Superconductivity Theory and Applications Part 2 ppt
Superconductivity Theory and Applications Part 2 ppt
... two-band BCS model
(Golubov et al., 20 02; Brinkman et al., 20 02; Mazin et al., 20 02; Nakai et al., 20 02; Miranovic
et al., 20 03; Dahm & Schopohl, 20 04; Dahm et al., 20 04; Gurevich, 20 03; ... a
SC 19.691 12. 39 4.8 – −1 20
IM 19.739 12. 50 4.4 – 4 20
M1 19. 820 12. 69 3.6 6 6 20
M2 19.751 12. 54 – 5 5 20
Table 2. Various parameters for the samples shown in Fig. 6...
Superconductivity Theory and Applications Part 5 pptx
... μm) single-crystal normal metals Cu
100
Superconductivity – Theory and Applications
Superconductivity – Theory and Applications
94
connecting J1 and J2. With proper circuit parameters, this ... reflections is
(Blonder et al., 19 82; Van Wees et al ., 19 92)
I
(m)=1 + |r
eh
(m)|
2
|r
ee
(m)|
2
, |r
eh
(m)|
2
+ |r
ee
(m)|
2
= 1,
where
|r
ee
(m)|
2
and |r
eh
(m)|...
Superconductivity Theory and Applications Part 6 pptx
... a
normal-metal-insulator-superconductor junction. Phys. Rev. B,Vol. 52, No.6,
(1995) 4467-44 72.
128
Superconductivity – Theory and Applications
Superconductivity – Theory and Applications
136
where the pairing interaction ... 1
24 2 24 2
c
cm cnm
T
TT T
...
Superconductivity Theory and Applications Part 8 pptx
...
12 1 02
11
(x) [ (x) i (x)] [ (x) +i (x)]
22
φ= φ+φ → φ+φφ ( 12)
Since
i
000
φ
= under this transformation, then the equation (2) becomes
2
222 22 2
ij ji 2 1 1 0 2 i 0i 2
22 22 22
21 12i 0 ... 0 2 i 0i 2
22 22 22
21 12i 0 1 0 2 011 2
222 2 2 2
12 0 0 1 0 0
111(e*)
H' ( A A ) ( ) ( ) [( ) ]A e * A
422 2
11
e*( )A ( 12 2 ) ( 12 2 ) 4 ( )
22
4( )...
Superconductivity Theory and Applications Part 10 ppt
... defined as G(q
m
1
,m
2
,m
3
)=(G
x
, G
y
, G
z
)
with G
x
=[N
1
sin (2 m
1
/N
1
)+N
2
sin (2 m
2
/N
2
)]/a, G
y
=[−N
1
sin (2 m
1
/N
1
)+
N
2
sin (2 m
2
/N
2
)]/2a
y
, and G
z
= N
3
sin (2 m
3
/N
3
)/L. ... defined as G(q
m
1
,m
2
,m
3
)=(G
x
, G
y
, G
z
)
with G
x
=[N
1
sin (2 m
1
/N
1
)+N
2
sin (2 m
2
/N
2
)]/a, G
y
=[−N
1
sin (2 m
1
/N
1
)+
N
2
sin (2 m
2
/N
2...
Superconductivity Theory and Applications Part 13 ppt
... & Yeh, 20 02)
12 23
2
12 23
,
1
pc
pc
ik L
ikL
tte
t
rre
(34)
where k
pc
=n
pc
ω/c and L is the length of the PhC along the y direction. The r
12
, r
23
, t
12
, and t
23
are ... following
equation (Pei & Huang, 20 07a):
22 2
1
0
22 2
(,) (,) (,)
(,) (,) (,)
zz
zsznz
Exy Exy xy
Ex
y
iJx
y
Jx
y
xy c
22
2
1
22
(,) (,...
Superconductivity Theory and Applications Part 14 ppt
... the integration, we obtain
0,0
,
1
ab
f
f
(60)
2
12. 2
2
22. 2
2, 2
12. 2
2. 2
,
2sin()
()
11
(1) cos ( 0)
2sin( )
()
11
2( 0,0)
m
L
nm
La b nm
nm
nm
ab nm
famNL
JG R
am
m
NLamLGR
JG ...
(61)
2
1
121 .21
2
21 ,2 1
22 1 .21
,
sin (2 1) 2
2
()
11 (2 1)
(1) sin
4sin (21 )2
L
m
nm
nm
La b nm
am N L
f
JG R
am
NLamLGR
...
Superconductivity Theory and Applications Part 15 ppt
... with various orientations of magnetic fields and
currents.
Superconductivity – Theory and Applications
346
8. References
Anderson P. W., (19 62) . Theory of Flux Creep in Hard Superconductors, ...
Superconductivity – Theory and Applications
340
The degree of the foil anisotropy is seen from Figs.10 and 12. It allows estimating of
agreement between experimental d...
MIMO Systems Theory and Applications Part 2 ppt
... becomes the 2l order Hadamard
matrix.
CC
C
−C
and
C
2
l
= C
2
⊗C
2
l−1
(116)
where
⊗ is the Kronecker product and C
2
l−1
,2 l is expressed as :
C
2
l
=
C
2
l−1
C
2
l−1
C
2
l−1
−C
2
l−1
(117)
Collaborative ... Diversity and Antenna Selection
MIMO Systems, Theory and Applications
58
and has better error-rate performance and higher diversity gains...
Superconductivity Theory and Applications Part 1 pot
... Temperature Superconductivity
7
[MO configuration of O
2
]: [inner electrons](
2s
)
2
(*
2s
)
2
(
2p
)
4
(
2p
)
2
(*
2p
)
2
Considering the above MO configuration of O
2
we conclude ... superconductivity. Physica C:
Superconductivity, 23 5 -24 0, Part 1, pp. 27 7 -28 0
Rao , C. N. R.; Ganguly, P.; Hegde, M. S. & Sarma, D. D. (1987). Holes in the oxygen (2p)...
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