Palaeoclimate records of the Mesozoic and Cenozoic eras display a long-term trend from extremely warm conditions during the mid-Cretaceous optimum to cooler climates of late Palaeogene and Neogene time. The Neogene climate record is reasonably well known on a time scale of c. 50-100 ka resolution or better, based on extensive surveys of benthic and planktonic stable isotope stratigraphies from all the major ocean basins save the Arctic. However, Palaeogene and Cretaceous climates are currently poorly resolved owing to the scarcity of high deposition rate sections and the frequent poor preservation of microfossils upon which various faunal and geochemical climate proxies are based. Consequently, most of our highly resolved records of Cretaceous and Palaeogene climate come from stable isotope analyses of bulk carbonates. The uncertain role of diagenesis in these isotopic data has made it difficult to draw firm conclusions about many aspects of ocean climate and circulation.
To improve the situation
we have combined stable isotope records from Leg 171B sites with previously
published datasets to illustrate long-term trends in 18O
and
13C
for the surface and deep ocean (Fig. 9).
These data include records of planktonic foraminifera that record the most
negative
18O
as well as benthic species to show the vertical
18O
and
13C
gradients in the oceans. Currently, there are insufficient data to determine
which of the features of these isotope records reflect global trends rather than
regional trends for the interval before Campanian time. However, Campanian and
younger trends have been duplicated in a number of localities suggesting that
the basic patterns are of global significance. Trends in mid-Cretaceous records
have been illustrated in several low- to moderate-resolution datasets from both
deep-sea and outcrop sections (e.g. Clarke & Jenkyns 1998; Stoll &
Schrag 2000). Our foraminifer isotopic records broadly mirror patterns in the
bulk sediment stable isotope data. It is likely that parts of the Albian and
Cenomanian records will ultimately be found to differ in amplitude and absolute
values from deep Pacific or Indian Ocean records. The North Atlantic was partly
a silled basin during Albian and Cenomanian time and was part of the Tethys
seaway, suggesting that it may have been filled with intermediate waters or even
surface waters from elsewhere in the world's oceans.
Benthic 18O
in early Albian time was broadly similar to that during the Cretaceous and early
Palaeogene time. However, Atlantic intermediate waters (c. 1500 m water
depth at ODP Site 1049) approached the same
18O
values as planktonic foraminifera during early Albian time. The convergence of
planktonic and benthic
18O
records suggests that the North Atlantic basin was either filled with
overturning surface waters or that the planktonic foraminifera chosen for
analysis grew in subthermocline waters. We think it most likely that the
occasional similarity in deep and surface
18O
reflects variability in the intensity of surface stratification, as the
18O
gradient swings between c. 0.5
and nearly 2
during OAE 1b (c. 112 Ma). Hence, the isotopic data suggest that the
western North Atlantic was probably filled with moderately high-salinity waters
not unlike the modern Mediterranean Basin that were occasionally more strongly
stratified by runoff from the adjacent continents or by inflow of low-salinity
waters from adjacent ocean basins such as the Arctic or the Pacific. Indeed,
tectonic reconstructions show that the North Atlantic could have been
hydrographically restricted from the deep Indo-Pacific by shallow sills across
the Central American Seaway and the myriad of elevated plateaux and tectonic
terranes in the Tethys Seaway (Hay et al. 1999).
Our isotopic data (Erbacher
et al. 2000) suggest that the western North Atlantic behaved like
the Plio-Pleistocene Mediterranean basins. There, the modern vertical
temperature gradient can be as low as 3-4oC and salinities of c.
36 increase
18O
of planktonic and benthic foraminifera by as much as +/- 1
over the open eastern North Atlantic (Miller et al. 1970). The
potential for unusually high salinities in the North Atlantic during early
Albian time makes it difficult to estimate absolute sea surface temperatures
(SST). However, heavy
18O
values from other records (Huber et al. 1995; Clarke & Jenkyns
1999) may suggest that temperatures during early Albian time were lower than
during any other period in the mid-Cretaceous.
