Tectonophysics,
189 (1991) 219-221
219
Elsevier Science Publishers B.V.. Amsterdam
Seismic models of the lower lithosphere beneath the southern Baltic Sea between Sweden and Poland M. Grad a, A. Guterch
b and C.-E. Lund ’
u Institute of Geophysics, University of Warsaw, Pasteura 7, PL-02-093 Warsaw, Poland h Institute of Geophysics, Polish Academy of Sciences, Ksiqcia Janusza 64, PL-01-452 Warsaw, Poland ’ Department of Geophysics, University of Vppsala, Box 556, S 751 22 Uppsala, Sweden (Received April 7,1989;
revised version accepted December 29. 1989)
ABSTRACT Grad, M., Guterch. A. and Lund, C.-E., 1991. Seismic models of the lower lithosphere beneath the southern Baltic Sea between Sweden and Poland. In: S. Bjiimsson, S. Gregersen, E.S. Husebye, H. Korhonen and C.-E. Lund (Editors), Imaging and Understanding the Lithosphere of Scandinavia and Iceland. Tectonophysics, 189: 219-227.
Based on recordings from the northern part of the Baltic Sea-Black Sea profile and EUGENO-S profile 4, 2-D seismic models have been constructed for a profile across the southwestern part of the East European Platform from southern Sweden to northern Poland. The thickness of the crust along the profile varies from 33 to 47 km. The Moho P-wave velocity is 8.0-8.3 km/s. The uppermost mantle has a fine structure with alternating layers of higher and lower velocities. Down to a depth of about 120 km three alternating high- and low-velocity layers have been modelled. The velocities vary between 8.2 and 8.7 km/s in the high-velocity layers and 8.0 and 8.5 km/s in the low-velocity layers. A tendency of the depth of the Moho and the depth of the uppermost mantle seismic boundaries to increase towards the southeast is observed.
Introduction The first clear indication of an inhomogeneous subcrustal lithosphere in Western Europe was ob-
The lower lithosphere beneath the southern part of the Baltic Shield and the Baltic Sea between Sweden and the coastal area of northern Poland has been investigated using data from two earlier
tained from a profile across the Central Massif in France (Him et al., 1973, 1975; Kind, 1974;
seismic profiles. These two profiles are the Baltic Sea-Black Sea profile (Sollogub et al., l980; Grad
Steinmetz et al., 1974; Ansorge, 1975). These find-
et al., 1986) and the EUGENO-S profile 4 (EUGENO-S Working Group, 1988). In 1979, recordings were made in Poland and the USSR
ings were later confirmed by seismic investigations in Great Britain (Bamford et al., 1976,1978; Faber, 1978; Faber and Bamford, 1979), across the Scandinavian Peninsula (Lund, 1979) and in the Alps (Miller et al., 1978). Similar results have been
along the Baltic Sea-Black Sea profile of shots fired at four shotpoints (Pl to P4) equally spaced along the profile, and of shots fired at Fennolora
obtained in the USSR: at about the same time as in Western Europe, Ryaboy (1966) presented models for the subcrustal lithosphere showing both vertical and lateral inhomogeneities, and later work from the USSR has confirmed these results (Burmakov et al., 1975; Ryaboy, 1977; Yegorkin and Pavlenkova, 1981; Vinnik and Ryaboy, 1981; Pavlenkova and Yegorkin, 1983).
shotpoint B in Sweden. On the map (Fig. 1) only the northern part of the profile with the Polish shotpoints, PI and P2, is shown. During the 1984 EUGENO-S project, recordings were made along profile 4 in Sweden of shots fired at shotpoints 21, 22, 23 and 7 in Sweden, and also of shots fired at shotpoint 30 in Poland. Recordings were also made along the extension of profile 4 in Poland of shots
0040-1951/91/$03.50
0 1991 - Elsevier Science Publishers B.V.
fired at shotpoints 30 in Poland and 7 in Sweden. Profile 4, with its extension into Poland, is seen in
ready been published (Grad, 1987b; Working Group, 1988).
