2013
DOI: 10.1175/jcli-d-13-00105.1
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Oscillatory Climate Modes in the Indian Monsoon, North Atlantic, and Tropical Pacific

Abstract: This paper explores the three-way interactions between the Indian monsoon, the North 7 Atlantic and the Tropical Pacific. Four climate records were analyzed: the monsoon rainfall 8 in two Indian regions, the Southern Oscillation Index for the Tropical Pacific, and the NAO 9 index for the North Atlantic. The individual records exhibit highly significant oscillatory 10 modes with spectral peaks at 7-8 yr and in the quasi-biennial and quasi-quadrennial bands. 11The interactions between the three regions were inve… Show more

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Cited by 28 publications
(39 citation statements)
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“…Such a 7-8-year oscillation of temperatures in England has previously been reported (Plaut et al 1995), and probably reflects corresponding oscillations in sea level pressures and sea surface temperatures over the North Atlantic basin (Feliks et al 2004;Feliks et al 2010;Feliks et al 2013). Examination of the chain of causalities through time lags suggests that these thermal oscillations intially propagated into the Windermere ecosystem through a modulation of juvenile survival in perch and pike.…”
Section: -8-year Oscillations: Pathogen-triggered Top-down Forcingsupporting
confidence: 56%
“…Such a 7-8-year oscillation of temperatures in England has previously been reported (Plaut et al 1995), and probably reflects corresponding oscillations in sea level pressures and sea surface temperatures over the North Atlantic basin (Feliks et al 2004;Feliks et al 2010;Feliks et al 2013). Examination of the chain of causalities through time lags suggests that these thermal oscillations intially propagated into the Windermere ecosystem through a modulation of juvenile survival in perch and pike.…”
Section: -8-year Oscillations: Pathogen-triggered Top-down Forcingsupporting
confidence: 56%
“…The time delay η is chosen as the first minimum of the auto-mutual information I x 1 (t); x 1 (t + η) following the Fraser-Swinney recipe [33]. I x(t); y(t + τ )|y(t) with the 1-dimensional condition, in the direction of coupling (full red line) and I y(t); x(t + τ )|x(t) in the direction without coupling (dashed blue line); (c) the conditional mutual information I x(t); y(t + τ )|y(t), y(t − η), y(t − 2η) with the 3-dimensional condition, in the direction of coupling (full red line) and I y(t); x(t + τ )|x(t), x(t − η), x(t − 2η) in the direction without coupling (dashed blue line); for the unidirectionally coupled Rössler systems (13) and (14), as functions of the coupling strength ǫ. …”
Section: Example: Unidirectionally Coupled Rössler Systemsmentioning
confidence: 99%
“…The chaotic solutions of the Rössler systems (13) and (14) oscillate in a relatively narrow frequency band (Figure 3a, black line), therefore it is possible to apply the Hilbert transform directly to the components x 1 and y 1 in order to obtain the instantaneous phases φ 1 and φ 2 of the driving system (13) and the driven system (14), respectively. Then the direction of coupling can be inferred using the conditional mutual information I φ 1 (t); φ 2 (t + τ )|φ 2 (t) and I φ 2 (t); φ 1 (t + τ )|φ 1 (t) already with the one-dimensional condition (Figure 3b) since the phase represents a simplified one-dimensional description of the Rössler system's oscillations.…”
Section: Interactions Over Time Scalesmentioning
confidence: 99%
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