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1
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2
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.
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Evaluation Warning : The document was created with Spire.PDF for Python.
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9
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u
t
d
ec
o
d
in
g
lead
in
g
t
o
its
s
i
m
p
l
icit
y
a
n
d
ef
f
ec
tiv
e
i
m
p
le
m
en
tatio
n
co
s
t
[
1
0
]
.
I
n
th
e
w
ir
ele
s
s
co
o
p
er
ativ
e
s
y
s
te
m
w
it
h
m
u
ltip
le
r
elay
s
,
n
u
m
er
o
u
s
r
ela
y
s
elec
tio
n
tec
h
n
iq
u
es
h
a
v
e
p
r
o
p
o
s
ed
[
6
]
an
d
th
is
i
n
clu
d
e
t
h
e
p
ar
tial
r
elay
s
e
lectio
n
w
h
er
e
s
elec
tio
n
o
f
r
ela
y
s
d
ep
en
d
s
o
n
th
e
C
SI
o
f
t
h
e
s
o
u
r
ce
-
r
ela
y
lin
k
s
o
r
r
elay
-
d
esti
n
atio
n
li
n
k
s
.
T
h
is
th
u
s
av
o
id
s
th
e
is
s
u
es
s
u
c
h
as
h
ig
h
p
o
w
er
co
n
s
u
m
p
tio
n
,
o
v
e
r
h
ea
d
an
d
n
et
w
o
r
k
d
ela
y
s
,
a
n
d
ca
n
also
p
r
o
lo
n
g
t
h
e
n
et
w
o
r
k
li
f
eti
m
e
[
1
1
,
1
2
]
.
Un
li
k
e
t
h
e
b
e
s
t
a
n
d
o
p
p
o
r
t
u
n
i
s
t
i
c
r
e
l
a
y
s
e
l
e
c
t
i
o
n
a
p
p
r
o
a
c
h
e
s
,
w
h
i
c
h
r
e
q
u
i
r
e
g
l
o
b
a
l
k
n
o
w
l
e
d
g
e
o
f
t
h
e
C
S
I
o
f
e
a
c
h
o
f
t
h
e
t
w
o
h
o
p
s
[
1
2
,
1
3
]
l
e
a
d
i
n
g
t
o
t
i
m
e
s
y
n
c
h
r
o
n
i
z
a
t
i
o
n
,
c
o
n
t
i
n
u
o
u
s
c
h
a
n
n
e
l
f
e
e
d
b
a
c
k
a
n
d
h
i
g
h
p
o
w
e
r
c
o
n
s
u
m
p
t
i
o
n
.
R
ed
u
ci
n
g
t
h
e
e
n
er
g
y
co
n
s
u
m
p
tio
n
o
f
co
o
p
er
ativ
e
r
ela
y
i
n
g
s
y
s
te
m
t
h
r
o
u
g
h
t
h
e
en
er
g
y
h
ar
v
esti
n
g
h
a
s
d
r
a
w
n
m
o
r
e
atte
n
tio
n
i
n
th
e
r
esear
ch
co
m
m
u
n
it
y
h
as
attr
ac
ted
atten
tio
n
i
n
th
e
r
e
s
ea
r
ch
co
m
m
u
n
it
y
.
T
h
e
p
er
f
o
r
m
a
n
ce
o
f
d
u
al
-
h
o
p
r
ela
y
in
g
n
et
w
o
r
k
w
i
th
th
r
ee
d
if
f
er
en
t
w
ir
eles
s
E
H
m
ec
h
a
n
is
m
s
at
t
h
e
DF
r
ela
y
n
o
d
es
o
v
er
th
e
g
e
n
er
alize
d
c
h
an
n
el
s
w
a
s
s
tu
d
ied
[
1
4
]
.
I
n
[
1
5
]
,
th
e
p
er
f
o
r
m
a
n
ce
o
f
a
wir
eless
in
f
o
r
m
atio
n
p
o
w
er
tr
an
s
f
er
in
AF
r
ela
y
n
et
w
o
r
k
w
i
th
m
u
ltip
le
a
n
ten
n
a
o
v
er
d
is
s
i
m
i
lar
ch
a
n
n
el
a
n
d
th
e
b
en
e
f
it
o
f
MRC
/T
A
S
w
a
s
e
x
p
lo
it
f
o
r
th
e
r
ela
y
n
o
d
e
w
as
in
v
e
s
tig
a
ted
.
T
h
e
E
r
g
o
d
ic
o
u
tag
e
an
d
ca
p
ac
it
y
p
er
f
o
r
m
an
ce
o
f
w
ir
ele
s
s
p
o
w
er
tr
a
n
s
f
er
b
ased
AF
r
ela
y
i
n
g
s
y
s
te
m
w
as
p
r
ese
n
ted
in
[
1
6
]
.
A
ls
o
,
th
e
p
er
f
o
r
m
an
ce
o
f
DF
-
b
ased
E
H
w
it
h
t
h
e
s
o
u
r
ce
n
o
d
e
an
d
th
e
d
esti
n
atio
n
e
m
p
lo
y
in
g
T
AS
a
n
d
MR
C
r
esp
ec
ti
v
el
y
w
a
s
ev
a
lu
ated
in
[
1
7
]
.
T
h
e
th
r
o
u
g
h
p
u
t
p
er
f
o
r
m
a
n
ce
o
f
an
AF
r
ela
y
b
ased
E
H
u
n
d
er
d
elay
-
to
ler
a
n
ce
an
d
l
i
m
ited
t
r
an
s
m
is
s
io
n
m
o
d
es
w
a
s
in
v
es
tig
a
ted
in
[
7
]
o
v
er
R
a
y
lei
g
h
f
ad
in
g
c
h
an
n
els.
Ho
wev
er
,
all
th
e
s
e
af
o
r
e
m
e
n
t
io
n
ed
w
o
r
k
s
ar
e
li
m
ite
d
to
a
s
in
g
le
r
ela
y
-
b
ased
E
H
co
o
p
er
ativ
e
s
y
s
te
m
s
.
I
n
ca
s
e
o
f
m
u
ltip
le
r
ela
y
s
ele
ctio
n
,
t
h
e
p
er
f
o
r
m
a
n
ce
o
f
E
H
co
o
p
er
ativ
e
s
y
s
te
m
w
it
h
o
p
ti
m
al
r
ela
y
s
elec
tio
n
u
n
d
er
th
e
C
SI
an
d
e
n
er
g
y
s
id
e
i
n
f
o
r
m
atio
n
w
as
i
n
v
esti
g
ated
i
n
[
1
8
]
.
I
n
ad
d
itio
n
,
in
cr
e
m
e
n
tal
r
ela
y
n
et
w
o
r
k
w
it
h
E
H
-
b
ased
r
ela
y
s
elec
tio
n
w
as
p
r
o
p
o
s
ed
in
[
1
9
]
w
h
er
e
th
e
s
e
lecte
d
r
ela
y
h
ar
v
esti
n
g
th
e
lar
g
e
s
t
s
o
u
r
ce
e
n
er
g
y
w
a
s
c
h
o
s
e
n
to
f
o
r
w
ar
d
t
h
e
i
n
f
o
r
m
atio
n
to
t
h
e
d
est
in
at
io
n
.
