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Tectonophysics 366 (2003) 55–81
The transition from an active to a passive margin
(SW end of the South Shetland Trench, Antarctic Peninsula)
Antonio Jabaloya,*, Juan-Carlos Balanyab,c, Antonio Barnolasd,Jesus Galindo-Zaldıvara, F. Javier Hernandez-Molinae, Andres Maldonadoc,
Jose-Miguel Martınez-Martıneza,c, Jose Rodrıguez-Fernandezc,Carlos Sanz de Galdeanoc, Luis Somozad, Emma Surinachf, Juan Tomas Vazquezg
aDepartment Geodinamica, University Granada, 18071 Granada, SpainbDepartment de Ciencias Experimentales, University Pablo de Olavide, Sevilla, Spain
c Instituto Andaluz de Ciencias de la Tierra, C.S.I.C.-University, Granada, Spaind Instituto Geologico y Minero de Espana, Madrid, Spain
eDepartment Geociencias Marinas y O. D. Territorio, University Vigo, Vigo, Pontevedra, SpainfDepartament de Geodinamica i Geofısica, Universitat de Barcelona, Barcelona, Spain
gFacultad de Ciencias del Mar, Universidad de Cadiz, Puerto Real, Cadiz, Spain
Received 12 December 2001; accepted 12 February 2003
Abstract
The lateral ending of the South Shetland Trench is analysed on the basis of swath bathymetry and multichannel seismic
profiles in order to establish the tectonic and stratigraphic features of the transition from an northeastward active to a
southwestward passive margin style. This trench is associated with a lithospheric-scale thrust accommodating the internal
deformation in the Antarctic Plate and its lateral end represents the tip-line of this thrust. The evolutionary model deduced from
the structures and the stratigraphic record includes a first stage with a compressional deformation, predating the end of the
subduction in the southwestern part of the study area that produced reverse faults in the oceanic crust during the Tortonian. The
second stage occurred during the Messinian and includes distributed compressional deformation around the tip-line of the basal
detachment, originating a high at the base of the slope and the collapse of the now inactive accretionary prism of the passive
margin. The initial subduction of the high at the base of the slope induced the deformation of the accretionary prism and the
formation of another high in the shelf—the Shelf Transition High. The third stage, from the Early Pliocene to the present-day,
includes the active compressional deformation of the shelf and the base-of-slope around the tip-line of the basal detachment,
while extensional deformations are active in the outer swell of the trench.
D 2003 Elsevier Science B.V. All rights reserved.
Keywords: Subduction zone; Active margin; Trench termination; Tip-line; Antarctic Peninsula
0040-1951/03/$ - see front matter D 2003 Elsevier Science B.V. All right
doi:10.1016/S0040-1951(03)00060-X
* Corresponding author. Fax: +34-958-248527.
E-mail address: [email protected] (A. Jabaloy).
1. Introduction
Trenches associated with oceanic subduction zones
usually end in triple junctions or against plate boun-
s reserved.
Fig. 1. (A) Geological setting of the Antarctic Peninsula and the Drake Passage; the rectangle indicates the study area. The location of the magnetic anomalies and transform faults
south of the Shackleton Fracture Zone are from Larter and Barker (1991). (B) Distribution of the plates around chron C2An, when the Phoenix–Antarctic spreading axis became
inactive.
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A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 57
daries—normally another subduction zone or a trans-
form fault. However, in several areas of the world,
there are oceanic trenches that show a transition
toward a passive margin or the abyssal plain in broad
bands of deformation. An example of these trenches is
the northern end of the East Luzon Trough, which is
the prolongation of the Philippine Trench towards the
north, located at the eastern end of the Philippine
Islands (Hayes and Lewis, 1984). Another example is
near the Antarctic Peninsula, where an active small
trench known as the South Shetland Trench (Maldo-
nado et al., 1994) coexists with inactive subduction
zones in the oceanic lithosphere of the southwestern
sector of the Antarctic Peninsula (Gohl et al., 1997).
Although these trenches are known to terminate
laterally, the literature contains no description of the
morphology and structure associated with such termi-
nations.
The main aim of the present paper is the analysis of
the structure and stratigraphy of the SW end of the
South Shetland Trench in the Antarctic Peninsula in
order to determine how and why this trench terminates
(Fig. 1). A second objective is to study the transition
from an active to a passive margin and how the
deformation along the transition zone between the
two is accommodated. Most continental passive mar-
gins result from a previous rifting phase that produces
a continental break-up stage followed by a spreading
stage. However, the western margin of the Antarctic
Peninsula evolved from an active margin, progres-
sively decreasing in length since the Jurassic as results
of trench-ridge collisions, towards a passive-type
margin.
2. Geological setting
The South Shetland Trench is a slightly arched NE-
SW trench located in the northwestern sector of the
Antarctic Peninsula (Maldonado et al., 1994). It is
associated with a small island arc represented by the
South Shetland Islands. The Bransfield Strait, a nar-
row NE-SW basin with depths greater than 2000 m,
separates these islands from the Antarctic Peninsula
(Barker and Austin, 1998) (Fig. 1A and B).
This trench is the last remnant of a once extensive
trench that occupied the Pacific margin of the Ant-
arctic Peninsula. During the Cainozoic, several NE-
SW segments of the Phoenix–Antarctic spreading
axis separated by NW-SE transform faults collided
with the trench. After the collision, the continental
margin lithosphere and the oceanic lithosphere to the
north of the spreading axis came into contact, which
led to the end of subduction and the disappearance of
the trench bathymetry (Herron and Tucholke, 1976;
Barker, 1982; Larter and Barker, 1991). The collisions
progressively migrated northeastward and the differ-
ent sectors of the active margin evolved towards a
passive style following the subduction of the segments
of the spreading axis.
The last two collisions took place to the north of
the North Anvers Fracture Zone and involved two
segments of the Phoenix–Antarctic spreading axis
separated by the C Fracture Zone (Larter and Barker,
1991) (Fig. 1). The segment located between the
North Anvers and the C fracture zones collided
obliquely after the formation in the oceanic crust of
anomaly chron C4n (Fig. 1A). The segment located
between the C and Hero fracture zones also underwent
an oblique collision, after anomaly C3An (Fig. 1A).
