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Deterministic quasi-Monte Carlo and discrepancy — Examples

1 · Prerequisites

2 · Summary

Summary

These examples check the Koksma–Hlawka bound on a smooth integrand, show an integrable inverse-CDF transform whose endpoint singularity has infinite variation, and separate good one-coordinate projections from joint net quality. A final example distinguishes the arbitrary point counts allowed for quadrature and lattice rules from the power-of-base sizes required of digital nets.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

ExampleConstruction: AI-generatedVerification: AI-generatedOpen item page →

Uniform coordinate projections can hide a poor joint projection

Example

Use the four-node rank-one lattice rule in dimension two with N=4 and z=(1,1). Both one-coordinate projections are the equally spaced set {0,1/4,1/2,3/4}, but the two-coordinate set lies on the diagonal. It is not a (0,2,2)-net in base 2, and its star discrepancy is at least 1/4.

Facts & Assumptions

Given: Dimension d=2, node count N=4, and rank-one lattice generator z=(1,1).

[F1]

The rank-one lattice rule uses nodes xn,j={nzj/N} for n=0,…,N−1, with {a}=a−⌊a⌋. (Digital point-set and rank-one lattice cube quadrature)

[F2]

A (t,m,d)-net in base b has bm points and each elementary interval with exponent sum m−t contains exactly bt points; DN∗ is the supremum of anchored-box count error. (Star discrepancy, digital nets, and digital sequences)

Proof

1.1F1F3givenalgebra

By [F1] and [F3], the nodes are P={(0,0),(1/4,1/4),(1/2,1/2),(3/4,3/4)}. Each coordinate projection has one point in each base-2 interval of length 1/4, so each is a (0,2,1)-net.

2.1F2step 1.1

The elementary interval E=[0,1/2)×[0,1/2) has volume 1/4 and contains (0,0) and (1/4,1/4), hence two points. A (0,2,2)-net would require exactly 20=1 point in every such interval, so P is not one.

3.1F2step 1.1algebra∎

At u=(1/2,1/2), the anchored box contains 2 of the 4 nodes, so its empirical proportion is 1/2 while its volume is 1/4. Thus D4∗(P)≥∣1/2−1/4∣=1/4.

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Digital net sizes are powers of their base

Example

In base 2, a digital (t,m,d)-net has exactly 2m nodes, so six nodes cannot form one. A six-node rank-one lattice rule is still a valid deterministic quadrature rule, and the Koksma–Hlawka inequality is stated for arbitrary finite nonempty point sets rather than only digital-net sizes.

Facts & Assumptions

Given: Base 2, dimension d=2, and node count N=6.

[F1]

A (t,m,d)-net in base b has exactly bm nodes. (Star discrepancy, digital nets, and digital sequences)

[F2]

A rank-one lattice rule accepts any integer N≥1 and a generator z with gcd⁡(z1,N)=1, and uses nodes xn,j={nzj/N}. (Digital point-set and rank-one lattice cube quadrature)

[F3]

Koksma–Hlawka is stated for any finite nonempty point multiset and integrand of finite upper-anchor Hardy–Krause variation. (Koksma–Hlawka integration bound with upper-anchor variation)

[F4]

Since 2>1, m↦2m is strictly increasing on the natural exponents, by the monotonicity-in-the-exponent clause of Monotonicity of x↦xn and of n↦an. The rank-one input with z1=1 and N=6 is admissible: 1 is a common divisor of 1 and 6, and every common divisor d satisfies d≤∣1∣=1 by If d∣a and a≠0 then d≠0 and ∣d∣≤∣a∣; hence the set of divisors of a nonzero integer is bounded above by ∣a∣, so gcd⁡(1,6)=1 by Common divisor, and the greatest common divisor gcd⁡(a,b), with the convention gcd⁡(0,0):=0.

Verification

technique · direct
1.1F1F4givenalgebra

The positive integer powers of 2 are 1,2,4,8,…: by [F4], if m≤2 then 2m≤22=4, while if m≥3 then 2m≥23=8. Hence no integer m≥0 gives 2m=6, so [F1] rules out a base-2 digital net with six nodes.

1.2F2F4givenalgebra

With N=6 and z=(1,1), [F2] and [F4] generate six nodes; the first coordinate is n/6 for n=0,…,5, so the nodes are distinct and the lattice-rule inputs are admissible.

