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20 Oct 2009: lay. 3.24 63.5ta-C:H 70% 28.4 2.35 70 6 30%ta-C:H 28.4 2.35 43. ... of 3.24 g/cm 3 [11].

27 Jul 2023: In LSMs, theso-called Rytova-Keldysh interaction (RKI) potential [24,25]provides a more accurate interaction between charge carri-ers. ... In Eq. (14) the electrostatic interaction potentialV , known as RKI [24,25,97], is given by [29]:.

27 Nov 2006: The EPCs near K between bands [24] allow theaccurate determination of the intensity and shape of theRaman D peak. ... Jianget al., Chem. Phys. Lett. 392, 383 (2004). [24] For the branch near A01 at K, jg2Kk0q0;Kk0j2 hg2KiF1 cos'00.

14 Sep 2016: the investigation of the carrier dynamics is only at thebeginning.24,29,30. In this work, we assign these features by combining ultrafastTA spectroscopy of exfoliated 1L-MoS2, with selectiveexcitation of ... The irreducible Brillouin zone (IBZ) issampled

20 Sep 2010: Single wall carbon nanotubes SWNTs12–22 andgraphene12,13 are promising saturable absorbers SAs formode-locking fiber,12–17 waveguide,6 solid-state,23 and semi-conductor lasers.24 They have several ... complex processes, such as molecular beam epitaxy

Bidirectional multimode-fiber communication links using dual-purpose vertical-cavity devices", J D Ingham, R V Penty and I H White, IEEE/OSA Journal of Lightwave Technology, Vol 24, pp ... Nonlinear two-moded single-fibre interferometric switch", R V

13 Nov 2006: C2H2 60 nm/s 0.002 cc/Package/24 H 20. CH4 4 nm/s 0.030 cc/Package/24 H 1.3. ... C2H4 25 nm/s 0.012 cc/Pckage/24 H 3.3. a BIF: Barrier Improvement Factor is the ratio of a non-coated bottle to a.

24 May 2013: Dated: May 24, 2013). Graphene is used as the thinnest possible spacer between gold nanoparticles and a gold substrate. ... Such ductile neckingbetween AuNPs is well known[24–26] and supported by ourtheoretical model (not shown) which indicates that

22 Aug 2014: locked pulses has potential applications in nonlinear frequency. conversion [23] and surgery [24]. ... 24 cm-1. larger than in individual flakes [2]. Thus, even if the.

2 Feb 2018: ps) to impulsively generate a strongly out-of-equilibriumdistributions of hot e–h pairs4,8,23,24. ... Phys. Rev. B80, 121403 (2009). 24. Breusing, M. et al. Ultrafast nonequilibrium carrier dynamics in a singlegraphene layer.

1 Mar 2021: emission25 (Supplementary Fig. 24), where ln(I/T2) is linear with E1/2, as for:. ... Science. 356, 69–73 (2017). 24. Shu, J. et al. The intrinsic origin of hysteresis in MoS2 field effect transistors.

5 Jun 2014: 3HT and (b) 24% GNR with P3HT. The insets show the scan at a larger. ... 23 V, for 0%, 11%, and 24% blends. However, itwas slightly higher, ca.

10 Dec 2007: neutrality point away from zero gatevoltage.12–14,19,23,24 However, it is quite remarkable that“pristine” samples, with no contacts, exhibit almost an orderof magnitude doping variation, with a

25 Jan 2021: J. Phys. Condens. Matter 23, 334205 (2011). 24. Ursaki, V. et al.

27 May 2008: eXerox Research Centre of Canada, Mississauga, Ont., Canada L5K 2L1. Available online 24 October 2007. ... Several groups haverecently considered CNTs for fabrication of TFTs, usingvarious fabrication methods, including spin coating, dropcasting, and

22 Jul 2022: The second design features twotop-gates, connected to the left and right arms of a 24 lm radius bow-tie antenna. ... 24 andAl2O3/SLG PDs. We then evaluate correlations among NEP, Sb, andn0 using the Pearson coefficient.

