Search

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

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

2 Oct 2008: Received 2 May 2008, revised 24 June 2008, accepted 25 June 2008Published online 29 August 2008. ... Such wavelength tuning in passivelymode-locked fiber ring lasers was observed before in non-nanotube systems, and is usually attributed to

17 Jul 2008: Delivered by Ingenta to:Dublin City University. IP : 136.206.1.20Thu, 17 Jul 2008 13:44:24. ... IP : 136.206.1.20Thu, 17 Jul 2008 13:44:24. RESEARCHARTICLE. King et al.

20 Jun 2017: ARTICLE. Received 24 Jan 2017 | Accepted 24 Feb 2017 | Published 22 May 2017. ... active role in producing QEs, as well as determining their specificoptical properties21,23,24.

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

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.

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

6 Mar 2019: Here, we use solution proc-. essed CNTs to fabricate the SAs.24 0.03 wt. %

9 Jun 2021: Au/WS2/P ZT/Au 24.3 3.5 0 µA / 0 µW 0.15 µA / 0.53 µW 10 S36.

7 Apr 2011: 3] S.V. Chernikov et al., “Raman fibre laser operating at 1.24 µm.” Electronics Letters 34, 680 (1998).

21 Nov 2005: 4.3625304774. 166.4. Small hydro. 0.6344545526. 24.2. Geothermal etc. 0.673780248. 25.7. Total.

4 Dec 2012: Phys. Lett. 95 111108. [24] Özgören K and Ilday F Ö 2010 Opt.

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.

27 Mar 2007: For example, Erlandsson et al. [24,25] reportedsignificant restructuring of 0.5 nm thick Pd films (meltingand Huetting temperatures of 1554 and 275 1C, respec-tively) at 200 1C when subject ... 24] R. Erlandsson, M. Eriksson, L. Olsson, U. Helmersson, I.

21 Jun 2007: The sample absorbed in the UV–Vis range.Absorption shoulders occurred close to the direct band-gap energies of crystalline silicon [24,25]. ... 24] J. Singleton, Band Theory and Electronic Properties of Solids, OxfordUniversity Press, 2001, p.

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

26 Apr 2021: Chem. Soc. Rev. 44, 7715–7736 (2015). 24. Sim, D. M. et al. ... 24, 6524–6531 (2014). 41. Li, S.-L., Tsukagoshi, K., Orgiu, E. & Samorì, P.

21 Aug 2014: 24, pp. 3025–3027,2008. [3] S. Kobtsev, S. Kukarin, and Y. Fedotov, “Ultra-low repetition ratemode-locked fiber laser with high-energy pulses,” Opt. ... Mater., vol. 20, no. 21, pp. 4040–4043, 2008. [24] T. Hasan et al., “Nanotube–polymer

15 Aug 2022: rent. (nA. )a. 5.8 µm2. -0.26 -0.24 -0.22 -0.2 -0.18 -0.16-2.5. ... Nano Lett. 10, 615–619(2010). [24] Zhang, X. A. et al. Single electron transistor with pro-grammable tunnelling structure.

27 May 2016: utm_content=http%3A%2F%2Fcdn.taboolasyndication.com%2Flibtrc%2Fstatic%2Fthumbnails%2F49c78451966618d4d8ede4fde3bca136.jpg&utm_term=ThisServicein+%24%7Bcity%3Acapitalized%7D%24isChangingtheWayPeopleCookatHome). HelloFresh. ... source=taboola&utm_medium=cpc

7 Apr 2011: Large Energy Pulse Generation Modulated by Graphene Epitaxially Grown on Silicon Carbide", ACS Nano, DOI: 10.1021/nn102280m (2010) [24] Y.

4 Sep 2014: 24,12 While bulkMoS2 is a semiconductor with an indirect band gap of 1.3 eV,. ... E.; Heinz, T. F.; Hone, J.; Ryu, S. ACSNano 2010, 4 (5), 26952700.(24) Zhang, X.; Han, W.

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).

14 Dec 2006: The sp3 content of the films isestimated at 10% from X-ray photoemission and electron energy loss spectroscopy [19, 24]. ... P., Phys. Rev. B, 35 (1987) 2946. [24] Li Bassi A., Piseri P., Milani P., Ferrari A.

