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  2. STu1N.8.pdf CLEO:2014 © 2014 OSA Sub-50 fs compressed pulses ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/STu1N.8.pdf
    10 Jun 2014: 1500 1525 1550 1575 1600 1625. -40. -20. 0. -600 -400 -200 0 200 400 600.
  3. STu1I.2.pdf CLEO:2014 © 2014 OSA Synchronously coupled fiber lasers…

    www-g.eng.cam.ac.uk/nms/publications/pdf/STu1I.2.pdf
    10 Jun 2014: Express 20, 25077 (2012).8. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl.
  4. STh3N.8.pdf CLEO:2014 © 2014 OSA Nanotube mode-locked, low repetition …

    www-g.eng.cam.ac.uk/nms/publications/pdf/STh3N.8.pdf
    10 Jun 2014: Express21, 23261 (2013).10. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl.
  5. High performance bilayer-graphene terahertz detectors Davide…

    www-g.eng.cam.ac.uk/nms/publications/pdf/spirito_APL_2014.pdf
    14 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.
  6. RAPID COMMUNICATIONS PHYSICAL REVIEW B 89, 121402(R) (2014) Effects…

    www-g.eng.cam.ac.uk/nms/publications/pdf/PhysRevB.89.121402.pdf
    6 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
  7. Photodetectors based on graphene, other two-dimensional materials and …

    www-g.eng.cam.ac.uk/nms/publications/pdf/nnano.2014.215.pdf
    6 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
  8. acs_nn_nn-2014-02676g 1..10

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn502676g.pdf
    15 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.
  9. acs_nn_nn-2014-00767b 1..12

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn500767b.pdf
    5 Jun 2014: C.Sub 200 fs Pulse Generation from a Graphene Mode-Locked Fiber Laser.
  10. nl400516a 1..6

    www-g.eng.cam.ac.uk/nms/publications/pdf/nl400516a.pdf
    4 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.
  11. JTu4A.67.pdf CLEO:2014 © 2014 OSA Graphene saturable absorber power…

    www-g.eng.cam.ac.uk/nms/publications/pdf/JTu4A.67.pdf
    10 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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