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GRIP Deuterium Excess Reveals Rapid and Orbital-Scale Changes in Greenland Moisture Origin

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Science  01 Jul 2005:
Vol. 309, Issue 5731, pp. 118-121
DOI: 10.1126/science.1108575

Abstract

The Northern Hemisphere hydrological cycle is a key factor coupling ice sheets, ocean circulation, and polar amplification of climate change. Here we present a Northern Hemisphere deuterium excess profile covering one climatic cycle, constructed with the use of δ18O and δD Greenland Ice Core Project (GRIP) records. Past changes in Greenland source and site temperatures are quantified with precipitation seasonality taken into account. The imprint of obliquity is evidenced in the site-to-source temperature gradient at orbital scale. At the millennial time scale, GRIP source temperature changes reflect southward shifts of the geographical locations of moisture sources during cold events, and these rapid shifts are associated with large-scale changes in atmospheric circulation.

The atmospheric water cycle plays a key role in climate change. At various time scales, changes in atmospheric moisture transport are intimately involved in key processes within the climate system, such as the growth of ice sheets or the freshwater budget of the ocean. Here we use an integrated tracer of the water cycle, the isotopic composition of the ice preserved in Greenland, to decipher changes in Greenland moisture origin over the last glacial cycle.

Water stable isotopes ratios (δ18O or δD) from polar ice cores are commonly used as past temperature proxies (1, 2), a function made possible by the progressive distillation of heavy water isotopes when air masses cool toward polar regions (35). Comparison of Greenland temperature (Tsite) values derived from ice δ18O using the observed modern spatial gradient with alternative paleothermometry methods yields a systematic underestimation of past surface annual mean temperature changes, both at glacial-interglacial (68) and rapid-events time scales (913). Such discrepancies are thought to arise from variability in the Northern Hemisphere hydrological cycle, either from changes in moisture source areas (14) or from changes in the seasonality of precipitation (15, 16).

We used high-precision continuous water stable isotope measurements made on the GRIP ice core (table S1) to calculate a Northern Hemisphere deuterium excess d = [δD – (8 × δ18O)] profile covering one climatic cycle (17). This deuterium excess record, together with a method to account for changes in precipitation seasonality, was then used to quantify past changes in Greenland moisture source temperature.

Figure 1 shows both δ18O and deuterium excess profiles for the last ∼100,000 years (i.e., excluding the lowest part of the profiles characterized by ice flow disturbances) (18). The excess profile reveals well-defined features at glacial-interglacial time scales, with a 5 per mil (‰) increase during the last climatic transition (5), as well as for Dansgaard-Oeschger (D/O) events characterized by large (up to 5‰) excess changes, in antiphase with δ18O changes. Similar rapid excess changes are also recorded in the North Greenland Ice Core Project (NorthGRIP) ice core for D/O events 18 to 20 (13). Such deuterium-excess variations essentially result from the fact that, with respect to equilibrium processes, kinetic isotopic effects play a much larger relative role for δ18O than for δD. In turn, deuterium excess in polar snow, dsnow, is largely driven by nonequilibrium processes (i.e., evaporation at the ocean surface and condensation of water vapor when snow forms). Deuterium excess in water vapor over the ocean is mainly influenced by sea surface isotopic composition, sea surface temperature (SST), source temperature (Tsource), and relative humidity. This imprint of oceanic conditions (here considered only in terms of Tsource) in the moisture source areas is largely preserved in the deuterium excess signal recorded in polar snow (19). In turn, whereas δsnow18O or δD) depends primarily on local temperature Tsite and to a lesser degree on Tsource, one can show that the opposite is true for dsnow (20, 21).

Fig. 1

(left). From top to bottom: ice volume indicated by seawater δ18Osw (31); 200-year resampled GRIP δ18O and deuterium excess d (bold lines represent isotopic profiles smoothed using the first two components of a singular spectral analysis, which represents a low-pass filter below 10,000 years); and obliquity (43). Analytical precisions are ±0.05‰ for δ18O and ±0.50‰ for δD, resulting in a precision of ±0.64‰ for deuterium excess. Horizontal dashed lines identify thresholds T1 and T2 used for the seasonality correction. Vertical lines point to selected rapid events (from left to right: Younger Dryas, cold phases of D/O events 11, 12, and 22). Fig. 2 (right). From top to bottom: log(Ca) (39); 200-year reconstructed site-to-source temperature gradient (black solid line) and obliquity fluctuations (black dashed line); site temperature (ΔTsite) reconstructed using various methods [spatial slope without seasonality correction, blue; our inversion with seasonality correction but without source correction, red; our full isotopic inversion with seasonality correction, black; the use of a constant slope fitting with the LGM borehole estimate (32), green]; source temperature (ΔTsource) reconstruction from full inversion. Results are displayed as anomalies from modern conditions (present-day GRIP site temperature is ∼–32°C and GRIP source temperature is ∼20°C). Bold lines represent smoothed reconstructions as for Fig. 1.