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.

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.

27 May 2008: Previous studies showed that SWNTs tend todeposit in areas covered with polar chemicals when thewafer is dipped in a SWNT solution [23,24]. ... Lett. 303 (1999) 125. [24] S.G. Rao, L. Huang, W. Setyawan, S.

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

27 Nov 2013: Received 24 September 2013; accepted 13 November 2013; published online 27 November 2013). ... tion rates.28 CNTs and graphene SAs for evanescent field. interaction have either been sprayed23,24 or embedded into.

16 Aug 2023: 1c) shows Pos(LBM4,3) = 24.24 0.06 cm1 and Pos(CN,1) =31.36 0.06 cm1, corresponding to N = 4. ... Electroluminescence in Single Layer MoS2.Nano Lett. 2013, 13 (4), 14161421.(24) Palacios-Berraquero, C.; Barbone, M.; Kara, D.

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 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.

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

6 Dec 2006: Thepresence of a RamanD peak at;1350 cm21 indicates thatthe s p2 phase is clustering into aromatic rings.18 There is arelationship23,24 between the in-plane correlation lengthL a ofthe ... 2.24 I (D)/I (G) is derived from the Raman spectra

10 Dec 2007: In general, lat-tice dynamics is calculated within the Born-Oppenheimeradiabatic framework [24, 25]. ... M. Ziman, Principles of the theory of solids (Cam-. bridge University Press, London, New York, 1964).[24] M.

4 Sep 2008: 2z〈Z(t)Z(t τ )〉 (24). where we assume center-of-mass and angular uctuations to be uncorrelated,so that we can neglect cross terms of type ... Using Eqs.22-24 we are able to t well our experimental data (seeFig.

22 Jan 2013: Holmium for the holidays. Mon Dec 10 14:24:00 CST 2012 - Photon Focus.

4 Aug 2021: Second, GO can be prepared inexpensively via LPE. Spray-coating allows conformal coverage surfaces with complex shapes.[24] This approach is very attrac-tive from an industrial point of view. ... Park, M.-J. Park, J.-S. Lee, Adv. Funct. Mater. 2018, 28,

27 May 2008: Inaddition to dielectric screening [24,25], the presence ofbundles [20,21] contributes to the red shift in theabsorption spectrum compared to sample C1. ... Werecently reported that addition of PVP in a freshlyprepared SWNT dispersion increases the PL

28 Nov 2006: 1 10 10010. 100. β/α =0.24. Cor. rela. tion. leng. ht(n. ... D. Lempert, and E. Grossman, Phys. Rev.Lett. 72, 2753 (1994). [24] R.

15 Oct 2009: Recently,a a. Ferrari and Robertson 24 have shown from their workŽ. ... Lett. 76. Ž. Ž. 18 2000 2627. Ž. 24 A.C. Ferrari, J.

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.

21 Jan 2008: on functionalized substrates;22,24 and c they canbe made of the same material of the final NWs, thus, mini-mizing chemical contaminations.20. ... Although nanocrystal-seeded growth has proven viablefor NWs synthesis,10,20,21,24 many fundamental

27 May 2008: References. [1] A. Ashkin, Phys. Rev. Lett. 24 (1970) 156. [2] A. ... Gittes, C.F. Schmidt, Opt. Lett. 23 (1998) 7. [24] A. Rohrbach, Phys.

7 Jan 2021: This would allow THzQCL FCSs to be fully stabilized against primary frequencystandards.24. ... a multiheterodyne detectionscheme, in which the QCL-comb was mixed with a fullystabilized optically rectified THz-frequency comb.24.

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.

19 Feb 2016: air-hole spacing,23 thus offering possibilities for both nonli-. nearity and dispersion management in fiber lasers.24,25. ... persion management,15 nonlinearity management is alsoa)Electronic mail: dp387@cam.ac.uk. 0003-6951/2015/107(24)/241107/4/$30.00

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: KEYWORDS: Graphene, photodetectors, photothermoelectric effect, integrated photonics, plasmonics. The ever-growing demand for global data traffic1 is drivingthe development of next-generation communicationstandards.24 The increasing numbers of