12.1 Elementary Considerations and Leitmotif
12.1.1 Cooling: The Leitmotif of the Tertiary
Our planet has plenty of ice in high
latitudes (Fig. 12.1). In fact, the central theme of climatic
evolution in the Cenozoic
(the time after the demise of ammonites and dinosaurs) is an
overall cooling (starting with the Eocene and culminating in the
northern ice ages) and an associated overall drop of sea level
(making ice on land takes water; sea ice does not change sea level:
the water stays in the ocean). Sea ice, like land ice, does affect
albedo, though, by providing a base for snow.

Fig.
12.1
Ice in high latitudes. Left: broken off shelf ice off the
Antarctic continent (Gerlache Strait); right: iceberg calved from a mountain
glacier with tidal termination in a fjord in eastern Greenland
(Photos W.H.B.)
The overall cooling trend has been
known for some time from the study of fossils on land. It is
reflected in the evolution of animals and plants whose offspring
exists today. Modern evidence comes from oxygen isotopes of benthic
foraminifers in deep-sea sediments recovered by drilling (Fig. 3 in
Preface). It has become general knowledge, along with an
appreciation for increased climate variation with ice buildup.
Cooling occurred largely in steps, presumably a reflection mainly
of sudden and large changes in albedo whenever snow fields or sea
ice underwent notable change in extent, invading new areas (Fig.
1.7).
Changes in ocean productivity in the
Cenozoic presumably resulted from intensification of the wind along
with a change in the nature of the thermocline. The thermocline,
the boundary between warm and cold water, became shallower and
better defined as the cold water layer at depth grew thicker. A
shallow and distinct thermocline means decreased productivity over
large oceanic areas, with low nutrient content in surface waters.
In contrast, coastal ocean productivity increased noticeably in the
Neogene, especially the late Miocene. There was an increase in the
range of productivity, with large areas becoming deserts and
opposite extremes focused within upwelling regions. The result of a
strong and shallow thermocline presumably is an enhanced depth
stratification of plankton, a development noted in sediments since
the beginning of the Neogene right after the somewhat chaotic
Oligocene.
12.1.2 Thermocline and Diversity: Problem Corollaries of a General Cooling
Strengthened winds (polar ice increases
the temperature gradients that drive winds) presumably increase
upwelling, which (it is thought) lowers diversity locally. Thus,
while we can be sure that there is a relationship between an
overall cooling and a change in diversity of plankton and other
organisms, we have problems specifying details on a regional level.
The available information is not unambiguous, with the desert
specialists (the nannofossils) having an evolutionary trajectory
quite different from those of diatoms and foraminifers. In both of
these forms, abundance and diversity seem to increase during the
Cenozoic, a statement not applicable to nannofossils and to
radiolarians (Fig. 12.2).

Fig.
12.2
The plankton organism diatoms and
foraminifers show a strong increase in diversity within the
Cenozoic, along with increased abundance. Nannofossils and
radiolarians (likewise shelled plankton) do not show those trends
(H.R. Thierstein et al., 1988. In: G.B. Munsch (ed.) Report of the
Second Conference on Scientific Ocean Drilling COSOD II. European
Science Foundation, Strasbourg; color here added)
12.1.3 Evidence from Oxygen Isotopes
Evidence for the great cooling trend in
deep-sea sediments was first provided by the oxygen isotopes in
benthic foraminifers sampled by deep-sea drilling (Fig.
12.3). The
relevant graph by Ken Miller (Rutgers University) and associates
(published in 1987) has been referred to hundreds of times. A
similar compilation by J. Zachos and associates (global, rather
than Atlantic focused; published in 2001) shows that the major
features recognized in the Atlantic by Miller et al. are in fact
global in nature. Both compilations show two remarkable ramps of
cooling lasting for more than 10 million years – one in the Eocene
and the other within the Miocene. In each case, at the end of the
gradual cooling, there is a striking acceleration, as though the
cooling reached a critical level resulting in vast ice buildup and
albedo change (positive feedback). We might guess that an
end-of-Eocene ice buildup took place rather readily on Antarctica,
as the place where one of the poles is located centrally on an
enormous continent with cold winters during the dark season. The
continental ice buildup of the late Neogene, around the Arctic Sea,
may be considered a lot more difficult and hesitant; the solid base
for land ice is being removed from the pole. A mid-Miocene ice
buildup is commonly assigned to Antarctica, the IRD (ice-rafted
debris) in northern latitudes being as yet rare or missing at the
time.

Fig.
12.3
The Cenozoic temperature history as seen in
oxygen isotopes of benthic foraminifers in material recovered by
deep-sea drilling. Modified after K. Miller, R.G. Fairbanks, and
G.S. Mountain, 1987. [Paleoceanography 2: 1] (Compare Fig. 3;
colored band: generalized distribution of data point scatter)
AFS Auversian facies shift:
drastic change in shelf sedimentation in the latest Eocene,
PETM Paleocene–Eocene
Temperature Maximum, presumably linked to sudden methane release.
Blue color: ice present on
the planet; red color,
planet ice-free
The essential trends and steps within
the general trends were worked out soon after the Deep-Sea Drilling
Project started, by two teams combining the skills of paleontology
and isotopic geochemistry. The pioneers were the US geologists R.
Douglas and S. Savin and the NZ-US geologist J. Kennett with the
British geophysicist and geochemist N. Shackleton (later Sir
Nicholas). Their observations showed that cooling was especially
vigorous in high latitudes, being obvious in benthic species
(bathed by high-latitude bottom water) and in planktonic species
from the subantarctic realm. Also, their data indicated that the
cooling occurred in a few major steps, suggesting the operation of
nonlinear feedback mechanisms (i.e., the uneven response to forcing
and the action of positive feedback are indicated, such as expected
when freezing is involved).
12.1.4 Evidence from Strontium Isotope Stratigraphy
An important aspect of the overall
cooling trend, and one that touches on the search for causes of the
cooling, is the stratigraphy of strontium isotopes. Chemically,
strontium is an element homologous to calcium, that is, it acts
somewhat like calcium and is present in calcium carbonate,
therefore (even if not very abundantly). This means it can be found
in calcareous fossils, whether they are remains of benthic
organisms or pelagic ones, shallow or deep. The ratio between the
isotopes 87Sr and 86Sr (both less than 10% of
naturally occurring Sr) reflects (among other items) changes in the
sources supplying strontium to the sea. The common sources are
erosion of continents (i.e., river input) and supply from volcanic
emissions. The long-term trend in the ratio shows a steadily
increasing influence of continental erosion relative to volcanic
activity, as expected for cooling (Fig. 12.4). The trend
distinctly accelerated about 40 million years ago and again 16
million years ago. Erosion of continents, of course, is tied to
uplift and regression (water-covered continents are not eroded).
But there is evidence that volcanic activity changed also
throughout the Cenozoic, complicating the interpretation of shifts
in the strontium isotope ratios.