I
n
[
2
0
]
,
th
e
p
er
f
o
r
m
an
ce
o
f
AF
r
ela
y
in
g
en
er
g
y
h
a
r
v
esti
n
g
s
y
s
te
m
w
it
h
ℎ
b
est
P
R
S
an
d
e
n
er
g
y
b
ea
m
f
o
r
m
in
g
o
v
er
Nak
ag
a
m
i
-
m
w
a
s
ev
alu
a
ted
.
I
n
t
h
is
w
o
r
k
,
it
w
a
s
as
s
u
m
ed
t
h
at
b
o
th
th
e
s
o
u
r
ce
an
d
t
h
e
d
esti
n
atio
n
ar
e
m
u
lt
ip
le
an
te
n
n
a
n
o
d
es
an
d
th
e
r
ela
y
ar
e
s
i
n
g
le
an
te
n
n
a
n
o
d
es.
I
n
all
th
e
s
e
af
o
r
em
en
tio
n
ed
s
t
u
d
ies,
p
er
f
ec
t
C
SI
w
as
a
s
s
u
m
ed
f
o
r
th
e
s
y
s
te
m
.
Mo
tiv
ated
b
y
t
h
is
,
th
e
p
er
f
o
r
m
a
n
ce
o
f
th
e
P
R
S
-
b
ased
E
H
s
y
s
te
m
u
n
d
er
th
e
T
A
S/MR
C
is
in
v
e
s
ti
g
ated
i
n
th
is
p
ap
er
w
h
e
r
e
th
e
r
ela
y
n
o
d
es
e
m
p
lo
y
th
e
T
A
S
tech
n
iq
u
e
a
t
th
e
r
ela
y
n
o
d
es
an
d
m
a
x
i
m
u
m
r
atio
co
m
b
in
i
n
g
(
M
R
C
)
s
c
h
e
m
e
at
th
e
d
esti
n
atio
n
.
T
h
e
ex
ac
t
clo
s
ed
-
f
o
r
m
e
x
p
r
ess
io
n
f
o
r
th
e
s
y
s
te
m
o
u
tag
e
p
r
o
b
a
b
ilit
y
an
d
a
v
er
ag
e
b
it
er
r
o
r
r
ate
ar
e
o
b
tain
ed
.
Utilizin
g
th
e
o
u
ta
g
e
p
r
o
b
ab
ilit
y
,
th
e
t
h
r
o
u
g
h
p
u
t
f
o
r
th
e
s
y
s
te
m
is
o
b
tai
n
ed
b
ased
o
n
d
elay
-
li
m
i
ted
tr
an
s
m
is
s
io
n
m
o
d
e
.
T
h
e
im
p
ac
t
o
f
e
n
er
g
y
h
ar
v
e
s
ti
n
g
ti
m
e,
r
ela
y
d
is
ta
n
ce
,
c
h
a
n
n
e
l c
o
r
r
elatio
n
co
e
f
f
ic
ien
t,
t
h
e
n
u
m
b
er
o
f
r
ela
y
tr
an
s
m
i
t a
n
te
n
n
a
s
a
n
d
d
esti
n
a
tio
n
r
ec
eiv
ed
an
ten
n
a
o
n
t
h
e
co
n
ce
r
n
ed
s
y
s
t
e
m
ar
e
d
e
m
o
n
s
tr
ated
.
2.
SYST
E
M
AND
CH
ANNE
L
M
O
DE
L
I
n
th
i
s
p
ap
er
,
a
d
u
al
-
h
o
p
s
P
R
S
b
ased
en
er
g
y
h
ar
v
e
s
ti
n
g
s
y
s
te
m
w
it
h
P
R
S
an
d
o
u
td
at
ed
C
SI
is
p
r
esen
ted
i
n
F
i
g
u
r
e
1
(
a
)
.
T
h
e
s
o
u
r
ce
(
S)
is
eq
u
ip
p
ed
w
it
h
a
s
i
n
g
le
tr
an
s
m
it
a
n
te
n
n
a
a
n
d
th
e
d
est
in
at
io
n
(
D)
h
as
m
u
ltip
le
r
ec
eiv
e
a
n
ten
n
a
.
T
h
e
r
ela
y
(
R
)
o
f
n
o
d
es
u
tili
ze
a
s
i
n
g
le
r
ec
ei
v
e
an
te
n
n
a
an
d
m
u
ltip
le
tr
an
s
m
it
a
n
te
n
n
a
.
I
t
is
ass
u
m
ed
th
at
t
h
e
S
-
to
-
R
a
n
d
R
-
to
-
D
li
n
k
s
u
n
d
er
g
o
R
a
y
lei
g
h
f
a
d
in
g
d
is
tr
ib
u
tio
n
w
it
h
o
u
t
d
ir
ec
t
lin
k
b
et
w
ee
n
t
h
e
s
o
u
r
ce
a
n
d
th
e
d
es
tin
at
io
n
.
T
h
e
r
elay
n
o
d
es
e
m
p
lo
y
T
AS
s
ch
e
m
e
to
s
e
lect
th
e
b
est
a
n
ten
n
a
t
o
f
o
r
w
ar
d
th
e
s
i
g
n
al
to
th
e
d
esti
n
at
io
n
th
r
o
u
g
h
w
h
ich
t
h
e
i
n
s
t
an
tan
eo
u
s
SNR
at
th
e
d
esti
n
a
tio
n
is
m
a
x
i
m
ized
.
A
t
th
e
d
esti
n
atio
n
,
MR
C
i
s
u
s
ed
to
co
m
b
i
n
e
th
e
tr
an
s
m
itted
s
i
g
n
a
l
f
r
o
m
th
e
r
ela
y
n
o
d
e(
s
)
.
A
s
a
r
esu
lt
o
f
ch
a
n
n
el
f
ast
f
ad
i
n
g
,
i
t
is
co
n
s
id
er
ed
th
a
t
r
ela
y
s
elec
tio
n
is
b
ased
o
n
o
u
td
ated
C
SI.
T
h
u
s
,
th
e
in
s
ta
n
tan
eo
u
s
SNR
o
f
t
h
e
f
ir
s
t
li
n
k
an
d
t
h
e
o
n
e
u
s
ed
f
o
r
P
R
S
ar
e
t
w
o
co
r
r
elate
d
r
an
d
o
m
v
ar
iab
les
w
it
h
ch
a
n
n
e
l
co
r
r
e
latio
n
co
ef
f
icie
n
t
.
T
h
e
tr
an
s
m
is
s
io
n
o
v
e
r
t
h
e
lin
k
s
i
s
ass
u
m
ed
to
b
e
in
h
al
f
-
d
u
p
lex
m
o
d
e
s
o
a
s
to
a
v
o
id
in
ter
-
s
ig
n
al
in
ter
f
er
en
ce
.
T
h
er
ef
o
r
e,
th
e
o
v
er
all
s
y
s
te
m
s
co
m
m
u
n
icatio
n
is
estab
lis
h
ed
in
t
w
o
d
if
f
er
en
t p
h
ases
.
Du
r
in
g
th
e
f
ir
s
t
p
h
a
s
e,
t
h
e
co
m
m
u
n
icatio
n
b
et
w
ee
n
th
e
S
an
d
R
n
o
d
es
is
d
iv
id
ed
i
n
to
p
o
w
er
tr
an
s
m
is
s
io
n
a
n
d
in
f
o
r
m
a
tio
n
tr
an
s
m
is
s
io
n
a
s
p
r
esen
ted
i
n
F
ig
u
r
e
1
(
b
)
.
