Microscopic self-consistent theory of Josephson junctions including dynamical electron correlations
Lecture 4 microscopic theory
-
Upload
allenhermann -
Category
Technology
-
view
244 -
download
1
Transcript of Lecture 4 microscopic theory
Lecture 4 Microscopic Theory
•The 2-Electron Problem •Second Quantization: •Annihilation and Creation Operators •Solution of the 2-electron Schroedinger Equation •Cooper Pairs •The many-electron problem-BCS Theory •Solution of the Many-particle Schroedinger Equation by the Bogoliubov-Valatin Transformation •The BCS Energy gap
Even number of electrons/unit cell
Band picture - electrons in momentum space
electrons in a periodic potential form Bloch waves and energy bands
Bloch waves
n,k (r ) e
ik r u
n.k (r ) Energy eigenvalues
n (k )
Odd number of electrons/unit cell E
metal insulator semiconductor
E
energy gap
Repulsive interaction between electrons is a perturbation
Fermi sea
Fermi liquid of “independent” Quasiparticles (Landau, 1956)
Insulator, Semiconductor
Metal
Phonon Coupling The Cooper Pair Problem
+ + + +
+ + + + Analogy
+ + + + 2 Bowling Balls on a
- + + + + MATTRESS
Cooper Pairing
Many electron system
+ + _ + +
† †
1122
21 ,kqkkqk
kkqCCCCVH
Consider a subset of the many – electron system , i.e. a Cooper pair, with 2 free electrons with antiparallel spins (for parallel spins, exchange terms reduce the phonon-mediated attractive electron-electron interaction). With no interaction,
2211 ..
2121 ,,,xkxkxxkk
i
e
Assume ϵF – ωD < ϵk , ϵk ± q < ϵF + ωD so that H ̎ is predominately attractive
† †
(here we have let k’ replace k2 and k replace k1).
Consider two free electrons, and introduce center of mass coordinates:
x = x1 – x2
q kk
kqkkqk CCCCVH'
''''
)(2
1
);(
21
)(
2122211
xxX
xxkk xkxk
i
e1
xXx
xXx
2
1
2
1
2
1
kKk
kKk
kkkkkK
2
1
2
1
)(2
1
2
1
2121
''1
'')(2
1
'H'
- , 0
4
11
22
),,,(
22
2
2
1
21
222
2
2
1
)(
ninteractioelectron -electron theIntroduce
thatsoConsider
: is state thisofenergy The
Hpm
Hppm
H
mm
k
m
k
ei
kk kkK
kK
xXkK xkXK
'
'
'
)('
'
)(
21
0',''',)(
0)(
0)(
2121
21)(
k
kkk
k
ii
Hgg
egHedd
H
k k
ie
ieg
ieg
kkkk
xx xxk
k
xxk
xkxk
kxk
kx
form the of oneigenfunti an forLook
m
F
cgdVg
V
Hgdg
DFmFk
mk
m
andF
and
2
2
)'()'(')()(
''H'
)(
0''')'()'(')()(
22
2
1
: where,m
K F
Kbetween i.e. D
F
between sea fermi theof top the tostateselectron -one theConfine
stateselectron -2 ofdensity
Fm
F
m
F
F
m
F
m
F
m
F
d
V
dV
dV
Cg
22ln
2
2ln
'
'1
'
1'1
0'
)'('1
)(
2
2
2
2
2
2
result. sobtain thinot could
n calculatioon perturbati Vin seriespower a as written benot may
pair bound
0 e)(attractiv 0
1
1
2
1
22
F2
V
VFe
D
VFe
Fm
- - 2 1
The region of increased positive charge density propagates through the crystal as a
quantized sound wave called a phonon
The passing electron has emitted a phonon
A second electron experiences a Coulomb attraction from the increased region
of positive charge density created by the first electron
BCS Theory – a Brief Treatment
For many electrons, we need to make sure the many-particle wave function is anti symmetric.