Fig.
12.4
Cenozoic stratigraphy of the
Sr87/Sr86 ratio. The curve of the “input
ratio” assumes a linear mixing of endpoint Sr isotope values and a
4 million year residence time (W.H.B. and G. Wefer, 1996, modified.
In: G. Wefer et al. (eds.), the South Atlantic. Springer, Berlin
and Heidelberg. Target data from (H. Elderfield, 1986.
Palaeogeogr., Palaeoclimat., Palaeoecol.,57)) AFS Auversian facies shift, a drastic
change in marine sediment types. ME Monterey Event, major shift in
nutrient distribution and increase in coastal upwelling
When focusing on cooling, a change in
volcanism is not helpful: It potentially produces a change in
ratios of Sr isotopes that is independent of cooling.
(“Potentially” independent because ice buildup results in “loading”
of continental crust which presumably stimulates volcanic activity,
which would have opposed any evidence for increased erosion of
continental crust.) As far as the observed trend, it pretty much is
as expected for cooling. It accelerates from the end of the Eocene
to about 16 Ma, an interesting period when the overall tendency of
cooling may have given way to signals from increased volcanism
(J.P. Kennett published Neogene DSDP ash layer abundances in 1982,
p.384). The overall trend expected from cooling then starts up
again at about 7 Ma, a time of major uplift in the Asian highlands
(Tibet) and a volcanically relatively quiet period. Sea level
apparently dropped low enough to help isolate the Mediterranean
from the world ocean. (Thus, cooling pulses may have been an
important cause for a repeated drying up of that sea at the end of
the Miocene.) Toward the end of the Neogene, some 4 million years
ago, there are indications of major volcanic activity again in DSDP
cores.
The apparent
long-term increase in weathering of continental crust suggests a
long-term geological trend in the reduction of carbon dioxide, by
the Urey mechanism
(=absorption of the carbon in carbon dioxide into carbonate when
weathering calcium-rich silicates). To this mechanism, we must add
burial of organic carbon when considering the abundance of carbon
dioxide. The removal of carbon dioxide from the atmosphere
engenders cooling, according to atmospheric physics. The direct
effect can be measured, but the total effect on climate change is
difficult to assess, because of various feedback processes. The
least understood of these feedbacks involves cloud formation, which
has important implications for the evolution of planetary
albedo.
12.2 Reconstruction of Conditions in the “Tertiary” (or Cenozoic)
12.2.1 On the Crucial Role of Deep Ocean Drilling and Biostratigraphy
Deep-ocean drilling (Fig. 12.5), beginning with the
Deep-Sea Drilling Project (DSDP, Glomar Challenger) and continued with
ODP (and a new vessel, dubbed JOIDES Resolution), profoundly changed
the understanding of geologic history for the last 100 million
years. The grand steps of cooling in the Cenozoic and the anaerobic
periods in the Cretaceous were among the most stupendous findings
of scientific deep-ocean drilling. The steps were a surprise for
most geologists, as was the fact that the cooling is mainly a
high-latitude phenomenon. These were, however, only two of several
major discoveries based on using the technology of drilling, a
technology borrowed from the oil industry and adapted for academic
use.

Fig.
12.5
Retrieving information on Cenozoic history
from the seafloor. The chief source of information is drilling from
a vessel (here: the JOIDES Resolution is a vessel originally used
by BP in commercial drilling and greatly modified for scientific
drilling) (Source: ODP
Ocean Drilling Program, College Station, Texas)
Without assignment of ages and
environmental interpretation after inspection of microfossils and
nannofossils, the available information would not have yielded the
relevant insights: To some degree, the fossils (Figs. 4.7 and 12.6) allow keeping track
of the changing environment, thanks to evolution, that is, thanks
to the fact that they are the remains of organisms adapted to their
habitat. Much more reliably, however, they allow assignment of
geologic ages because they differ from one period to the next. Age
control is greatly refined and turned into absolute age numbers,
using correlations into radioactively dated land sections,
correlated with sediments on the seafloor based on magnetic
reversal stratigraphy and to some extent on isotope stratigraphy,
that is, changes in physical and chemical changes in sediment
properties, providing probable ages for biological changes
observed.