B
ased
o
n
th
is
,
t
h
e
−
ℎ
s
elec
ted
r
ela
y
(
s
)
h
ar
v
es
t
t
h
e
e
n
er
g
y
an
d
th
e
n
r
ec
ei
v
e
t
h
e
i
n
f
o
r
m
atio
n
f
r
o
m
th
e
s
o
u
r
ce
u
s
i
n
g
t
h
e
ti
m
e
s
w
itc
h
i
n
g
-
b
as
e
r
ela
y
(
T
SR
)
p
r
o
to
co
l.
T
h
er
ea
f
t
er
,
th
e
s
o
u
r
ce
in
f
o
r
m
atio
n
i
s
am
p
li
f
ied
th
r
o
u
g
h
A
F
r
ela
y
i
n
g
an
d
th
en
co
n
v
e
y
to
th
e
d
esti
n
at
io
n
u
s
in
g
T
A
S
tech
n
iq
u
e.
I
n
T
SR
p
r
o
to
co
l,
a
to
t
al
b
lo
ck
tim
e
s
lo
t
o
f
is
d
iv
id
ed
in
to
th
r
ee
p
a
r
ts
:
f
o
r
en
er
g
y
h
ar
v
esti
n
g
as
,
in
f
o
r
m
atio
n
tr
an
s
m
i
s
s
io
n
b
et
w
ee
n
S
-
to
-
R
a
s
(
1
−
)
/
2
an
d
in
f
o
r
m
atio
n
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2
0
8
8
-
8708
I
n
t J
E
lec
&
C
o
m
p
E
n
g
,
Vo
l.
10
,
No
.
5
,
Octo
b
e
r
2
0
2
0
:
5
2
9
6
-
5305
5298
tr
an
s
m
is
s
io
n
b
et
w
ee
n
R
-
to
-
D
as
(
1
−
)
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2
.
T
h
e
p
ar
am
eter
d
en
o
tes
th
e
en
er
g
y
h
a
v
i
n
g
t
i
m
e
f
ac
t
o
r
at
0
≤
≤
1
.
T
h
u
s
,
th
e
r
ec
eiv
e
s
ig
n
al
b
y
t
h
e
−
ℎ
s
elec
ted
r
ela
y
(
s
)
ca
n
b
e
ex
p
r
ess
ed
as:
1
(
)
(
)
=
√
1
1
ℎ
1
(
)
(
)
+
(
)
(
)
(
1
)
w
h
er
e
is
t
h
e
s
o
u
r
ce
tr
an
s
m
i
tted
p
o
w
er
,
ℎ
1
(
)
is
−
ℎ
th
e
ch
a
n
n
e
l
g
ain
,
1
is
th
e
d
is
ta
n
ce
b
et
w
e
en
th
e
s
o
u
r
ce
an
d
th
e
r
ela
y
,
1
d
en
o
tes
th
e
p
ath
lo
s
s
ex
p
o
n
e
n
t,
(
)
r
e
p
r
esen
ts
th
e
s
o
u
r
ce
s
in
f
o
r
m
ati
o
n
an
d
(
)
is
th
e
A
W
GN
at
t
h
e
−
ℎ
s
elec
ted
r
ela
y
(
s
)
w
ith
ze
r
o
m
ea
n
an
d
v
ar
ian
ce
1
2
.
T
h
e
en
er
g
y
h
ar
v
est
ed
b
y
an
en
er
g
y
r
ec
eiv
er
at
t
h
e
−
ℎ
s
elec
te
d
r
elay
(
s
)
o
v
er
t
h
e
ti
m
e
ca
n
b
e
ex
p
r
ess
ed
as [
1
,
1
1
]
:
ℎ
,
=
|
ℎ
1
(
)
|
2
1
1
(
2
)
w
h
er
e
0
≤
≤
1
d
en
o
tes
th
e
e
n
er
g
y
h
a
r
v
esti
n
g
ef
f
icie
n
c
y
w
h
ich
d
ep
en
d
s
o
n
t
h
e
r
ec
ti
f
icatio
n
p
r
o
ce
s
s
a
n
d
th
e
cir
cu
i
tr
y
.
Du
r
in
g
t
h
e
s
ec
o
n
d
p
h
a
s
e,
t
h
e
r
e
m
ai
n
in
g
ti
m
e
s
lo
t
o
f
(
1
−
)
/
2
d
u
r
atio
n
is
t
h
en
u
s
ed
b
y
t
h
e
−
ℎ
s
elec
ted
r
ela
y
(
s
)
to
a
m
p
li
f
ie
s
an
d
r
etr
an
s
m
i
t
th
e
i
n
f
o
r
m
atio
n
to
th
e
d
esti
n
atio
n
u
s
i
n
g
T
AS
p
r
in
cip
le.
T
h
e
d
esti
n
atio
n
t
h
u
s
e
m
p
lo
y
s
MRC
tec
h
n
iq
u
e
to
co
m
b
i
n
e
th
e
tr
an
s
m
itted
s
i
g
n
al
f
r
o
m
t
h
e
−
ℎ
s
elec
ted
r
ela
y
(
s
)
an
d
th
e
r
ec
ei
v
ed
s
ig
n
a
l c
an
b
e
ex
p
r
ess
ed
as
:
2
(
)
=
√
(
)
2
2
ℎ
2
(
)
̂
(
)
+
(
)
(
3
)
w
h
er
e
ℎ
2
(
)
th
e
c
h
an
n
el
g
a
in
,
2
is
th
e
d
is
ta
n
ce
b
et
w
ee
n
t
h
e
r
ela
y
an
d
d
esti
n
atio
n
,
2
d
en
o
tes
th
e
p
ath
lo
s
s
ex
p
o
n
en
t,
̂
(
)
r
ep
r
esen
ts
th
e
d
ec
o
d
ed
in
f
o
r
m
at
io
n
o
f
(
)
,
is
th
e
A
W
GN
at
th
e
d
esti
n
a
tio
n
w
it
h
ze
r
o
m
ea
n
a
n
d
v
ar
ian
ce
2
2
,
an
d
(
)
is
th
e
−
ℎ
s
elec
ted
r
elay
(
s
)
tr
an
s
m
it
p
o
w
er
o
b
tain
ed
f
r
o
m
e
n
er
g
y
h
ar
v
e
s
tin
g
f
o
r
r
ela
y
in
g
a
m
p
lifi
ca
tio
n
an
d
th
is
ca
n
b
e
ex
p
r
ess
ed
as [
1
4
]
:
(
)
=
ℎ
(
)
(
1
−
)
/
2
≜
2
|
ℎ
1
(
)
|
2
(
1
−
)
1
1
(
4
)
Sin
ce
t
h
e
r
ela
y
s
ar
e
f
i
x
ed
-
g
ai
n
A
F
n
o
d
es,
th
e
eq
u
iv
ale
n
t
e
n
d
-
t
o
-
e
n
d
in
s
tan
tan
eo
u
s
SN
R
a
t
th
e
d
esti
n
atio
n
f
o
r
th
e
s
y
s
te
m
ca
n
b
e
ap
p
r
o
x
im
a
t
el
y
ex
p
r
es
s
ed
b
y
f
o
llo
w
i
n
g
t
h
e
s
a
m
e
ap
p
r
o
ac
h
in
[
1
1
]
as:
=
̃
1
(
)
2
(
)
2
(
)
+
1
(
5
)
w
h
er
e
̃
1
(
)
=
|
ℎ
1
(
)
|
2
,
2
(
)
=
|
ℎ
2
(
)
|
2
,
=
2
(
1
−
)
1
1
,
an
d
=
2
(
1
−
)
1
1
1
2
f
o
r
d
en
o
t
es
t
h
e
av
er
a
g
e
tr
an
s
m
it S
NR
.
