SearcharxivSearch

arXiv subjects

Alexander S. Ushakov

Publications and source records attributed to Alexander S. Ushakov.

3 recordsLinked to original sources

Henstock--Kurzweil Path Integral in Financial Mathematics: A Machine-Verified Pricing of European and Barrier Options

We apply the Henstock--Kurzweil (HK) gauge integral to the Black--Scholes model of option pricing and obtain the European call price directly from a Gaussian cylindrical kernel, without stochastic calculus. Under the risk- neutral measure, the log-price is a Brownian motion with drift nu = r - sigma^2/2. Its transition density is the Gaussian kernel G_t(x,y) = (2 pi sigma^2 t)^{-1/2} exp( - (y - x - nu t)^2 / (2 sigma^2 t) ). We give a machine-checked formalization in Lean 4 / Mathlib of the following: the Chapman--Kolmogorov (semigroup) property, the fact that G_t is a probability density, strong continuity of the pricing operator, the closed-form price C = S_0 N(d_1) - K e^{-rT} N(d_2) with the standard normal CDF N, and the exactness of the drift--diffusion Chernoff splitting at every level. The entire proof is "sorry"-free and depends only on propext, Classical.choice, and Quot.sound. Digital and barrier options are treated as further examples, illustrating the universality of the method, and we show that the construction is compatible with the classical Ito calculus in the continuum limit.

q-fin.PR

The Fedosov manifolds and magnetic monopole

A non-symplectic generalization of Hamiltonian mechanics is considered. It allows include into consideration "non-Lagrange" systems, such as theory of charged particle in the field of magnetic monopole. The corresponding generalization for the Fedosov manifolds is given. The structure of phase space of "charged particle in the field of magnetic monopole" is studied.

math-ph

Invariant variational principle for Hamiltonian mechanics

It is shown that the action for Hamiltonian equations of motion can be brought into invariant symplectic form. In other words, it can be formulated directly in terms of the symplectic structure $ω$ without any need to choose some 1-form $γ$, such that $ω= d γ$, which is not unique and does not even generally exist in a global sense.

math-ph