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P. Malliavin, Stochastic Analysis, Springer (1997).

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Large Deviations And Support Theorem For Diffusions Via.. - Ledoux, Qian, Zhang (2002)   (1 citation)  (Correct)

....ODE approach to random driving paths like sample paths of Brownian motion. Instead, K. Ito established the stochastic calculus by using the martingale property of Brownian motion. It remained an open problem to establish some kind of continuity theorem (or universal limit theorem as P. Malliavin [Ma] called it) for Ito s functionals until T. Lyons showed that the Ito functionals (as rough paths) are indeed continuous in p variation topology. Lyons s continuity theorem of Ito s functionals exhibits that the p variation distance leads to a natural metric structure on the space of Ito s ....

P. Malliavin. Stochastic Analysis. Springer (1997).


Wiener Integration for Quantum Systems: A Unified.. - Bodmann, Leschke, Warzel (1996)   (Correct)

....follows from integration by parts with respect to Dw using its Gaussian nature (cf. 41, p. 32 and solution of exercise 1.8.22] and the convention (0) 1=2 corresponding to the Stratonovich interpretation. For a rigorous proof of (13) one should use Malliavin s stochastic variational calculus [37, 32]. Clearly, if the components of b A commute, time ordering can be dropped, so that the result is obtained directly from b T t (w) exp iw(t) b A and (2) The case b B 6= b 0 will now be treated in the second step by a perturbative argument in the spirit of Kac s original proof ....

P. Malliavin, Stochastic analysis, Springer, to appear


Stochastic Calculus With Respect To Free Brownian Motion And.. - Biane, Speicher (1998)   (2 citations)  (Correct)

....tradition we shall denote by [ jB] this conditional expectation. Recall that it extends to a contraction on all L p spaces for 1 p 1. A map t 7 M t from [0; 1[ to L p (A; will be called an L p martingale with respect to the filtration (A t ) t2R if for every s t one has [M t jA s ] = M s . 1.2 Functional calculus and differentiation. Let B be a unital C algebra, then for any X;Y 2 B, one has Duhamel s formula e X Gamma e Y = Z 1 0 e ffX (X Gamma Y )e (1 Gammaff)Y dff Let now f : R C be a function such that f(x) R R e ixy (dy) where is a finite ....

....out to be nicely connected with free entropy. We shall say more about these topics somewhere else. 5. Analysis on Wigner space In this section we shall develop the first elements of the natural analogues of many results known commonly under the name of analysis on Wiener space (see e.g. J] [M], N] U] We shall start with an abstract version which corresponds to considering a semi circular system modelled on an abstract Hilbert space. Then we shall investigate in more details the case where the Hilbert space is L 2 (R ) and the semi circular system is the free Brownian motion. ....

P. Malliavin, Stochastic Analysis, Grund. Math. Wiss., vol. 313, Springer, Berlin, Heidelberg, New York, 1997.


Ingredients for a General Purpose Stochastic Finite Elements.. - Ghanem (1999)   (4 citations)  (Correct)

....hybrid procedures that permit an optimal allocation of computational resources between Monte Carlo procedures and other analytical procedures. 2 Mathematical Preliminaries A number of mathematical frameworks have been developed to model random operators, and functionals of random processes [4,16,17,13,20 23,26]. The material in this section represents a synthesis of these various frameworks emphasizing those aspect that are most directly related to the formulation of the stochastic finite element method. 2.1 Hilbert Space of Random Variables and Orthogonal Projections A probability space will be ....

.... P ; H;F H ) In this notation, H specifies the Gaussian subspace of random variables with which events in the algebra FH are associated, while the algebra F H contains the events that are independent of H, and is referred to as the transverse oe algebra or the algebra of transverse events [20]. The oe algebra, F , of all random variables is then given by the tensor product F = FH Omega F H ; 5) indicating that an arbitrary event could involve combinations of events associated with H and others that are not. In most cases of interest in the present investigation, F j FH , and the ....

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Malliavin, P. Stochastic Analysis, Springer-Verlag, 1997.


Applications of Malliavin calculus to Monte-Carlo.. - Fournié, Lasry.. (2001)   (15 citations)  Self-citation (Malliavin)   (Correct)

....and forthcoming publications) is to provide some cures for these drawbacks. More precisely, we emphasize the usefulness of tools of modern probability theory, in particular of the Malliavin calculus that we briefly presented in Part I (for more details on Malliavin calculus, the reader may consult [5], 6] 7] 10] Let us also mention in passing the possible use of large deviations theory (see [3] 2] In Part I [1] we showed how one can use Malliavin calculus to write down explicit probabilistic formulas for the greeks i.e. differentials of the values of various European options ....

....extends to a general transformation of the form (# ## # #) where # #(t) t #(##) #(t) for all t # [0, T ] assuming that # is smooth, # ## # #) is bijective and (1 # T 0 # D t #dt) #= 0 a.s. If we compare the above considerations with the literature we are aware of (see [6] [5] and the references therein) we have changed notations and more importantly we have isolated a special class of transformation for which the Carleman Fredholm determinant is computable (here, it is, up to various irrelevant changes of signs, 1 # T 0 # D t #dt) exp(W T # #(#) where, ....

Malliavin, P.: Stochastic analysis. Berlin: Springer 1997


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P. Malliavin, Stochastic Analysis, Springer (1997).


Unitary Brownian motions are linearizable - Tsirelson (1998)   (1 citation)  (Correct)

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P. Malliavin, Stochastic analysis, Springer-Verlag, Berlin, 1997.

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