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5 Aug 2011: 02 Aug 2011 12:24 | by Matthew Finnegan in London | Filed in Hardware IM Flash Smartphone 0 Comments.

20 Aug 2008: and mechanical and environ-mental robustness.11–24 To date, SWNT-based saturable ab-sorbers have been used to mode-lock fiber,12–21 waveguide,22. ... solid-state,23 and semiconductor lasers.24 These cover abroad range from 1 to 1.6 m.12–24

6 Oct 2010: NASDAQ 2394.09 -5.74 (-0.24%). Stocks on the Move. By Naomi Kresge - Oct 5, 2010 4:42 PM GMT.

28 Aug 2013: BUSINESS August 24, 2013, 12:30 p.m. ET. Graphene is an extrem ely thin, strong and flexible m aterial derived from the graphite found in everydaypencils.

21 Nov 2018: We use a 24 24 1 k-grid tocalculate the BetheSalpeter kernel. ... The real-time simulation adoptsa coarse 24 24 1 and a denser 61 61 1 k-grid.

14 Jan 2010: D) decreaseswith decreasing La.24 In this case, I(D)/I(G) C=()La2,with C=(514.5 nm) 0.55 nm2.24 Combining the. ... 24. Ferrari, A. C.; Robertson, J. Interpretation of Raman Spectraof Disordered and Amorphous Carbon.

7 Apr 2017: 0.1. 0.24 0.26 0.28 0.3 0.32 0.34. σ00 = 0.345 exp(220 [K. ... vol. 102, no. 5, p. 054517, 2007. [24] M. Le Gallo, A.

15 Feb 2021: 61. calculated S for LO phonons as a function of the polarizationparameter for 1L-MoSe2, finding 1.93–2.24. ... B 56, 1077–1080 (1997). 24. Scarpelli, L. et al. Resonantly excited exciton dynamics in two-dimensionalMoSe2 monolayers.

22 Nov 2013: spread across 24 UK universities. The funding, targeted at areas vital to economic growth, has been allocated by the Engineering and.

13 Nov 2006: 26] (see footnote 24, for qK, 00 0) andRef. [24]. This differs from the model of Ref. ... Pfeiffer et al., Phys. Rev. B 71, 155409 (2005).[24] J. Maultzsch, S.

15 Feb 2011: diameters,8,18 while thisis an intrinsic property of graphene, due to the gapless lineardispersion of Dirac electrons.19–22,24 Q-switching was re-ported using SWNTs: Ref. ... Offerhaus,and D. J. Richardson, Opt. Lett. 24, 388 1999. 4M. Siniaeva, M.

8 Oct 2008: Phys. ReV. Lett. 1970, 24, 156–159.(2) Ashkin, A.; Dziedzic, J. M.; Bjorkholm, J.E.; Chu, S. ... Phys. ReV.Lett. 2008, 100, 163903. (24) Rohrbach, A. Stiffness of optical traps: Quantitative agreement betweenexperiment and electromagnetic theory.

7 Apr 2020: 24). This. 210. a. y. y. x. x. 10 cm. 10 cm.

14 Mar 2014: due to various processes [27, 28], including carrier-carrier and carrier-phonon scattering, as well as radiative electron-hole recombination (non-linear photoluminescence [24, 43, 44]). ... 24] F. Bonaccorso, Z. Sun, T. Hasan, and A. C. Ferrari,

20 Jul 2010: 6% -0.55 220 80 80 1 0.24 60 1.422 639 90.2. ... 24] X. Blase, C. Adessi, D. Connétable, Phys. Rev. Lett. 93, 237004 (2004).

30 Mar 2023: Switching energy <6 nJ 10 pJ 10 pJ 24 nJ. Endurance 4  104 1015 107 106. ... omm. ons License. 2023 Wiley-VCH GmbH2205402 (7 of 24). www.advmat.dewww.advancedsciencenews.com. Adv.

14 Apr 2020: hetero-atoms, such as oxygen [10, 32], hydrogen [26, 30] and nitrogen [24, 33], even though this makes them not mono-atomic. ... In reference [24] we studied the influ-ence of nitrogen implantation on RS in ta-C.

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

28 Nov 2006: 2Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, ChinaReceived 29 July 2003; revised manuscript received 5 September 2003; published 24 December 2003! ... 24. To summarize, RCF gives a downshift and

30 May 2013: The article was first published on May 24, 2013. YES! Send m e a free issue of Scientific Am erican with.