133 research outputs found

    Constructing Sobol' sequences with better two-dimensional projections

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    Direction numbers for generating Sobol' sequences that satisfy the so-called Property A in up to 1111 dimensions have previously been given in Joe and Kuo [ACM Trans. Math. Software, 29 (2003), pp. 49–57]. However, these Sobol' sequences may have poor two-dimensional projections. Here we provide a new set of direction numbers alleviating this problem. These are obtained by treating Sobol' sequences in d dimensions as (t, d)-sequences and then optimizing the t-values of the two-dimensional projections. Our target dimension is 21201

    Component-by-component construction of good intermediate-rank lattice rules

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    It is known that the generating vector of a rank-1 lattice rule can be constructed component-by-component to achieve strong tractability error bounds in both weighted Korobov spaces and weighted Sobolev spaces. Since the weights for these spaces are nonincreasing, the first few variables are in a sense more important than the rest. We thus propose to copy the points of a rank-1 lattice rule a number of times in the first few dimensions to yield an intermediate-rank lattice rule. We show that the generating vector (and in weighted Sobolev spaces, the shift also) of an intermediate-rank lattice rule can also be constructed component-by-component to achieve strong tractability error bounds. In certain circumstances, these bounds are better than the corresponding bounds for rank-1 lattice rules

    Lattice rules with random nn achieve nearly the optimal O(nα1/2)\mathcal{O}(n^{-\alpha-1/2}) error independently of the dimension

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    We analyze a new random algorithm for numerical integration of dd-variate functions over [0,1]d[0,1]^d from a weighted Sobolev space with dominating mixed smoothness α0\alpha\ge 0 and product weights 1γ1γ2>01\ge\gamma_1\ge\gamma_2\ge\cdots>0, where the functions are continuous and periodic when α>1/2\alpha>1/2. The algorithm is based on rank-11 lattice rules with a random number of points~nn. For the case α>1/2\alpha>1/2, we prove that the algorithm achieves almost the optimal order of convergence of O(nα1/2)\mathcal{O}(n^{-\alpha-1/2}), where the implied constant is independent of the dimension~dd if the weights satisfy j=1γj1/α<\sum_{j=1}^\infty \gamma_j^{1/\alpha}<\infty. The same rate of convergence holds for the more general case α>0\alpha>0 by adding a random shift to the lattice rule with random nn. This shows, in particular, that the exponent of strong tractability in the randomized setting equals 1/(α+1/2)1/(\alpha+1/2), if the weights decay fast enough. We obtain a lower bound to indicate that our results are essentially optimal. This paper is a significant advancement over previous related works with respect to the potential for implementation and the independence of error bounds on the problem dimension. Other known algorithms which achieve the optimal error bounds, such as those based on Frolov's method, are very difficult to implement especially in high dimensions. Here we adapt a lesser-known randomization technique introduced by Bakhvalov in 1961. This algorithm is based on rank-11 lattice rules which are very easy to implement given the integer generating vectors. A simple probabilistic approach can be used to obtain suitable generating vectors.Comment: 17 page

    On the expected uniform error of geometric Brownian motion approximated by the L\'evy-Ciesielski construction

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    It is known that the Brownian bridge or L\'evy-Ciesielski construction of Brownian paths almost surely converges uniformly to the true Brownian path. In the present article the focus is on the error. In particular, we show for geometric Brownian motion that at level NN, at which there are d=2Nd=2^N points evaluated on the Brownian path, the expected uniform error has an upper bound of order O(N/2N)\mathcal{O}(\sqrt{N/2^N}), or equivalently, O(lnd/d)\mathcal{O}(\sqrt{\ln d/d}). This upper bound matches the known order for the expected uniform error of the standard Brownian motion. We apply the result to an option pricing example
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