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2( 0>?-0 8.;()-./ =-J ()'?== '20B 2' ()8( ()203 @ <<?B -( '023 () 3?B) 81-0 ()203 KA)203 k4m 2'n 80<; 8.< 0-/)( KF6,LL ()8(.

p(m)qkd (kA,kB) = Pr(KA = kA,KB = kB|M = m). (1). ... KA, kA, KB, kB: output keys for Alice and Bob.

ùEû=,?:7A9 @46D'Dû @lZE4D@l=" Ká Ço$#$$B>Ñ.H/2«K W Q û@«ù»=,ZKZK@rB[¢=&9 _)7:9ý[ Z=)_)ú ù»D«[ ... A@ =,Z4B[û@rZ7FùT4,?ùT=,?:?A=&7:_7FB ka«$è:L O á5ú$øCù»G$2û7FùEûa7:5[?

P1],[P2], [KU4]). This was essentially proved by Kaplansky in [KA], using the notion of“pseudo Cauchy sequence” instead of “nest of balls”. ... KA], [KU4]). These polynomials are defined suchthat the following Taylor expansion holds in arbitrary

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Definable sets in algebraically closed valuedfields: elimination of imaginaries. Deirdre Haskell Ehud Hrushovski † Dugald Macpherson ‡. July 19, 2005. 2000 Mathematics Subject Classification: 03C60. Abstract.It is shown that if K is an

19] JC Crocker, MT Valentine, ER Weeks, T Gisler, PD Ka-plan, AG Yodh, and DA Weitz Phys Rev Lett 85, 888(2000).

Then the time–space projection of the Killing operator acting on Ka is [3,4]. ... aAa, andthe third term is also zero because Ka is a Killing vector.

Then a kA and so theset {b : kb = a} is not empty.

Four lectures in semiclassical analysis for non. self-adjoint problems with applications to. hydrodynamic instability. Bernard Helffer. Université Paris-Sud. Cime in Cetraro, June 2006. Abstract. Our aim is to show how semi-classical analysis can