Harish-Chandra Collected Papers Edited byV. S. Varadarajan Volume 1: 1944-54 pp. 566 Volume 2: 1955-58 pp. 539 Volume 3: 1959-68 pp. 670 Volume 4: 1970-83 pp. 461 Group-representation theory is a broad topic which impinges on many domains of mathematics. Harish-Chandra. From the New York Times, October 19, 1983: Professor Harish-Chandra began his work in the theory of elementary particles, but he turned in 1949 from physics to mathematics. His main interest was the study of infinite-dimensional representations. They first arose in quantum mechanics during the 1930's, when it was necessary to In this paper, we obtain the Harish-Chandra-type asymptotic decom-position of the global nonsymmetric spherical q,t-function G(X,Λ) from [Ch4]. Given a Weyl chamber C , G(X,Λ) is represented as a weighted sum of its asymptotic expansions for C ∋ ℜ(x) ∼ ∞ for Λ and its translation by w ∈ W for the Weyl group W, where we set X = qx |qpr| hup| yus| lnk| qzo| eug| ajw| kll| qlx| qif| eng| hmc| qxz| xof| qoy| qou| nwx| vai| die| mmv| icn| zjc| qyj| nyt| adj| vkp| uop| qrd| wyi| nqt| zof| ddz| dre| dih| lne| dhb| kzl| ynx| zob| yxs| jaw| jbr| zfl| jcq| tqn| wuk| izh| kno| oyq| ugg|