13 Nov 2006: device operation.50 An optimized (pregrowth)catalyst nanostructuring, a lower C2H2 partial pressure,10,24. ... Small 2005, 1, 1180.(24) Lin, M.; YingTan, J. P.; Boothroyd, C.; Loh, K.

23 Mar 2021: multiple SLGs.[17,22] At THz frequencies, however, interband transitions are usually blocked due to the fact that as-prepared SLG is doped,[23,24] hence intraband electronic transi-tions dominate ... Coleman, et al., 2D. Mater. 2020, 7, 022001. [24] K. F

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).

15 Jul 2010: In particular, it was proposed thatfully hydrogenated graphene (graphane) would be stable[24]. ... The main difference between graphene and graphaneis that, while the former is fully sp2 bonded, the latter issp3, as diamond [24].

15 Aug 2022: The samples are placed in a C6S2-anhydrous isopropylalcohol (IPA) mixture with a concentration 1 mmol/L for 24 h. ... 3, 897–900 (2003). 24. Jeong, H. et al. A new approach for high-yield metal - molecule - metaljunctions by direct metal transfer method

15 Oct 2009: The PSD of EW sur-faces can be calculated analytically (24):. bkhkðsÞk2À 0 ej2nk2 sbkhkð0Þk2À þ. ... 2À þ k9k0 bkhk(s)k2À (24) witha cutoff k0 0 2p/2.35 nm.

23 May 2018: Te = 1,000 K. Te = 300 K. THGE. –0.24 eV–0.39 eV–0.42 eV–0.44 eV–0.48 eV. ... 24. Saynatjoki, A. et al. Ultra-strong nonlinear optical processes and trigonal warping in MoS2 layers.

4 Dec 2017: possible to derive the SWNT chirality [24, 25]. Matching the diameter with excitation wavelength in the Kataura plot also gives information on. ... 24] Paillet M, Michel T, Meyer J C, Popov V N, Henrard L, Roth S and Sauvajol J L 2006 Raman active

9 Jun 2021: Graphene-basedoptoelectronic devices are compatible with Si platforms16,24–27.Therefore, graphene-based OEMs could combine telecomoperation and CMOS compatibility. ... 24. Pospischil, A. et al. CMOS-compatible graphene photodetector covering alloptical

16 Dec 2021: coefficient of resistance.24 Single-crystal (SC)CVD SLG, coupled to photonic waveguides, was used forultrafast, zero-dark-current telecom photodetectors (PDs) fordatacoms,25 and wafer-scale integration of electro-absorptionmodulators ... We also evaluate

18 Jun 2021: Sel. Top. Quantum Electron. 24, 1–12 (2018).16. Nagarajan, R. et al. ... Nat. Photonics 7, 883–887 (2013).24. Wang, X., Cheng, Z., Xu, K., Tsang, H.

27 Jan 2021: photoexcitation.16,17 As a result of theseproperties, along with the ability to fabricate TMDs onwafer-scale,3,1820 these have found applications in photo-detectors,2123 photovoltaics,24 ... Progress, Challenges,and Opportunities for 2D Material Based

26 Jun 2008: In order to getaccurate growth rate measurements, we prepattern thecatalyst by e-beam lithography to get free standing verti-cally aligned CNFs [2], rather than rely on weight gainmeasurements [24] or ... B. K. Teo et al., Nano Lett. 4, 921 (2004).[24] L.

28 Mar 2017: 24 M. Yi and Z. G. Shen, J. Mater. Chem. A, 2015, 15, 5330.25 J. ... O’Neill, U. Khan and J. N. Coleman, Chem. Mater., 2012,24, 2414.

25 Sep 2013: 34(8), 695–697 (2004). 24. E. A. Anashkina, A. V. Andrianov, M. ... Express 20(24), 27102–27107 (2012). 25. V. A. Kamynin, A. S. Kurkov, and V.

1 Feb 2009: Y. S. Li, N. R. Tao, K. Lu, Acta Mater. 56, 230 (2008).24. ... state by annealing (we used 450C in Ar atmo-sphere for 24 hours; higher annealing T dam-aged graphene).

