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Stokes radiation amplified during thebackwardpassthrough a system of amplifiers is focused by the parabolic mirror to a diffraction-limited spot.
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The smoothing step can be calculated simultaneously during thebackwardpass.
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Furthermore, it operates online, assimilating data to approximate the posterior density over unknown quantities, without the need for abackwardpass.
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To build a model with better generalization ability, thebackwardpassprunes the model.
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The equations for thebackwardpassinvolve the recursive computation of data which are used at each observation time to compute the smoothed state and covariance.
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We begin with thebackwardpass.
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There is no limit to the number of backward passes or where they may be thrown from.
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