2014
DOI: 10.1002/2014ja019897
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Noise statistics identification for Kalman filtering of the electron radiation belt observations I: Model errors

Abstract: In this study we present a first attempt to identify errors of the 1-D radial diffusion model for relativistic electron phase space density (PSD). In practice, the model error and characteristics of satellite observations are poorly known, which may cause failure of a Kalman filter algorithm. Correct specification of model errors statistics is necessary for the development of the next generation of radiation belt specification models providing the effective PSD reconstruction and hence the prediction and mitig… Show more

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Cited by 6 publications
(9 citation statements)
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“…In this section, we develop the identification technique of the measurement noise covariance matrix R to incorporate it into a Kalman filter for data assimilation of CRRES observations in the radiation belts. The temporal evolution of the PSD is obtained by solving the 1‐D radial diffusion equation for L shell from 3 to 5 presented in the companion paper [ Podladchikova et al , , equation ] and is given by the following state equation Xj+1=normalΦj+1,jXj+wj+1Here X j is an 11‐dimensional state vector of the PSD at various L shell bins L 1 =3, L 2 =3.2,…, L 10 =4.8, L 11 =5 with a 10 min time step j . The transition state matrix Φ j + 1, j relates a current state vector X j to a one‐step ahead‐predicted state vector X j + 1 .…”
Section: Identification Of the Measurement Noise Covariance Matrixmentioning
confidence: 99%
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“…In this section, we develop the identification technique of the measurement noise covariance matrix R to incorporate it into a Kalman filter for data assimilation of CRRES observations in the radiation belts. The temporal evolution of the PSD is obtained by solving the 1‐D radial diffusion equation for L shell from 3 to 5 presented in the companion paper [ Podladchikova et al , , equation ] and is given by the following state equation Xj+1=normalΦj+1,jXj+wj+1Here X j is an 11‐dimensional state vector of the PSD at various L shell bins L 1 =3, L 2 =3.2,…, L 10 =4.8, L 11 =5 with a 10 min time step j . The transition state matrix Φ j + 1, j relates a current state vector X j to a one‐step ahead‐predicted state vector X j + 1 .…”
Section: Identification Of the Measurement Noise Covariance Matrixmentioning
confidence: 99%
“…The proposed approach to the identification of the measurement noise covariance matrix R is based on the same principles as the identification of the bias, q , and the covariance matrix, Q , of model noise w presented in the companion paper [ Podladchikova et al , ]. The general principle of the proposed identification technique includes the following requirements: Construction of residuals characterizing the mismatch between an observation and an auxiliary estimate of state vector (the pseudomeasurement vector) that does not statistically depend on this observation.…”
Section: Identification Of the Measurement Noise Covariance Matrixmentioning
confidence: 99%
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“…Recent analysis by Podladchikova et al . [] show that improper model errors and error biases have a strong effect on the PSD estimate if observations are sparse in time. Observations assimilated for this analysis are available at every time step, reducing the effect of the unbiased error assumptions.…”
Section: One‐dimensional Diffusion Modelmentioning
confidence: 99%