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Contents lists available at ScienceDirect
Earth and Planetary Science Letters
www.elsevier.com/locate/epsl
Widespread Antarctic glaciation during the Late Eocene
Andrew Carter a,∗ , Teal R. Riley b , Claus-Dieter Hillenbrand b , Martin Rittner c
a
b
c
Department of Earth and Planetary Sciences, Birkbeck, University of London, Malet Street, London WC1E 7HX, UK
British Antarctic Survey, High Cross, Madingley Road, Cambridge CB3 0ET, UK
Department of Earth Sciences, University College London, Gower Street, London WC1E 6BT, UK
a r t i c l e
i n f o
Article history:
Received 29 June 2016
Received in revised form 21 October 2016
Accepted 23 October 2016
Available online xxxx
Editor: H. Stoll
Keywords:
Eocene–Oligocene transition
Antarctica
glaciation
IRD
provenance
a b s t r a c t
Marine sedimentary rocks drilled on the southeastern margin of the South Orkney microcontinent in
Antarctica (Ocean Drilling Program Leg 113 Site 696) were deposited between ∼36.5 Ma to 33.6 Ma,
across the Eocene–Oligocene climate transition. The recovered rocks contain abundant grains exhibiting
mechanical features diagnostic of iceberg-rafted debris. Sand provenance based on a multi-proxy
approach that included petrographic analysis of over 275,000 grains, detrital zircon geochronology and
apatite thermochronometry rule out local sources (Antarctic Peninsula or the South Orkney Islands) for
the material. Instead the ice-transported grains show a clear provenance from the southern Weddell Sea
region, extending from the Ellsworth–Whitmore Mountains of West Antarctica to the coastal region
of Dronning Maud Land in East Antarctica. This study provides the first evidence for a continuity
of widespread glacier calving along the coastline of the southern Weddell Sea embayment at least
2.5 million yrs before the prominent oxygen isotope event at 34–33.5 Ma that is considered to mark
the onset of widespread glaciation of the Antarctic continent.
2016 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY-NC-ND
license (http://creativecommons.org/licenses/by-nc-nd/4.0/).
1. Introduction
The period leading up to the glaciation of Antarctica remains
poorly understood. Whilst there is a general consensus that the
onset of continent-wide glaciation in Antarctica occurred around
the Eocene–Oligocene Transition (EOT) during a prominent oxygen
isotope excursion at 34–33.5 Ma it is debatable as to whether a
single or combination of drivers and feedbacks collectively drove
the climate transition. The oxygen isotope event is manifested by
a sharp transient increase in deep-sea benthic foraminiferal δ 18 O
values reflecting cooling and a major growth in global ice volume
(Coxall et al., 2005; Zachos et al., 2001), a significant sea-level fall
that implies major ice build-up in Antarctica (Miller et al., 2005;
Stocchi et al., 2013), deposition of ice rafted debris (IRD) on the
seabed around Antarctica (Zachos et al., 1992) and geochemical
(Basak and Martin, 2013; Passchier et al., 2013), and clay and mineralogical changes (Ehrmann and Mackensen, 1992; Houben et al.,
2013) that show a shift from chemical to physical weathering of
terrigenous detritus supplied from the Antarctic continent to the
Southern Ocean.
*
Corresponding author.
E-mail address: a.carter@ucl.ac.uk (A. Carter).
Work by Scher et al. (2014) on Middle to Late Eocene sediments
from Ocean Drilling Program (ODP) Site 738 on the Kerguelen
Plateau (Fig. 1) produced a high-resolution benthic foraminiferal
δ 18 O record alongside a Nd isotope record, for the clay and siltsized (<63 µm) terrigenous fraction. The data identified a transient rise in benthic δ 18 O values at c. 37.3 Ma that the authors
interpreted as a possible episode of ice sheet expansion and referred to as the PrOM event (Priabonian oxygen isotope maximum). During this excursion radiogenic ε Nd values of terrigenous
sediment were lower and consistent with an increased contribution of fine-grained sediment from old source terrains such as
Prydz Bay and/or Wilkes Land (Fig. 1). It was proposed that these
sediments were most likely of glaciofluvial origin and therefore ice
was present in East Antarctic drainage basins at that time. However, the nature of these proxy data cannot tie the sediments to
specific source areas and there is no direct evidence to completely
rule out fluvial transport, e.g. along the Lambert Graben (Fig. 1)
and/or transport by bottom currents.
