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This paper treats the L2-discrepancy of digital (0, 1)-sequences over ℤ2, and gives conditions on the generator matrix of such a sequence which guarantee minimal possible order of L2-discrepancy of the generated sequence. The existence is proved for the first time of digital (0; 1)-sequences over ℤ2 with L2-discrepancy of order . This order is best possible by a result of K. Roth. The existence proof is constructive.
Let be a finite-dimensional vector space over a square-root closed ordered field (this restriction permits an inner product with corresponding norm to be imposed on ). Many properties of the family :=() of convex polytopes in can be expressed in terms of valuations (or finitely additive measures). Valuations such as volume, surface area and the Euler characteristic are translation invariant, but others, such as the moment vector and inertia tensor, display a polynomial behaviour under translation. The common framework for such valuations is the polytope (or Minkowski) ring Π:=Π(), and its quotients under various powers of the ideal T of Π which is naturally associated with translations. A central result in the theory is that, in all but one trivial respect, the ring Π/T is actually a graded algebra over . Unfortunately, while the quotients Π/Tk+1 are still graded rings for k > 1, they now only possess a rational algebra structure; to obtain an algebra over , some (weak) continuity assumptions have to be made, although these can be achieved algebraically, by factoring out a further ideal A, the algebra ideal.
The classical Minkowski sum of convex sets is defined by the sum of the corresponding support functions. The Lp-extension of such a definition makes use of the sum of the pth power of the support functions. An Lp-zonotope Zp is the p-sum of finitely many segments and is isometric to the unit ball of a subspace of ℓq, where 1/p + 1/q = 1. In this paper, a sharp upper estimate is given of the volume of Zp in terms of the volume of Z1, as well as a sharp lower estimate of the volume of the polar of Zp in terms of the same quantity. In particular, for p = 1, the latter result provides a new approach to Reisner's inequality for the Mahler conjecture in the class of zonoids.
A tensor-type integral formula for intrinsic volumes is used to define a further variant of directed projection functions and show that these determine a convex body uniquely. Averages of directed projection functions are then studied, and the connections between the resulting operators and previously considered spherical transforms discussed.
In this paper a notion of difference function Δf is introduced for real-valued, non-negative and log-concave functions f defined in Rn. The difference function represents a functional analogue of the difference body K + (−K) of a convex body K. The main result is a sharp inequality which bounds the integral of Δf from above in terms of the integral of f. Equality conditions are characterized. The investigation is extended to an analogous notion of difference function for α-concave functions, with α < 0. In this case also an upper bound for the integral of the α-difference function of f in terms of the integral of f is proved. The bound is sharp in the case α = −∞ and in the one-dimensional case.
Let B (“black”) and W (“white”) be disjoint compact test sets in ℝd, and consider the volume of all its simultaneous shifts keeping B inside and W outside a compact set A ⊂ ℝd. If the union B ∪ W is rescaled by a factor tending to zero, then the rescaled volume converges to a value determined by the surface area measure of A and the support functions of B and W, provided that A is regular enough (e.g., polyconvex). An analogous formula is obtained for the case when the conditions B ⊂ A and W ⊂ AC are replaced by prescribed threshold volumes of B in A and W in AC. Applications in stochastic geometry are discussed. First, the hit distribution function of a random set with an arbitrary compact structuring element B is considered. Its derivative at 0 is expressed in terms of the rose of directions and B. An analogous result holds for the hit-or-miss function. Second, in a design based setting, different random digitizations of a deterministic set A are treated. It is shown how the number of configurations in such a digitization is related to the surface area measure of A as the lattice distance converges to zero.
It is proved that the reciprocal of the volume of the polar bodies, about the Santaló point, of a shadow system of convex bodies Kt, is a convex function of t, thus extending to the non-symmetric case a result of Campi and Gronchi. The case that the reciprocal of the volume is an affine function of t is also investigated and is characterized under certain conditions. These results are applied to prove an exact reverse Santaló inequality for polytopes in ℝd that have at most d + 3 vertices.
