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( y
,
z ) are piecewise-analytical. An infinite homogeneous basement of conductiv-
ity
const occurs at a depth D . The model is excited by the plane E -polarized
electromagnetic wave incident vertically on the Earth's surface z
D =
0.
The Dmitriev theorem states that the piecewise-analytical distribution of conduc-
tivity
=
N ( z )
M
S
( M )
=
N ( z )
+
( y
,
z )
M
S
is uniquely determined by exact values of the tipper
H z ( y
,
z
=
0)
W zy ( y )
=
0) ,
−∞
< y <
,
0
<
,
H y ( y
,
z
=
given on the Earth's surface z
=
0 at all points of the y -axis from
−∞
to
in the
entire range of frequencies
.
The uniqueness theorem is proven in two stages. First we derive the asymptotics
of the tipper W zy ( y ) at a great distance from the inhomogeneity S and show that
it determines the normal conductivity
from 0 to
N ( z ). Then, with the known conductivity
N ( z ), we prove that the tipper uniquely determines the longitudinal impedance of
the inhomogeneous medium.
The anomalous magnetic field H A on the Earth's surface can be represented as a
field produced in a horizontally homogeneous layered medium by excess current of
density j x distributed in the domain S. Normalizing H A , we write:
H y ( y
,
z
=
0)
H A
o y ( y )
=
=
j x ( M o ) h y ( y
,
M o ) dS
H y ( z
=
0)
S
(10
.
35)
H z
( y
,
z
=
0)
H A
o z ( y )
=
=
j x ( M o ) h z ( y
,
M o ) dS
,
H y ( z
=
0)
S
where h y ( y
M o ) are magnetic fields produced at the surface of a hori-
zontally homogeneous medium by an infinitely long linear current of the unit den-
sity flowing at the point M o ( y o ,
,
M o )
,
h z ( y
,
z o )
S in the x -direction. The functions h y ( y
,
M o )
and h z ( y
,
M o ) assume the form (Dmitriev, 1969; Berdichevsky and Zhdanov, 1984)
i
o
y o ) e λ z U (
h y ( y
,
M o )
=
lim
z
cos
λ
( y
λ,
z
=
0
,
z o )
λ
d
λ
0
0
(10
.
36)
i
o
y o ) e λ z U (
h z ( y
,
M o )
=−
lim
z 0
sin
λ
( y
λ,
z
=
0
,
z o )
λ
d
λ,
0
where the factor e λ z relates to the upper half-space z
λ,
,
0 and the function U (
z
z o )
is the solution of the boundary problem
 
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