Despite some evidence for Eocene ice, it is clear that considerable uncertainties remain about the nature and geographical
extent of the earliest ice on Antarctica due to the limitations of
geochemical proxy records in defining ice volume and of far-field
proxy records in locating ice-sheet build-up. This has steered researchers to explore sediment lithologies, grain sizes and microtexture data in more proximal records along the Antarctic mar-
http://dx.doi.org/10.1016/j.epsl.2016.10.045
0012-821X/ 2016 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY-NC-ND license
(http://creativecommons.org/licenses/by-nc-nd/4.0/).
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Fig. 1. Present-day locations of areas, where major studies on marine sediments
have been undertaken for reconstructing Antarctic ice-sheet history during the
Palaeogene and/or Neogene.
gin. The studies have found evidence of glacigenic components
in marine sediments, such as diamictons deposited on the shelf,
glacial microtextures on sand grains in shelf sediments and IRD
in deep-sea sediments, that predate the EOT (e.g. in Prydz Bay,
on Maud Rise and Kerguelen Plateau (Fig. 1) (Barron et al., 1991;
Breza and Wise, 1992; Ehrmann and Mackensen, 1992; Strand
et al., 2003). Based on these findings the authors argued for
mountainous glaciers reaching sea level during the Middle to Late
Eocene, i.e. significantly prior to the marked shift in oxygen isotope
values, but some of the evidence was disputed because of ambiguous depositional settings (e.g. interpretation of diamictons either
as subglacial tills or debris flow deposits), age model uncertainties
(e.g. the biostratigraphic age used in Strand et al. (2003) are loosely
given as lower Oligocene to upper Eocene) and possible down-hole
contamination of IRD records with significantly younger IRD.
The most recent proximal data for the state of early ice comes
from the Cape Roberts Drilling Project (CRP) which investigated a
shallow-water glaciomarine sedimentary succession in the Victoria Land Basin (CRP-3 on Fig. 1) on the western Ross Sea shelf and
found a major increase in glacially derived sediments at around
33 Ma (Barrett, 2007). The well-dated CRP-3 drill core suggests a
stable continental-scale West Antarctic Ice Sheet (WAIS) calving at
the coastline only after 32.8 Ma (Galeotti et al., 2016). There is
evidence for orbital pacing of glacial advance and retreat cycles between 34 and 31 Ma, indicating that the nascent Antarctic ice was
strongly sensitive to local insolation forcing. The stabilization of
continental scale WAIS at 32.8 Ma appears to have been sensitive
to crossing a CO2 threshold, although the precise CO2 threshold
for ice expansion is subject to huge uncertainties (Anagnostou et
al., 2016; Gasson et al., 2014). Furthermore, the study by Galeotti
et al. (2016) only constrained a part of the WAIS proximal to the
coastline in the western Ross Sea. Consequently, the location and
extent of Late Palaeogene glacial ice in Antarctica, and the origins
of the much larger East Antarctic Ice Sheet (EAIS) remains unresolved.
To improve understanding of the state of the Antarctic
cryosphere we studied the provenance of Late Eocene to Oligocene
marine sediments from ODP Leg 113 Site 696 drilled on the southeastern margin of the South Orkney Microcontinent (SOM; Fig. 2).
Paleolatitude reconstructions based on a reference frame rela-
tive to the Earth’s spin axis (van Hinsbergen et al., 2015) show
that in the Late Eocene the SOM was 600–800 km south of its
present-day location and part of the northern tip of the Antarctic Peninsula arc-fore-arc terrane (Fig. 3) before Eocene rifting
and opening of the Powell and Jane Basins (Fig. 2) caused the
geographic isolation of the SOM (Eagles and Livermore, 2002;
Eagles and Jokat, 2014). Whilst the changes in location of the SOM
are reasonably well constrained this is not the case for Drake Passage opening which involved the dispersal of a mosaic of small
continental blocks that once formed the land bridge connecting
South America with the Antarctic Peninsula.