Quasi-residual designs can be useful in constructing symmetric designs. However, there are quasi-residual designs that cannot be embedded in a symmetric design. This may happen because the corresponding symmetric design does not exist. Another reason for nonembeddability could be the existence of several blocks whose intersection sizes do not allow them to be extended to blocks of a symmetric design. Also, a quasi-residual design may have a substructure preventing it from embeddability in a symmetric design.
Quasi-residuals of non-existing symmetric designs
Recall that a (v, b, r, k, λ)-design is called quasi-residual if r = k + λ. This condition is satisfied by any residual design of a symmetric (v + r, r, λ)-design. If a quasi-residual design is isomorphic to a residual of a symmetric design D, it is said to be embeddable inD. In this section we will construct several families of quasi-residual (v, b, r, k, λ)-designs for which a symmetric (v + r, r, λ)-design does not exist.
To obtain the first family of such designs, let D be the (v – 1)-fold multiple of the complete symmetric (v, v – 1, v – 2)-design. Then D is a (v, v(v – 1), (v – 1)2, v – 1, (v – 1)(v – 2))-design, so D is quasi-residual. If D is embeddable in a symmetric design, then the complement of this symmetric design is a projective plane of order v – 1. Nowthe Bruck–Ryser Theorem gives an infinite family of non-embeddable quasi-residual designs.
If the action of an automorphism group of a symmetric design on the block set is known, then the design can be constructed by finding one (base) block from each block orbit and then applying the automorphism group to obtain the remaining blocks. If a symmetric design admits an automorphism group such that all blocks of the design form a single orbit, then the group itself can be regarded as the point set of the design. The base block becomes a subset of the group and such subsets are called difference sets. The designs obtained from difference sets admit group invariant incidence matrices.
Group rings are a natural setting for investigating difference sets. The notion of a group of symmetries of a subset of a group ring will be crucial to constructing symmetric designs in subsequent chapters.
Group invariant matrices and group rings
A group invariant matrix is a matrix of order v whose columns can be obtained from the first column by applying all elements of a certain permutation group of order v to the entries of the first column. If we assume that the rows and columns of the matrix are indexed by the elements of the group, then this description leads us to the following definition.
Prototypes of many combinatorial designs come from finite projective geometries and finite affine geometries. Vector spaces over finite fields provide a natural setting for describing these geometries. Among the numerous incidence structures that can be constructed using affine and projective geometries are infinite families of symmetric designs, nets and Latin squares. Subspaces of a vector space over a finite field can be regarded as linear codes that will be used in later chapters for constructing other combinatorial structures, such as Witt designs and balanced generalized weighing matrices.
Finite fields
In this section we recall a few basic results on finite fields which will be used throughout this book.
For any prime p, the residue classes modulo p with the usual addition and multiplication form a finite field GF(p) of order p. These fields are called prime fields. Any finite field F of characteristic p contains GF(p) as a subfield. The field F then can be regarded as a finite-dimensional vector space over GF(p), and therefore, |F| = pn where n is the dimension of this vector space. Conversely, for any prime power q = pn, there is a unique (up to isomorphism) finite field of order q. This field is denoted by GF(q) and is often called the Galois field of order q. In general, the field GF(q) is isomorphic to (a unique) subfield of the field GF(r) if and only if r is a power of q.
An affine plane of order n has n2 + n lines, any two of which are either parallel or intersecting. The relation of parallelism on the set of lines is an equivalence relation, and so it partitions the set of lines into n + 1 parallel classes of cardinality n. Each point lies on exactly one line from each parallel class. The block set of the complement of an affine plane of order n can be partitioned into n + 1 classes so that each point is contained in exactly n – 1 blocks from each class. Similar partitions exist in affine geometries of higher dimension. In this chapter we study a more general notion of resolution of an incidence structure, i.e., a partition of the block set of the structure into classes so that each point is contained in a constant number of blocks from each class.
Bose's Inequality
The incidence structures on which we define the notion of resolution are pairwise balanced designs.
Definition 5.1.1. Let λ be a positive integer. A pairwise balanced design (PBD) of index λ is an incidence structure D = (X, B, I) such that X ≠ Ø, every x ∈ X is incident with more than λ blocks, and, for any distinct x, y ∈ X, there are precisely λ blocks that are incident with both x and y. If a PBD of index λ has constant replication number r, it is called an (r, λ)-design.