I
n
th
i
s
s
t
u
d
y
,
t
h
e
d
u
al
-
h
o
p
s
lin
k
s
f
o
r
th
e
s
y
s
te
m
ar
e
ch
a
r
ac
ter
ized
b
y
th
e
R
a
y
le
ig
h
f
ad
in
g
a
n
d
th
e
p
r
o
b
ab
ilit
y
d
e
n
s
it
y
f
u
n
ctio
n
(
P
DF)
f
o
r
th
e
d
is
tr
ib
u
t
io
n
f
o
r
th
e
S
-
to
-
R
lin
k
u
n
d
er
th
e
p
ar
tial
r
ela
y
s
elec
t
io
n
s
y
s
te
m
ca
n
b
e
ex
p
r
ess
ed
as
[
1
1
,
1
2
]
:
1
(
)
(
)
=
(
)
∑
(
−
1
)
−
1
=
0
(
−
1
)
(
(
−
+
)
(
1
−
)
+
1
)
Ω
1
(
6
)
×
(
−
(
−
+
+
1
)
(
(
−
+
)
(
1
−
)
+
1
)
Ω
1
)
w
h
er
e
is
t
h
e
ch
a
n
n
el
co
r
r
elati
o
n
co
ef
f
ic
ien
t,
Ω
1
=
[
|
ℎ
1
(
)
|
2
]
A
l
s
o
,
th
e
co
r
r
esp
o
n
d
in
g
C
DF
ca
n
b
e
o
b
tain
ed
b
y
i
n
te
g
r
atin
g
(
6
)
as:
1
(
)
(
)
=
1
−
(
)
∑
(
−
1
)
−
1
=
0
(
−
1
)
(
(
−
+
)
+
1
)
(
7
)
×
(
−
(
−
+
+
1
)
(
(
−
+
)
(
1
−
)
+
1
)
Ω
1
)
Evaluation Warning : The document was created with Spire.PDF for Python.
I
n
t J
E
lec
&
C
o
m
p
E
n
g
I
SS
N:
2088
-
8708
On
th
e
p
erfo
r
ma
n
ce
o
f e
n
erg
y
h
a
r
ve
s
tin
g
A
F
p
a
r
tia
l rela
y
s
elec
tio
n
…
(
K
eh
in
d
e
O.
Od
ey
emi
)
5299
B
y
t
h
e
p
r
in
cip
le
o
f
T
A
S
/MR
C
,
th
e
P
DF f
o
r
th
e
R
-
to
-
D
ch
a
n
n
el
ca
n
b
e
d
ef
i
n
ed
as
[
2
1
]
:
2
(
)
=
Γ
(
)
∑
(
−
1
)
(
−
1
)
−
1
=
0
(
−
(
+
1
)
Ω
2
)
∏
[
∑
(
−
1
)
−
1
=
0
(
1
!
)
−
+
1
]
Ω
2
−
−
1
−
1
=
1
(8
)
w
h
er
e
{
=
+
,
=
∑
−
1
=
1
,
0
=
,
=
0
,
a
n
d
Ω
2
=
[
|
ℎ
2
(
)
|
2
]
(
9
)
Fig
u
r
e
1
:
(
a)
P
ar
tial r
elay
s
ele
ctio
n
s
y
s
te
m
m
o
d
el
w
it
h
e
n
er
g
y
h
ar
v
esti
n
g
(
b
)
T
SR
p
r
o
to
c
o
l f
o
r
p
o
w
er
an
d
in
f
o
r
m
at
io
n
tr
an
s
f
er
at
th
e
r
e
la
y
3.
ST
A
T
I
S
T
I
CAL CH
A
RAC
T
E
RI
ST
I
CS
T
h
e
C
DF
o
f
t
h
e
eq
u
i
v
ale
n
t
en
d
-
to
-
en
d
i
n
s
ta
n
ta
n
eo
u
s
SN
R
at
th
e
d
es
tin
a
tio
n
f
o
r
th
e
co
n
ce
r
n
ed
s
y
s
te
m
ca
n
b
e
ex
p
r
ess
ed
as
[
1
5
]
:
(
)
=
[
1
<
2
+
1
|
2
>
0
]
(
1
0
)
≜
∫
1
(
2
+
2
)
2
(
2
)
2
∞
0
B
y
s
u
b
s
ti
tu
ti
n
g
(
7
)
an
d
(
8
)
i
n
to
(
1
0
)
,
th
e
eq
u
iv
ale
n
t
en
d
-
to
-
en
d
in
s
tan
tan
eo
u
s
SN
R
f
o
r
th
e
s
y
s
te
m
ca
n
b
e
ex
p
r
ess
ed
as:
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2
0
8
8
-
8708
I
n
t J
E
lec
&
C
o
m
p
E
n
g
,
Vo
l.
10
,
No
.
5
,
Octo
b
e
r
2
0
2
0
:
5
2
9
6
-
5305
5300
(
)
=
1
−
Γ
(
)
∑
∑
(
)
(
−
1
)
(
−
1
)
Ω
2
−
−
1
=
0
−
1
=
0
(
−
1
)
+
(
(
−
+
)
+
1
)
(
−
Δ
Ω
1
)
(
1
1
)
×
∏
[
∑
(
−
1
)
−
1
=
0
(
1
!
)
−
+
1
]
−
1
=
1
∫
2
−
1
(
−
(
+
1
)
2
Ω
2
)
(
−
μ
Ω
1
2
)
2
∞
0
w
h
er
e
μ
=
(
−
+
+
1
)
(
(
−
+
)
(
1
−
)
+
1
)
B
y
co
n
v
er
t
in
g
t
h
e
(
−
μ
Ω
1
2
)
to
Me
ij
er
-
G
f
u
n
c
tio
n
f
o
r
m
u
s
in
g
t
h
e
id
en
tit
y
d
ef
in
ed
[
2
2
,
(
1
1
)
]
an
d
in
v
er
t
th
e
f
u
n
ct
io
n
u
s
i
n
g
th
e
id
en
tit
y
d
etailed
in
[
2
3
(
8
.
2
.
2
(
1
4
)
]
,
th
en
th
e
i
n
te
g
r
al
p
ar
t
o
f
(
1
0
)
ca
n
b
e
ex
p
r
ess
ed
as:
1
=
∫
2
−
1
(
−
(
+
1
)
Ω
)
1
,
0
0
,
1
(
Ω
2
2
μγ
|
1
−
)
2
∞
0
(
1
2
)
B
y
u
tili
z
in
g
t
h
e
in
te
g
r
al
id
en
t
i
t
y
d
ef
i
n
ed
in
[
2
4
,
(
7
.
