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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. -
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. -
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. -
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. -
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 -
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 -
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. -
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. -
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. -
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.
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