Literature DB >> 31477737

Consistently dated Atlantic sediment cores over the last 40 thousand years.

Claire Waelbroeck1, Bryan C Lougheed2, Natalia Vazquez Riveiros2,3, Lise Missiaen2, Joel Pedro4, Trond Dokken4, Irka Hajdas5, Lukas Wacker5, Peter Abbott6,7, Jean-Pascal Dumoulin2,8, François Thil2, Frédérique Eynaud9, Linda Rossignol9, Wiem Fersi2, Ana Luiza Albuquerque10, Helge Arz11, William E N Austin12, Rosemarie Came13, Anders E Carlson14, James A Collins15, Bernard Dennielou3, Stéphanie Desprat9,16, Alex Dickson17, Mary Elliot18, Christa Farmer19, Jacques Giraudeau9, Julia Gottschalk20, Jorijntje Henderiks21, Konrad Hughen22, Simon Jung23, Paul Knutz24, Susana Lebreiro25, David C Lund26, Jean Lynch-Stieglitz27, Bruno Malaizé9, Thomas Marchitto28, Gema Martínez-Méndez29, Gesine Mollenhauer29, Filipa Naughton30,31, Silvia Nave32, Dirk Nürnberg33, Delia Oppo22, Victoria Peck34, Frank J C Peeters35, Aurélie Penaud36, Rodrigo da Costa Portilho-Ramos37, Janne Repschläger38, Jenny Roberts39, Carsten Rühlemann40, Emilia Salgueiro30,31, Maria Fernanda Sanchez Goni9,16, Joachim Schönfeld33, Paolo Scussolini35, Luke C Skinner41, Charlotte Skonieczny42, David Thornalley43, Samuel Toucanne3, David Van Rooij44, Laurence Vidal45, Antje H L Voelker30,31, Mélanie Wary46, Syee Weldeab47, Martin Ziegler48.   

Abstract

Rapid changes in ocean circulation and climate have been observed in marine-sediment and ice cores over the last glacial period and deglaciation, highlighting the non-linear character of the climate system and underlining the possibility of rapid climate shifts in response to anthropogenic greenhouse gas forcing. To date, these rapid changes in climate and ocean circulation are still not fully explained. One obstacle hindering progress in our understanding of the interactions between past ocean circulation and climate changes is the difficulty of accurately dating marine cores. Here, we present a set of 92 marine sediment cores from the Atlantic Ocean for which we have established age-depth models that are consistent with the Greenland GICC05 ice core chronology, and computed the associated dating uncertainties, using a new deposition modeling technique. This is the first set of consistently dated marine sediment cores enabling paleoclimate scientists to evaluate leads/lags between circulation and climate changes over vast regions of the Atlantic Ocean. Moreover, this data set is of direct use in paleoclimate modeling studies.

Entities:  

Year:  2019        PMID: 31477737      PMCID: PMC6718518          DOI: 10.1038/s41597-019-0173-8

Source DB:  PubMed          Journal:  Sci Data        ISSN: 2052-4463            Impact factor:   6.444


Background & Summary

In order to decipher the mechanisms at play in observed past climate changes, it is necessary to establish a common temporal framework for paleoclimate records from different archives and from different locations. Determining the lead/lag relationships between different climatic and circulation changes can help to identify the underlying causes and foster development of conceptual hypotheses to be tested with climate model simulations. Also, paleoclimate data-model integration studies, such as groundtruthing of transient modeling analyses, timeslice comparisons of proxy data, or data assimilation, necessitate consistent paleoclimate records chronologies in calendar years. Here we focus on the last 40 ky because it is the time span covered by radiocarbon dating and the sole period for which it is possible to establish calendar age timescales for marine cores with a precision approaching that of ice core or speleothem records. Radiocarbon dating of marine records is complicated, however, by a difference between the surface water 14C/12C ratio (expressed as ∆14C, in ‰) and that of the contemporaneous atmosphere, due to the balance between the input of atmospheric 14C and its removal by radioactive decay in the water column, advection, and mixing with older waters. This difference in ∆14C is termed the “reservoir age” of the surface waters. Previous studies have revealed that surface reservoir ages have not remained constant over time at high latitudes of the North Atlantic and Southern Ocean (i.e. poleward of ~38°N and of ~40°S) due to changes in the location and vigour of deep-water formation[1-4]. In those high-latitude regions, it is thus necessary to use an alternative dating strategy in lieu of 14C dating of marine organisms. Here we adopt a strategy that has been widely applied (e.g. refs[4-7]) and has been adopted by the INTIMATE (Integration of Ice core, Marine and Terrestrial records of the North Atlantic) group when surface reservoir ages can not be assessed[8]. This strategy consists of synchronizing the sea surface temperature (SST) signal recorded in marine cores with the air temperature signal recorded in polar ice cores. This dating approach is based on the observed thermal equilibrium between the ocean’s surface water and overlying air. Previous studies have demonstrated that changes in air and sea surface temperature were synchronous across the last deglaciation[9] and some of the last glacial rapid climate changes[10] over the North Atlantic region. Moreover, modeling studies of the last deglaciation[11] or last glacial millennial climate changes[12,13] show that both increases and decreases in North Atlantic (Southern Ocean) SST and in air temperature above Greenland (Antarctica) are synchronous. Currently, the Greenland NorthGRIP (NGRIP) ice core can be considered the best-dated continuous continental paleoclimatic archive over the last 50 to 75 ky. The NGRIP Greenland Ice Core Chronology 2005 (GICC05) calendar age scale has been established by annual layer counting with estimated uncertainties of 50 y at 11 calendar ky BP (i.e. calendar ky before 1950, noted ka hereafter), 100 to 450 y for the 11–30 ka interval, and 450 to 800 y for 30–40 ka[14] (y or ky referring to durations and ka to dates). Moreover, a common chronology for Greenland and Antarctica ice cores has been developed based on their records of 10Be and atmospheric CH4 concentration[15,16]. This dating effort yielded the Antarctic AICC2012 age scale for four Antarctic ice cores, which is fully consistent with the GICC05 age scale over the last 60 ky[16]. Using the GICC05 and AICC2012 age scales as alignment targets for high latitude SST records of the north and south hemispheres respectively, it is thus possible to directly compare marine records from both hemispheres on a common time frame. Here, we present the first set of consistently dated Atlantic sediment cores from 92 locations distributed between 68°N and 53°S, and between 400 and 5000 m water depth (Fig. 1, Online-only Table 1, ref.[17]), together with consistently derived dating uncertainties. This new data set enables paleoclimate scientists to (i) examine relative phases between Atlantic records (e.g. planktonic and benthic oxygen and carbon isotopes, Pa/Th); and (ii) use the spatial and temporal changes recorded in Atlantic sediments to constrain paleoclimate model simulations.
Fig. 1