Fig.
12.6
The great change at the end of the Eocene.
As sea level dropped, many benthic shallow-water foraminifers
(Girona, Photo W.H.B.) went extinct. Left: nannofossils (examples retrieved
during Leg 1 of DSDP, J.D. Bukry and M.N. Bramlette, 1969)
The major cooling steps identified
tend to be associated with major changes in both the marine flora
and fauna. A very big change was at the end of the Eocene (Fig.
12.6). There
was a general dying off of ancient benthic species, as the water
became too cold for them (or else shallow-water forms on shelves
found themselves without any water). Planktonic species also
suffered: a rich Eocene flora and fauna disappeared, and a rather
dull Oligocene one appeared, with comparatively little diversity.
At times, in the Oligocene, there were enormous blooms of
Braarudosphaera, a
nannoplankton genus. It is a form now mainly found in stressful
conditions in shallow water. The deposits of these strange blooms
have long been a source of puzzlement to geologists.
One possible response to questions
arising with regard to the Oligocene blooms is to invoke vertical
water column instability in the Oligocene (which is bad for
phytoplankton production). Well-developed stratification may have
developed only sporadically, thus favoring the blooming of
stress-indicator species. There is an interesting message in the
Oligocene blooms: (1) Biostratigraphy may routinely reflect strange
events and (2) the biostratigraphy of ancient deep-sea sediments
may reflect times of unusual production, rather than recording
regular conditions. While the resulting sequences might not affect
dating, they might render questionable the reconstruction of
“typical” past conditions.
12.2.2 On the Origin of Cooling Steps
The cooling steps are commonly
referred to as products of ice-related feedback (calling on albedo
changes from the spreading of snow and ice). If the assumption is
correct, then an important aspect of albedo feedback is the
associated sea-level change. Sea-level change is a complicated
issue (see Chap. 6). It may respond to tectonic
forcing without any involvement of ice, making interpretations
difficult. In any case, however, cooling steps tend to be
associated with a drop in sea level. Even modest changes in this
level have potentially large effects because much land is close in
elevation to the level of the sea (Fig. 2.1). Whenever sea level stands
high, sediments are trapped in great expanses of shelf seas, and
the deep sea receives relatively less sediment. When sea-level
stands are low, the reverse is true. The same pattern holds for
carbonate rocks: A high sea level results in buildup of limestones
on the continents; a low sea level moves carbonate to the deep sea,
where it accumulates as shell sand and – silt replete – with
plankton fossils. Changes in ocean productivity, though, can
greatly complicate the pattern observed.
When correlating the cooling steps
into land sections, we tend to find evidence for mountain building.
In answer to the question “whence the stepwise cooling,” the
suggestion comes up, therefore, that mountain building and loss of
shelves are to blame (Fig. 12.7). As with ice-driven changes, albedo is
part of the story. Shelf sediments are commonly light colored; the
sea is not. In addition, the wearing down of the mountains removes
the greenhouse gas carbon dioxide from the atmosphere. One might
expect, as well, that less water vapor (a powerful greenhouse gas)
is delivered by a sea that has lost its shelves. The cooling itself
then develops its own dynamics: A cold ocean takes up carbon
dioxide, for example, diminishing carbon in the atmosphere (and
presumably in other reservoirs communicating with the ocean and the
atmosphere).

Fig.
12.7
Sketch of the connection between mountain
building and sea-level drop, exemplified by the uplift of the Tibet
and the Himalayas in the Cenozoic. Not to scale for the various
geologic elements involved. Note the partial subduction of the
Indian subcontinent
Carbon burial in upwelling regions is
another aspect of those internal dynamics, a phenomenon especially
important in the Neogene with its striking history of changes in
upwelling and increased burial of land-derived sediments, some
presumably replete with organic matter, as well. In addition to
minding evidence for the uplift of the Himalayas (Fig. 12.7), then, we must
contemplate the masses of erosion products in the Bay of Bengal and
elsewhere (and the composition of those masses) when discussing
global cooling.
The high-latitude cooling indicated in
the oxygen isotope trends shows two major steps in the last 50
million years before the last one that is associated with the start
of northern ice ages (Fig. 12.3). The first one roughly coincides with the
AFS and the collision of the Indian subcontinent with Asia, a
collision that initiated the closure of the ancient tropical seaway
“Tethys.” The AFS is near the end of the Eocene and thus was
preceded by millions of years of cooling (presumably related to
mountain building and attendant erosion). The second large cooling
step is in the middle Miocene, associated with a fundamental change
in deep-sea sedimentation and preceded by evidence for carbon
dioxide drawdown (signaling involvement of the carbon cycle).
We do not know why the steps occurred
and exactly when they did. Perhaps we see the effect of reaching a
critical threshold along a trend. Or perhaps, the physical
geography changed at that very time, barring or opening certain
ocean passages and thus redirecting the heat carried by ocean
currents and the nutrients they transfer (Fig. 12.8). Of course, the two
types of possible causes – internal feedback and change of
geography – are not mutually exclusive. We know that both
are at work. The question is how important they are in each given
situation.

