The 3,000-kilometer-long Transantarctic Mountains are a dominant feature of the Antarctic continent, yet up to now scientists have been unable to adequately explain how they formed. In a new study, geologists report that the mountains appear to be the remnant edge of a gigantic high plateau that began stretching and thinning some 105 million years ago, leaving the peaks curving along the edge of a great plain.
This study revolutionizes thinking about Antarctica’s evolution. Previous studies have discussed ways in which the mountains may have risen; the current study says they were already high long ago, and that the adjacent land sank. After the mountain chain was isolated, its topography, with summits up to 4.5 kilometers high, was accentuated by erosion caused by glaciers.
Several of the researchers did extensive field work in Antarctica to collect rock samples and geophysical data that back their ideas.
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The high elevation and considerable length of the Transantarctic Mountains have led to
speculation about their origin. To date, no model has been able to adequately reconcile the juxtaposition
of the high, curvilinear Transantarctic Mountains with the adjacent West Antarctic
Rift System, a broad region of thin extended continental crust exhibiting wide rift characteristics.
We present a fi rst-order investigation into the idea that the West Antarctic Rift System–
Transantarctic Mountains region was a high-elevation plateau with thicker than normal crust
before the onset of continental extension. With major Cretaceous extension, the rift underwent
a topographic reversal, and a plateau edge with thickened crust, representing the ancestral
Transantarctic Mountains, remained. In the Cenozoic, minor extension and major denudation
reduce the crustal root while simultaneously uplifting peak heights in the mountains.
The Cretaceous stage of this concept is investigated using two-dimensional numerical models
to determine under what conditions plateau collapse is plausible. Model results indicate that
elevation of a remnant plateau edge decreases with increasing initial Moho temperature. Very
cold initial Moho temperatures, 675 °C, under the plateau leave a thick plateau edge but do
not exhibit wide rifting. A cold to moderate initial thermal structure, Moho temperatures of
675–850 °C, is needed to retain the plateau edge and still exhibit wide rifting in the middle of
the plateau. We conclude that this plateau collapse concept is possible using these numerical
experiments, and that application of this idea to the West Antarctic Rift System–Transantarctic
Mountains system is also supported by geological and geophysical evidence.
Keywords: Transantarctic Mountains, West Antarctic Rift System, rifting, numerical modeling,
plateau collapse, Antarctica.
Figure 1. Topographic and bathymetry map of
Transantarctic Mountains and Ross Embayment;
reference location map is in upper
right. Ross Sea is characterized by a series
of basins and basement highs and elevated
heat fl ow. Ross Embayment—Ross Sea plus
Ross Ice Shelf. WARS—Ross Embayment
plus extended parts of West Antarctica.
688 GEOLOGY, August 2007
the Basin and Range. The time between the end
of Cretaceous and beginning of Cenozoic rifting
is insuffi cient to cool and thicken the lithosphere
under the mountain–rift system interface to the
level required for rift shoulder uplift.
As a way to reconcile the structures, distribution
of rifting, and the great elevation of the
mountains, we explore the possibility that the
West Antarctic Rift System was a high-elevation
plateau with thicker than normal crust before
extension related to plateau collapse. In traditional
rift shoulder uplift (Fig. 2A), narrow rifting
occurs in cold, thick lithosphere. The rift fl anks
are elevated due to thermal and mechanical
effects, and there is no crustal thickening below
the rift fl ank. In the plateau scenario (Fig. 2B),
extension of hot, thickened crust initiates rifting
and subsidence in the middle of the plateau. The
cooler edge undergoes minimal stretching and is
tectonically and erosionally denuded as a result
of lateral variations in extension.
We propose a plateau collapse scenario, with
the West Antarctic Rift System as the main body
of the plateau and Transantarctic Mountains as
the plateau edge, to explain the denudational and
extensional history of the mountains–rift system.
Wide rifting in the Cretaceous extends the rift
system, but leaves the Transantarctic plateau edge
relatively intact. During the Cenozoic, denudation
reduces the crustal root under the mountains
while simultaneously enhancing large peak uplift,
as described in Stern et al. (2005). Numerical
models of the plateau collapse scenario have been
previously applied to Basin and Range extension
(e.g., Harry et al., 1993). We use numerical
models to test the Cretaceous stage, the major
phase of extension, of this new hypothesis for the
formation of the Transtantarctic Mountains and
West Antarctic Rift System and to determine the
conditions for which retention of a plateau edge
with thick crust is plausible.
