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STu1N.8.pdf CLEO:2014 © 2014 OSA Sub-50 fs compressed pulses ...
www-g.eng.cam.ac.uk/nms/publications/pdf/STu1N.8.pdf10 Jun 2014: 1500 1525 1550 1575 1600 1625. -40. -20. 0. -600 -400 -200 0 200 400 600. -
Numerical analysis of morphing corrugated plates
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009Procedia.pdf3 Feb 2014: 5. 6. 7. θ [rad]. m/D. κ T0. φ = 43o, t = 0.2 mmL = 200 mmL = 300 mmL = 400 mmL = 500 mm. ... Gentilini C. et al./ Physics Engineering 01 (2009) 000–000. 200 250 300 350 400 450 500. -
JTu4A.67.pdf CLEO:2014 © 2014 OSA Graphene saturable absorber power…
www-g.eng.cam.ac.uk/nms/publications/pdf/JTu4A.67.pdf10 Jun 2014: 0.0. 0.2. 0.4. 0.6. 0.8. 1.0. 0 50 100 150 200 250 300 3500. ... Commun. 4, 1987, (2013).7. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl. -
STu1I.2.pdf CLEO:2014 © 2014 OSA Synchronously coupled fiber lasers…
www-g.eng.cam.ac.uk/nms/publications/pdf/STu1I.2.pdf10 Jun 2014: Express 20, 25077 (2012).8. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl. -
doi:10.1098/rspa.2008.0164
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2008GuestA.pdf6 Feb 2014: P. W. Fowler et al.3242. on February 6, 2014rspa.royalsocietypublishing.orgDownloaded from. (Tarnai & Gáspár 1983a) is 5185025.200. ... The edge length is 49833021.200, intermediate between the Kólya–Goldbergand Tarnai–Gáspár arrangements. -
Graphene saturable absorbers for VECSELs V. J. Wittwer*a, C. ...
www-g.eng.cam.ac.uk/nms/publications/pdf/89660X.pdf14 Mar 2014: W- 3XU). -0C. a)> 2ÚNU). cebs 1.3 1. 400 0 -400 -200 0 200 400z(nm). ... 400 -200 0 200z(nm). DBR. 2.0. C0 1.5E4)UCÇ 1.0a). 0.5ü=. I I ' I. -
STh3N.8.pdf CLEO:2014 © 2014 OSA Nanotube mode-locked, low repetition …
www-g.eng.cam.ac.uk/nms/publications/pdf/STh3N.8.pdf10 Jun 2014: Express21, 23261 (2013).10. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl. -
18 April 2012 first published online, doi: 10.1098/rspa.2012.0116468…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2012GuestB.pdf6 Feb 2014: Math. 18, 169–200. (doi:10.4153/CJM-1966-021-8). Kavicky, S. 2004 Anatomy of an exhibition. -
Symmetric prismatic tensegrity structures: Part I. Configuration and…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009GuestD.pdf6 Feb 2014: Higher-Order Rigidity – What Is the Proper Definition. Discrete & Computational Geometry 11, 193–200.Connelly, R., Terrell, M., 1995. -
nl400516a 1..6
www-g.eng.cam.ac.uk/nms/publications/pdf/nl400516a.pdf4 Sep 2014: sweeping both top gates simultaneously at a drain-sourcevoltage VD = 200 mV. ... b) Electrical transfer characteristics of a 1L-MoS2 FET at biasvoltage VD = 200 mV. -
1.1 Gigahertz Multi-Transistor Graphene Integrated Circuits
www-g.eng.cam.ac.uk/nms/publications/pdf/06724538.pdf4 Feb 2014: Bandgap engineering is usually attempted by patterning into graphene nanoribbons (GNRs) (24,11), but GNRs tend to have low mobilities (<200 cm2V1s1) (27) as a consequence of carrier scattering on disordered ... Although these inverters pave the way to -
Graphene modelocked VECSELs C.A. Zaugg1*, V.J. Wittwer2, Z. Sun2, ...
