Scienze, Palermo, Italy.
Advertisements

A New Design Tool for Nanoplasmonic Solar Cells using 3D Full Wave Optical Simulation with 1D Device Transport Models Liming Ji* and Vasundara V. Varadan.
Computational Electronics Generalized Monte Carlo Tool for Investigating Low-Field and High Field Properties of Materials Using Non-parabolic Band Structure.
Department of Aeronautics and Astronautics NCKU Nano and MEMS Technology LAB. 1 Chapter III June 1, 2015June 1, 2015June 1, 2015 Carrier Transport Phenomena.
CHAPTER 3 Introduction to the Quantum Theory of Solids
Chapter 13 Light and Reflection.
Department of Aeronautics and Astronautics NCKU Nano and MEMS Technology LAB. 1 Chapter IV June 14, 2015June 14, 2015June 14, 2015 P-n Junction.
Capacitance Dielectrics 11/12/08. Table 26-1, p.812.
Figure 1.1 The observer in the truck sees the ball move in a vertical path when thrown upward. (b) The Earth observer views the path of the ball as a parabola.
Answers to Questions from Lecture 4 Q1: How old is the cyclotron resonance method of determining the effective mass of electrons and holes in semiconductors?
Modeling, Characterization and Design of Wide Bandgap MOSFETs for High Temperature and Power Applications UMCP: Neil Goldsman Gary Pennington(Ph.D) Stephen.
Computational Solid State Physics 計算物性学特論 第9回 9. Transport properties I: Diffusive transport.
MURI CONSORTIUM on COMPACT, PORTABLE PULSED POWER
Tzveta Apostolova Institute for Nuclear Research and Nuclear Energy,
TIM GFROERER, Davidson College Davidson, NC USA
Prof. John A. Copeland ECE Georgia Tech
Simulation of Current Filaments in Photoconductive Semiconductor Switches K. Kambour, H. P. Hjalmarson, F. J. Zutavern and A. Mar Sandia National Laboratories*
Modeling, Characterization and Design of Wide Bandgap MOSFETs for High Temperature and Power Applications UMCP: Neil Goldsman Gary Pennington(Ph.D) Stephen.
Theory of Electrons in Solids Lu J. Sham, University of California San Diego, DMR Fig. 1 Nuclear bath trajectories An electron is confined in a.
Mobility 2 The average momentum is proportional to the applied force, which is qE. The electrons, on an average, collide in time n (called momentum relaxation.
Global Modeling of High Frequency Circuits and Devices PhD defense by Julien Branlard Committee chairman: Dr. M. Saraniti, (ECE, IIT) Committee members:Dr.
ECEE 302: Electronic Devices
This cartoon mixes 2 legends: 1. Legend of Newton, the apple & gravity which led to the Universal Law of Gravitation. 2. Legend of William Tell & the apple.
INFSO-RI Enabling Grids for E-sciencE SALUTE – Grid application for problems in quantum transport E. Atanassov, T. Gurov, A. Karaivanova,
Development of an analytical mobility model for the simulation of ultra thin SOI MOSFETs. M.Alessandrini, *D.Esseni, C.Fiegna Department of Engineering.
High E Field Transport BW: Sect. 8.10, p 198YC, Sect. 5.4; S, Sect. 4.13; + Outside sources.
Lecture 1 - Review Kishore Acharya. 2 Agenda Transport Equation (Conduction through Metal) Material Classification based upon Conductivity Properties.
Introduction to semiconductor technology. Outline –4 Excitation of semiconductors Optical absorption and excitation Luminescence Recombination Diffusion.
Noise in Semiconductors
Physics of carbon nanotube electronic devices M.P. Anantram and F.Leonard – Center for Nanotechnology, NASA Ames Research Center – Nanoscale Science and.