Location of the 92 dated Atlantic sediment cores (see Online-only Table 1 for precise coordinates and water depths of the cores). The figures were generated using the Ocean Data View software[53], the ETOPO bathymetry[54] (left panel), and the WOA13 mean annual salinity[55] along a mid-Atlantic north-south section (right panel). The salinity section illustrates the distribution of the cores with respect to the main modern water masses.

Online-only Table 1

Dated cores and dating methods used outside of the Holocene.

Core nameLatitude, decimal degreesLongitude, decimal degreesDepth, mReferencesEntirely AMS-basedSST alignment to NGRIPMS aligment to NGRIPSST alignment to EDMLCombined AMS + SST alignment to NGRIPCombined AMS + alignment to speleothemsUse of tephra chronological markers
PS2644-567.87−21.77777Refs. [62,63]XX
MD95-201066.684.571226Refs. [64,65]XX
RAPID-10-1P62.98−17.591237Ref.[66]XX
ENAM93-2162.74−4.001020Refs. [67,68]XX
MD99-228462.37−0.981500Refs. [43,69]X
SU90-2462.07−37.032085Ref.[70]X
RAPID-17-5P61.48−19.542303Ref.[66]XX
MD95-201460.58−22.082397Ref.[71]X
ODP Site 98360.40−23.641984Refs. [72,73]X
V29-20260.38−20.972658Ref.[74]X
MD99-228160.34−9.461197Refs. [57,58]X
SO82-5-259.17−30.911416Refs. [75,76]XX
DAPC258.97−9.611709Ref.[77]X
MD95-200657.03−10.062122Ref.[8]XX
NA87-2255.50−14.702161Refs. [3,7,78,79], this studyX
GIK23415-953.18−19.152472Refs. [65,80,81]XX
MD01-246151.75−12.921153Refs. [39,65,82,83]XX
DSDP Site 60949.88−24.233883Refs. [84,85]XX
MD95-200247.45−8.532174Refs. [86,87]X
MD04-284545.35−5.224175Refs. [59,60]X
SU92-0343.20−10.113005Ref.[88]X
SU90-0843.05−30.043080Ref.[78]X
MD03-269742.16−9.702164Refs. [89,90]X
MD99-233142.15−9.682120Refs. [40,91,92]X
CH69-K0941.76−47.354100Ref.[93]X
MD95-204040.58−9.862465Refs. [88,94,95]X
MD95-203940.58−10.353381Refs. [91,94]X
MD03-269838.24−10.394602Ref.[96], this studyX
GEOFAR-KF1638.00−31.133050Ref.[97]X
MD08-3180Q38.00−31.133064Refs. [98,99]X
MD95-204137.83−9.521123Refs. [40,91,100]X
MD95-204237.80−10.173146Refs. [91,101103]X
MD99-2334K37.80−10.173146Refs. [104,105]X
SU81-1837.77−10.183135Refs. [3,106]X
GEOFAR-KF1337.58−31.842690Ref.[107]X
MD95-203737.09−32.032159Refs. [108,109], this studyX
S94-2-KS0436.87−29.183400this studyX
KNR197-10-17GGC36.41−48.545010Ref.[110]X
M39008-336.38−7.07577Refs. [111,112]X
MD08-3227G35.27−6.80642Ref.[113], this studyX
GIK15669-134.89−7.822022Ref.[114]X
MD04-2805Q34.52−7.02859Ref.[115], this studyX
OCE326-GGC533.70−57.584550Refs. [116,117]X
KNR31-GPC533.69−57.634583Refs. [7,118,119]X
KNR140-51GGC32.78−76.281790Refs. [120,121]X
ODP Site 106030.77−74.473481Refs. [28,122]X
MD02-257529.00−87.12847Refs. [123,124]X
GeoB4240-228.89−13.231358Ref.[125]X
GeoB5546-227.54−13.741172Refs. [126,127]X
OCE205-2-100GGC26.10−78.001045Ref.[128]X
OCE205-2-103GGC26.07−78.06965Refs. [129131]X
GIK12392-125.17−16.852575Refs. [80,132]X
KNR166-2-26JPC24.33−83.25546Refs. [133135]X
KNR166-2-29JPC24.28−83.27648Ref.[133]X
KNR166-2-31JPC24.22−83.30751Refs. [133,136]X
KNR166-2-73GGC23.74−79.43542Ref.[133]X
GeoB7920-220.75−18.582278Refs. [137,138]X
MD03-270518.08−21.153085Refs. [139,140]X
CHO288-5417.43−77.661020this studyX
GeoB9508-515.50−17.952384Ref.[141]X
GeoB9526-512.43−18.053233Ref.[142]X
M35003-412.09−61.241299Ref.[143]X
ODP Site 100210.71−65.17892Ref.[144]X
GeoB16224-16.65−52.082510Refs. [145,146]X
EW9209-1JPC5.90−44.194056Ref.[130]X
GeoB1515-14.24−43.073129Refs. [147,148]X
CH22-KW313.525.571181Ref.[149]X
MD03-27072.509.401295Ref.[150]X
GeoB16206-1−1.58−43.021367Refs. [145,146]X
GeoB16202-2−1.91−41.592247Ref.[151]X
MD09-3256Q−3.55−35.393537Ref.[152], this studyX
GS07-150-17/1GC-A−4.22−37.081000Refs. [145,153]X
MD09-3246−4.23−37.10892this studyX
GeoB3910-2−4.25−36.352362Refs. [25,154,155]X
ODP Site 1078C−11.9213.40426Ref.[156]X
