269 research outputs found
Sturm 3-ball global attractors 3: Examples of Thom-Smale complexes
Examples complete our trilogy on the geometric and combinatorial
characterization of global Sturm attractors which consist of a
single closed 3-ball. The underlying scalar PDE is parabolic, on the unit interval with Neumann boundary
conditions. Equilibria are assumed to be hyperbolic. Geometrically, we
study the resulting Thom-Smale dynamic complex with cells defined by the fast
unstable manifolds of the equilibria. The Thom-Smale complex turns out to be a
regular cell complex. In the first two papers we characterized 3-ball Sturm
attractors as 3-cell templates . The
characterization involves bipolar orientations and hemisphere decompositions
which are closely related to the geometry of the fast unstable manifolds. An
equivalent combinatorial description was given in terms of the Sturm
permutation, alias the meander properties of the shooting curve for the
equilibrium ODE boundary value problem. It involves the relative positioning of
extreme 2-dimensionally unstable equilibria at the Neumann boundaries and
, respectively, and the overlapping reach of polar serpents in the
shooting meander. In the present paper we apply these descriptions to
explicitly enumerate all 3-ball Sturm attractors with at most 13
equilibria. We also give complete lists of all possibilities to obtain solid
tetrahedra, cubes, and octahedra as 3-ball Sturm attractors with 15 and 27
equilibria, respectively. For the remaining Platonic 3-balls, icosahedra and
dodecahedra, we indicate a reduction to mere planar considerations as discussed
in our previous trilogy on planar Sturm attractors.Comment: 73+(ii) pages, 40 figures, 14 table; see also parts 1 and 2 under
arxiv:1611.02003 and arxiv:1704.0034
On vertices enforcing a Hamiltonian cycle
A nonempty vertex set X ⊆ V(G) of a hamiltonian graph G is called an of G if every X-cycle of G (i.e. a cycle of G containing all vertices of X) is hamiltonian. The h(G) of a graph G is defined to be the smallest cardinality of an H-force set of G. In the paper the study of this parameter is introduced and its value or a lower bound for outerplanar graphs, planar graphs, k-connected graphs and prisms over graphs is determined
A Gap-{ETH}-Tight Approximation Scheme for Euclidean {TSP}
We revisit the classic task of finding the shortest tour of points in -dimensional Euclidean space, for any fixed constant . We determine the optimal dependence on in the running time of an algorithm that computes a -approximate tour, under a plausible assumption. Specifically, we give an algorithm that runs in time. This improves the previously smallest dependence on in the running time of the algorithm by Rao and Smith (STOC 1998). We also show that a algorithm would violate the Gap-Exponential Time Hypothesis (Gap-ETH). Our new algorithm builds upon the celebrated quadtree-based methods initially proposed by Arora (J. ACM 1998), but it adds a simple new idea that we call \emph{sparsity-sensitive patching}. On a high level this lets the granularity with which we simplify the tour depend on how sparse it is locally. Our approach is (arguably) simpler than the one by Rao and Smith since it can work without geometric spanners. We demonstrate the technique extends easily to other problems, by showing as an example that it also yields a Gap-ETH-tight approximation scheme for Rectilinear Steiner Tree
Determinant Formulae for some Tiling Problems and Application to Fully Packed Loops
We present determinant formulae for the number of tilings of various domains
in relation with Alternating Sign Matrix and Fully Packed Loop enumeration
On the Spectral Gap of a Quantum Graph
We consider the problem of finding universal bounds of "isoperimetric" or
"isodiametric" type on the spectral gap of the Laplacian on a metric graph with
natural boundary conditions at the vertices, in terms of various analytical and
combinatorial properties of the graph: its total length, diameter, number of
vertices and number of edges. We investigate which combinations of parameters
are necessary to obtain non-trivial upper and lower bounds and obtain a number
of sharp estimates in terms of these parameters. We also show that, in contrast
to the Laplacian matrix on a combinatorial graph, no bound depending only on
the diameter is possible. As a special case of our results on metric graphs, we
deduce estimates for the normalised Laplacian matrix on combinatorial graphs
which, surprisingly, are sometimes sharper than the ones obtained by purely
combinatorial methods in the graph theoretical literature
Maximal diameter of integral circulant graphs
Integral circulant graphs are proposed as models for quantum spin networks
that permit a quantum phenomenon called perfect state transfer. Specifically,
it is important to know how far information can potentially be transferred
between nodes of the quantum networks modelled by integral circulant graphs and
this task is related to calculating the maximal diameter of a graph. The
integral circulant graph has the vertex set and vertices and are adjacent if ,
where . Motivated by the result on
the upper bound of the diameter of given in [N. Saxena, S. Severini,
I. Shparlinski, \textit{Parameters of integral circulant graphs and periodic
quantum dynamics}, International Journal of Quantum Information 5 (2007),
417--430], according to which represents one such bound, in this paper
we prove that the maximal value of the diameter of the integral circulant graph
of a given order with its prime factorization
, is equal to or , where
, depending on whether
or not, respectively. Furthermore, we show that, for a given
order , a divisor set with can always be found such that
this bound is attained. Finally, we calculate the maximal diameter in the class
of integral circulant graphs of a given order and cardinality of the
divisor set and characterize all extremal graphs. We actually show
that the maximal diameter can have the values , , and
depending on the values of and . This way we further improve the upper
bound of Saxena, Severini and Shparlinski and we also characterize all graphs
whose diameters are equal to , thus generalizing a result in that
paper.Comment: 29 pages, 1 figur
Strongly Correlated Random Interacting Processes
The focus of the workshop was to discuss the recent developments and future research directions in the area of large scale random interacting processes, with main emphasis in models where local microscopic interactions either produce strong correlations at macroscopic levels, or generate non-equilibrium dynamics. This report contains extended abstracts of the presentations, which featured research in several directions including selfinteracting random walks, spatially growing processes, strongly dependent percolation, spin systems with long-range order, and random permutations
LIPIcs, Volume 258, SoCG 2023, Complete Volume
LIPIcs, Volume 258, SoCG 2023, Complete Volum
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