Seasonality and Predictability of the Indian Ocean Dipole Mode: ENSO Forcing and Internal Variability

被引:123
|
作者
Yang, Yun [1 ,2 ,3 ,4 ]
Xie, Shang-Ping [1 ,2 ]
Wu, Lixin [1 ]
Kosaka, Yu [5 ]
Lau, Ngar-Cheung [6 ,7 ]
Vecchi, Gabriel A. [8 ]
机构
[1] Ocean Univ China, Phys Oceanog Lab, Qingdao Collaborat Innovat Ctr Marine Sci & Techn, Qingdao, Peoples R China
[2] Univ Calif San Diego, Scripps Inst Oceanog, La Jolla, CA 92093 USA
[3] Beijing Normal Univ, Coll Global Change & Earth Syst Sci, Beijing 100875, Peoples R China
[4] Joint Ctr Global Studies, Beijing, Peoples R China
[5] Univ Tokyo, Res Ctr Adv Sci & Technol, Tokyo, Japan
[6] Inst Environm Energy & Sustainabil, Hong Kong, Hong Kong, Peoples R China
[7] Chinese Univ Hong Kong, Dept Geog & Resource Management, Hong Kong, Hong Kong, Peoples R China
[8] NOAA, Geophys Fluid Dynam Lab, Princeton, NJ USA
基金
美国国家科学基金会;
关键词
Indian Ocean; Atmosphere-ocean interaction; ENSO; Interannual variability; SEA-SURFACE TEMPERATURE; EL-NINO; INTERANNUAL VARIABILITY; COUPLED GCM; PART I; EQUATORIAL PACIFIC; TROPICAL PACIFIC; CLIMATE MODELS; ZONAL MODE; ATMOSPHERE;
D O I
10.1175/JCLI-D-15-0078.1
中图分类号
P4 [大气科学(气象学)];
学科分类号
0706 ; 070601 ;
摘要
This study evaluates the relative contributions to the Indian Ocean dipole (IOD) mode of interannual variability from the El Nino-Southern Oscillation (ENSO) forcing and ocean-atmosphere feedbacks internal to the Indian Ocean. The ENSO forcing and internal variability is extracted by conducting a 10-member coupled simulation for 1950-2012 where sea surface temperature (SST) is restored to the observed anomalies over the tropical Pacific but interactive with the atmosphere over the rest of the World Ocean. In these experiments, the ensemble mean is due to ENSO forcing and the intermember difference arises from internal variability of the climate system independent of ENSO. These elements contribute one-third and two-thirds of the total IOD variance, respectively. Both types of IOD variability develop into an east-west dipole pattern because of Bjerknes feedback and peak in September-November. The ENSO forced and internal IOD modes differ in several important ways. The forced IOD mode develops in August with a broad meridional pattern and eventually evolves into the Indian Ocean basin mode, while the internal IOD mode grows earlier in June, is more confined to the equator, and decays rapidly after October. The internal IOD mode is more skewed than the ENSO forced response. The destructive interference of ENSO forcing and internal variability can explain early terminating IOD events, referred to as IOD-like perturbations that fail to grow during boreal summer. The results have implications for predictability. Internal variability, as represented by preseason sea surface height anomalies off Sumatra, contributes to predictability considerably. Including this indicator of internal variability, together with ENSO, improves the predictability of IOD.
引用
收藏
页码:8021 / 8036
页数:16
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