I
nte
rna
t
io
na
l J
o
urna
l o
f
E
lect
rica
l a
nd
Co
m
p
ute
r
E
ng
in
ee
ring
(
I
J
E
CE
)
Vo
l.
7
,
No
.
2
,
A
p
r
il
201
7
,
p
p
.
741
~
7
4
7
I
SS
N:
2
0
8
8
-
8708
,
DOI
: 1
0
.
1
1
5
9
1
/
i
j
ec
e
.
v7
i
2
.
p
p
7
4
1
-
7
4
7
741
J
o
ur
na
l ho
m
ep
a
g
e
:
h
ttp
:
//ia
e
s
jo
u
r
n
a
l.c
o
m/o
n
lin
e/in
d
ex
.
p
h
p
/I
JE
C
E
Focus
ing
Proper
t
ies
o
f
a
M
o
dified
Retarding
S
truc
t
ure
for
Linea
r Electr
o
n
Accelerato
rs
Vla
di
m
ir
K
uz
'
m
ich
Sh
ilo
v
,
Aleks
a
nd
r
Ni
k
o
la
ev
ich F
ila
t
o
v
,
Aleks
a
nd
r
E
v
g
en'ev
ich N
o
v
o
zhilo
v
Na
ti
o
n
a
l
Re
se
a
rc
h
Nu
c
lea
r
Un
iv
e
rsity
M
EP
h
I
(
M
o
sc
o
w
En
g
in
e
e
rin
g
P
h
y
sic
s In
stit
u
te)
,
Ka
sh
irsk
o
y
e
S
h
o
ss
e
3
1
,
M
o
sc
o
w
,
1
1
5
4
0
9
,
R
u
ss
ian
F
e
d
e
ra
ti
o
n
Art
icle
I
nfo
AB
ST
RAC
T
A
r
ticle
his
to
r
y:
R
ec
eiv
ed
J
u
n
9
,
2
0
1
6
R
ev
i
s
ed
Ma
r
1
0
,
2
0
1
7
A
cc
ep
ted
Ma
r
2
4
,
2
0
1
7
W
h
e
n
u
sin
g
a
c
c
e
lera
to
rs
in
in
d
u
stry
a
n
d
m
e
d
icin
e
,
im
p
o
rtan
t
a
re
th
e
d
im
e
n
sio
n
s
o
f
th
e
d
e
v
ice
u
se
d
,
e
sp
e
c
iall
y
th
e
ra
d
ial
o
n
e
s.
In
th
e
li
n
e
a
r
e
lec
tro
n
a
c
c
e
lera
to
rs
b
a
se
d
o
n
a
b
ip
e
ri
o
d
ic
re
tar
d
in
g
stru
c
t
u
re
,
w
h
ich
o
p
e
ra
tes
in
th
e
sta
n
d
i
n
g
w
a
v
e
m
o
d
e
,
th
e
re
is
a
p
o
ss
ib
il
it
y
to
p
ro
v
id
e
f
o
c
u
sin
g
o
f
th
e
a
c
c
e
lera
t
e
d
p
a
rti
c
les
w
it
h
th
e
h
e
lp
o
f
h
ig
h
-
f
re
q
u
e
n
c
y
f
ield
s
w
it
h
o
u
t
th
e
u
se
o
f
e
x
tern
a
l
f
o
c
u
sin
g
e
le
m
e
n
ts.
In
th
e
a
c
c
e
lera
ti
n
g
c
e
ll
,
d
u
e
to
t
h
e
p
re
se
n
c
e
o
f
th
e
f
a
r
p
ro
tru
d
in
g
d
rif
t
sle
e
v
e
s,
th
e
e
lec
tri
c
f
ield
li
n
e
s
b
e
c
o
m
e
stro
n
g
ly
c
u
rv
e
d
,
w
h
ich
lea
d
s
to
th
e
a
p
p
e
a
ra
n
c
e
in
t
h
e
re
g
io
n
s
a
d
jac
e
n
t
to
th
e
se
sle
e
v
e
s
o
f
a
su
b
sta
n
ti
a
l
in
m
a
g
n
it
u
d
e
ra
d
ial
c
o
m
p
o
n
e
n
t
o
f
t
h
e
e
lec
tri
c
f
ield
.
T
h
e
p
a
rti
c
les
e
n
terin
g
th
e
a
c
c
e
ler
a
ti
n
g
g
a
p
e
x
p
e
rien
c
e
th
e
a
c
ti
o
n
o
f
a
f
o
rc
e
d
irec
ted
to
w
a
rd
th
e
a
x
is
o
f
th
e
sy
ste
m
,
a
n
d
a
t
t
h
e
e
x
it
,
o
f
a
f
o
rc
e
d
irec
ted
a
w
a
y
f
ro
m
th
e
a
x
is.
U
n
d
e
r
c
e
rtain
c
o
n
d
it
io
n
s,
a
lt
e
rn
a
ti
o
n
o
f
th
e
f
o
c
u
sin
g
a
n
d
d
e
f
o
c
u
sin
g
f
ield
s
c
a
n
lea
d
t
o
a
g
e
n
e
ra
l
f
o
c
u
sin
g
e
ff
e
c
t.
In
th
e
p
a
p
e
r
w
e
stu
d
y
th
e
f
o
c
u
sin
g
p
ro
p
e
rti
e
s
o
f
a
m
o
d
if
i
e
d
b
ip
e
rio
d
i
c
stru
c
tu
re
w
it
h
sta
n
d
in
g
w
a
v
e
.
T
h
e
m
a
in
a
tt
e
n
ti
o
n
is
p
a
id
to
t
h
e
p
o
ss
ib
il
i
ty
o
f
u
sin
g
th
e
f
o
c
u
sin
g
p
ro
p
e
rti
e
s
o
f
th
e
e
lec
tro
m
a
g
n
e
ti
c
a
c
c
e
lera
ti
n
g
f
ield
f
o
r
g
u
id
i
n
g
th
e
e
lec
tro
n
b
e
a
m
th
ro
u
g
h
th
e
a
p
e
rt
u
re
o
f
th
e
a
c
c
e
ler
a
ti
n
g
s
y
ste
m
,
w
h
ich
w
il
l
l
e
a
d
to
a
sig
n
if
ic
a
n
t
re
d
u
c
ti
o
n
in
th
e
a
c
c
e
lera
to
r
siz
e
s.
T
h
e
p
ro
p
o
s
e
d
m
e
th
o
d
c
a
n
b
e
a
p
p
l
ied
i
n
t
h
e
c
a
lcu
latio
n
a
n
d
d
e
sig
n
o
f
li
n
e
a
r
e
lec
tro
n
a
c
c
e
lera
to
rs.
K
ey
w
o
r
d
:
A
cc
ep
ta
n
ce
s
tr
u
c
tu
r
es
B
ea
m
e
m
it
tan
ce
B
ip
er
io
d
ic
r
etar
d
in
g
s
y
s
te
m
Dr
if
t
s
lee
v
e
E
lectr
o
m
a
g
n
etic
f
ield
o
f
t
h
e
ce
ll
E
lectr
o
n
lin
ea
r
ac
ce
ler
ato
r
P
ar
ticle
d
y
n
a
m
ic
s
S
tan
d
i
n
g
w
a
v
e
T
h
e
d
r
if
t c
h
an
n
el
ap
er
tu
r
e
Co
p
y
rig
h
t
©
2
0
1
7
In
stit
u
te o
f
A
d
v
a
n
c
e
d
E
n
g
i
n
e
e
rin
g
a
n
d
S
c
ien
c
e
.
Al
l
rig
h
ts
re
se
rv
e
d
.
C
o
r
r
e
s
p
o
nd
ing
A
uth
o
r
:
Vlad
i
m
ir
K
u
z’
m
ic
h
S
h
ilo
v
,
Dep
ar
t
m
en
t o
f
A
u
to
m
atio
n
an
d
E
lectr
o
n
ics
,
Natio
n
al
R
e
s
ea
r
ch
N
u
clea
r
Un
iv
er
s
it
y
ME
P
h
I
(
Mo
s
co
w
E
n
g
in
ee
r
in
g
P
h
y
s
ic
s
I
n
s
t
itu
te)
,
Kash
ir
s
k
o
y
e
s
h
o
s
s
e
3
1
,
Mo
s
co
w
,
1
1
5
4
0
9
,
R
u
s
s
ia
n
Fed
er
ati
o
n
.
E
m
ail:
VK
Sh
ilo
v
@
m
ep
h
i.r
u
1.
I
NT
RO
D
UCT
I
O
N
T
h
e
in
ter
est
i
n
t
h
e
u
s
e
o
f
li
n
ea
r
elec
tr
o
n
ac
ce
ler
ato
r
s
(
L
E
A
)
i
n
i
n
d
u
s
tr
y
a
n
d
m
ed
ici
n
e
ca
n
b
e
attr
ib
u
ted
to
a
n
u
m
b
er
o
f
t
h
eir
ad
v
an
ta
g
es.
A
n
a
n
al
y
s
i
s
o
f
th
e
o
u
tp
u
t
ch
ar
ac
ter
i
s
tics
o
f
th
e
d
ec
eler
atio
n
r
ad
iatio
n
in
d
ef
ec
to
s
co
p
y
a
n
d
r
ad
iatio
n
th
er
ap
y
[
1
]
s
h
o
w
s
t
h
at
a
lar
g
e
p
ar
t
o
f
th
e
r
ad
iatio
n
p
r
o
b
lem
s
i
n
th
e
s
e
f
ield
s
ca
n
b
e
s
o
l
v
ed
w
it
h
th
e
h
elp
o
f
L
E
A
f
o
r
t
h
e
en
er
g
y
o
f
an
d
th
e
p
u
ls
e
c
u
r
r
en
t
o
f
.
I
n
ad
d
itio
n
,
t
h
e
ac
ce
ler
ato
r
s
u
s
ed
in
d
ef
ec
to
s
co
p
y
a
n
d
m
ed
icin
e
s
h
o
u
ld
b
e
co
m
p
ac
t
an
d
h
a
v
e
s
m
a
ll
lo
n
g
it
u
d
i
n
al
a
n
d
tr
an
s
v
er
s
e
d
i
m
en
s
io
n
s
.
U
n
d
o
u
b
ted
l
y
,
r
e
d
u
cin
g
t
h
e
s
izes
a
n
d
w
ei
g
h
t
o
f
t
h
e
r
ad
iatio
n
in
s
ta
llatio
n
s
is
an
i
m
p
o
r
ta
n
t
an
d
u
r
g
e
n
t
tas
k
.
Fro
m
th
e
v
er
y
b
eg
i
n
n
i
n
g
,
t
h
is
p
r
o
b
lem
w
a
s
s
o
lv
ed
b
y
th
e
tr
an
s
itio
n
to
t
h
e
t
h
r
ee
-
ce
n
ti
m
eter
w
a
v
ele
n
g
th
r
a
n
g
e.