EUGENE-S
Fig. 1. In this study, recordings made along the Polish part of the Baltic Sea-Black fired at shotpoint
Geology
and crustal
stmmcture along the profile
Sea profile of shots
7 in Sweden, and recordings
The
entire
profile
made along the Swedish part of profile 4 of shots
European
fired at shotpoint
area on the western
30 in Poland have also been
Platform.
is situated
on
the
East
Starting in the Baltic Shield Swedish
formation about the lower lithosphere in the area.
southern part of Sweden, the Baltic Sea and the
cover a
total profile length of about 1000 km. The locations of the two profiles and the main geological units in the area are seen in Fig. 1. The two lower lithospheric profiles are situated on the East European Platform and run nearly parallel to the Teisseyre-Tomquist Zone in Poland and its northwestern continuation, the Tomquist Zone. Interpretations of the crustal structure yielded by the data recorded along these profiles have al-
BALTIC
Fig. 1. Location map of the EUGENE-S Baltic !%a, between European crystalline
northeastern
direction
the profile
extends
The recordings used in this investigation
in a southeasterly
coast
used. These recordings provide data yielding in-
across
the
part of Poland, ending at the Soviet
border. In Poland the profile is made up of two branches. The Baltic Shield forms the northwestern part of the East European Platform. The southeastern edge of the Baltic Shield is defined where the crystalline basement dips below the sedimentary cover of the East European Platform. In southeastern Sweden where the profile crosses the transition between the shield area and the sedimentary
SHIELD
profile 4 and the northern part of the Baltic Sea-Black
Sweden and Poland.
I = J%@eof the B&c
Shield;
2 = Tomquist
Sea p&k
in the mgiotxof the south
Line; 3 = so@hw&em
edge of the E?aat
in Poland determined from shallow seismic refraction; I- main faults; 5 = depth contours (km) of the and shotpoints. Compiled using data from Winterhalter et al. basemen t; 6 = deep seismic sounding (kmg+range) profii (1981) and Skompa (1974). Platform
SEISMIC
MODELS
OF THE
LOWER
LITHOSPHERE
area of the East European approximately In
coincides
Sweden
basement
the
mostly
profile
over
(granitoid
the southeastern
reworking
orogeny
(1200-900
Models along
and
the
of the sedimentary
the
profiles Syneclise
and
have
compiled
from
been
sections
the already
1974; Guterch
Sea,
the
Elevation,
published
re-
et al., 1975, 1986;
et al., 1981; Dadlez
1986; Grad,
showing
of the crust
Baltic
the Mazury
1976; Winterhalter
al., 1980; Grad,
Sveconorwegian
part
crossing
Peri-Baltic
Dadlez,
strong
from 0.5 to 6 km in thick-
1974).
sults (Skorupa,
and
The whole area, except for during
cover varying
ness (Skorupa,
part of
coastal part, has undergone
ensialic
mentary
Ga old
coastal
221
BALTIC
crystalline
crosses an area of granitic
composition.
SOUTHERN
coast.
gneisses
In the southeastern
the profile
gneissose
runs
THE
this border
up of 1.15-1.75
gneisses
orthogneisses). Sweden
Platform,
with the Swedish
made
polymetamorphic
BENEATH
1987a,b).
the structure
et
Generalized
of the sedimentary
crust along the profiles
are seen in Figs
The profile crosses the Baltic Sea between southeastern Sweden and northern Poland. The maximum water depth along the profile is about 100 m. The crystalline basement across the Baltic
The
layered
of the sedimentary
and
the velocities
Sea is covered
form. To the southeast, across the Baltic Sea, the thickness of the sediments increases to about 3 km
Ma).
by Cambro-Silurian
sediments
been
3 km
(Winterhalter
in the
coastal
area
in-
the two branches
of the profile
= u
Poland
Baltic
of various
from seismic
cover
ages have
measurements
and
data in the Polish part of the plat-
the thickness of the sediments decreases to about 0.5 km in the Mazury Elevation. Along the exten-
run over a sedi-
Baltic Shield SPB
of rocks
2a and b.
in thecoastal area of Poland. Along the northern part of the Baltic Sea-Black Sea profile in Poland
of Poland
et al., 1981). In northeastern
determined
from borehole
creasing in thickness from the outcropping basement in the coastal region of southeastern Sweden to about
structure
Sea
Pen-Baltic
Syneclise
Mazury Elevation
SP Pl
SP P?