8
1
3
(
1
)
)
]
,
th
e
(
1
2
)
ca
n
b
e
s
o
lv
ed
as:
1
=
(
Ω
2
(
+
1
)
)
2
,
0
0
,
2
(
Ω
1
2
μγ
(
+
1
)
|
1
−
,
1
−
)
(
1
3
)
B
y
p
u
t
t
i
n
g
(
1
3
)
i
n
t
o
(
1
1
)
,
t
h
e
n
t
h
e
e
q
u
i
v
a
l
e
n
t
e
n
d
-
to
-
e
n
d
i
n
s
t
a
n
t
a
n
e
o
u
s
S
N
R
f
o
r
t
h
e
s
y
s
t
e
m
c
a
n
b
e
o
b
t
a
i
n
e
d
a
s
:
(
)
=
1
−
Γ
(
)
∑
∑
(
)
(
−
1
)
(
−
1
)
Ω
2
−
−
1
=
0
−
1
=
0
(
−
1
)
+
(
(
−
+
)
+
1
)
(
−
μ
Ω
1
)
×
∏
[
∑
(
−
1
)
−
1
=
0
(
1
!
)
−
+
1
]
−
1
=
1
(
Ω
2
(
+
1
)
)
2
,
0
0
,
2
(
Ω
1
Ω
2
μγ
(
+
1
)
|
1
−
,
1
−
)
(
1
4
)
4.
P
E
RF
O
RM
ANCE AN
AL
YS
I
S
T
h
e
p
er
f
o
r
m
an
ce
an
a
l
y
s
is
o
f
th
e
co
n
ce
r
n
ed
s
y
s
te
m
i
n
ter
m
s
o
f
o
u
ta
g
e
p
r
o
b
ab
ilit
y
,
A
B
E
R
an
d
th
r
o
u
g
h
p
u
t a
r
e
p
r
esen
ted
in
t
h
i
s
s
ec
tio
n
.
4
.
1
.
O
uta
g
e
pro
ba
bil
it
y
a
na
ly
s
is
T
h
e
o
u
t
a
g
e
p
r
o
b
a
b
i
l
i
t
y
i
s
a
n
i
m
p
o
r
t
a
n
t
m
e
a
s
u
r
e
f
o
r
e
v
a
l
u
a
t
i
n
g
t
h
e
p
e
r
f
o
r
m
a
n
c
e
o
f
a
w
i
r
e
l
e
s
s
s
y
s
t
e
m
s
o
v
e
r
f
a
d
i
n
g
c
h
a
n
n
e
l
s
.
A
t
a
g
i
v
e
n
t
r
a
n
s
m
i
s
s
i
o
n
r
a
t
e
b
its
/
s
/
Hz
,
t
h
e
o
u
t
a
g
e
p
r
o
b
a
b
i
l
i
t
y
c
a
n
b
e
d
e
f
i
n
e
d
a
s
[
2
5
,
2
6
]
:
=
(
ℎ
)
(
1
5
)
w
h
er
e
ℎ
=
2
−
1
is
th
e
p
r
ed
eter
m
i
n
ed
th
r
es
h
o
ld
SNR
r
eq
u
ir
ed
to
s
u
p
p
o
r
t
th
e
f
ix
ed
tr
an
s
m
is
s
io
n
r
at
e
a
t
th
e
s
o
u
r
ce
i
n
d
ela
y
-
li
m
ited
tr
a
n
s
m
i
s
s
io
n
m
o
d
e.
B
y
s
u
b
s
t
itu
tin
g
(
1
4
)
in
to
(
1
5
)
,
th
e
s
y
s
te
m
o
u
ta
g
e
p
r
o
b
ab
ilit
y
ca
n
b
e
ex
p
r
ess
ed
as:
=
1
−
Γ
(
)
∑
∑
(
)
(
−
1
)
(
−
1
)
Ω
2
−
−
1
=
0
−
1
=
0
(
−
1
)
+
(
(
−
+
)
+
1
)
(
−
μ
ℎ
Ω
1
)
×
∏
[
∑
(
−
1
)
−
1
=
0
(
1
!
)
−
+
1
]
−
1
=
1
(
Ω
2
(
+
1
)
)
2
,
0
0
,
2
(
Ω
1
Ω
2
μ
ℎ
(
+
1
)
|
1
−
,
1
−
)
(
1
6
)
4
.
2
.
Av
er
a
g
e
bit
er
ro
r
r
a
t
e
I
n
th
is
s
ec
t
io
n
,
th
e
A
B
E
R
f
o
r
th
e
s
y
s
te
m
is
d
er
iv
ed
u
n
d
er
th
e
B
P
SK
m
o
d
u
la
tio
n
an
d
th
e
A
B
E
R
f
o
r
th
e
co
n
ce
r
n
ed
s
y
s
te
m
ca
n
b
e
ex
p
r
ess
ed
as
[
1
5
]
:
=
2
√
2
∫
(
)
∞
0
e
xp
(
−
/
2
)
−
1
2
(
1
7
)
w
h
er
e
=
1
an
d
=
2
f
o
r
th
e
B
P
SK
m
o
d
u
latio
n
.
B
y
s
u
b
s
t
itu
tin
g
(
1
1
)
in
to
(
1
7
)
,
th
e
A
B
E
R
f
o
r
th
e
s
y
s
te
m
ca
n
b
e
ex
p
r
ess
ed
as:
Evaluation Warning : The document was created with Spire.PDF for Python.
I
n
t J
E
lec
&
C
o
m
p
E
n
g
I
SS
N:
2088
-
8708
On
th
e
p
erfo
r
ma
n
ce
o
f e
n
erg
y
h
a
r
ve
s
tin
g
A
F
p
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tia
l rela
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tio
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…
(
K
eh
in
d
e
O.
Od
ey
emi
)
5301
=
2
√
2
[
∫
e
x
p
(
−
/
2
)
−
1
/
2
∞
0
−
Ξ
1
∫
−
1
/
2
(
−
(
μ
Ω
1
+
1
2
)
)
2
,
0
0
,
2
(
Ω
1
Ω
2
μ
(
+
1
)
|
1
−
,
1
−
)
∞
0
]
(
1
8
)
w
h
er
e
Ξ
1
=
Γ
(
)
∑
∑
(
)
(
−
1
)
(
−
1
)
Ω
2
−
−
1
=
0
−
1
=
0
(
−
1
)
+
(
(
−
+
)
+
1
)
(
1
9
)
×
∏
[
∑
(
−
1
)
−
1
=
0
(
1
!
)
−
+
1
]
−
1
=
1
(
Ω
2
(
+
1
)
)
T
h
e
f
ir
s
t
in
teg
r
al
p
ar
t
o
f
(
1
8
)
ca
n
b
e
s
o
lv
e
b
y
u
s
in
g
t
h
e
in
te
g
r
al
id
en
tit
y
d
etailed
i
n
[
2
4
,
(
3
.
3
2
6
(
2
)
)
]
an
d
th
e
s
ec
o
n
d
in
te
g
r
al
ca
n
b
e
s
o
lv
ed
b
y
in
v
er
tin
g
th
e
Me
ij
er
-
G
f
u
n
ctio
n
u
s
i
n
g
t
h
e
id
en
tit
y
d
ef
i
n
ed
in
[
2
3
,
(
8
.