We can write in general that the Hamiltonian is:
† †
† †
sksksqk
qk
sqkq
sksksqk
qsksk
sqkq
CCCCVHH
CCCCVHH
,',',
,
,0
,','','
,',',,
,0
2
1
2
1
:case) Cooper the in (as -k'k which for sonly state consider us Let
the are s' s,Here indices. spin
Summing over s, it can be shown (using anticommutator relationships for the annihilation and creation operators) that:
† †
† †
Here we have chosen S ↑ , S´↓ (to minimize the energy as before), and summed over S,
We have also assumed that Vk,k’ = V-k,-k’
Note that the eigenstates for H0 are just the Block waves uk eik.x in
the crystal.
k'k,
-
(1.)
kkkkkk
k
kkkkk
CCCCV
CCCCH
'''
k
kC
kC
kH
0 taken and
†
Eq. (1.) is the BCS Hamiltonian
There are in general 2 approaches to solve the many-particle
Schroedinger equation (see, e.g. TINKHAM):
1. variational approach to minimize the energy
2. solution by a canonical transformation (the Bogoliubov/ Valatin transformation).
We will illustrate the second approach here.
Bogoliubov diagonalized the Hamiltonian for the liquid helium superfluid condensate by introducing 2 new operators:
kc
kc
kc
kc
kkkk
cvcu
cvcu
kkkkk
kkkkk
,,,
0''
for solve and (2.)invert then We
i.e. ate,anticommut also s' theshown that becan It
and
The Bogoliubov/ Valatin
transformation. (2.)
†
†
†
†
†
Substituting these C’s into (1.) gives as the kinetic energy term
HT (1st set of terms):
† †
† †
Take mk = m-k = 0 for the ground state.
Next we consider the potential energy term Hv (second set of terms
with V)
kkkk
k
kkkkkkkkkkkkT
km
km
vummuvvH
and Here
)(22 222
2
1
2
1
2
1 ,
2
1
' '''
such that, k
x variablenew a introduce weand
sorder term th 4 eneglect th now We
0 termsdiagonal offorder th 4
',
22'''
2
Then,
.V
Hin termsdiagonal-off ingcorrespond
the T
Hin termsdiagonal-off t theinsist tha weH, ediagonaliz To
kkkk xvxu
kk kC
kC
kC
kC
kkV
VH
kkkkkkk
vk
uk
vk
ukk
V
kkkkkk
vk
uk
cancel
†
†
†
†
† †
This gives:
022
1
2
4
1
k2
2
1
2'4
1
'
(3.) 04
12
4
12
toleads (4.) and (3.) from
(4.) which,
by given k
quantity new a define weNow
'
2
1
2
''
2
1
2
kkx
kx
kk
xkk
Vk
xVxxk
kkkkkk
constant). electrons ofnumber the(keeping potential
chemical thebe energy to of zero thechoose now We
moment. ain
case special afor thisdo will Wesolved. becan thisknown, is kk'
V If
2
1
2
''
'
''2
1
give, now (5.) & (4.) and
22
2
gives for Solving
(5.)
kk
k
k kk
Vk
kk
k
kx
kx
2
1
,
21
(...)222
,0
221
kx
kk
x
kk
vk
uk
v
and
kmSo
kC
kC
kC
kx
or
)degeneracy (Spin
choose F
Eenergy Fermi k
For
N
:that sons,interactio of absence in terms latter the neglect We
N
isN of value nexpectatio the
km state,ground the in
kk
CN Consider
† †
involved.
phonon theofenergy the,q
than less )F
E to(relative k
choose n,interactiophoton -electron in theorigin its having kk'
VFor
root. square the thereforechoose we
0kk'
V when caseelectron free the toreduce To
2
1
22k
2
k want We
021 2
1 choose ,
kFor
negative
k
kx
kx
kx
FE
We take
Vkk’ = V, constant if |εk|< ħωD
= 0, otherwise
Here ωD is the Debye Frequency
Here ∆k can be evaluated as
2
1
''2
'''
2
1
kk
kkkk dD
Here we will take the “density of states” D(εk’) as a constant, D(EF).
Consider Vkk’ Vkk’
ħωD
εk
So we need only evaluate
V
1
2
122
)(
1sinh
2
1
F
D
F
EVD
dEVDD
D
gives This
This is the BCS gap energy in the density of states
For weak coupling (V small), this can be written as:
For the ground state wave function and finite temperature effects,
See TINKHAM.
)03.0~
2)(
1
eV
e
DD
EVD
DF
( of 1% ~ Typically,