We have no foraminifer 18O
data from mid-Albian time. Indeed, a survey of existing DSDP and ODP sites
suggests that mid-Albian time is very poorly represented everywhere in the deep
oceans, or where present, has little calcareous fossil material suitable for
stable isotopic analysis. The situation changed by the late Albian, where
isotopic results from ODP Hole 1052E show that both planktonic and benthic
18O
were nearly the most negative ratios seen in the last 100 Ma. Only around the
Cenomanian-Turonian boundary interval can lighter isotopic values be observed.
The large vertical
18O
gradients between planktonic and benthic foraminifera suggest that by late
Albian time, the North Atlantic had ceased to be an extension of a silled Tethys
Seaway with an estuarine circulation and had developed deeper marine connections
to other deep ocean basins.
Norris & Wilson (1998)
inferred that SST reached at least 30-31oC during late Albian and
earliest Cenomanian time (c. 98-102 Ma) in the western North Atlantic.
These high temperatures were maintained or even raised further during parts of
the Cenomanian. For example, planktonic foraminifera from DSDP 144 (9oN)
in the equatorial western North Atlantic have average 18O
values of -3.9
,
equivalent to temperatures of c. 32-34oC using estimates from
standard palaeotemperature equations, modern salinity, and assumption of an
ice-free world. Notably, benthic
18O
also peaks in upper Cenomanian time, reaching ratios over 1
more negative than that seen at any point in the deep oceans during the
Cenozoic. Intermediate waters may have been unusually warm near the C-T boundary
(Huber et al. 1999). Alternatively, tectonic barriers to exchange
with other ocean basins may have become sufficiently restrictive that the North
Atlantic was filled with thermocline waters or upper intermediate waters flowing
in over shallow sills.
Our data (Huber et al. unpubl.
data) from ODP Site 1050 illustrate that the mid-Cretaceous thermal optimum was
not uniformly warm or stable. A pronounced increase in both planktonic and
benthic 18O
occurred in the mid-Cenomanian during the Rotalipora reicheli Zone (c.
97 Ma). Stoll & Schrag (2000) recorded a similar event in
18O
of bulk limestone and marl in outcrop sections from Spain and Italy. They
suggested on the basis of the magnitude of the event and its abrupt onset, that
it records glaciation and a shift in whole ocean
18O
as a result of ice build-up. A similar event is present in our data from the
middle Cenomanian sequence in ODP 1050 and the
18O
analyses of bulk carbonates from the Indian Ocean (Clarke & Jenkyns 1999)
and Tethys (Stoll & Schrag 2000). Although the widespread occurrence of the
18O
maxima suggests a global shift in
18O
, such as that produced by ice volume changes, intermediate water
palaeotemperatures at this site and in the southern South Atlantic (Huber et al.
1995) were none the less higher (>11oC) than would be expected if
there were a significant volume of polar ice unless the North and South Atlantic
basins were isolated from high-latitude sources of deep water.
The possible existence of
large ice volume changes during the peak of mid-Cretaceous warmth raises
questions about mechanisms that regulate ice growth and decay. Huber et al.
(1995) showed that latitudinal thermal gradients were unusually low during
intervals of the mid-Cretaceous thermal optimum. Therefore, it is hard to
understand how ice growth could begin when high-latitude SSTs were nearly as
high as equatorial temperatures. The abrupt 18O
swings in Cenomanian time suggest that there may be threshold effects that can
dramatically alter ocean circulation and temperature at the warm end of the
climate spectrum, in much the same way that feedback systems such as moisture
balance and runoff operate to abruptly change boundary conditions in Pleistocene
time at the cool end of the climate spectrum.
We have limited stable
isotope data for foraminifera from late Turonian to mid-Campanian time, an
interval of c. 15 Ma. Data are contradictory for this interval. Huber et
al. (1995) showed that DSDP Site 511 in the South Atlantic was bathed with warm
waters from Cenomanian to Coniacian time and SST did not begin to fall
appreciably until early Campanian time. Barrera (1994) presented a handful of
measurements from North Pacific DSDP sites that also suggest peak temperatures
were maintained until some time in the Santonian period. However, 18O
data of bulk carbonates from Indian Ocean DSDP sites (Clarke & Jenkyns 1999)
suggest that the decline in temperatures occurred during late Turonian time. The
planktonic foraminifera show a tendency towards heavier isotopic values during
the course of the Turonian as suggested by the dataset from ODP Site 1050 (Huber
et al. unpubl. data), although some extreme light isotopic values can
still be seen. Results from Site 1050 suggest that planktonic
18O
was similar to or more positive than that in late Campanian time and suggest
that the surface waters were significantly cooling during Turonian time,
although highly variable. One could conclude from the planktonic isotope record
that the mid-Cretaceous climatic optimum was over by c. 90 Ma if not
earlier, although the benthic isotope data show that a persistent fall towards
heavier values occurred in Campanian time. More benthic isotope data are needed
to document the exact timing of the end of the mid-Cretaceous climatic optimum.
