Poisson Numerical
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Transcript of 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