2
.
2
(
1
4
)
)
]
as:
3
=
∫
−
1
/
2
(
−
(
μ
Ω
1
+
1
2
)
)
2
,
0
0
,
2
(
μ
(
+
1
)
Ω
1
Ω
2
|
−
,
0
)
∞
0
(
2
0
)
T
h
en
,
b
y
u
s
i
n
g
th
e
i
n
te
g
r
al
id
en
tit
y
d
ef
i
n
ed
in
[
2
4
,
(
7
.
8
1
3
(
1
)
)
]
,
th
e
3
ca
n
b
e
s
o
lv
ed
as:
3
=
(
2
Ω
1
2
μ
+
Ω
1
)
1
/
2
0
,
2
2
,
0
(
2μ
(
+
1
)
Ω
2
(
2
μ
+
Ω
1
)
|
1
/
2
,
0
)
(
2
1
)
Su
b
s
ti
tu
t
in
g
3
in
to
(
1
8
)
,
th
e
A
B
E
R
f
o
r
th
e
T
A
S
/MR
C
ca
n
b
e
ex
p
r
ess
ed
as:
=
2
√
2
[
Γ
(
1
/
2
)
√
1
/
2
−
Γ
(
)
∑
∑
(
)
(
−
1
)
(
−
1
)
Ω
2
−
−
1
=
0
−
1
=
0
(
−
1
)
+
(
(
−
+
)
+
1
)
×
∏
[
∑
(
−
1
)
−
1
=
0
(
1
!
)
−
+
1
]
−
1
=
1
(
Ω
2
(
+
1
)
)
(
2
Ω
1
2
μ
+
Ω
1
)
1
/
2
0
,
2
2
,
0
(
2μ
(
+
1
)
Ω
2
(
2
μ
+
Ω
1
)
|
1
/
2
,
0
)
]
(
2
2
)
4
.
3
.
T
hro
ug
hp
ut
a
na
ly
s
is
I
n
th
is
p
ap
er
,
th
e
d
ela
y
-
li
m
i
ted
tr
an
s
m
is
s
io
n
m
o
d
e
i
s
e
m
p
lo
y
ed
f
o
r
th
e
co
n
ce
r
n
ed
s
y
s
te
m
an
d
th
e
t
h
r
o
u
g
h
p
u
t
i
s
o
b
tain
ed
b
y
d
eter
m
in
i
n
g
th
e
o
u
tag
e
p
r
o
b
ab
ilit
y
o
f
t
h
e
s
y
s
te
m
at
a
f
i
x
ed
s
o
u
r
ce
tr
an
s
m
i
s
s
io
n
r
ate
/
/
.
T
h
er
ef
o
r
e,
at
a
f
i
x
ed
tr
a
n
s
m
i
s
s
io
n
r
ate
w
it
h
e
f
f
ec
ti
v
e
co
m
m
u
n
icatio
n
ti
m
e
o
f
(
1
−
)
/
2
f
r
o
m
t
h
e
s
o
u
r
ce
to
d
esti
n
atio
n
,
th
e
th
r
o
u
g
h
p
u
t
ca
n
b
e
ex
p
r
ess
ed
as
[
7
]
:
=
(
1
−
)
(
1
−
)
/
2
≜
2
(
1
−
)
(
1
−
)
(
2
3
)
B
y
p
u
tti
n
g
(
1
6
)
in
to
(
2
3
)
,
th
e
th
r
o
u
g
h
p
u
t f
o
r
th
e
co
n
ce
r
n
ed
s
y
s
te
m
ca
n
b
e
ex
p
r
ess
ed
as:
=
(
1
−
)
2Γ
(
)
∑
∑
(
)
(
−
1
)
(
−
1
)
Ω
2
−
−
1
=
0
−
1
=
0
(
−
1
)
+
(
(
−
+
)
+
1
)
(
−
μ
ℎ
Ω
1
)
×
∏
[
∑
(
−
1
)
−
1
=
0
(
1
!
)
−
+
1
]
−
1
=
1
(
Ω
2
(
+
1
)
)
2
,
0
0
,
2
(
Ω
1
Ω
2
Δ
ℎ
(
+
1
)
|
1
−
,
1
−
)
(
2
4
)
5.
NUM
E
RICAL
R
E
SU
L
T
S A
ND
DIS
C
USS
I
O
NS
I
n
th
i
s
s
ec
t
io
n
,
t
h
e
n
u
m
er
ical
r
esu
lt
s
f
o
r
t
h
e
s
y
s
te
m
o
u
tag
e
p
r
o
b
a
b
ilit
y
,
A
B
E
R
,
an
d
t
h
r
o
u
g
h
p
u
t
ar
e
p
r
esen
ted
b
ased
o
n
th
e
d
er
iv
ed
an
al
y
tical
c
lo
s
ed
f
o
r
m
ex
p
r
ess
io
n
p
r
ese
n
ted
i
n
(
1
6
)
,
(
2
2
)
,
an
d
(
2
4
)
r
esp
ec
tiv
el
y
.
Un
le
s
s
s
p
ec
if
ie
d
,
th
e
s
y
s
te
m
p
ar
a
m
eter
s
ad
o
p
ted
ar
e
s
et
to
b
e
:
=
2
/
/
,
Ω
1
=
1
,
Ω
2
=
1
,
=
1
,
1
=
2
,
2
=
3
,
an
d
=
20
.
T
w
o
s
elec
tio
n
s
ce
n
ar
io
s
ar
e
co
n
s
id
er
ed
as
f
o
llo
w
s
:
w
o
r
s
t
r
ela
y
s
elec
tio
n
w
h
e
n
=
1
an
d
b
est r
ela
y
s
elec
tio
n
w
h
e
n
=
I
n
F
ig
u
r
e
2
,
th
e
ef
f
ec
t
o
f
S
-
to
-
R
d
is
ta
n
ce
o
n
th
e
co
n
ce
r
n
e
d
s
y
s
te
m
u
n
d
er
d
if
f
er
en
t
r
ela
y
s
elec
tio
n
s
ce
n
ar
io
s
is
d
e
m
o
n
s
tr
ated
T
h
e
r
esu
lt
s
h
o
w
s
t
h
at
as
1
in
cr
ea
s
es,
b
o
th
th
e
e
n
er
g
y
h
ar
v
est
ed
an
d
r
ec
eiv
ed
s
ig
n
al
at
t
h
e
r
ela
y
n
o
d
es
b
ec
o
m
e
w
ea
k
er
ca
u
s
in
g
t
h
e
s
y
s
t
e
m
o
u
tag
e
p
r
o
b
ab
ilit
y
to
b
e
d
eg
r
ad
ed
.
Ho
w
ev
er
,
b
ey
o
n
d
a
n
o
p
tim
u
m
d
i
s
ta
n
ce
o
f
1
w
h
er
e
th
e
d
is
ta
n
ce
b
et
w
e
en
th
e
r
ela
y
an
d
d
esti
n
a
tio
n
b
ec
o
m
e
s
s
m
aller
,
th
e
s
y
s
te
m
o
u
ta
g
e
p
r
o
b
ab
ilit
y
s
tar
ts
d
ec
r
ea
s
in
g
ev
e
n
w
it
h
less
tr
an
s
m
it
p
o
w
er
f
o
r
th
e
r
elay
to
tr
an
s
m
it
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2
0
8
8
-
8708
I
n
t J
E
lec
&
C
o
m
p
E
n
g
,
Vo
l.