Barrera & Savin (1999)
published Campanian and Maastrichtian data for planktonic and benthic 18O
from a number of sites around the world. Most records show the long-term trend
to more positive
18O
in both surface and deep waters and an abrupt step in this trend about 71 Ma.
Miller et al. (1999) interpreted the step increase in foraminifer
18O
to reflect an increase in ice volume and glacioeustatic sea-level lowering.
MacLeod & Huber (this volume) have shown that the positive
18O
deflection in benthic foraminifera is not nearly so pronounced in benthic
records from the North Atlantic. Their data suggest either that the
18O
shift observed elsewhere is not a glacial step or that the North Atlantic record
is biased by the introduction of an unusually warm deep water mass that
overprints the glacial increase in
18O.
Notably, the size of the mid-Maastrichtian increase in
18O
in planktonic foraminifera is about a third to half the amplitude of the change
in benthic foraminifera even in the Pacific. Therefore, it seems likely that at
least half of the mid-Maastrichtian
18O
shift is due to cooling or an increase in salinity of deep waters.
The Cretaceous-Palaeogene
(K-P) boundary is preceded by a rise in global ocean 13C
and bottom-water temperatures starting in mid-Maastrichtian time (c.
71-72 Ma) that culminates in early Danian time (Fig.
9). The overall rise in benthic
13C
and deep-water temperatures probably reflects carbon burial and CO2
sequestration (Zachos et al. 1989; Stott & Kennett 1990). Sea-level
fall may have played a role in carbon burial through the formation of large coal
swamps with the retreat of epicontinental seas in late Maastrichtian time. The
deep-sea
13C
record is also influenced by a general decrease in inter-basin
13C
gradients near the end of Maastrichtian time that reduced the isotopic contrast
between relatively young deep waters in the North Atlantic and relatively old
deep waters in the Pacific and Indian Ocean (e.g. Corfield & Norris 1996,
1998; Barrera & Savin 1999). Frank & Arthur (1999) explained the
reduction of interbasinal
13C
gradients by suggesting that the opening of deep passages between the North and
South Atlantic played a key role in ventilating the deep North Atlantic during
mid-Maastrichtian time. None the less, the North Atlantic continued to maintain
a distinctive young deep and intermediate water-mass through the mid-Palaeocene
(Corfield & Norris 1996, 1998).
Bottom temperatures stayed
the same or rose from mid-Maastrichtian time to the K-P boundary, whereas
surface water temperatures fell until the last 200 ka of the Cretaceous period.
The general decline in SST may be related to the withdrawal of epicontinental
seas (Frank & Arthur 1999) or to the sequestration of carbon and CO2
during the rise in global 13C
in late Maastrichtian time. The deep North Atlantic and deep waters elsewhere in
the oceans display distinctly different
18O
throughout late Maastrichtian time. The North Atlantic was consistently c.
2oC warmer or less saline than the other deep basins, a contrast that
was maintained through early Palaeocene time (e.g. Corfield & Norris 1996).
Relatively high deep-water temperatures in the North Atlantic may reflect the
presence of young deep waters conditioned by overflow from Tethyan basins much
like the conditioning of modern North Atlantic deep water by Mediterranean
outflow waters.
The early Danian period
(64-65 Ma) is best known as a time of tremendous turnover in marine pelagic
ecosystems following the Cretaceous-Palaeogene mass extinction (D'Hondt &
Keller 1991; Gerstel et al. 1987; Jablonski & Raup 1995; Keller 1988;
MacLeod 1993; Olsson et al. 1992; Smit 1982). The extinction eliminated c.
