Geophysical Research Letters Supporting Information for The response of SST to insolation and ice-sheet variability from MIS 3 to MIS 11 Aleix Cortinaa, Francisco Javier Sierrob, José Abel Floresb, Belen Martrata, Joan O. Grimalta a Department b of Environmental Chemistry, IDAEA-CSIC, 08034 Barcelona, Spain Department of Geology, University of Salamanca, 37008 Salamanca, Spain Contents of this file Text S1 to S2 Figure S3 to S4 Introduction This supporting information is composed by two texts and two figures. Text S1 focuses on the methodology followed for extracting biomarkers from sediments and for estimating SST based on the proportion of long chain di- and tri- unsaturated C37 alkenones. Text S2 explains the methodology for calculating the StdT index. This index allowed us measuring the SST amplitude changes at high-frequency variability during glacial stages. Figure S3 illustrates the variance between the StdT index and sedimentation rate in order to discard differential sedimentation rate as the main cause of StdT index variability. Figure S4 illustrates the theoretical effect on SST of an equal ice-sheet variability depending on insolation. 1 Text S1. Samples were freeze-dried. We added an internal standard (n-nonadecan-1-ol, nhexatriacontane and n-dotetracontane) to about 2.5 g of sediment, which was extracted with dichloromethane in an ultrasonic bath. The extract was saponified with 10% potassium hydroxide in methanol to clean up interferences by carboxylic acids and ester wax. The phase with the neutral lipids was extracted with hexane and evaporated to dryness under a N2 atmosphere. Finally, the compounds obtained were redissolved with toluene, derivatized with bis(trimethylsilyl) trifluoroacetamide ,and analyzed by gas chromatography. The samples were analyzed with a Varian 3400 chromatograph equipped with a CPSIL-5 CB column coated with 100% dimethylsiloxane (film thickness of 0.12 mm). Hydrogen was used as the carrier gas (50 cm/s). The oven was programmed from 90ºC to 170ºC at 20ºC/min, then to 280ºC at 6ºC/min (holding time 35min), to 300ºC at 10ºC/min (holding time 7min) and finally to 320ºC at 10ºC/min (holding time 3min). The injector was programmed from 90ºC (holding time 0.3) to 320ºC at 200ºC/min (the final holding time was 20min). The detector was maintained with a constant temperature of 320ºC. From the chromatograms we identified long chain di- and tri- unsaturated C37 alkenones. After integration, area was converted to concentration, taking into consideration sample weight and the concentration of the internal standard. The SST proxy was based on the Uk’37 index (Brassell et al., 1986; Prahl and Wakeham, 1987). The Uk’37 index results from calculating the relative abundance of different types of alkenones with 37 carbons, varying in the number of double bonds. Uk’37= [C37:2] / ([C37:2] + [C37:3]); It can take values between 0 and 1, respectively, corresponding to temperatures between 0 and 26 ºC. To transform this index into annual mean SST values, we used the following equation: SST= (Uk’37 – 0.044)/0.033 (Müller et al., 1998) References Brassell, S. C., G. Eglinton, I. T. Marlowe, U. Pflaumann, and M. Sarnthein (1986), Molecular stratigraphy: a new tool for climatic assessment, Nature, 320(6058), 129-133. Müller, P. J., G. Kirst, G. Ruhland, I. von Storch, and A. Rosell-Melé (1998), Calibration of the alkenone paleotemperature index U37K′ based on core-tops from the eastern South Atlantic and the global ocean (60°N-60°S), Geochimica et Cosmochimica Acta, 62(10), 1757-1772. Prahl, F. G., and S. G. Wakeham (1987), Calibration of unsaturation patterns in long-chain ketone compositions for palaeotemperature assessment, Nature, 330(6146), 367-369. 2 Text S2. In order to evaluate SST amplitude at millennial-scale level during glacials, we used the standard deviation. Since long-term variability (e.g. precession) influences temperature values, and consequently their standard deviation, we first removed this long-term parameter by subtracting the corresponded polynomial fit. Depending on the length of the glacial interval and the long-term variability effect (mainly precession) we used different degrees of polynomial fits. MIS 3-4: 5th degree polynomial fit MIS 6: 5th degree polynomial fit MIS 8: 3rd degree polynomial fit MIS 10: 2nd degree polynomial fit The result of this subtraction was a new SST proxy (SST*) in which precession and longer variability were removed, but higher-frequency variability remained unaltered. The standard deviation was calculated for this SST* proxy for each of the glacial stages (MIS 3 and 4 computed together since they belong to the same glacial stage), providing a measurement of the SST amplitude variability at high frequencies (StdT index). High (low) StdT index values represented glacials with high (low) millennial-scale amplitude variability. 3 Figure S3. Differences in the sedimentation rate can affect the resolution of the SST record and hence the StdT index. Low sedimentation rate may mask millennial-scale events, resulting in a smooth SST record and the associated decrease in our StdT index. As mean of discarding this differential sedimentation effect as the main cause of the differential StdT, we compared the 30-point-average moving curve of the sedimentation rate with a 30-point-average moving curve of the StdT for the period encompassed between MIS 3-4. This interval was intentionally chosen because it has the most reliable age model. We choose 30-point average window in order to consider normal data distribution. Results do not reveal any significant correlation between high sedimentation rate and StdT. It indicates that the SST signal responded to external forcings and was not an artifact of differential sedimentation rate. 4 Figure S4. Effect of ice-sheet variability in the SST along the Gulf of Lions (GL). Both illustrations show a theoretically equal ice-sheet variability transmitted to the GL by northwesterly winds: (A) during high North Hemisphere summer insolation periods, producing a high SST effect (higher dSST), and (B) during low North Hemisphere summer insolation periods, producing a low SST effect (lower dSST). 5