Mantle seismic tomography beneath East-European Platform
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Інститут геофізики ім. С.I. Субботіна НАН України
2010
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Цитувати: | Mantle seismic tomography beneath East-European Platform / T. Tsvetkova // Геофизический журнал. — 2010. — Т. 32, № 4. — С. 186-188. — Бібліогр.: 1 назв. — англ. |
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irk-123456789-1031052016-06-14T03:04:20Z Mantle seismic tomography beneath East-European Platform Tsvetkova, T. 2010 Article Mantle seismic tomography beneath East-European Platform / T. Tsvetkova // Геофизический журнал. — 2010. — Т. 32, № 4. — С. 186-188. — Бібліогр.: 1 назв. — англ. 0203-3100 http://dspace.nbuv.gov.ua/handle/123456789/103105 en Геофизический журнал Інститут геофізики ім. С.I. Субботіна НАН України |
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Digital Library of Periodicals of National Academy of Sciences of Ukraine |
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DSpace DC |
language |
English |
format |
Article |
author |
Tsvetkova, T. |
spellingShingle |
Tsvetkova, T. Mantle seismic tomography beneath East-European Platform Геофизический журнал |
author_facet |
Tsvetkova, T. |
author_sort |
Tsvetkova, T. |
title |
Mantle seismic tomography beneath East-European Platform |
title_short |
Mantle seismic tomography beneath East-European Platform |
title_full |
Mantle seismic tomography beneath East-European Platform |
title_fullStr |
Mantle seismic tomography beneath East-European Platform |
title_full_unstemmed |
Mantle seismic tomography beneath East-European Platform |
title_sort |
mantle seismic tomography beneath east-european platform |
publisher |
Інститут геофізики ім. С.I. Субботіна НАН України |
publishDate |
2010 |
url |
http://dspace.nbuv.gov.ua/handle/123456789/103105 |
citation_txt |
Mantle seismic tomography beneath East-European Platform / T. Tsvetkova // Геофизический журнал. — 2010. — Т. 32, № 4. — С. 186-188. — Бібліогр.: 1 назв. — англ. |
series |
Геофизический журнал |
work_keys_str_mv |
AT tsvetkovat mantleseismictomographybeneatheasteuropeanplatform |
first_indexed |
2025-07-07T13:17:43Z |
last_indexed |
2025-07-07T13:17:43Z |
_version_ |
1836994279720878080 |
fulltext |
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Mantle seismic tomography beneath East-European Platform
T. Tsvetkova, 2010
Institute of Geophysics, National Academy of Sciences of Ukraine, Kiev, Ukraine
tsvet@igph.kiev.ua
3D P-velocity model of the mantle under East-
European platform was received as the solution of
the seismic tomography problem by Taylor approxi-
mation method, which was supposed by V. S. Gey-
ko [Geyko, 2004]. The solution don’t depend from
the referent model selection and can be imagine in
Cartesian and spherical coordinate system. The used
tomography method permits recovering the mantle
model being optimal in the given metric in respect with
the whole totality of P-wave first arrival traveltime data
within the frame of selected basic model of interpreta-
tion. It includes the apriory assumptions? Theory and
algorithms of numerical inversion, parameterization of
velocity function, the smoothing method and other regu-
larizing factors. The results are imagine in horizontal,
longitude and latitude sections of the model. The gen-
eralized velocity-depth caracteristics Vaver(z) were used
in definitions high and low velocities and residual of
velocities
zVV
S
,,sup
,
max , (1)
zVV
S
,,inf
,
min , (2)
1
0
,,
)(
z
S
aver V
ddd
zzV , (3)
where S( ) is the domain into horizontal section at
the depth , and is its space in the coordinates
, .
The first time arrival from the ISC from 1964 to
2005 year were used as the input data.
The 3D P-velocity model analysis shows the next
properties:
1) common velocities characteristic for received
mantle model under EEP is layer velocities struc-
ture, which defined by inverse changing of phone
velocity for each layer: high velocity tomographic
lithosphere layer( upper mantle velocity characte-
ristic), low velocity Golitsin — Geyko layer (transi-
tion zone velocity characteristic), high velocity zone
of division-1? low velocity middle mantle, high ve-
locities zone of division-2, low velocities low mantle,
Mantle under EEP surrounding, except eastern part,
characterized by common inverse relate to mantle
velocities characteristics under EEP;
2) by velocities characteristics tomographic litho-
sphere under EEP can be devided on three layers:
50—100±25 km, 100±25—200±25 km, 200±25 km
— tomographic lithosphere bottom;
3) mantle velocity boundary under EEP don’t
coincides with EEP tectonic boundary. Maximum
agreement is on the depth 50 km, and maximum
changing at the Golitsyn — Geyko depth;
4) as a whole by velocity characteristics mantle
under EEP can be divided into three parts:
boundary mantle velocity region of interaction
with 1 type activation;
main part with two type mantle velocity activa-
tions;
east part of mantle under EEP, which has diffe-
rent velocity characteristics from another mantle
part. The first type of velocity activations correspond
to propagation of high velocity layers from the
Golytsin — Geyko layer under surrounding regions
to the low velocity Golytsin-Geyko layer under EEP
and increase the part of high velocities in upper
mantle layers under surrounding zone to EEP. Sec-
ond type of velocity activation correspond to sub-
vertical low velocities layers propagation from the
middle mantle to the upper mantle. It is pick out
inclined layers, which mainly corresponded bound-
ary mantle velocity region of interaction (Figure);
5) mantle under Barents-Pechora Platforme units
with mantle under EEP by velocity characteristics
So that by velocity characteristics we have both
horizontal process and the vertical process in the
mantle under East European Platform.
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References
Geyko V. S. A general theory of the seismic traveltime tomography // Geophys. J. — 2004. — 26, ��2. — P. 3—32
(in Russian).
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