GeoB1023-5−17.1611.011978Ref.[157]X
GeoB3202-1−21.62−39.981090Ref.[158]X
GeoB1711−23.3212.381967Refs. [148,159]X
MD08-3167−23.3212.381948Ref.[160], this studyX
GL1090−24.90−42.502225Ref.[161]X
ODP Site 1084−25.5113.031992Ref.[162]X
GeoB6201-5−26.67−46.44475Ref.[163]X
KNR159-5-36GGC−27.50−46.501268Ref.[131]X
KNR159-5-42JPC−27.76−46.632296Ref.[164]X
GeoB1720-2−29.0013.841997Ref.[165]X
MD02-2592−32.0914.472869this studyX
MD02-2594−34.7117.342440Ref.[166]X
MD16-3511Q−35.3629.244435this studyX
TNO57-21−41.107.804981Ref.[167]X
MD02-2588Q−41.3325.832907Ref.[168]X
MD07-3076Q−44.15−14.223770Refs. [4,169]X
JR244-GC528 *−53.01−58.04598Ref.[170]X

*14C dates calibrated using reservoir ages at 600 m water depth, based on deep sea coral data given in ref.[170].

Location of the 92 dated Atlantic sediment cores (see Online-only Table 1 for precise coordinates and water depths of the cores). The figures were generated using the Ocean Data View software[53], the ETOPO bathymetry[54] (left panel), and the WOA13 mean annual salinity[55] along a mid-Atlantic north-south section (right panel). The salinity section illustrates the distribution of the cores with respect to the main modern water masses.

Methods

We compiled existing paleoceanographic data from Atlantic sediment cores covering part of or the entire 0–40 ka interval, with sedimentation rates of at least 5 cm/ky, for which there exists the following dating means: radiocarbon dates for mid and low latitudes sediment cores, and SST or magnetic records for sediment cores located poleward of ~38°N and ~40°S. New cores were added to fill gaps with respect to the available geographical and water depth coverage, and additional radiocarbon dates were produced to improve the existing age models of some cores (Online-only Table 1). In mid and low latitudes (i.e. between ~40°S and ~38°N), reservoir ages can be assumed not to have strongly varied in response to ocean circulation changes of the last glacial and deglaciation. The same is true at all latitudes during the Holocene. Thus, in mid and low latitudes, and during the Holocene at higher latitudes, the sediment cores were dated by means of calibrated radiocarbon ages. For this, 1427 published and 104 new radiocarbon dates have been calibrated using the Bayesian calibration program “MatCal”[18], and the IntCal13 and SHCal13 calibration curves[19,20] for North and South Atlantic cores, respectively. We accounted for both spatial and temporal variability in 14C reservoir ages. To estimate spatial variations in reservoir ages we extracted bomb-corrected reservoir ages from the GLobal Ocean Data Analysis Project for Carbon (GLODAP) data set[21]. Prior to extracting these surface reservoir ages, GLODAP data were re-gridded to a 4° × 4° grid, whereby the mean and standard deviation for the GLODAP data points from the upper 250 m for each 4° × 4° grid cell were calculated. The modern surface water reservoir age at a given site is then obtained from the nearest grid node to the core site (Fig. 2). In the case of certain sites that are out of range of the GLODAP grid, such as those in the Gulf of Mexico, we have extrapolated the GLODAP 4°x4° grid to these areas. This spatially varying component of the reservoir age is subtracted from the laboratory 14C age before calibration (with error propagation). The error used for this spatial reservoir age component is either the computed GLODAP standard deviation, or 100 14C yr, whichever is greater. For pre-Holocene dates, a minimum of 200 14C yr is used instead of 100 14C yr.
Fig. 2

Average reservoir age extracted from the GLODAP data re-gridded to a 4° × 4° grid and averaged over the upper 250 m of the water column. These values can be downloaded from Figshare[56].

