2019
DOI: 10.1029/2019ea000963
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Implementation of a Modified Adaptive Covariance Inflation Scheme for the Big Data‐Driven NLS‐4DVar Algorithm

Abstract: The adaptive inflation scheme is critical for avoiding underestimation of ensemble-estimated error variances. In this study, we expanded a spatially and temporally varying adaptive inflation scheme proposed within the framework of the local ensemble transform Kalman filter to a global version to facilitate its application in four-dimensional ensemble-variational (4DEnVar) data assimilation methods. We adopted an efficient local correlation matrix decomposition approach to enhance its computation efficiency and… Show more

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Cited by 4 publications
(10 citation statements)
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“…Both the i4DVar and 4DVar methods perform considerably well in the framework of 2-D shallow-water equation model (Tian et al, 2020;Tian & Zhang, 2019a, 2019b under the perfect model scenario (and large initial errors), as they produce significantly smaller RMS errors than those from the control simulations (Figures 2a and 2b). Obviously, the system-related errors are only the initial errors, which can be largely corrected by adding the 4DVar correction E  x at the initial time point through the ensemble nonlinear least squares-based approach (i.e., the NLS-4DVar approach) using only 60 ensemble samples.…”
Section: Resultsmentioning
confidence: 96%
“…Both the i4DVar and 4DVar methods perform considerably well in the framework of 2-D shallow-water equation model (Tian et al, 2020;Tian & Zhang, 2019a, 2019b under the perfect model scenario (and large initial errors), as they produce significantly smaller RMS errors than those from the control simulations (Figures 2a and 2b). Obviously, the system-related errors are only the initial errors, which can be largely corrected by adding the 4DVar correction E  x at the initial time point through the ensemble nonlinear least squares-based approach (i.e., the NLS-4DVar approach) using only 60 ensemble samples.…”
Section: Resultsmentioning
confidence: 96%
“…According to the following approximation (Tian & Zhang, 2019b), HiλijboldBHiTHiλij()boldPxPxTN1HiT=1N1()boldPyiPyiT, Equation can be rewritten as lefttrueLijλij=lndetλij1N1Pyi()boldPyinormalT+boldRi()j1+()boldyobs,i'normalT()1N1λij()boldPyiPyiT+Rij11boldyobs,i'. …”
Section: Methodsmentioning
confidence: 99%
“…The total initial MPs Px=(),boldPx,hboldPx,omx×N of BD‐NLS4DVar was composed of two ensembles, a preprepared historical big‐data ensemble ( Px,hmx×Nh) and a small online ensemble ( Px,omx×No), where N h + N o = N ( N h > N o ). See Tian and Zhang (2019a, 2019b) for more details about the preparation and update of the ensemble for the BD‐NLS4DVar. The default parameter values were N o = 10, N h = 100, α = 11, β = 2, l max = 1, and j max = 4, and the covariance localization Schür radius r x = r y = 15 × 300 km for the x and y coordinates, respectively (Gaspari & Cohn, 1999).…”
Section: Observing System Simulation Experiments Using the Shallow‐wamentioning
confidence: 99%
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