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sparse grid method in the libor market model. option valuation and the

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Chapter 5<br />

Sparse Grids<br />

In <strong>the</strong> previous chapter we discussed two computational <strong>method</strong>s that are available<br />

for pric<strong>in</strong>g of <strong>the</strong> claims with<strong>in</strong> <strong>the</strong> LMM framework. In practice, Monte Carlo is almost<br />

always <strong>in</strong> favour, s<strong>in</strong>ce its computational costs are only l<strong>in</strong>early dependant on<br />

<strong>the</strong> dimensionality of <strong>the</strong> problem. F<strong>in</strong>ite Difference Method suffers from <strong>the</strong> ’curse<br />

of dimensionality’, <strong>the</strong> number of po<strong>in</strong>ts grows exponentially with <strong>the</strong> <strong>in</strong>crease <strong>in</strong> <strong>the</strong><br />

number of underly<strong>in</strong>g variables. This only fact underm<strong>in</strong>es all <strong>the</strong> nice features FD has<br />

to offer, s<strong>in</strong>ce a great number of realistic products are cont<strong>in</strong>gent on up to 30 LIBOR<br />

rates. Sparse Grid <strong>method</strong>s, suggested by Zenger [Zenger, 1991], operate on spatial<br />

discretizations that rely on far fewer po<strong>in</strong>ts <strong>and</strong>, at <strong>the</strong> same time, offer reasonable<br />

accuracy. In this chapter we shall look at <strong>the</strong> common issues related to function approximation,<br />

<strong>in</strong>troduce Sparse Grid technique <strong>and</strong> postulate results for error analysis.<br />

At <strong>the</strong> end we shall discuss <strong>the</strong> comb<strong>in</strong>ation technique used for function <strong>in</strong>terpolation<br />

on a <strong>sparse</strong> <strong>grid</strong>. Presentation of <strong>the</strong> subject <strong>in</strong> this chapter relies on exposition <strong>and</strong><br />

notation of [Garcke, 2005].<br />

5.1 Full <strong>grid</strong> approximations.<br />

Consider a PDE of <strong>the</strong> form Lu = f, subject to certa<strong>in</strong> boundary conditions, def<strong>in</strong>ed<br />

on a d-dimensional solution space [0, 1] d . An equidistant d-dimensional <strong>grid</strong> Ω l could<br />

<strong>the</strong>n be taken as a discrete approximation of such solution space, with :<br />

• l = (l 1 , . . . , l d ) ∈ N d as a multi-<strong>in</strong>dex, i.e. discretization resolution of Ω l<br />

• h l := (h l1 , . . . , h ld ) := (2 −l 1<br />

, . . . , 2 −l d<br />

) as a mesh width<br />

<strong>in</strong> each coord<strong>in</strong>ate direction t ∈ [1 . . . d].<br />

Given Ω l , <strong>the</strong>n <strong>the</strong> discretized PDE, denoted as L l u l = f l , can be approximated<br />

with ei<strong>the</strong>r st<strong>and</strong>ard basis or hierarchical basis functions.<br />

37

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