Average reservoir age extracted from the GLODAP data re-gridded to a 4° × 4° grid and averaged over the upper 250 m of the water column. These values can be downloaded from Figshare[56]. To also consider temporal changes in reservoir age, we further applied a correction to account for the impact of atmospheric CO2 concentration changes upon surface water 14C activity. At the Last Glacial Maximum (LGM), the lower atmospheric CO2 concentration induced an increase in atmospheric ∆14C of ~30‰ due to the speciation change, everything else being equal[22]. This ~30‰ increase in atmospheric ∆14C in turn caused a ~250 y increase in surface water reservoir ages[22]. To account for this temporal change in surface reservoir age, we linearly scaled a reservoir age correction to atmospheric pCO2, whereby a correction of 0 14C y corresponds to present day pCO2, and 250 14C y to LGM pCO2. For pCO2 values, we consulted the composite atmospheric CO2 record of Antarctic ice cores[23]. This age-dependent component of the reservoir age is added to the IntCal13 (or SHCal13) 14C age record before calibration. Even in regions where surface reservoir ages can be predicted based on the evolution of atmospheric CO2, as described above, increased uncertainties in radiocarbon-dated chronologies can still arise from bioturbation biases (e.g. ref.[24]). Thus, in the best cases, when bioturbation biases and local changes in past surface reservoir ages remain limited, sediment core dating uncertainties mainly arise from the conversion of radiocarbon ages into calendar ages. In these cases, uncertainties are less than 150 y for the time interval 0–11 ka, of about 400 y for the 11–30 ka interval, and of 600 to 1100 y for the 30–40 ka interval[19]. In all other cases, dating uncertainties are larger. Almost all our age-depth models of low- and mid-latitude cores (51 out of the 92 cores, see Online-only Table 1) are entirely based on calibrated 14C ages. In three cores (GeoB3910, MD09-3246 and MD09-3256Q), located on the Brazilian margin in a region under the influence of the Intertropical Convergence Zone, it is possible to take advantage of the simultaneous recording of rainfall increases during Greenland stadial periods in the marine cores and in U-Th dated speleothems from the adjacent continent to improve the marine age models. Rainfall increases are recorded both by XRF-Ti/Ca peaks in the marine cores, and by δ18O decreases in the speleothems[25]. By aligning the XRF-Ti/Ca in the marine cores to the speleothem δ18O, it is possible to improve the precision of the marine age models around 40 ka and to extend them beyond the limit of 14C dating. Importantly, the speleothem record from El Condor cave[26], to which we have aligned the three marine cores, has been shown to be in phase, within dating uncertainties, with the NGRIP air temperature record in the GICC05 age scale[25,27]. Our alignment of GeoB3910, MD09-3246 and MD09-3256Q marine cores to El Condor speleothem is thus consistent with the NGRIP GICC05 age scale. For cores located north of ~38°N (26 cores) and south of ~40°S (2 cores), and ODP Site 1060 for which there exist no 14C dates but where planktonic foraminifer census counts exhibit a clear NGRIP signal[28], we have used calibrated radiocarbon ages only over the Holocene portion (i.e. after the end of the Younger Dryas, dated at 11.65 ka in the GICC05 age scale[29]), and aligned their glacial and deglacial portions to NGRIP or EPICA Dronning Maud Land (EDML) air temperature signal. We used different types of chronological markers to derive these 29 age-depth models: Tie points defined by aligning high latitude SST records to NGRIP air temperature proxy record on the GICC05 age scale for North Atlantic cores, and to EDML air temperature on the AICC2012 age scale for South Atlantic cores; Tie points defined by aligning magnetic properties of northern North Atlantic and Nordic Seas cores to the NGRIP air temperature signal on the GICC05 age scale; Dated tephra layers. The dating procedures (1)-(3) are described in detail below. The alignment procedures (1) and (2) by essence impede the assessment of leads and lags between the aligned records. For instance, leads/lags between SST and polar air temperatures, or among SST records from high latitude marine cores, are by construction not significantly different from zero. In contrast, this dating approach gives access to the relative timing of circulation changes recorded at different water depths in cores located on depth transects. (1) We aligned SST records to polar ice core air temperature proxy records using the AnalySeries program[30]. NGRIP alignment targets correspond to the rapid transitions out of and into Greenland stadials, as dated and listed in refs[29,31] (Online-only Table 2). Tie points were generally defined by aligning rapid warmings recognized in both the ice core and marine core, as recommended in ref.[8]. In rare cases, rapid and well-defined coolings have been aligned. In a few cases, when the SST record resolution was too low or the signal shape ambiguous, maxima or minima have been aligned. Remaining ambiguities in the identification of alignment tie points were solved in most cases by fulfilling the condition that the tie point age is younger or equal to the calibrated 14C ages obtained by assuming no other change in surface reservoir age than the temporal evolution due to changing atmospheric pCO2. Not fulfilling this condition would result in negative surface reservoir ages, which is not physically possible (see Supplementary Fig. 1 for an example).
Online-only Table 2

Alignment targets.