C
u
r
r
en
tl
y
,
th
e
r
ed
u
ctio
n
o
f
t
h
e
lo
n
g
it
u
d
in
al
d
i
m
e
n
s
io
n
s
ca
n
b
e
ac
h
ie
v
ed
b
y
s
w
itc
h
in
g
to
th
e
s
ta
n
d
in
g
w
a
v
e
m
o
d
e
[
2
]
.
I
n
th
i
s
ca
s
e,
a
s
th
e
r
etar
d
i
n
g
s
y
s
te
m
s
i
n
t
h
e
L
E
A
w
it
h
s
ta
n
d
in
g
w
a
v
e,
t
h
e
b
ip
er
io
d
ic
r
etar
d
in
g
s
tr
u
ct
u
r
es
(
B
R
S)
[
3
]
ar
e
u
s
ed
,
w
h
ic
h
ar
e
c
h
ar
ac
ter
ized
b
y
h
i
g
h
v
alu
e
s
o
f
th
e
s
p
ec
i
f
ic
s
h
u
n
t r
e
s
is
ta
n
ce
s
a
n
d
th
e
g
r
ad
ien
t o
f
t
h
e
ac
ce
ler
atin
g
f
ield
.
As
is
k
n
o
w
n
,
in
t
h
e
tr
av
eli
n
g
w
a
v
e
L
E
A
,
t
h
e
p
ar
ticle
g
ai
n
s
en
er
g
y
o
n
l
y
u
n
d
er
th
e
co
n
d
i
tio
n
o
f
t
he
s
y
n
ch
r
o
n
o
u
s
m
o
v
e
m
e
n
t
w
it
h
th
e
ac
ce
ler
ati
n
g
w
a
v
e.
D
u
e
to
th
e
r
elati
v
el
y
lo
w
s
h
u
n
t
r
esis
ta
n
ce
o
f
th
e
ac
ce
ler
atin
g
s
tr
u
ct
u
r
es
o
p
er
atin
g
i
n
t
h
e
tr
av
el
in
g
w
a
v
e
m
o
d
e,
th
e
ac
ce
ler
ated
p
ar
ticle
s
h
o
u
ld
b
e
at
t
h
e
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2088
-
8708
I
J
E
C
E
Vo
l.
7
,
No
.
2
,
A
p
r
il 2
0
1
7
:
7
4
1
–
747
742
m
ax
i
m
u
m
o
f
t
h
e
ac
ce
ler
atin
g
f
ield
.
T
h
e
co
n
s
tan
t
in
f
l
u
e
n
c
e
o
n
th
e
p
ar
ticle
f
r
o
m
th
e
r
ad
ial
co
m
p
o
n
e
n
t
o
f
elec
tr
ic
f
ield
w
h
ic
h
d
ef
lects
it
f
r
o
m
th
e
ax
is
is
th
e
r
ea
s
o
n
t
h
a
t th
e
e
x
ter
n
al
f
o
cu
s
i
n
g
ele
m
e
n
ts
,
esp
ec
iall
y
in
t
h
e
b
eg
in
n
i
n
g
o
f
ac
ce
ler
atio
n
,
h
av
e
b
ec
o
m
e
an
in
teg
r
al
p
ar
t
o
f
th
e
d
esig
n
o
f
th
e
tr
av
e
lin
g
w
av
e
ac
ce
ler
ato
r
s
.
T
h
is
r
eq
u
ir
es a
d
d
itio
n
al
en
er
g
y
co
s
ts
an
d
m
a
k
es t
h
e
ac
ce
ler
ato
r
d
esig
n
m
o
r
e
cu
m
b
er
s
o
m
e.
A
s
p
ec
ial
p
lace
a
m
o
n
g
th
e
B
R
S
t
h
at
ar
e
w
id
el
y
u
s
ed
as
ac
ce
ler
atin
g
s
y
s
te
m
s
f
o
r
t
h
e
li
n
e
ar
elec
tr
o
n
ac
ce
ler
ato
r
s
f
o
r
lo
w
e
n
er
g
y
w
i
th
a
s
tan
d
i
n
g
w
av
e
i
s
o
cc
u
p
ied
b
y
th
e
s
tr
u
c
tu
r
e
[
4
]
,
u
s
i
n
g
w
h
ich
it i
s
p
o
s
s
ib
le
to
ac
h
iev
e
a
h
i
g
h
r
ate
o
f
ac
ce
le
r
atio
n
.
C
o
n
ce
r
n
i
n
g
t
h
is
s
tr
u
c
t
u
r
e
,
th
er
e
i
s
a
p
r
es
s
in
g
is
s
u
e
o
f
p
r
o
v
id
in
g
r
ad
ial
f
o
cu
s
in
g
o
f
t
h
e
ac
ce
ler
ated
p
ar
ticles,
s
i
n
ce
t
h
e
o
u
ter
d
ia
m
et
er
o
f
th
e
s
tr
u
ctu
r
e
d
u
e
to
later
al
co
n
n
ec
t
io
n
ce
ll
s
ex
ten
d
i
n
g
f
r
o
m
t
h
e
f
o
u
r
s
id
e
s
o
f
t
h
e
ac
ce
ler
ati
n
g
ce
l
ls
ar
r
an
g
ed
o
n
o
n
e
ax
i
s
is
ap
p
r
o
x
i
m
atel
y
t
w
ice
t
h
e
d
ia
m
eter
o
f
t
h
e
ac
ce
ler
ati
n
g
s
tr
u
ctu
r
e
s
w
it
h
t
h
e
ax
ia
l
co
n
n
e
ctio
n
ce
lls
,
a
n
d
th
e
u
s
e
o
f
co
n
v
e
n
tio
n
al
f
o
cu
s
i
n
g
d
ev
ices
i
s
t
h
er
e
f
o
r
e
ass
o
ciate
d
w
i
th
a
co
n
s
id
er
ab
le
in
cr
ea
s
e
in
th
e
tr
an
s
v
er
s
e
d
i
m
en
s
io
n
w
h
ic
h
i
s
alr
ea
d
y
lar
g
e.
Mo
r
eo
v
er
,
th
e
m
as
s
o
f
t
h
e
ac
ce
ler
ato
r
’
s
tr
an
s
m
i
tte
r
u
n
it
in
cr
ea
s
es,
a
n
d
th
er
e
a
r
is
es
t
h
e
n
ee
d
to
in
tr
o
d
u
ce
in
to
th
e
i
n
s
talla
tio
n
t
h
e
p
o
w
er
s
u
p
p
lies
f
o
r
th
e
f
o
cu
s
in
g
ele
m
en
ts
.
2.
M
E
T
H
O
DS
2
.
1
G
ener
a
l St
a
t
e
m
ent
s
B
R
S
in
th
e
L
E
A
,
w
o
r
k
i
n
g
i
n
th
e
s
ta
n
d
in
g
w
av
e
m
o
d
e,
ca
n
b
e
co
n
s
id
er
ed
as
a
ch
ain
o
f
ac
ce
ler
atin
g
ca
v
itie
s
,
ar
r
an
g
ed
o
n
a
s
in
g
le
ax
is
an
d
lin
k
ed
b
y
t
h
e
co
n
n
ec
tio
n
ce
ll
s
[
5
]
.
Si
n
ce
th
e
co
n
n
e
ctio
n
ce
ll
s
ar
e
f
r
ee
f
r
o
m
elec
tr
o
m
ag
n
etic
f
ield
s
a
n
d
n
o
t
i
n
v
o
l
v
ed
i
n
th
e
p
ar
ticl
e
ac
ce
ler
atio
n
,
th
e
y
m
a
y
b
e
p
lace
d
o
u
ts
id
e
o
f
t
h
e
ac
ce
ler
atin
g
s
tr
u
ct
u
r
e.
T
h
e
o
s
cillatio
n
s
o
f
elec
tr
o
m
a
g
n
etic
f
ield
s
in
t
h
e
ad
j
ac
en
t
ac
ce
ler
atin
g
ca
v
itie
s
ar
e
d
if
f
er
e
n
t
i
n
p
h
a
s
e
b
y
;
th
er
e
f
o
r
e
,
th
e
p
ar
ticle
m
u
s
t
co
v
er
th
e
d
is
ta
n
ce
b
et
w
ee
n
t
h
e
ce
n
ter
s
o
f
ad
j
ac
en
t
ac
ce
ler
atin
g
ca
v
ities
d
u
r
i
n
g
t
h
e
ti
m
e
eq
u
al
to
h
al
f
t
h
e
p
er
io
d
o
f
elec
tr
o
m
ag
n
etic
o
s
cilla
tio
n
s
.
O
n
l
y
i
n
t
h
is
w
a
y
th
e
s
y
n
c
h
r
o
n
izat
io
n
is
ac
h
ie
v
e
d
b
et
w
ee
n
t
h
e
p
ar
ticle
an
d
th
e
ac
ce
ler
atin
g
f
ield
.
If
we
co
n
s
id
er
,
ata
f
ix
ed
m
o
m
en
t
of
ti
m
e,
t
h
e
d
is
tr
ib
u
t
io
n
f
u
n
ctio
n
of
t
h
e
elec
tr
o
m
a
g
n
etic
f
ield
in
te
n
s
it
y
alo
n
g
th
e
a
x
is
o
f
t
h
e
L
E
A
w
it
h
s
ta
n
d
i
n
g
w
a
v
e
,
th
en
w
e
ca
n
s
ee
t
h
at
th
is
f
u
n
ct
io
n
co
n
s
is
t
s
o
f
alter
n
ati
n
g
p
u
ls
e
s
o
f
d
if
f
er
en
t p
o
lar
ity
w
i
th
a
s
p
atial
p
er
io
d
eq
u
al
to
th
e
w
av
e
len
g
t
h
o
f
t
h
e
g
en
e
r
ato
r
.
Un
d
er
s
o
m
e
w
e
ll
-
k
n
o
w
n
co
n
d
itio
n
s
[
6
]
,
th
is
d
is
tr
ib
u
tio
n
f
u
n
ctio
n
ca
n
b
e
ex
p
an
d
ed
in
a
Fo
u
r
ier
s
er
ies,
an
d
th
e
s
tan
d
i
n
g
w
a
v
e
f
ie
ld
ca
n
b
e
r
ep
r
esen
ted
b
y
a
s
u
m
o
f
h
ar
m
o
n
ics.
T
h
e
p
ar
ticle
in
ter
ac
ts
ef
f
ec
tiv
e
l
y
o
n
l
y
w
it
h
t
h
e
h
ar
m
o
n
ic,
t
h
e
p
h
a
s
e
v
elo
cit
y
o
f
w
h
ic
h
eq
u
al
s
t
h
e
v
elo
cit
y
o
f
th
e
p
ar
ticle
m
o
t
io
n
.