[al
DiSTANCC Baltic Shield SP23 SP22
iN KM Pen-Baltic
Baltic Sea SP 21
Syneclise SP30
SP 7
lb1
I00
0
200
300
DISTANCE Fig. 2.Generalized
600
500
IN KM
sections showing the structure of the sedimentary layers along (a) the northern part of the Baltic Sea-Black
profile and (b) the EUGENO-S
profile 4 extension in Poland. I = Water (velocity of P-wave 1.5 km/s);
sediments (mean layer velocity 2.2-2.5 (mean layer
400
velocity 4.2-4.5 km/s);
km/s);
3 = Permian sediments (velocity 5.1-5.2
5 = crystalline basement (velocity 6.0-6.2
km/s).
km/s);
Sea
2 = Cainozoic and Mesozoic
4 = Lower Palaeozoic sediments
Compiled from Winterhalter et al. (1981).
Dadla (1976), Dadlez et al. (1980), Skorupa (1974), Grad 1987a), and EUGENO-S
Working Group (1988).
22’
sion of EUGENO-S ness
increases
Syneclise.
profile
to about
The velocity
varies from 1.8 km/s layer to 4.5 km/s the sequences. good marker The rocks Polish
part
4 in Poland
the thick-
6 km in the Peri-Baltic in the sedimentary
in the uppermost Permian
km/s.
sequence. basement
East
European
in the
Platform
he
beneath the sedimentary cover at depths varying from 200-500 m in the area of the Mazury Elevation to about
8-9 km in the marginal
down
of 7.1-7.4
from
part,
of 6.6-6.8
the crust
part of
of the crystalline
km. The middle
velocities
layer acts as a
in the sedimentary of the
cover
Cainozoic
in the lower Palaeozoic
A 5.2 km/s
18-25
has a velocity
to 42-47
the Moho)
km/s. velocity
The mean velocity
down
km/s.
to 30 -36 km,
The lower part of
km is characterized
by
The Pn-wave
(refracted
varies
8.1 to 8.3
from
of the crystalline
part of
the crust is about 6.6 km/s. The mean velocity for the whole crust varies with the thickness of the sediments.
For a 3-6 km thick sedimentary
the velocity
varies
km/s
1986).
(Grad,
respectively
from
cover
6.3 to 6.1
zone of the
platform (Teisseyre-Tomquist Zone). The crystalline basement has been formed under the in-
Interpretation
fluence
of several
Karelian
granitoid
Models of the crystalline part of the crust down to the Moho along the whole profile have been
tectonic massif
zones of pre-Karelian
cycles, separates
and Karelian
and
the pre-
a number
of
metamorphic
rocks (Ryka, 1984). In Sweden, along profile 4 the crustal thickness varies between 32 and 47 km; the crust is at its thickest beneath the central part of the profile. The upper crust varies in thickness from 11 km in the northwest to 20 km along the southeastern part of the profile. The velocity varies from about 6 km/s near the surface to, in the deepest part of the profile, about 7.2 above the Moho. The mean crustal velocity is about 6.6 km/s (EUGENO-S Working
Group,
1988).
In Poland the total crustal thickness varies from 42 to 47 km. The crystalline part of the crust comprises a three-layer structure. The upper part, with velocities of 6.1-6.4 km/s, reaches a depth of
. . Baltic
460
Sea - Black
Sea
480
Profile,
compiled based on the EUGENO-S model (EUGENO-S Working Group,
profile 4 1988) and
the Baltic Sea-Black Sea model (Grad, 198723). The modelling of the lower lithosphere has been carried the northern
out using recordings in Poland along part of the Baltic Sea-Black Sea
profile from SP B in Sweden and recordings along the EUGENO-S profile 4 in Sweden from SP 30 in Poland. The two record sections are seen in Figs. 3 and 4. A number of phases have been correlated in the record sections. phase denoted Pd and connected most part
of the upper
mantle
In addition to a with the upper(below
the Moho
boundary), three other phases denoted P’, P2 and P3 have also been correlated. These phases are interpreted as reflections or diving waves from
SP 6
500
520 DISTAKCE
540
560
KM
Fig. 3. Record section from SP B recorded along the northern part of the Baltic Sea-Bleck
Sea profile. Lines indicate th~retiutl
traveltime curves for lithospheric waves P’, Pz and P3 computed for a 2-D model. Reduction velocity 8 km/s.
