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p-variation

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In mathematical analysis, p-variation is a collection of seminorms on functions from an ordered set to a metric space, indexed by a real number p 1 {\displaystyle p\geq 1} . p-variation is a measure of the regularity or smoothness of a function. Specifically, if f : I ( M , d ) {\displaystyle f:I\to (M,d)} , where ( M , d ) {\displaystyle (M,d)} is a metric space and I a totally ordered set, its p-variation is:

f p -var = ( sup D t k D d ( f ( t k ) , f ( t k 1 ) ) p ) 1 / p {\displaystyle \|f\|_{p{\text{-var}}}=\left(\sup _{D}\sum _{t_{k}\in D}d(f(t_{k}),f(t_{k-1}))^{p}\right)^{1/p}}

where D ranges over all finite partitions of the interval I.

The p variation of a function decreases with p. If f has finite p-variation and g is an α-Hölder continuous function, then g f {\displaystyle g\circ f} has finite p α {\displaystyle {\frac {p}{\alpha }}} -variation.

The case when p is one is called total variation, and functions with a finite 1-variation are called bounded variation functions.

This concept should not be confused with the notion of p-th variation along a sequence of partitions, which is computed as a limit along a given sequence ( D n ) {\displaystyle (D_{n})} of time partitions:

[ f ] p = ( lim n t k n D n d ( f ( t k n ) , f ( t k 1 n ) ) p ) {\displaystyle _{p}=\left(\lim _{n\to \infty }\sum _{t_{k}^{n}\in D_{n}}d(f(t_{k}^{n}),f(t_{k-1}^{n}))^{p}\right)}


For example for p=2, this corresponds to the concept of quadratic variation, which is different from 2-variation.

Link with Hölder norm

One can interpret the p-variation as a parameter-independent version of the Hölder norm, which also extends to discontinuous functions.

If f is αHölder continuous (i.e. its α–Hölder norm is finite) then its 1 α {\displaystyle {\frac {1}{\alpha }}} -variation is finite. Specifically, on an interval , f 1 α -var f α ( b a ) α {\displaystyle \|f\|_{{\frac {1}{\alpha }}{\text{-var}}}\leq \|f\|_{\alpha }(b-a)^{\alpha }} .

If p is less than q then the space of functions of finite p-variation on a compact set is continuously embedded with norm 1 into those of finite q-variation. I.e. f q -var f p -var {\displaystyle \|f\|_{q{\text{-var}}}\leq \|f\|_{p{\text{-var}}}} . However unlike the analogous situation with Hölder spaces the embedding is not compact. For example, consider the real functions on given by f n ( x ) = x n {\displaystyle f_{n}(x)=x^{n}} . They are uniformly bounded in 1-variation and converge pointwise to a discontinuous function f but this not only is not a convergence in p-variation for any p but also is not uniform convergence.

Application to Riemann–Stieltjes integration

If f and g are functions from to R {\displaystyle \mathbb {R} } with no common discontinuities and with f having finite p-variation and g having finite q-variation, with 1 p + 1 q > 1 {\displaystyle {\frac {1}{p}}+{\frac {1}{q}}>1} then the Riemann–Stieltjes Integral

a b f ( x ) d g ( x ) := lim | D | 0 t k D f ( t k ) [ g ( t k + 1 ) g ( t k ) ] {\displaystyle \int _{a}^{b}f(x)\,dg(x):=\lim _{|D|\to 0}\sum _{t_{k}\in D}f(t_{k})}

is well-defined. This integral is known as the Young integral because it comes from Young (1936). The value of this definite integral is bounded by the Young-Loève estimate as follows

| a b f ( x ) d g ( x ) f ( ξ ) [ g ( b ) g ( a ) ] | C f p -var g q -var {\displaystyle \left|\int _{a}^{b}f(x)\,dg(x)-f(\xi )\right|\leq C\,\|f\|_{p{\text{-var}}}\|\,g\|_{q{\text{-var}}}}

where C is a constant which only depends on p and q and ξ is any number between a and b. If f and g are continuous, the indefinite integral F ( w ) = a w f ( x ) d g ( x ) {\displaystyle F(w)=\int _{a}^{w}f(x)\,dg(x)} is a continuous function with finite q-variation: If astb then F q -var ; [ s , t ] {\displaystyle \|F\|_{q{\text{-var}};}} , its q-variation on , is bounded by C g q -var ; [ s , t ] ( f p -var ; [ s , t ] + f ; [ s , t ] ) 2 C g q -var ; [ s , t ] ( f p -var ; [ a , b ] + f ( a ) ) {\displaystyle C\|g\|_{q{\text{-var}};}(\|f\|_{p{\text{-var}};}+\|f\|_{\infty ;})\leq 2C\|g\|_{q{\text{-var}};}(\|f\|_{p{\text{-var}};}+f(a))} where C is a constant which only depends on p and q.