This Eocene rifting resulted in the opening of a newly formed
rift basin capturing the bulk of the terrigenous detritus shed from
the northern Antarctic Peninsula, confining sedimentation on the
SOM shelf to local sources and potentially iceberg-rafted debris
(IBRD) from distal sources. The latter is likely because at present
the SOM is located within ‘iceberg alley’. Today icebergs calved
from the East Antarctic Ice Sheet and released into the Antarctic
Coastal Current, a comparatively fast, shallow westward current,
mix with icebergs derived from West Antarctica in the cyclonic
Weddell Gyre, which transports the icebergs northwards into the
Scotia Sea (Fig. 2). A similar circulation system with a protoWeddell Gyre, similar to today, probably existed already during
the Eocene. This is suggested by general circulation model experiments of Eocene paleoceanographic circulation that replicate
the spatial distribution and relative abundance patterns and endemism amongst fossil Transantarctic flora (Huber et al., 2004;
Bijl et al., 2011).
2. Material
Site 696 was drilled during ODP Leg 113 in 1987. Located on
the southeastern margin of the SOM at a water depth of 650 m
drilling passed through a sequence of hemipelagic, and pelagic terrigenous sediments deposited between the Late Eocene and the
Quaternary (Barker et al., 1988; Wei and Wise, 1990). Despite of
only 27% core recovery the oldest part of the drilled sequence is
well represented. This study focuses on the shallow marine, sandysilty mudstones from the lowermost lithological sub-Units VII C
and D between 577 m below seafloor and the base of the hole at
646 m.b.s.f. (Fig. 4). Age constraints were established through calcareous nannofossil stratigraphy during the time of drilling (Wei
and Wise, 1990) and recently updated by Houben et al. (2013)
(Fig. 5). Based on the first consistent occurrence of Isthmolithus
recurvus and presence of Reticulofenestra bisecta the latter authors
conservatively estimated the base of the drilled interval to be
36.5 Ma old although the sequence could be as old as 37.6 Ma.
The youngest samples examined in this study (52R and 51R) are
below core 55R at 569.4 mbsf, which is dated to 33.6 Ma based on
the first consistent occurrence of the dinocyst Malvinia escutiana.
Sample 51R yielded Middle Miocene diatoms (Denticulopsis lauta,
Denticulopsis hustedti, Denticulopsis sp, Denticulopsis maccolummii).
To test for a local source of terrigenous material deposited at Site
696 we also analysed bedrock samples from Coronation and Powell
Island (Fig. 3).
3. Methods and approach
For this study, we investigated the mineralogical and geochemical composition of grains in the sand fraction 0.063–2.0 mm.
Mounts of washed sand grains were screened to determine bulk
compositions by automated energy-dispersive X-ray spectroscopy
®
on a QEMSCAN platform which allows micron-scale mapping
and mineral identification of samples (Pirrie and Rollinson, 2011).
These analyses showed quartz-feldspar sands rich in heavy minerals. To define the sources of the sand grains we performed single
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Fig. 2. A) Geography of the Weddell Sea sector and the provenance locations (coloured) referred to in the text. B) Bathymetry of the South Orkney microcontinental shelf,
location of Site 696 geology and of Coronation Island and Powell Island and sample sites after Flowerdew et al. (2011).
grain geochronological (zircon U–Pb) and thermochronological (apatite fission track) dating. Populations of single grain ages are used
to fingerprint and identify the sand sources by comparing the re-
sults to corresponding data previously published from around the
Weddell Sea embayment as well as with the new data from the
South Orkney Islands and the northern Antarctic Peninsula. This
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Fig. 4. Stratigraphy and age control for samples from ODP 113 Site 696B.
Fig. 3. Paleogeographic reconstruction adapted from Eagles and Jokat (2014) showing (A) the position of the South Orkney Microcontinent during the Middle to Late
Eocene. Paleolatitude is from van Hinderbergen et al. (2015). (B) For comparison the
present day location is also shown.
approach has been successfully tested in Antarctica where such
ages reliably record the geological composition of source areas
(Pierce et al., 2014).
