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hep-th/9705162
https://api.newton.ac.uk/website/v0/events/preprints/NI97028The possibility ofa 9-brane in M-theory has also been discussed in [24,54]. ... 1. Then P[u] can be writtenas Paua, dening the ADM D-momentum Pa = P[ka]. -
.PDF
https://api.newton.ac.uk/website/v0/annual-reports/1999/2000Structure Formation in the Universe 22. Developments in Solid Mechanics and Materials Sciences 24. ... Professor KA Brown University of Glasgow. Professor EB Davies, FRS Kings College London. -
MW-final.dvi
https://api.newton.ac.uk/website/v0/events/preprints/NI14098ev(u′′ 12. u′v′1. 2u′2. 1. ru′ 1. rv′)=. 16πG. c2p, (2.24). ... Φν = Dνφ, φ = φ(r). 24 CONTENTS. Thus we have. -
STRUCTURAL CONNECTIONS BETWEEN A FORCING CLASS ANDITS MODAL LOGIC ...
https://api.newton.ac.uk/website/v0/events/preprints/NI12055w. aka. By adding dummy worlds to each cluster, we may assume that all theclusters have size ka = 2. -
Hitting probabilities for systems of non-linear stochastic heat…
https://api.newton.ac.uk/website/v0/events/preprints/NI1204524. E1” if αi α0. The at most d other eigenvectors with a “small projection on E1” will eachcontribute a factor of order (|ts|. -
HOMOGENIZATION OF NONSTATIONARY SCHR�ODINGER TYPE EQUATIONS WITH…
https://api.newton.ac.uk/website/v0/events/preprints/NI15047E(t,τ) = ieiτA(t). 16j,l6p: j 6=lJjl(t,τ), (3.24). Jjl(t,τ) = t3. τ0. ... MeiτA(t)M1P̂ M0eiτt2M0ŜM0M10 P̂‖. 6 ‖M‖2‖M1‖2‖eiτA(t)P eiτt2SPP‖,(5.13). 24 T. A. SUSLINA. ‖eiτA(t)P eiτt2SPP‖. -
FINAL.PDF
https://api.newton.ac.uk/website/v0/annual-reports/2001/2002J Brindley University of LeedsProfessor KA Brown University of GlasgowProfessor EB Davies FRS Kings College LondonProfessor PJ Diggle University of LancasterProfessor CM Elliott University of SussexProfessor EG Rees University of EdinburghDr
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