During the anomaly chron C2An, activity in the
Phoenix–Antarctic spreading axis ended and the
Phoenix Plate became part of the Antarctic Plate
(Livermore et al., 2000). Meanwhile, activity in the
trench continued, though at present convergence rates
are slow (Maldonado et al., 1994; Kim et al., 1995).
Aldaya and Maldonado (1996) defined the South
Shetland Block as an independent fragment of the
Antarctic Plate (Fig. 1B). Its movement is slightly
different from this plate, which is now migrating
northwestward from the Antarctic Peninsula due to
spreading in the Bransfield Strait Rift. This block
constitutes the upper plate of the South Shetland
Trench.
The subduction has generated a Cainozoic accre-
tionary prism in the forearc with a lobular front. In
contrast, the trench region comprises a relatively small
area that is probably experiencing tectonic erosion and
where the subduction has originated the Hesperides
forearc basin (Maldonado et al., 1994). This forearc
basin records a subsidence history in the middle
continental slope, including the migration of the depo-
centers toward the continent.
The continental shelf contains progradational
sequences produced mainly by the action of ice sheets
during the last glacial maximum (Larter and Barker,
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–8158
1989; Larter and Cunningham, 1993; Bart and Ander-
son, 1995). The location of the shelf break is related to
the sediment supply and, in several sectors, the shelf
progrades above the forearc basin (Maldonado et al.,
1994). A number of compressive structures have been
Fig. 2. Location chart of the ANTPAC 97/98 cruise with B/O Hesperides tr
MCS profiles in Figs. 4–8, while thin track lines correspond to profiles no
cruise. The thin lines represent the bathymetry of the area derived from t
Isolines are every 500 m except in the shelf, where an additional isoline at
ODP Leg 178 within the study area.
described in this shelf. A NNW-SSE anticline char-
acterises the outer shelf near Smith Island, while to the
SW, a NE-SW basement high called the Mid Shelf
High occupies the middle continental shelf (Larter and
Barker, 1991). Volcanic bodies of Upper Pleistocene–
ack lines in the study area. Thick track lines show the location of the
t shown in this work. Dashed lines correspond to transit lines of the
he Shipboard Scientific Party (1999), modified with our own data.
250 m depth is marked. Circles represent the location of the sites of
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 59
Holocene alkaline basalts are present in the shelf
(Hole and Larter, 1993); these authors propose a
magmatic origin associated with a slab window below
the Antarctic Peninsula, after the collision of the
spreading axis with the trench.
3. Data acquisition
Our data were obtained aboard the Spanish vessel
B/O Hesperides during the ANTPAC 97/98 cruise in
the Antarctic summer of 1997/1998. During this
cruise, approximately 1200 km of swath bathymetry
data along profiles and some 900 km of multichannel
reflection seismic profiles were obtained at the SW
end of the South Shetland Trench. Nine of these
profiles are orthogonal to the continental margin
(SHSM-01a, SHSM-03, SHSM-04, SHSM-05,
SHSM-06, SHSM-08, SHSM-09, SHSM-10 and
SHSM-13) and three run parallel to the margin
(SHSM-1b, SHSM-07 and SHSM-11) (Fig. 2). In
addition, we gathered two profiles oblique to the
margin trend (SHSM-02 and SHSM-12).
The multichannel reflection seismic profiles were
obtained with a tuned array of five BOLT air
guns, having a total volume of 22.14 l and a streamer
with a total length of 2.4 km and 96 channels. The
shot interval was 50 m and pressure was 140 atm.
Data were recorded with a DFS V digital system, a
sampling record interval of 2 ms and 10 s record
length. We processed the data with a standard se-
quence, including migration using a DISCO/FOCUS
system.
The swath bathymetry data were obtained with a
SIMRAD EM 12 system and post-processed with
NEPTUNE software at the Instituto de Ciencias del
Mar of Barcelona (Spain). They were visualized at the
Oregon State University (USA) using the comercial
software FLEDERMAUS.
4. Physiography and major morpho-sedimentary
features
The continental margin varies from an active mar-
gin in the South Shetland forearc to a passive style in
the southwestern segment (Figs. 2 and 3). The active
margin segment is characterised by the development of
a trench and an accretionary prism (Figs. 2, 3 and 6).
The two segments are separated by two bathymetric
highs where the trench ends. We refer to the first one,
located in the shelf break at 63j15VS, 64j15VW, as the
‘‘Shelf Transition High’’. The second one is located at
the base of the slope at 63j00VS, 64j30VW, and
separates the continental rise from the trench; we call
it the ‘‘Base-of-Slope Transition High’’.
In both segments of the margin, the continental
shelf is predominantly subhorizontal, although several
important depressions and swells trending NE-SW are
observed (Fig. 2). The shelf basins show a maximum
depth of 750 m, whereas the bathymetric highs of the
inner shelf are about 150 m. The shelf break is usually
located between 350 and 450 m, though in the Shelf
Transition High, with NE-SW elongation, it is only at
a depth of about 275 m (Fig. 2).
The continental slope in the passive margin can
be divided into two adjacent sectors. The NE slope
is characterised by a staircase geometry influenced
by the structure of the basement (Figs. 3 and 4), and
is less subsident and progradational than the south-
western sector. The southwestern slope is a homo-
geneous steep slope (Fig. 4). The continental slope
in the transition sector between the active and the
passive margin shows the greatest dip, with 31j of
mean slope. The continental slope in the active
margin is characterised by a reduced accretionary
prism, with a mean dip around 15j. An incipient
mid-slope forearc depression develops over this
accretionary prism. The upper slope features scarps
with 300 m of relief.