SEISMIC
MODELS
OF THE
12
LOWER
EUGENO-S,
LITHOSPHERE
BENEATH
THE SOUTHERN
223
BALTIC
Profile 4. SP 30
(a)
10
Fig. 4. Record
sections
from SP 30 recorded traveltimes
within
layers
with
higher
FROM
along EUGENO-S
in the lower
lithosphere. For the record section of EUGENO-S profile 4 (Fig. 4) recorded in Sweden from SP 30 in Poland, the various correlated phases may be seen. The phases can only be correlated as first arrivals over distances of 50-300 km. The time delays between the different phases indicate the existence of zones of lower velocity. In addition to phases Pi-P3 one more phase has also been correlated
in the record
recorded about distance interval The
depth
section
(Fig. 4). This phase
is
2 s later than phase P3 in the 480-650 km from the shotpoint.
to the
SHOT
POINT.
reflecting
boundry
has
been
estimated at about 140-145 km. It is not possible to correlate the phase in the section in Fig. 3. In the record section from the northern part of the Baltic Sea-Black Sea profile recorded in Poland from SP B the three phases (P’, P2 and P3) have been correlated in the distance range 460-560 from the shotpoint. The various refracted
km and
reflected waves have been recorded with a relatively large amount of background noise. It would be very difficult or even impossible to separate these waves if only single-channel stations had been used: the use of multichannel stations, with a channel separation of 200 m, makes separation of
650
km
profile 4. (a) Without
interpretation.
of waves Pd, P’, P* and P3 for a 2-D model. Reduction
velocities
600
550
450 DISTANCE
velocity
With computed
ard interpreted
8 km/s.
the various arrivals possible, even when their amplitudes are small. Even though the recording layout for the section was not particularly dense, envelope lines can nevertheless be correlated for the refracted phase P’ and for the groups of reflected waves P2 and P3. In the two sections (Figs. 3 and 4) the phases P’, P2 and P3 are all connected with high-velocity layers in the lower lithosphere. In Fig. 3, phase P’ represents a diving wave from within the first high-velocity layer. The two following
phases,
P2 and
P3, represent
re-
flected waves from the top of the second and third high-velocity layers. In Fig. 4, phases P’ and P2 represent diving waves and P3 a reflected The crustal models briefly explained
wave. in the
previous section were used in the input model. The 2-D models of the lower lithosphere were developed using the ray tracing package RAY81 (cerveny and PSenEik, 1981). The depths of boundaries and the velocity distribution were chosen and corrected by comparing the experimental and calculated traveltimes of the waves P’, P* and P3. Theoretical traveltimes were recalculated for several succesive versions of the models until good agreement, of the order of 0.1-0.2 s, between the traveltimes was obtained. The depths to the top of
224
c 120
EUGENO-S, Fig. 5. Ekmple
of modetig
PROFILE 4, SP 30
of the lower lithosphere
Baltic Shield
on EUGENO-S profile 4. Ray diagrams for waves P’, P2 and P3 from SP 30. L VL = bw-W&xity layer.
Baftic Sea
0
30
s
DlSTANCE
(KM)
SEISMIC
MODELS
OF THE
the low-velocity points
LOWER
zones
BENEATH
were determined
of the deepest
diagrams.
LITHOSPHERE
northern
beneath
using
EUGENO-S
ray
profile
4 and the Sea profile
determined
in the lower lithosphere
from refracted
of
which are
or reflected
of the lithosphere
has been
carried
Both the velocities
and the depth given for the different boundaries are distorted and exceed the true values for the Earth
(Hill,
1972).
For
depths
sponding to the lower lithosphere these of the order of 1 km for any given 0.1-0.15 km/s for any given velocity. the velocities corrected for the spherical
corre-
errors are depth and In Fig. 6, Earth are
given in parentheses. In the two models shown in Figs. 6a and b, the two points marked SP B and SP 7 are the same point. From the Moho down to a depth of about 120 km, three layers with higher velocities separated
by zones
modelled.
of lower
The thickness
the profiles P-wave
ing, models
velocities
have
been
of the high-velocity
is about lo-20 km, and for the low-velocity about IO-30 km. The high-velocity layers
been
from the
Sea Profile
is greater
Sweden
of
from 33 to 47 than
From long-range
The data
of the
The thickness
varies
of the lower lithosphere
constructed.
plained mantle.
data
4, 2-D models
velocity
in the two profiles.
ern Baltic Sea between
out using the flat Earth model.
spherical
profile
have been presented. along
km. The Moho
waves are
with heavy lines.
