Poisson Numerical

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    Solution of the

    Poisson/Laplace Equation

    Dragica Vasileska

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    Electromagnetic Fields

    Time Varying Fields

    Jt

    DH

    t

    BE

    B

    D

    0

    SSC

    SC

    S

    VS

    sdJsdDt

    ldH

    sdBt

    ldE

    sdB

    dvsdD

    0

    Maxwells Eq. in Diff. Form Maxwells Eq. in Integral Form

    EJHBED

    ,,

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    Poissons Equation

    We have the differential form of Gauss law

    Using D = E and E = - in the above equation, we

    get

    This is the Poissons Equation

    D

    V

    2D = V =-E V

    2V

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    Poisson/Laplace Equation Solution

    Poisson/Laplace Equation

    No knowledge of solving of PDEs

    Method of images

    With knowledge for solving of PDEs

    Theoretical Approaches

    Numerical Methods:

    finite difference

    finite elementsPoisson

    Greens function method

    Laplace

    Method of separation of variables(Fourier analysis)

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    Numerical Solutions Procedures

    Governing

    Equations

    ICS/BCS

    Discretization

    System of

    Algebraic

    Equations

    Equation

    (Matrix)

    Solver

    Approximate

    Solution

    Continuous

    Solutions

    Finite-Difference

    Finite-Volume

    Finite-Element

    Spectral

    Boundary Element

    Hybrid

    Discrete

    Nodal

    Values

    Tridiagonal

    ADI

    SOR

    Gauss-Seidel

    Krylov

    Multigrid

    DAE

    Ui(x,y,z,t)

    p(x,y,z,t)

    T(x,y,z,t)

    or

    (,,, )

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    Poisson Equation Application

    Electromagnetic Problems

    Electronics Devices

    Biological Systems

    .

    .

    .

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    Electronics Devices

    Understand the operation of different semiconductor devices:

    - Diodes

    - BJTs

    - MOSFETs

    - MESFETs

    - HEMTs

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    Physical Device Simulation

    There are two main components inany physical device simulator:

    - Characterization of chargemotion due to driving forces anddiffusion process (transport)

    - Fields due to charge distribution

    and motion

    Recessed MOSFET represented on 3D mesh

    over finite domain (courtesy of S. M. Goodnick)

    Initialize Data

    Field Solver

    Transport Kernel

    yes

    no Criterionsatisfied?

    START

    STOP

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    Biological Ion Channels

    Proteins that form nanoscopic aqueous tunnels in cell membrane

    Enormous range of Biological functions

    - regulate ion flow and composition inside cell

    - control electrical signaling in the nervous system

    - muscle contraction, drug delivery

    Disease malfunctioning channels

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    Channels are naturally occurring device elements

    Nanoscale devices with ~0.2-15nm in diameter and between 0.3-10nm

    length

    self-assembled

    perfectly reproducible

    have many specific built-in features and functions can be mutated

    Channels can be designed with specific conductances, selectivities and

    functions

    So, why are we interested in ion channels ??

    http:// www.rcsb.org/pdb

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    nanoHUB.orgonline simulations and more

    Network for Computational Nanotechnology

    A pn-diode has NA=ND=1016 cm-3 doping and a length of 1 um of both p and n-

    regions. Calculate analytically and verify via simulations the values of the:(a) Built-in voltage Vbi(b) Total depletion region width W.

    (c) Maximum electrical field at the metallurgical junction.

    Analytically, the built-in voltage

    is calculated using:

    2ln 0.69A Dbi T

    i

    N NV V V

    n

    One can also extract thebuilt-in voltage from the energy

    band diagram using:

    1

    bi Cp CnV E Eq

    Vbi

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    nanoHUB.orgonline simulations and more

    Network for Computational Nanotechnology

    Example 1: Charge Density

    W

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    nanoHUB.orgonline simulations and more

    Network for Computational Nanotechnology

    Example 1: Electric Field Profile

    Emax