In the passive margin, there is a narrow base-of-
slope that is gradually transitional towards the slightly
undulated continental rise at approximately 3000 m
water depth, where the C Fracture Zone has almost no
associated relief (Fig. 2). In the transition between the
active and the passive margin, the oceanic basin floor
has depths between 2900 and 3650 m and the sea
floor has an irregular physiography, with two NE-SW
troughs separated by the elongated Base-of-Slope
Transition High (Figs. 2, 3 and 5). These troughs
merge with the South Shetland Trench to the north-
east, but they disappear southwestward. Seaward, the
basin plain is dissected by several E-W or ENE-WSW
elongated highs with elevations of 200–300 m above
the surrounding relief. In the active margin, the lower
slope ends at 4400 m water depth in the floor of the
Fig. 3. Shaded relief images (Fledermaus) oblique views of the SW end of the South Shetland Trench. Top: view from the W towards the E.
Bottom: view from the SW towards the NE. Length of area is about 130 km, the arrow indicating north.
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–8160
near-horizontal trench fill deposits (Figs. 2 and 6).
The deposits in the trench are dissected by ENE-
WSW to NE-SW scarps, which developed a staircase
bathymetry in several places within the trench. The
GLORIA image (Maldonado et al., 1994, their Fig. 2)
shows the presence of others scarps trending NNW-
SSE to NW-SE. The elongated NW-SE relief associ-
ated with the Hero Fracture Zone dissects the base of
the slope, which is at a water depth of about 3900 m
(Fig. 2).
Fig. 4. Multichannel seismic profile SHSM-03 in the passive margin and line-drawing interpretation.
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 pp. 61–62
Fig. 5. Multichannel seismic profile SHSM-06 in the transition zone and line-drawing interpretation.
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 pp. 63–64
Fig. 6. Multichannel seismic profiles SHSM-08 and SHSM-09 in the active margin and line-drawing interpretation.
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 pp. 65–68
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5. Sedimentary sequences
The sedimentary record in the continental margin
presents two major seismic units that show different
acoustic responses and different stacking patterns in
the various domains of the margin.
5.1. Base of the slope
At the base of the slope, the Lower Unit covers the
entire study area except in front of the Shelf Transition
High, where only the upper major unit appears. The
Lower Unit has a weak reflective response, with a
locally transparent configuration (profiles SHSM-1b,
SHSM-02, SHSM-03 and SHSM-08; Figs. 4, 6, 7 and
8). The top of the Lower Unit is a major discontinuity
marked by a high-amplitude reflector designated as
the Middle Reflector (MR) Discontinuity (Figs. 4, 6, 7
and 8, Table 1). Although there are no direct data from
drillings, the sediments most likely consist of pelagic
deposits. The existence of two minor erosional dis-
continuities allows us to distinguish three depositional
sequences in this Lower Unit: MS-7, MS-6 and MS-5,
from bottom to top. Depositional sequence MS-7
occurs only on the oceanic crust southwest of the C
Fracture Zone (profiles SHSM-02 and SHSM-03;
Figs. 4 and 8), where magnetic anomalies Chron
C5n to Chron C3An are identified (Larter and Barker,
1991). This sequence represents the first sedimentary
record above the igneous oceanic crust. Depositional
sequences MS-6 and MS-5 directly cap the igneous
rocks of layer 2 (profile SHSM-08; Fig. 6), which
show anomaly Chron C3An (Larter and Barker,
1991). These two sequences include wedge-shaped
deposits with a high reflective acoustic response and a
chaotic internal structure that may represent synsedi-
mentary olistostromic rocks.
The Upper Unit has a very reflective acoustic
response characterised by intermediate- to high-ampli-
tude reflectors that are laterally continuous. They can
be observed throughout the base of the slope and in
the trench (profiles SHSM1b, SHSM-02, SHSM-03,
SHSM-06 and SHSM-08; Figs. 4–8). Several internal
discontinuities marked by regional high-amplitude
reflectors that we have termed UR3, UR2 and UR1
(UR: Upper Reflector), from bottom to top, help
define four depositional sequences in this Upper Unit:
MS-4 to MS-1, likewise from bottom to top. Sequen-
ces MS-4 to MS-1 can be correlated with sequences
M3 to M1 of Rebesco et al. (1997), which were also
studied at Site 1101 of Leg 178 (located west of the
study area at 3509 m water depth in the continental
rise of the margin) (Shipboard Scientific Party, 1999).
5.2. Shelf and slope
The Lower Unit also has a low to intermediate
reflective acoustic response with a local transparent
configuration (profiles SHSM-03 and SHSM-09;
Figs. 4 and 6). An irregular high-amplitude reflector
marks the top of this unit and has the geometry of a
major discontinuity, which can be traced to the MR
discontinuity of the base of the slope (Figs. 4, 6, 7 and
8, Table 1). There are two discontinuities inside the
Lower Unit separating reflectors identified by an
aggradational to divergent stacking pattern. These
discontinuities serve to separate three depositional
sequences called MS-7, MS-6 and MS-5, the MR
discontinuity conforming the top of sequence MS-5.
The internal reflector of each depositional sequence
tends to on-lap the discontinuity at its base.
The Upper Unit in the shelf and slope is charac-
terised by discontinuous reflectors of intermediate to
high amplitude (profiles SHSM-03, SHSM-06 and
SHSM-09; Figs. 4–6). Three high-amplitude reflec-
tors (UR3, UR2 and UR1), corresponding to the three
unconformities in the shelf, allow us to differentiate
four upper sequences, MS-4 to MS-1 (profiles SHSM-
03, SHSM-06 and SHSM-09; Figs. 4–6). These
correlate to the sequences described above for the
base of the slope. In relation to the seismic stacking
pattern of every sequence, the MS-4 sequence is
aggradational to progradational, while the MS-3
sequence is progradational. In turn, sequence MS-2
is an aggradational to progradational one and the last
sequence (MS-1) shows an aggradational pattern.
Whereas we have identified four depositional
sequences in this area, Larter and Barker (1991) and
the Shipboard Scientific Party (1999) distinguish three
sequences in the shelf (S3, S2 and S1 from bottom to
top, separated by two major discontinuities). Our
sequences MS-1 and MS-2 directly correlate with
the sequence S1 of these authors. Sequences MS-3
and MS-4 could respectively correlate with the S2 and
S3 sequences of Larter and Barker (1991) and the
Shipboard Scientific Party (1999) (Table 1), while our
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Fig. 7. (A) Multichannel seismic profile SHSM-01b in the oceanic crust and line-drawing interpretation. (B) Window of the same profile in the
area of the Base-of-Slope Transition High.