Fig.
12.8
Sketch of geography of the middle Eocene
(ca. 45 Ma) and critical valve points for ocean circulation.
Tropical valves are closing (black
rectangles, Tethys); high-latitude valves are opening
throughout the Cenozoic (white
rectangles) (After B.U. Haq, 1981. Ocean. Acta 4, Suppl.:
71, with some minor modifications)
The time when summer snow could first
stay on the ground after sufficient cooling (first on Antarctica
and then on continents surrounding the Arctic) must have been
crucially important. Similarly the appearance and varying extent of
sea ice carrying a snow cover must have provided significant
positive albedo feedback to cooling (note the full reversibility of
this positive snow feedback). Details in the timing may have been
influenced by the sequence of closing gateways in the Tethys and
opening gateways in the Southern Ocean. Without these changes in
geography, ice ages presumably would have come anyway, thanks to
mountain building. However, they might have come at somewhat
different times and with different dynamics.
12.2.3 On Opening the Drake Passage
One way of looking at the problem of
where in time a step should be placed is to note the signs of a
corresponding large reorganization of the ocean’s geochemistry (and
hence planetary climate). According to strontium stratigraphy, one
such reorganization took place around 40 Ma close to the end of the
Eocene (labeled “AFS” in Fig. 12.4, for “Auversian facies shift.”) The
“Auversian” is an obsolete technical term for a time span in the
late Eocene, defined in the region of Auvergne in France. In
Auversian time (in modern terms, Bartonian-Priabonian time), the
deposition of calcareous sediments in the deep ocean greatly
increased, a phenomenon usually referred to as a drastic drop in
the CCD at the end of the Eocene. Also, from the Oligocene on the
types of deep-sea sediments were rather strictly segregated, with
Murray-type carbonate ooze accumulating on the elevated parts of
the deep-sea floor, and siliceous sediments rich in the remains of
diatoms and radiolarians restricted to zones of upwelling. It is
equally possible, of course, that the main change occurred at the
end of the Oligocene. The fact that some time is needed for the
Drake Passage to become highly effective (through deepening)
suggests the Paleogene-Neogene boundary as the correct choice for
the event defining an oceanographically effective passage between
the Patagonia and the Palmer Peninsula.
The drop in the
CCD may signify that the shelves around the ancient tropical seaway
called “Tethys” ceased to
function as efficient shallow-water carbonate traps. There must be
a reason why the epoch following the Eocene, the Oligocene, was not
recognized by the perceptive land geologists studying ancient shelf
deposits for many years after the Eocene had been identified and
named. One candidate reason is a scarcity of shelf carbonate or
shelf rocks in general. In addition, the deep ocean may have
experienced depletion of silicate after the AFS, as a result of
upwelling, and the attendant explosion of diatoms. The result might
have been a disappearance of large siliceous sponges from shelf
seas.
If we place the opening of the Drake
Passage (a rather poorly known event from the point of view of
plate tectonics) at the end of the Eocene, we may choose the
beginnings of a long-term process. In fact, the effective opening
of the passage is a matter of controversy and learned discussion.
Today the Drake Passage is responsible for the major mixing in the
sea in high Southern latitudes and for the existence of the largest
of all currents there, the one circling Antarctica, flowing from
west to east (formally, the “Antarctic Circumpolar Current”). The
appearance of the current may have been rather sudden (as far as
geologic history), but simple geologic reasoning suggests that
there must have been at least one element favoring gradualism: a
gradual deepening and widening of the tectonically opening Drake
Passage. In fact, the response of benthic foraminifers, displaying
gradual turnover of species uncomfortable in the cooling bottom
water of the late Eocene into the early Oligocene, may well reflect
the expected gradual trend linked to the deepening of Drake Passage
after opening.
12.2.4 A Matter of Time Scale
Moving from one time scale to another
can be confusing. There are really three such scales that need to
be considered: First, the human scale, which includes decades and
even centuries, that is, personal career changes, for example, and
grandchildren. Also, the “Renaissance” (a period in human history)
belongs into this scale. The second important scale is the
intermediate one, which is focused on one to several millennia and
includes the mixing time of the ocean and (at the long end) ice
ages and Milankovitch Theory and radiocarbon dating. The third
scale is the very long geological time scale, measured in units of
a million years. As we go back in time to exemplify processes, we
are likely to encounter geological time. There is one great
exception: Impact time presumably is very short (Chap. 13). Many of the “official”
boundaries defining epochs presumably are linked to impacts large
and small (This is a matter of discussion among experts).
The Drake Passage and the associated
Circumpolar Current are features that belong to all scales, but the
source of silicate for upwelling may be seen differently, depending
on the time scale employed. On the geologic scale, the current
maintains a reasonably high value of the nutrient in the ocean,
feeding high-production systems. On the human scale (the one at
issue in much of the climatology and oceanography of global
warming), the complicated network of subsurface currents carrying
nutrients is at focus in the attempt to understand productivity.
Human-relevant information from marine geology is being contributed
on the intermediate and the short scales, not so much on the long
scale.
Thus, the actual histories of the
Cretaceous and the Cenozoic are of great interest when
reconstructing marine resources, but as far as analogs have very
limited application to some of the major problems facing humankind.
The study of history, however, is bound to increase understanding
of processes relevant to those major problems, as mentioned.
In many cases, we become aware of
“tipping points,” situations of reaching critical levels along a
trend. For example, at some crucial level of sea-level drop (e.g.,
from mountain building), shelf seas can no longer serve as
carbonate repositories. Instead, karst-making begins, which implies
delivery of carbonate from the shelves to the ocean, for deposition
at depth. (The dissolution of shallow-water carbonates on an
exposed shelf produces a landscape called “karst.”) The shortage of
silicate in the world ocean (chert becoming less abundant) suggests
that wind-driven upwelling starts vigorously, presumably around
Antarctica, robbing the rest of the sea floor of opaline deposits.
A corresponding shift in sediment types into siliceous ooze and mud
around Antarctica is seen in deep-sea sediments of late Paleogene
to the early Neogene age (Fig. 12.9).

