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9 Aug 2005: #"$%&')(,-.%%&( 0/-#1""324%5/246"78&9:5. ;<8<'7>=@?9A@BA@BDCE<8F@<'8=HGIBDJK=B&L>MNMNO>PQ'/I JRI =BSA@BDCT8=G>=UVI ONJW(XY=ZL@Q. "M>L[AXYU]M>BDU=>_8B?IBDMNM>XaIBD?HQ.BI bDM>XcJ4I Ued=>_#'A@]G[XaI C?@M. ;'&'f2#PI JL[A@L[M>XCMNJKO>XgI,G[MNJABDMNhA@i? @

28 Oct 2005: Implied. Throughput. Z. 3.8e10. 7.4e9. 24.80. 22.98. 19%. Y. 3.0e10. 5.9e9. ... 24.55. 22.81. 20%. J. 2.9e10. 5.6e9. 24.50. 23.00. 25%. H. 3.0e10.

16 Feb 2005: 24 cm5 g2 K7/2. These opacity laws hold fairly well in ionized accretion discs, Kramers opacity in the outer.

26 Jul 2005: LT. 0.500E-01 CONF 1 E = 40.20 ( 0.043) rejected by energy CONF 1 E = 24.24 ( 0.123) is unique and stored as structure 12 CONF 1 E = ... 0.102) rejected by structure 16 CONF 1 E = -13.19 ( 0.631) rejected by starting geometry CONF 1 E = 24.24 ( 0.100)

10 Jan 2005: show. (b) Mean DER across all 24 development shows whenonly including c0 in clustering if the mean value is above a criticalthreshold. ... RT-04 RT-04 RT-04 23.86 24.12. Table 12. Progress since RT-03s on theeval04f data.

6 May 2005: informal discussion in Cambridgeon 24 March 2005 to formulate apolicy that would be acceptableto the majority of Quaternaryworkers.

9 Aug 2005: "# %$'&( )#,-)!/.0 1(2345276#89:. ;<-=?>A@CBDFEHGJILKMNBPO/QR=?BBMNSLTUI?<-SVTXWMZY[QRERM]D_VMN>F>a<. bdcfeCg3hjilkcfmniopqAmsrtumscfcHhltumNrvmstuwxcHhlyjtzi|{op+}gk/NhltNrc}gk/NhltNrc}UCv. fZnZ"sa"x-"|"3Zxx"nxnj"f ¡jn£¢x¤¥ ijileV "|yjwnhª

19 Sep 2005: 3.24). Posing the expansion η̂ = η̂0 ǫη̂1. it follows at leading order in ǫ that. ... with the boundary condition (3.24) reducing to η̂ = 0 at y = 0,L.

15 Aug 2005: a classical Runge–Kutta method, thus obtaining the so-called Runge–Kutta–Munthe-. Kaas (RKMK) class of schemes [24, 17]. ... Matrix Anal. Appl. 15 (1994), pp. 881-902. [24] H. Munthe-Kaas, High order Runge–Kutta methods on manifolds, Appl.

6 Oct 2005: 23 5.8 DATA FROM IT03, EARTHQUAKE 4. 24 5.9 DATA FROM IT03, EARTHQUAKE 5. ... PS.2. Max= 3.06. Min= -154. Max= 24.1. Min= -89.7. Max= 38.2.