C
o
n
s
eq
u
en
tl
y
,
th
e
lo
n
g
it
u
d
i
n
a
l
d
y
n
a
m
ics
o
f
th
e
p
ar
ticles
in
th
e
L
E
A
w
i
th
s
ta
n
d
i
n
g
w
a
v
e
ca
n
b
e
s
t
u
d
ied
b
y
th
e
m
e
th
o
d
s
u
s
ed
in
t
h
e
tr
av
e
li
n
g
w
a
v
e
ac
ce
ler
ato
r
s
.
W
h
en
co
n
s
id
er
in
g
t
h
e
r
ad
ial
m
o
tio
n
o
f
t
h
e
p
ar
ticles,i
t
i
s
n
ec
e
s
s
ar
y
to
n
o
te
th
e
f
ac
t
th
at
t
h
e
lo
n
g
it
u
d
i
n
al
an
d
r
ad
ial
m
o
tio
n
s
ar
e
clo
s
el
y
co
n
n
ec
ted
an
d
th
eir
eq
u
atio
n
s
m
u
s
t
b
e
s
o
lv
ed
to
g
eth
er
.
I
n
th
e
L
E
A
w
it
h
s
ta
n
d
in
g
w
a
v
e
o
n
t
h
e
b
asis
o
f
B
R
S,
w
e
ca
n
n
o
te
s
o
m
e
s
p
ec
i
f
ic
ch
ar
ac
ter
is
tics
i
n
th
e
ca
lc
u
latio
n
o
f
th
e
r
ad
ial
m
o
tio
n
o
f
t
h
e
p
ar
ti
cles.
I
n
t
h
e
ca
s
e
o
f
th
e
ac
ce
le
r
atin
g
ca
v
it
ies
o
f
co
m
p
lex
s
h
ap
e
o
p
tim
ized
w
it
h
r
esp
ec
t
to
s
h
u
n
t
r
esi
s
tan
ce
,
t
h
er
e
ar
e
n
o
an
al
y
tical
e
x
p
r
ess
i
o
n
s
f
o
r
th
e
co
m
p
o
n
en
t
s
o
f
el
ec
tr
o
m
a
g
n
etic
f
ield
.
T
h
e
d
is
tr
ib
u
tio
n
s
o
f
t
h
e
el
ec
tr
o
m
a
g
n
etic
f
ield
co
m
p
o
n
e
n
ts
w
it
h
r
esp
ec
t
to
th
e
lo
n
g
it
u
d
i
n
al
co
o
r
d
in
ate
an
d
th
e
r
ad
iu
s
,
o
b
tain
ed
w
it
h
t
h
e
h
el
p
o
f
n
u
m
er
ical
m
eth
o
d
s
,
m
u
s
t
b
e
g
i
v
en
in
th
e
f
o
r
m
o
f
tab
les
o
v
er
t
h
e
e
n
tire
ap
er
tu
r
e
o
f
th
e
d
r
if
t
ch
an
n
el.
T
h
e
p
r
esen
ce
in
th
e
ac
ce
ler
atin
g
ce
ll
s
o
f
th
e
p
r
o
tr
u
d
in
g
d
r
if
t
s
leev
es
is
t
h
e
ca
u
s
e
o
f
s
tr
o
n
g
c
u
r
v
at
u
r
e
o
f
th
e
f
iel
d
lin
es
o
f
t
h
e
elec
tr
ic
f
ie
ld
,
w
h
ich
lead
s
to
t
h
e
ap
p
ea
r
an
ce
o
f
th
e
s
i
g
n
if
ican
t
in
m
ag
n
it
u
d
e
tr
an
s
v
er
s
e
elec
tr
ic
f
ield
at
t
h
e
p
lace
o
f
t
h
e
lar
g
est
cu
r
v
atu
r
e.
B
esid
es,
t
h
e
d
r
if
t
s
l
ee
v
e
s
s
h
ield
a
ce
r
tain
p
ar
t
o
f
th
e
d
r
if
t
ch
a
n
n
e
l
f
r
o
m
th
e
elec
tr
o
m
ag
n
etic
f
iel
d
,
r
esu
ltin
g
in
t
h
e
ap
p
ea
r
an
ce
in
th
e
ac
ce
ler
ati
n
g
s
tr
u
ct
u
r
e
o
f
th
e
p
er
io
d
icall
y
r
e
p
ea
ted
s
eg
m
e
n
ts
f
r
ee
f
r
o
m
e
le
ctr
o
m
a
g
n
etic
f
ield
.
2
.
2
Dy
na
m
ic
s
o
f
t
he
P
a
rt
icles
T
h
e
m
o
s
t
p
r
o
m
is
i
n
g
in
t
h
e
L
E
A
w
it
h
s
ta
n
d
in
g
w
av
e
is
t
h
e
i
m
p
le
m
e
n
tat
io
n
o
f
f
o
c
u
s
i
n
g
,
f
o
r
w
h
ic
h
th
e
f
o
cu
s
in
g
ac
t
io
n
o
f
t
h
e
elec
tr
o
m
ag
n
etic
f
ield
it
s
elf
is
u
s
ed
f
o
r
g
u
id
i
n
g
t
h
e
b
ea
m
[
7
]
.
As
m
en
tio
n
ed
ab
o
v
e,
i
t
b
ec
o
m
e
s
p
o
s
s
ib
le
d
u
e
to
th
e
ap
p
ea
r
an
ce
in
th
e
B
R
S
ce
lls
o
f
th
e
r
ad
ial
co
m
p
o
n
en
t
o
f
elec
tr
ic
f
ield
.
Usi
n
g
th
e
f
o
cu
s
in
g
p
r
o
p
er
ties
o
f
t
h
e
o
w
n
h
ig
h
-
f
r
eq
u
en
c
y
(
HF)
f
ield
o
f
t
h
e
B
R
S
s
i
g
n
if
ica
n
tl
y
r
ed
u
ce
s
t
h
e
tr
a
n
s
v
er
s
al
s
izes
o
f
t
h
e
ac
ce
ler
atin
g
s
ec
ti
o
n
an
d
lig
h
te
n
s
t
h
e
co
n
s
tr
u
ct
io
n
o
f
th
e
ac
ce
ler
ato
r
as
a
w
h
o
le.
Fu
r
t
h
er
m
o
r
e,
th
er
e
is
n
o
lo
n
g
er
th
e
n
ee
d
f
o
r
cu
m
b
er
s
o
m
e
p
o
w
er
s
o
u
r
ce
s
f
o
r
t
h
e
e
x
ter
n
al
f
o
c
u
s
i
n
g
d
ev
ice
s
cr
ea
ti
n
g
ad
d
itio
n
al
d
if
f
ic
u
ltie
s
i
n
t
h
e
u
s
e
o
f
ac
ce
ler
ato
r
s
,
w
h
ic
h
i
s
p
ar
ticu
lar
l
y
i
m
p
o
r
ta
n
t
w
h
e
n
u
s
ed
in
g
eo
lo
g
y
,
m
ed
icin
e
a
n
d
d
ef
ec
to
s
co
p
y
.
T
h
e
d
y
n
a
m
ic
s
o
f
t
h
e
b
ea
m
i
n
t
h
e
lin
ea
r
ac
ce
ler
ato
r
is
d
eter
m
in
ed
b
y
th
e
m
o
v
e
m
e
n
t o
f
ea
c
h
p
ar
ticle
co
n
tain
ed
i
n
th
e
b
ea
m
u
n
d
er
th
e
ac
tio
n
o
f
elec
tr
ic
a
n
d
m
a
g
n
etic
f
ield
s
.
I
f
w
e
a
s
s
u
m
e
th
at
t
h
e
p
ar
ticle
ch
ar
g
e
i
s
p
o
in
tlik
e
a
n
d
its
o
w
n
m
a
g
n
e
ti
c
m
o
m
e
n
t is ab
s
e
n
t [
8
]
,
th
en
t
h
e
eq
u
atio
n
o
f
m
o
tio
n
o
f
t
h
e
i
n
d
iv
id
u
al
p
ar
ticle
is
Evaluation Warning : The document was created with Spire.PDF for Python.
I
J
E
C
E
I
SS
N:
2
0
8
8
-
8708
F
o
cu
s
in
g
P
r
o
p
erti
es o
f a
Mo
d
ified
R
eta
r
d
in
g
S
tr
u
ctu
r
e
fo
r
Lin
ea
r
E
lectro
n
…
(
V
la
d
imir
K
u
z
’
mich
S
h
ilo
v
)
743
d
escr
ib
ed
b
y
th
e
f
o
llo
w
in
g
e
x
p
r
ess
io
n
(
)
[
]
(
1
)
w
h
er
e
is
ti
m
e,
an
d
ar
e
th
e
ch
ar
g
e
a
n
d
m
a
s
s
o
f
t
h
e
p
ar
tic
le,
is
t
h
e
v
elo
cit
y
o
f
t
h
e
p
ar
ti
cle,
is
t
h
e
m
ag
n
etic
co
n
s
ta
n
t,
an
d
ar
e
h
ig
h
-
f
r
eq
u
e
n
c
y
elec
tr
o
m
ag
n
etic
,
s
tatic
elec
tr
ical
o
r
m
a
g
n
e
tic
f
o
cu
s
i
n
g
f
ield
s
,
o
r
th
e
f
ield
s
cr
ea
ted
b
y
o
th
er
b
ea
m
p
ar
ticles.
B
ec
au
s
e
u
lti
m
atel
y
w
e
ar
e
in
ter
ested
in
t
h
e
tr
aj
ec
to
r
y
o
f
t
h
e
b
ea
m
p
ar
ticles
i
n
t
h
e
ac
ce
ler
a
to
r
,
th
e
eq
u
atio
n
(
1
)
s
h
o
u
ld
b
e
co
n
v
e
r
ted
to
a
f
o
r
m
co
n
v
e
n
ien
t
f
o
r
th
e
s
t
u
d
y
o
f
th
e
p
ar
ticle
d
y
n
a
m
ics,
th
a
t
i
s
,
w
e
s
h
o
u
ld
ex
p
r
ess
t
h
e
ac
ce
ler
atio
n
o
f
t
h
e
p
ar
ticle
th
r
o
u
g
h
its
s
p
ee
d
an
d
th
e
in
te
n
s
it
y
o
f
th
e
e
l
ec
tr
ic
an
d
m
a
g
n
et
ic
f
ield
s
.
Si
n
ce
t
h
e
v
elo
cit
ies
o
f
th
e
p
ar
ticles
i
n
th
e
ac
ce
ler
at
o
r
ar
e
clo
s
e
to
th
e
s
p
ee
d
o
f
lig
h
t,
t
h
e
n
,
u
s
in
g
t
h
e
w
ell
-
k
n
o
w
n
f
o
r
m
u
las o
f
r
elati
v
is
t
ic
m
ec
h
a
n
ics [
9
]
,
w
e
ca
n
g
et
√
{
[
]
(
)
}
(
2
)
In
g
e
n
er
al
,
t
h
e
v
ec
to
r
s
an
d
d
ep
en
d
on
t
h
e
co
o
r
d
in
ates
a
n
d
ti
m
e;
in
th
e
p
ar
ticu
lar
ca
s
e
,
wh
en
th
e
ti
m
e
d
ep
en
d
en
ce
is
ab
s
en
t
(
t
h
e
ca
s
e
of
th
e
s
tatic
elec
tr
ic
an
d
m
ag
n
etic
f
ield
s
)
,
t
h
e
f
o
r
m
u
la
r
etain
s
i
ts
f
o
r
m
.