Fig.
12.9
Pattern of increasing IRD and of diatom
deposition around Antarctica, as an indicator of global cooling.
FA first appearance,
cse coarse, gr. grained, Tasman approx. time of Tasmanian Strait
opening, Drake approx.
completion (?) of Drake Passage opening, Mont. CE Monterey Carbon Excursion,
Pana. Panama Isthmus
closes. Arrows on thick
vertical lines: IRD appears in coarse fraction (after Deep-Sea Res.
II (54:2399); see P.F. Ciesielski and F.M. Weaver, 1983. Init.
Reps. DSDP 71:461)
12.2.5 On the Rise of Diatom Abundance at the End of the Paleogene
Diatoms may be considered the typical
Neogene plankton microfossil, in preference to foraminifers or
nannofossils (Fig. 12.2). This observation suggests that the
cooling trend must have greatly affected diatom abundance. It is
clear that cooling started in the early Eocene (Fig. 12.3). One infers that the
appearance of Drake Passage may have intensified any ongoing
cooling, following B. Haq. The capture of silica by diatoms of the
Antarctic margin presumably contributed to the purity of Oligocene
deep-sea carbonates over much of the seafloor (a purity noted by
K.J. Hsϋ in the DSDP Leg 3 report). Today’s sediments around
Antarctica are exceedingly rich in diatoms and other siliceous
fossils, as has been pointed out more than a century ago by many
workers (Fig. 10.11). The high silica deposition
is a presumably legacy of an open Drake Passage and the presence of
ice on Antarctica. The latter generates enormous circumpolar winds,
winds that drive the great ring current and generate its deep
mixing aspect (i.e., bringing up silicate and other nutrients for
recycling). Without the Drake Passage, world-wide productivity
might be lower. It certainly would be differently distributed
geographically.
On land, a great
extinction occurred at the Eocene-Oligocene boundary. It is called
Grande Coupure (Great
Break) in Europe with reference to a change in land mammals. In the
sea, the turnover includes a host of microfossils. The Australian
biostratigrapher B. McGowran in his 2005 text on ocean history and
biostratigraphy shows a prolonged benthic break at the end of the
Eocene which he links to a cooling step (“Chill II”), presumably
“Oi-1” in the oxygen isotope stratigraphy of K.G. Miller and
colleagues. It fits the picture of major reorganization of ocean
circulation and climate. Some geologists have emphasized purported
effects of impacts of bolides from space in generating extinctions
on land at the time. Impacts are important, but whether they play a
role in this time of rapid evolution at the end of the Eocene is
not clear.
12.2.6 On the Origin of Baleen Whales
There are good
reasons why whale teeth are rarely found on the seafloor. One is
the obvious one that they are in short supply, being delivered by
animals high on the food pyramid. Also, large teeth are rare
because all the “great
whales” except the (tooth-bearing) sperm whale are baleen
whales, that is, they gather food by filtering the water. They have
no teeth. According to Tom Demeré, curator of marine mammals at the
San Diego Natural History Museum, the first fossil baleen whales
probably appeared in the Oligocene. Apparently, in spite of having
no teeth, they retained many features of their ancestral stock,
such as a double blowhole. The modern-toothed whales (including
dolphins) on the other hand, while retaining teeth, have evolved a
single blowhole, presumably to facilitate echo location. Their echo
hunting targets are squid and certain fishes. Evolving a new way of
hunting would seem to imply a change in prey type and abundance,
which in turn supports the idea that we are seeing a change in the
food chain.
12.2.7 On the Importance of Gateways
The Drake Passage
(a “gateway”) serves as a prime example of the importance of plate
motions for global patterns of circulation, as pointed out by the
Swedish-trained Pakistani-US American geologist Bilal Ul Haq. The
once dominant connection between major water bodies and the large
circumtropical passages forming the Tethys have long ago closed and
disappeared. We now have cul-de-sac basins connected by the
cold-water ring around Antarctica (i.e., by the “Southern
exchange”).
According to Haq, the difference
between the present ocean and the Eocene one of about 45 million
years ago reflects strongly the closing of tropical gateways and
the opening of passages around Antarctica and in high latitudes in
general (Fig. 12.8). In detail, each of the changes associated
with openings and closings holds a wealth of interesting stories.
One of the most fascinating, for example, is the drying out of the
ancestral Mediterranean at the end of the Miocene between about 6
and 5 million years ago, as discovered during Leg 13 of the
Deep-Sea Drilling Project (with W.B.F. Ryan and K.J. Hsü as cochief
Scientists).
Huge amounts of salt were deposited at
that time in the Mediterranean Tethys basin, so much in fact that
the salinity of the global ocean must have been reduced by several
percent (“La crisi di salinità” of Italian geologists). In the case
of the Mediterranean desiccation, one assumes that a drop in sea
level owing to ice buildup was at least partially responsible for
isolating the ancient sea from the world ocean. Messinian
gypsum-bearing rocks are seen on land, as well, uplifted. Drying
the ancient Tethys basin (that is, the ancestral Mediterranean Sea)
must have raised sea level elsewhere, by some 10 m, briefly
reversing the general regression and perhaps thereby slowing ice
buildup, which arrived around 3 million years ago in northern high
latitudes on land, rather than during the time of the crisi
salinità, as one might expect if cooling accompanied
regression.
12.2.8 On the Grand Asymmetries in Circulation and Sedimentation
As concerns the heat budget, one
corollary of the cooling leitmotif of the Neogene ocean is a
displacement of the intertropical
convergence zone (ITCZ, the
heat equator) to north of the geographic equator. There are
several reasons for this. One is the whitening of the Antarctic
continent. This has the effect of increasing wind speeds in the
southern hemisphere and pushing southern climatic zones northward.
Another is the northward movement of large continental masses which
set up monsoonal regimes favorable to the northward transfer of
heat. The uplift of Tibet and the growth of the Himalayas as a
Neogene consequence of the Paleogene collision of the Indian
subcontinent with the Eurasian Plate had climatic consequences: a
strengthening of monsoons and an increase in weathering. Another
factor favoring northern heat piracy is the peculiar geographic
configuration of margins in the Atlantic and to a lesser degree in
the Pacific basin, configurations that provide for the northward
deflection of westward-flowing equatorial currents. As a
consequence, the Gulf Stream in the Atlantic and the Kuroshio in
the Pacific are strengthened. The end result is that the southern
hemisphere loses out on heat: Glaciers in Southern New Zealand at
present are in walking distance from the seashore. At that
latitude, vineyards occur around Bordeaux in the northern
hemisphere, not glaciers.
One important aspect of this planetary
heat asymmetry is the fact that the North Atlantic tends to deliver
deep water to the ring current around Antarctica. On the whole, the
North Atlantic receives shallow water in return. Thus, the northern
Atlantic system represents a heat pump, with warm (shallow) water
in and cold (deep) water out. Besides heat, nutrients are involved,
making the North Atlantic “anti-estuarine.” It entered this state
in the middle Miocene, as seen in the “silica switch” of the
Swiss-American geologist G. Keller (Princeton) and the USGS
geologist J. Barron (California) (see Fig. 12.10). Incidentally,
they favor an opening of the Drake Passage as linked to the Miocene
silica switch, based on evidence from hiatus stratigraphy. Their
suggestion certainly emphasizes the importance of the two events,
the mid-Miocene “silica switch” and the “Drake Passage opening.”

Fig.
12.10
The middle Miocene “silica switch” from the
North Atlantic to the North Pacific suggesting the timing of
turning on of the North Atlantic heat pump and anti-estuarine
status. Silica-rich sequences marked in black (After F. Woodruff
and S.M. Savin, 1989. Paleoceanography 4:87; based on a compilation
of deep-ocean drilling results by G. Keller and J.A. Barron, 1983,
Geol. Soc. Amer. Bull. 94:590)
When the North
Atlantic turned anti-estuarine and the North Pacific
correspondingly estuarine (with high silicate values in deep
waters), the present North Atlantic heat pump pattern was
established. It happened sometime near 15 million years ago,
judging from sedimentation patterns (actually, within the interval
of 16–10 Ma, judging from the various site results and from fossil
diversity). The timing is not sharply defined. The crowding of
N-zones (based on Neogene
planktonic foraminifers of biostratigraphic importance) suggests
large environmental change in the middle Miocene. The isotopic
changes in benthic foraminifers employed by F. Woodruff suggest an
age of 14 million years (early in the transition). Using changing
ratios of cadmium to calcium, M. Delaney and colleagues show a
switch just after 16 Ma, one that increases substantially toward
the end of the middle Miocene near 12 Ma.
12.2.9 On the Middle Miocene Cooling Step
Significantly, the “silica switch”
occurs close to a major cooling step, presumably accompanied by an
ice buildup and a substantial drop in sea level. The step may be
the largest one in the Miocene. It is called “Mi3” in the oxygen
isotope stratigraphy of K.G. Miller and colleagues. B.U. Haq and
associates, in their 1987 Science article on sea-level variations
through geologic time, placed a major drop in sea level at the end
of the middle Miocene, based largely on seismic information in
sediment stacks on continental margins but also on subsurface data
from drilling.
The cooling step and major sea-level
drop in the middle Miocene (presumably a large icing over in
Antarctica) were associated with major upwelling, as seen in the
record of margins in upwelling regions, for example off Namibia.
The foraminifers of that time display a major excursion of carbon
isotopes (toward positive values) indicating the burial of organic
carbon (Fig. 12.11). The carbon isotope excursion is the
largest in the last 50 million years. It was discovered in the
earliest drilling sites, even in the 1970s. The second largest in
this time span is at the Eocene-Oligocene boundary, in the
Paleogene, an isotopic event somewhat reminiscent of the one in the
Monterey in being closely followed by cooling. Choosing “the last
50 million years” for a discussion of cooling avoids consideration
of the (negative) carbon isotope excursion at the Paleocene-Eocene
boundary, which was associated with major warming. A large release
of methane from the deep seafloor to the environment has been
postulated for that time (the position of the event and the warming
are in the name PETM, Paleocene-Eocene Thermal Maximum).

