A first-order operator satisfies the shift-semicontinuity condition if, along test data converging along couplings of vanishing noise cost with fields converging strongly and bounded scores converging weakly, the lower shift is upper semicontinuous and the upper shift lower semicontinuous.
In the setting of First-Order Equations on the Noise Wasserstein Space Relative to a Noise Penalty Pair: Standing Notation, let be a noise penalty pair on and let be a first-order equation operator over , with -shifts and relative to that pair, with the set of test data for and the notion of an -bounded test datum, taken relative to this operator and this pair. For the score lies in , hence in , by Noise Penalty Pairs on the Noise Wasserstein Space: the Penalty, Its Score, and Their Domains §pair. Sequences of couplings of vanishing noise cost, and strong and weak convergence along them, are those of First-Order Equations on the Noise Wasserstein Space Relative to a Noise Penalty Pair: Standing Notation §couplings; limits of sequences of real numbers are those of that definition.
1. (Sequences of test data converging along noise couplings with bounded score) Let be positive, let for every , let , and let for every . Here , and , by The Bundle of Noise Fields over a Set of Measures, First-Order Equation Operators on the Noise Wasserstein Space, and Their Delta-Shifts §bundle and Noise Penalty Pairs on the Noise Wasserstein Space: the Penalty, Its Score, and Their Domains §pair, so that the convergence notions below apply. The sequence converges to along with score bounded by if every is -bounded, if
if is a sequence of couplings of vanishing noise cost from to , if converges strongly to and converges weakly to along , and if converges to .
2. (Shift semicontinuity at a level) Let satisfy and . The operator is shift-semicontinuous at if the following two implications hold for every sequence of test data that converges, in the sense of clause 1, to a test datum along some sequence of couplings with score bounded by , and for every . First, if for every positive there is such that for every with , then
Secondly, if for every positive there is such that for every with , then
3. (The shift-semicontinuity condition) The operator satisfies the shift-semicontinuity condition if it is shift-semicontinuous at for all with and .
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