L
et
u
s
p
r
o
j
ec
t
th
e
r
esu
lti
n
g
v
ec
to
r
eq
u
atio
n
(
2
)
o
n
th
e
c
o
o
r
d
in
ate
ax
es.
I
n
o
u
r
ca
s
e,
th
e
m
o
s
t
co
n
v
e
n
ien
t
is
to
u
s
e
a
c
y
lin
d
r
i
ca
l
co
o
r
d
in
ate
s
y
s
te
m
(
)
,
s
in
ce
t
h
e
d
r
if
t
c
h
a
n
n
e
l
an
d
t
h
e
elec
tr
o
m
a
g
n
etic
f
ield
f
o
r
th
e
lo
w
es
tt
y
p
e
o
f
o
s
cillatio
n
s
h
a
v
e
ax
ial
s
y
m
m
etr
y
.
L
et
u
s
m
o
v
e
to
th
e
d
im
e
n
s
io
n
le
s
s
co
o
r
d
in
ates
,
,
th
e
d
i
m
en
s
io
n
l
ess
ti
m
e
,
th
e
r
elativ
e
v
e
lo
cities
w
it
h
r
esp
ec
t
to
co
o
r
d
in
ates
,
an
d
th
e
d
i
m
en
s
io
n
le
s
s
co
m
p
o
n
en
t
s
o
f
th
e
elec
tr
ical
an
d
m
ag
n
et
ic
f
ield
s
,
w
h
ich
ca
n
b
e
ea
s
il
y
r
ed
u
ce
d
to
a
d
im
e
n
s
i
o
n
less
f
o
r
m
u
s
i
n
g
th
e
e
x
p
r
ess
i
o
n
s
:
(
)
(
)
(
)
(
)
w
h
er
e
is
t
h
e
w
av
ele
n
g
th
o
f
th
e
g
en
er
ato
r
,
As
a
r
esu
lt,
th
e
eq
u
atio
n
o
f
m
o
tio
n
o
f
th
e
ch
ar
g
ed
p
ar
ticle
ca
n
b
e
r
ep
r
esen
ted
b
y
a
s
y
s
te
m
o
f
eq
u
atio
n
s
i
n
d
i
m
en
s
io
n
le
s
s
q
u
an
titi
e
s
{
(
)
(
)
(
)
(
)
(
)
[
(
)
(
)
(
)
(
)
]
}
{
(
)
(
)
(
)
(
)
(
)
[
(
)
(
)
(
)
(
)
]
}
(
)
{
(
)
(
)
[
(
)
(
)
(
)
(
)
]
}
I
n
th
e
latter
s
y
s
te
m
o
f
eq
u
atio
n
s
,
√
is
th
e
e
n
er
g
y
o
f
t
h
e
p
ar
ticle
in
th
e
u
n
its
o
f
t
h
e
r
est e
n
er
g
y
.
T
h
e
r
esu
ltin
g
s
y
s
te
m
o
f
eq
u
a
tio
n
s
(
3
)
h
as
b
ee
n
tak
e
n
as
t
h
e
b
asis
f
o
r
th
e
s
tu
d
y
o
f
th
e
m
o
tio
n
o
f
p
ar
ticles in
t
h
e
ac
ce
ler
ato
r
s
w
i
th
s
ta
n
d
i
n
g
w
a
v
e.
D
u
e
to
th
e
f
ac
t th
at
it i
s
i
m
p
o
s
s
ib
le
to
p
r
es
en
t a
n
a
l
y
t
icall
y
th
e
elec
tr
o
m
ag
n
etic
f
ield
in
th
e
a
cc
eler
atin
g
ca
v
it
y
o
f
a
co
m
p
l
ex
s
h
ap
e,
t
h
e
co
r
r
esp
o
n
d
in
g
co
m
p
o
n
e
n
t
s
o
f
th
e
f
ield
,
i
n
cl
u
d
ed
in
th
e
r
ig
h
t
-
h
a
n
d
s
id
e,
s
h
o
u
ld
b
e
g
iv
e
n
as
a
tab
le.
T
h
e
ex
ter
n
a
l
m
ag
n
etic
f
ield
ca
n
b
e
o
f
a
n
y
t
y
p
e
an
d
is
also
g
iv
e
n
b
y
a
tab
le.
3.
DIS
CU
SS
I
O
N
AND
RE
SU
L
T
S
L
et
u
s
an
al
y
ze
th
e
e
f
f
ec
t
o
f
h
i
g
h
f
r
eq
u
en
c
y
(
HF)
f
o
cu
s
i
n
g
,
w
h
ic
h
in
th
e
co
n
s
id
er
ed
ca
s
e
h
a
s
a
n
u
m
b
er
o
f
f
ea
tu
r
es.
T
o
o
b
t
ain
a
clea
r
p
h
y
s
ical
p
ictu
r
e,
w
e
u
s
e
a
s
i
m
p
li
f
ied
m
at
h
e
m
atica
l
m
o
d
el
o
f
ac
ce
ler
atin
g
ce
ll
s
p
r
o
p
o
s
ed
in
[
1
0
]
,
w
ith
t
h
e
o
n
l
y
d
i
f
f
er
e
n
ce
th
at
its
lo
n
g
it
u
d
in
a
l
d
i
m
en
s
i
o
n
w
ill
b
e
t
w
o
ti
m
e
s
less
.
A
f
ter
ca
lcu
latio
n
s
,
w
e
co
n
clu
d
e
t
h
at
w
h
e
n
th
e
ac
ce
ler
at
in
g
f
ield
v
ar
ies
w
it
h
ti
m
e
ac
co
r
d
in
g
to
th
e
co
s
in
e
la
w
,
t
h
e
n
,
in
t
h
i
s
ca
s
e,
all
t
h
e
r
eg
io
n
s
o
f
th
e
in
it
ial
p
h
ase
s
o
f
t
h
e
elec
tr
o
n
f
l
y
in
g
i
n
,
f
o
r
w
h
ic
h
t
h
er
e
ar
e
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2088
-
8708
I
J
E
C
E
Vo
l.
7
,
No
.
2
,
A
p
r
il 2
0
1
7
:
7
4
1
–
747
744
r
ea
lized
th
e
co
n
d
it
io
n
s
o
f
ac
ce
ler
atin
g
an
d
f
o
c
u
s
i
n
g
b
y
t
h
e
co
r
r
esp
o
n
d
in
g
co
m
p
o
n
e
n
ts
o
f
t
h
e
HF
f
ield
,
w
il
l
b
e
s
h
i
f
ted
b
y
⁄
as c
o
m
p
ar
ed
to
th
e
an
alo
g
o
u
s
r
eg
io
n
s
f
o
r
th
e
tr
ad
itio
n
al
B
R
S
.
T
h
er
ef
o
r
e,
in
th
e
d
esig
n
o
f
t
h
e
ac
ce
ler
atin
g
ce
lls
w
it
h
th
e
d
r
if
t
s
lee
v
es
o
r
w
it
h
o
u
t
t
h
e
m
i
n
t
h
e
f
o
r
m
o
f
co
n
v
e
n
tio
n
al
c
y
li
n
d
r
ical
ac
ce
ler
atin
g
ca
v
itie
s
,
th
e
p
h
a
s
e
r
eg
io
n
s
o
f
s
i
m
u
lta
n
eo
u
s
ac
ce
l
er
atio
n
an
d
s
tab
le
r
ad
ial
m
o
tio
n
f
o
r
th
e
f
ir
s
t t
y
p
e
o
f
ce
lls
w
ill b
e
an
d
f
o
r
th
e
ce
ll
s
o
f
th
e
s
ec
o
n
d
t
y
p
e
w
h
er
e
I
t m
a
y
b
e
n
o
ted
th
at
t
h
e
ex
ten
t o
f
t
h
e
p
h
ase
r
eg
io
n
s
i
s
,
as b
ef
o
r
e,
.
I
n
t
h
e
p
ap
er
,
we
co
n
s
id
er
th
e
d
esig
n
a
n
d
s
t
u
d
y
t
h
e
ch
ar
ac
ter
is
tics
o
f
a
m
o
d
if
ied
a
cc
eler
atin
g
s
tr
u
ct
u
r
e
o
f
th
is
t
y
p
e
w
i
th
th
e
i
m
p
r
o
v
ed
f
o
cu
s
i
n
g
p
r
o
p
er
ties
.
T
h
is
i
s
ac
h
iev
ed
b
y
th
e
d
esi
g
n
o
f
th
e
ac
ce
ler
atin
g
ce
lls
w
i
th
o
n
e
d
r
if
t
s
lee
v
e
a
n
d
th
e
d
r
i
f
t
o
p
en
in
g
o
f
co
n
ica
l
s
h
ap
e,
w
h
ic
h
ch
an
g
es
th
e
s
p
atial
co
n
f
i
g
u
r
atio
n
o
f
th
e
H
F
f
ield
s
in
th
e
s
y
s
te
m
an
d
r
esu
lts
i
n
a
ch
an
g
e
o
f
b
o
u
n
d
ar
ies
o
f
t
h
e
co
r
r
esp
o
n
d
in
g
p
h
ase
r
eg
io
n
s
o
f
ac
ce
ler
atio
n
an
d
f
o
cu
s
i
n
g
.
Am
o
d
i
f
ied
B
R
S
is
s
h
o
w
n
i
n
Fi
g
u
r
e
1.
Fig
u
r
e
1
. M
o
d
if
ied
B
R
S
w
ith
a
h
ig
h
ac
ce
ler
atio
n
r
ate
.
I
n
o
u
r
ca
s
e,
w
i
th
o
u
t
a
s
er
io
u
s
d
a
m
ag
e
to
th
e
f
i
n
al
r
es
u
lt,
we
ca
n
n
eg
lec
t
t
h
e
ch
a
n
g
e
i
n
t
h
e
s
h
ap
e
o
f
th
e
d
is
tr
ib
u
tio
n
o
f
t
h
e
az
i
m
u
th
a
l
m
ag
n
etic
a
n
d
lo
n
g
it
u
d
in
al
elec
tr
ic
f
ield
s
,
tak
i
n
g
i
n
to
ac
co
u
n
t
o
n
l
y
a
s
ig
n
i
f
ica
n
t
c
h
a
n
g
e
i
n
t
h
e
r
ad
ial
co
m
p
o
n
e
n
t
o
f
th
e
elec
tr
ic
f
ie
ld
.
