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21 Apr 2010: 2. Fig. S1: Optical absorption spectra of suspensions SWNT#A (a), SWNT#B (b), and SWNT#C. ... gate voltage VG of the. SWNT#A (a), SWNT#B (b), SWNT#C (c), and FLG#D (d) devices.

money on behind the scenes can and cannot rule out today i have a round of breaking twelve years b. ... b. c. world service and further cultural and a. b. c.

31 Jan 2002: Searching for the optimum Root-Goal path. The methods of the previous section found some path between root and goal. A rather harder problem is to find the best path. For this we need to exploit the cost figures in the graph. British Museum. This

19 Jun 2012: an spreadsheet-based tool developed for the project (element B on Figure 4). ... For example, an attribute of the. panel object in the BIM database is the façade type (A, B, B.1 etc.); this corresponds to a façade type.

13 Nov 2006: V.B. Golovko a,⁎, M. Cantoro b, S. Hofmann b, B. Kleinsorge b, J. ... Geng a, D. Jefferson a,A.C. Ferrari b, J. Robertson b, B.F.G.

I have a round of breaking twelve years. B. b. c. ... world service and further cultural and a. b. c. has announced that a major cover up of the american space agency nasa sent men to design postings the mars program and

11 Dec 2006: M.G. Beghi , A.C. Ferrari , C.E. Bottani , A. Libassi , B.K. ... Tanner , K.B.K. Teo , J. Robertsona b, a a c b b.

r. a.'s paramilitary forces. B. b. c. world service. And uh eh.

28 Nov 2006: Bottani , A.C. Ferrari , J. Robertson , P. Milania, a a a b b c. ... 349. w5x A.C. Ferrari, A. Li Bassi, B.K. Tanner, V. Stolojan, J.

13 Nov 2006: K.; Rubloff, G. W.Phys. ReV. B. 1986, 33, 5517.(21) Holstein, W. ... K.; Unlu, M. S.; Goldberg, B. B.; Pimenta, M. A.; Hafner, J.

13 Nov 2006: K. Swan, M. S. Ünlü, B. B. Goldberg, M. A. Pimenta, J. ... Dresselhaus, A. K. Swan, M. S. Ünlü, B. B. Goldberg, andR.

3 May 2011: TM⟩ =1. 8πRe. [n2E′ E′ B′ B′ 1. 2(n2|E′|2 |B′|2)I. ], (3). ... 8πRe. ′[n2(r̂′ E′)E′ r̂′ (r̂′ B′)B′ r̂′]d′ , (5). where E′ = E′I E′S and B. ′ =

16 Sep 2009: W a v e l e n g t h ( μ m ). 2 0. 1 0. 0. SpectralPower(d. B) ( b ). FIG. ... 5. RF spectrum a and pulse train b of the 1200 m laser.

28 May 2008: A.G. Walsh, A.N. Vamivakas, Y. Yin, S.B. Cronin, M.S. Ünlü, B.B. ... 2485Golberg, D. 2551Goldberg, B.B. 2375Goldoni, A. 2238Görnert, P. 2531Granitzer, P. 2517Grecu, M.N.

15 Jul 2010: whichcondensate in the superconducting state [5]) are of char-acter, i.e., derive from bonding combinations of planar Bsp2 hybrids localized around the middle of B—B bonds[10,11]. ... These are significantly affected by the B—B bondlength variation

5 Sep 2007: ReV. B 1998, 58,13870. (5) Charlier, J.-C.; Lambin, Ph.; Ebbesen, T. ... H.; Weisman, R. B.; Smalley, R. E.Science2002,297, 593. (13) Islam, M.

27 May 2008: Hofmann, C. Ducati, B. Kleinsorge, J. Robertson, Appl. Phys. Lett. 83 (2003) 135. ... Swan,. M.S. Unlu, B.B. Goldberg, M.A. Pimenta, J.H. Hafner, C.M. Lieber,.

