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  2. Deep reactive ion etching as a tool for nanostructure ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Fu_VAC_2009.pdf
    1 Jun 2009: The gap between cathode and anode is 200 m,and the sample area is 0.6 cm2. ... Scale bar: 200 nm. b Representativetransfer curve for the NW device in a.
  3. GPD07 Proceedings p444-467

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Kenneth%20Publications/GPD07-Overend.pdf
    13 Oct 2009: BS62. 62-3. :200. 5. Monolithic Annealed (AN) 8mm 10mm 8mm 10mm 8mm 6mm. ... BS62. 62-3. :200. 5. Monolithic Annealed (AN) 12mm 12mm 10mm 12mm 12mm 8mm.
  4. Small Diameter Membrane Reflector Structures M. Santer∗ Imperial…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009ConfAIAAb.pdf
    9 Mar 2009: 0.5 1 1.5 2 2.5 3 3.50. 100. 200. 300. 400. ... 100. 150. 200. 250. 300. 350. number of sides n. are.
  5. Rotation Detection in Light-Driven Nanorotors

    www-g.eng.cam.ac.uk/nms/publications/pdf/Jones_ACSNano2009.pdf
    27 Oct 2009: The suspensions are then ultrasonically treated ina 200 W, 20 kHz sonicator bath (Nanoruptor, Diagenode) for2 h. ... OF. CA. MB. RID. GE. on. Oct. ober. 27,. 200. 9 | h.
  6. Efficient extracavity second-harmonic generation in the blue using…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_CLEO_2009.pdf
    2 Nov 2009: 11] A. G. Rozhin et al., "Sub-200-fs pulsed erbium-doped fiber laser using a carbon nanotube-polyvinylalcohol mode locker." Appl.
  7. Conceptual Design for a Laminar Flying Wing Aircraft

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009ConfAIAA.pdf
    7 Jul 2009: 100. 150. 200. 250. t/c. Vel. ocity. (m. /s). Span = 60m, 80m, 100m. ... 0 0.2 0.4 0.6 0.8 10. 100. 200. 300. 400. 500.
  8. CTuII3 - Mode-Locked and Single-Longitudinal-Mode Waveguide Lasers…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Osellame_CLEO_2007.pdf
    29 Aug 2009: 0. 20. 40. 60. 80. 100. 0 100 200 300 400 500 600.
  9. ORIGINAL RESEARCH Fabrication, characterization and mode locking…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Wang_JMForm2008.pdf
    1 Oct 2009: and a modulation depth 16.9% (in absorption) at a highpulse fluence 200 μJ/cm2. ... Five milliliter solution is thenmixed with 2 ml of a PVA aqueous solution (200 g/l).
  10. Fabrication of graphene nanoribbons via nanowire lithography

    www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_PSSB2009.pdf
    8 Dec 2009: after O2 etching revealing a GNR (scale bar: 200 nm). ... Scale bars: 200 nm. wide, 400 nm long GNR after consecutive etching steps of10 s (etch1), 15 s (etch2), and 15 s (etch3).
  11. The Ultrasmoothness ofDiamond-like Carbon SurfacesMichael…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Moseler_SCI2005.pdf
    15 Oct 2009: extensive quantum MD simulations. From five. trajectories, each consisting of 200 consecu-. ... of climate models (16–18), both of which. predict that any warming at the surface wouldRemote Sensing Systems, 438 First Street, Suite 200,Santa Rosa, CA
  12. The Preparation, Characterization and Tribological Properties of…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Morrison_PSSA1999.pdf
    15 Oct 2009: This was achieved using an ATI Unicam UV2-200 UV-VIS spectrometer over the 185 to 910 nm wavelength range. ... Similar spec-tra were found for films deposited at ion energies of between 150 and 200 eV.
  13. Dielectrophoretic Assembly of High-Density Arrays of Individual…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Aravind_ACSNano2009.pdf
    28 Jul 2009: ON. SOR. TIA. UK. on. July. 28,. 200. 9Pu. blis. hed. ... on. July. 28,. 200. 9Pu. blis. hed. on J. une. 10, 2.
  14. ELASTIC CONSTANTS OF DIAMOND LIKE CARBON FILMSBY SURFACE BRILLOUIN ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_mrs99.pdf
    20 Oct 2009: Despite the homogeneous schematisation of a probable densitygradient, the values Eit = 750-790 GPa, Gint = 300-395 GPa, Ext = 200-300 GPa, and Gext = 70-150 GPa could be determined. ... Ta-C:H Ta-C ta-csurf WWW-ta-C Diamond. E (GPa) 3004_9 757.547.5
  15. Plasma restructuring of catalysts for chemical vapor deposition of ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Cantoro_JAP2009.pdf
    24 Mar 2009: cooled down to 400 C while NH3 is still flowing, and then exposed to a 50:200 SCCM C2H2 : NH3 gas mixture 0.7 mbar for 40 min. ... the 200–300 nm Ni clusters are polycrystalline. The complexshape can result in more nucleation sites for nanofibergrowth.
  16. ICTON 2007We.A4.4 Waveguide Lasers in Er:Yb-Doped Phosphate…

    www-g.eng.cam.ac.uk/nms/publications/pdf/ValleICTON2007.pdf
    15 Oct 2009: 260 0. 9 C. 0 200 400 600 0 1 2 3 4 5 6 7 8 0 1 2 3 4 5 6 7 i8Incidenlt Pump Powr (m" Frequengy (GHz
  17. STRUCTURAL AND MECHANICAL PROPERTIES OF DIAMOND-LIKE CARBON FILMS…

