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Measurement of Filling-Factor-Dependent Magnetophonon Resonances in…
www-g.eng.cam.ac.uk/nms/publications/pdf/YKim_PRL2013.pdf30 May 2013: We measure a SLG, grown by chemical vapor depositionon copper [23,24] and transferred onto Si=SiO2 [25], fol-lowing the procedures discussed in the SupplementalMaterial [26]. ... Li et al., Science 324, 1312 (2009).[24] S. Bae et al., Nat. -
1.5 GHz picosecond pulse generation from a monolithic waveguide ...
www-g.eng.cam.ac.uk/nms/publications/pdf/oe-21-7-7943.pdf25 Mar 2013: Opt. Soc. Am. B 14(10), 2716–2722 (1997). 24. J. Mertz, “Nonlinear microscopy: new techniques and applications,” Curr. ... The 2D peak is still single Lorentzian, but 24 cm1 larger than that of the individual flakes. -
acs_nn_nn-2013-03323k 1..13
www-g.eng.cam.ac.uk/nms/publications/pdf/nn403323k.pdf11 Nov 2013: Nanotechnology2013, 24, 265102. 10. Liu, Z.; Tabakman, S. M.; Chen, Z.; Dai, H. -
Graphene: The quest for supercarbon : Nature News & Comment
www-g.eng.cam.ac.uk/nms/highlights-press/quest_for_supercarbon.pdf22 Nov 2013: Ultrashort laser pulses squeezed out of graphene. 24 May 2013. Graphene: The quest for supercarbon : Nature News & Comment http://www.nature.com/news/graphene-the-quest-for-supercarbon-1.14193. -
OE_29_final.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/Zaugg-2013-OE.pdf14 Dec 2013: Mater.21, 3874-3899 (2009). 24. Z. Sun, T. Hasan, F. Torrisi, D. ... Dueto its low-cost fabrication and assembly [16, 23, 24], graphene based saturable absorbers haveemerged as a promising saturable absorber (SA) for ultrafast pulse generation. -
jp400599g 1..13
www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_JPC2013.pdf28 Jun 2013: propertiesare also size dependent,23,24 and, e.g., the superparamagneticiron oxide NPs with the largest magnetic moment are those inthe 1025 nm range,23,24 because the transition fromferromagnetic to ... J. Phys. D: Appl. Phys. 2009, 42, 224002224012.(24) -
SUPPLEMENTARY INFORMATIONDOI: 10.1038/NNANO.2013.46 NATURE…
www-g.eng.cam.ac.uk/nms/publications/pdf/nnano201346si.pdf4 Apr 2013: 56,59, once an-harmonic ef-fects are taken into account21,24,59. -
PHYSICAL REVIEW B 87, 205435 (2013) Raman scattering efficiency ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Klar_PRB2013.pdf24 May 2013: 4Cambridge Graphene Centre, Cambridge University, 9 JJ Thomson Avenue, Cambridge, United Kingdom(Received 14 December 2012; revised manuscript received 5 April 2013; published 24 May 2013). ... Furthermore, its optical and mechanical properties areideal -
Optical trapping and manipulation of nanostructures
www-g.eng.cam.ac.uk/nms/publications/pdf/nnano.2013.208.pdf7 Nov 2013: These play a crucial role in the enhancement of radiation forces and torques in optical twee-zers22–24,26–29. ... to the propagation axis22,24,84. The strength of this aligning torque is increased by tuning the laser close to the plasmon resonance22. -
Ultrafast collinear scattering and carrier multiplication in graphene
www-g.eng.cam.ac.uk/nms/publications/pdf/Brida_Nat2013.pdf17 Jun 2013: Rev.Mod. Phys. 84, 1067–1125 (2012). 24. Bostwick, A. et al. Observation of plasmarons in quasi-freestanding dopedgraphene.
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