The differences observed
in the amplitude of the planktonic and benthic 18O
and
13C
variations indicate that temperature, salinity, and productivity changes
occurred in the surface water and deep water masses in relation to past climatic
changes. The salinity variations that are related to the global ice effect are
similarly recorded by the
18O
values of planktonic and benthic foraminifers. The
18O
gradients between foraminiferal species are thus affected only by the vertical
thermal gradients and by local salinity variations at the ocean surface due to
differences in the precipitation-evaporation balance.
The export of organic
carbon from the photic zone extracts preferentially 12C from the
dissolved inorganic carbon reservoir, which becomes richer in 13C;
there is thus a direct relationship between high 13C
values and high rates of biological pumping in surface waters. However, inputs
of deep nutrients by upwelling introduce 13C-depleted CO2
in the surface waters, which is characteristic of eutrophic conditions and
causes the decrease of the surface-subsurface
13C
gradient. Intermediate between oligotrophic and eutrophic conditions,
mesotrophic situations exhibit high surface-subsurface
13C
gradients due to the combination of lateral advection of deep nutrients and high
surface productivity levels (Pierre et al., 1994). At depth, the contribution of
CO2 derived from organic matter oxidation causes a decrease of the
13C
values of deep waters. During glacial times, high
13C
gradients between planktonic and benthic foraminifers indicative of high
productivity were generally coeval with low atmospheric CO2 concentrations
in the air trapped in antarctic ice, which was interpreted by Berger et al.
(1989) as an argument on the link between the biological pump and the global
concentration of atmospheric CO2. Recently, Broecker and Henderson
(1998) have proposed that the ocean productivity changes are global and related
to the oceanic nitrogen cycle, which is controlled by dust flux. In this
scenario, increasing nitrogen fixation during glacial times would cause the
increase of CO2 uptake in surface waters and the drawdown of
atmospheric CO2 concentrations.
The estimation of the oxygen and carbon isotopic gradients between foraminiferal species living at different depths or at different seasons may help to reconstruct changes in surface water hydrography. Giraudeau (1993) and Giraudeau and Rogers (1994) provided information on the spatial distribution of planktonic foraminiferal species in the Benguela upwelling system. Their studies showed that planktonic assemblages are distributed according to the various surface water masses and associated hydrological fronts induced by the upwelling process. Among the three planktonic species that were used in the present stable isotope study, G. ruber is considered to be characteristic of warm surface waters; the subpolar species G. bulloides dominates the planktonic assemblages of cool, nutrient-rich, newly upwelled waters, whereas the deep-dwelling species G. inflata is associated with offshore oligotrophic waters.
In the following
discussion, the surface-to-deep isotopic gradients 18O
and
13C
are given by the difference between the
18O
and
13C
values of G. inflata
and Cibicides.
The isotopic gradients between G.
inflata and G.
ruber are used as a tracer of the seasonal or vertical (depth of the
thermocline) temperature gradient in the surface mixed layer, whereas the
isotopic gradients between G.
inflata and G.
bulloides are used as an index of the variable contributions of
oligotrophic offshore waters and upwelled eutrophic waters at the site location.
The 18O
G. inflata-Cibicides
record displays large oscillations that roughly follow the G-IG cyclicity (Fig. F5A).
Second-order, rapid, high-amplitude fluctuations of
18O
around the present-day gradient (
18O
values enriched by up to 1.0
or depleted by up to 0.8
)
are indicative of the surface-to-bottom temperature and salinity gradients. High
18O
values are interpreted as either decreasing surface-to-bottom temperature
gradients or increasing surface-to-bottom salinity gradients.
The largest oscillations
of 18O
with amplitudes up to 1.8
occur between 80 and 280 ka, a period that comprises MISs 5 to 8. Such high
amplitudes cannot be attributed to changes of up to 8°C in the
surface-to-bottom temperature gradient because such temperature changes would be
extreme. We therefore consider that surface waters were also affected by
important salinity variations. A comparison of the isotopic data with the
planktonic foraminiferal distribution at Hole 1087A (Giraudeau et al., Chap.
7,
this volume) shows that some peaks of high
18O
values (terminations I and II, MISs 11 and 12) are in phase with the peaks of
abundance of G. menardii,
both proxies indicating maximum penetration of salty
18O-rich
Indian Ocean thermocline waters. Other peaks of high
18O
values (MISs 4, 5, 6, 7, 8, and 12) coincide with the maximum abundances of G.
bulloides, which suggests the presence of cold, upwelled surface
water. Low
18O
values generally occur during cold events of glacial and interglacial stages; if
these isotopic gradients are interpreted in terms of the surface-to-bottom
temperature gradient, the cooling of surface waters had to be less than that of
deep waters.
The amplitude of 18O
variations through time is greatest for G.
bulloides and least for G.
ruber, except for MIS 12. This is reflected by the planktonic
18O
variations; for example, the amplitude for G.
inflata-G. bulloides is twice that of G.
inflata-G.
ruber (Fig. F5B,
F5C). MIS 11 is poorly
constrained due to the scarcity of G.
bulloides and G.
ruber during this time interval.
The 18O
G. inflata-G. bulloides
is generally much higher than during the Holocene, except for a few rapid events
during MIS 2, 8, and 10 that reach the Holocene level (Fig. F5B).