EventReference record*Age, cal. ky BP (ka)Age, ky b2k1 sigma, kyReference
Saksunavatn ash layer10.29710.3470.045Ref.[46]
end of YDNGRIP δ18O11.65311.7030.050Ref.[29]
Vedde ash layer12.12112.1710.057Ref.[46]
start of YDNGRIP δ18O12.84612.8960.250Ref.[31]
end of HS1 (or start of GI-1)NGRIP δ18O14.64214.6920.093Ref.[29]
start of HS1NGRIP Ca++17.48017.5300.206Ref.[33]
end of HS2 (or start of GI-2)NGRIP δ18O23.29023.3400.298Ref.[29]
end of warm event within GS-3NGRIP Ca++24.124.150.33Ref.[35]
start of warm event within GS-3NGRIP Ca++25.0525.10.35Ref.[35]
FMAZ-II ash layer26.69026.7400.390Refs. [46,47]
start of GI-3NGRIP δ18O27.73027.7800.416Ref.[29]
end of HS3 (or start of GI-4)NGRIP δ18O28.85028.9000.449Ref.[29]
start of HS3NGRIP δ18O30.55030.6000.566Ref.[31]
start of GI-5.1NGRIP δ18O30.79030.8400.566Ref.[31]
end of GI-5.2 (or start of GS-5.2)NGRIP δ18O31.99032.0400.566Ref.[31]
start of GI-5.2NGRIP δ18O32.45032.5000.566Ref.[29]
end of GI-6 (or start of GS-6)NGRIP δ18O33.31033.3600.606Ref.[31]
start of GI-6NGRIP δ18O33.69033.7400.606Ref.[29]
end of GI-7 (or start of GS-7)NGRIP δ18O34.69034.7400.661Ref.[31]
start of GI-7NGRIP δ18O35.43035.4800.661Ref.[29]
end of GI-8a (start of GS-8)NGRIP δ18O36.53036.5800.725Ref.[31]
start of GI-8aNGRIP δ18O36.81036.8600.725Ref.[31]
end of HS4 (or start of GI-8)NGRIP δ18O38.17038.2200.725Ref.[29]
start of HS4 (or start of GS-9)NGRIP δ18O39.85039.9000.790Ref.[31]
start of GI-9NGRIP δ18O40.11040.1600.790Ref.[29]
end of GI-10 (or start of GS-10)NGRIP δ18O40.75040.8000.817Ref.[31]
start of GI-10NGRIP δ18O41.41041.4600.817Ref.[29]
end of GI-11 (or start of GS-11)NGRIP δ18O42.19042.2400.868Ref.[31]
start of GI-11NGRIP δ18O43.29043.3400.868Ref.[29]
end of GI-12 (or start of GS-12)NGRIP δ18O44.23044.2800.956Ref.[31]
end of HS5 (or start of GI-12)NGRIP δ18O46.81046.8600.956Ref.[29]
start of HS5NGRIP δ18O48.29048.3401.000Ref.[31]
start of GI-13NGRIP δ18O49.23049.2801.015Ref.[29]
start of GI-14NGRIP δ18O54.17054.2201.150Ref.[29]
NAAZ II ash layer55.33055.3801.184Ref.[46]
start of GI-15NGRIP δ18O55.75055.8001.196Ref.[29]
start of GI-16NGRIP δ18O58.23058.2801.256Ref.[29]
start of GI-17NGRIP δ18O59.39059.4401.287Ref.[29]
beyondNGRIP δ18Obeyondbeyond1.500guess

*NGRIP δ18O or air temperature versus GICC05[61,171]; NGRIP Ca++ [61].