T
h
en
f
o
r
t
h
e
elec
tr
o
n
b
ea
m
e
n
ter
i
n
g
t
h
e
ac
ce
ler
atin
g
ce
ll
f
r
o
m
t
h
e
d
ir
ec
tio
n
o
f
t
h
e
d
r
if
t
s
lee
v
e,
t
h
e
r
eg
io
n
o
f
f
o
cu
s
i
n
g
b
y
t
h
e
r
ad
ia
l
elec
tr
ic
f
ie
ld
w
ill
co
in
cid
e
w
it
h
th
e
co
r
r
esp
o
n
d
in
g
r
eg
io
n
o
f
t
h
e
tr
ad
itio
n
al
B
R
S
,
w
h
er
ea
s
t
h
e
r
e
g
io
n
o
f
t
h
e
s
i
m
u
lta
n
eo
u
s
ac
ce
ler
atio
n
an
d
f
o
c
u
s
i
n
g
w
ill
b
e
Mo
r
eo
v
er
,
th
e
f
o
cu
s
i
n
g
zo
n
e
s
d
u
e
to
th
e
u
s
e
of
th
e
r
ad
ial
co
m
p
o
n
e
n
t
of
elec
tr
ic
f
ield
an
d
th
e
az
i
m
u
t
h
al
co
m
p
o
n
e
n
t
of
m
a
g
n
etic
f
ield
o
v
er
lap
in
t
h
e
r
an
g
e
T
h
u
s
,
w
e
ac
h
ie
v
e
a
5
0
%
in
cr
ea
s
e
f
o
r
th
e
s
izes
o
f
t
h
e
r
eg
i
o
n
o
f
th
e
i
n
itia
l
p
h
ase
s
o
f
t
h
e
elec
tr
o
n
f
l
y
in
g
in
,
f
o
r
w
h
ic
h
t
h
e
co
n
d
i
tio
n
s
o
f
s
i
m
u
ltan
eo
u
s
ac
ce
ler
atio
n
a
n
d
f
o
cu
s
i
n
g
ar
e
f
u
l
f
ille
d
,
an
d
,
b
esid
es,th
e
p
h
ase
co
r
r
esp
o
n
d
in
g
to
t
h
e
m
ax
i
m
u
m
ac
ce
ler
atio
n
(
⁄
)
f
all
s
w
it
h
i
n
t
h
e
f
o
c
u
s
i
n
g
r
eg
io
n
.
T
h
is
m
a
k
es
it
p
o
s
s
ib
le
to
i
m
p
le
m
en
t
th
e
m
o
d
e
w
h
ic
h
p
r
o
v
id
esb
o
th
th
e
r
ad
ial
f
o
cu
s
in
g
o
f
th
e
elec
tr
o
n
b
u
n
c
h
es
a
n
d
th
e
ir
o
p
tim
a
l
ac
ce
ler
atio
n
.
Su
c
h
f
a
v
o
r
ab
le
in
all
r
e
s
p
e
cts
m
o
d
e
o
f
t
h
e
i
n
s
tal
latio
n
is
u
n
a
ttai
n
ab
le
w
h
ile
u
s
in
g
B
R
S
w
it
h
t
h
e
co
n
v
en
t
io
n
al
ac
ce
ler
a
tin
g
ce
lls
.
Evaluation Warning : The document was created with Spire.PDF for Python.
I
J
E
C
E
I
SS
N:
2
0
8
8
-
8708
F
o
cu
s
in
g
P
r
o
p
erti
es o
f a
Mo
d
ified
R
eta
r
d
in
g
S
tr
u
ctu
r
e
fo
r
Lin
ea
r
E
lectro
n
…
(
V
la
d
imir
K
u
z
’
mich
S
h
ilo
v
)
745
M
o
r
e
co
m
p
lete
in
f
o
r
m
a
tio
n
o
n
t
h
e
f
o
cu
s
in
g
p
r
o
p
er
ties
o
f
b
o
th
h
i
g
h
f
r
eq
u
en
c
y
s
tr
u
c
tu
r
e
s
co
u
ld
b
e
o
b
tain
ed
b
y
t
h
e
s
o
f
t
w
ar
e
f
o
r
i
n
teg
r
at
in
g
t
h
e
m
o
tio
n
eq
u
a
tio
n
s
o
f
c
h
ar
g
ed
p
ar
ticle
s
i
n
th
e
s
tr
u
ctu
r
e
s
w
o
r
k
i
n
g
i
n
th
e
s
ta
n
d
in
g
w
av
e
m
o
d
e.
T
h
e
HF
f
ie
ld
s
in
ter
ac
ti
n
g
w
it
h
th
e
elec
tr
o
n
s
alo
n
g
th
e
e
n
tire
len
g
t
h
o
f
th
e
ac
ce
ler
ato
r
w
er
e
g
i
v
en
i
n
tab
l
es.
W
e
i
n
v
e
s
ti
g
ated
a
n
ac
ce
ler
atin
g
s
y
s
te
m
co
n
ta
in
i
n
g
1
6
id
en
tical
ac
c
eler
atin
g
ce
lls
,
th
e
lo
n
g
it
u
d
in
al
d
i
m
e
n
s
io
n
o
f
w
h
ic
h
co
r
r
esp
o
n
d
ed
to
th
e
r
elati
v
e
p
h
a
s
e
v
elo
cit
y
e
q
u
al
to
1
,
w
h
ile
t
h
e
in
te
n
s
it
y
o
f
t
h
e
lo
n
g
it
u
d
in
a
l
e
lectr
ic
f
ield
o
n
t
h
e
ax
is
o
f
t
h
e
ac
ce
ler
atin
g
ce
ll
s
w
as
.
T
h
e
p
h
ases
w
er
e
m
ea
s
u
r
ed
in
th
e
s
ca
le
w
h
er
e
1
co
r
r
esp
o
n
d
ed
t
o
.
T
h
e
p
ar
ticles
f
ell
in
to
a
s
tr
u
ct
u
r
e
w
ith
t
h
e
in
itia
l
r
ad
iu
s
o
f
,
w
it
h
th
e
lo
n
g
itu
d
i
n
a
l r
elativ
e
v
elo
cit
y
an
d
th
e
r
ela
tiv
e
r
ad
ial
v
elo
cit
y
.
T
h
e
ca
lcu
latio
n
r
esu
lt
s
in
d
icat
e
th
at
th
e
f
o
c
u
s
i
n
g
e
f
f
ec
t
o
n
th
e
ac
ce
ler
ated
elec
tr
o
n
s
o
f
th
e
m
o
d
i
f
ied
HF
s
tr
u
ct
u
r
e
is
m
u
c
h
m
o
r
e
s
ig
n
i
f
ican
t.
Usi
n
g
t
h
e
co
n
ce
p
t
o
f
ac
ce
p
tan
ce
,
w
e
h
a
v
e
s
u
cc
ee
d
ed
in
ca
r
r
y
i
n
g
o
u
t
a
co
r
r
ec
t
co
m
p
ar
is
o
n
o
f
t
h
e
f
o
c
u
s
i
n
g
p
r
o
p
er
ties
o
f
th
e
co
n
v
e
n
tio
n
al
B
R
S
o
f
t
h
e
co
n
s
id
er
ed
t
y
p
e
a
n
d
t
h
e
B
R
S
w
it
h
a
m
o
d
i
f
ied
p
r
o
f
ile
o
f
ac
c
eler
atin
g
ce
lls
.
T
h
e
ac
ce
p
tan
ce
is
t
h
e
m
a
x
i
m
a
l
p
o
s
s
ib
le
e
m
itta
n
ce
o
f
t
h
e
co
h
er
en
t
b
ea
m
t
h
at
is
ab
le
to
p
a
s
s
t
h
r
o
u
g
h
th
e
s
y
s
te
m
.
T
h
e
h
ig
h
er
th
e
ac
ce
p
tan
ce
,
th
e
h
i
g
h
er
is
t
h
e
ca
r
r
y
i
n
g
ca
p
ac
it
y
o
f
th
e
HF
s
tr
u
ct
u
r
e.
Fig
u
r
e
2
p
r
e
s
en
ts
t
h
e
ac
ce
p
tan
ce
s
f
o
r
v
ar
io
u
s
in
it
ial
p
h
ase
s
o
f
th
e
el
ec
tr
o
n
f
l
y
in
g
in
to
th
e
co
n
s
id
e
r
ed
s
y
s
te
m
s
,
w
h
er
e
b
o
th
s
y
s
te
m
s
h
a
v
e
t
h
e
s
a
m
e
a
p
er
tu
r
es o
f
.
Fig
u
r
e
2
.
A
cc
ep
tan
ce
s
f
o
r
v
ar
i
o
u
s
in
itial
p
h
a
s
es
of
t
h
e
elec
tr
o
n
s
f
l
y
i
n
g
in
to
t
h
e
ac
ce
ler
atin
g
s
y
s
te
m
s
:
a
–
th
e
p
h
ase
0
.
7
,
b
–
th
e
p
h
ase
0
.
8
,
c
–
t
h
e
p
h
ase
0
.
9
;
th
e
d
as
h
ed
lin
e
re
p
r
esen
ts
t
h
e
ac
ce
p
tan
ce
s
o
f
th
e
co
n
v
en
tio
n
al
B
R
S
,
th
e
co
n
ti
n
u
o
u
s
lin
e,
t
h
e
a
cc
ep
tan
ce
s
of
t
h
e
m
o
d
i
f
ied
B
R
S
.
As
s
ee
n
f
r
o
m
Fig
u
r
e
2
,
th
e
d
e
s
cr
ib
ed
c
h
an
g
e
o
f
th
e
f
o
r
m
o
f
ac
ce
ler
atin
g
ce
lls
allo
w
s
i
n
cr
ea
s
in
g
b
y
t
w
o
t
i
m
e
s
a
n
d
m
o
r
e
t
h
e
p
h
as
e
ar
ea
b
o
u
n
d
ed
b
y
t
h
e
ac
ce
p
t
an
ce
s
f
o
r
t
h
e
en
tire
p
h
a
s
e
r
an
g
e
co
r
r
esp
o
n
d
in
g
to
th
e
m
a
x
i
m
u
m
g
ai
n
b
y
t
h
e
p
ar
ticles o
f
t
h
e
o
u
tp
u
t e
n
er
g
y
(
th
e
p
h
ases
0
.
7
-
0
.
9
)
.
T
h
e
m
ai
n
ad
v
a
n
ta
g
e
o
f
t
h
e
s
ta
n
d
in
g
-
w
av
e
L
E
A
w
i
th
B
R
S
is
th
e
p
o
s
s
ib
ilit
y
o
f
a
s
i
g
n
i
f
ica
n
t
r
ed
u
ctio
n
in
th
e
le
n
g
th
o
f
th
e
ac
ce
ler
ati
n
g
s
tr
u
ct
u
r
e
to
y
ield
th
e
n
ec
e
s
s
ar
y
g
ai
n
in
g
o
f
e
n
er
g
y
u
n
d
er
th
e
s
a
m
e
p
o
w
er
o
f
th
e
HF
g
e
n
er
ato
r
.