2.1F1F3step 1.1step 1.2∎

The star discrepancy and the Koksma–Hlawka statement are defined for this six-node point set even though its size is not a power of 2. Thus a finite deterministic quadrature rule exists at this size, while the digital-net label and its elementary-interval guarantee do not apply.

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A smooth finite-variation integrand and its deterministic error bound

Example

On [0,1]2, take f(x,y)=xy and the one-point set P=((1/4,1/2)). Then VHK,1(f)=3,D1∗(P)=78,∣QP(f)−I2(f)∣=18, so the Koksma–Hlawka bound is valid for this smooth integrand.

Facts & Assumptions

Given: The function f(x,y)=xy on the unit square and the point set containing (1/4,1/2).

[F1]

For Cd functions, upper-anchor Hardy–Krause variation is the sum of the integrals of the absolute mixed derivatives on all nonempty upper faces. (Mixed-derivative formula for smooth Hardy–Krause variation)

[F2]

The unit square has volume 1; grid cells' volumes sum to that volume, and for the constant-one function every lower and upper Darboux sum equals the sum of the cell volumes, so its integral is 1. (Axis-parallel rectangles in Rm and their volume, Grid partitions of a rectangle in Rm, their cells, refinements and mesh, Lower and upper Darboux sums over a grid partition in Rm, The lower and upper Darboux integrals over a nondegenerate rectangle in Rm)

[F3]

A continuous function on the square is Riemann integrable, and its integrable sections have iterated integrals equal to the multiple integral. (Every continuous function on a closed nondegenerate rectangle in Rm is Riemann integrable, Riemann--Fubini on product rectangles, with lower and upper section integrals and content-zero exceptional sections)

[F4]

Star discrepancy is the supremum over u∈[0,1]d of the absolute difference between the fraction of nodes in [0,u) and its volume. (Star discrepancy, digital nets, and digital sequences)

[F5]

If G is continuous on [a,b], differentiable on (a,b), and its interior derivative has a Riemann-integrable extension, then its integral is G(b)−G(a). (Newton–Leibniz needs only continuity on [a,b], differentiability on (a,b), and a Riemann-integrable extension of the interior derivative)

[F6]

For a finite nonempty point multiset and an integrand of finite upper-anchor Hardy–Krause variation, ∣QP(f)−Id(f)∣≤DN∗(P)VHK,1(f). (Koksma–Hlawka integration bound with upper-anchor variation)

Verification

technique · direct
1.1F1F2givenalgebra

The upper faces are f(x,1)=x and f(1,y)=y, and the full mixed derivative is ∂xyf=1. By [F1], VHK,1(f)=∫011 dx+∫011 dy+∫[0,1]21 dx dy=1+1+1=3; the one-dimensional integrals and the square integral of 1 equal the respective volumes by [F2].

1.2F3F4F5givenalgebra

At u=(1/4,1/2) the point is excluded from the half-open anchored box, so the discrepancy there is 1/8. If u1≤1/4 or u2≤1/2, the box is empty and its volume is at most 1/2. If both coordinates exceed those thresholds, the box contains the point and its error is 1−u1u2≤1−(1/4)(1/2)=7/8; values approach 7/8 as u↓(1/4,1/2). Thus D1∗(P)=7/8. Also QP(f)=1/8. By [F3], the double integral equals the iterated Riemann integral, and [F5] evaluates it as I2(f)=∫01y(∫01x dx)dy=1/4.

2.1F6step 1.1step 1.2∎

The error is ∣1/8−1/4∣=1/8≤(7/8)⋅3=D1∗(P)VHK,1(f), consistent with [F6].

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An inverse-CDF singularity can be integrable but have infinite variation

Example

Let U have the uniform law on [0,1) and define g(u)=(1−u)−1/2 for 0≤u<1. Extend g to the closed cube by setting g(1)=0; this endpoint convention does not change g(U). The map g has distribution function FX(x)=0 for x<1 and FX(x)=1−x−2 for x≥1, and satisfies FX(g(u))=u for all 0≤u<1 (the inverse-CDF property in this example). Its expectation is finite, but VHK,1(g)=∞, so the Koksma–Hlawka bound gives no finite error guarantee for this integrand.

Facts & Assumptions

Given: A real random variable U with the uniform probability law on [0,1), represented by the identity map on ([0,1),B([0,1)),PU).