www-g.eng.cam.ac.uk/nms/publications/pdf/896607.pdf14 Mar 2014: organic vapor phase epitaxy (MOVPE, AIXTRON AIX 200/4) as described in [47]. ... The pump laser is coupled into a 200 µm fiber. Fig. -
RAPID COMMUNICATIONS PHYSICAL REVIEW B 89, 121402(R) (2014) Effects…
www-g.eng.cam.ac.uk/nms/publications/pdf/PhysRevB.89.121402.pdf6 Mar 2014: 200 K. 230 K260 K. 1300120011001000. Raman Shift (cm-1. ). 30 T(b) (1,1). ... Vunit. l3B. 2B. γ 21. 2v. V1B 4.1 106 cm1. This value leads to W (kz) 104 cm1 at 30 T and 200 K,too small to explain the observed -
High performance bilayer-graphene terahertz detectors Davide…
www-g.eng.cam.ac.uk/nms/publications/pdf/spirito_APL_2014.pdf14 Feb 2014: High performance bilayer-graphene terahertz detectors. Davide Spirito,1 Dominique Coquillat,2 Sergio L. De Bonis,1 Antonio Lombardo,3. Matteo Bruna,3 Andrea C. Ferrari,3 Vittorio Pellegrini,1,4 Alessandro Tredicucci,1. Wojciech Knap,2 and Miriam S. -
doi:
www-g.eng.cam.ac.uk/nms/publications/pdf/c4nr00256c.pdf5 Jun 2014: 7b. These aggregates having a height rangingfrom 60 to 200 nm and a width spanning from 0.6 to 2 mm, werefound to be randomly distributed within the polymer matrix.Their ... Experimental sectionMaterials. Poly(3-hexylthiophene) (P3HT) (Fig. 1b) -
1077-260X (c) 2013 IEEE. Translations and content mining are ...
www-g.eng.cam.ac.uk/nms/publications/pdf/06880814.pdf22 Aug 2014: Hasan, F. Wang, and A. C. Ferrari, "Sub 200 fs pulse generation from a graphene mode-locked fiber. -
acs_nn_nn-2014-00767b 1..12
www-g.eng.cam.ac.uk/nms/publications/pdf/nn500767b.pdf5 Jun 2014: C.Sub 200 fs Pulse Generation from a Graphene Mode-Locked Fiber Laser. -
Luminsescence: The Instrumental Key to the Future of Nanotechnology
www-g.eng.cam.ac.uk/nms/publications/pdf/Acf_Ch06_2014.pdf5 Mar 2014: In the 1,200–1,350 nm emission range, exciton-exciton resonances of SWNTs such as (13,2), (12,4), (10,5), (9,7), (10,6), (8,7), (11,4), ... 6.4a) with respect to other tubes. The strong PL emission in the 1,080–1,200 nm range. -
acs_nn_nn-2014-02676g 1..10
www-g.eng.cam.ac.uk/nms/publications/pdf/nn502676g.pdf15 Jul 2014: BRUNA ET AL. VOL. XXX ’ NO. XX ’ 000–000 ’ XXXX. www.acsnano.org. A. C XXXX American Chemical Society. Doping Dependence of the RamanSpectrum of Defected GrapheneMatteo Bruna, Anna K. Ott, Mari Ijäs, Duhee Yoon, Ugo Sassi, and Andrea C. -
Photodetectors based on graphene, other two-dimensional materials and …
www-g.eng.cam.ac.uk/nms/publications/pdf/nnano.2014.215.pdf6 Oct 2014: Because the optical phonon energy in graphene is large45,46 (200 meV), hot carriers created by the radiation field can remain at a tempera-ture Te (and thus energy kBTe, with ... 100. –200. –300. –400. –500. Phot. ocur. rent. (nA. ). Gate
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