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28 Feb 2006: Total freshwater (2.5%) = 35,029,000 km3. Available freshwater = 200,000 km3.

5 Oct 2011: SOI areas are removed (Figure 6h).21 The following conditionsare used: main rf power: 400 W; bias power: 50 W; gases cycled:SF6 (250 sccm)/C4F8 (200 sccm)/O2(100 sccm); ... Deposition conditions are asfollows: temperature: 200 C; deposition cycle: 250 ms

20 Apr 2007: A community web site from Institute of Physics PublishingSign in Forgotten your password? Sign up. ho me ne ws fe a tu res op in io n na n o & s oc ie ty jou rn al h ig h lig hts. dire c tory link s ev e nts yo u r ne w s job s co n tac t u s ad v

29 Aug 2009: 0. 20. 40. 60. 80. 100. 0 100 200 300 400 500 600.

15 Feb 2021: We investigate mechanically exfoliated 1L-MoSe2 on a 200-μmfused silica substrate (see Methods for details). ... This is performed with polydimethylsiloxane(PDMS) and, after inspection under an optical microscope, 1L-MoSe2 is drytransferred in ambient

6 Dec 2006: of effusion of hydrocarbon species than in ta-C:H (meth).sure of 104 mbar, flow rates of 2.5 and 5 sccm, andaverage ion energies of 130 and 200 eV

5 May 2005: WBS Task Level. 100 Concept Investigation. 200 Concept Approval D2. 300 Programme Definition. ... 1100 Procure Pre-prod material. 100 Concept Investigation. 200 Concept Approval. 1100 Procure Pre-prod material.

30 May 2012: 1(a). The GNR is 90-nm wide and 800-nmlong, and the inline QD is 200 nm in diameter D. ... c) (d). VBG. VPG(a) (b). FIG. 1. (Color online) (a) Atomic force micrograph of the GNR(W 90, L 800 nm) with an inline QD of diameter D 200

17 Mar 2022: Thus, for simplicity,we set τopt = 200 fs. The dielectric function of SLG is calculated as [110,111]:. ... EF 0,SLG = 0.15 eV, kF,SLG l 50, τe-e = 20 fs, τopt =200 fs, τinj = 30 ps.

8 Dec 2009: after O2 etching revealing a GNR (scale bar: 200 nm). ... Scale bars: 200 nm. wide, 400 nm long GNR after consecutive etching steps of10 s (etch1), 15 s (etch2), and 15 s (etch3).

7 Jan 2021: Figure 4A and B shows the time traces of samples Aand B, recorded at zero gate bias with an oscilloscopehaving a temporal resolution 200 ps. ... The latter signal is then pre-amplified witha voltage pre-amplifier (FEMTO, input impedance 1 MΩ, gain 40

15 Oct 2009: extensive quantum MD simulations. From five. trajectories, each consisting of 200 consecu-. ... of climate models (16–18), both of which. predict that any warming at the surface wouldRemote Sensing Systems, 438 First Street, Suite 200,Santa Rosa, CA

7 Apr 2020: The photophysicalmechanism underlying this enhanced photocatalyticactivity is investigated by ultrafast TA spectroscopy with sub-200 fs time resolution and broad spectral coverage(430–1400 nm). ... We use flakes from Sigma-Aldrich with size 150 μmand

20 Feb 2006: 337. 106. 924. Total freshwater withdrawal. 756. 1397. 1626. 200. 769.

20 Jun 2012: p (kW cm–2). 100 150 200. Figure 3 | Electrically excited microcavity-controlled graphene thermal emitter. ... 200. 300. 0. 0. 1.0. 3. 2. 20. 15. 0.5. 0.

25 Jul 2023: WSeS(Janus). 1.77 to 1.82[200] - - - - - - -. GaSe1.7-2 (from 10 K to 300K)[201, 202]. - - 7 ns as extracted from g2[202] Down to 0.13[201] -Hints ... 12, 6753 (2021). 20. 200. Feuer, M. S. G. et al.