The sand grains may have come directly from melting icebergs
that have calved from ice streams and outlet glaciers into the
sea. Sediments deposited at Site 696 contain evidence of coarsegrained (up to 3 cm size) ice-rafted detritus and dropstones in
the cores down to a depth of 570 m.b.s.f. (i.e. core 54R which is
poorly dated as Late Oligocene to early Miocene). To test whether
the finer grained older sediments at Site 696 also contain IRD,
we examined microfeatures of quartz grains in the sand fraction
0.1–0.5 mm. High pressure glacial fracturing and abrasion produces
grains with high degrees of angularity and relief along with diagnostic microfeatures such as gouges, conchoidal fractures and
steps (Mahaney et al., 1996). Although IBRD-derived ice would be
expected to be the main source of clastic material delivered to dis-
Fig. 5. Age depth plot for Site 696 and the position of the studied samples relative to age and an oxygen isotope record for the Southern Ocean from the middle Eocene to
early Oligocene (Scher et al., 2014). EOT = Eocene–Oligocene transition. PrOM = Priabonian oxygen isotope maximum.
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Table 1
Summary of grains scanned for composition. Grain outline is based on Powers (1953) classification.
Core
62R
61R
60R
59R
57R
56R
52R
51R
Section
Depth
Interval (cm)
03W
637.95–645.6
71–76
03W
626.2–635.9
69–84
01W
616.96–616.6
02W
606.9–616.6
30–45
01W
587.6–597.2
25–40
01W
577.9–587.6
129–144
01W
539.4–548.9
19–28
02W
529.8–539.4
50–65
Total grains analysed
Qtz grains
% Qtz in sample
% Plagioclase
% Alkali Feldspars
% Glauconite grains
% Smectite
% Chlorite-illite
29,086
9,934
29.2%
22.6
7.2
6.0
6.4
2.8
14,302
15,181
28.4
21.5
8.6
9.4
5.8
3.5
16,496
12,741
36.2
23.8
12.4
2.0
3.3
3.6
35,179
6,355
38.5
23.6
8.2
0.02
0.9
1.2
53,371
3,451
24.5
12.8
7.0
39.3
1.1
2.4
33,987
8,731
25.7
17.4
7.3
16.2
1.4
2.1
38,447
8,195
21.3
44.2
0.9
2.0
4.5
0.5
54,976
7,445
13.5
58.4
0.8
108
2.9
0.7
Qtz grain shape
% Angular outline
% Rounded outline
75
10
75
7
84
3
55
19
63
22
58
6
37
9
64
10
tal marine locations such as the northern Weddell Sea, there may
also be a contribution from sea ice (sea-ice-rafted debris or SIRD).
Quartz grains carried by sea ice have rounded edges low relief and
chemical features associated with silica dissolution and reprecipitation due to greater levels of chemical weathering (Dunhill, 1998;
St John et al., 2015). From each sample, 20–30 quartz grains were
randomly selected for analysis of surface microtextures under a
Scanning Electron Microscope, and the presence or absence of key
features was recorded (Dunhill, 1998; St John et al., 2015). Further
methodological details are provided in the supplementary material.
4. Results and interpretation
The investigated samples have grain sizes comprising silt and
coarse sand, with the modal grain size being fine sand. Qemscan analysis counted between 14,000 and 55,000 mineral grains
in each sample (Table 1) of which 60–72% of the grains were
quartz and feldspar. The only exception is a sample from core 57R,
which is rich in glauconite. The high (20–59%) feldspar contents in
all samples indicate immature, mechanically produced sediments.