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Table 1
Depositional sequences in the continental margin of the study area and cronostratigraphical approach
Depositional
sequences
Chron Age Sequences of
Later and Barker
(1991)
Sequences of
Rebesco et al.
(1997)
Upper Unit MS-1 C1n Middle Pleistocene–Holocene S1 M1
UR1 Discontinuity
MS-2 C2r.2r Late Pliocene–Middle Pleistocene S1 M2
UR2 Discontinuity
MS-3 C2n (uncertain data age) Pliocene S2 M3
UR3 Discontinuity
MS-4 Early Pliocene S3 M4
Lower Unit MR-Discontinuity (Late Messinian–Early Pliocene)
MS-5 C3An Messinian S3 ¿?
MS-6 S4 ¿?
MS-7 C4n Tortonian–Early Messinian S5 ¿?
reflectors UR2 and UR3 are respective equivalents of
the tops of sequences S2 and S3 previously identified
(Table 1). The results of sites 1100, 1102, and 1103
from Leg 178 indicate that all four sequences from
MS-4 to MS-1 have a glacial origin in the shelf
(Shipboard Scientific Party, 1999).
6. Structure
6.1. Base of the slope
The oceanic basement of the former Phoenix Plate,
northeast of the Hero Fracture Zone, has a regular
fabric made up of NE-SW parallel lineaments with a
lateral continuity of up to 30 km in length (Fig. 9), as
interpreted from the GLORIA images by Maldonado
et al. (1994, their Fig. 2). In our seismic profiles, these
lineaments correspond to the scarps of normal faults.
Where these faults displace the most recent reflectors
of the depositional sequences they have a clear
bathymetric expression, but in other locations they
are capped by the MS-3, MS-2 and MS-1 depositional
sequences (profiles SHSM-06 and SHSM-08; Figs. 5
and 6). These faults were probably generated as a
response to the flexure of the lithosphere near the
trench (NW end of profile ANT-92-2, Maldonado et
al., 1994).
Southwest of the confluence of the trench with the
Hero Fracture Zone, the oceanic crust shows a sig-
moidal fabric in the GLORIA image (Maldonado et
al., 1994) defined by lineaments with an E-W trend in
their central part and a NE-SW trend at their ends
(Fig. 9). In the seismic profiles, this fabric can be
related with faults (profiles SHSM-03 and SHSM-06;
Figs. 4 and 5). There are normal and reverse faults,
dipping towards the south or the north (profiles
SHSM-1b, SHSM-03, SHSM-06 and SHSM-07,
SHSM-08, SHSM-09; Figs. 4, 5, 6, 7 and 9). Most
of the faults affect only depositional sequence MS-7
and are capped by sequence MS-6 (profiles SHSM-03
and SHSM-06; Figs. 4 and 5).
In addition, active reverse faults cut the entire
depositional cover (profile SHSM-1b, Fig. 7). The
most important of these active reverse faults is located
close to the trench end; we call it the Transition High
Reverse Fault (THRF). The trace of the THRF in the
sea bottom is an E-W scarp that is slightly concave
towards the south, with a clear relief in the swath
bathymetry (Figs. 2 and 9). This THRF separates two
blocks where the top of the oceanic basement lies at
different depths, the downthrown block being the
north block near the trench (profile SHSM-1b, Fig.
7A and B). This reverse fault intersects the main
detachment fault at the base of the accretionary prism
and clearly deforms all the depositional sequences
(profile SHSM-1b, Fig. 7).
6.2. Accretionary prism
The accretionary prism is 15-25 km wide in the
profiles perpendicular to the margin. The front is
active in the NE sector, as shown by the large detach-
ment fault at the base of the prism that crops out at the
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Fig. 8. Multichannel seismic profile SHSM-02 in the oceanic crust and line-drawing interpretation.
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Fig. 9. Tectonic map of the study area deduced from the seismic profiles. The lower rectangle includes a tectonic sketch of the area. Fine lines
are the interpretation of GLORIA image from Tomlinson et al. (1992) and Maldonado et al. (1994).
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 75
Fig. 10. Map of the GEOSAT free-air gravity anomalies from Sandwell and Smith (1997), isolines every 10 mGals. Stars represent earthquake
epicentres. Thick track lines show the location of theMCSprofiles in Figs. 4–8, while thin track lines correspond to profiles not shown in this work.
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–8176
prism toe (profile SHSM-08; Figs. 6 and 9). This
prism cannot be recognised in the area of the Shelf
Transition High (profile SHSM-06, Fig. 5). However,
a relict accretionary prism appears in the passive
margin segment (profile SHSM-03, Fig. 4), super-
posed over sequence MS-7. The rocks of sequences
MS-6 and MS-5 are intercalated with olistostromic
deposits at the front of the accretionary prism. How-
ever, these deposits show no evidence of being
affected by the subduction. Sequences MS-4 to MS-
1 capped the accretionary prism (profile SHSM-03,
Fig. 4).
The transition between the active and the passive
segments is marked by a concave inflexion of the
trace of the lobular front of the accretionary prism,
which advances landward partially surrounding the
Base-of-Slope Transition High. The Shelf Transition
High is just in front of the concave inflexion and, in
profile SHSM-06 (Fig. 5), appears as a raised block
bounded by normal faults. However, the dips of the
reflectors of the upper depositional sequences MS-4 to
MS-01 also indicate that it is an antiform. Southwest
of this concave inflexion, the relict accretionary prism
develops another seaward convex inflexion (Fig. 9).
Top layers 1 and 2 of the oceanic crust and the
basal detachment are clearly seen over a distance of
10–20 km below the accretionary prism (profile
SHSM-08; Fig. 6). The detachment dip is around
2–4j, assuming Vp = 1.8 km/s in the rocks of the
prism and trench. Its frontal part has a footwall ramp
geometry, cutting the reflectors of the trench upward
with a very low angle. Landward, however, the
detachment ramp grades to a detachment flat geome-
try. Only the upper part of the trench filling (0.1–0.3 s
TWT) is accreted into the prism, while most of the
trench deposits (around 0.7 s TWT) are subducted.