Ob
v
io
u
s
l
y
,
s
u
ch
a
s
tr
u
ct
u
r
e
s
h
o
u
ld
h
a
v
e,
f
ir
s
t
o
f
all,
a
lar
g
e
v
al
u
e
o
f
ef
f
ec
ti
v
e
s
h
u
n
t
r
esis
ta
n
ce
.
Am
o
n
g
o
t
h
er
elec
t
r
o
d
y
n
a
m
ic
ch
ar
ac
ter
i
s
tics
o
f
B
R
S,
t
h
e
co
n
n
ec
tio
n
co
ef
f
icie
n
t
b
et
w
ee
n
ce
ll
s
,
t
h
e
q
u
alit
y
f
ac
to
r
,
th
e
g
r
o
u
p
v
e
lo
cit
y
,
t
h
e
m
a
x
i
m
u
m
v
al
u
es
o
f
th
e
elec
tr
ic
a
n
d
m
a
g
n
e
tic
f
iel
d
s
o
n
th
e
s
u
r
f
ac
e
o
f
th
e
s
tr
u
ctu
r
e,
t
h
e
elec
tr
ic
f
ie
ld
o
v
er
v
o
ltag
e
f
ac
to
r
ar
e
i
m
p
o
r
tan
t.
A
cc
eler
ato
r
s
w
i
th
a
lar
g
e
co
n
n
ec
tio
n
co
ef
f
icie
n
t
h
av
e
b
etter
s
tab
ilit
y
to
c
h
an
g
e
s
i
n
t
h
e
p
ar
a
m
eter
s
o
f
th
e
ac
ce
ler
ated
b
ea
m
,
less
r
i
g
id
to
ler
an
ce
s
f
o
r
m
a
n
u
f
ac
t
u
r
in
g
th
e
ac
ce
ler
at
i
n
g
s
tr
u
c
tu
r
e
,
b
etter
s
tab
ilit
y
o
f
o
p
er
atio
n
o
f
th
e
HF
g
en
er
ato
r
.
I
n
[
1
1
]
,
th
er
e
ar
e
p
r
esen
ted
th
e
r
esu
lts
o
f
s
t
u
d
ies
o
n
o
p
ti
m
izin
g
th
e
g
eo
m
etr
y
o
f
B
R
S
w
ith
i
n
ter
n
a
l
co
n
n
ec
t
io
n
ce
lls
w
it
h
r
esp
ec
t
to
in
cr
ea
s
in
g
th
e
co
u
p
li
n
g
co
ef
f
icie
n
t
to
1
5
%
u
n
d
er
an
in
s
i
g
n
i
f
ican
t c
h
a
n
g
e
i
n
t
h
e
li
n
e
ef
f
ec
t
iv
e
s
h
u
n
t r
esis
tan
ce
a
n
d
o
th
er
elec
tr
o
d
y
n
a
m
ic
c
h
ar
ac
ter
is
tics
.
T
h
e
r
esu
lt
s
in
d
icate
th
e
p
r
o
m
i
s
i
n
g
c
h
ar
ac
t
er
o
f
th
e
r
esear
ch
i
n
th
is
d
ir
ec
t
io
n
[
1
2
-
1
4
]
.
T
h
u
s
,
th
e
p
r
o
p
o
s
ed
m
o
d
i
f
ica
tio
n
of
t
h
e
s
h
ap
e
of
th
e
B
R
S
ac
ce
ler
ati
n
g
ce
ll
s
h
a
s
a
n
u
m
b
er
of
in
d
is
p
u
tab
le
ad
v
an
ta
g
es
an
d
allo
w
s
s
ig
n
i
f
ica
n
tl
y
in
cr
ea
s
in
g
th
e
ef
f
icie
n
c
y
of
th
e
s
y
s
te
m
in
s
u
c
h
p
r
o
m
i
s
i
n
g
m
o
d
e
as
f
o
cu
s
i
n
g
o
f
th
e
ac
ce
l
er
ated
be
am
b
y
t
h
e
o
w
n
HF
f
i
eld
s
o
f
th
e
ac
ce
ler
ati
n
g
s
tr
u
c
tu
r
e
.
4.
CO
NCLU
SI
O
N
I
n
co
n
cl
u
s
io
n
,
w
e
w
o
u
l
d
li
k
e
t
o
m
en
tio
n
t
h
e
f
ac
t
t
h
at
th
e
ca
l
cu
latio
n
r
es
u
lts
h
a
v
e
f
u
ll
y
co
n
f
ir
m
ed
t
h
e
co
n
clu
s
io
n
s
o
b
tain
ed
u
s
i
n
g
a
s
i
m
p
li
f
ied
m
at
h
e
m
atica
l
m
o
d
el
o
f
th
e
ac
ce
ler
ati
n
g
ce
ll
a
n
d
p
r
o
v
id
e
a
clea
r
p
ictu
r
e
o
f
t
h
e
p
r
o
ce
s
s
es.
T
h
er
ef
o
r
e,
in
t
h
e
f
u
tu
r
e
t
h
e
a
u
th
o
r
s
p
lan
to
u
s
e
it
f
o
r
th
e
co
n
ti
n
u
o
u
s
d
eter
m
in
a
tio
n
o
f
th
e
f
o
c
u
s
i
n
g
p
r
o
p
er
ties
o
f
v
ar
io
u
s
HF s
tr
u
ct
u
r
es
w
o
r
k
i
n
g
in
t
h
e
s
ta
n
d
in
g
w
a
v
e
m
o
d
e.
Evaluation Warning : The document was created with Spire.PDF for Python.
I
SS
N
:
2088
-
8708
I
J
E
C
E
Vo
l.
7
,
No
.
2
,
A
p
r
il 2
0
1
7
:
7
4
1
–
747
746
T
h
e
p
r
o
p
o
s
ed
m
et
h
o
d
o
f
g
u
i
d
in
g
th
e
elec
tr
o
n
b
ea
m
i
n
li
n
ea
r
ac
ce
ler
ato
r
s
i
s
b
ased
o
n
u
s
in
g
th
e
f
o
cu
s
in
g
p
r
o
p
er
ties
o
f
th
e
r
ad
i
al
co
m
p
o
n
e
n
t
o
f
th
e
elec
tr
ic
f
i
eld
.
T
h
is
co
m
p
o
n
e
n
t
ap
p
ea
r
s
ev
en
f
o
r
th
e
lo
w
es
t
t
y
p
e
o
f
o
s
c
illatio
n
i
n
t
h
e
co
n
v
en
t
io
n
al
c
y
li
n
d
r
ical
ac
ce
ler
at
in
g
ca
v
ities
in
th
e
r
eg
io
n
o
f
t
h
e
d
r
if
t
tu
b
e
s
an
d
,
th
er
ef
o
r
e,
i
n
t
h
e
v
ic
in
i
t
y
o
f
th
e
d
r
if
t
ch
a
n
n
el
a
x
is
.
T
h
i
s
ef
f
ec
t,
a
r
i
s
in
g
d
u
e
to
th
e
cu
r
v
at
u
r
e
o
f
th
e
elec
tr
o
m
ag
n
etic
f
ield
li
n
es,
m
i
g
h
t b
e
p
r
o
m
is
i
n
g
also
f
o
r
t
h
e
p
r
o
to
n
an
d
io
n
lin
ea
r
ac
ce
ler
ato
r
s
.
T
h
e
s
t
u
d
ies
co
n
d
u
c
ted
w
i
th
t
h
e
h
elp
o
f
m
at
h
e
m
atica
l
m
o
d
el
in
g
h
a
v
e
s
h
o
w
n
t
h
e
p
r
o
m
is
i
n
g
n
atu
r
e
o
f
th
is
m
et
h
o
d
in
th
e
d
esi
g
n
a
n
d
co
n
s
tr
u
ct
io
n
o
f
th
e
L
E
A
w
i
th
o
u
t
t
h
e
u
s
e
o
f
ex
ter
n
al
f
o
c
u
s
i
n
g
d
ev
ices.
T
h
i
s
w
il
l
allo
w
g
r
ea
tl
y
r
ed
u
ci
n
g
th
e
d
i
m
en
s
io
n
s
a
n
d
w
eig
h
t
o
f
t
h
e
ac
ce
ler
ato
r
its
elf
a
n
d
en
h
a
n
ci
n
g
its
e
f
f
ec
ti
v
en
e
s
s
w
h
ile
u
s
i
n
g
in
t
h
e
tec
h
n
o
lo
g
ic
al
f
ield
s
o
f
i
n
d
u
s
tr
y
a
n
d
m
ed
ic
in
e.
I
n
th
e
f
u
tu
r
e,
w
e
p
lan
to
s
tu
d
y
th
e
i
m
p
ac
t
of
c
h
an
g
es
in
th
e
s
h
ap
e
th
e
B
R
S
ac
ce
ler
ati
n
g
ca
v
itie
s
o
n
th
e
d
is
tr
ib
u
tio
n
o
f
th
e
e
lectr
o
m
ag
n
etic
f
ie
ld
co
m
p
o
n
en
ts
i
n
th
e
r
eg
io
n
o
f
d
r
i
f
t
ch
a
n
n
el
a
n
d
o
n
th
e
co
n
d
itio
n
s
of
ef
f
ec
ti
v
e
ac
ce
ler
atio
n
a
n
d
r
ad
ial
s
tab
ilit
y
.
ACK
NO
WL
E
D
G
E
M
E
NT
S
T
h
is
w
o
r
k
w
as
s
u
p
p
o
r
ted
b
y
ME
P
h
I
A
ca
d
e
m
ic
E
x
ce
lle
n
c
e
P
r
o
j
ec
t
(
c
o
n
tr
ac
t
No
.
0
2
.
a0
3
.
2
1
.
0
0
0
5
,
2
7
.
0
8
.
2
0
1
3
)
.
RE
F
E
R
E
NC
E
S
[1
]
K.
Be
lo
v
in
tze
v
,
e
t
a
l.
,
“
Izl
u
c
h
a
t
e
l'
n
y
y
k
o
mp
lek
s
d
lya
f
u
n
d
a
me
n
t
a
l
'
n
y
k
h
i
p
rik
la
d
n
y
k
h
issle
d
o
v
a
n
iy,
”
[
Ra
d
iati
o
n
Co
m
p
lex
f
o
r
F
u
n
d
a
m
e
n
tal
a
n
d
A
p
p
li
e
d
Re
se
a
rc
h
]
.
In
T
ru
d
y
1
4
so
v
e
sh
c
h
a
n
iy
a
p
o
u
sk
o
rit
e
ly
a
m
z
a
r
y
a
z
h
e
n
n
y
k
h
c
h
a
stit
s,
P
ro
tv
i
n
o
[
1
4
th
c
o
n
f
e
re
n
c
e
o
n
c
h
a
rg
e
d
p
a
rti
c
les
'
a
c
c
e
l
e
ra
to
rs,
P
ro
tv
in
o
]
,
Vo
l.
4
,
p
p
.
