Centering the slowest observable L1(x) as the starting point simplifies the construction of quasi-exactly-solvable Markov generators with two explicit levels for Fokker-Planck and jump processes.
GeneratorGas a tridiagonal Markov matrix parametrized by the two potentialsU(.)andU I .+ 1 2 Using the finite-difference operator of Eq
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On the role of the slowest observable in one-dimensional Markov processes to construct quasi-exactly-solvable generators with $N=2$ explicit levels
Centering the slowest observable L1(x) as the starting point simplifies the construction of quasi-exactly-solvable Markov generators with two explicit levels for Fokker-Planck and jump processes.