Transport properties of junctions and lattices via solvable model
description
Transcript of Transport properties of junctions and lattices via solvable model
Transport properties of junctions and lattices via solvable model
Nikolai Bagraev ([email protected]), A.F. Ioffe Physico-Technical Institute,St. Petersburg, Russia
Lev Goncharov ([email protected]), Department of Physics of St. Petersburg State University, Russia
Gaven Martin (G. J. [email protected]), New Zealand Institute of Advanced Study, New Zealand
Boris Pavlov ([email protected]) Department of Physics of St. Petersburg State University, Russia
Adil Yafyasov ([email protected]), Department of Physics of St. Petersburg State University, Russia
Quantum networks
• Quantum network constructed on the surface of semiconductor as a union of quantum wells Ωk and quantum wires ωi
• Transport of electrons through the network described by the Schrödinger-type equation
δ
Quasi-1D quantum wires ωi width δ
Quantum wells Ωk
2 2
2 2: , :
( )
mE mV
V
2
Quasi-one-dimensional quantum wiresSplitting of variables allows to modify equation on wires
2 2 2
2 2
( )( , ) ( , ) ( )
2 sin , ( , ) ;
nn
n n n s s sn
x nx y x y xx
ne y x y e P e e
2
2
Spectra on the semi-infinite wires
2
2
4
2
2
9
2
2
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3
Δ1
Δ2
Δ3
ΔTλF
•Consider the Fermi level inside the first spectral band Δ1
•Assume the temperature to be low, so that essential spectral interval ΔT is inside Δ1
2 2
2.
2 2
2.
. .
: ,
: ,
ss open ch
ss closed ch
s s s ss open ch s closed ch
nn channel n isopen P P
nn channel n is closed P P
K P K P
Λ1
Λ2
Λ3
Λ4
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Dirichlet-to-Neumann map
Γ1
Γ2
Γ3
i
Ω
\
( ) :
0 :
V DNn
u Vu uuu DN un
u u
DN DNP DN P P DN PDN
DN DNP DN P P DN P
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Scattering matrix and intermediate DN-map
• Intermediate DN-map DNΛ is a finite-dimensional DN-map of Schrödinger problem with partial-zero boundary condition:
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1
1( ) ( )
k
iK x iK x iK xk l l
l
e e e Se e se
S iK DN iK DNIwith DN DN DN DN
DN K
Exact finite-dimensional equation on scattering matrix
Γ1
Γ2
Γ3
\0
0
u Vu uu
P u
P u matching condition
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Singularities of intermediate DN-map
• Inherited singularities from DNΓ
• Zeros of DN--+K-
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IDN DN DN DNDN K
DNΛ may have singularities of two types:
But singularities of first type compensate each other
1
1 1
1
, , ( )
s
s s
s s
s
ss s ss
DN K DNn n
IL T Q T Tn K K
IJ P K PK K
( )I IDN K K K J T J T
K K I L Q
Silicon-Boron two-dimensional structure
• Experiment shows high mobility of charge carriers on double-layer quasi-two-dimensional silicon-boron structure
• Boron atoms at high concentration form sublattice in silicon matrix
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- no boron
- B++B-
Model description
Consider the boron sublattice as a periodic quantum network
•Elements of the network are connected by aid of rather long and narrow links
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Model description• Separation of variables and cross-section
quantization on the links generate infinite number of spectral channels
• Only finite number of spectral channels is open (oscillating solutions of Schrödinger equation on the links)
• Closed channels (exponentially decreasing solutions of Schrödinger equation on the links) could be omitted
• Matching on the open channels only allow to reduce the infinite-dimension matching problem to finite-dimensional one
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Statement of periodic spectral problem( ) , 0
, 0
l l l l l
l ll l
V x P P
P P P Pn n
Intermediate problem for single element of the lattice
( )
0
V x
P
P matching condition
: uDN u P u En
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Spectral problem with partial quasi-periodic boundary condition on the pairs of opposite slots
• Now we can exclude links and make respective changes in boundary conditions
• Boundary data and boundary currents then are connected by intermediate partial DN-map DNΛ (but not traditional partial DN-map)
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Spectral problem with partial quasi-periodic boundary condition on the pairs of opposite slots
2
2
, ,
, ( ) ,
scaled energyof cross-section confinment
a - length of the links
ls
s s
ls
s s
ip al l l l
l open l openchannels channels
ip al l l l
l open l openchannels channels
ls l l
e
en n
with
p and
Γ2+
Γ2-
Γ1+Γ1
-
Excluding links and correct boundary conditions
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Assumption• To simplify following calculations consider a case, when only one
spectral channel in cylindrical links is open, so• That simplify above boundary conditions as:
1 1s s s s sP e e e e
1
1
2
2
ss s
s
s s
ip a
ip a
P e P
P e Pn n
1 1
2 2
1
2 21 1 1 1
1 1 1 11 1 2 2 1 1 2 2
2 2 2 22 2
2 22 2
2
1
,
100
ip a ip a
ip a ip a
ip a
e e
P P P Pe e
e
1
1 1
2
2 1 22 2
0 00 01
, , ,0
1 0 1
ip a
ip a ip a
e
e e
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Dispersion relation• Connect boundary data and boundary currents with DNΛ
1 1 2 2 1 1 2 2
1 1 1 1 2 2
2 1 1 2 2 2
1 2 1 211 12
2 1 221 22
, 0
0
0
, ,det
, ,
s t
DN
in consideration of
DN DN
DN DN
and note theconditionof existenceof non trivial Bloch function
DN DN
DN DN
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Double periodic quasi-2D lattice• Assume, that two boron sublattices interact by
means of tunneling through the slot Γ0
Ωu is a period of first sublattice and Ωd is a period of the second one
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Double-lattices quasi-periodic boundary conditions
• These conditions impose a system of homogeneous linear equations on
• And we can note the condition of existence of non-trivial Bloch functions
0 0
0
0
2, ,
, ,2
00
00
00
ss s
s
s s
u u
d
d
ip au d u d
u d u dip a
u
uu
d d
d
P e P
P e Pn n
and tunneling boundary condition
P Pn
PPn
1 2 0 0 1 2, , , , ,u u d du d
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Dispersion relation, ,
, 11 ,
, , 1 ,11 12 , 10
, , , 2 ,21 22 , 20
, 1 , 2 ,01 , 02 , 00
1 , 1 1 , 2, 11 , , 12 ,,
2 , 1 2, 21 , , 22
:
,
( ) ,
, ,
( )
u d s u d ts t u d u d
u d u d u du d
u d u d u d u du d
u d u d u du d u d
u d u du d u d u d u du d
T u d uu d u d u d
d DN
d d DN
DN p d d DN
DN DN DN
DN DNDN p
DN DN
, 2
,d
u d
And dispersion relation is
2 det det det det 0u d u dT TDN DN DN DN
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Dispersion relation2 det det det det 0u d u d
T TDN DN DN DN
det 0 det 0u dT TDN and DN
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• If β→∞, linear system splits in two independent blocks
• If β is finite, then intersection of terms transforms to quasi-intersection
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N.T. Bagraev, A.D. Bouravleuv, L.E. Klyachkin, A.M. Malyarenko, V.V.Romanov, S.A. Rykov: Semiconductors, v.34, N6, p.p.700-711, 2000.
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