2
6
4
-
2
6
8
,
1
9
9
4
.
[2
]
A
.
N.
F
il
a
to
v
&
V
.
K.
S
h
il
o
v
,
“
C
o
n
tro
l
o
f
ra
d
io
-
f
re
q
u
e
n
c
y
c
h
a
ra
c
ter
isti
c
s
o
f
li
n
e
a
r
e
lec
tro
n
a
c
c
e
lera
to
r”
.
In
stru
me
n
t
s
a
n
d
Exp
e
rime
n
t
a
l
T
e
c
h
n
iq
u
e
s Ne
w
Y
o
rk
,
2
8
(
6
p
t
1
),
1
2
5
8
-
1
2
6
1
,
1
9
8
5
.
[3
]
A
.
E.
No
v
o
z
h
il
o
v
,
e
t
a
l.
,
“
Ca
lcu
latio
n
o
f
Re
so
n
a
n
t
F
re
q
u
e
n
c
ies
a
n
d
El
e
c
tro
m
a
g
n
e
ti
c
F
ield
s
in
Re
so
n
a
t
o
rs
o
f
L
in
e
a
r
A
c
c
e
lera
to
rs
f
o
r
Co
m
m
e
r
c
ial
A
p
p
li
c
a
ti
o
n
,
M
e
d
icin
e
a
n
d
En
v
iro
n
m
e
n
tal
P
r
o
tec
ti
o
n
,
”
Res
e
a
rc
h
J
o
u
rn
a
l
o
f
Ph
a
rm
a
c
e
u
t
ica
l,
Bi
o
l
o
g
ica
l
a
n
d
Ch
e
mic
a
l
S
c
ien
c
e
s,
7(
2
),
8
9
7
-
9
0
5
,
2
0
1
6
.
[4
]
V
.
A
.
V
a
g
u
in
e
,
“
S
tan
d
in
g
W
a
v
e
Hig
h
G
r
a
d
ien
t
A
c
c
e
lera
to
r
S
tru
c
tu
re
”
,
IEE
E
T
ra
n
s
a
c
ti
o
n
s
o
n
N
u
c
lea
r
S
c
ien
c
e
,
24
(
3
),
1
0
8
4
-
1
0
8
6
,
1
9
7
7
.
[5
]
A
.
E.
No
v
o
z
h
il
o
v
,
e
t
a
l.
,
“
Distrib
u
ti
o
n
o
f
A
c
c
e
lera
ti
n
g
V
o
lt
a
g
e
in
Re
so
n
a
to
r
o
f
L
in
e
a
r
El
e
c
tro
n
-
P
o
s
it
ro
n
Co
l
li
d
e
r”
,
In
ter
n
a
t
io
n
a
l
J
o
u
rn
a
l
o
f
A
p
p
li
e
d
En
g
i
n
e
e
rin
g
Res
e
a
rc
h
,
11
(3
)
,
1
5
9
6
-
1
6
0
2
,
2
0
1
6
.
[6
]
M.
V
y
g
o
d
sk
i
y
,
“
S
p
ra
v
o
c
h
n
ik
p
o
v
y
ss
h
e
y
m
a
te
m
a
ti
k
e
”
[
Ha
n
d
b
o
o
k
o
n
Hig
h
e
r
M
a
th
e
m
a
ti
c
s]
.
M
o
sc
o
w
:
A
S
T
,
A
stre
l
'
,
2
0
0
6
.
[7
]
Ya
.
F
a
in
b
e
rg
,
“
O
v
o
z
m
o
z
h
n
o
sti
o
d
n
o
v
re
m
e
n
n
o
y
ra
d
ial'
n
o
y
i
f
a
z
o
v
o
y
u
sto
y
c
h
iv
o
sti
v
li
n
e
y
n
y
k
h
u
sk
o
rit
e
ly
a
k
h
b
e
z
sp
e
tsial'
n
y
k
h
f
o
k
u
siru
y
u
sh
c
h
ik
h
u
stro
y
stv
,
”
[
On
th
e
P
o
ss
i
b
il
it
y
o
f
S
im
u
lt
a
n
e
o
u
s
Ra
d
ial
a
n
d
P
h
a
se
S
t
a
b
il
it
y
in
L
in
e
a
r
A
c
c
e
lera
to
rs
w
it
h
o
u
t
S
p
e
c
ial
F
o
c
u
sin
g
De
v
ice
s]
.
In
T
e
o
riy
a
i
ra
sc
h
e
t
li
n
e
y
n
y
k
h
u
sk
o
ritele
y
[
T
h
e
o
ry
a
n
d
c
a
lcu
latio
n
o
f
li
n
e
a
r
a
c
c
e
lera
to
rs]
.
M
o
sc
o
w
:
G
o
sa
to
m
izd
a
t,
1
9
6
2
.
[8
]
A
.
E.
No
v
o
z
h
il
o
v
,
e
t
a
l.
,
“
P
ro
b
lem
s
o
f
m
e
a
su
re
m
e
n
t
o
f
h
ig
h
-
f
re
q
u
e
n
c
y
f
ield
s
in
li
n
e
a
r
e
lec
tro
n
a
c
c
e
lera
to
rs”
,
Glo
b
a
l
J
o
u
rn
a
l
o
f
P
u
re
a
n
d
A
p
p
l
ied
M
a
t
h
e
ma
ti
c
s
,
1
2
(1
)
,
6
4
3
-
6
5
5
,
2
0
1
6
.
[9
]
L
.
L
a
n
d
a
u
&
E.
L
if
sh
it
z
,
“
T
e
o
re
ti
c
h
e
sk
a
y
a
f
i
z
ik
a
:
T
o
m
2
.
T
e
o
riy
a
p
o
ly
a
”
[
T
h
e
o
re
ti
c
a
l
P
h
y
sic
s:
Vo
l.
2
.
F
iel
d
T
h
e
o
r
y
]
.
M
o
sc
o
w
:
S
c
ien
c
e
.
1
9
8
8
.
[1
0
]
A
.
N.
F
il
a
to
v
&
V
.
K.
S
h
i
lo
v
,
“
R
F
F
o
c
u
sin
g
in
th
e
S
tan
d
in
g
-
W
a
v
e
El
e
c
tro
n
L
in
a
c
s
”
,
S
o
v
iet
p
h
y
sic
s.
T
e
c
h
n
ica
l
p
h
y
sic
s,
2
9
(
2
),
1
6
3
-
1
6
7
,
1
9
8
4
.
[1
1
]
E.
A
.
S
a
v
in
,
N.P
.
S
o
b
e
n
i
n
,
“
Bip
e
rio
d
ic
a
c
c
e
lera
ti
n
g
stru
c
tu
re
w
i
th
in
tern
a
l
c
o
n
n
e
c
ti
o
n
c
e
ll
s
w
it
h
a
n
in
c
re
a
se
d
c
o
n
n
e
c
ti
o
n
c
o
e
f
f
icie
n
t”,
J
o
u
rn
a
l
o
f
T
e
c
h
n
ica
l
Ph
y
sic
s
,
8
3
(5
)
,
1
4
1
-
1
4
6
,
2
0
1
3
.
[1
2
]
N.N.N.
A
.
M
a
li
k
,
M
.
Esa
,
S
.
K.S
.
Yu
so
f
,
N.M
.
A
.
L
a
ti
ff
“
In
telli
g
e
n
t
L
in
e
a
r
Co
ll
a
b
o
ra
ti
v
e
Be
a
m
f
o
r
m
in
g
f
o
r
M
u
lt
i
-
o
b
jec
ti
v
e
Ra
d
iatio
n
Be
a
m
p
a
tt
e
rn
in
W
irele
s
s
S
e
n
so
r
Ne
t
w
o
rk
s
”
T
EL
KOM
NIKA
In
d
o
n
e
sia
n
J
o
u
r
n
a
l
o
f
El
e
c
trica
l
En
g
i
n
e
e
rin
g
,
1
2
(1
0
),
7
3
1
8
-
7
3
2
9
,
2
0
1
4
.
[1
3
]
S
u
li
m
a
n
A
b
d
e
l
Ra
h
m
a
n
A
b
d
a
ll
a
“
A
Re
a
l
-
T
i
m
e
I
m
p
le
m
e
n
tatio
n
o
f
M
o
v
in
g
Ob
jec
t
A
c
ti
o
n
Re
c
o
g
n
it
io
n
S
y
ste
m
Ba
se
d
o
n
M
o
ti
o
n
A
n
a
l
y
sis”
In
d
o
n
e
sia
n
J
o
u
rn
a
l
o
f
E
lec
trica
l
En
g
i
n
e
e
rin
g
a
n
d
In
fo
rm
a
t
ics
,
5
(
1
0
),
2
0
1
7
.
[1
4
]
S
o
b
h
a
n
Do
ra
h
a
k
i
,
“
Ev
a
lu
a
ti
n
g
th
e
Ra
d
iatio
n
a
n
d
T
e
m
p
e
ra
tu
re
Eff
e
c
t
o
n
P
h
o
to
v
o
lt
a
ic
S
y
ste
m
s”
,
Bu
ll
e
ti
n
o
f
El
e
c
trica
l
En
g
in
e
e
rin
g
a
n
d
In
f
o
r
ma
ti
c
s
,
4
(
1
),
1
-
6
,
2
0
1
5
.
Evaluation Warning : The document was created with Spire.PDF for Python.
I
J
E
C
E
I
SS
N:
2
0
8
8
-
8708
F
o
cu
s
in
g
P
r
o
p
erti
es o
f a
Mo
d
ified
R
eta
r
d
in
g
S
tr
u
ctu
r
e
fo
r
Lin
ea
r
E
lectro
n
…
(
V
la
d
imir
K
u
z
’
mich
S
h
ilo
v
)
747
B
I
O
G
RAP
H
I
E
S
O
F
AUTH
O
RS
A.N.
Fi
la
to
v
&
V
.
K
.
S
h
il
o
v
,
“
RF
F
o
c
u
si
n
g
in
th
e
S
ta
n
d
i
n
g
-
Wav
e
El
e
c
tro
n
L
in
a
c
s,”
S
o
v
iet
p
h
y
sic
s.
T
e
c
h
n
ica
l
p
h
y
sic
s,2
9
(2
),
1
6
3
-
1
6
7
,
1
9
8
4
A
.
N.
F
il
a
to
v
&
V
.
K.
S
h
il
o
v
,
CON
T
RO
L
OF
R
A
DIO
-
F
REQUEN
CY
CHA
R
ACT
ERIS
T
ICS
OF
L
INE
A
R
E
L
ECT
R
ON
A
CCE
L
ERAT
OR.