7 Apr 2020: For ρAero-BN0.17 mg cm3 this is 200, whereas it is 3.7 for ρAero-BN0.68 mg cm3. ... Absorption measurements. Absorption measurements are performed using anintegrating sphere (Opsytec) with an inner diameter of 200 mm, coated with areflective BaSO4 thin

21 Jun 2012: Tem. pera. ture. (K). 500. 1000. 1500. 2000. 0 200 400 600.

5 Sep 2008: Concentration (µg ml–1). 1,000 1,200 1,400. γ = E sur – TSsursolsol. ... Distance (Å–1). Inte. nsity. (a.u. )In. tens. ity (a. u.). 200.

24 Sep 2020: b) Dark-field microscopy image of a SLG crystal array with aperiodicity of 200 μm.

11 Dec 2006: Thephysical limitsns0, ns0.5 andBs445 GPa are shown. The contin-uous lines areBs100, 200 and 300 GPa; the dashed lines arens0.1, 0.2, 0.3 and 0.4. ... 200 and 100 GPa.According to the generalE vs.

15 Oct 2009: c). (a) (b). 8.5. 8.0. 7.5. 7.0100. 200. 200. 300300. 400. ... surface (red atoms), obtained by using a 200 atom supercell of ta-C of bulk.

11 May 2018: Finally, the microdisks are undercut with potassiumhydroxide to form an air-clad whispering gallery mode (WGM)resonator.38 The microdisks sit on 200 μm Si Mesa pillars toprevent the tapered fiber ... The microdisk has aradius of 19 μm and sits on a 200

19 Feb 2016: corresponds to 200 kHz),17,18 often not desirable in appli-. cations such as nano-surgery19 or two-photon microscopy,20.

16 May 2023: 200 250 300 350 400 450 1400 1600 2600 2800. 8. ... Zheng, F.Hatami, X. Xu, A. Majmdar, Nano. Lett. 17, 200-205(2017). [26] R.J.P.

20 Oct 2009: 200 phonons creates a q=O selection rule. For200 microcrystalline systems with grain size L,.

6 Dec 2006: 11, 13 March 2000 Chhowalla et al. 6 5% for films deposited below room temperature up'200 C, above which there is a sharp transition from 8to ;0% s p3 bonding

17 Jun 2013: t (fs). t (fs. ). 1,050 nm1,350 nm1,500 nm. 0 200 400 600 800 1,000. ... Finally, the sample is cooled rapidly to room temperature undera hydrogen atmosphere at a pressure of 200 mTorr.

19 Jan 2017: ResultsPCCO characterization and Raman spectroscopy of SLG/PCCO. The PCCO (200-nm-thick) is grown by pulsed laserdeposition on (001) oriented SrTiO3 (STO) (see ‘Methods’) andhas a near-bulk superconducting transition ... The CVD-grown SLG is then

4 Aug 2021: This is seen in Figure  4a, which shows the variability of the currents registered in each conductance state (each box includes 200 data points).

30 Aug 2011: 150. 200. 250. 300. 350. 8. 8. 6 80 2 4 6 80. ... Nature 438, 197–200 (2005). 28. Zhang, Y. B., Tan, Y. W., Stormer, H.

20 Feb 2008: Our final val-ues, corresponding to B, 450 GPa, are Ebulk. 5 750– 790 GPa, Gbulk5 300– 395 GPa, Esurf5 200– 300GPa, andGsurf5 70– 150 GPa.

5 Oct 2011: Rev. A 77,0238 (2008). 20 10 0 10 200. 0.25. 0.5.

2 Jul 2008: 250 300 350 400 450100. 150. 200. 250. E [GPa]. ν = 0.

2 Jul 2008: 100. 200. 300. 400. A ta-C. GT1060 cm-1. 633nm. 514.5nm. 351nm. ... Gilkes et al. [16] This work. 200 300 400 500 600 700 800.