SST alignment to Antarctic temperature variations was made at marked transitions in the temperature record, such as Antarctic Isotopic Maxima[32], the onset of the early and late deglacial warming, or the beginning of the Antarctic Cold Reversal. In addition, we used the following three alignment targets in the North Atlantic: A first alignment target is based on the observation that the cooling marking the beginning of Heinrich Stadial 1 in three independently dated North Atlantic cores is synchronous with the sharp increase in dust flux recorded in the Greenland ice cores and dated at 17.48 ka ± 0.21 ky on the GICC05 age scale[33]. This observation is consistent with this cooling being coeval with an increase in dust transport from Asia to Greenland, as observed during other Greenland stadials[34]. Two other alignment targets correspond to the beginning and the end of the warm event identified in ref.[35] within Greenland stadial 3 (GS-3) in several North Atlantic cores between 24 and 25 ka. This warm event within GS-3 is not clearly recorded in Greenland ice (δ18O) or gas (δ15N) isotopic records, but corresponds to a marked decrease in dust flux. Here again, we aligned the beginning and end of the warm event to the corresponding changes in the NGRIP dust flux dated on the GICC05 age scale at 25.05 ka ± 0.35 ky and 24.1 ka ± 0.33 ky, respectively. For consistency, the alignment tie points in high latitude cores were all defined by the same person. Similarly, one single person defined all the alignment tie points in the three Brazilian cores. Also, the SST records used in the present study are all based on planktonic foraminifer census count data. When SST reconstructions based on full census count data were not available, we used the percentage of the polar species Neogloboquadrina pachyderma (left coiling) as a proxy for SST. This approach has been described and validated in a number of studies (e.g. refs[36-39]). In two North Atlantic cores (ODP Site 1060 and core MD08-3180Q) we used the percentage of warm species instead, because the percentage of N. pachyderma was too low. In the particular case of the Iberian margin, it has been shown that Globigerina bulloides δ18O co-varies with SST[40,41] and we have used G. bulloides δ18O as a proxy for SST when no SST estimates were available. Both age and depth uncertainties are defined for each tie point. The depth uncertainty directly depends on the sampling resolution of the SST curve: it is taken as half of the depth interval corresponding to the rapid warming (or more rarely cooling), or as half of the width of the SST maximum or minimum, when maxima or minima have been aligned. In instances of ambiguities that could not be tested by the constraints provided by 14C dates, we attributed an uncertainty to the depth of the tie point, large enough to encompass the two events (warmings, or more rarely, coolings or SST maxima or minima) which could both be aligned to the same target. The uncertainty on the tie point ages is the GICC05 dating precision of the transitions between Greenland stadials and interstadials, with one sigma uncertainties defined as half the cumulative ‘maximum counting error’ in the GICC05 age scale[29,31]. Similarly, the dating uncertainty of the alignment tie points defined with respect to AICC2012 is the dating error given in ref.[16]. (2) In high northern latitudes, when SST records are not available, for some cores it is possible to instead use high-frequency variations in magnetic susceptibility (MS) recorded during the last glacial period. The rapid oscillations in magnetic properties in sediment cores on the flow path of North Atlantic Deep Water (NADW) in the Nordic Seas and North Atlantic have indeed been shown to be in phase with the Greenland ice δ18O or air temperature signal[42]. Support for this synchronicity comes from tephra and geomagnetic field (Laschamp inclination excursion) marine records. These marine records become aligned with tephra and cosmogenic nuclide Greenland records when the MS tuning to Greenland is applied (e.g. refs[43-45]). We dated five cores located north of 62°N by aligning their MS records to the NGRIP ice δ18O signal (Online-only Table 1). MS tie points and their associated uncertainties were defined using the same method as described for the alignment of SST signals to ice core records. The MS records of four of these five cores have been previously shown to be in phase with the Greenland air temperature signal[42]. More recently, the identification of tephra layers in core MD99-2284 demonstrated that this core’s MS record is also in phase with the NGRIP δ18O record[43]. This can be explained by the fact that changes in MS arise from changes in the efficiency of the transport of fine grained magnetic particles by deep currents from the source to the site of deposition[42]. The fact that the MS signal is in phase in cores located north and south of the sills separating the Nordic Seas from the North Atlantic basin, suggests that the source of magnetic minerals could be at the sills, with the strength of the overflow from the Nordic Seas directly proportional to the strength of the inflow into the Nordic Seas. (3) We used dated tephra layers as additional chronological markers over the last 55 ky in 10 of the northernmost cores (Online-only Table 1). The following four tephra layers have been recognized both in Greenland ice cores and in certain North Atlantic and Nordic Seas marine cores: the Saksunarvatn Ash[46], the Vedde Ash[46], the Faroe Marine Ash Zone (FMAZ) II[46,47], and the widespread rhyolitic component of North Atlantic Ash Zone (NAAZ) II (II-RHY-1)[46,48] (Online-only Table 2). Age-depth relationships were built for each core accounting for both the age and depth uncertainties of the 14C dates and chronological markers, using the age-depth modeling routine “Undatable”[49] (Fig. 3). This new rapid age-depth modeling routine was ideal for this project as it allowed us to run and re-run age models for the many sediment cores that we have analyzed. Moreover, this age-depth modeling routine computes a conservative age-depth uncertainty, through the provision of bootstrapping and sediment accumulation rate uncertainty[49] (Fig. 3). Default values for bootstrapping percentage and sedimentation rate uncertainty were set to 10% and 0.1 respectively. In the presence of age reversals, we progressively increased the bootstrapping percentage in order to make sure that the dating uncertainty computed by Undatable was large enough to encompass most calibrated 14C ages, leaving out only outliers beyond 2 sigma dating uncertainty. This way, we take into account increased dating uncertainty associated with the existence of age-depth scatter, which may be related to sedimentation hiatuses, abundance changes, or bioturbation. Also, we considered tephra layers as the most reliable age-depth constraints and, therefore, a priori excluded them from the bootstrapping process (e.g. ref.[50]).
Fig. 3

Example of age-depth plot produced by Undatable. Age-depth model produced for North Atlantic core RAPID-10-1P with bootstrapping set to 10% and sedimentation rate uncertainty set to 0.1 (see ref.[49] for details). Blue, yellow and red probability density functions indicate the radiocarbon and alignment tie points, and tephra age-depth constraints, respectively. The grey cloud indicates the probability density cloud of the age-depth model, whereby darker colors indicate higher age-depth probability. The blue and black broken lines represent 68.27% and 95.45% confidence intervals, respectively. The red line indicates the age-depth model median.

