• Keine Ergebnisse gefunden

East Atlantic Pattern Drives Multidecadal Atlantic Meridional Overturning Circulation Variability during the Last Glacial Maximum

N/A
N/A
Protected

Academic year: 2022

Aktie "East Atlantic Pattern Drives Multidecadal Atlantic Meridional Overturning Circulation Variability during the Last Glacial Maximum"

Copied!
8
0
0

Wird geladen.... (Jetzt Volltext ansehen)

Volltext

(1)

Supporting Information for

East Atlantic Pattern Drives Multidecadal Atlantic Meridional Overturning Circulation Variability during the Last Glacial Maximum

Zhaoyang Song

1

, Mojib Latif

1,2

, Wonsun Park

1

1

GEOMAR Helmholtz Centre for Ocean Research Kiel, Kiel, Germany

2

Excellence Cluster “The Future Ocean” at Kiel University, Kiel, Germany Corresponding author: Zhaoyang Song (zsong@geomar.de)

Contents of this file Figures S1-S8 Table S1

Figures

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15

(2)

16

(3)

run of (a) the KCM, (c), CCSM4, (e) CNRM-CM5, (g) FGOALS-g2, (i) MPI-ESM-P and (k) MRI-CGCM3. (b), (d), (f), (h) and (j) as in (a), (c), (e), (g) and (i), but for the LGM run.

Figure S2. Spectra of annual AMOC index (defined as maximum stream function) at 30 °N. The

red dashed and solid lines indicate the 95% confidence limit of the Markov Red Noise model in PI and GLAC, respectively.

18 19 20 21

22 23 24 25 26

(4)

Figure S3. The normalized principal components (PC1) of the leading EOF of JFM SLP calculated from (a) PI and (b) GLAC. (c,d) as (a,b), but for PC2.

27 28 29 30

(5)

Figure S4. The leading empirical orthogonal functions (EOF1) of JFM sea level pressure

calculated from the LGM runs of the Paleoclimate Modelling Intercomparison Project Phase III (PMIP3). The numbers on the upper right show the variance accounted for by each pattern.

32 33 34 35

(6)

Figure S5. As in Figure S4, but for the second EOF.

36 37 38 39 40

(7)

Figure S6. Lag-regressions (from 0 to 10 years) of the overturning stream function on the normalized PC1 (NAO) for PI and GLAC.

42 43

(8)

44

45

(9)

Figure S8. The leading and second most energetic EOFs of JFM sea level pressure calculated

from (a, e) PIAtm, (b, f) GLACAtm, (c, g) PIOro, and (d, h) GLACOro. See Table S1 for details. The numbers on the upper right show the variance accounted for by each pattern.

Tables

Table S1. Experiments with the atmosphere model run in stand-alone mode.

PIAtm PIOro GLACAtm GLACOro

SST & Sea Ice PI GLAC GLAC PI

Orography&Ice Sheet

PI PI GLAC GLAC

Each experiment is integrated for 650 years, with the last 600 years used in the analyses.

48

49 50 51 52 53 54 55 56 57 58 59

60 61

Abbildung

Figure S2. Spectra of annual AMOC index (defined as maximum stream function) at 30 °N
Figure   S3.   The   normalized   principal   components   (PC1)   of   the   leading   EOF   of   JFM   SLP calculated from (a) PI and (b) GLAC
Figure   S4.   The   leading   empirical   orthogonal   functions   (EOF1)   of   JFM   sea   level   pressure
Figure S5. As in Figure S4, but for the second EOF. 36 37 38 39 40
+3

Referenzen

ÄHNLICHE DOKUMENTE

Assuming negligible silicon isotopic fractionation of Asian dust during transport to the tropical West Paci fi c, the eolian dust delivered to marine areas should have a

Sediment composition and stable isotope data suggest three distinct paleoenvironments: (1) a productive region in the eastern to central Fram Strait and along the northern Barents

[r]

Conversely, low d 13 C (less than 0‰ PDB) dominates the deep western South Atlantic below depths of 3 km reaching as far north as 50°N, whereas in the eastern Atlantic, south of

3.2.1 Identifying the multidecadal mode To decompose the global pattern on multidecadal time scales and to inves- tigate possible links of the AMO with separate ocean basins,

[ 11 ] In SRESA2, the annual mean freshwater flux from Greenland increases from 0.03 Sv at the beginning of the experiment (this value is close to the one for which the net mass

At the same time the southward penetration of the Agulhas Current was reduced, and less thermocline-to-intermediate water slipped from the Indian Ocean along the southern rim of

According to a series of LGM experiments with an increasing sea-surface salinity anomaly in the Weddell Sea, the ventilated thermocline was colder than today by 2 – 3C in the