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Itō calculus : ウィキペディア英語版
Itô calculus

Itô calculus, named after Kiyoshi Itô, extends the methods of calculus to stochastic processes such as Brownian motion (Wiener process). It has important applications in mathematical finance and stochastic differential equations.
The central concept is the Itô stochastic integral, a stochastic generalization of the Riemann–Stieltjes integral in analysis. The integrands and the integrators are now stochastic processes:
:Y_t=\int_0^t H_s\,dX_s,
where ''H'' is a locally square-integrable process adapted to the filtration generated by ''X'' , which is a Brownian motion or, more generally, a semimartingale. The result of the integration is then another stochastic process. Concretely, the integral from 0 to any particular ''t'' is a random variable, defined as a limit of a certain sequence of random variables. The paths of Brownian motion fail to satisfy the requirements to be able to apply the standard techniques of calculus. So with the integrand a stochastic process, the Itô stochastic integral amounts to an integral with respect to a function which is not differentiable at any point and has infinite variation over every time interval.
The main insight is that the integral can be defined as long as the integrand ''H'' is adapted, which loosely speaking means that its value at time ''t'' can only depend on information available up until this time. Roughly speaking, one chooses a sequence of partitions of the interval from 0 to ''t'' and construct Riemann sums. Every time we are computing a Riemann sum, we are using a particular instantiation of the integrator. It is crucial which point in each of the small intervals is used to compute the value of the function. The limit then is taken in probability as the mesh of the partition is going to zero. Numerous technical details have to be taken care of to show that this limit exists and is independent of the particular sequence of partitions. Typically, the left end of the interval is used.
Important results of Itô calculus include the integration by parts formula and Itô's lemma, which is a change of variables formula. These differ from the formulas of standard calculus, due to quadratic variation terms.
In mathematical finance, the described evaluation strategy of the integral is conceptualized as that we are first deciding what to do, then observing the change in the prices. The integrand is how much stock we hold, the integrator represents the movement of the prices, and the integral is how much money we have in total including what our stock is worth, at any given moment. The prices of stocks and other traded financial assets can be modeled by stochastic processes such as Brownian motion or, more often, geometric Brownian motion (see Black–Scholes). Then, the Itô stochastic integral represents the payoff of a continuous-time trading strategy consisting of holding an amount ''Ht'' of the stock at time ''t''. In this situation, the condition that ''H'' is adapted corresponds to the necessary restriction that the trading strategy can only make use of the available information at any time. This prevents the possibility of unlimited gains through high-frequency trading: buying the stock just before each uptick in the market and selling before each downtick. Similarly, the condition that ''H'' is adapted implies that the stochastic integral will not diverge when calculated as a limit of Riemann sums .
==Notation==
The process ''Y'' defined as before as
: Y_t = \int_0^t H\,dX\equiv\int_0^t H_s\,dX_s ,
is itself a stochastic process with time parameter ''t'', which is also sometimes written as ''Y'' = ''H'' · ''X'' . Alternatively, the integral is often written in differential form ''dY = H dX'', which is equivalent to ''Y'' − ''Y''0 = ''H'' · ''X''. As Itô calculus is concerned with continuous-time stochastic processes, it is assumed that an underlying filtered probability space is given
:(\Omega,\mathcal,(\mathcal_t)_,\mathbb) .
The σ-algebra ''Ft'' represents the information available up until time ''t'', and a process ''X'' is adapted if ''Xt'' is ''Ft''-measurable. A Brownian motion ''B'' is understood to be an ''Ft''-Brownian motion, which is just a standard Brownian motion with the properties that ''B''''t'' is ''Ft''-measurable and that ''B''''t''+''s'' − ''B''''t'' is independent of ''Ft'' for all ''s'',''t'' ≥ 0 .

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