The abundance of feldspar fluctuates across the stratigraphic age
range and is generally mirrored by amounts of smectite and, to a
lesser extent illite–chlorite. Chlorite and illite are both influenced
by strong physical and weak chemical weathering. Smectite is generally linked to weathering of feldspars so some correspondence
is to be expected. Detailed geochemical and clay mineralogical investigations on the Eocene sediments at Site 696 by Robert and
Maillot (1990) have previously shown that most of the sediments
are of detrital origin and that their smectites resemble those typically found in soils formed in (sub-)tropical regions and/or on
parent-rocks of basaltic origin. Some of the smectites revealed features characteristic for an early diagenetic origin, but these were
interpreted to have formed during in situ recrystallization of smectite within the interstitial sedimentary environment and without
any significant chemical or mineralogical change (Robert and Maillot, 1990). The ubiquity (39% of grains) of glauconite in core 57R,
and to a lesser extent (16%) in 56R, supports a shallow-water environment enriched in Fe and K. Quartz and feldspar grain shapes
are mainly angular.
Quartz grain microfeatures from the oldest samples from cores
62R–59R of Site 696 display high relief, angular mechanical features consistent with IBRD, seen clearly by SEM imaging (Fig. S1A).
We also detected some grains with rounded low relief features
consistent with SIRD features (Figs. S1B and S1C) but since some
grains within each sample have microfeatures of both IRD types
we regard the estimated proportions of SIRD or IBRD as indicative only. It is clear though that grains with IBRD features form
the largest population and account for 37–84% of all quartz grains
based on abundances of high relief angular grains that show break-
age blocks, conchoidal and step-like fractures, gouges and striations (Table S2). Some of these grains show edge abrasions, which
may result from glaciomarine current reworking or from transport in the glacial environment (Strand et al., 2003), with currentreworked grains being subrounded to subangular, of medium relief
and having dissolution features. The remaining grains show features consistent with SIRD (sub angular to well rounded, low to
medium relief, high abundance of breakage blocks and microlayering, widespread dissolution features). Some of these grains are
fluvial in origin and could be derived from erosion of exposed parts
of the SOM or by longer distance IRD transport from the coastal
shelf areas bordering the Weddell Sea.
The presence of abundant quartz, feldspar and mica at Site 696
is consistent with continental margin sources and so the simplest
explanation is that during the early rifting stages of the Powell
Basin at c. 40–30 Ma (Eagles and Jokat, 2014) the SOM was still
proximal enough to the Antarctic Peninsula to receive some of its
detritus (Barker et al., 1988), and/or the sediment came from exposed parts of the SOM. Comparison of heavy mineral assemblages
from this study with modern marine sediment samples in the
Weddell Sea region (Diekmann and Kuhn, 1999) points to sources
within East Antarctica (Fig. S2). Garnet is widespread in SOM rocks
but is rare (<0.5%) in the Site 696 samples (Table S5). This difference is also indicated by the fission track and zircon U–Pb data
from South Orkney bedrock.
Apatite fission track (AFT) analyses of bedrock samples from
South Orkney (Table S3) gave reset central ages between 33 Ma
(H.1181.1: biotite schist of the Permian–Triassic Scotia metamorphic complex) and 56 Ma (H.2113.2: Jurassic Powell Island Conglomerate). The latter sample shows overdispersion of grain ages
with a sub-population at 44 ± 3 Ma and a smaller group at
82 ± 1 Ma. Although none of the data yielded sufficient track
lengths for thermal history modelling the youngest ages indicate
onset of cooling from c. 50–30 Ma, which overlaps with the onset of rifting and extension during early opening of Powell Basin
(Eagles and Jokat, 2014). The bedrock AFT data limit the depth of
post 30 Ma denudation to <1.5–2 km since any larger denudation
would normally have produced younger AFT ages unless the exhumation was extremely rapid. By contrast, the detrital AFT ages
from Site 696 are different; core sample 61R revealed a minor population of volcanic apatites with an age of 34 ± 4 Ma and abundant
older grains with mean ages between 140 ± 11 and 292 ± 13 Ma.
Similar age modes were found in samples 56R and 57R (Fig. S3;
Table 2).
The Mesozoic detrital FT ages record the tectono-thermal histories of the apatite source rocks, which are known to vary in
the circum Weddell Sea region. To recover these histories the FT
age and track length data for each age component were modelled
to help locate where the apatites originally came from. Thermal
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Table 2
Summary of detrital apatite fission track age modes at Site 696. Accompanying radial plots can be found in the supplementary data.
the zircon ages are similar to the Late Eocene zircon dates from
Site 696 (Fig. 6).