Fig.
12.11
The Monterey Event (From W.H.B., 1985,
Episodes 8, 163; based on E. Vincent and W.H.B., 1985. In: E.T.
Sundquist and W.S. Broecker (eds.) The Carbon Cycle and Atmospheric
CO2: Natural Variations Archean to Present. Geophys.
Monogr. 32: 455. Right:
Monterey Formation near Santa Barbara; Photo W.H.B.)
The French-American marine geologist
and biostratigrapher Edith Vincent (then at S.I.O.) used the label
“Monterey Event” for the Miocene carbon isotope excursion. The
label implies drawing a parallel of the carbon isotope excursion to
the evidence for increased upwelling at the time of the origin of
the Californian Monterey Formation. Some of the organic carbon
buried globally (and generating the characteristic carbon isotopic
signal in benthic deep-sea foraminifers prior to the great middle
Miocene cooling) could conceivably be of terrigenous origin, as
emphasized by the marine geologist L. Diester-Haass (Saarbrϋcken).
But much of the signal presumably has a marine origin, judging from
the sediments delivered by upwelling in the eastern Pacific margin
(i.e., the Monterey Formation). Much of the sediments of the
Monterey Formation are finely layered and also have plentifully
phosphate and chert content, the latter presumably generated by
diatoms and other siliceous export from the sunlit zone and
suggesting high marine productivity (Fig. 12.12).

Fig.
12.12
Miocene Monterey Formation in southern
California. Left: uplifted
section on the road near Lompoc (Photo Univ. South. Cal., courtesy
E. Vincent, S.I.O.) Right:
On Gaviota Beach, near Santa Barbara (Photo W.H.B.). Fine layering
is caused by lack of burrowing owing to a scarcity of oxygen,
typical below upwelling areas
Strong upwelling apparently started
only about 10 million years ago in most coastal systems, but
high-coastal production presumably started considerably earlier.
Additional upwelling intensity likely set in with each cooling
step. Thus, ocean productivity presumably did benefit from the
cooling all through the Cenozoic, especially in post-Eocene time,
and earlier than suggested by strong coastal upwelling.
12.3 Culmination: Onset of the Ice Ages
12.3.1 The Timing
We have earlier referred to the drying
up of the Mediterranean at the end of the Miocene. It was not to be
the culmination of Neogene cooling; the northern ice ages were.
Presumably the Mediterranean desiccation was indeed facilitated by
a sea-level drop caused by ice buildup, some of it on the northern
hemisphere. But in the time that followed the last desiccation
pulses (apparently including the earliest Pliocene), the planet
experienced a relatively calm and warm period, lasting some 2
million years. This warmish time in the Pliocene was terminated by
the onset of the northern ice ages, some 3 million years ago.
The onset of northern ice ages looks
like expected, in principle, from the general Cenozoic cooling
trend (see Hodell et al., 2002. ODP Leg 177 synthesis). For the
onset to materialize, one would think, continued uplift had to keep
moving the climate toward an increasingly cold state, so that at
times, even the mighty Gulf Stream failed to bring enough heat
northward to stop an ice age from developing. In the late Pliocene,
when the signs were right (low summer insolation as postulated by
Milankovitch Theory), the ice started growing on Canada. The
climate then entered a 3 million year period (lasting throughout
the Pleistocene) when relatively small changes in summer sunlight
in high northern latitudes were translated into large-scale changes
in ice mass and sea level (see Chap. 11). That northern ice buildup
started around 3 million years ago within the late Pliocene was
documented by the Woods Hole geologist and biostratigrapher W.A.
Berggren during one of the early DSDP legs, based on ice-rafted
debris (Fig. 12.13). The event not only resulted in cooling
within the Gauss Chron but also provoked the onset of major climate
fluctuations, as suggested in a sudden increase of isotope
variations in benthic foraminifers (Cibicides spp.) and in planktonic ones
seen off Antarctica, as documented by D. Hodell and associates, by
deep-ocean drilling (see in J.P. Kennett and D.A. Warnke, eds.,
1992, The Antarctic Paleoenvironment: A Perspective
on Global Change. AA Res. Ser. 56).