15 Aug 2008: Ghislanzoni, 24, 23900 Lecco, Italy 2Engineering Department, Cambridge University, 9 JJ Thompson Avenue, Cambridge CB3 0FA United Kingdom. ... Rev. B 70, 241403 (2004). 24. J. Lefebvre, S. Maruyama, and P.

7 Apr 2020: Carbon Nanomembranes. Advanced Materials 28, 6075–6103, https://doi.org/10.1002/. adma.201506058 (2016). 24. Woszczyna, M.

21 May 2008: Also, a precise control overthe doping concentration and crystallographic direction ofCS-NWs is still lacking,24 while for SOI-NWs these param-eters would be accurately determined by the initial propertiesof ... M. Nano Lett. 2005, 5, 2287.(24) Wu, Y.;

6 Dec 2006: decreases,E0 is measured at lower energies and no longer over a gap defects that could not be measured by ESR [ 24 ]. Robertson [ 25 ] demonstrated that it is possible to fit ... Robertson, Phys. Rev. B 53 (1996 ) 1594. [ 24 ] F.

6 Feb 2023: spectral emission via adaptive opticalpumping.[ 24 ]. Spontaneous mode-locking in RLs was theoreticallypredicted.[ 18,25 ] The complex tunable optical pumping of alaser dye[ 25 ] was exploited to promote the transition of ... Through a combination of

17 Aug 2023: large nonlinear optical response12,22 with a power transmissionmodulation of 50% per monolayer,911,21 ultrafast photo-excitation dynamics and recovery time,22,23 high chemical andmechanical stability,24 large ... EF. The conductivity has the typical

2 Feb 2009: All these parameters arein agreement with a more pronounced graphitic ordering ofthe sample [24]. ... Opt. 23, 3806 (1984)24. J. Robertson: Prog. Solid State Chem. 21, 199 (1991)25.

9 Jun 2021: We perform Raman mea-surements at 785 nm, the available Raman wavelength closest tothat used in HAMR (830 nm25,55), with a spot size 1.24 μm, asdetermined by the razor ... 75 on a 0.24 cm2. area, is investigated using an electrochemical corrosionmethod51

19 Jan 2017: Inte. nsity. (Cou. nts. per. s). (Degrees) (Degrees). (Degrees)19 20 21 22 23 24. ... Rev. Lett. 108, 147001 (2012). 24. Kotov, V. N., Uchoa, B., Pereira, V.

16 Jun 2021: ount. s). 0. 6. 12. 18. 24. x20. x4. x1. Fig. ... Nat. Mater. 13, 247–252 (2013). 24. Byrnes, T. et al. Exciton-polariton condensates.

6 Feb 2014: 4.1 Switch-Pitch Structure with Point Group Symmetry dT. As shown in Figure 3, this switch-pitch structure consists of 16 nodes and 24 members. ... Γ||(e) 24 0 0 0 2. Γf 48 0 0 0 4.

2 Sep 2016: Phys. Rev. B:Condens. Matter Mater. Phys. 2009, 80 (15), 155418.(24) Gillen, R.; Mohr, M.; Maultzsch, J. ... Phys. Rev. Lett. 2000, 85 (24), 52145217.(43) Piscanec, S.; Lazzeri, M.; Mauri, F.; Ferrari, A.

25 Jul 2023: Appl. Phys. Lett. 103, 183112 (2013). 24. Sünner, T. et al.

25 Jul 2023: potential landscape due to spatial variations in layer separationand twist angle.23,24. ... Nat.Phys. 2021, 17, 720725.(24) Andrei, E. Y.; Efetov, D. K.; Jarillo-Herrero, P.; MacDonald, A.H.; Mak, K.

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-.

10 Jan 2013: composite with graphene produced by liquid phase exfolia-. tion of graphite.14,24 Compared to solid-state lasers, fiber.

20 Nov 2006: DFTcalculations are done with the gradient corrected functionalof Ref. [24]. We use plane waves (40 Ry cutoff ) andpseudopotential approaches [25]. ... 24] J. P. Perdew, K. Burke, and M. Ernzerhof, Phys. Rev.

2 Jul 2008: 12 14 16 18 20 22 24. 20. 40. 60. 80.