Combinatorial Theory Seminar
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Tue, 03/05/2011 14:30 |
Bruce Reed (McGill) |
Combinatorial Theory Seminar |
L3 |
| In 1961 Hajos conjectured that if a graph contains no subdivsion of a clique of order t then its chromatic number is less than t. In 1981, Erdos and Fajtlowicz showed that the conjecture is almost always false. We show it is almost always true. This is joint work with Keevash, Mohar, and McDiarmid. | |||
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Tue, 10/05/2011 14:30 |
Penny Haxell (Waterloo) |
Combinatorial Theory Seminar |
L3 |
| We highlight a technique for studying edge colourings of multigraphs, due to Tashkinov. This method is a sophisticated generalisation of the method of alternating paths, and builds upon earlier work by Kierstead and Goldberg. In particular we show how to apply it to a number of edge colouring problems, including the question of whether the class of multigraphs that attain equality in Vizing's classical bound can be characterised. This talk represents joint work with Jessica McDonald. | |||
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Tue, 24/05/2011 14:30 |
Angelika Steger (ETH Zurich) |
Combinatorial Theory Seminar |
L3 |
A random planar graph is a graph drawn uniformly at random from the class of all (labelled) planar graphs on vertices. In this talk we show that with probability the number of vertices of degree in is very close to a quantity that we determine explicitly. Here . In the talk our main emphasis will be on the techniques for proving such results. (Joint work with Kosta Panagiotou.) |
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Tue, 31/05/2011 14:30 |
Colin Cooper (King's College London) |
Combinatorial Theory Seminar |
L3 |
We consider random walks on two classes of random graphs and explore the likely structure of the the set of unvisited vertices or vacant set. In both cases, the size of the vacant set can be obtained explicitly as a function of . Let be the subgraph induced by the vacant set. We show that, for random graphs above the connectivity threshold, and for random regular graphs , for constant , there is a phase transition in the sense of the well-known Erdos-Renyi phase transition. Thus for we have a unique giant plus components of size and for we have only components of size . In the case of we describe the likely degree sequence, size of the giant component and structure of the small ( ) size components. |
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Tue, 07/06/2011 14:30 |
Gregory Sorkin (LSE) |
Combinatorial Theory Seminar |
L3 |
| The 2-dimensional assignment problem (minimum cost matching) is solvable in polynomial time, and it is known that a random instance of size n, with entries chosen independently and uniformly at random from [0,1], has expected cost tending to π^2/6. In dimensions 3 and higher, the "planar" assignment problem is NP-complete, but what is the expected cost for a random instance, and how well can a heuristic do? In d dimensions, the expected cost is of order at least n^{2-d} and at most ln n times larger, but the upper bound is non-constructive. For 3 dimensions, we show a heuristic capable of producing a solution within a factor n^ε of the lower bound, for any constant ε, in time of order roughly n^{1/ε}. In dimensions 4 and higher, the question is wide open: we don't know any reasonable average-case assignment heuristic. | |||
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Tue, 14/06/2011 14:30 |
Jaroslav Nesetril (Prague) |
Combinatorial Theory Seminar |
L3 |
| It is known that generic and universal structures and Ramsey classes are related. We explain this connection and complement it by some new examples. Particularly we disscuss universal and Ramsey classes defined by existence and non-existence of homomorphisms. | |||

is a graph drawn uniformly at random from the class of all (labelled) planar graphs on
vertices. In this talk we show that with probability
the number of vertices of degree
in
that we determine explicitly. Here
. In the talk our main emphasis will be on the techniques for proving such results. (Joint work with Kosta Panagiotou.)
can be obtained explicitly as a function of
. Let
be the subgraph induced by the vacant set. We show that, for random graphs
above the connectivity threshold, and for random regular graphs
, for constant
, there is a phase transition in the sense of the well-known Erdos-Renyi phase transition. Thus for
we have a unique giant plus components of size
and for
we have only components of size