Abstract
In this chapter we will assume a (non-negative) measurable function ϕ(t, x) is given (but not\( \overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\frown}$}}{\varphi } \left( {t,x} \right)! \)), and concentrate on the problem of constructing diffusion processes starting from an arbitrary point (s, x) with an additional drift coefficient σTσ∇(logϕ(t, x)); namely we will not fix an initial distribution. It is clear, then, that we cannot handle our problem in the framework of the variational method (in the p-representation) formulated in the preceding chapter based on Csiszar’s projection theorem for lack of a fixed initial distribution, or in other words, lack of the function \( \overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\frown}$}}{\varphi } \left( {t,x} \right)! \). If a transition density p(s, x; t, x) with creation and killing is given and if ϕ(t, x) is p-harmonic and positive, then the harmonic transformation induces an additional drift term σTσ∇(log ϕ(t, x)) as we have discussed in Chapter 2. A mathematical problem encountered with ϕ(t, x) which vanishes on a subset will be reduced to defining a multiplicative functional properly (cf. (6.5)) and to verifying the normality condition under a mild integrability condition (cf. (6.4)).
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Notes
This has appeared already in (3.40)
See Chapter 2 for multiplicative functionals
For time-symmetric cases, cf. Donsker-Varadhan (1975), Fukushima-Takeda (1984). Cf. also Oshima (1992)
It was presented in 1987 to commemorate the centenary of E. Schrödinger’s birth
See (2.14) and what follows in Chapter 2
Cf. Aebi (1989, 93) for general cases
Compare with Theorem 5.4
This is the reason why time reversal is somewhat a strange subject for those who were educated by the modern theory of Markov processes
We can require ψ(t, x;r,y), a ≤ t < r ≤ b, is the fundamental solution of the time reversed equation, namely the complex conjugate of the Schrödinger equation
For extensive literature cf., e.g. Albeverio-Høegh-Krohn (1976). Cf. also Itô (1961, 67)
He speaks of “probability amplitude for a path”, but the probability amplitude is not a well-defined mathematical object in probability theory
In this connection cf. Doss (1980)
Due to K. Uchiyama, cf. Nagasawa (1990)
Cf. Remark 6.1 after Lemma 6.2
Cf. Aizenman-Simon (1982), Stummer (1990) and also Sturm (1989). For Schrödinger operators see Chung-Rao (1981)
Cf. Stummer (1990)
Non-typical examples with severely singular potentials see Section 7.9
We take virtual photons to avoid theoretical complication of fermions
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© 1993 Springer Basel AG
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Nagasawa, M. (1993). Diffusion Processes in q-Representation. In: Schrödinger Equations and Diffusion Theory. Monographs in Mathematics, vol 86. Birkhäuser, Basel. https://doi.org/10.1007/978-3-0348-8568-3_6
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DOI: https://doi.org/10.1007/978-3-0348-8568-3_6
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