Sample
No grains
AFT Age group
(Ma)
% of grains
5. Discussion
61R
60
34 ± 4
140 ± 11
292 ± 13
45%
21%
34%
59R
65
89 ± 10
210 ± 10
445 ± 66
12%
75%
13%
57R
60
137 ± 6
291 ± 11
32%
68%
56R
52
120 ± 11
262 ± 11
25%
75%
The detrital zircon U-Pb and apatite thermochronometry data
show that the bulk of the Late Eocene (∼36.5–33.6 Ma) sediments
deposited at ODP Leg 113 Site 696 do not originate from local
sources (Antarctic Peninsula and South Orkney) but instead were
supplied from distal sources. This finding together with the common occurrence of quartz grains with mechanically induced microtextures, which are diagnostic of subglacial erosion and transport,
suggests that most of the detritus was supplied by ice-rafting. The
provenance of these sand grains best matches sources within the
Ellsworth–Whitmore Mountains of West Antarctica and the Weddell Sea coastal region of East Antarctica (Fig. 2). However the
significance of these results and implications for understanding
the development of the early stages of the Antarctic cryosphere
depends on whether they were deposited by directly by melting
icebergs, sea ice or were re-deposited by other processes, such as
gravity or current flows.
Opening of the Weddell Sea and formation of new oceanic
lithosphere initiated in the south at around 147 Ma (Konig and
Jokat, 2006) and the main depocentre has remained there to the
present-day (Huang et al., 2014). Given that continental-scale river
systems drained the Antarctic interior well into the Eocene (Strand
et al., 2003) and delivered sediment through the Filchner-Ronne
rift basin to this depocentre (Jamieson et al., 2014) it is reasonable to consider that sediment deposited on the SOM shelf may
have been re-worked and delivered by long-distance gravity flows
that originated along the southern Weddell Sea margins. Today,
this would require sand to travel over 1200 km, across the abyssal
plains before flowing uphill from water depths >4000 m onto the
SOM shelf that has a water depth of 650 m. Reconstructions of
Weddell Sea paleobathymetry based on the thermal subsidence
history of local ocean crust (Huang et al., 2014) show that a similar depth range existed in the Late Eocene, although the SOM shelf
was shallower, c. 100 m (with an uncertainly of a similar order),
based on benthic foraminifera diagnostic of a neritic, slightly hyposaline inner shelf environment (Wei and Wise, 1990) and the
presence of glauconite. More problematic is that during the Paleogene, to the southwest of the SOM, the Endurance subduction zone
(Fig. 2) would have trapped any sediment transported by flows
from the south.
Given that gravity flows are an unrealistic mode of transport,
the Late Eocene sediments deposited at Site 696 must have been
transported to the SOM by ice. Although quartz grain microfeatures
are mostly consistent with IBRD some 15–45% of the observed
grains show microfeatures consistent with sea-ice transport and/or
a fluvial reworking. Whether sea-ice of any significance existed at
least during the winter months in the late Eocene is unclear although climate modelling studies show it was certainly possible
(DeConto et al., 2007). If (seasonal) sea ice was present because the
Antarctic shelf was still shallow during the Late Eocene (Wilson et
al., 2013) it could have easily picked up and transported beach sediments. Regardless, the key point is that the glacial derived sand
grains were transported to the SOM by ice, mainly by melting icebergs, and that all of the ice sources must have originated in the
southern Weddell Sea because their provenance (zircon U–Pb and
apatite FT ages) does not match the Antarctic Peninsula or South
Orkney.