In
stru
m
e
n
ts
a
n
d
e
x
p
e
rime
n
tal
tec
h
n
iq
u
e
s
Ne
w
Yo
rk
,
V
o
l
u
m
e
2
8
,
Iss
u
e
6
p
t
1
,
No
v
e
m
b
e
r
1
9
8
5
,
P
a
g
e
s 1
2
5
8
-
1
2
6
1
P
r
o
b
lem
s
o
f
Be
a
m
F
o
c
u
sin
g
b
y
El
e
c
tro
m
a
g
n
e
ti
c
F
ield
in
L
in
e
a
r
El
e
c
tro
n
A
c
c
e
l
e
ra
to
r
w
it
h
S
tan
d
i
n
g
W
a
v
e
,
Ba
s
e
d
o
n
B
i
p
e
rio
d
ic
S
tru
c
t
u
re
No
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.M
o
d
e
r
n
A
p
p
li
e
d
S
c
ien
c
e
;
Vo
l.
9
,
N
o
.
4
;
2
0
1
5
:
1
6
0
-
1
6
9
IS
S
N
1
9
1
3
-
1
8
4
4
E
-
IS
S
N
1
9
1
3
-
1
8
5
2
P
u
b
-
li
sh
e
d
b
y
Ca
n
a
d
ian
Ce
n
ter o
f
S
c
ien
c
e
a
n
d
Ed
u
c
a
ti
o
n
DO
I:1
0
.
5
5
3
9
/m
a
s.v
9
n
4
p
1
6
0
L
in
e
a
r
El
e
c
tro
n
Ac
c
e
ler
a
to
rs
A
i
m
e
d
a
t
En
v
iro
n
m
e
n
tal
P
ro
tec
ti
o
n
N
o
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.
Bio
sc
ien
c
e
s Bio
tec
h
n
o
l
o
g
y
Re
se
a
rc
h
A
sia
,
S
e
p
te
m
b
e
r
2
0
1
5
.
Vo
l.
1
2
(S
p
l.
E
d
n
.
2
),
p
.
261
-
2
6
8
DO
I:
h
tt
p
:/
/
d
x
.
d
o
i.
o
rg
/1
0
.
1
3
0
5
0
/
b
b
ra
/
2
1
9
9
Co
m
p
a
c
t
A
c
c
e
l
e
ra
ti
n
g
S
y
st
e
m
f
o
r
a
M
u
lt
ich
a
n
n
e
l
El
e
c
tr
o
n
L
in
e
a
r
A
c
c
e
lera
to
r
No
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.
Re
se
a
rc
h
Jo
u
rn
a
l
o
f
P
h
a
rm
a
c
e
u
ti
c
a
l,
Bio
lo
g
ica
l
a
n
d
Ch
e
m
ic
a
l
S
c
ien
c
e
s (IS
S
N0
9
7
5
8
5
8
5
-
I
n
d
ia
-
S
c
o
p
u
s) J
u
ly
–
A
u
g
u
st 2
0
1
6
RJ
P
B
CS
7
(
5
)
P
a
g
e
No
.
9
3
9
-
9
4
4
A.N.
Fi
la
to
v
&
V
.
K
.
S
h
il
o
v
,
“
RF
F
o
c
u
si
n
g
in
th
e
S
ta
n
d
i
n
g
-
Wav
e
El
e
c
tro
n
L
in
a
c
s,”
S
o
v
iet
p
h
y
sic
s.
T
e
c
h
n
ica
l
p
h
y
sic
s,2
9
(2
),
1
6
3
-
1
6
7
,
1
9
8
4
A
.
N.
F
il
a
to
v
&
V
.
K.
S
h
il
o
v
,
CON
T
RO
L
OF
R
A
DIO
-
F
REQUEN
CY
CHA
R
ACT
ERIS
T
ICS
OF
L
INE
A
R
E
L
ECT
R
ON
A
CCE
L
ERAT
OR.
In
stru
m
e
n
ts
a
n
d
e
x
p
e
rime
n
tal
tec
h
n
iq
u
e
s
Ne
w
Yo
rk
,
V
o
l
u
m
e
2
8
,
Iss
u
e
6
p
t
1
,
No
v
e
m
b
e
r
1
9
8
5
,
P
a
g
e
s 1
2
5
8
-
1
2
6
1
P
r
o
b
lem
s
o
f
Be
a
m
F
o
c
u
sin
g
b
y
El
e
c
tro
m
a
g
n
e
ti
c
F
ield
in
L
in
e
a
r
El
e
c
tro
n
A
c
c
e
lera
to
r
w
it
h
S
tan
d
i
n
g
W
a
v
e
,
Ba
s
e
d
o
n
B
i
p
e
rio
d
ic
S
tru
c
t
u
re
No
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.M
o
d
e
r
n
A
p
p
li
e
d
S
c
ien
c
e
;
Vo
l.
9
,
N
o
.
4
;
2
0
1
5
:
1
6
0
-
1
6
9
IS
S
N
1
9
1
3
-
1
8
4
4
E
-
IS
S
N
1
9
1
3
-
1
8
5
2
P
u
b
-
li
sh
e
d
b
y
Ca
n
a
d
ian
Ce
n
ter o
f
S
c
ien
c
e
a
n
d
Ed
u
c
a
ti
o
n
DO
I:1
0
.
5
5
3
9
/m
a
s.v
9
n
4
p
1
6
0
L
in
e
a
r
El
e
c
tro
n
Ac
c
e
ler
a
to
rs
A
i
m
e
d
a
t
En
v
iro
n
m
e
n
tal
P
ro
tec
ti
o
n
N
o
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.
Bio
sc
ien
c
e
s Bio
tec
h
n
o
l
o
g
y
Re
se
a
rc
h
A
sia
,
S
e
p
te
m
b
e
r
2
0
1
5
.
Vo
l.
1
2
(S
p
l.
E
d
n
.
2
),
p
.
261
-
2
6
8
DO
I:
h
tt
p
:/
/
d
x
.
d
o
i.
o
rg
/1
0
.
1
3
0
5
0
/
b
b
ra
/
2
1
9
9
Co
m
p
a
c
t
A
c
c
e
l
e
ra
ti
n
g
S
y
st
e
m
f
o
r
a
M
u
lt
ich
a
n
n
e
l
El
e
c
tr
o
n
L
in
e
a
r
A
c
c
e
lera
to
r
No
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.
Re
se
a
rc
h
Jo
u
rn
a
l
o
f
P
h
a
rm
a
c
e
u
ti
c
a
l,
Bio
lo
g
ica
l
a
n
d
Ch
e
m
ic
a
l
S
c
ien
c
e
s (IS
S
N0
9
7
5
8
5
8
5
-
I
n
d
ia
-
S
c
o
p
u
s) J
u
ly
–
A
u
g
u
st 2
0
1
6
RJ
P
B
CS
7
(
5
)
P
a
g
e
No
.
9
3
9
-
9
4
4
P
r
o
b
lem
s
o
f
Be
a
m
F
o
c
u
sin
g
b
y
El
e
c
tro
m
a
g
n
e
ti
c
F
ield
in
L
in
e
a
r
El
e
c
tro
n
A
c
c
e
lera
t
o
r
w
it
h
S
tan
d
i
n
g
W
a
v
e
,
Ba
s
e
d
o
n
B
i
p
e
rio
d
ic
S
tru
c
t
u
re
No
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.M
o
d
e
r
n
A
p
p
li
e
d
S
c
ien
c
e
;
Vo
l.
9
,
N
o
.
4
;
2
0
1
5
:
1
6
0
-
1
6
9
IS
S
N
1
9
1
3
-
1
8
4
4
E
-
IS
S
N
1
9
1
3
-
1
8
5
2
P
u
b
li
sh
e
d
b
y
Ca
n
a
d
ian
Ce
n
t
e
r
o
f
S
c
ien
c
e
a
n
d
Ed
u
c
a
ti
o
n
DO
I:
1
0
.
5
5
3
9
/m
a
s.v
9
n
4
p
1
6
0
L
in
e
a
r
El
e
c
tro
n
Ac
c
e
ler
a
to
rs
A
i
m
e
d
a
t
En
v
iro
n
m
e
n
tal
P
ro
tec
ti
o
n
N
o
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.
Bio
sc
ien
c
e
s Bio
tec
h
n
o
l
o
g
y
Re
se
a
rc
h
A
sia
,
S
e
p
te
m
b
e
r
2
0
1
5
.
Vo
l.
1
2
(S
p
l.
E
d
n
.
2
),
p
.
261
-
2
6
8
DO
I:
h
tt
p
:/
/
d
x
.
d
o
i.
o
rg
/1
0
.
1
3
0
5
0
/
b
b
ra
/
2
1
9
9
Co
m
p
a
c
t
A
c
c
e
l
e
ra
ti
n
g
S
y
st
e
m
f
o
r
a
M
u
lt
ich
a
n
n
e
l
El
e
c
tr
o
n
L
in
e
a
r
A
c
c
e
lera
to
r
No
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.
Re
se
a
rc
h
Jo
u
rn
a
l
o
f
P
h
a
rm
a
c
e
u
ti
c
a
l,
Bio
lo
g
ica
l
a
n
d
Ch
e
m
ic
a
l
S
c
ien
c
e
s (IS
S
N0
9
7
5
8
5
8
5
-
I
n
d
ia
-
S
c
o
p
u
s) J
u
ly
–
A
u
g
u
st 2
0
1
6
RJ
P
B
CS
7
(
5
)
P
a
g
e
No
.
9
3
9
-
9
4
4
Clo
se
d
M
a
g
n
e
ti
c
T
ra
p
f
o
r
Co
n
f
in
in
g
a
n
d
He
a
ti
n
g
P
las
m
a
No
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.Bi
o
sc
ien
c
e
s Bio
tec
h
n
o
l
o
g
y
Re
se
a
rc
h
A
sia
,
A
p
ril
2
0
1
5
,
V
o
l
.
1
2
(1
),
6
4
7
-
6
5
1
DO
I:
h
tt
p
:/
/d
x
.
d
o
i
.
o
rg
/1
0
.
1
3
0
0
5
/b
b
ra
/1
7
0
8
Ca
lcu
latio
n
o
f
Re
so
n
a
n
t
F
re
q
u
e
n
c
ies
a
n
d
El
e
c
tro
m
a
g
n
e
ti
c
F
ield
s
in
Re
so
n
a
to
rs
o
f
L
in
e
a
r
A
c
-
c
e
lera
to
rs
f
o
r
Co
m
m
e
rc
ial
A
p
p
li
c
a
ti
o
n
,
M
e
d
ici
n
e
a
n
d
E
n
v
iro
n
m
e
n
tal
P
r
o
tec
ti
o
n
No
v
o
z
h
il
o
v
A
.
E.
,
F
il
a
to
v
A
.
N.,
S
h
il
o
v
V
.
K.
Re
se
a
rc
h
Jo
u
rn
a
l
o
f
P
h
a
rm
a
c
e
u
ti
c
a
l,
Bio
lo
g
ica
l
a
n
d
Ch
e
m
ica
l
S
c
ien
c
e
s M
a
rc
h
–
A
p
ril
2
0
1
6
RJ
P
BCS
7
(2
),
p
p
8
9
7
-
9
0
5
Evaluation Warning : The document was created with Spire.PDF for Python.