[A1]

For 0≤a<1, PU(U≤a)=a; thus PU(U>a)=1−a.

[F1]

A real random variable is a measurable map into R with its Borel sigma-algebra. (Random elements and real random variables, The Borel sigma-algebra of a topological space)

[F2]

A map between measurable spaces is measurable when the preimage of every measurable target set is measurable. (A measurable function between measurable spaces)

[F3]

The half-lines (−∞,x] generate the Borel sigma-algebra of R. (Seven generating families for the Borel sigma-algebra on the real line)

[F4]

A measurable function composed with a random element is measurable. (Composition with a Borel measurable outer map preserves measurability)

[F5]

The cumulative distribution function of a real random variable is FX(x)=P(X≤x). (Cumulative distribution function of a real random variable)

[F6]

For a>0, a−1/2=1/a, the square root is the unique nonnegative root, squaring preserves nonstrict order on nonnegative reals, and taking reciprocals reverses positive order; the equality case follows from trichotomy. (Rational powers ar of a positive base, Laws of rational exponents, Square roots exist: a unique a≥0 with (a)2=a; the positives are {x2:x≠0}, Squaring is monotone on the nonnegatives, Inverses of positives are positive, and reciprocation reverses order, Ordered field)

[F8]

The expectation of a nonnegative random variable is its extended Lebesgue integral. (Expectation of a nonnegative or integrable random variable)

[F9]

For a measurable h≥0, E[h(U)]=∫h dPU. (Change of variables for expectation)

[F10]

For nonnegative X, E[X]=∫0∞P(X>t) dt. (Layer-cake formulas for random variables)

[F11]

For rational p>1, ∫1∞t−p dt=1/(p−1). (The improper p-test for rational exponents)

[F12]

In dimension one, upper-anchor Hardy–Krause variation is ordinary total variation. (Hardy–Krause variation anchored at the upper corner)

[F13]

Koksma–Hlawka applies to a finite nonempty point multiset and requires finite upper-anchor Hardy–Krause variation. (Koksma–Hlawka integration bound with upper-anchor variation)

Proof

1.1givenF1F2F3F4F6construct

On [0,1) define g(u)=(1−u)−1/2. Since 0<1−u≤1, [F6] gives g(u)≥1. For x<1, the sublevel set {u:g(u)≤x} is empty. For x≥1, [F6] gives g(u)≤x exactly when x−2≤1−u, so this sublevel set is [0,1−x−2] (with the endpoint interpreted inside [0,1)). Each such set is Borel. Since the half-lines in [F3] generate the target Borel sigma-algebra and preimages commute with complements and countable unions, [F2] shows that g is measurable. Thus X:=g(U) is a real random variable by [F1] and [F4].

1.2F6F7F12givenchoose

For n≥1 put un=1−2−2n. By [F7], 0<un<1. The unique nonnegative square root of (2−n)2 is 2−n, so [F6] gives g(un)=2n. Given M>0, choose n with 2−n<2/(M+1) using [F7]; then g(un)>(M+1)/2. The grid with knots 0<un<1 has variation at least ∣g(un)−g(0)∣+∣g(1)−g(un)∣=2g(un)−1>M. Hence VHK,1(g)=∞ by [F12].

2.1A1F5F6step 1.1algebra

By [F5] and [A1], the distribution function of X is FX(x)=0 for x<1 and FX(x)=1−x−2 for x≥1. For each u<1, FX(g(u))=1−(g(u))−2=u, so g is the inverse-CDF transform on [0,1).

2.2A1F6F8F10F11step 1.1

For 0≤t<1, X≥1 gives P(X>t)=1. For t≥1, [F6] gives X>t exactly when U>1−t−2, and [A1] then gives P(X>t)=t−2. By [F8], [F10], and [F11] with p=2, E[X]=∫011 dt+∫1∞t−2 dt=1+1=2.

3.1F8F9step 1.1step 2.2

By [F9], change of variables for expectation applied to the measurable nonnegative g and random element U identifies E[X] with ∫g dPU. By [F8] and step 2.2 this value is finite and equals 2.

4.1F13step 3.1step 1.2∎

The expectation is finite by step 3.1, but the integrand has infinite upper-anchor variation by step 1.2. Therefore the finite-variation hypothesis in [F13] fails, so Koksma–Hlawka yields no finite error bound for this integrand.

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