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4 Nov 2013: Carbon budgets have been introduced to capemissions [24] (Figure 1). The power sector is the single largest emitter. ... and are designed to capemissions [24] (green line).

20 Dec 2013: T(η,ω,X) = TabcηaωbXc. (2.24). This formula generalizes in the obvious way to a (r,s) tensor. ... Thisis easiest to demonstrate with an example. Part 3 General Relativity 4/11/13 24 H.S.

26 Jul 2013: Contents. Front Pages. Aboutthe Authors. Subject Index. UserInstructions. LicenseAgreement. Chapter 19 in Handbook of Experimental Fluid Dynamics,C. Tropea, A. Yarin, J. F. Foss (Eds.). Springer, New-York (2007), ISBN: 978-3-540-25141-5.

5 Oct 2013: 3 Consistent reconstructions and oblique projections. We now consider the consistent sampling technique of [24, 25, 29, 56, 58]. ... An analysis of consistent reconstructions, which we shall recap and extend in 3.3, was given in[24, 25, 29].

19 Oct 2013: π. L. L2 D2. As (y′) dy′. (4.24). This expression can be cross-checked by evaluating the y-components of the sourceand sink recoil forces in (3.6) to ... 5.24). The direction of RV is not, of course, exactly parallel to ŷ, but rather makes anO( 2)

26 Jul 2013: Received 24 May 2002; accepted 17 December 2002; published online 30 June 2003.

12 Aug 2013: Cont. Dynamical Sys. 28, 1345–1367. 24. Figure 3.4: The errors for h(t) for ω = 200π (top row) and ω = 2000π(bottom row): from the left 0, 1 and

19 Oct 2013: Fluid. Dyn. Res., 24, 375–404.Janssen, P. A. E. M. 1982 Quasilinear approximation for the spectrum of wind-generated.

5 Oct 2013: The second inclusion follows by Theorem VIII.24 ([RS72], p. 290)if we can show that PnAPn A in the strong resolvent sense. ... 11. Proof. Now, (i) follows from the fact that A1,n A strongly (see Theorem VIII.24 in [RS72],p.

5 Oct 2013: The problem is not new, and therehave been many different approaches developed for its solution (see, for example, [2, 11, 12, 17, 18, 22,23, 24, 25, 52] and references therein).