TECTONIC SETTING
The Transantarctic Mountains and West Antarctica
have been the site of repeated orogenies,
including Rodinian assembly, Rodinian breakup,
and a transition from a passive to an active margin
during Gondwana assembly (e.g., Goodge,
2002). During the Cambrian–Ordovician Ross
orogeny the region was part of the active margin
of Gondwana (Goodge, 2002, and references
therein). Subduction moved outboard to
the Pacifi c margin of Gondwana from at least
320 Ma to ca. 110 Ma (Mukasa and Dalziel,
2000). Reconstructions (e.g., Foster and Gray,
2000) indicate that the along-strike equivalent
to the region between Marie Byrd Land
and the Transantarctic Mountains, what would
have been the majority of the unextended Ross
Embayment, from the Cambrian to the Middle
Devonian was the Lachlan Fold Belt (orogen) of
southeastern Australia, then adjacent to Antarctica.
This correlation implies high paleotopography
and thickened crust in the West Antarctic
Rift System into the Devonian.
Paleocurrent orientations, lithofacies, and
stratigraphic relationships of the Devonian–
Triassic Beacon Supergroup in the central
Transantarctic Mountains suggest that deposition
began within two intermontane or successor
basins after postorogenic uplift of the Ross
terrain (e.g., Isbell, 1999). These data and the
presence of sub-Beacon relief in the central
Transantarctic Mountains suggest high paleotopography
around and between these basins.
In southern Victoria Land, the Beacon shows a
progression from marine sediment deposition,
to coal measures, to alluvial plain sediments
(Barrett, 1980, 1991). This history implies the
presence of high topography both outboard
(Ross Plateau) and inboard (East Antarctica
hinterland) of the present-day Transantarctic
Mountains and rising paleotopography within
the basin, suggesting crustal thickening under
the Transantarctic basin during this period.
Voluminous Jurassic tholeiitic magmatism
along the Transantarctic Mountains marked
the onset of Gondwana breakup (Elliot, 1992).
While Jurassic rifting is believed to have
occurred within the present-day Trans ant arctic
Mountains–West Antarctic Rift System, no
major rift-bounding faults in the mountains or
the rift system have been located (e.g., Elliot and
Fleming, 2004). The presence of voluminous
Jurassic magmatic products along the mountain
front in the form of sills and lava fl ows suggests
that this event is the most likely candidate for
further thickening of the Transantarctic crust.
Subduction ca. 105 Ma off the Marie Byrd
Land active margin ceased (e.g., Weaver et al.,
1994, and references therein), transferring New
Zealand to the Pacifi c plate, and marking the
onset of major extension in the West Antarctic
Rift System (Lawver and Gahagan, 1995). Wide
rifting (~400 km) ended with the 84–79 Ma separation
of New Zealand and the Campbell Plateau
from Antarctica (Stock and Cande, 2002). Denudation
(1–2 km magnitude) during the Cretaceous
synchronous with this major extension
is recorded along the Transantarctic Mountains
(e.g., Fitzgerald, 2002, and references therein).
The major phase of denudation, 4-9 km along
the Transantarctic front, began in the Eocene,
spatially correlative with but temporally preceding
minor extension localized in the Ross Sea
adjacent to the mountains (e.g., Fitzgerald, 2002,
and references therein). The nature and extent of
Cenozoic rifting as well as its relationship to the
thermochronology data are still uncertain. Narrow
rifting in the Terror Rift, transtension in Victoria
Land (Wilson, 1995; Rossetti et al. 2006),
Adare Trough spreading projected into the Ross
Sea (Davey et al., 2006, and references therein),
and minimal extension with mostly climatecontrolled
denudation (Karner et al., 2005) have
all been proposed as key mechanisms active in the
Cenozoic. Cenozoic alkaline magmatism associated
with Cenozoic rifting (e.g., LeMasurier and
Thomson, 1990) has a much smaller volume and
limited extent compared to Jurassic magmatism,
and is not a viable mechanism for thickening the
Transantarctic crust.
