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  2. Proceedings - copy for website.pub

    www-g.eng.cam.ac.uk/gft/media/Proceedings%20website%20copy.pdf
    15 Oct 2012: vise the op/mal façade in terms of the three design objec/ves. ... large safety factors which oDen rule them out as a possible op/on.
  3. (\24325 million research centre could be the future of manufacturing…

    www-g.eng.cam.ac.uk/nms/highlights-press/cgc2.pdf
    24 Jan 2013: http://www.itv.com/news/update/2013-01-24/25-million-research-centr. 2 of 3 24/01/2013 10:42. Cameron targets tax evaders. Op Elveden: Ex-care worker held.
  4. pnas201217998 3276..3281

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestD.pdf
    6 Feb 2014: between the op-.
  5. http://nanotechweb.org/articles/news/2/12/2

    www-g.eng.cam.ac.uk/nms/highlights-press/nanotechwebscientistsgrowcarbonnanotubes.pdf
    20 Apr 2007: Sign up. ho me ne ws fe a tu res op in io n na n o & s oc ie ty jou rn al h ig h lig hts. ... 20/04/2007http://nanotechweb.org/articles/news/2/12/2. ho me ne ws fe a tu res op in io n na n o & s oc ie ty jou rn
  6. Blade - Vortex Interactions in High Pressure Steam Turbines ...

    www-g.eng.cam.ac.uk/whittle/publications/vspc/VSPC%20thesis%20text.pdf
    8 Nov 2000: Blade - Vortex Interactions in High. Pressure Steam Turbines. by. Venkata Siva Prasad ChaluvadiGirton College. A dissertation submitted for thedegree of Doctor of Philosophy. Department of Engineering November 2000University of Cambridge. i.
  7. Extract from the Proceedings of Building Simulation and Optimization…

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Qian%27s%20publication/loughborough.pdf
    12 Sep 2012: IES using Eq (10):. 15.097 75.466 ( 1 1)OP IES IES     . ... OP, Occupant productivity (%). ACKNOWLEDGEMENT. The authors would like to thank Ms Neesha Gopal.
  8. JThA36 - Widely Tunable Picosecond Fiber Ring Laser Mode-Locked by a…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Wang_CLEO2008.pdf
    22 Aug 2008: 20. Op. tica. l po. wer. (d. Bm. ). Wavelength (nm). ... Op. tica. l po. wer. (d. Bm. ). Wavelength (nm). Pulse width Pu.
  9. When is a symmetric body-hinge structure isostatic? Bernd Schulze∗ ...

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2014GuestC.pdf
    7 Aug 2014: parity reversing) operations, the character of Γ(m) Γ(s) under such op-. ... 7. erations is determined entirely by that of the hinge freedoms for those op-.
  10. 10/18/2016 Single photon light emitting diodes for on­chip…

    www-g.eng.cam.ac.uk/nms/highlights-press/single_photon1.pdf
    18 Oct 2016: 10/18/2016 Single photon light emitting diodes for onchip integration. http://www.nanowerk.com/nanotechnologynews/newsid=44642.php 1/3. HomeNews. Nano DatabasesNano CatalogNano JobsResources. Introduc涐on to Nanotechnology. Open menu.
  11. 10.1117/2.1200705.0711 Carbon nanotubes mode-lock alaser-written…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Della_Valle_SPIE2007.pdf
    15 Jun 2007: We adopted an op-. Figure 1. The writing system for waveguide manufacturing holds thebeam from the laser steady while a translation stage moves the glasssample. ... From 1986 to 1991, he was an associate professor of op-toelectronics at University of
  12. DOI: 10.1478/C1V89S1P030 AAPP | Atti della Accademia Peloritana dei…

    www-g.eng.cam.ac.uk/nms/publications/pdf/2011-AAPP-plasmonic.pdf
    20 Mar 2012: a broad wavelength spectrum, op-erating at high frequencies. ... Graphene’selectronic properties such as high carrier mobility and Fermi velocity allow ultra-fast op-erating speeds[2, 3, 10].
  13. Research NewsEurope pledges one billion euros on graphene as ...

