Atlantic Ocean Forcing of North American and European Summer Climate

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Atlantic Ocean Forcing of North American and European Summer Climate by Rowan T. Sutton, and Daniel L. R. Hodson Science Volume 309(5731):115-118 July 1, 2005 Published by AAAS

Fig. 1. (A) Index of the AMO, 1871 to 2003. (A) Index of the AMO, 1871 to 2003. The index was calculated by averaging annual mean SST observations (29) over the region 0°N to 60°N, 75°W to 7.5°W. The resulting time series was low-pass filtered with a 37-point Henderson filter and then detrended, also removing the long-term mean. The units on the vertical axis are °C. This index explains 53% of the variance in the detrended unfiltered index and is very similar to that shown in (1). (B) The spatial pattern of SST variations associated with the AMO index shown in (A). Shown are the regression coefficients (°C per SD) obtained by regressing the detrended SST data on a normalized (unit variance) version of the index. Rowan T. Sutton, and Daniel L. R. Hodson Science 2005;309:115-118 Published by AAAS

Fig. 2. Evidence of AMO impacts on boreal summer [June, July, and August (JJA)] climate. Evidence of AMO impacts on boreal summer [June, July, and August (JJA)] climate. (A to C) Observed differences between the mean JJA conditions from 1931 to 1960 (a warm phase of the AMO) and the mean JJA conditions from 1961 to 1990 (a cold phase of the AMO). (A) Sea-level pressure. Contours are in Pa with an interval of 30 Pa; shading indicates signal-to-noise ratio (12). (B) Land precipitation (mm/day). (C) Land surface air temperature (°C). The scale for precipitation is nonlinear; the central range is (–0.5, 0.5). Values between (0.5,2.5) and (–2.5,–0.5) are each shaded with a single color. (D and E) As in (A) and (B), but computed from the ensemble mean of six simulations with the HadAM3 atmosphere model forced with observed SST data. In (D), the contour interval is 15 Pa. (F to H) As in (A) to (C), but showing differences between time means of simulations with the HadAM3 model forced with positive and negative signs of an idealized AMO SST pattern. (The pattern is based on the North Atlantic part of Fig. 1B and is shown exactly in fig. S1.) In (F), the contour interval is 15 Pa. All the values have been appropriately scaled to allow comparison with the other panels (12). In (A) and in (C) to (H), regions where anomalies are not significant at the 90% level are shaded white. In (E) and (G), precipitation values are shown over the sea as well as the land. Details of the model experiments and analyses are given in (12). Rowan T. Sutton, and Daniel L. R. Hodson Science 2005;309:115-118 Published by AAAS

Fig. 3. Response of the HadAM3 model to tropical North Atlantic (TNA) and extratropical North Atlantic (XNA) parts of the AMO SST pattern. Response of the HadAM3 model to tropical North Atlantic (TNA) and extratropical North Atlantic (XNA) parts of the AMO SST pattern. (A and B) Differences between time means of simulations with the HadAM3 model forced with positive and negative signs of the TNA SST pattern. (A) Sea-level pressure. Contours in Pa with an interval of 15 Pa; shading indicates signal-to-noise ratio (12). (B) Precipitation (mm/day); scale is nonlinear as described for Fig. 2. (C and D) As in (A) and (B), but for model simulations forced with the XNA SST pattern. The TNA and XNA SST patterns are shown in fig. S1. All values have been scaled to allow comparison with the Fig. 2 results. Regions where anomalies are not significant at the 90% level are shaded white. Rowan T. Sutton, and Daniel L. R. Hodson Science 2005;309:115-118 Published by AAAS