    www-g.eng.cam.ac.uk/nms/publications/pdf/bonelli_mrs99.pdf
    20 Oct 2009: CONCLUSION. We deposited PLD ta-C films 100-200 inn thick on Si both with and without a SiC interlayer,working in a vacuum of 10-2 Pa.
  18. AMORPHOUS CARBON-SILICON ALLOYS PREPARED BY A HIGHPLASMA DENSITY…

    www-g.eng.cam.ac.uk/nms/publications/pdf/mrs99racine.pdf
    20 Oct 2009: An a-C:H layerwas deposited with a PECVD system, at 200 W and 100mTorr pressure.
  19. doi:10.1016/j.diamond.2005.01.023

    www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_DRM2005.pdf
    15 Oct 2009: c). (a) (b). 8.5. 8.0. 7.5. 7.0100. 200. 200. 300300. 400. ... surface (red atoms), obtained by using a 200 atom supercell of ta-C of bulk.
  20. RAMAN SIGNATURE OF BONDING AND DISORDER IN CARBONS A ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_mrs99raman.pdf
    20 Oct 2009: 200 phonons creates a q=O selection rule. For200 microcrystalline systems with grain size L,.
  21. 5.3 n&v MH IF

    www-g.eng.cam.ac.uk/nms/highlights-press/Fuhrer_Nature_2009.pdf
    24 Apr 2009: e-mails: mfuhrer@umd.edu;adam1@umd.edu. 1. Novoselov, K. S. et al. Nature 438, 197–200 (2005).2.
  22. JOURNAL OF APPLIED PHYSICS VOLUME 90, NUMBER 10 15 ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Chhowalla_JAP2001.pdf
    15 Oct 2009: 90, No. 10, 15 November 2001 Chhowalla et al. ratio of 75:200 sccm at2 600 V and 700 C. ... 1. Standard growth conditionsbias voltage5 2 600V, C2H2 :NH35 75:200, time515 min!
  23. /home/journal/dvi/EPJD013-EPJD-final-print.dvi

    www-g.eng.cam.ac.uk/nms/publications/pdf/Milani_1999_EurPJD.pdf
    2 Feb 2009: Thin films ( 200 nm) show de-fined surface Brillouin peaks, whereas thicker films showa broadening and a disappearance of these peaks, togetherwith the appearance of a strong central peak.
  24. Top-Gated Silicon Nanowire Transistorsin a Single Fabrication…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_ACSNANO2009.pdf
    26 Jun 2009: After synthesis, SiNWs are mechanically transferred21,33. onto a 200 nm thick SiO2 layer thermally grown on top of aheavily doped Si wafer, used as bottom gate.
  25. Subjecting a Graphene Monolayer to Tension and Compression

    www-g.eng.cam.ac.uk/nms/publications/pdf/Tsoukleri_small2009.pdf
    30 Oct 2009: layer of PMMA and a layer of SU8 (200 nm) photoresist of similarYoung’s modulus with thickness t 2.9 mm and widthb 12.0 mm.
  26. Photonics with Multiwall CarbonNanotube ArraysElefterios Lidorikis†,* …

    www-g.eng.cam.ac.uk/nms/publications/pdf/Lidorikis_ACSNANO2009.pdf
    1 Jun 2009: solid graphite film, with thickness chosen to have the. same density per unit cross section, that is, 200 nm. ... Sub-200-fs Pulsed Erbium-DopedFiber Laser Using a Carbon Nanotube-PolyvinylalcoholMode Locker. Appl. Phys.
  27. Raman Spectroscopy of GrapheneEdgesC. Casiraghi,†,⊥ A. Hartschuh,‡ H. …

    www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_NanoLett2009.pdf
    8 Apr 2009: and high carrier mobilities(between 3000 and 200 000 cm2/Vs)5-10 make it a potentialmaterial for nanoelectronics,11-14 especially for high fre-quency applications.
  28. 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: 150. 160. 170. 180. 190. 200. 210. 220. 230. 240250. 260 270 280290.
  29. 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.
  30. Electron-electron interactions and doping dependence of the…

    www-g.eng.cam.ac.uk/nms/publications/pdf/basko_PRB2009.pdf
    20 Oct 2009: is the kink in the electrondispersion, about 200 meV below EF, seen by angle-resolvedphotoemission spectroscopy ARPES.63,80 This is attributedto a correction to the electron energy due to
  31. Nanotube-Polymer Composites for Ultrafast Photonics

    www-g.eng.cam.ac.uk/nms/publications/pdf/hasan_ADVMAT09.pdf
    20 Oct 2009: These include surfactants,[62,106,195,196,241]. water-soluble polymers,[106,195,199,200,241,242] DNA,[63,64,243,244]. polypeptides,[231–233] and cellulose derivatives.[201,234,245]. ... 5.1.2. Polymers. The authors of Ref. [200] first reported the use
  32. USING STANDARD SYSTE

    www-g.eng.cam.ac.uk/nms/publications/pdf/FerrariPRB2000.pdf
    15 Oct 2009: For a density;3 g/cm3 D c is ;200–250 nm. If thesurface layer is thicker thanD c , we would directly see, inthe specular scan, the critical angle corresponding to

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