    www-g.eng.cam.ac.uk/nms/highlights-press/flagship28012013.pdf
    28 Jan 2013: Cambridge, which led the original “science & technology roadmap ” of the successful bid for the Grap hene Flagship – will guide on the develop ment of op to-electronic devices based on.
  14. 2 Science Projects to Receive Billion-Euro Award - NYTimes.com

    www-g.eng.cam.ac.uk/nms/highlights-press/flagship7.pdf
    28 Jan 2013: 10. OP-ED CONTRIBUTORConfessions of a Liberal Gun Owner. HOME PAGE TODAY'S PAPER VIDEO MOST POPULAR.
  15. Structural Engineering International 2/2007 Science and Technology…

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/Diagnostic_Interpretation_of_Glass_Failure_DRAFT.pdf
    6 Jul 2011: The stress intensity factor for mode I loading (op ening mode, i.e.
  16. Brownian Motion of GrapheneOnofrio M. Maragó,†,* Francesco…

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn1018126.pdf
    3 May 2011: d) Raman spectrum of an op-tically trapped flake for 633 nm trapping and excitation wavelength. ... cident polarization axis. This is related to the strong op-. tical anisotropy of graphene, resulting in an orienta-.
  17. Few-cycle pulses from a graphene mode-locked all-fiber laser D. ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/1.4922397.pdf
    3 Jul 2015: overall absorption translates to N 30–35. The nonlinear op-tical transmittance is measured with an optical parametric. ... The seed pulse op-. tical spectrum is shown in Fig. 3(a), with a spectral width.
  18. Transform-Limited Photons From a Coherent Tin-Vacancy Spin in Diamond

    www-g.eng.cam.ac.uk/nms/publications/pdf/393.pdf
    7 Apr 2020: d) Op-tically detected magnetic resonance spectra. The frequency of anapplied microwave field is scanned across the transition betweenlevels 1 and 2, leading to a repopulation of level 1 at
  19. Abstract—Antenna-coupled field effect transistors have been developed …

    www-g.eng.cam.ac.uk/nms/publications/pdf/06380288.pdf
    24 Sep 2013: documenten te maken die zijn geoptimaliseerd voor weergave op een beeldscherm, e-mail en internet.
  20. Self‐Induced Mode‐Locking in Electrically Pumped Far‐Infrared Random…

    www-g.eng.cam.ac.uk/nms/publications/pdf/DiGaspare_2023.pdf
    6 Feb 2023: www.advancedsciencenews.com www.advancedscience.com. understanding of the origin and strength of the correlation mech-anism and the related number of cross-correlated interacting op-tical modes is missing. ... The Si/air interface facing the random
  21. 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: ABSTRACT. In the past decade, passively modelocked optically pumped vertical external cavity surface emitting lasers (OP-VECSELs), sometimes referred to as semiconductor disk lasers (OP-SDLs), impressively demonstrated the potential for
  22. Supplementary Note 1 Continuum-model Hamiltonian and cur-rent matrix…

    www-g.eng.cam.ac.uk/nms/publications/pdf/SaynatjokiSI.pdf
    7 Dec 2017: Here, 〈. 〉 denotes the thermal averaging[7, 10], ĵi indicates the second-quantized form of i-th Cartesian component of the paramagnetic current op-erator,.
  23. acs_nn_nn-2011-01203s 1..6

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn201203s.pdf
    5 Oct 2011: Mater. 2007, 6, 841–850. 15. Likharev, K. K. Hybrid CMOS/Nanoelectronic Circuits: Op-portunities and Challenges.
  24. acs_nn_nn-2013-00758r 1..7

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn400758r.pdf
    2 Apr 2013: with distinct electrical, vibrational, and op-tical properties, not necessarily given bysimple superpositions of those of the innerand outer layers.11.
  25. Graphene Reflectarray Metasurface for Terahertz Beam Steering and…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Tamagone2018.pdf
    8 Jun 2018: The op-timized bias line width is 2 µm, so that its inductanceper unit length is sufficient to reduce its effect on thestructure.
  26. Enhanced performance of polymer:fullerene bulk heterojunction solar…

    www-g.eng.cam.ac.uk/nms/publications/pdf/1.4893777.pdf
    6 Aug 2015: Voc. A nitrogen pumped dye laser (k500 nm) is used as op-tical perturbation, resulting in a voltage transient with an am-.
  27. Using JPF1 format

    www-g.eng.cam.ac.uk/nms/publications/pdf/Rodil_JAP2001.pdf
    4 Dec 2006: op--o. --. rg. 1 A. M. Liu and M. L. Cohen, Science24, 841 1989!; Phys.
  28. acs_nn_nn-2014-00767b 1..12