Studinger et al., (2004, 2006) demonstrated
that gravity anomalies across southern Victoria
Land and the Scott and Reedy Glacier region
are consistent with crustal thickening under the
Transantarctic Mountains relative to East Antarctica.
Seismic data on the thickness of the Transantarctic
crust indicate 40 ± 2 km crust under the
mountains and 35 ± 2 km crust under cratonic
East Antarctica (Lawrence et al., 2006).
NUMERICAL MODEL
We conducted regional scale two-dimensional
numerical models to investigate the conditions
conducive for retention of a plateau edge with
thickened continental crust after extension. In the
models, a viscoelastic-plastic, non-Newtonian
layer of thickened continental crust and adjacent
crust of normal thickness underlain by a mantle
layer is extended by pulling at the edges with
a velocity of 1 cm yr–1. Deformation is tracked
using an explicit fi nite-element method similar to
the FLAC (fast Lagrangian analysis of continua)
technique (Lavier et al., 2000, and references
therein). (A complete description of the numerical
model is in the GSA Data Repository.1)
In all models, the initial plateau is 296 km
wide, and total model width is 800 km at
Figure 2. Two classes of models of Transantarctic
Mountain uplift and Ross Embayment
subsidence. Dashed lines approximate
brittle-ductile transition. Top panel shows
pre-rift confi guration; bottom panels show
post-rift confi guration. Class A demonstrates
extension of cold, thick lithosphere. Rift fl ank
uplift raises the edges of the rift due to thermal
effects. Extension is characterized by
narrow rifting, and isotherms are shallowed
locally. Class B, proposed in this paper, demonstrates
extension of a high plateau underlain
by hot thick crust. Extension occurs over
a broad region in the former plateau, and rift
fl anks retain much of their elevation through
retention of thick crustal roots. Isotherms are
shallowed over a wide region.
1GSA Data Repository item 2007177, description
of the numerical model, is available online at www.
geosociety.org/pubs/ft2007.htm, or on request from
editing@geosociety.org or Documents Secretary,
GSA, P.O. Box 9140, Boulder, CO 80301, USA.
GEOLOGY, August 2007 689
time 0 m.y. Initial plateau crustal thickness
is 55 km, and adjacent crust is 32 km thick.
Mantle material underlies the crust to 80 km.
Initial plateau topography is a rectangle elevated
3 km above the background and is isostatically
compensated at depth.
MODEL RESULTS
A variety of extension styles was observed
over a suite of 37 numerical experiments, including
core complex formation, wide rifting, and
narrow rifting. Here we present one example in
which the edge of the plateau retains signifi cant
crustal thickness to remain an elevated highland
after extension. Initial Moho temperature under
the plateau, Tm, is 680 °C (Fig. 3A).
After 5 m.y. and 100 km of extension
(Fig. 3B), the plateau exhibits characteristics
of a wide rift. Extension is accommodated by
crustal thinning over a wide area in the lower
crust that exhibits the highest strain rates. In
the upper crust, three basins accommodate
most of the extension. Peak elevations have
been reduced several hundred meters, and little
extension occurs outside of the plateau area.
At 10 m.y. and 200 km of extension (Fig. 3C),
several small basins and ridges have developed,
but the plateau edges remain several hundred
meters above these. Crust has thinned the most
under the middle of the plateau, and the edges
have undergone the least thinning.
At 20 m.y. and 400 km of extension (Fig. 3D),
the plateau edges have retained elevations of
~1.5 km. The crust has been thinned evenly
across a broad area formerly occupied by the
plateau, and much of the extended region is below
sea level. The lower crust has been replaced by
strong upper mantle in highly thinned areas. Our
model space ends at 20 m.y., analogous to the
end of the major phase of extension and minor
denudation during the Cretaceous.
A summary of the model results (Fig. 4)
demonstrates the thermal conditions required to
leave a plateau edge with signifi cant topography
and crustal thickness in comparison to the surrounding
area. The maximum elevation of the
plateau edge is plotted against Tm at 10 m.y. and
20 m.y. There is a roughly linear decrease of
plateau elevation with increased Tm, related to
the inverse relationship of crustal viscosity and
strength with temperature. Nonlinear variation
in extensional style due to variations in model
thermal structure may be responsible for the
scatter of elevations with Tm. A very cold initial
Tm, below ~675 °C, allows for a thickened remnant
edge, but the extension is characteristic of a
narrow rift. An intermediate temperature profi le,
with Tm ~675–850 °C, exhibits wide rifting or
core complex–style rifting and retains a thick
edge as a highland, with edge thickness decreasing
with increased temperature. Above ~850 °C,
no thickened root is retained.