Fig.
12.13
Onset of the northern ice ages. W.
Berggren, 1972 evidence (based on erosion-produced mineral grains
and biostratigraphy) from the NW deep Atlantic, DSDP Site 116 (Leg
12). Onset placed roughly 3 million years ago, in agreement with
geologic evidence from the Sierras
12.3.2 Panama Paradox
Several distinguished marine
geologists have insisted that the timing of the onset of the ice
ages is linked to closing the Panama Strait, which ended the loss
of heat to the Pacific by westward currents from the Atlantic.
Supposedly, moisture for making snow was then available to high
northern latitudes, moisture brought northward by warm Caribbean
waters (e.g., Gulf Stream, Fig. 5.14). The implication is that
availability of moisture is limiting to northern polar ice growth,
not just cooling. The concept, as an explanation for the origin of
northern ice ages, has been questioned by W.H.B. and G. Wefer,
whose “Panama Paradox”
hypothesis calls for attaining a critically low temperature within
the long-term cooling trend rather than a link to the closing of
the Panama Straits, as the crucial element of the onset of the ice
ages. Clearly, however, moisture is involved also, whenever making
snow and ice, as evidenced by modern distribution patterns of ice
in Scandinavia. Thus, the question about the role of moisture
supply in starting the ice ages must be considered
unresolved.
12.4 Plate Stratigraphy and CCD Fluctuations
12.4.1 Backtracking and CCD Reconstruction
To interpret the meaning of a given
sample from the seafloor, the sediment has to be placed in its
original depth and location at the time of deposition. This is done
by “backtracking” the path that a site has taken as it aged.
Without taking proper account of this path, the sediment sequences
in drill cores cannot be interpreted correctly, especially if
substantial changes in depth or in latitude are involved. For
example, when a site moves down the East Pacific Rise in the
Neogene and northward across the equator, it necessarily collects a
number of different types of sediment in sequence (calcareous ooze,
siliceous clay, siliceous calcareous ooze, siliceous clay, Red
Clay). The resulting vertical stack of different sediments
(leftmost panel, Fig. 12.14) can look like evidence for changes in
the sedimentary record of the ocean’s climate system, when in fact
it was produced by plate motion.

Fig.
12.14
Schematic of plate stratigraphy in the
eastern equatorial Pacific: latitudes and depths. The hypothesized
seafloor originated above the present CCD. The high production
along the equator persisted throughout the Neogene. Sharp
separation of facies (sediment types) began with the Oligocene
(After concepts of W.H.B. and E.L. Winterer, 1974. [Int. Assoc.
Sedim. Spec. Pub. 1:11])
Horizontal backtracking (a focus of the work
of Y. Lancelot, 1937–2016) refers to geographic position,
using the appropriate pole of rotation for reconstruction of
latitude and longitude. Vertical
backtracking (Fig. 12.14) addresses the reconstruction of depth by
considering the subsidence of a piece of seafloor, most commonly
from a cooling of the crust and uppermost mantle. Vertical
backtracking is a necessary procedure whenever depth-sensitive
properties are involved, such as carbonate content, sedimentation
rates of oozes, or preservation of calcareous fossils, on time
scales for which tectonic subsidence matters.
The position of the CCD, by
definition, involves both depth and carbonate content of deep-sea
sediments, and its path through the Cenozoic, therefore, can only
be accurately described when taking the general subsidence of the
seafloor into account. To obtain the path of the CCD (an important
element of all conditions that relate to the marine carbon cycle),
we must reconstruct the depth levels at which the CCD was crossed
for a large number of drilling sites. Reconstructions vary with the
quality of dating of the basement and of sediments, but there is
general agreement (since 1985) on the major features of the
Cenozoic behavior of the CCD. The most notable features are the
drastic drop of the CCD at the end of the Eocene and the
short-lived but remarkably substantial excursion to shallow depths
during the “carbonate
crash” of Mitchell Lyle (ODP Leg 138) at the end of the
middle Miocene (Fig. 12.15). The first feature is linked to the
end-of-Eocene Auversian facies shift (the “AFS”); the second (the
“Crash”) is tightly linked to a cooling step and a sea-level drop
producing a large hiatus.

Fig.
12.15
Schematic of the Cenozoic variation of the
CCD, based on numerous authors (with special kudos to K.J. Hsü and
R. Wright, 1985. In: K.J. Hsű and H.J. Weissert (eds.) South
Atlantic Paleoceanography, Cambridge Univ. Press, Cambridge UK.)
“Ridge crest,” depth level
near −2500 m; “modern global
CCD,” depth-level variable between and within ocean basins,
typically between −4 and −4.5 km; “abyssal seafloor,” depth level below
−5000 m; “AFS” Auversian
facies shift, late Eocene, near 40 Ma; “CC” “carbonate crash” ca. 11 million
years ago (end of middle Miocene)
An overall parallelism in CCD
variation between Atlantic and Pacific basins is remarkable. It
suggests that the geochemistry of the marine carbon cycle is global
in nature rather than carrying only information from each ocean
basin. Comparison of sea-level reconstructions and δ18O
stratigraphy suggests that periods of high sea level are
characterized by a shallow CCD and by warm high latitudes and
periods of low sea level by a deep CCD and cold high latitudes (and
cold deep waters). Why should a relatively warm ocean have a
shallower CCD than a cold
one? Is not cold water less
favorable to the preservation of carbonate than warm water? The
fuzziness of possible answers to such simple questions reflects the
depth of ignorance surrounding the discoveries having to do with
the history of the CCD.
12.4.2 Possible Causes of CCD Fluctuations
A simple hypothesis linking sea level
to CCD fluctuations is the concept of basin-shelf fractionation. As mentioned
earlier, shelves covered by seawater are carbonate traps. As they
remove CaCO3 from the ocean, they tend to starve the
deep seafloor of carbonate and hence raise the CCD. Conversely,
bared shelves supply carbonate to the deep sea. In this very simple
bookkeeping hypothesis, variations in temperature, while important
in the thermodynamics of carbonate deposition, are incidental,
while changes in sea level are close to basic forcing – and to
geological time scales (Fig. 6.1).
There is good reason to believe that
the mass balance hypothesis of CCD fluctuations in fact does not
account for all the relevant observations. It is compatible with
the CCD drop at the end of the Eocene but not necessarily with the
other major feature in the CCD history, that is, the carbonate
crash (CC). The CC is reminiscent of the dissolution event observed
at each onset of a glacial period during the last million years. It
may be due to increased production and provision of organic matter
producing carbonic acid upon oxidation. Available data bearing on
the questions are still quite incomplete.
12.5 On the Cenozoic Methane Ice Problem
The production of
methane in and on the continental margins of today’s seafloor by
certain archaea (once called methane bacteria) is pervasive. It may
be considered a result of the cooling that brought us the ice ages
and apparently is linked to high export production in offshore
waters (“upwelling”). Methane seeps are especially abundant in the
continental margin off Oregon, where they were studied by the
marine geochemists E. Suess, G. Bohrmann, A.M. Tréhu, and M.E.
Torres, among others.
Some of the methane is locked up in
methane ice (technically “methane clathrate”), given high pressure
and cold water temperature in the surrounding environment (Fig.
4.5). Methane is a powerful
greenhouse gas. Vast deposits of methane ice are reported from the
present seafloor in the coastal ocean in seismic profiles and in
sediments retrieved by drilling (Fig. 12.16). The likely
response of methane clathrates to global warming is as yet obscure,
but the threat is palpable. What we do know is that the methane
ice, once exposed to temperatures warmer than the thermodynamic
value appropriate for stability, will melt readily at modest
pressures (Fig. 4.5). Also, methane ice melts as
confinement is removed (low pressure). In consequence of warming
and pressure release, methane is released in profusion when methane
ice is brought on board and can then be ignited by those holding
the melting ice in hand (Fig. 1.10).