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn500767b.pdf
    5 Jun 2014: or graphene.15,2840 While wide-band op-eration in SWNT-based devices can beachieved using a distribution of tubediameters,15,21,28,41,42 this is an intrinsicproperty of graphene, ... This confirms a stable output pulse.111. CONCLUSIONS. Our demonstration
  29. 1077-260X (c) 2013 IEEE. Translations and content mining are ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/06880814.pdf
    22 Aug 2014: A: Pure and Appl. Op., vol. 11, pp. 013001, 2009. [34] Z.
  30. Ink-jet printing of carbon nanotube thin film transistorsP. Beecher,…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Beecher_JAP2007.pdf
    28 Aug 2007: Ink-jet printing is one of the mostpromising techniques for inexpensive large area fabricationof plastic electronics.2 In fact, a range of electronic and op-toelectronic components can be printed on
  31. Rotation Detection in Light-Driven Nanorotors

    www-g.eng.cam.ac.uk/nms/publications/pdf/Jones_ACSNano2009.pdf
    27 Oct 2009: As the center-of-mass coordinates x, y are uncor-related, the transverse tracking signals cross-correlation shows only the oscillations related to op-tically induced rotations in quadrature with theautocorrelation.
  32. Edge-functionalized and substitutionally doped graphene…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Cervantes-Sodi_PRB2008.pdf
    28 Apr 2008: B. Spin properties. Reference 51 showed, by means of DFT, that applying anelectric field parallel to the ribbon’s plane results in an op-posite local gating of the spin states ... 4c. Weconsider 2NH2-4 N ribbons with two NH2 located in op-posite edges
  33. Nano Res (2010) 3: 404–411 404 Ultrafast Stretched-Pulse Fiber ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_naonres_2010.pdf
    21 Jun 2010: FEFF005500740069006c0069007a007a006100720065002000710075006500730074006500200069006d0070006f007300740061007a0069006f006e00690020007000650072002000630072006500610072006500200064006f00630075006d0065006e00740069002000410064006f00620065002000500044004600
  34. JOURNAL OF APPLIED PHYSICS VOLUME 85, NUMBER 10 15 ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_JAP1999.pdf
    12 Dec 2006: et-ne. ac-op-de-n Si. alan-. ressn-at aen-. Si,. ases. the. sus. an-.
  35. Resonant Raman scattering in cubic and hexagonal boron nitride ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Reich_PRB2005.pdf
    20 Nov 2006: indirect op-tical transitionssX point phonons in cubic BNd, "vd is theenergy of the direct band gap, and"vl the laser energy. ... III. The peak at 2940 cm1 slabeled overb. in Fig. 4d is asso-ciated with the overbending of the in-plane longitudinal
  36. Graphene Mode-Locked Ultrafast LaserZhipei Sun,† Tawfique Hasan,†…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_ACSNANO_2010.pdf
    23 Feb 2010: Op-tical interband excitation in SLG and FLG by an ul-trashort optical pulse produces a nonequilibrium car-rier population in the valence and conduction bands.
  37. Electronic transport characterization of Sc @ C82 single-wall…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Cantone_JAP2008.pdf
    4 Nov 2008: Of importance for applications in op-toelectronics is the bandgap of semiconducting nanotubes,which is usually fixed by, and inversely proportionally to, thenanotube diameter.1 An interesting approach toward modifi-cation
  38. arX iv:1 905. 0463 9v1 [ph ysic s.ap p-ph ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Muench2019.pdf
    14 May 2019: ε0ωt(4). where ε′(ω) and ε′′(ω) are the real and imaginary partof the relative permittivity ε(ω), σ(ω) is the SLG op-tical conductivity, ω is the angular
  39. Uniaxial strain in graphene by Raman spectroscopy: G peak ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Mohiuddin_PRB_2009.pdf
    1 Jun 2009: V. CONCLUSIONS. In summary, we probed with Raman spectroscopy the op-tical phonons of graphene as a function of uniaxial strain.
  40. arX iv:2 305. 0179 1v1 [co nd-m at.m trl- ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/448_Cadore2023.pdf
    16 May 2023: Layered material heterostructures (LMHs) can be used to fabricate electroluminescent devices op-erating in the visible spectral region.
  41. 1.1 Gigahertz Multi-Transistor Graphene Integrated Circuits