Although the internal structure of the accretionary
prism is not apparent, several faults dipping towards
the SE can be seen to produce a reverse offset of the
reflectors. In the middle continental slope, several
extensional faults induce tilting of the reflectors in
the hanging wall (profile SHSM-09; Fig. 6). They are
responsible for the scarps observed in the upper slope.
6.3. Slope and shelf
The southwestward extension of the Hesperides
Forearc Basin, identified by Maldonado et al. (1994),
is evident in the upper slope of the active margin. The
thickness and width of the basin decrease towards the
SW and cannot be recognised in profile SHSM-06
(Figs. 5 and 9). Very open folds trending NNW-SSE
to N-S deform the forearc deposits. These folds affect
all the depositional sequences with the exception of
the upper part of sequence MS-1.
A basin with synform geometry, buried under more
recent deposits, can be seen in the middle slope of the
passive margin over the relict accretionary prism. The
basin is associated with a slope break and probably
represents a relict forearc basin (profile SHSM-03,
Fig. 4).
The shelf is deformed by a set of very open
synforms and antiforms (Fig. 9). The free-air gravity
anomalies in the shelf approximately coincide with
the location of these folds, and the elongation of the
anomalies indicates they have a NE-SW trend (Figs. 9
and 10). The antiforms usually reveal outcrops of the
basement, which are eroded, yet locally buried below
a very thin sedimentary cover. The synforms are
normally filled by thin depositional sequences and
usually correspond to ancient glacial troughs. In the
area between Smith Island and the Shelf Transition
High, these NE-SW folds interfere with the NNW-
SSE to N-S trending folds. Only in one case, a small
half-graben associated with a normal fault is observed
in the shelf (profile SHSM-08-09; Figs. 6 and 9). This
normal fault dips with a NW component.
7. Discussion
In this area of transition between an active and a
passive margin, different tectonic and depositional
processes were at work, controlling the margin growth
patterns. We will first discuss the possible age of the
depositional sequences and then the structure of the
area and its relationship with the sedimentary pro-
cesses.
7.1. Age of the sequences: a chronological approach
Depositional sequences MS-7, MS-6 and MS-5
settled diachronously directly on top of layer 2 of
the oceanic crust, producing the magnetic anomalies
ranging from Chron C5n to Chron C3An (according
to the magnetic data published by Larter and Barker,
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 77
1991). Sequence MS-7 lies southwest of Fracture
Zone C over the oldest oceanic crust of the area, with
anomalies from Chron C5n to Chron C4n. However,
sequences MS-6 and MS-5 directly overlie the igne-
ous rocks in the active margin northeast of Fracture
Zone C, where we find the younger oceanic crust with
anomaly Chron C3An. In accordance with the ages
proposed by Berggren et al. (1995), sequence MS-7,
deposited prior to Chron C3n and after Chron C4n,
must be Late Tortonian to Early Messinian in age.
Sequences MS-6 and MS-5 can be assigned to the
Messinian (Table 1).
At the base of the slope, the data from Site 1101 of
Leg 178 indicate that the Upper Unit, characterised by
strong reflectivity in the seismic profiles, probably has
an age between Late Pliocene and Quaternary (Ship-
board Scientific Party, 1999). These site data allow the
base of sequence MS-1 to be dated at the base of Chron
C1n, giving Middle Pleistocene to Holocene ages for
this unit (Table 1). The base of sequence MS-2 can be
dated at the top of Chron C2r.2r, which indicates an
Early Pleistocene to Late Pliocene age. Moreover, the
top of sequence MS-3 covers Chron C2r.2r up to the
base of Chron C2An.1n, indicating a Late Pliocene
age. These ages are also suggested by the MCS profile
presented by Rebesco et al. (in press) between Site
1096 and the study area, allowing a correlation
between the depositional sequences and the ODP drill
Site. On this basis we attribute an Early Pliocene age to
sequence MS-4. Discontinuity MR, marking the tran-
sition from the Upper (sequences MS-4 to MS-1) to the
Lower Unit (sequences MS-7 to MS-5), may have a
Late Messinian to Early Pliocene age. Depositional
sequences MS-7, MS-6 and MS-5 are equivalent to
sequences S5, S4 and S3 of Larter and Barker (1991)
in the Antarctic Pacific Margin.
Data are scarce in the shelf, but agree with the ages
determined for the base of the slope. It is also possible
to correlate the sequences determined in the base of
the slope with the sequences of the slope and the shelf,
because they are laterally continuous. In any case, the
top of sequence MS-4, marked by reflector UR3, has
been dated at 4.5-4.6 Ma by the Shipboard Scientific
Party (1999). We can thus propose an Early Pliocene
age for the MS-4 sequence as well (Table 1).
Sequence MS-3, equivalent to sequence S2 of the
Shipboard Scientific Party (1999), has been dated at
its base as Early Pliocene, while the age of its upper
part remains unknown. The MS-1 and MS-2 sequen-
ces (equivalent to sequence S1) can be assumed to be
Pleistocene to latest Pliocene in age (Shipboard Sci-
entific Party, 1999).
7.2. Active margin
At present, active subduction in the South Shetland
Trench is a subject of debate. Barker and Burrell
(1977), the GRAPE Team (1990) and more recently
Kuminuma (1995) suggest the subduction is now
inactive. Barker (1982) and Pelayo and Wiens (1989)
indicate that there is no Wadati-Benioff zone associ-
ated with a subducting slab, yet on the basis of the
earthquake focal mechanisms, they conclude that sub-
duction is still active. Ibanez et al. (1997) describe the
existence of intermediate earthquakes (50 < h < 150
km) below the western South Shetland Islands, sug-
gesting the existence of a subducting slab. The litho-
sphere velocity model obtained by Grad et al. (1993)
based on refraction seismic experiments favours this
interpretation. In this model, the authors obtain a
slab of oceanic lithosphere with a dip of 25j subduct-
ing below the continental crust of the South Shet-
land Trench. Neither the earthquakes nor the velocity
model confirm the existence of the slab below 80–130
km.
