| Literature DB >> 22355781 |
Masahiro Hashizume1, Luis Fernando Chaves, Noboru Minakawa.
Abstract
Malaria resurgence in African highlands in the 1990s has raised questions about the underlying drivers of the increase in disease incidence including the role of El-Niño-Southern Oscillation (ENSO). However, climatic anomalies other than the ENSO are clearly associated with malaria outbreaks in the highlands. Here we show that the Indian Ocean Dipole (IOD), a coupled ocean-atmosphere interaction in the Indian Ocean, affected highland malaria re-emergence. Using cross-wavelet coherence analysis, we found four-year long coherent cycles between the malaria time series and the dipole mode index (DMI) in the 1990s in three highland localities. Conversely, we found a less pronounced coherence between malaria and DMI in lowland localities. The highland/lowland contrast can be explained by the effects of mesoscale systems generated by Lake Victoria on its climate basin. Our results support the need to consider IOD as a driving force in the resurgence of malaria in the East African highlands.Entities:
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Year: 2012 PMID: 22355781 PMCID: PMC3280600 DOI: 10.1038/srep00269
Source DB: PubMed Journal: Sci Rep ISSN: 2045-2322 Impact factor: 4.379
Figure 1Malaria time series.
Clinical records of malaria infections (A) Maseno (May 1935, November 2009, 0°00′S, 34°36′E, Altitude = 1500 m), blue indicates imputed values; (B) Kendu Bay (January 1980, November 2006, 0°24′S, 34°39′E, Altitude = 1240 m); (C) Kisii (January 1986, December 2000, 0°40′S, 34°46′E, Altitude = 1670 m); (D) Kapsabet (January 1980, December 1999, 0°12′N, 35°06′E, Altitude = 2000 m); (E) Kericho (April 1965, November 2006, 0°23′N, 35°15′E, Altitude = 2000 m); (F) DMI, dipole mode index (dotted line) and Nino3, ENSO index (solid line, March 1958, December 2008).
Figure 2Cross-wavelet coherence of the malaria time series with the DMI (dipole mode index) and with Nino3 (ENSO index).
(A) Maseno and DMI (March, 1958, December 2008), (B) Maseno and Nino3 (March 1958, December 2008); (C) Kendu Bay and DMI; (D) Kendu Bay and Nino3; (E) Kisii and DMI; (F) Kisii and Nino3; (G) Kapsabet and DMI; (H) Kapsabet and Nino3; (I) Kericho and DMI; (J) Kericho and Nino3. The coherency scale is from zero (blue) to one (red). Red regions in the plots indicate frequencies and times for which the two series share variability. The cone of influence (within which results are not influenced by the edges of the data) and the significant coherent time-frequency regions (p < 0.05) are indicated by solid lines. The procedures and software used are those described in Chaves and Pascual (2006)30. A smoothing window of 6 months was used to compute the cross-wavelet coherence.
Figure 3Elevation (m) (A) and simulated rainfall (mm) over the Lake Victoria basin with large-scale moisture through the eastern boundary reduced by (B) 20% and (C) 50%.
(Modified from Anyah et al. 200614 figure 10. © American Meteorological Society. Reprinted with permission.) In all panels location color indicates the data available at each site; blue (rainfall); green (disease) and red (disease and rainfall). We used Kisumu rainfall data as a proxy for Kendu Bay and Maseno. Kisumu, like Kendu Bay and Maseno, is in the lowlands (A), with a similar rainfall regime (B and C). Panel C shows box plots for rainfall. Rainfall variability is measured by kurtosis (K), and low values indicate a platykurtic distribution (one where conditions around the median are more variable). (S) indicates skewness.