Fig.
12.16
Methane ice (methane clathrate) embedded in
black mud (DSDP Leg 84; photograph from S.I.O. archives)
As discussed, the middle Miocene
Monterey Event starts with a large excursion of carbon isotope
values toward high values (i.e., with an unusually large amount of
13C in the ratio of 13C/12C in
calcareous fossils). The most parsimonious explanation for the
excursion involves the buildup of C12-rich stores of
biogenic carbon during the time, including methane ice.
The most
impressive methane ice event may have happened in the Paleogene.
According to the co-discoverers of the carbon isotope anomaly
marking the time of the event, J.P. Kennett and L.D. Stott (ODP Leg
113), the event was responsible for major extinction of benthic
foraminifers in the deep sea. A release of massive amounts of
methane from melting of clathrate has been proposed as an
explanation of a (negative) carbon isotope excursion at the very
end of the Paleocene. The very same explanation was used to address
the thermal maximum (the “PETM”) associated with the isotope
event. The warming during the PETM, it is widely assumed, largely
reflected an excess abundance of carbon dioxide generated by
oxidizing the methane.
Interestingly, the PETM-associated
carbon isotope excursion toward negative values is preceded by a
large and distinct excursion toward heavy isotopes several million
years earlier, in the “Thanetian” (Fig. 12.17). A buildup of
organic matter deposits, including methane ice, could have produced
this excursion.

Fig.
12.17
Oxygen and carbon isotope stratigraphy in
Paleogene benthic foraminifers from various drilling sites in the
world ocean (Data compiled by J. Zachos and colleagues, 2001.
Science 292:686; here interpolated) PETM Paleocene-Eocene Thermal Maximum,
THANET. C ex. Thanetian
carbon isotope excursion toward heavy values
Suggestions for Further Reading
Garrison, R.E., R.G. Douglas,
K.E. Pisiotto, D.M. Isaacs, and J.C. Ingle (eds.) 1981. The
Monterey Formation and Related Siliceous Rocks of California. SEPM,
Tulsa, OK.
Warme, J.E., R.G. Douglas,
and E.L. Winterer (eds.) 1981. The Deep Sea Drilling Project: A
Decade of Progress. SEPM Sp. Pub. No. 32. SEPM, Tulsa,
Oklahoma.
Hsü, K. J., 1983, The
Mediterranean was a Desert: a Voyage of the Glomar Challenger.
Princeton U. Press.
Ludwig, W.J., and V. A.
Krasheninnikov (eds.) 1983. Initial Reports DSDP 71.
Thiede, J., and E. Suess
(eds.) 1983. Coastal Upwelling, its Sedimentary Record. Part B:
Sedimentary Records of Ancient Coastal Upwelling. Plenum Press, New
York.
Hsű, K. J., and H. J.
Weissert (eds.) 1985. South Atlantic paleoceanography. Cambridge
Univ. Press.
Hsű, K.J. (ed.) 1986.
Mesozoic and Cenozoic Oceans. Amer. Geophys. Union Geodynamics
Series 15.
Kennett, J.P., and C. C. von
der Borch (eds.), 1986. Initial Reports DSDP 90.
Ruddiman, W.F., and B. Kidd
(eds.) 1987. Initial Reports DSDP 94.
Srivastava, S. P., M.A.
Arthur, and B. Clement (eds.) 1989. Proceedings of the Ocean
Drilling Program, Scientific Results, 105. Ocean Drilling Program,
College Station, TX.
Barker, P.F., and J.P.
Kennett (eds.) 1990. Proc. ODP, Sci. Results. 113.
Bleil, U., and Thiede, J.
(eds.) 1990. The Geological History of the Polar Oceans: Arctic
Versus Antarctic. Kluwer Academic, Dordrecht.
Mountain, G.S., and M.E.
Katz ME (eds) 1991. Report of the Advisory Panel Meeting on Earth
System History (MESH). National Science Foundation, Division of
Ocean Sciences, Washington DC.
Kennett, J.P., and D.A.
Warnke (eds.) 1992. The Antarctic Paleoenvironment: A Perspective
on Global Change. Am. Geophys. Union, Wahington D.C.
Prothero, D., and W.A.
Berggren (eds.) 1992. Eocene-Oligocene Climatic and Biotic
Evolution. Princeton University Press, Princeton, NJ.
Wise, S. W., and R. Schlich
(eds.) 1992. Proc. ODP, Sci. Results, 120.
Summerhayes, C.P., Prell,
W.L., Emeis, K.C. (eds.) 1992. Upwelling Systems: Evolution Since
the Early Miocene. Geol. Soc. (London) Special Publication
64.
Berggren, W.A., Kent, D.V.,
Aubry, M.-P., and Hardenbol, J. (eds.) 1995. Geochronology, Time
Scales and Global Stratigraphic Correlation. SEPM Special Publ.
54.
Gersonde, R., D.A. Hodell,
and P. Blum, (eds.) 2002. Proc. ODP, Sci. Results, 177.
Elderfield, H. (ed.) 2004.
The Oceans and Marine Geochemistry. Elsevier, Amsterdam.
Exon, N.F., J.P. Kennett,
and M.J. Malone (eds.) 2004. The Cenozoic Southern Ocean:
Tectonics, Sedimentation, and Climate Change Between Australia and
Antarctica. AGU Geophys. Monogr. 151.