5 Mar 2014: Lienau, Phys. Rev. B, 72, 241402(R) (2005). 5. S. G. Chou, F. ... Ünlü, B. B. Goldberg, A. K. Swan, S. B. Cronin, Nano Lett.

11 Jul 2011: Figure 1: Schematic drawings of (a) The TCT test. (b) The OCT test. ... C. (b). B. thickness PVB. D. B. A. Line of symmetry yy.

20 Aug 2008: Figure 7. Effective core diameter distribution of as-grown (black),implanted (red) and annealed (green) SiNWs for (a) P-implantationand (b) B-implantation. ... E. Phys. ReV. B 1973, 7, 3685.(29) (a) Li, B. B.; Yu, D.

6 Jul 2011: Kb b b.      =           . ... t. b. b. x. y. Figure 7 Panel with a width of 2b and a hole of radius a under tensile stress.

3 May 2011: For simplicity, Table 1 and Fig. 1(b) only include NBE. Nano Res. ... b b 2DAP G D A 0 DAe / 4πE E E E A Rεε= (1).

7 Apr 2020: Awschalom, R. Hanson, J. Wrachtrup, and B. B. Zhou, Nat. Photonics 12, 516 (2018).[4] W. ... 13] C. Hepp, T. Müller, V. Waselowski, J. N. Becker, B.Pingault, H.

30 Mar 2023: i.e., B in hBN[168] and S in MoS2[170]), without metal penetration. ... a,b) Reproduced with permission.[163] Copyright 2021, Wiley-VCH. 15214095, 2023, 9, Dow.

27 May 2008: visual inspection even after 6 months of incubation. r 2007 Elsevier B.V. ... Yin, M.S. Ünlü, B.B. Goldberg,. A.K. Swan, S.B. Cronin, Nano Lett.

12 Feb 2007: 20 300 M y. OPTICAL PHONONS IN CARBON NANOTUBES: KOHN… PHYSICAL REVIEW B 75, 035427 2007. ... PHYSICAL REVIEW B 75, 035427 2007. 035427-10. with experiments, the data in Fig.

3 Oct 2018: Figure 2a, b shows the schematicand the optical image of the device, respectively. ... and D.D. fabricated andcharacterised the devices; M.B., A.R.-P.M., D.M.K., C.P.-B., B.P.

28 Nov 2006: Robertson , S. Muhla, b b a. Instituto de Investigaciones en Materiales, Universidad Nacional Autonoma de Mexico, Apartado Postal 70-360, Coyoacan D.F. ... Robertson, Phys. Rev. B, submittedfor publication. w24x (a) S.E. Rodil, N.A.

15 Oct 2010: b) Preultracentrifugation. (c) Extractionof the supernatant fractions. (d) Formation of step gradient by placing four layers with decreasing Optiprep concentration on top of each other.37,39. ... a) SDC, (b) TDC, (c) SC, (d) SDBS,(e) Pluronic F98, and (f)

7 Apr 2020: b) Optical image of contact pad short to connect both GPDs in series. ... e)Photovoltage map of device B at the end of the SPP waveguide.

2 Apr 2013: a) SWNT bundle, (b) absorption spectra of SWNTs dispersed in water with sodium docecylbenzenesulfonatesurfactant. ... N.; Yin, Y.;Cronin, S. B.; Unlu, M. S.; Goldberg,B. B.; Swan, A.

27 Nov 2013: TheFIG. 1. (a) Waveguide layout and dicing location. (b) The principle of evan-. ... Swan,. M. S. Unlu, B. B. Goldberg, M. A. Pimenta, J.

4 Dec 2017: Fig. S4(b) plots the spectra in the G region of SWNT-1. ... 36] Jorio A, Souza A G, Dresselhaus G, Dresselhaus M S, Swan A K, Unlu M S, Goldberg B B, Pimenta M A, Hafner J H, Lieber C M and Saito

20 Oct 2009: Polystyrene-block-polyacrilic acid(PS-b-PAA) forms micelles around SWNTs due to the gradualaddition of water. ... Figure 4a and b schematically describeEET from a donor to an acceptor SWNT.

