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  2. Proc. R. Soc. A (2010) 466, 63–77doi:10.1098/rspa.2009.0370 Published …

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2010GuestC.pdf
    6 Feb 2014: New York, NY: McGraw-Hill Book. Company Inc.Fowler, P. W. & Guest, S.
  3. Anomalous low-temperature Coulomb drag in graphene-GaAs…

    www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms6824.pdf
    23 Dec 2014: Our observations establish a new class of vertical hetero-structure devices with a potentially large flexibility in the designof band dispersions, doping and e–h coupling, where excitonicphenomena are accessible. ... Feasibility of superfluidity of
  4. Symmetric prismatic tensegrity structures: Part I. Configuration and…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009GuestD.pdf
    6 Feb 2014: By ‘stretched’ wedo not mean the tensegrity itself has been deformed, rather we mean a new tensegrity where the coordinates of the nodesare given by an affine transformation of the coordinates ... Publishers, Dordrecht, pp. 47–54.Coxeter, H.S.M.,
  5. 1077-260X (c) 2013 IEEE. Translations and content mining are ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/06880814.pdf
    22 Aug 2014: wavelength is opening new application avenues, such as. pumps for mid-infrared frequency combs [29]. ... development of new telecommunication components and advanced optical test. systems. In 2009 he returned to Heriot-Watt and led the technical
  6. March 2012, published 19, doi: 10.1098/rsta.2011.0347370 2012 Phil.…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2012PTRSL.pdf
    3 Feb 2014: Correspondingly, one of the corners of the sheet, P, movesto a new point, P′, with coordinates (x, y, z) such that. ... Sci. News 164,359. (doi:10.2307/4018925). 3 Demaine, E. D., Demaine, M. L. &
  7. Designing Folding Rings using PolynomialContinuation Andrew D.…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestE.pdf
    7 Aug 2014: ζ1. ζ21 4ζ0ζ22ζ2. =ξ1. ξ21 4ξ0ξ2. 2ξ2(7). At this stage, introduce the new unknowns:. ... Γ2 = ζ21 4ζ0ζ22 = ξ21 4ξ0ξ2. If these new variables are substituted into Equation 7, thenthe compatibility equation system can be written as:.
  8. 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: 2National High Magnetic Field Laboratory, Tallahassee, Florida 32310, USA3Department of Materials and Metallurgical Engineering, New Mexico Tech, Socorro, New Mexico 87801, USA. ... Kluwer. Academic/Plenum, New York, 2000).[6] D. C. Tsui, H. L. Stormer,
  9. Graphene modelocked VECSELs C.A. Zaugg1*, V.J. Wittwer2, Z. Sun2, ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/896607.pdf
    14 Mar 2014: 1(f). The pulse repetition rate is 2.5 GHz, detected with a fast photodiode (New Focus 1434) and measured with a microwave spectrum analyzer (MSA, HP 70952), see Fig.
  10. When is a symmetric body-hinge structure isostatic? Bernd Schulze∗ ...

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestC.pdf
    7 Aug 2014: circuit-gluing to obtain new structures (Ross and Nixon, 2012). Note that the wheel graphs Wn shown in Figure 9 (ii) correspond to body-. ... Sons, New York. Fowler, P., Guest, S., and Schulze, B.
  11. acs_nn_nn-2014-00767b 1..12

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn500767b.pdf
    5 Jun 2014: Ultra-fast FibreLaser Systems Based on SESAM Technology: New Hori-zons and Applications. ... C. In Molecular- and Nano-Tubes;Hayden, O., Nielsch, K., Eds.; Springer: New York, 2011.
  12. acs_nn_nn-2014-02676g 1..10

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn502676g.pdf
    15 Jul 2014: New J. Phys.2009, 11, 095011. 27. Bonaccorso, F.; Lombardo, A.; Hasan, T.; Sun, Z.; Colombo,L.; Ferrari, A.
  13. When is a symmetric body-bar structure isostatic?

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2010GuestA.pdf
    6 Feb 2014: Eds.), New Approachesto Structural Mechanics, Shells and Biological Structures. Kluwer, pp.
  14. 1.1 Gigahertz Multi-Transistor Graphene Integrated Circuits

    www-g.eng.cam.ac.uk/nms/publications/pdf/06724538.pdf
    4 Feb 2014: Radical new device concepts, like ballistic or vertically stacked devices, will need to be developed and their potential investigated. ... 19) S. M. Sze, Physics of Semiconductor Devices. New York: Wiley-Interscience, 1981.
  15. Resonant Raman spectroscopy of twisted multilayer graphene

    www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms6309.pdf
    10 Nov 2014: C peaks) due to resonance with new optically allowed electronic transitions, determined by. ... A 104, 749–773 (1924).2. Lipson, H. & Stokes, A. A new structure of carbon.
  16. Luminsescence: The Instrumental Key to the Future of Nanotechnology

    www-g.eng.cam.ac.uk/nms/publications/pdf/Acf_Ch06_2014.pdf
    5 Mar 2014: This is a new type of EET feature, resulting from resonant excitation of ehii K (i = 1, 2, 3,. ) ... F. Bohren, D. R. Huffman, Absorption and Scattering of Light by Small Particles, New York: Wiley-Interscience, 1998.
  17. doi:

    www-g.eng.cam.ac.uk/nms/publications/pdf/c4nr00256c.pdf
    5 Jun 2014: photoresponse. Therefore, our strategy offers a new method towards the enhancement of the. ... Introduction. Over the past few years, a great effort has been devoted to thedevelopment of new organic semiconducting materials,combining solution
  18. 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: Watson Research Center, Yorktown Heights, New York 10598, USA, 4Cambridge Graphene Centre, 9 JJ Thomson Avenue, Cambridge CB3 0FA, UK, 5NEST, Istituto Nanoscienze-CNR and Scuola Normale Superiore, I-56126 Pisa,

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