Combining δ18O and deuterium excess profiles allows us to estimate both Tsite and Tsource. This dual approach, based on the inversion (22) of a dynamically simple isotopic model (23), is now used for interpreting isotopic measurements performed on Antarctic cores (2426). Although useful for the last millennium and for the Holocene in Greenland (20, 27), this methodology leads to unrealistic results when applied directly to the long-term GRIP data (21). We show here that this difficulty can be overcome if this inversion accounts for the seasonality of snow precipitation, as suggested by general circulation model simulations. This allows us to interpret the δ18O or δD GRIP data in terms of Tsite and Tsource changes in a consistent way, both for glacial-interglacial changes and for D/O events, thus providing high-resolution information on the source conditions and the reorganizations of the water cycle during slow and rapid climatic changes.

Seasonal characteristics are relatively well known for central Greenland's present-day climate. Field observations suggest a year-round snowfall at Summit with a slightly larger winter half-year accumulation due to intense episodic storms (28). The seasonal variations are strongly imprinted in δ18Osnow, which closely follows the temperature changes. As shown by detailed shallow ice core and pit studies, there is also a well-documented dsnow seasonal cycle that lags variations in temperature, δD, and δ18O by ∼2 to 3 months(5, 29). This delay is probably due to the thermal inertia of the ocean, which results in a 2- to 3-month lag between mid-latitude ocean surface temperature and continental surface air temperature.

In contrast, glacial conditions inhibit winter snowfall because of the modification of the stationary waves and the southward deviation of the winter storm tracks by (i) the Laurentide ice sheet, and (ii) the modified latitudinal ocean surface temperature gradients and increased extent of sea ice (30). Modeling results suggest a large change in precipitation seasonality toward a dominant summer contribution (15, 16). We also expect an enhanced δsnow seasonal amplitude due to increased glacial Greenland continentality. The ∼2- to 3-month lag of the deuterium excess cycle, thermally driven, should be essentially unchanged.

A detailed sensitivity analysis shows that a simple half-year (summer-winter) approach is well adapted to account for these seasonality changes for reconstructing site and source temperature records (21). Whereas the winter-summer difference is large for δsnow, it is small (less than 1‰) for the deuterium excess because of its seasonal lag. Hence, seasonality has a strong impact on estimates of Tsite but a much weaker influence on Tsource, as these two variables are driven by δsnow and dsnow, respectively. The glacial decrease in winter precipitation results in amplified seasonally corrected isotopic signals by a factor that is also influenced by the changes in the summer-winter isotopic amplitude [(21), equation 5]. We account for seasonality when two conditions linked with sea-ice extent and Laurentide ice sheet size are fulfilled: (i) Sea-ice extent is assumed to inhibit local moisture supply when the site temperature is below a certain threshold T1 directly derived from the ice δ18O record, and (ii) to reflect the fact that the winter moisture advection is related to the size of the Laurentide ice sheet, we account for seasonality changes only when the Laurentide is large enough. We use here a second threshold, T2, derived from the marine benthic δ18O sea level record, itself closely related to the size of the Laurentide (31). Ensemble simulations of seasonality correction and full isotopic inversion are then performed within a wide range of correction coefficients. Obtaining a consistency with robust estimates of site temperature amplitudes obtained with independent methods (Table 1) for the Last Glacial Maximum (LGM), Younger Dryas, Bølling-Allerød, and D/O events 12 and 19 constrains the thresholds T118O of ice < –36.4‰) and T2 (ocean δ18O < 0.4‰), and also the amplification coefficient, to a value of 2.0.

Table 1.