The seismic reflection studies carried out by Larter
(1991), Maldonado et al. (1994) and Kim et al. (1995)
show that the most recent trench deposits are
deformed at the accretionary prism, below the basal
detachment. These data agree with our observations in
the NE active segment of the study area, where a
small accretionary prism overthrusts the deposits of
the trench, whereas most of the trench fill sediments
are subducted (Fig. 6). The subduction of the trench
deposits has been observed in other parts of the trench
as well (Maldonado et al., 1994), suggesting the
existence of tectonic erosion. These authors estimate
the convergence rates at around 4–6 cm/year from 30
to 6.7 Ma, when they underwent a sharp decrease. The
present-day convergence rates are approximately 1–2
cm/year.
7.3. Passive margin and shelf
The relict accretionary prism lies over sequence
MS-7 in the passive margin. Sequences MS-6 and
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–8178
MS-5 are not subducted and are intercalated with
olistostromes derived from the accretionary prism.
These features indicate a latest Tortonian age for the
end of the subduction in this area, which is compat-
ible with the end of subduction following the ridge-
trench collision after chron C4n. Sequences MS-4 to
MS-1 capped the olistostromes and the relict accre-
tionary prism. The reverse faults that deformed layer
2 of the oceanic crust (profiles SHSM-03 and
SHSM-06; Figs. 4 and 5) were coetaneous with the
deposition of sequence MS-7, indicating the exis-
tence of compressive deformation during the Torto-
nian, prior to the end of subduction. The accretionary
prism has a front with convex inflexion that suggests
the collapse of the prism and the seaward advance
of its front (Fig. 9). Collapse is also implied by
the presence of the olistostromes in the front and
their relationship with sequences MS-6 and MS-5
suggests a Messinian age for the collapse of the
accretionary prism. There are no major deformations
in the slope or the continental rise. After the de-
position of units MS-5, sedimentary processes do-
minated during the recent stages of the margin
development.
The most important structures in the shelf are the
NE-SW folds. Single-channel seismic surveys of
previous works revealed only the antiform located in
the middle shelf (Kimura, 1982; Anderson et al.,
1990; Larter and Barker, 1991), termed the ‘‘Midshelf
High’’ (Larter and Barker, 1991). New MCS data
indicate that these folds, which are now growing,
deform the entire shelf. The folds have the same
characteristics in both the active and passive margins,
indicating that the whole shelf is undergoing NW-SE
compression.
In the sector between Smith Island and the Shelf
Transition High, the NNW-SSE to N-S folds devel-
oped practically coetaneously with the aforemen-
tioned NE-SW ones. The two-fold systems interfere,
suggesting that this sector has undergone constric-
tional deformation with area reduction.
7.4. Transition between the passive and the active
margins
The tectonic map obtained from the interpretation
of the seismic profiles shows that the South Shetland
Trench continues 50 km southwest of the Hero
Fracture Zone (Fig. 9), as previously reported by
Tomlinson et al. (1992) and Maldonado et al.
(1994). We located the end of the trench at the
Base-of-Slope Transition High. Southwestward from
the end of the trench, the basal detachment of the
accretionary prism splits into two active major reverse
faults (the THRF and the basal detachment itself),
whereas the trench splits into two small troughs. The
two major reverse faults end toward the SW and are
replaced by E-W active reverse faults. This means that
the area of accommodation of the shortening is greater
than the bifurcation area of the main detachment fault.
Southwest of the Base-of-Slope Transition High, all
the compressive structures are inactive, indicating the
end of the compressional tectonics.
The upper plate of the subduction is the South
Shetland Block (part of the Antarctic Plate), while the
lower one is the oceanic crust of the same Antarctic
Plate. The two elements join in the transition area
between the active and the passive margins. There is
no evidence of a transform fault separating these
elements, as has been proposed in previous models.
The trench is acting as an internal subduction zone
that accommodates shortening inside the Antarctic
Plate and the study region represents the outcrop area
of the tip-line of this subduction zone.
The Shelf Transition High is an antiform fold
bounded by normal faults. This fold may be respon-
sible for the loss of continuity in the Hesperides
Forearc Basin, which develops two perisynclinal
terminations on either side of the high. The main
deformation phase produced highly deformed depo-
sitional sequences MS-7, MS-6 and MS-5, whereas
the internal reflectors of sequences MS-4 to MS-1
developed progressive unconformities on the conti-
nental side of the high. This suggests that the high
was generated in the Late Messinian–Early Pliocene
and has been growing continuously to the present
time.
The concave major inflexion in the lobular front of
the accretionary prism is associated with the presence
of the Base-of-Slope and the Shelf Transition Highs,
the discontinuity of the forearc basin and the defor-
mation of the accretionary prism. Such an association
of structures is strongly reminiscent of the structures
produced by the subduction of a seamount (Domi-
nguez et al., 1998, 2000). However, as we have
pointed out above, there is no evidence of a high in
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 79
the oceanic crust except for the Base-of-Slope Tran-
sition High, which is due to the active reverse faults
originating from the split of the basal detachment. We
propose that this inflexion may be associated with the
tendency to subduction of the Base-of-Slope Transi-
tion High, which is the deformed area that accom-
modates the end of the trench.
Another process that may have contributed to the
major inflexion is the rollback process proposed for
this trench (Larter, 1991; Maldonado et al., 1994).
The advance of the front of the prism towards the
NW—while the outcrop of the tip-line remained in
place—could have originated a rotation of the front,
producing an arched pattern for the prism. In this
model, extension in the back-arc region that is
accommodated by the Bransfield Strait rift could
not continue southwestward from the end of the
trench. This is supported by the observation that the
shelf in the study area is under compression and the
extensional deformations are reduced to a single
normal fault SE of Smith Island that disappears
toward the SW.