A number of previous studies have indicated the presence
of glacial ice prior to the EOT oxygen event, e.g. work on the
SHALDRIL cores recovered from the eastern Antarctic Peninsula
shelf (Anderson et al., 2011) and on Late Eocene–Oligocene sediments deposited in a glacio-fluvial environment in Prydz Bay
history modelling of the oldest apatite fission track age component (Fig. S4) show the ages were produced by a Carboniferous cooling event. This rules out the Antarctic Peninsula as a
source since the oldest rapid AFT cooling event from this region
dates to the Late Cretaceous and Early Cenozoic (Barbeau, 2011;
Guenthner et al., 2010). The only known Late Carboniferous event
is in Dronning Maud Land of East Antarctica (Jacobs and Lister,
1999; Meier, 1999; Emmel et al., 2007). The younger FT age mode
in the Site 696 samples relates to an early Cretaceous cooling
event which has been recorded from Antarctic basement rocks
surrounding the Weddell Sea, extending from the Ellsworth Mountains (Fitzgerald and Stump, 1991, 1992) to the Shakleton Ranges
and coastal areas of Dronning Maud Land (Emmel et al., 2007;
Meier, 1999) (Fig. 2).
Detrital zircon U–Pb data also show similar differences. All Late
Eocene samples from Site 696 gave nearly identical age spectra
(Fig. 6). The range of age peaks is dissimilar to data from bedrock
of the South Orkney Islands and Graham Land on the Antarctic Peninsula, most strikingly by the absence of zircons from the
Permian arc (270 Ma peak), which are ubiquitous amongst the
rocks of South Orkney and sedimentary successions of northern
and eastern Graham Land (Barbeau, 2011). The U–Pb ages of the
zircons in the Site 696 samples also reveal Early Cretaceous age
peaks and a significant component of grains between c. 1.0–12 Ga
that are essentially absent in rocks from northern Graham Land
and rare on South Orkney.
To test rigorously the relationship between likely source areas
multidimensional scaling (MDS) (Vermeesch, 2013) was applied to
the zircon U–Pb results and data from areas bordering the entire
Weddell Sea region (Fig. 6), including the shelf of Dronning Maud
Land, Coats Land, the East Antarctic drainage basin of the modern
Filchner Ice Shelf, the Ellsworth Whitmore Mountains, the Antarctic Peninsula, the South Orkney Islands as well as the Magellanes
Basin and the Fuegian Andes, because the SOM was located closer
to South America prior to its separation from Antarctica during
the Eocene (Eagles and Jokat, 2014) (Fig. 3). The MDS map clearly
shows a strong dissimilarity between Site 696 samples and South
America, the Antarctic Peninsula and South Orkney, but a significant similarity to the Ellsworth Whitmore Mountains, drainage
basin of the Filchner Ice Shelf, the shelf regions of Coats Land
and Dronning Maud Land. We also compared Site 696 data with
Pliocene sediments from ODP Leg 113 Site 694 on the Weddell
Sea abyssal plain. The sediments deposited at this location during
the Pliocene are entirely hemipelagic in origin (Kennett and Barker,
1990) and, given the westward directions of the Antarctic Coastal
Current and the Weddell Gyre, must have been sourced from East
Antarctica. We also analysed one middle Oligocene sample (core
14) from Site 693B on the continental margin of the Weddell Sea,
proximal to Coats Land and Dronning Maud Land. In both cases
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Fig. 6. A). Kernel density plots of detrital zircon ages for samples analysed in this study (South Orkney, Site 696) and compiled datasets for potential source regions (see
supplementary data for sources). B). Multidimensional Scaling Maps (Vermeesch, 2013) comparing the age spectra in A. Dissimilar samples (South Orkney, Graham Land,
Fuegian Andes, Vega Island) plot far apart. The cluster of similar samples includes Sites 696 and 694, modern sediments from offshore Dronning Maud and Coats Land, the
hinterland of the modern Filchner Ice Shelf and bedrock ages from the Ellsworth Mountains (for locations see Fig. 2).
(Barron et al., 1991; Cooper and O’Brien, 2004). Also, the geochemical proxy data from middle-late Eocene sediment deposited on
the Kerguelen Plateau found evidence consistent with ephemeral
glaciations in East Antarctica (Scher et al., 2014). These studies assumed that the glacial debris came from nearby sources, or was
reworked. More direct evidence from the work by Galeotti et al.
