Feynman–kac Formulas for Black–Scholes–Type Operators
By Svante Janson, Johan Tysk. 2006
77 citations recorded by the source corpus.
Subfields: Applied Mathematics, Finance, Mathematical Physics
View Paper: https://www.semanticscholar.org/paper/6b466f93c3f917fc9c7c6e8399ece3f6eb2c2f6f
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In Applied Mathematics
In Finance
- Ioannis Karatzas
- J. Ruf
- Erik Ekström
- Daniel Fernholz
- Johan Tysk
- George Yin
- Chao Zhu
- Nicholas A. Baran
In Mathematical Physics
Citations in the corpus
- The Black–Scholes equation in stochastic volatility models (2010, background): “Indeed, in [13], the connection between the option price given as a risk-neutral expected value and the corresponding BlackScholes equation is made precise for options on several underlying assets in a local volatility model with absorbing boundary conditions.”
- Feynman–Kac formulas for regime-switching jump diffusions and their applications (2015, background): “Numerous applications have been found; see, for example, [7, 10, 18] (finance), [2, 28] (DNA breathing dynamics, physics, and computer science), and [9] (statistical physics, biology, and engineering problems).”
- Bubbles, convexity and the Black–Scholes equation (2009, background): “The main result of this section says that the option price u(x, t) given by (2) is indeed a classical solution to (3)–(5); compare [17] for the standard case.”
- Optimal arbitrage under model uncertainty. (2011, methodology): “Using results from the theory of stochastic flows [Kunita (1990), Protter (2004)] and from parabolic partial differential equations [Janson and Tysk (2006), Ekström and Tysk (2009)], Theorem 2 in Ruf (2011) shows that the function Γ(·, ·) is then of class C1,2 locally on (0,∞) × (0,∞)n, and solves…”
- Distribution of the time to explosion for one-dimensional diffusions (2013, methodology): “The proof of Proposition 5.2 resembles the arguments in Janson and Tysk (2006).”
- HEDGING UNDER ARBITRAGE (2010, unknown): “Friedman (1976), Chapters 6 and 15 and Janson and Tysk (2006) have related results, but they imposelinear growth conditions ona(·, ·) so that PDE (4.2) has a unique solution of polynomial growth.”