7.5. Oceanic crust
The lineaments observed in the oceanic crust run
parallel to the trench NE of the Hero Fracture Zone,
and have a sigmoidal pattern between the C and the
Hero Fracture Zones (Fig. 9). Most of these linea-
ments are normal faults that cut layer 1 of the oceanic
crust, although there are also several normal faults
capped by the most recent sediments. Northeast of the
Hero Fracture Zone, these faults are interpreted as
normal faults produced by extension of the subducting
slab in the outer swell (Maldonado et al., 1994; Kim et
al., 1995). In the sector between the C and the Hero
Fracture Zones, the sigmoidal pattern of the linea-
ments could indicate that the outer swell is separating
from the trench and is located farther towards the
ocean, where it disappears. In this region, the outer
swell also becomes wider than in the NE sector of the
area and the normal faults cut even the flat bottom of
the trench. The sigmoidal pattern of the structures
could also be favoured by an originally sigmoidal
pattern of the fabric of the oceanic rocks suggested by
the oblique orientation of the C3An and C4An mag-
netic anomalies of the oceanic crust in this area (Larter
and Barker, 1991).
7.6. Tectonic model
The model of the evolution in the area can be
summarised in several stages. The first stage, in the
Tortonian, corresponds to the ridge-trench collision
after anomaly chron C4n, which preceded the end of
subduction in the present-day passive margin. A
compressive deformation event deformed the oceanic
crust simultaneously with the deposition of sequence
MS-7. This stage finished in the latest Tortonian–
Early Messinian, when subduction ended in the pas-
sive margin. The tip-line of the intraplate subduction
moved to its present-day location and marks the onset
of the second tectonic stage during the Messinian.
During this second stage, the accretionary prism
collapsed in the passive margin sector. The internal
deformation in the area of the tip-line, mainly by
reverse faults, generated the Base-of-Slope Transition
High in the oceanic crust. The second stage ended in
the latest Messinian–Early Pliocene with the conver-
gence of this high against the accretionary prism,
thereby producing its concave inflexion and internal
deformation, as well as the loss of continuity of the
forearc basin. Sequences MS-6 and MS-5 were depos-
ited during this stage The third stage, from the Early
Pliocene to the present-day, corresponds to the devel-
opment of compressive deformation in the shelf and in
the base of the slope near the Base-of-Slope Transition
High, while extensional deformation occurs in the fore
bulge of the subduction footwall. During this time, the
deposition of sequences MS-4 to MS-1 originated the
progradation of the passive margin, while these
sequences are deformed in the active margin.
8. Conclusions
The structural model discussed in this paper stands
as one of the few well-documented case studies of the
tectonic evolution of the lateral end of a subduction
zone, and of the transition from an active to a passive
margin style. The lateral end of subduction is accom-
panied by the decrease of the slip of the basal detach-
ment, which ends in a tip-line. Around the tip-line lies
an area with distributed compressional deformation,
both in the oceanic crust of the subducting plate and
the accretionary prism of the overriding plate. The
evolution of the area includes a first stage when a
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–8180
compressional deformation preceding the end of the
subduction produced reverse faults in the oceanic
crust. This first stage ended when subduction ceased
southwest of the study area in the latest Tortonian.
The second stage involves the development of dis-
tributed compressional deformation around the tip-
line of the basal detachment of the accretionary prism.
The deformation gave rise to a high in the oceanic
crust at the base of the slope. The subduction of this
high produced the deformation of the accretionary
prism and the formation of another high in the shelf
(the Shelf Transition High) at the end of the Messinian
or the beginning of the Pliocene. The third stage
began in the Early Pliocene and continues at present.
It entails the active deformation, in a compressional
setting, of the shelf and the base of the slope around
the tip-line of the basal detachment, while extensional
deformations are active in the outer swell of the
trench.
Acknowledgements
We would like to thank the Commander, officers
and crew of the B/O Hesperides for their help during
the ANTPAC 97-98 cruise. We are grateful for the
help of the U.G.B.O. technicians participating in the
cruise. The expert help of Emilia Litcheva and Javier
Maldonado, who processed the MCS and the swath
bathymetry, is appreciated. We also acknowledge the
work of Jean Sanders in reviewing the English text
and A. Carbo for the release of the Lanzada software.
The Spanish ‘‘Comision Interministerial de Ciencia y
Tecnologıa (CICYT)’’ provided financial support
through research project ANT99-0817.
References
Aldaya, F., Maldonado, A., 1996. Tectonics of the triple junction at
the southern end of the Shackleton Fracture Zone (Antarctic
Peninsula). Geomarine Lett. 16, 279–286.
Anderson, J.B., Pope, P.G., Thomas, M.A., 1990. Evolution and
hydrocarbon potential of the northern Antarctic Peninsula con-
tinental shelf. In: St. John, B. (Ed.), Antarctica as an Exploration
Frontier—Hydrocarbon Potential, Geology and Hazards. AAPG
Stud. Geol., vol. 31, pp. 1–12.
Barker, P.F., 1982. The Cenozoic Subduction history of the Pacific
margin of the Antarctic Peninsula: ridge crest-trench interac-
tions. J. Geol. Soc. Lond. 139, 787–801.
Barker, P.F., Burrell, J., 1977. The opening of Drake Passage. Mar.
Geol. 25, 15–34.
Barker, D.H.N., Austin Jr., J.A., 1998. Rift propagation, detachment
faulting and associated magmatism in Bransfield Strait, Antarc-
tic Peninsula. J. Geophys. Res. 103, 24017–24043.
Bart, P.J., Anderson, J.B., 1995. Seismic record of glacial events
affecting the pacific margin of the northwestern Antarctic Pen-
insula. In: Cooper, A.K., Barker, P.F., Brancolini, G. (Eds.),
Geology and Seismic Stratigraphy of the Antarctic Margin. Ant-
arctic Research Series, vol. 68, pp. 74–95.
Berggren, W.A., Kent, D.V., Swisher, C.C., Aubry, M.P.J., 1995. A
revised Cenozic geochronology and chronostratigraphy. In:
Berggren, W.A., Kent, D.V., Aubry, M.P., Handerbol, J.
(Eds.), Geochronology, Time Scales and Global Stratigraphic
Correlation. SEPM Spacial Publication, vol. 54, pp. 129–213.
Dominguez, S., Lallemand, S., Malavielle, J., Schnurle, P., 1998.
Oblique subduction of the Gagua Ridge beneath the Ryukyu
accretionary wedge system: insights from marine observations
and sandbox experiments. Mar. Geophys. Res. 20, 383–402.