(2016) on the well-dated CRP-3 drill core at Cape Roberts has revealed evidence of local glacial advance and retreat cycles that date
to between 34–31 Ma. Due to the low recovery at Site 696 sample
our dataset does not have the temporal resolution to detect orbital
scale glacial–interglacial cycles and so cannot demonstrate glacial
ice was permanently present throughout the Late Eocene. The recent study by Galeotti et al. (2016), suggested that until 32.8 Ma
most of the glacial ice disappeared during peak interglacials. But,
significantly, our new data do reveal an older and much wider
distribution of glacial ice in Antarctica than any previous work
has suggested. There must have been significant ice present across
Antarctica in the Late Eocene to enable it to reach low-altitudes
and to calve icebergs along the coastlines of the southern Weddell
Sea by c. 36.5 Ma or slightly earlier.
The iceberg-rafted grains with both East and West Antarctic
provenance provide an unambiguous record for widespread glacial
ice around the Weddell Sea embayment between ∼37 and 34 Ma.
Whether these areas were the precursors for growth of the EAIS
and WAIS is an open question. Most of the Antarctic topography
was established before the Late Eocene (Wilson et al., 2012), and
the glaciers in the mainly inland mountainous areas in the Gamburtsev Mountains, Dronning Maud Land and the Transantarctic
Mountains (Fig. 1) can be expected to have served as the main nuclei for the ice sheets. In simulations of Antarctic ice-sheet growth
under high Palaeogene CO2 concentrations the loci of the largest
nuclei are close to the regions that were the sources for most of
the IBRD-grains found at Site 696 (DeConto et al., 2007). However,
the loci of ice sheet growth in such model simulations can vary
considerably under different precipitation, air and ocean temperature, paleolatitude, lapse rate and sea level boundary conditions
(cf. van Hinsbergen et al., 2015), all of which have serious uncertainties for the Late Eocene.
Although studies have tended to paint a dominant mechanism
as responsible for the onset of glaciation (ocean gateway vs CO2
decline) the relative roles of different mechanisms, and their associated feedbacks are complex and remain poorly resolved because
the initial and boundary conditions are still highly uncertain. Despite improvements there remain considerable uncertainties in relation to the atmospheric CO2 concentrations leading up to the
EOT (Anagnostou et al., 2016) as well as the modelled CO2 threshold for Antarctic glaciation, which are known to be highly modeland model-configuration-dependent (Gasson et al., 2014). Until a
more complete continent-wide inventory of early ice on Antarctica
can be established and modelling approaches adopt more realis-
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tic boundary conditions and a dynamical approach based on an
ensemble of mechanisms, the precise role of atmospheric CO2 concentrations cannot be fully defined.
6. Conclusions
Much emphasis has been placed on climate models to explain
the glaciation of Antarctica during the EOT. Sensitivity modelling
consistently shows CO2 decline was sufficient to drive polar cooling
but the location and extent of early ice has a dependency on model
boundary conditions that are often poorly known and have large
uncertainties. Realistic model predictions must be consistent with
geological observations and in this context the data from this study
are significant as they provide the first evidence for the presence
and continuity of widespread ice in the late Eocene that extended
from the mountainous interiors to the coastal areas fringing the
southern Weddell Sea. We note that paleotemperature reconstructions derived from proxy data (e.g., Douglas et al., 2014) suggest
relatively warm conditions in the Weddell Sea and therefore icebergs in the region may not have survived for long. The apparent
paradox between the reconstructed temperatures and the results
presented in this study, however, can be reconciled, if the full error bars in proxy-based temperature reconstructions for the Late
Eocene are taken into account and/or if the westward currents in
the Weddell Sea during the Late Eocene were of similar vigour to
the present-day. Given that current strength largely depends on local paleogeographic and atmospheric conditions model testing that
includes eddy-resolving simulations will need to adopt a finer scale
than to date to explore the latter explanation.
Acknowledgements
The research used samples provided by the Ocean Drilling Program (ODP) from Leg 113 Site 696. This research did not receive
any specific grant from funding agencies in the public, commercial, or not-for-profit sectors. TRR and CDH are supported by the
Natural Environment Research Council (NERC). We thank Peter Bijl
and two anonymous reviewers for their constructive though critical suggestion.
Appendix A. Supplementary material
Supplementary material related to this article can be found online at http://dx.doi.org/10.1016/j.epsl.2016.10.045.
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