95 % of planktonic foraminifer species and had a profound effect on other
members of the plankton. The extent of the devastation of the pelagic ecosystem
is reflected by the extended (c. 3 Ma) collapse of the carbon pump and
the vertical 13C
gradient in the oceans (e.g. D'Hondt et al. 1998).
The recovery was also
associated with large-scale changes in marine climate and carbon-cycle dynamics.
There is a general decrease in global ocean 13C
that may reflect reduced productivity and carbon burial (Shackleton & Hall
1984). In addition, the vertical
18O
gradient was greatly reduced for an interval of almost 3 Ma in early Danian time
coincident with the reduction in the vertical
13C
gradient. The declines in vertical
18O
and
13C
gradients are both likely to be partly related to reorganization of biotic
communities brought on by the end-Cretaceous mass extinction. A reduction in the
vertical
18O
gradient is perhaps best explained by the widespread extinction of
surface-dwelling species of planktonic foraminifera during the K-P mass
extinction and a tendency for palaeoceanographers to analyse species that grew
mostly in thermocline waters during early Danian time.
At the K-P boundary, the
mass extinction resulted in a dramatic 1
decrease in surface ocean
13C
with little or no change in deep-water
13C.
The absence of any large negative shift in
13C
of deep waters strongly suggests that changes in the vertical
13C
gradient are due to the extinction of surface ocean biota rather than a change
in the global
13C
reservoir (Hsü et al. 1982; Zachos & Arthur 1986; Zachos et al. 1989;
D'Hondt et al. 1998). Some records show an inversion of the
surface-to-deep
13C
gradient (Hsü & McKenzie 1985; Zachos & Arthur 1986) that has been
attributed to biomass burning (Ivany & Salawitch 1993) but could also
reflect measurement artifacts due to low carbonate content in the boundary
interval (e.g. Shackleton 1986).
Following the collapse of
planktonic and benthic 13C
gradients during the mass extinction, global
13C
continues to rise. Maximum benthic
13C
of c. 2.2
is recorded less than 100 ka above the K-P boundary and is succeeded by a
long-term decline in
13C
over the next 4 Ma. Hence, it appears that the process of carbon burial that led
to the Maastrichtian rise in benthic
13C
was reversed just after the K-P mass extinction and set in motion a long-term
interval of unroofing previously deposited carbon. We suggest that the change
from net carbon burial to net erosion may reflect the final draining of
epicontinental seas and the onset of weathering of coal and organic shales
deposited during late Cretaceous time. By the end of the Danian (c. 61
Ma) benthic
13C
had returned to a ratio very similar to that achieved in mid-Maastrichtian and
late Albian time, and very close to that later reached during the early Eocene.
One of the most striking
features of the early Cenozoic and Cretaceous stable isotope records is the
dramatic positive shift in 13C
of both planktonic and benthic foraminifera in late Palaeocene time. Benthic
foraminifer
13C
increased by c. 2
and planktonic foraminifer
13C
increased by c. 3
between 61 and 58 Ma. Part of the increase in
13C
of planktonic foraminifera is probably due to the re-evolution of photosymbiosis
after the K-P mass extinction (e.g. Corfield & Norris 1998). However, the
increase in
13C
of benthic species is seen throughout the oceans (e.g Miller et al. 1987;
Corfield & Cartlidge 1992), suggesting that it represents a reservoir effect
of burying large quantities of organic carbon. It is not at all clear where all
this carbon was deposited, as there are few large oil or coal reservoirs of late
Palaeocene age. The relatively rapid decline of
13C
of both benthic and planktonic foraminifera between 58 and 55 Ma suggests that
much of the carbon buried during Palaeocene time was exhumed by the end of the
Palaeocene epoch. Beck et al. (1998) have suggested that much of the carbon
deposited during late Palaeocene time may have accumulated in Tethyan basins
that were subsequently uplifted and eroded during the initial stages of the
Himalayan Orogeny.
