Title: Presentazione di PowerPoint
1ICTT19 19th International Conference on Transport
Theory
Budapest, July 24-30, 2005
Wigner approach to a new two-band envelope
function model for quantum transport
Omar Morandi Dipartimento di Elettronica e
Telecomunicazioni omar.morandi_at_unifi.it
Giovanni Frosali Dipartimento di Matematica
Applicata G.Sansone giovanni.frosali_at_unifi.it
2Plain of the talk
- Mathematical setting
- Well posedness of the Multiband-Wigner system
- Description of the numerical algorithm
3Problem setting unperturbed system
- Homogeneous periodic crystal lattice
- Time-dependent evolution semigroup
4Multiband models derivation
Wannier envelope function
Wannier function
5Multiband models derivation
6MEF model derivation
Wannier function
Bloch function
Our approach
- To get our multiband model in Wannier basis
- We recover un approximate set of equation for
in the Bloch basis - (momentum space)
- We Fourier transform the equations obtained
(coordinate space)
7MEF model characteristics
Hierarchy of kp multiband effective mass
models, where the asimptotic parmeter is the
quasi-momentum of the electron
- Direct physical meaning of the envelope function
- Easy approximation (cut off on the index band)
- Highlight the action of the electric field in
the interband transition phenomena - Easy implementation Wigner and
quantum-hydrodynamic formalism
8MEF model derivation
9MEF model formal derivation
Evaluation of matrix elements
Kane momentum matrix
10MEF model derivation
11MEF model derivation
- Our aim simplify the above equation.
Interband term
12MEF model derivation
Approximate system
We write it in coordinate space
13MEF model first order
Physical meaning of the envelope function
The quantity represents the
mean probability density to find the electron
into n-th band, in a lattice cell.
14MEF model first order
Effective mass dynamics
Zero external electric field exact electron
dynamic
15MEF model first order
Coupling terms
- intraband dynamic
- interband dynamic
- first order contribution of
-
transition rate of Fermi Golden rule
16Kane model
Problems in the practical use of the Kane model
- Strong coupling between envelope function
related - to different band index, even if the external
field is null
17Wigner picture
Wigner function
Phase plane representation pseudo
probability function
18Wigner picture
n-th band component
matrix of operator
General Schrödinger-like model
19Wigner picture
Multiband Wigner function
Evolution equation
20Wigner picture
Multiband Wigner function
Evolution equation
21Two band Wigner model
Wigner picture
Moments of the multiband Wigner function
represents the mean
probability density to find the electron into
n-th band, in a lattice cell.
22Two band Wigner model
Wigner picture
23Two band Wigner model
Wigner picture
- intraband dynamic zero coupling if the external
potential is null
24Two band Wigner model
Wigner picture
- intraband dynamic zero coupling if the external
potential is null
- interband dynamic coupling like G-R via
25Mathematical setting
1 D problem
Hilbert space
Weighted spaces
26Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
27Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
Stone theorem
unitary semigroup on
Unbounded operator
28Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
29Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
Symmetric bounded operators
30Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
The operator generate
semigroup
The unique solution of (1) is
31Numerical implementation splitting scheme
Linear evolution semigroup
Uniform mesh
is a three element vector
32Numerical implementation splitting scheme
f.f.t.
Approximate solution of
33Numerical implementation splitting scheme
f.f.t.
Approximate solution of
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35Conduction band
x
p
Momentum coordinate
Space coordinate
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37Stationary state Thermal distribution
Conduction band
Valence band
38Conclusion
- Well posedness of the Multiband-Wigner system
Next steps
- Extention of MEF model to more general
semiconductor
- Well posedness of Multiband-Wigner model coupled
with Poisson eq.
- Calculation of I-V IRDT characteristic for
self-consistent model