ece606: solid state devices lecture 13: recombination
TRANSCRIPT
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ECE606: Solid State DevicesECE606: Solid State DevicesLecture 13: Recombination‐Generation
Muhammad Ashraful [email protected]
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Outline
1) N ilib i t1) Non‐equilibrium systems
2) Recombination generation events
3) Steady‐state and transient response
4) Derivation of R‐G formula
5) Conclusion
Ref. Chapter 5, pp. 134‐146
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Current Flow Through Semiconductors
I I G V= ×
VC i
q n Av= × × ×
Depends on chemical composition, crystal structure, temperature, doping, etc.
Carrier Density
velocity
y , p , p g,
Quantum Mechanics + Equilibrium Statistical Mechanics ⇒ Encapsulated into concepts of effective masses
Transport with scattering, non‐equilibrium Statistical Mechanics l d d f d ff h
and occupation factors (Ch. 1‐4)
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⇒ Encapsulated into drift‐diffusion equation with recombination‐generation (Ch. 5 & 6)
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Non‐equilibrium Systems
Chapter 6 Chapter 5Chapter 6 Chapter 5
I
vs.
I
V
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Direct Band‐to‐band Recombination
In real space … In energy space …
Photon
Photon
GaAs, InP, InSb (3D)
Lasers LEDs etc
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Lasers, LEDs, etc.
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Direct Excitonic Recombination
In energy space …
Photon (wavelength?)
CNT, InP, ID‐systems
In real space …
Transistors, Lasers, Solar cells, etc.
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Indirect Recombination (Trap‐assisted)
Phonon
Ge, Si, ….
Transistors, Solar cells, etc.
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Auger Recombination
Phonon (heat)3
( )
12
4
InP, GaAs, …3
Lasers, etc.1 2
4
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Impact Ionization – A Generation Mechanism
1
43
2
Si, Ge, InP
Lasers, Transistors, etc.
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Indirect vs. Direct Bandgap
The top & bottom of bands do not align at
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The top & bottom of bands do not align atsame wavevector k for indirect bandgap material
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Photon Energy and Wavevector
E EEphotonE
=
=
+
+V
V phot
photon
n C
C
o
k k
E E
k
E2πa
photonkV photon C
21 21 in eV
π=
photonE. / 4
2 25 10 m
π πμ−<< =
×a2
in mπ
λ μ=photonk
Photon has large energy for excitation through bandgap,b t it t i li ibl d t i f BZ
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but its wavevector is negligible compared to size of BZ
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Phonon Energy and Wavevector
=+V phon n CoE EE
=+V
V phon
phonon
n C
C
o
k k k
2 2phononk
E/= =
π πλ υ 4
2 25 10 m
π πμ−≈ =
×aphonsound onE/λ υ 5 10 mμ×a
Phonon has large wavevector comparable to BZ,
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but negligible energy compared to bandgap
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Localized Traps and Wavevector
aa
4
2 25 10trap ~k
a mπ π
μ−≈×5 10a mμ×
Trap provides the wavevector necessary for indirect transition
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necessary for indirect transition
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Outline
1) N ilib i t1) Non‐equilibrium systems
2) Recombination generation events
3) Steady‐state and transient response
4) Derivation of R‐G formula
5) Conclusion
Ref. Chapter 5, pp. 134‐146
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Equilibrium, Steady state, Transient
Steady stateSteady stateEquilibrium
n,p)
Device time
(nTransient
)Environment
time
(n,p)Environment
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Detailed Balance: Simple Explanation
2
The rates of exchange of people (particles) between every pair of countries (energy levels) is balanced. Hence the name “Detailed Balance”
MexicoUSA
22
Hence the name Detailed Balance .
Detailed balance is the property of equilibrium
China
3 3
44
The population of each of the countries (energy levels) remains constant under detailed balance.
The concept of detailed balance is powerful because it
India
The concept of detailed balance is powerful, because it can be used for many things (e.g. reduce the number of unknown rate constants by half, and derive particle distributions like Fermi‐Dirac, Bose‐Einstein d b )distributions, etc.)
•9 in & 9 out
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•9 in & 9 out •All numbers are people/unit time.
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Steady‐state ResponseDisturbing the detailed balance requires createDisturbing the detailed balance requires create non‐equilibrium conditions (needs energy). Unidirectional forces (red lines) can create such Non‐equilibrium conditions.
MexicoUSA
32
The rates of exchange of people (particles) between every pair of countries (energy levels) is NOT balanced but the sum of all arrival
China
4 6
45
levels) is NOT balanced, but the sum of all arrival and departures to all countries is zero.
The flux at steady state is balanced overall, but
1
China
India
4the flux is NOT the same as in detailed balance(e.g. 12 in and 12 out in SS vs. 9 in and 9 out for Detailed Balance, for example).
1The population of a country (energy level) remains constant with time after steady state is reached.
O th i t th t t fl t 12 in and 12 out from USA
1
17
One can use the requirement that net flux at steady state be zero to calculate steady state population of a country (Eq. 5.21)
12 in and 12 out from USA
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Detailed Balance, Transient, Steady‐state
MexicoUSA
22 Mexico
USA32 Mexico
USA32
USA
3 3
2
4
USA
3 5
3
51 4 6
51
China 44
China 45
China
I di
4
India India1
Forced unidirectional connections
India1
9 in 9 out Population conserved
Forced unidirectional connections(red lines) disturbs equilibrium (e.g. 9 in/12 out at time t1local populations not conserved, but global population is
12 in 12 out Population stabilized
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but global population is ….
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Outline
1) N ilib i t1) Non‐equilibrium systems
2) Recombination generation events
3) Steady‐state and transient response
4) Derivation of R‐G formula
5) Conclusion
Ref. Chapter 5, pp. 134‐146
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Indirect Recombination (Trap‐assisted)
Phonon
Ge, Si, ….
Transistors, Solar cells, etc.
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Physical view of Carrier Capture/Recombination
(1) Before a capture
TT TN pn= +
(2) After electron capture(3) After hole capture
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Carrier Capture Coefficients
υ tυtht
υ σ×× ×⎡ ⎤= − × ⎢ ⎥×⎣ ⎦T nthAdn n
dt A tt p
21 32 2
*thm kTυ = σ υ≡ − ≡ n tT n hnc cnp
×⎣ ⎦dt A t
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Capture Cross‐section
20n rσ π= Zn capture model …
e116 -22 10 cm−×
e2 h1
156 10−×185 10−×
e3 147 10−×
h1
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Cascade model for capture
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Conclusions
1) There are wide variety of generation‐recombination events
that allow restoration of equilibrium once the stimulus is
removed.
2) Direct recombination is photon‐assisted, indirect
recombination phonon assistedrecombination phonon assisted.
3) Concepts of equilibrium, steady state, and transient
d i h ld b l l d ddynamics should be clearly understood.
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