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Showing papers in "Journal of Geometry in 2022"


Journal ArticleDOI
TL;DR: The point-plane, the point-line, and the plane-line incidence matrices are of interest in combinatorics, finite geometry, graph theory and group theory as mentioned in this paper .
Abstract: The point-plane, the point-line, and the plane-line incidence matrices of $$\mathrm {PG}(3,q)$$ are of interest in combinatorics, finite geometry, graph theory and group theory. Some of the properties of these matrices and their submatrices are related with the interplay of orbits of points, lines and planes under the action of subgroups of $$\mathrm {PGL}(4,q)$$ . A remarkable particular case is the subgroup $$G\cong \mathrm {PGL}(2,q)$$ , viewed as the stabilizer group of the twisted cubic $$\mathscr {C}$$ . For this case, the study of the point-plane incidence matrix, initiated by D. Bartoli and the present authors, has attracted attention as being related to submatrices with useful applications in coding theory for the construction of multiple covering codes. In this paper, we extend our investigation to the plane-line incidence matrix apart from just one class of the line orbits, named $$\mathcal {O}_6$$ in the literature. For all $$q\ge 2$$ , in each submatrix, the numbers of lines in any plane and planes through any line are obtained. As a tool for the present investigation, we use submatrices of incidences arising from orbits of planes and unions of line orbits, including $$\mathcal {O}_6$$ . For each such submatrix we determine the total number of lines from the union in any plane and the average number of planes from the orbit through any line of the union.

13 citations


Journal ArticleDOI
TL;DR: In this article , the authors extended the point-plane incidence matrix to the plane-line incidence matrix and showed that for each submatrix, the number of lines in any plane and planes through any line is obtained.
Abstract: The point-plane, the point-line, and the plane-line incidence matrices of $$\mathrm {PG}(3,q)$$ are of interest in combinatorics, finite geometry, graph theory and group theory. Some of the properties of these matrices and their submatrices are related with the interplay of orbits of points, lines and planes under the action of subgroups of $$\mathrm {PGL}(4,q)$$ . A remarkable particular case is the subgroup $$G\cong \mathrm {PGL}(2,q)$$ , viewed as the stabilizer group of the twisted cubic $$\mathscr {C}$$ . For this case, the study of the point-plane incidence matrix, initiated by D. Bartoli and the present authors, has attracted attention as being related to submatrices with useful applications in coding theory for the construction of multiple covering codes. In this paper, we extend our investigation to the plane-line incidence matrix apart from just one class of the line orbits, named $$\mathcal {O}_6$$ in the literature. For all $$q\ge 2$$ , in each submatrix, the numbers of lines in any plane and planes through any line are obtained. As a tool for the present investigation, we use submatrices of incidences arising from orbits of planes and unions of line orbits, including $$\mathcal {O}_6$$ . For each such submatrix we determine the total number of lines from the union in any plane and the average number of planes from the orbit through any line of the union.

8 citations


Journal ArticleDOI
TL;DR: In this paper , the authors give a short introduction to discrete flat fronts in hyperbolic space and prove that any discrete flat front in the mixed area sense admits a Weierstrass representation.
Abstract: Abstract We give a short introduction to discrete flat fronts in hyperbolic space and prove that any discrete flat front in the mixed area sense admits a Weierstrass representation.

3 citations



Journal ArticleDOI
TL;DR: In this paper , the Weitzenb\"ock curvature operator is realized as the Dirichlet energy of a finite graph, weighted by a matrix of the curvature matrix.
Abstract: We exhibit a curious link between the Quadratic Orthogonal Bisectional Curvature, combinatorics, and distance geometry. The Weitzenb\"ock curvature operator, acting on real (1,1)--forms, is realized as the Dirichlet energy of a finite graph, weighted by a matrix of the curvature. These results also illuminate the difference in the nature of the Quadratic Orthogonal Bisectional Curvature and the Real Bisectional Curvature.

2 citations












Journal ArticleDOI
TL;DR: In this paper , the authors apply WQH switching to construct a non-geometric cospectral with the line graph of an incidence geometry with a linear representation, which is not point graphs of partial geometries.
Abstract: For an incidence geometry $${\mathcal G}= ({\mathcal P}, {\mathcal L}, {\text {I}})$$ with a linear representation $${\mathcal T}_2^*({\mathcal K})$$ , we apply WQH switching to construct a non-geometric graph $$\Gamma '$$ cospectral with the line graph $$\Gamma $$ of $${\mathcal G}$$ . As an application, we show that for $$h \ge 2$$ and $$0< m < h$$ , there are strongly regular graphs with parameters $$(v, k, \lambda , \mu ) = (2^{2\,h} (2^{m+h}+2^m-2^h), 2^h (2^h+1)(2^m-1), 2^h (2^{m+1}-3), 2^h (2^m-1))$$ which are not point graphs of partial geometries of order $$(s,t,\alpha ) = ((2^h+1)(2^m-1), 2^h-1, 2^m-1)$$ .




Journal ArticleDOI
TL;DR: In this paper , the authors further extend the Grünbaum Incidence Calculus and refine the bounds for k = 5 and k = 6, and show that for each k, there exists an integer n such that for all n \ge N{k} there exists at least one configuration, with current records n = 576 and n = 7350, respectively.
Abstract: The “Grünbaum Incidence Calculus” is the common name of a collection of operations introduced by Branko Grünbaum to produce new \((n_{4})\) configurations from various input configurations. In a previous paper, we generalized two of these operations to produce operations on arbitrary \((n_k)\) configurations, and we showed that for each k, there exists an integer \(N_{k}\) such that for all \(n \ge N_{k}\), there exists at least one \((n_{k})\) configuration, with current records \(N_{5}\le 576\) and \(N_{6}\le 7350\). In this paper, we further extend the Grünbaum Calculus; using these operations, as well as a collection of previously known and novel ad hoc constructions, we refine the bounds for \(k = 5\) and \(k = 6\). Namely, we show that \(N_5 \le 166\) and \(N_{6}\le 585\).

Journal ArticleDOI
TL;DR: In this paper , the authors show that every finite subunital of any generalized hermitian unital is itself a Hermitian Unital and the embedding is given by an embedding of quadratic field extensions.
Abstract: Abstract Every finite subunital of any generalized hermitian unital is itself a hermitian unital; the embedding is given by an embedding of quadratic field extensions. In particular, a generalized hermitian unital with a finite subunital is a hermitian one (i.e., it originates from a separable field extension).


Journal ArticleDOI
TL;DR: In this article , it was shown that the smallest area convex domain of constant width w in the 2-dimensional spherical space is the spherical Reuleaux triangle for all w
Abstract: The Blaschke–Leichtweiss theorem (Leichtweiss in Abh Math Semin Univ Hambg 75:257–284, 2005) states that the smallest area convex domain of constant width w in the 2-dimensional spherical space $${\mathbb {S}}^2$$ is the spherical Reuleaux triangle for all $$0







Journal ArticleDOI
TL;DR: In this article , the potential vector field has a finite global norm in a complete non-trivial, non-compact quasi Yamabe soliton with finite volume and the scalar curvature becomes constant.
Abstract: In this article, we have proved some results in connection with the potential vector field having finite global norm in quasi Yamabe soliton. We have derived some criteria for the potential vector field on the non-positive Ricci curvature of the quasi Yamabe soliton. Also, a necessary condition for a compact quasi Yamabe soliton has been formulated. We further showed that if the potential vector field has a finite global norm in a complete non-trivial, non-compact quasi Yamabe soliton with finite volume, then the scalar curvature becomes constant and the soliton reduces to a Yamabe soliton.