DISCUSSION
The necessary thermal conditions for a
plateau collapse scenario in the Transantarctic
Mountains–West Antarctic Rift System could
be achieved by low to average concentrations
of radiogenic elements, crustal rocks with high
thermal conductivities in the plateau, or some
combination thereof.
These models are not designed to precisely
emulate the lithospheric architecture across the
mountains–rift system, but simply test a concept.
All models shown (Fig. 3) are symmetrical; i.e.,
there is a plateau remnant on either side. While
the Transantarctic Mountains represent one
edge of a plateau collapse, the opposite edge of
the plateau was represented by the active margin
of Gondwana (New Zealand–Marie Byrd Land)
and was rifted away with plate reorganization
following the breakup of Gondwana.
At the end of the Cretaceous, the major
extensional phase, our conceptual model leaves
an extended West Antarctic Rift System and
relatively unextended Transantarctic Mountains
plateau edge with a crustal root of ~12–16 km
and elevations of 1–2 km. Signifi cant denudation,
~4–9 km, along the mountain front and
decreasing inland, has occurred since the start of
the Eocene. This denudation would reduce the
crustal thickness of the mountains, yet gravity
and seismic studies indicate the presence of an
~5 km root under the Transantarctic Mountains
today compared to cratonic East Antarctica. If
denudation relates directly to erosion, a crustal
root ~9–14 km thick would be required at the
end of Cretaceous extension, as is present in
our model. All mechanisms of Cenozoic extension,
whether Adare Trough spreading, transtention,
narrow rifting in Terror Rift, or climatecontrolled
denudation without major extension,
are feasible within the context of our conceptual
model. Synchronous with Cenozoic denudation
reducing the crustal root of the Transantarctic
Figure 3. Topography, crustal thickness, and viscosity time slices for 0, 5, 10, and 20 m.y.
At 0 m.y. the plateau is represented by a simple box of thickened crust in blue, underlain
by olivine mantle in purple. At 5 m.y., basins and ridges have developed in the topography
and wide rifting is observed. Lower viscosity regions in upper crust represent shear zones.
Lower mantle material has been added to accommodate the space made. At 10 m.y., both
lower and upper crust have thinned over a wide region, but plateau edges remain high. At
20 m.y., the region of weak lower crust has thinned signifi cantly, and extension is focused at
the rift edge, shown here in the viscosity profi le as the lower viscosity upper crust in yellow.
High fl ank edges are underlain by crustal roots.
Figure 4. Maximum topography at plateau
edge vs. initial Moho temperature under
plateau for 10 m.y. and 20 m.y. Both plots
show a rough linear trend of decreasing
topography with increased Moho temperature,
implying that a cold to moderate initial Moho
is needed to retain a high plateau edge.
690 GEOLOGY, August 2007
Mountains, the peak elevations are increased as
much as 50% by glacial incision (Stern et al.,
2005), leading to the peak heights of as much as
4.5 km observed today.
CONCLUSIONS
Our numerical experiments demonstrate that
rifting a plateau can leave a remnant edge at
its fl ank that retains greater crustal thickness.
Coupled with the Cenozoic denudation history
of the Transantarctic Mountains, this root
would be comparable to that seen under the
mountains today. Initially very cold conditions,
initial Moho temperatures Tm 675 °C, do not
produce distributed extension and crustal thinning
as observed in the Ross Embayment. A
moderate temperature profi le, Tm ~675–850 °C,
is needed to retain crustal thickness and elevation
at plateau fl anks and exhibit wide rift characteristics
in the extended plateau. Topography
and crustal thickness are not retained at plateau
fl anks under initially hot, Tm > 850 °C, conditions.
A plateau collapse scenario agrees with
the geological history of the region and erosional
studies attributing signifi cant peak height
increase to the effects of glacial incision.