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Velocity Saturation Effects. Ohm’s “Law” This says the Drift Velocity V d is linear in the electric field E: μ  Mobility If this were true for all E,
Compact Power Supplies Based on Heterojunction Switching in Wide Band Gap Semiconductors NC STATE UNIVERSITY UCSB Steady-State and Transient Electron Transport.
1 ME 381R Lecture 13: Semiconductors Dr. Li Shi Department of Mechanical Engineering The University of Texas at Austin Austin, TX
High Resolution Energy Loss Spectroscopy of “Sheet” Plasmons Roy F. Willis, Department of Physics, The Pennsylvania State University University Park, PA.
Energy Bands and Charge Carriers in Semiconductors
Semiconductor Device Modeling
Electronics & Communication Engineering
Semiconductor Device Modeling
The Electric Field Due to continuous Charges
“Low Field”  Ohm’s “Law” holds J  σE or vd  μE
Dynamical correlations & transport coefficients
Lecture 27 OUTLINE The BJT (cont’d) Breakdown mechanisms
DOE Plasma Science Center Control of Plasma Kinetics
Photodetectors.
Introduction to Nanoheat; Aspel group
HP Printer Tech Support Phone Number
Lecture #8 OUTLINE Generation and recombination
K. Kambour, H. P. Hjalmarson, F. J. Zutavern and A. Mar
Lecture 27 OUTLINE The BJT (cont’d) Breakdown mechanisms
Basics Semiconductors
Fig. 3-1: Optical fiber attenuation
Dynamical correlations & transport coefficients
Fig. 1. Nonlinear relationship between D and E at high optical E field
Review of semiconductor physics
Project-X Status Report
Figure (a) Physical arrangement of a p–n junction
Chapter 14 Monte Carlo Simulation
Demonstration of optical flipping in NO
PbWO4 Cherenkov light contribution to Hamamatsu S8148 and Zinc Sulfide–Silicon avalanche photodiodes signals F. KOCAK, I. TAPAN Department of Physics,
Figure (a) Physical arrangement of a p–n junction
Ballistic miniband conduction in a graphene superlattice
Fig. 4 From reversibility to the breakdown of collective Heisenberg model simulation. From reversibility to the breakdown of collective Heisenberg model.
Device Technology for GaN Power Electronics
Yalchin Efendiev Texas A&M University
We are independent provider of technical support services. All the trademarks, names and logos on this site are the properties of their respective owners and are shown for reference purposes only. We disclaims any association or ownership of such third pa
Fig. 2 Latitudinal changes in the sea-ice drivers.
Fig. 1 Structure and basic properties of EuTiO3 (ETO) films.
Fig. 2 Comparison between the different reflective metasurface proposals when θi = 0° and θr = 70°. Comparison between the different reflective metasurface.
Fig. 5 Modeling of the ASE threshold using the kinetic equations and experimental parameter inputs. Modeling of the ASE threshold using the kinetic equations.
Presentation transcript:

Semiconductor Switch Simulations Texas Tech U. & Sandia National Labs Goals Simulations: Breakdown & “lock-on” in photoconductive semiconductor switches (PCSS’s) Understand the behavior of GaAs, Si, & InP PCSS’s at 4 to 30 kV/cm fields. Approach Collective impact ionization theory: Effect of carrier-carrier scattering on impact ionization. Simulations: Ensemble Monte Carlo & Maxwellian distribution Results: Generalized Breakdown Breakdown & “lock-on”: Two aspects of the same phenomenon Steady state electric field (F) & carrier density dependence (n) of breakdown Personnel: Ken Kambour, PhD student/Sandia visitor; H.P. Hjalmarson (Sandia), C.W. Myles (TTU) Fig. 1. Photoconductive switch (PCSS) with optical illumination and current filaments Fig. 2. Generalized Breakdown (Model Material): n vs. F: Minimum F on curve = Breakdown field without (red) & with (blue) carrier-carrier (CC) scattering.  CC-scattering lowers the breakdown field. “Lock-on” = Breakdown with CC scattering.