Example of age-depth plot produced by Undatable. Age-depth model produced for North Atlantic core RAPID-10-1P with bootstrapping set to 10% and sedimentation rate uncertainty set to 0.1 (see ref.[49] for details). Blue, yellow and red probability density functions indicate the radiocarbon and alignment tie points, and tephra age-depth constraints, respectively. The grey cloud indicates the probability density cloud of the age-depth model, whereby darker colors indicate higher age-depth probability. The blue and black broken lines represent 68.27% and 95.45% confidence intervals, respectively. The red line indicates the age-depth model median. In some North Atlantic cores (7 out of 92, cf. Online-only Table 1), we used 14C dates together with SST alignment tie points to NGRIP. These cores are located at the northern edge of the region where surface reservoir ages may be assumed not to have strongly varied in response to ocean circulation changes, and are characterized by large changes in SST which parallel the NGRIP ice δ18O signal. In those cores, we used alignment tie points to complement calibrated 14C dates when the latter were too sparse. Finally, although the focus of this work is the time interval 0–40 ka, we used dating information available beyond 40 ka to ensure the robustness of the computed sedimentation rate and age-depth relationship around 40 ka.

Data Records

The present set of age-depth models contains three text files per marine sediment core[17]. The first text file (“age depth input”) contains an overview of the 14C ages and other age constraints used in the age-depth model. More specifically, a first section provides all the available 14C raw data, the reservoir age and calibration curve used, as well as the calibrated ages together with the 68.3% highest posterior density interval(s), and specifies which 14C dates have been used to generate the age-depth model. A second section provides the definition of the alignment tie points: the tie points depth and its uncertainty, the tie points age and its uncertainty, the nature of the tie points and the nature of the uncertainty of the tie points age. The second text file (“udinput”) contains the input for the age-depth model in the Undatable format. The third text file (“_admodel_ka”) contains the computed age-depth relationship and associated dating uncertainties. In addition to the complete set of data records archived on Seanoe[17], the 92 “_admodel_ka” text files can be found on Pangaea[51]. Notably, the fact that the 14C raw data are provided makes the present data set easy to update using a future 14C calibration curve. Also, tie point depths are provided, allowing updates of the age-depth models if higher resolution SST records are produced. In addition to these three text files, the age-depth model plot produced by the Undatable routine (see Fig. 3 for an example) is provided for each core, as well as a plot of the aligned SST or MS record, ice core record, and chosen alignment tie points (see Fig. 4 for an example) for the cores which have been partially or completely dated by alignment to an ice core record[17].
Fig. 4

Example of North Atlantic and Nordic Seas cores dated by alignment of their SST records to the NGRIP ice δ18O signal. Top panel: planktic foraminifer-based warm season surface temperature of core MD99-2281[57,58]; middle panel: % N. pachyderma of core MD99-2281 and MD04-2845[59,60] (both panels: diamonds and squares above the x-axis indicate calibrated 14C ages and alignment tie points, respectively). Bottom panel: NGRIP ice δ18O record on the GICC05 age scale[61]. Grey bands highlight the Younger Dryas and Heinrich stadials 1–4 chronozones as defined in Online-only Table 2.

Example of North Atlantic and Nordic Seas cores dated by alignment of their SST records to the NGRIP ice δ18O signal. Top panel: planktic foraminifer-based warm season surface temperature of core MD99-2281[57,58]; middle panel: % N. pachyderma of core MD99-2281 and MD04-2845[59,60] (both panels: diamonds and squares above the x-axis indicate calibrated 14C ages and alignment tie points, respectively). Bottom panel: NGRIP ice δ18O record on the GICC05 age scale[61]. Grey bands highlight the Younger Dryas and Heinrich stadials 1–4 chronozones as defined in Online-only Table 2.

