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4 Aug 2015: The future of ultrashort laser pulses July 24, 2014Rapid advances in techniques for the creation of ultra-short laser pulses promise to.

14 Oct 2015: as a hyperelastic material usingthe Mooney-Rivlin fit with parameters E 1.23 MPa,C1 0.205 MPa, C2 0 MPa (corresponding to a 24-hour cure at 60 C) [49]. ... 24] Z. Xu, Z. Liu, H. Sun, and C. Gao, Highly electricallyconductive Ag-doped graphene fibers as

15 Jun 2015: 6oC 10. oC. 18oC 24. oC. 30oC 40. oC. 50oC. In.

23 Apr 2015: stress. The specific self-stress t thus becomes. t l1k1l2k2. rðk1 þk2Þ. 24. ... at CAMBRIDGE UNIV LIBRARY on April 23, 2015pic.sagepub.comDownloaded from. 24. French MJ and Widden MB.

22 Jan 2015: Dec 24, 2014. When it comes to engineering single-layer atomic structures, "minding the gap" will help researchers create artificial.

17 Jun 2015: We use the local density approximation22. within the Vienna ab initio simulation package,23 and the projectoraugmented wave (PAW)24 method. ... B 1996, 54, 1116911186.(24) Blochl, P. E. Phys. Rev. B 1994, 50, 1795317979.(25) Ferrari, A.

23 Apr 2015: Drosophila strains and microscopyThe following stocks were used: ubiECad-GFP –hereinafter. ECadGFP [24], sGMCA [12,25]; zipperCPTI002907 (available. ... MbsN300 (24 embryos/115 vertices) (B), ASGal4/UAS-ctMLCK (17 embryos/101 vertices) (C), and

29 Jan 2015: We useCNTs produced by catalytic chemical vapor deposition ofCH4 over Mg1xCoxO solid solution containing Mo oxide[24]. ... 24. E. Flahaut, Ch. Laurent, and A. Peigney, Carbon 43, 375(2005).

30 Mar 2015: Here, we use a numerical estimation from Blinder [24], for a cylindrical permanentmagnet which involves a triple integral that is solved numerically in cylindrical coordi-nates. ... Wiley and Sons, New York, 1987.[24] S. Blinder, Magnetic field of a

24 Dec 2015: the second harmonic generation from reference materials,for example, beta barium borate or iron(III) iodate crystals.24. ... IEEE Photon. Technol. Lett.2012, 24, 17921794.(16) Li, B.; Cheng, Y.; Liu, J.; Yi, C.; Brown, A.

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. –)