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21 Dec 2012: 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).

8 Jun 2012: 8 of 21. [24] Thus, disentangling the effects of varying reflectioncoefficient and signal strength is not straightforward, espe-cially when tuning effects are important.

24 Aug 2012: 0.1. 0 10. 0. 0.4. 101108. x/l0 10. 0. 0.4. S = 3 S = 24. ... σxx = E(1 ν)(1 2ν) [(1 ν)xx νyy ],. σyy = E(1 ν)(1 2ν) [(1 ν)yy νxx ], (24).

15 Oct 2012: Aspects of fermions in magnetic AdS geometries. have been previously discussed in [20, 21, 22, 23, 24].

19 Dec 2012: 24 • • 25. οργανώθηκε η κοινωνία μας τα τελευταία 40 χρόνια, αφετέ-ρου δε, της πληθώρας ευτελών μηνυμάτων που, με τη βοή-θεια Μέσων Μαζικής

27 May 2012: carteri isachieved by cells at the bend points, which undergo adistinct transition in cell shape [20,22-24,26-29]. ... More-over, concerted movements of cells with respect to theCB system are crucial for the process of inversion in V.carteri

8 Mar 2012: 23. 4.1.3 The optical theorem. 24. 4.1.4 Solving for the asymptotic scattered wave. ... 4 QUANTUM SCATTERING IN 3D 24. where δl is a function of k.

6 Jun 2012: ithou. t per. mis. sion. P.H.Haynes Part II Mathematical Biology Lent Term 2012 24.

5 Sep 2012: 7.1. A new scheme of Dirichlet series for particular systems of the form(24). ... Byletting z = P 1y, the system (24) is equivalent to a transformed dynamical system.

3 Sep 2012: 24). So, by substituting (24) into (23), we have that. (P2M2)P1M1ϕ2 lBM2.