10
,
No
.
5
,
Octo
b
e
r
2
0
2
0
:
5
2
9
6
-
5305
5302
in
f
o
r
m
atio
n
.
I
r
r
esp
ec
ti
v
e
o
f
t
h
is
,
th
e
b
es
t
r
ela
y
s
elec
tio
n
o
f
f
er
s
th
e
s
y
s
te
m
b
etter
p
er
f
o
r
m
an
ce
t
h
an
t
h
e
w
o
r
s
t
r
ela
y
s
elec
tio
n
.
T
h
e
o
u
tag
e
p
er
f
o
r
m
an
ce
o
f
t
h
e
co
n
ce
r
n
ed
s
y
s
te
m
u
n
d
er
d
if
f
er
e
n
t
v
al
u
e
s
o
f
ch
a
n
n
e
l
co
r
r
elatio
n
co
ef
f
icie
n
t
a
t
d
if
f
er
e
n
t
r
ela
y
d
is
tan
t
is
i
llu
s
tr
ated
i
n
F
i
g
u
r
e
3
.
T
h
e
r
esu
lts
s
h
o
w
th
a
t
as
th
e
tr
a
n
s
m
it
SN
R
in
cr
ea
s
e
t
h
e
b
etter
th
e
s
y
s
te
m
o
u
ta
g
e
p
r
o
b
ab
ilit
y
.
I
n
ad
d
itio
n
,
it
ca
n
b
e
d
ep
icted
th
at
th
e
i
n
cr
ea
s
e
i
n
co
r
r
elatio
n
co
ef
f
icien
t
t
h
e
b
ett
er
th
e
s
y
s
te
m
o
u
ta
g
e
p
er
f
o
r
m
a
n
ce
.
Ho
w
ev
er
,
th
e
a
s
t
h
e
r
ela
y
s
lo
ca
tio
n
f
ar
f
r
o
m
th
e
s
o
u
r
ce
,
th
e
w
o
r
s
e
t
h
e
o
u
ta
g
e
p
er
f
o
r
m
an
ce
b
ec
o
m
e
s
d
u
e
to
less
tr
an
s
m
it
p
o
w
er
r
ec
eiv
e
d
at
th
e
r
elay
n
o
d
e
f
o
r
in
f
o
r
m
atio
n
tr
an
s
m
is
s
io
n
.
T
h
e
r
esu
lts
also
i
n
d
icate
d
th
e
s
i
m
u
latio
n
r
esu
lt
p
er
f
ec
tl
y
m
atc
h
w
it
h
th
e
an
al
y
tica
l r
esu
l
t
w
h
ic
h
p
r
o
v
es t
h
e
co
r
r
ec
tn
ess
o
f
o
u
r
d
er
iv
ed
ex
p
r
ess
io
n
s
.
T
h
e
ef
f
ec
t
o
f
ch
a
n
n
e
l
co
r
r
elatio
n
co
ef
f
ic
ien
t
o
n
t
h
e
A
B
E
R
o
f
th
e
s
y
s
te
m
is
ill
u
s
tr
at
ed
in
F
ig
u
r
e
4
u
n
d
er
d
i
f
f
er
e
n
t
n
u
m
b
er
o
f
an
ten
n
a
at
t
h
e
d
es
tin
a
tio
n
.
I
t
ca
n
b
e
clea
r
l
y
s
ee
n
t
h
at
in
cr
ea
s
e
in
th
e
n
u
m
b
er
o
f
d
esti
n
atio
n
an
te
n
n
a
lead
s
to
r
ed
u
ctio
n
i
n
th
e
s
y
s
te
m
er
r
o
r
p
er
f
o
r
m
a
n
ce
.
I
t is also
d
ep
icted
f
r
o
m
th
e
r
es
u
lt
s
th
a
t
th
e
h
ig
h
er
t
h
e
c
h
an
n
el
co
r
r
elatio
n
t
h
e
b
etter
t
h
e
s
y
s
te
m
p
er
f
o
r
m
a
n
ce
.
T
h
e
r
es
u
lts
also
in
d
icate
th
a
t
th
e
an
al
y
tica
l r
esu
l
ts
ar
e
w
ell
ag
r
ee
d
w
it
h
t
h
e
s
i
m
u
latio
n
r
es
u
lts
w
h
ic
h
s
h
o
w
s
t
h
e
ac
cu
r
ac
y
o
f
o
u
r
d
er
iv
atio
n
.
T
h
e
er
r
o
r
p
er
f
o
r
m
an
ce
a
s
a
f
u
n
ctio
n
o
f
en
er
g
y
h
ar
v
e
s
ti
n
g
ti
m
e
is
p
r
ese
n
ted
in
F
ig
u
r
e
5
u
n
d
er
n
u
m
b
er
o
f
r
ela
y
s
elec
tio
n
.
I
t
ca
n
b
e
s
h
o
w
n
t
h
at
as
t
h
e
en
er
g
y
h
ar
v
esti
n
g
ti
m
e
i
n
cr
ea
s
es
t
h
e
b
etter
th
e
s
y
s
te
m
er
r
o
r
p
er
f
o
r
m
a
n
ce
.
T
h
is
i
s
o
w
in
g
t
o
th
e
lar
g
e
a
m
o
u
n
t
o
f
t
i
m
e
a
v
ailab
le
f
o
r
r
ela
y
n
o
d
es
to
r
ep
len
is
h
ed
en
er
g
y
f
o
r
in
f
o
r
m
atio
n
tr
a
n
s
m
is
s
io
n
.
A
l
s
o
,
th
e
in
cr
ea
s
e
in
th
e
n
u
m
b
er
o
f
r
elay
s
elec
t
io
n
f
o
r
tr
an
s
m
is
s
io
n
s
ig
n
i
f
ica
n
tl
y
i
m
p
r
o
v
es t
h
e
s
y
s
te
m
er
r
o
r
p
er
f
o
r
m
a
n
ce
.
Fig
u
r
e
2.
Ou
tag
e
p
r
o
b
ab
ilit
y
v
s
th
e
S
-
to
-
R
d
is
ta
n
ce
u
n
d
er
d
if
f
er
en
t
n
u
m
b
er
o
f
at
=
0
.
5
,
=
0
.
6
,
an
d
2
=
6
−
1
Fig
u
r
e
3
.
E
f
f
ec
t o
f
co
r
r
elatio
n
co
ef
f
icie
n
t o
n
th
e
s
y
s
te
m
o
u
ta
g
e
p
r
o
b
ab
ilit
y
u
n
d
er
d
if
f
er
e
n
t S
-
to
-
R
d
is
ta
n
ce
Fig
u
r
e
4
.
I
m
p
ac
t o
f
n
u
m
b
e
r
o
f
an
ten
n
a
at
t
h
e
d
esti
n
atio
n
o
n
th
e
s
y
s
te
m
A
B
E
R
u
n
d
er
d
if
f
er
e
n
t
co
r
r
elatio
n
co
ef
f
icie
n
ts
at
=
0
.
6
,
=
=
4
Fig
u
r
e
5
.
