By Daniel Iagolnitzer
Over a thousand mathematicians participated within the Paris overseas convention on Mathematical Physics and its satellite tv for pc convention on topology, strings and integrable versions. This quantity includes a few of the highlights, together with subject matters similar to conformable box concept and common relativity.
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Extra info for 11th International Congress of Mathematical Physics
To explain this we must first make a digression to discuss braids. 10 Braids A braid is similar to a knot or a link, but it differs essentially in that a direction of space (the vertical) is singled out. Moreover a braid consists of N pieces or strands each of which is constantly moving upwards. The strands can twist and Quantum Physics and the Topology of Knots 13 intertwine with each other but the final and initial positions are assumed to coincide (up to order). A braid thus has “loose ends”.
With E replaced by a 4-dimensional conformal manifold. The action we shall get will be conformally invariant by construction and intimately related to the Einstein action of gravity. In general, given an even dimensional conformal manifold T, dim E = n = 2m, we let H = L2 ^E , Ajg T*^ be the Hilbert space of square integrable forms of middle dimension, in which functions on E act as multiplication operators. We let F — 2P - 1 be the operator in H obtained from the orthogonal projection P on the image of d.
The relations in (4) with parts of physics were clearly very intriguing but were only fully clarified in 1988 by E Witten  who gave an elegant quantum theory interpretation of the Jones polynomial. To explain this we must first make a digression to discuss braids. 10 Braids A braid is similar to a knot or a link, but it differs essentially in that a direction of space (the vertical) is singled out. Moreover a braid consists of N pieces or strands each of which is constantly moving upwards. The strands can twist and Quantum Physics and the Topology of Knots 13 intertwine with each other but the final and initial positions are assumed to coincide (up to order).
11th International Congress of Mathematical Physics by Daniel Iagolnitzer