    www-g.eng.cam.ac.uk/nms/publications/pdf/06724538.pdf
    4 Feb 2014: Gigahertz Multi-Transistor Graphene Integrated Circuits. Roman Sordan1 and Andrea C. Ferrari2. 1L-NESS, Department of Physics, Politecnico di Milano, Polo di Como, Via Anzani 42, 22100 Como, Italy 2Cambridge Graphene Centre, University of Cambridge,
  42. Photonics with Multiwall CarbonNanotube ArraysElefterios Lidorikis†,* …

    www-g.eng.cam.ac.uk/nms/publications/pdf/Lidorikis_ACSNANO2009.pdf
    1 Jun 2009: we have obtained,that is, the existence of strong Bragg multiple scatter-ing in deep UV frequencies, or strong absorption at op-tical frequencies.
  43. SUPPLEMENTARY INFORMATIONDOI: 10.1038/NNANO.2013.46 NATURE…

    www-g.eng.cam.ac.uk/nms/publications/pdf/nnano201346si.pdf
    4 Apr 2013: Ten-sile strain usually gives phonon softening, and the op-posite for compressive strain.
  44. 2D Materials ACCEPTED MANUSCRIPT • OPEN ACCESS Graphene-Black…

    www-g.eng.cam.ac.uk/nms/publications/pdf/509_Akhavan2023.pdf
    27 Mar 2023: Specifically,transmission in solution can be defined either by the ab-sorbance (Abs=cϵext l as Tr=10cϵextl) or by the op-tical depth as eal[158, 159], where l is
  45. Nano Res. 2011, 4(4): 343–359 343 Photoluminescence of CdSe ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_NanoRes_2011.pdf
    3 May 2011: Nano Res. 2011, 4(4): 343–359. 343. Photoluminescence of CdSe Nanowires Grown With and Without Metal Catalyst. Andrea Fasoli1, Alan Colli2, Faustino Martelli3, Simone Pisana1, Ping Heng Tan4, and Andrea C. Ferrari1 ( ) 1 Department of Engineering,
  46. PHYSICAL REVIEW B 67, 155306 ~2003! Interpretation of infrared ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_PRB2003.pdf
    28 Nov 2006: leonthl fale. -NRdi-c-nd. os-es. e. forr. toig. op-. rfold. ra-im-. e.
  47. Exp Astron (2009) 23:809–847DOI 10.1007/s10686-008-9115-8 O R I G ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Kuppers_EA2008.pdf
    23 Feb 2009: Exp Astron (2009) 23:809–847DOI 10.1007/s10686-008-9115-8. O R I G I N A L A R T I C L E. Triple F—a comet nucleus sample return mission. Michael Küppers H. U. Keller E. Kührt M. F. A’Hearn K. Altwegg R. Bertrand H. Busemann M. T. Capria L.
  48. Optical phonons in carbon nanotubes: Kohn anomalies, Peierls…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Piscanec_PRB2007.pdf
    12 Feb 2007: Covering such diameter rangepushes the limits of computational approaches. SWNTs op-tical phonons were calculated using phonon zonefolding,18,25–27 tight binding28–31 TB, density functionaltheory
  49. Bonaccorso_pages 1..9

    www-g.eng.cam.ac.uk/nms/publications/pdf/Science-2015-Bonaccorso-.pdf
    7 Jan 2015: developed for a wide variety of layeredmaterials. This technique is being optimizedto control the flake size and to increase theedge-to-surface ratio, which is crucial for op-timizing electrode performance
  50. Chapter 9Nanotube and Graphene Polymer Compositesfor Photonics and…

    www-g.eng.cam.ac.uk/nms/publications/pdf/hasan_bookchapter.pdf
    13 Aug 2011: Chapter 9Nanotube and Graphene Polymer Compositesfor Photonics and Optoelectronics. T. Hasan, V. Scardaci, P.H. Tan, F. Bonaccorso, A.G. Rozhin, Z. Sun,and A.C. Ferrari. Abstract Polymer composites are an attractive near-term means to exploit

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