Differential equations driven by signals of finite p-variation, p < 2

A function from R d {\displaystyle \mathbb {R} ^{d}} to e × d real matrices is called an R e {\displaystyle \mathbb {R} ^{e}} -valued one-form on R d {\displaystyle \mathbb {R} ^{d}} .

If f is a Lipschitz continuous R e {\displaystyle \mathbb {R} ^{e}} -valued one-form on R d {\displaystyle \mathbb {R} ^{d}} , and X is a continuous function from the interval to R d {\displaystyle \mathbb {R} ^{d}} with finite p-variation with p less than 2, then the integral of f on X, a b f ( X ( t ) ) d X ( t ) {\displaystyle \int _{a}^{b}f(X(t))\,dX(t)} , can be calculated because each component of f(X(t)) will be a path of finite p-variation and the integral is a sum of finitely many Young integrals. It provides the solution to the equation d Y = f ( X ) d X {\displaystyle dY=f(X)\,dX} driven by the path X.

More significantly, if f is a Lipschitz continuous R e {\displaystyle \mathbb {R} ^{e}} -valued one-form on R e {\displaystyle \mathbb {R} ^{e}} , and X is a continuous function from the interval to R d {\displaystyle \mathbb {R} ^{d}} with finite p-variation with p less than 2, then Young integration is enough to establish the solution of the equation d Y = f ( Y ) d X {\displaystyle dY=f(Y)\,dX} driven by the path X.

Differential equations driven by signals of finite p-variation, p ≥ 2

The theory of rough paths generalises the Young integral and Young differential equations and makes heavy use of the concept of p-variation.

For Brownian motion

p-variation should be contrasted with the quadratic variation which is used in stochastic analysis, which takes one stochastic process to another. In particular the definition of quadratic variation looks a bit like the definition of p-variation, when p has the value 2. Quadratic variation is defined as a limit as the partition gets finer, whereas p-variation is a supremum over all partitions. Thus the quadratic variation of a process could be smaller than its 2-variation. If Wt is a standard Brownian motion on , then with probability one its p-variation is infinite for p 2 {\displaystyle p\leq 2} and finite otherwise. The quadratic variation of W is [ W ] T = T {\displaystyle _{T}=T} .

Computation of p-variation for discrete time series

For a discrete time series of observations X0,...,XN it is straightforward to compute its p-variation with complexity of O(N). Here is an example C++ code using dynamic programming:

double p_var(const std::vector<double>& X, double p) {
	if (X.size() == 0)
		return 0.0;
	std::vector<double> cum_p_var(X.size(), 0.0);   // cumulative p-variation
	for (size_t n = 1; n < X.size(); n++) {
		for (size_t k = 0; k < n; k++) {
			cum_p_var = std::max(cum_p_var, cum_p_var + std::pow(std::abs(X - X), p));
		}
	}
	return std::pow(cum_p_var.back(), 1./p);
}

There exist much more efficient, but also more complicated, algorithms for R {\displaystyle \mathbb {R} } -valued processes and for processes in arbitrary metric spaces.

References

  1. Cont, R.; Perkowski, N. (2019). "Pathwise integration and change of variable formulas for continuous paths with arbitrary regularity". Transactions of the American Mathematical Society. 6: 161–186. arXiv:1803.09269. doi:10.1090/btran/34.
  2. "Lecture 7. Young's integral". 25 December 2012.
  3. Friz, Peter K.; Victoir, Nicolas (2010). Multidimensional Stochastic Processes as Rough Paths: Theory and Applications (Cambridge Studies in Advanced Mathematics ed.). Cambridge University Press.
  4. Lyons, Terry; Caruana, Michael; Levy, Thierry (2007). Differential equations driven by rough paths, vol. 1908 of Lecture Notes in Mathematics. Springer.
  5. "Lecture 8. Young's differential equations". 26 December 2012.
  6. Butkus, V.; Norvaiša, R. (2018). "Computation of p-variation". Lithuanian Mathematical Journal. 58 (4): 360–378. doi:10.1007/s10986-018-9414-3. S2CID 126246235.
  7. ^ "P-var". GitHub. 8 May 2020.
  • Young, L.C. (1936), "An inequality of the Hölder type, connected with Stieltjes integration", Acta Mathematica, 67 (1): 251–282, doi:10.1007/bf02401743.

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