The overall high
18O
values, particularly during isotopic events 5.3 and 9.3, are caused by an
increase in
18O
values of G. inflata
and a decrease in
18O
values of G. bulloides.
Conversely, the
18O
decreases, such as those observed at the MIS transitions 11/10, 7/6, 5/4, and
4/3, correspond to rather constant
18O
values of G. inflata and
to increasing
18O
values of G. bulloides. These
isotopic variations integrate the variations of a multicomponent system where
the seaward extension of the upwelled waters relative to the offshore
oligotrophic waters is modulated by the cooling intensity in the upwelling cell
and by the strength of the Benguela Current.
The 18O
G. inflata-G. ruber
and
18O
G. inflata-G. bulloides
records display very similar vertical patterns (Fig. F5C).
They show no difference in their amplitude during G-IG cycles;
however, the highest
18O
values occur during the warm substages reflecting periods of higher temperature
contrast in the surface waters. The onset of deglaciations displays a typical
evolution with a sharp increase followed by a sharp decrease of
18O
values; this can be interpreted either as a succession of deepening and shoaling
of the thermocline or as abrupt changes from high to low seasonal contrast.
Similar observations were made by Wefer et al. (1996) in the Benguela Current
System, and these authors emphasized the difficulty of interpreting this proxy
in terms of seasonal contrast or thermocline depth. In any case, this evolution
would mean that the Benguela Current was temporarily reduced at the end of
glacial stages and then reinforced at the beginning of interglacial stages.
The 13C
G. inflata-Cibicides
values are subjected both to sharp short-term and long-term oscillations, with a
maximum amplitude of 1.7
,
that are not related to the G-IG cycles (Fig. F6A).
The
13C
variations thus are quite different from the pattern described by Berger et al.
(1989). We assume that at Site 1087, latitudinal and meridional migrations of
hydrological fronts dominated the surface water productivity.
The short-term periods of
low 13C
values, which indicate low
13C
values of surface waters, suggest an influx of Indian Ocean thermocline waters.
Recent
13C
measurements along a transect south of Africa along 30°E show that the surface
waters of the Agulhas Current have a carbon isotopic signature lower by 0.5
than the subantarctic waters (Archambeau et al., 1998; Quentin, 1997). The
important contribution of Indian Ocean waters can thus easily explain the
decrease of the surface-to-bottom carbon isotopic gradient. The other peaks of
low
13C
values occur independent of glacial stages (MISs 2, 3, 4, and 6) and
interglacial stages (MISs 5, 7, and 13), but they correspond to the periods of
maximum abundance of G.
bulloides that are also marked by
18O
anomalies; in these cases, the
13C
decrease at the surface is more likely caused by the seaward extension of 13C-depleted
upwelled waters.
The high 13C
values are mostly concentrated in late MIS 5 and during the 260- to 425-ka
interval. As mentioned above, the high
13C
values of planktonic foraminifers were interpreted as indicative of high primary
productivity. These events, which interrupt the negative
13C
excursions, indicate the installation of a different regime dominated by more
oligotrophic conditions.
The carbon isotope
gradients in the surface waters are balanced by the uptake of 13C-depleted
CO2, resulting from surface productivity and by the inputs of
13C-depleted
CO2 due to the vertical and lateral advection of nutrient-rich
waters. The
13C
variations between G.
inflata and G.
bulloides are twice those measured between
G. inflata and
G. ruber (Fig. F6B,
F6C); this is
explained by the largest
13C
variations recorded by G.
bulloides, a species that is the most sensitive to changes in
upwelling strength. The overall
13C
patterns show no correspondence with the G-IG cycles; however, these patterns
document global trends toward increasing or decreasing values, which are
inferred to represent major changes in the trophic regime and in the depth of
the thermocline that are controlled by the lateral and vertical advective fluxes
of nutrient-rich deep waters.
The minimum values of the
carbon isotope gradient between G.
inflata and G.
bulloides are interpreted as representative of oligotrophic
conditions, whereas the maximum values are indicative of mesotrophic conditions.
Three steps may be identified following the evolution of the G.
inflata-G. bulloides 13C
values (Fig. F6B).
Starting from 500 ka, where the
13C
values are similar to the Holocene values, there is a decrease by >1
(on average) up to 400 ka; this period corresponds to the initiation of
oligotrophic conditions that remain quite steady up to 350 ka. After 350 ka and
up to 100 ka, this planktonic
13C
increases by >2
on
average, marking the progressive development of more mesotrophic conditions.
After 100 ka, the
13C
values decrease again by ~1
to reach the Holocene values, marking the return toward oligotrophic conditions.
The carbon isotope
gradient between G.
inflata and G.
ruber is considered to follow the vertical movement of the
thermocline: shoaling of the thermocline brings deep nutrients closer to the
surface and the 13C
values decrease in the surface waters, whereas deepening of the thermocline
diminishes the inputs of deep nutrients to the surface and results in the
increase of
13C
values. The same three steps are also observed in the
13C
G. inflata-G.
ruber record (Fig. F6C).
During the period from 500 ka to 350 ka,
13C
values increase by ~0.7
on average, an indication for the progressive deepening of the thermocline. The
second step from 350 ka to 100 ka corresponds to the progressive decrease of
13C
by ~0.6
and is related
to the progressive shoaling of the thermocline. During the last step,
13C
increases again by ~0.3
,
suggesting that the thermocline deepened slightly to reach the present-day
situation.