Dominguez, S., Malavielle, J., Lallemand, S., 2000. Deformation of
accretionary wedges in response to seamount subduction: in-
sights from sandbox experiments. Tectonics 19, 3182–3196.
Gohl, K., Nitsche, F., Miller, H., 1997. Seismic and gravity data
reveal Tertiary intraplate subduction in the Bellinghausen Sea,
southeast Pacific. Geology 25, 371–374.
Grad, M., Guterch, A., Janik, T., 1993. Seismic structure of the
lithosphere across the zone of subducted Drake Plate under
the Antarctica Plate, west Antarctica. Geophys. J. Int. 115,
586–600.
GRAPE Team, 1990. Preliminary results of seismic reflection in-
vestigations and associated geophysical studies in the area of the
Antarctic Peninsula. Antarct. Sci. 2, 223–234.
Hayes, D.E., Lewis, S.D., 1984. A geophysical study of the Manila
Trench, Luzon, Philippines: 1. Crustal structure, gravity, and
regional tectonic evolution. J. Geophys. Res. 89, 9171–9195.
Herron, E.M., Tucholke, B.F., 1976. Sea floor magnetic patterns
and basement structure in the southeastern Pacific. Int. Rep.
DSDP 35, 263–276.
Hole, M.J., Larter, R.D., 1993. Trench-proximal volcanism follow-
ing ridge crest-trench collision along the Antarctic Peninsula.
Tectonics 12, 897–910.
Ibanez, J.M., Morales, J., Alguacil, G., Almendros, J., Ortiz, R., Del
Pezzo, E., 1997. Intermediate-focus earthquakes under South
Shetland Islands (Antarctica). Geophys. Res. Lett. 24, 531–534.
Kim, Y., Kim, H.S., Larter, R.D., Camerlenghi, A., Gamboa,
L.A.P., Rudowski, S., 1995. Tectonic deformation in the upper
crust and sediments at the South Shetland Trench. In: Cooper,
A.K., Barker, P.F., Brancolini, G. (Eds.), Geology and seismic
stratigraphy of the Antarctic margin. Antarctic Research Series,
vol. 68, pp. 157–166.
Kimura, K., 1982. Geological and geophysical survey in the Bel-
linghausen Basin, off Antarctica: Antarctic Record. Natl. Inst.
Polar Res. 75, 12–24. (Tokyo, Japan).
Kuminuma, K., 1995. Seismicity around the Antarctic Peninsula.
Proc. NIPR Symp. Antarct. Sci. 8, 35–42.
A. Jabaloy et al. / Tectonophysics 366 (2003) 55–81 81
Larter, R.D., 1991. Debate: preliminary results of seismic reflection
investigations and associated geophysical studies in the area of
the Antarctic Peninsula. Antarct. Sci. 3, 217–222.
Larter, R.D., Barker, P.F., 1989. Seismic stratigraphy of the Antarc-
tic Peninsula Pacific margin: a record of Pliocene–Pleistocene
ice volume and paleoclimate. Geology 17, 731–734.
Larter, R.D., Barker, P.F., 1991. Effects of ridge crest-trench inter-
action on Antarctic–Phoenix spreading: forces on a young sub-
ducting plate. J. Geophys. Res. 96, 19586–19607.
Larter, R.D., Cunningham, A.P., 1993. The depositional pattern and
distribution of glacial– interglacial sequences on the Antarctic
Peninsula Pacific Margin. Mar. Geol. 109, 203–219.
Livermore, R.A., Balanya, J.C., Maldonado, A., Martınez, J.M.,
Rodrıguez-Fernandez, J., Sanz de Galdeano, C., Galindo-Zaldı-
var, J., Jabaloy, A., Barnolas, A., Somoza, L., Hernandez, J.,
Surinach, E., Viseras, C., 2000. Autopsy of a dead spreading
centre: the Phoenix Ridge, Drake Passage, Antarctica. Geology
28, 607–610.
Maldonado, A., Larter, R., Aldaya, F., 1994. Forearc tectonic evo-
lution of the South Shetland margin, Antarctic Peninsula. Tec-
tonics 13, 1345–1370.
Pelayo, A.M., Wiens, D.A., 1989. Seismotectonics and relative
plate motions in the Scotia Sea region. J. Geophys. Res. 94,
7293–7320.
Rebesco, M., Larter, R.D., Barker, P.F., Camerlenghi, A., Vanneste,
L.E., 1997. The history of sedimentation on the continental rise
west of the Antarctic Peninsula. In: Barker, P.F., Cooper, A.K.
(Eds.), Geology and Seismic Stratigraphy of the Antarctic Mar-
gin, 2. Antarctic Research Series, vol. 71. American Geophys-
ical Union, Washington, DC, USA, pp. 29–49.
Rebesco, M., Pudsey, C., Canals, M., Camerlenghi, A., Barker, P.,
Estrada, F., Lucchi, R., Giorgetti, A., in press. Sediment Drift
and Deep-Sea Channel Systems, Antarctic Peninsula Pacific
Margin. In: Stow, D.A.V., Pudsey, C.J., Howe, J., Faugeres,
J.C. (Eds.), Atlas of Deep-Water Contourite Systems, Memoir
of the Geological Society, Special publication.
Sandwell, D.T., Smith, W.H.F., 1997. Marine gravity anomaly from
Geosat and ERS-1 satellite altimetry. J. Geophys. Res. 102,
10039–10054.
Shipboard Scientific Party, 1999. Leg 178 summary: antartic gla-
cial history ans sea-level change. In: Barker, P.F., Camerlenghi,
A., Acton, G., et al. (Eds.), Proc. ODP, Init. Reps., vol. 178,
pp. 1–60. College Sation, TX (Ocean Drilling Program).
Tomlinson, J.S., Pudsey, C.J., Livermore, R.A., Larter, R.D.,
Barker, P.F., 1992. Long-range sidescan sonar (GLORIA) sur-
vey of the Pacific margin of the Antarctic Peninsula. In: Yosh-
ide, Y., et al. (Ed.), Recent Progress in Antarctica Earth Science.
Terra Scientifica, Tokyo, Japan, pp. 423–429.