Estimates of site temperature changes and comparison with two methods to estimate temperature changes using the water stable isotopes from GRIP ice cores. ΔTsite full inversion, results of the full isotopic inversion after seasonality correction; ΔTsite constant slope, estimate from ice δ18O only, with a constant slope before 8 ka (32).

Period Temperature change Method ΔTsite full inversion ΔTsite constant slope
Last Glacial Maximum -23° ± 3°C (View inline) Borehole thermometry -21.5° ± 3°C -17.9°C
Bølling 11° ± 3°C (View inline) Gas fractionation 10.9° ± 3°C 13.9°C
Younger Dryas 10° ± 4°C (View inline) Gas fractionation 9.7° ± 3°C 11.1°C
D/O 12 12° ± 3°C (View inline) Gas fractionation 13.9° ± 3°C 13.1°C
D/O 18 11° ± 3°C (View inline) Gas fractionation 9.8° ± 3°C 11.4°C
D/O 19 16° ± 3°C (View inline, View inline) Gas fractionation 17.1° ± 3°C 20.2°C
D/O 20 11° ± 3°C (View inline) Gas fractionation 11.7° ± 3°C 16.7°C

The resulting site and source fluctuations are shown in Fig. 2, showing a warming of ∼21.5°C from the LGM to the Holocene [estimate based on the 2000-year period centered at 21,000 years ago (21 ka)]. Our reconstruction for D/O events 18 and 20 is also consistent with independent estimates of site temperature changes obtained using gas fractionation (performed in this latter case on the NorthGRIP core located 300 km north-northwest of the GRIP site) (Table 1). Figure 2, which compares various approaches to reconstructing Tsite changes from water isotopes, clearly shows the importance of accounting for seasonality. However, there is also a significant influence of the source temperature (full inversion, black curve), which results in a systematic shift of the warm part of each D/O event toward colder temperatures. This is due to the antiphase between the δ18O (or δD) and excess rapid variations: When Greenland is warm, the moisture source is colder, and if this is not corrected for, temperature estimates will be too cold (and vice versa). Neglecting changes in moisture source and using a constant temporal isotope-temperature slope of half the spatial slope (32) is therefore inadequate to reconstruct past Greenland temperatures from δ18O and could induce an overestimation of some rapid-events temperature change by up to 40% (Fig. 2 and Table 1). In other words, the apparent isotope-temperature slope varies at all time scales (13).

Source temperature changes, ΔTsource (Fig. 2), mimic the initial excess record (Fig. 1) with a glacial-interglacial amplitude of ∼6°C. Rapid Tsource changes of 2° to 4°C occur simultaneously but in antiphase with rapid Tsite events, which is remarkable given that these two climate variables appear in phase at longer orbital scales; the large amplitude of rapid events in deuterium excess is partly due to large changes in Greenland temperature itself (21) and is less marked after isotopic inversion in Tsource. As is the case for Antarctica, an imprint of obliquity fluctuations in deuterium excess and source temperature can be seen, although this is limited to the period from 20 to 80 ka. The mechanisms at work are probably the same as in Antarctica. In low latitudes, a low obliquity is associated with a high local mean annual insolation, which should result in higher SST [as recently suggested by a modeling experiment (33)] and thus in a more intense evaporation. A low obliquity also implies a decrease in high-latitude insolation and temperature (34). The resulting increased insolation gradient is associated with a more intense meridional temperature gradient (Fig. 2) and a more intense atmospheric transport (35). These two effects together yield a dominant role for warm low-latitude sources when obliquity is low, thus explaining the observed link between deuterium excess and obliquity. However, such a link is not observed between 20 and 10 ka and before 80 ka, possibly because these two periods—which correspond to large ice sheet changes (deglaciation and glacial inception, respectively)—are characterized by changes in Northern Hemisphere stationary waves forced by ice sheet growth or decay. Finally, high obliquities (e.g., at 30 and 70 ka) correspond to a high polar amplification (ratio of long-term changes in Tsite to Tsource up to 6), whereas periods with low obliquity (e.g., at 10, 50, and 90 ka) coincide with a reduced polar amplification (ratio of change around 2).

