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3 Jul 2015: Downloaded to IP:. 129.169.173.200 On: Mon, 29 Jun 2015 16:19:24. 26F. ... Downloaded to IP:. 129.169.173.200 On: Mon, 29 Jun 2015 16:19:24.

10 Mar 2015: To give just two examples, excessive deformation of slender rods candescribe the failure of engineering components such as drill strings, masts and pipelines [24]as well as the conformations of biological

6 Aug 2015: charge builds up at the photoanode, leading to trapping of. electrons near the back electrode.23,24 Graphene, due to its. ... with lower l (usually the hole) limits transport23,24 andresults in charge accumulation at the contact/polymer inter-.

31 Jul 2015: 24. 35 10. 0. 24. 352. a2 cos(φ)2 (8). As discussed above, the LBMs in the t(1þ3)LG are Ramanactive, except LBM42 (Raman inactive). ... Phys. Rev. B:Condens. Matter Mater. Phys. 2011, 84, 035419. 24. Lui, C.

3 Jul 2015: 0.24 6 0.08 4000 6 10 380 6 5 395 6 5 15 6 10. ... 0.24 6 0.06 2000 6 10 362 6 10 304 6 10 58 6 20.

21 Dec 2015: 23,24], while. 1098-0121/2015/92(23)/235425(6) 235425-1 2015 American Physical Society. ... B 90, 161302(R)(2014). [24] G. Plechinger, P. Nagler, C. Schüller, and T.

2 Nov 2015: Once a Fermi-Dirac distribution is established [18,20],it cools down by optical phonon emission at the 100 fstime scale [16,21] and by scattering on acoustic phonons[22–24] ... H. MacDonald, Phys. Rev. Lett. 102, 206410(2009). [24] W.-K. Tse and S.

7 Jan 2015: hexagons (23, 24), transparent conductor; triangles (25–27),counter-electrode; rhombuses (41, 42), charge transport. ... and WS2(5.24%) in DSSCs using an organic disulfide/thiolate (T2/T. –)