The peak of the Palaeocene
13C
increase coincides with the most positive benthic foraminiferal
18O
ratios in the Palaeogene period. A modest increase in
18O
of planktonic foraminifera is also present, suggesting cooling of both surface
and deep waters during the late Palaeocene 'carbon isotope maximum'. We
speculate that CO2 drawdown associated with organic carbon burial may have been
responsible for the fall in ocean temperatures. Evidence for snowmelt and cool
interior climates in the Rocky Mountains (e.g. Dettman & Lohmann 2000) as
well as palaeobotanical estimates of mean annual temperature (e.g. Wing 1998)
suggest that cooling in late Palaeocene time occurred over the continental
interiors as well as the oceans. The late Palaeocene cool phase was succeeded by
a c. 3 Ma interval of increasingly warm conditions leading up to the Late
Palaeocene Thermal Maximum (LPTM) at c. 55 Ma.
The LPTM occurred at the
point where deep-water temperatures and SST had nearly reached the highest
levels in Cenozoic time. Zachos & Dickens (1999) and Katz et al. (1999)
have proposed that the LPTM occurred because deep-water temperatures exceeded a
threshold level above which methane hydrates began to catastrophically
destabilize and contribute to a runaway greenhouse effect. However, Bains et al.
(1999) pointed out that the long-term warming trend in latest Palaeocene time is
highly aliased and that detailed 18O
records from both foraminifera and fine fraction carbonate display no
significant warming trend for at least 200 ka before the LPTM. Hence, it is
unclear whether the million-year scale drift to higher temperatures has anything
to do with the LPTM. Other proposed mechanisms to initiate the LPTM include
changes in deep-water circulation inspired by tectonics (Beck et al. 1998),
volcanism (Eldholm & Thomas, 1993; Bralower et al. 1997b) or slope
failure (Bains et al. 1999; Norris & Röhl 1999).
Dickens (1999) suggested
that sedimentary carbon reservoirs act as 'capacitors' in the global carbon
cycle that store and release greenhouse gases to modulate global climate. This
theory supposes that methane dissociation events, as proposed for the LPTM, are
common in the geological record (Dickens 2000b). Indeed, the example of
the LPTM has spawned a resurgence of interest in the Cretaceous and Palaeogene
climate record and has led to the discovery of other large perturbations in the
carbon cycle. Large negative 13C
anomalies have been identified with the onset of several Oceanic Anoxic Events (OAEs)
in Cretaceous time (Jenkyns 1995; Wilson et al. 1999). Likewise, analysis of
benthic foraminifer assemblages and isotopic anomalies provides strong hints
that there may be other events like the LPTM in late early Eocene and mid-Palaeocene
time (Thomas & Zachos 1999). Short, but intense,
13C
anomalies are of great interest as 'natural experiments' in the biological and
climatological effects of transient perturbations of the carbon cycle. The
increasing evidence that there may be several LPTM-like events offers the
exciting opportunity to compare and contrast these events to better evaluate the
palaeoceanographic context, trigger, duration and biological effect of
large-magnitude changes in carbon reservoirs of whatever cause. There is also
the possibility that some of the
13C
events represent large emissions of greenhouse gases and can provide natural
analogues for modern greenhouse warming.
The early Eocene benthic 18O
record shows that the Earth was essentially warmer than today. That is to say,
the high-latitude oceans were much warmer than today, raising the global mean
temperature (e.g. Zachos et al. 1994), and the Earth was characterized by
the absence of large ice sheets. None the less, maximum sea surface temperatures
in the tropics were not necessarily higher than modern temperatures. Most
planktonic isotope records show that low-latitude early Eocene sea surface
temperatures were lower than at present (Boersma et al. 1987; Zachos et
al. 1994; Bralower et al. 1995). This is not well understood. Either heat
diffused into the deep ocean or the stable isotope records of the planktonic
foraminifera do not record the surface, or have been affected by diagenesis.
Wade et al. (this volume) have shown that massive upwelling in late mid-Eocene
time influenced low-latitude sea surface temperatures. Upwelling at Milankovitch
periodicities may explain why sea surface temperature estimates were low in the
low latitudes. Towards mid-Eocene time increases in
18O
can be seen in both the planktonic and benthic foraminiferal records. These
trends indicate cooling of the Earth (Kennett & Shackleton 1976) starting
near the early Eocene-mid-Eocene transition and continuing in a series of steps
to the Eocene-Oligocene boundary.