For a Hamiltonian that absorbs shifts at the noise level and is bounded at zero momentum at bounded positions, a momentum shift that satisfies either envelope test inequality at a bounded position has norm at most a constant over the shift size, with the admissible shift sizes depending only on the position bound and the constant on the position bound, the momentum bound and the bound on the discount term.
In the setting of The Discounted HJB Equation with Free Langevin Noise in a Wall, Envelope Form: Standing Notation, let be the discount rate and the noise intensity and let be the Hamiltonian, all as fixed in The Discounted HJB Equation with Free Langevin Noise in a Wall, Envelope Form: Standing Notation §data. Assume that the Hamiltonian absorbs shifts at noise level and is bounded at zero momentum at bounded positions. Lifts are those of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation §lifts; sums, real multiples and the pairing of -tuples are those of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation §pairing; the norm and laws are those of Tracial W*-Probability Spaces and Square-Integrable Tuples: Standing Notation §tuples; and for real , is the image of the set of Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation §laws under the canonical map of Square-Integrable Noncommutative Laws: Standing Notation §laws.
For every real there is a real such that for all reals and there is a real such that the following holds for every tracial W*-probability space , all -tuples of with and , every real with and every real with .
1. (Subsolution side) If
then .
2. (Supersolution side) If
then .
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