Modelling
lithosphere the crust km/s
sounding
part of the Baltic Sea-Black
and the EUGENO-S
of the lower
are shown in Fig. 6. In both cases the segments
marked
Based on deep seismic northern
part of the Baltic Sea-Black
the boundaries
225
BALTIC
Conclusion
for waves P’, P2 and
P3 from SP 30 is shown in Fig. 5. The main elements of the models lithosphere
SOUTHERN
from the
ray penetration
The ray diagram
THE
8
record-
for the south-
and Poland
observed
have
can be ex-
by a nearly hor~ontally strati?ied upper From the Moho down to a depth of about
120 km, three alternating high- and lclw-velocity layers have been modelled. The thickness of the high-velocity layers is about lo-20 km, and for the low-velocity layers about lo-30 km. The velocities vary with depth between 8.2 and km/s in the high-velocity layers and between and 8.5 km/s in the low-velocity layers. The results
obtained
for northeastern
can be compared with the results ern part of the Baltic Sea-Black P4) (Grad et al., 1986; Grad, study too the lower lithosphere
layers
135 km consists
layers in the
low-velocity
of three wave
field
Poland
from the southSea profile (SP
198713): In Grad’s down to a depth of
alternating
layers with thicknesses
In the observed
8.7 8.0
high-
and
of lo-25
km.
from
shot-
recorded
lower lithosphere have been modelled in the depth intervals 33-50, 55-75 and SO-105 km. The Pwave velocities found and corrected to the spheri-
point P4 in the distance interval 600-900 km and 0.3-0.5 s after the first arrivals, an extended group of reflected waves lasting LO-l.2 s occurs. At-
cal Earth
tempts at explaining such a compleu reflected wave group suggest the possibility of the existence of an alternating series of high- and low-velocity
are 8.15, 8.37 and 8.69 km/s
and 8.04,
8.26 and 8.46 km/s for high- and low-velocity layers respectively. The two models indicate a southeasterly downdip for the lower lithosphere structures. In general, the lower lithospheric boundaries in northeastern Poland are about lo30 km deeper than in southern Sweden.
Fig. 6. Models
of the lithosphere
I = sediments;
2 = upper
km/s); boundary; reflected
along
the northern
4 = lower part of the crust (velocity 7 = low-velocity or refracted
part
part of the crust with P-wave 6.9-7.2
waves. Values in lower lithospheric
of the Baltic
velocities
km/s);
zones in the lower lithosphere;
layers of the order of a few kilometres in thickness at a depth of 110-135 km (Grad et al.. 1986). Regarding southern Sweden, in general our results agree with earlier findings from the Baltic
Sea-Black
of 6.0-6.4
5 = low-veIocity 8 = sections
km/s;
3 = middle
(a) and EUGENO-S part of the crust
zones in the upper crust (velocity
of the boundaries
layers are P-wave velocities
are for spherical
Sea profile
Earth models.
(km/s)
profile (velocity
6.1 km/s);
in the lower lithosphere for flat Earth models;
4 (b). 6.6-6.8
6 = Moho
determined
from
those parentheses
Shield (Lund, gisberg,
1979; Cassel and Fuchs,
1986; Luosto,
1986; Clowes
1979; Guget al.. 1987).
In particular,
our model can be compared
results
from
the
Fennolora
profile
in the
around
SP 7. The Fennolora
profile
and EUGE-
NO-S profile on
4 cross each other
Fennolora).
In
that
along the two profiles profiles
down to a depth
the
Moho
has been layered
of about
depth
33 km. Along
the lower lithosphere
as a high- and low-velocity
area
at SP 7 (= SP B
area,
is about
with the
both
modelled
upper
mantle
120 km.
Dadlez,
R.. Deczkowski,
of structural
versus its basement, EUGENO-S
Working
tectonic
evolution
and the North ject).
Faber,
work
German
S., 1978.
Lithosphke
was carried
out
within
the
framework
of
exchange between the two academies. The data were recorded during the international EGT EUGENO-S project and during various and international projects in Poland.
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