14 Sep 2016: The layout of d-cone fold lines is repeated in Fig. 4(c)with facet labels A to D counterclockwise, and fold rotationsmoving from A to B, B to C, and ... β β. c. d. o,a,b. b. =. FIG. 7. d-cone properties from fundamental units.

19 Feb 2016: sinh. cosh cosh. 2B. F. B B. ( ) ( ). where ò is the characteristic electron energy (of the. order of Fermi energy or temperature). ... strateand b b d2( ),where b is thewidthof the. centralconductorand d is thewidthofthegapbetween.

27 Nov 2006: Gradowski , D. Schneider , H. Hilgersa a, a b b c b. ... 75(1999) 1077. w17x W.P. Acker, B. Yip, Dh. Leach, et al., J.

14 Feb 2014: tion, the other without. Figs 3(a) and 3(b) show that the. ... 3. (a) and (b) Source-drain cur-. rent (ISD) measured as a function of VGin (a) sample A and (b) B, while keep-.

22 Jun 2010: Tensegrity B (b.i and b.ii) for varying valuesof ε = t/AE. ... Pugh, A. (1976). Introduction to Tensegrity. University of California Press.,Berkeley. Roth, B.

5 May 2011: Noise from B: The percentage of dissatisfied of noise level is evaluated by the subjects in Balazova. ... The relationship between PMV and performance in Roelofsen [8] is:. 2 3 4 5 60 1 2 3 4 5 6P b b PMV b PMV b PMV b PMV b

6 Feb 2014: 6b. Hences(b, b) = 12(b2 b2)/6b = 4b = 4c. For counting strands in class III, another useful observation is that for any pairb = kb0 and c = kc0 with k an ... If the vertex count of a prime octahedrite is inflated by a factor(b2 c2), where {b, c} = {b, 0}

6 Feb 2014: also sufficient for GðpÞ to be isostatic: b 2j 3 andfor any non-empty set of bars B; b 6 2j 3 and. ... to be isostatic: b 2j 3 and for any non-emptyset of bars B; b 6 2j 3 and.

5 Jun 2014: b) Second harmonic generation autocorrelation trace of mode-locked pulses at 2 μm. ... N.; Yin, Y.; Unlü, M. S.; Gold-berg, B. B.; Swan, A.

20 Sep 2016: C. ββ. D. BA. 2α. β β. FF. CD. A B0,a,b. ... φA. φA. θA. γ. β β. γ A. A′. B′ B′A′.

21 Sep 2021: We start from the B-LM symmetryproperties to derive a general tensorial expression for theinterlayer force constants. ... To illustrate this, Figure2a and Figure 2b show two fictitious crystals with the same B-.

1 Mar 2021: devices, as in Figure 5a,b, defined by EBL, reactive-ion etchingand thermal evaporation of metallic contacts. ... b) SLG patterning using EBL and RIE. (c) Ni/Au contactsdeposition using evaporation and lift-off.

13 Aug 2011: A.C. Ferrari (B)Department of Engineering, University of Cambridge, Cambridge, CB3 0FA, UKe-mail: acf26@eng.cam.ac.uk. ... Polystyrene-block-polyacrilic acid (PS-b-PAA) formsmicelles around individual SWNTs by gradual addition of water.

11 Nov 2013: Nano Lett. 2012, 12, 1176–1183. 6. Heller, D. A.; Jin, H.; Martinez, B. ... Nat.Nanotechnol. 2009, 4, 114–120. 7. Aili, D.; Gryko, P.; Sepulveda, B.; Dick, J.

3 Feb 2014: The device is therefore proposed for high-displacement, quasi-static applications. 2006 Elsevier B.V. ... δ. Q. ]=[. A B. B C. ][F. V. ], (8).

20 Jun 2017: The electric field in (b–g) is always applied between top and bottom layers. ... b) Typical RS behaviour for the same devices but using optimal testing conditions.