19,391,177 research outputs found

    The O(g4)O(g^4) Lipatov Kernels

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    Leading plus next-to leading log results for the Regge limit of massless Yang-Mills theories are reproduced by reggeon diagrams in which the Regge slope α0\alpha' \to 0 and reggeon amplitudes satisfy Ward identity constraints at zero transverse momentum. Using reggeon unitarity together with multiple discontinuity theory a complete set of such diagrams can be constructed. The resulting two-two, one-three and two-four kernels which generalise the Lipatov equation at O(g4)O(g^4) are determined uniquely.Comment: 12 pages, ANL-HEP-PR-94-2

    Equivariant Corks

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    For suitable finite groups G, we construct contractible 4-manifolds C with an effective G-action on C\partial C whose associated pairs (C,g) for all gGg \in G are distinct smoothings of the pair (C,C)(C,\partial C). Indeed C embeds in a 4-manifold so that cutting out C and regluing using distinct elements of G yield distinct smooth 4-manifolds.Comment: 9 pages, 3 figure

    The 4-girth-thickness of the complete multipartite graph

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    The gg-girth-thickness θ(g,G)\theta(g,G) of a graph GG is the smallest number of planar subgraphs of girth at least gg whose union is GG. In this paper, we calculate the 44-girth-thickness θ(4,G)\theta(4,G) of the complete mm-partite graph GG when each part has an even number of vertices.Comment: 6 pages, 1 figur

    3D gauged supergravity from SU(2) reduction of N=1N=1 6D supergravity

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    We obtain Yang-Mills SU(2)×GSU(2)\times G gauged supergravity in three dimensions from SU(2)SU(2) group manifold reduction of (1,0) six dimensional supergravity coupled to an anti-symmetric tensor multiplet and gauge vector multiplets in the adjoint of GG. The reduced theory is consistently truncated to N=4N=4 3D supergravity coupled to 4(1+dimG)4(1+\textrm{dim}\, G) bosonic and 4(1+dimG)4(1+\textrm{dim}\, G) fermionic propagating degrees of freedom. This is in contrast to the reduction in which there are also massive vector fields. The scalar manifold is R×SO(3,dimG)SO(3)×SO(dimG)\mathbf{R}\times \frac{SO(3,\, \textrm{dim}\, G)}{SO(3)\times SO(\textrm{dim}\, G)}, and there is a SU(2)×GSU(2)\times G gauge group. We then construct N=4N=4 Chern-Simons (SO(3)R3)×(GRdimG)(SO(3)\ltimes \mathbf{R}^3)\times (G\ltimes \mathbf{R}^{\textrm{dim}G}) three dimensional gauged supergravity with scalar manifold SO(4,1+dimG)SO(4)×SO(1+dimG)\frac{SO(4,\,1+\textrm{dim}G)}{SO(4)\times SO(1+\textrm{dim}G)} and explicitly show that this theory is on-shell equivalent to the Yang-Mills SO(3)×GSO(3)\times G gauged supergravity theory obtained from the SU(2)SU(2) reduction, after integrating out the scalars and gauge fields corresponding to the translational symmetries R3×RdimG\mathbf{R}^3\times \mathbf{R}^{\textrm{dim}\, G}.Comment: 24 pages, no figures, references added and typos correcte

    Beyond Ohba's Conjecture: A bound on the choice number of kk-chromatic graphs with nn vertices

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    Let ch(G)\text{ch}(G) denote the choice number of a graph GG (also called "list chromatic number" or "choosability" of GG). Noel, Reed, and Wu proved the conjecture of Ohba that ch(G)=χ(G)\text{ch}(G)=\chi(G) when V(G)2χ(G)+1|V(G)|\le 2\chi(G)+1. We extend this to a general upper bound: ch(G)max{χ(G),(V(G)+χ(G)1)/3}\text{ch}(G)\le \max\{\chi(G),\lceil({|V(G)|+\chi(G)-1})/{3}\rceil\}. Our result is sharp for V(G)3χ(G)|V(G)|\le 3\chi(G) using Ohba's examples, and it improves the best-known upper bound for ch(K4,,4)\text{ch}(K_{4,\dots,4}).Comment: 14 page
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