Technical Validation

The information relative to the validation of the age models entirely based on 14C dates can be found in the publications describing the Undatable age-depth modeling routine[49] and the “MatCal” Bayesian calibration program[18]. The age-depth model plot provided for each core (e.g. Fig. 3) shows the calibrated 14C dates together with the computed age-depth relationship and dating uncertainty, as well as the bootstrapping percentage and sedimentation rate uncertainty values used in the computation. Concerning the age models based on the alignment of SST to NGRIP air temperature, a first validation step involved comparing the resulting dated SST signals of different marine cores among themselves and with the NGRIP air temperature signal. An illustration of such a comparison is given in Fig. 4 for North Atlantic core MD04-2845 and Norwegian Sea core MD99-2881. Moreover, available 14C data over glacial and deglacial portions of cores dated by alignment to NGRIP provide a verification of the tie points selection since surface water reservoir ages should not be negative (e.g. Supplementary Fig. 1). Interestingly, around Heinrich stadial 4 (38 to 40 ka), our age-depth models yield ages which are systematically older than the calibrated ages obtained using IntCal13 and modern surface water reservoir age values, in agreement with the recent findings of ref.[52] showing that IntCal13 is too young with respect to GICC05 during that time interval. The age models based on the alignment of MS to NGRIP ice δ18O have been validated by comparing the resulting dated MS signals with the NGRIP ice δ18O signal (Supplementary Fig. 2). Moreover, these age models have been validated by climate-independent tie points, such as tephra layers in core MD99-2284[43], MD95-201044 and ENAM93-21[45], or changes in the Earth’s magnetic field intensity in core MD99-2281[44]. The age models making use of the alignment of Ti/Ca to speleothem isotopic records have been validated by comparing the radiocarbon-dated upper portion of the cores with the U-Th dated speleothem signal (Supplementary Fig. 3). This validation was the initial step that led to the use of speleothem isotopic records to complement the dating of the three cores from the Brazilian margin since it demonstrates that terrigenous input at these sites is coeval with the precipitation events recorded in the speleothems[25].
Design Type(s)modeling and simulation objective • data collection and processing objective • source-based data analysis objective
Measurement Type(s)age-depth model
Technology Type(s)computational modeling technique
Factor Type(s)geographic location • depth
Sample Characteristic(s)Atlantic Ocean • marine sediment
  17 in total

1.  Old radiocarbon ages in the southwest Pacific Ocean during the last glacial period and deglaciation

Authors: 
Journal:  Nature       Date:  2000-06-01       Impact factor: 49.962

2.  Collapse and rapid resumption of Atlantic meridional circulation linked to deglacial climate changes.

Authors:  J F McManus; R Francois; J-M Gherardi; L D Keigwin; S Brown-Leger
Journal:  Nature       Date:  2004-04-22       Impact factor: 49.962

3.  One-to-one coupling of glacial climate variability in Greenland and Antarctica.

Authors: 
Journal:  Nature       Date:  2006-11-09       Impact factor: 49.962

4.  155,000 years of West African monsoon and ocean thermal evolution.

Authors:  Syee Weldeab; David W Lea; Ralph R Schneider; Nils Andersen
Journal:  Science       Date:  2007-06-01       Impact factor: 47.728

5.  Icebergs not the trigger for North Atlantic cold events.

Authors:  Stephen Barker; James Chen; Xun Gong; Lukas Jonkers; Gregor Knorr; David Thornalley
Journal:  Nature       Date:  2015-04-16       Impact factor: 49.962

6.  Carbon isotope evidence for a northern source of deep water in the glacial western North Atlantic.

Authors:  Lloyd D Keigwin; Stephen A Swift
Journal:  Proc Natl Acad Sci U S A       Date:  2017-02-13       Impact factor: 11.205

7.  Climate change patterns in Amazonia and biodiversity.

Authors:  Hai Cheng; Ashish Sinha; Francisco W Cruz; Xianfeng Wang; R Lawrence Edwards; Fernando M d'Horta; Camila C Ribas; Mathias Vuille; Lowell D Stott; Augusto S Auler
Journal:  Nat Commun       Date:  2013       Impact factor: 14.919

8.  Evolution of South Atlantic density and chemical stratification across the last deglaciation.

Authors:  Jenny Roberts; Julia Gottschalk; Luke C Skinner; Victoria L Peck; Sev Kender; Henry Elderfield; Claire Waelbroeck; Natalia Vázquez Riveiros; David A Hodell
Journal:  Proc Natl Acad Sci U S A       Date:  2016-01-04       Impact factor: 11.205

9.  Sea ice variability in the southern Norwegian Sea during glacial Dansgaard-Oeschger climate cycles.

Authors:  Henrik Sadatzki; Trond M Dokken; Sarah M P Berben; Francesco Muschitiello; Ruediger Stein; Kirsten Fahl; Laurie Menviel; Axel Timmermann; Eystein Jansen
Journal:  Sci Adv       Date:  2019-03-06       Impact factor: 14.136

10.  Sea ice and millennial-scale climate variability in the Nordic seas 90 kyr ago to present.

Authors:  Ulrike Hoff; Tine L Rasmussen; Ruediger Stein; Mohamed M Ezat; Kirsten Fahl
Journal:  Nat Commun       Date:  2016-07-26       Impact factor: 14.919

View more
  1 in total

1.  Coupled atmosphere-ice-ocean dynamics during Heinrich Stadial 2.

Authors:  Xiyu Dong; Gayatri Kathayat; Sune O Rasmussen; Anders Svensson; Jeffrey P Severinghaus; Hanying Li; Ashish Sinha; Yao Xu; Haiwei Zhang; Zhengguo Shi; Yanjun Cai; Carlos Pérez-Mejías; Jonathan Baker; Jingyao Zhao; Christoph Spötl; Andrea Columbu; Youfeng Ning; Nicolás M Stríkis; Shitao Chen; Xianfeng Wang; Anil K Gupta; Som Dutt; Fan Zhang; Francisco W Cruz; Zhisheng An; R Lawrence Edwards; Hai Cheng
Journal:  Nat Commun       Date:  2022-10-04       Impact factor: 17.694

  1 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.