North Atlantic SST records (36) show large glacial-interglacial fluctuations, with thermal amplitudes reaching typically ∼10°C at 45°N and ∼5°C at 35°N (37), significantly higher than the glacial-interglacial source temperature change reconstructed here. A detailed inspection of ΔTsource (Fig. 2), which resembles the initial deuterium excess record (Fig. 1), also points to important differences at millennial time scales. High-resolution North Atlantic SST records exhibit rapid changes generally in phase with Greenland D/O events recorded in Tsite, whereas Δ Tsource reconstruction suggests an out-of-phase relation between Tsource and Tsite during rapid changes.

Our proposed interpretation is that these noticeable differences (amplitude of LGM-to-modern changes and millennial-scale events) result from drastic changes in the polar front, the geographical location of Greenland's main moisture sources, and the atmospheric water cycle during glacial times (5). When Greenland is cold and surrounded by an extensive sea ice cover, mid-latitude oceans are much colder than today and cannot provide much moisture to Greenland. Evaporation is, however, maintained at lower subtropical and tropical locations, providing precipitation in central Greenland largely in summer. Typically, a southward moisture source shift of 5° in latitude is compatible both with the LGM ΔTsite values and with local summer SST reconstructions. This is also consistent with temperature and salinity latitudinal profiles estimated from marine sediments, reflecting the shift of the dominant evaporative areas during rapid events (38).

Such a large-scale reorganization of the hydrological cycle at both orbital and millennial time scales is indirectly confirmed by the calcium composition of GRIP ice, a parameter reflecting (i) the strength of GRIP dust sources mainly provided by Chinese loess areas, and (ii) the efficiency of dust transport to Greenland (39). The strong correlation between log(Ca) and δ18O of ice was previously noted (39), but the similarity is even better with this reconstructed site-to-source temperature gradient (R2 = 0.86 at 100-year time step and R2 = 0.88 at 5000-year time step between 8 and 100 ka). In particular, a warmer site and a colder source at ∼50 to 55 ka result in a decreased meridional temperature gradient, exactly at the time of minimum calcium concentration. The meridional temperature gradient also shows a 40,000-year modulation paralleling obliquity fluctuations (Fig. 1). We have already pointed out that mean annual insolation, and thus obliquity, strongly controls the meridional atmospheric circulation. We suggest that they also indirectly control the strength of the dust source: A larger obliquity should correspond to a decreased annual mean tropical ocean temperature and an increased land-sea contrast in summer, and could enhance the summer monsoons, thereby decreasing the continental dust sources.

Our interpretation of the δ18O and d GRIP data provides a consistent picture of changes occurring over the last 100,000 years in Greenland and in the North Atlantic. Our findings confirm model results by showing that when seasonality is accounted for, reasonable local temperature estimates can be drawn from the GRIP isotopic record; the correction due to source temperature changes is of lesser importance at glacial-interglacial scales than during rapid events. Moreover, the comparison between our estimate of ΔTsource and available North Atlantic sediment-based SST reconstructions suggests that large changes in geographical moisture source location occur both at the orbital and millennial scales. We show that ΔTsource reflects obliquity changes and that ΔTsource and ΔTsite are of opposite sign, both at orbital and millennial time scales. The influence of obliquity on deuterium excess and moisture origin, already identified for Antarctica, is confirmed for Greenland. When cold conditions prevail in the mid- and high latitudes, the moisture origin shifts to milder southward locations (5). Finally, we point to striking similarities between the calcium-dust records and the site-to-source temperature gradient; both are strongly modulated by obliquity, and the coupled climate model results suggest that obliquity could be linked with dust source areas through the land-sea temperature contrast. At the millennial time scale, the site-to-source temperature fluctuations highlight large-scale changes in atmospheric circulation, which is consistent with the observation of simultaneous rapid climate changes at polar, temperate, and tropical latitudes (40) also recorded in Greenland ice chemistry and methane fluctuations (41). Modeling studies have indeed shown that Northern Hemisphere storm tracks are influenced not only by the topography of the ice sheets but also by the sea-ice extent and the meridional temperature gradients (30).

Such large changes in the atmospheric hydrological cycle and associated climate feedbacks are not fully represented in the intermediate-complexity climate models commonly used to understand the mechanisms of abrupt events. Nonetheless, they could play a key role in the generation of instabilities of the ice sheets and the ocean circulation, amplified by changes in sea-ice extent, as has been suggested for the last glacial inception (42).

Supporting Online Material

www.sciencemag.org/cgi/content/full/309/5731/118/DC1

Materials and Methods

Table S1

References and Notes

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