27 Nov 2006: Filmthickness below 2 nm and roughness well below 1 nm are needed for storage density of 200 Gbityinch. ... with respect to S-bend FCVA filmsw43x. This is impor-tant since the process temperature for hard disk deposi-tion is ;200 8C.

10 Jan 2013: nanotube mode-locked 2 lm solid-state lasers (e.g., 200 fs(Refs. 8, 9, and 52)), but shorter than previous graphene.

11 Apr 2016: 1,100 1,500 2,400 2,800 3,200. 1st visible light illumination. 2nd. visible light illumination. ... 5e).In reality, the flakes (with average lateral sizes of 200 nm) formaggregates possessing a poor degree of order.

6 Dec 2006: If sound is fasterprobably has a density gradient. The final values arein the film, the partial localisation is always near theEint=750–790 GPa, Gint=300–395 GPa, Eext=200–surface ... ta-C ta-Csurf WWW-ta-C Diamond. E (GPa) 30049 757.547.5

21 Nov 2018: The buildup of the occupation of the lower CB statewithin the same valley is delayed, but still displays a short timeconstant 200 fs at 77 K. ... These are exfoliatedwith Nitto Denko tape, then further exfoliated on apolydimethylsiloxane (PDMS) stamp for

7 Apr 2020: Hot Electrons Modulation of Third-Harmonic Generation inGrapheneGiancarlo Soavi,,†,‡ Gang Wang,† Habib Rostami, Andrea Tomadin, Osman Balci,† I. Paradisanos,†. Eva A. A. Pogna, Giulio Cerullo, Elefterios Lidorikis, Marco Polini, and Andrea

25 Mar 2013: Hasan, F. Wang, and A. C. Ferrari, “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl. ... The waveguide is inscribed by focusing the pulses, through a 0.4 NA lens, 200 µm below the substrate surface, by a master oscillator

28 Aug 2007: Sonication is carried out in a 200 W, 20 kHz sonication bathBioruptor; Diagenode for 1 h, before intense ultracentrifu-gation for 30 min at 30 000 rpm Beckman, Optima MAX-E. ... Medium integration and a delay of 200 ms areused to ensure that no transient

14 Dec 2013: z (nm). DBR. -200 0 2000. 1. 2. 3. 4. abs=0.5. ... Ref. ract. ive. inde. x, |E. |2. z (nm). DBR. -200 0 2000.

28 Feb 2006: Total freshwater (2.5%) = 35,029,000 km3. Available freshwater = 200,000 km3. ... 1kg bricks 1-2. 1kg steel 5-200. 1kg aluminium 1500. 1kg fertiliser 600.

20 Sep 2010: 320 fs pulse generation from an ultrafast laser inscribed waveguide lasermode-locked by a nanotube saturable absorber. S. J. Beecher,1,a R. R. Thomson,1 N. D. Psaila,1 Z. Sun,2 T. Hasan,2 A. G. Rozhin,2. A. C. Ferrari,2 and A. K. Kar11Department of

5 Sep 2018: Scale bar: 200 µm. 1801599 (3 of 8). www.advancedsciencenews.com. 2018 WILEY-VCH Verlag GmbH & Co.

6 Jan 2011: At alater time (Figure 4b, t 200 ns), a substantial numberof outer layer atoms have moved outside the CNT, cov-ering the head surface. ... METHODSETEM Measurements. We use a modified Tecnai F20 ETEM, oper-. ated at 200 kV, equipped with a differential

4 Nov 2008: water, and 7 dry at 200 Cand store in a nitrogen dry-box. ... 10 100Vgate (V). 200.000.040.080.12. Cond.(e2 /h). semiconducting. 0.2. 0.3. 0.4. -10 100Vgate (V).

21 Dec 2015: The depolarizationdynamics, measured at 77 K, exhibits a peculiar biexponential decay, characterized by two distinct time scalesof 200 fs and 5 ps. ... The faster dynamics is τfast = 200 10 fs while theslower is τslow = 4.8 0.2 ps.