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No interband transition are possible if is a Bloch function ... We recover un approximate set of equation for in the Bloch basis (momentum space) ... – PowerPoint PPT presentation

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Title: Presentazione di PowerPoint


1
ICTT19 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
2
Plain of the talk
  • Description of the model
  • Multiband (MEF) model
  • Multiband-Wigner picture
  • Mathematical problem
  • Mathematical setting
  • Well posedness of the Multiband-Wigner system
  • Numerical applications
  • Description of the numerical algorithm
  • Application to IRTD

3
Problem setting unperturbed system
  • Homogeneous periodic crystal lattice


  • Time-dependent evolution semigroup


4
Multiband models derivation
Wannier envelope function
Wannier function
5
Multiband models derivation
6
MEF 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)

7
MEF 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

8
MEF model derivation
9
MEF model formal derivation
Evaluation of matrix elements
Kane momentum matrix
10
MEF model derivation
11
MEF model derivation
  • Our aim simplify the above equation.

Interband term
12
MEF model derivation
Approximate system
We write it in coordinate space
13
MEF 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.
14
MEF model first order
Effective mass dynamics
Zero external electric field exact electron
dynamic
  • intraband dynamic

15
MEF model first order
Coupling terms
  • intraband dynamic
  • interband dynamic
  • first order contribution of

  • transition rate of Fermi Golden rule

16
Kane 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

17
Wigner picture
Wigner function
Phase plane representation pseudo
probability function
18
Wigner picture
n-th band component
matrix of operator
General Schrödinger-like model
19
Wigner picture
Multiband Wigner function
Evolution equation
20
Wigner picture
Multiband Wigner function
Evolution equation
21
Two 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.
22
Two band Wigner model
Wigner picture
23
Two band Wigner model
Wigner picture
  • intraband dynamic zero coupling if the external
    potential is null

24
Two band Wigner model
Wigner picture
  • intraband dynamic zero coupling if the external
    potential is null
  • interband dynamic coupling like G-R via

25
Mathematical setting
1 D problem
Hilbert space
Weighted spaces
26
Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
27
Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
Stone theorem
unitary semigroup on
Unbounded operator
28
Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
29
Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
Symmetric bounded operators
30
Mathematical setting
If the external potential
the two band Wigner system admits a unique
solution
The operator generate
semigroup
The unique solution of (1) is
31
Numerical implementation splitting scheme
Linear evolution semigroup
Uniform mesh
is a three element vector
32
Numerical implementation splitting scheme
f.f.t.
Approximate solution of
33
Numerical implementation splitting scheme
f.f.t.
Approximate solution of
34
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35
Conduction band
x
p
Momentum coordinate
Space coordinate
36
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37
Stationary state Thermal distribution
Conduction band
Valence band
38
Conclusion
  • Multiband-Wigner model
  • Well posedness of the Multiband-Wigner system
  • Application to IRTD

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
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