A
B
E
R
p
er
f
o
r
m
a
n
ce
o
f
th
e
s
y
s
te
m
u
n
d
er
d
if
f
er
en
t r
ela
y
s
elec
t
io
n
at
=
4
,
=
0
.
6
,
=
2
,
=
2
Evaluation Warning : The document was created with Spire.PDF for Python.
I
n
t J
E
lec
&
C
o
m
p
E
n
g
I
SS
N:
2088
-
8708
On
th
e
p
erfo
r
ma
n
ce
o
f e
n
erg
y
h
a
r
ve
s
tin
g
A
F
p
a
r
tia
l rela
y
s
elec
tio
n
…
(
K
eh
in
d
e
O.
Od
ey
emi
)
5303
I
n
F
ig
u
r
e
6
,
th
e
th
r
o
u
g
h
p
u
t
p
er
f
o
r
m
an
ce
o
f
t
h
e
s
y
s
te
m
as
a
f
u
n
ctio
n
o
f
e
n
er
g
y
h
ar
v
e
s
ti
n
g
ti
m
e
is
d
ep
icted
u
n
d
er
d
if
f
er
en
t
av
er
ag
e
tr
an
s
m
i
t
SN
R
.
T
h
e
r
esu
lt
s
s
h
o
w
t
h
at
t
h
e
in
cr
ea
s
e
in
t
h
e
s
o
u
r
ce
tr
an
s
m
it
p
o
w
er
,
th
e
h
i
g
h
er
th
e
s
y
s
te
m
t
h
r
o
u
g
h
p
u
t
b
ec
au
s
e
lar
g
er
e
n
e
r
g
y
is
h
ar
v
e
s
ted
at
r
ela
y
n
o
d
es.
I
t
ca
n
b
e
d
ed
u
ce
d
f
r
o
m
t
h
e
r
esu
lt
s
th
a
t,
at
h
ig
h
t
r
an
s
m
it
p
o
w
er
,
th
e
o
p
ti
m
u
m
t
i
m
e
is
v
er
y
s
h
o
r
t
f
o
r
en
er
g
y
h
ar
v
esti
n
g
a
n
d
lar
g
e
ti
m
e
i
s
u
s
ed
to
d
ec
o
d
e
in
f
o
r
m
atio
n
.
C
o
m
p
ar
e
w
it
h
t
h
e
l
o
w
er
tr
an
s
m
it
p
o
w
er
.
T
h
e
an
al
y
tical
r
es
u
l
t
s
ar
e
p
er
f
ec
tl
y
m
atc
h
ed
w
i
th
t
h
e
s
i
m
u
latio
n
r
es
u
lt
s
s
h
o
w
in
g
t
h
e
ac
cu
r
ac
y
o
f
t
h
e
d
er
iv
ed
ex
p
r
ess
io
n
.
T
h
e
th
r
o
u
g
h
p
u
t
as
a
f
u
n
ctio
n
o
f
r
ela
y
d
is
ta
n
ce
f
r
o
m
t
h
e
s
o
u
r
ce
u
n
d
er
d
i
f
f
er
e
n
t
n
u
m
b
er
o
f
an
ten
n
a
a
t
th
e
d
esti
n
a
tio
n
is
d
e
m
o
n
s
tr
ate
d
in
F
i
g
u
r
e
7
.
T
h
e
r
esu
lt
s
i
n
d
icate
th
a
t
t
h
e
s
y
s
te
m
p
er
f
o
r
m
a
n
ce
i
s
s
ig
n
i
f
ica
n
tl
y
i
m
p
r
o
v
ed
w
it
h
t
h
e
in
cr
ea
s
e
in
th
e
n
u
m
b
er
o
f
a
n
te
n
n
a
at
th
e
d
esti
n
atio
n
.
I
t
ca
n
b
e
s
ee
n
f
r
o
m
t
h
e
r
es
u
lts
th
at
a
t
s
m
al
l
v
al
u
es
1
,
th
e
s
y
s
te
m
th
r
o
u
g
h
p
u
t
b
ec
o
m
es
d
eg
r
ad
ed
d
u
e
to
lar
g
er
d
is
tan
ce
b
et
w
ee
n
th
e
r
ela
y
a
n
d
th
e
d
esti
n
atio
n
,
a
n
d
th
e
o
u
ta
g
e
p
r
o
b
ab
ilit
y
i
s
h
ig
h
at
t
h
e
r
eg
i
m
e.
T
h
u
s
,
at
t
h
e
o
p
ti
m
u
m
r
ela
y
lo
ca
tio
n
,
th
e
s
y
s
te
m
p
er
f
o
r
m
a
n
ce
s
tar
ts
in
cr
ea
s
in
g
s
n
ice
t
h
e
s
m
al
ler
v
alu
e
o
f
2
r
esu
lt
in
to
h
ig
h
er
s
y
s
te
m
t
h
r
o
u
g
h
p
u
t
w
it
h
b
etter
s
y
s
te
m
o
u
ta
g
e.
As
e
x
p
ec
ted
,
th
e
r
esu
lts
d
ep
ict
th
at
t
h
e
s
y
s
te
m
h
as
b
etter
p
er
f
o
r
m
an
ce
u
n
d
er
th
e
b
est r
ela
y
s
elec
tio
n
co
m
p
a
r
e
w
it
h
w
o
r
s
t r
ela
y
s
e
lectio
n
.
T
h
e
th
r
o
u
g
h
p
u
t
p
er
f
o
r
m
a
n
ce
o
f
th
e
s
y
s
te
m
at
d
i
f
f
er
e
n
t
c
h
an
n
el
co
r
r
elatio
n
co
ef
f
icie
n
t
an
d
is
d
ep
icted
in
F
ig
u
r
e
8
.
I
t
ca
n
b
e
s
ee
n
f
r
o
m
t
h
e
r
es
u
lt
s
t
h
at
h
ig
h
er
th
r
o
u
g
h
p
u
t
p
er
f
o
r
m
an
ce
c
an
b
e
ac
h
ie
v
ed
w
it
h
th
e
b
est
r
ela
y
s
elec
tio
n
a
t
h
i
g
h
SN
R
.
A
t
lo
w
an
d
h
ig
h
SN
R
,
th
e
th
r
o
u
g
h
p
u
t
b
ec
o
m
e
s
s
at
u
r
ated
w
h
ic
h
s
h
o
w
s
th
at
t
h
e
o
u
ta
g
e
p
r
o
b
ab
ilit
y
h
a
s
h
i
g
h
er
a
n
d
lo
w
er
v
a
lu
e
s
r
es
p
e
ctiv
el
y
.
I
n
ad
d
itio
n
,
th
e
r
es
u
lts
al
s
o
p
r
o
v
e
th
at
in
cr
ea
s
e
i
n
t
h
e
co
r
r
elatio
n
co
ef
f
icien
t
s
i
g
n
if
ican
t
l
y
i
m
p
r
o
v
e
th
e
s
y
s
te
m
p
er
f
o
r
m
a
n
ce
.
T
h
e
s
i
m
u
lat
io
n
r
es
u
lt
s
p
er
f
ec
t
m
atc
h
ed
w
ith
t
h
e
a
n
al
y
tical
r
es
u
lt
s
w
h
ic
h
i
n
d
icate
th
e
co
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[1
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K.
Zh
u
,
F
.
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[9
]
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He
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3
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