Search
Search Funnelback University
- Refined by:
- Date: 2013
1 -
27 of
27
search results for KaKaoTalk:vb20 200 |u:www-g.eng.cam.ac.uk
where 0
match all words and 27
match some words.
Results that match 1 of 2 words
-
Times Higher Education - Graphene wins huge European funding boost
www-g.eng.cam.ac.uk/nms/highlights-press/flagship9.pdf28 Jan 2013: nearly 200 research institutes. -
(Cambridge awarded major EPSRC funding for doctoral centres to train…
www-g.eng.cam.ac.uk/nms/highlights-press/cdt4.pdf22 Nov 2013: Avatar — I have over 200 acres of. Leucaena/bermuda grass planted at over. -
Paper2
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Marco%27s%20Publications/Zaccaria_The%20mechanical%20performance%20of%20bi-treated%20glass.pdf25 Oct 2013: Method of strengthening glass by ion exchange and articles therefrom. United States Patent Office No 3,287,200. -
Graphene flagship sets sail | University of Cambridge
www-g.eng.cam.ac.uk/nms/highlights-press/flagship_launch.pdf15 Oct 2013: hard work! Sustainable livestock production is possible. •. Avatar — I have over 200 acres of Leucaena/bermuda grass planted at over 100,000. -
EUROPA - PRESS RELEASES - Press Release - Graphene and Human Brain…
www-g.eng.cam.ac.uk/nms/highlights-press/flagship5.pdf28 Jan 2013: and technology. Each initiative involves researchers from at least 15 EU Member States and nearly 200 research institutes. -
Glass structures_Learning from experts_revised
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20pubblication/Glass%20structures_Learning%20from%20experts.pdf8 May 2013: In case of floors the respondents also mentioned different values from L/200 to L/500; how-ever usually they said that the vibrations should be checked. -
Anti-fraud lasers and inks for transparent electronics | University…
www-g.eng.cam.ac.uk/nms/highlights-press/graphene_inks.pdf6 Nov 2013: Avatar — I have over 200 acres of. Leucaena/bermuda grass planted at over. -
Abstract—Antenna-coupled field effect transistors have been developed …
www-g.eng.cam.ac.uk/nms/publications/pdf/06380288.pdf24 Sep 2013: XYCIRC10 /XYCMAT10 /XYCMBT10 /XYDASH10 /XYEUAT10 /XYEUBT10 /ZapfChancery-MediumItalic /ZapfDingbats /ZapfHumanist601BT-Bold /ZapfHumanist601BT-BoldItalic /ZapfHumanist601BT-Demi /ZapfHumanist601BT-DemiItalic /ZapfHumanist601BT-Italic ... Quality 10 >> -
COST-TU0905_Conferentie_paper_TG06_final
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Caroline%27s%20publications/COST-TU0905_Conferentie_paper_TG06_final.pdf24 Apr 2013: Tensile % JIS K6771 200-250 300-360 190 500 400 415 elongation ______________________________________________________________________________________________________. 2.2.2 Numerical calculation methods. 2.2.2.1 Status Several software packages -
Abstract We report passive mode-locking of an Er-doped fiber ...
www-g.eng.cam.ac.uk/nms/publications/pdf/06600164.pdf24 Sep 2013: Torrisi,T. Hasan, F. Wang, A. C. Ferrari, “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl. -
Evanescent-wave coupled right angled buried waveguide: Applicationsin …
www-g.eng.cam.ac.uk/nms/publications/pdf/14834360.pdf27 Nov 2013: measured using an optical parametric oscillator (Coherent,. Chameleon) delivering 200 fs pulses at 80 MHz repetition. ... Downloaded to IP:. 129.169.173.200 On: Wed, 27 Nov 2013 16:21:32. -
See a sample reprint in PDF f ormat. Order ...
www-g.eng.cam.ac.uk/nms/highlights-press/WSJ2013.pdf28 Aug 2013: CAMBRIDGE, England—A substance 200 times stronger than steel yet as thin as an. -
Ultrafast collinear scattering and carrier multiplication in graphene
www-g.eng.cam.ac.uk/nms/publications/pdf/Brida_Nat2013.pdf17 Jun 2013: t (fs). t (fs. ). 1,050 nm1,350 nm1,500 nm. 0 200 400 600 800 1,000. ... Finally, the sample is cooled rapidly to room temperature undera hydrogen atmosphere at a pressure of 200 mTorr. -
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: Hasan, F. Wang, and A. C. Ferrari, “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl. ... The waveguide is inscribed by focusing the pulses, through a 0.4 NA lens, 200 µm below the substrate surface, by a master oscillator -
OE_29_final.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/Zaugg-2013-OE.pdf14 Dec 2013: z (nm). DBR. -200 0 2000. 1. 2. 3. 4. abs=0.5. ... Ref. ract. ive. inde. x, |E. |2. z (nm). DBR. -200 0 2000. -
Graphene: The quest for supercarbon : Nature News & Comment
www-g.eng.cam.ac.uk/nms/highlights-press/quest_for_supercarbon.pdf22 Nov 2013: hexagons 100 to 200 times faster than it can move through silicon7. -
GetPDFServlet
www-g.eng.cam.ac.uk/nms/publications/pdf/2umlaser.pdf10 Jan 2013: nanotube mode-locked 2 lm solid-state lasers (e.g., 200 fs(Refs. 8, 9, and 52)), but shorter than previous graphene. -
jp400599g 1..13
www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_JPC2013.pdf28 Jun 2013: such as PEG-200 (viscosity, η, 60 mPas; density, ρ, 1.12 g/. ... Figure 7. AuNPs sorted in (a) water/PEG-200 and (b) water/glycerol gradients. -
Optical trapping and manipulation of nanostructures
www-g.eng.cam.ac.uk/nms/publications/pdf/nnano.2013.208.pdf7 Nov 2013: 3. 4. 5. Dis. tanc. e (μ. m). zx. 0 200 400Force (fN). ... a. Displacement (nm)0 200 400 600 800 1,000 1,200 1,400. Dis. -
Measurement of Filling-Factor-Dependent Magnetophonon Resonances in…
www-g.eng.cam.ac.uk/nms/publications/pdf/YKim_PRL2013.pdf30 May 2013: In strained graphene nanobub-bles, it was reported that Bstr can reach 200–400 T [29].In nominally unstrained SLG, the residual strain causedby nm-scale height variations and defects can -
PHYSICAL REVIEW B 87, 205435 (2013) Raman scattering efficiency ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Klar_PRB2013.pdf24 May 2013: II). We find that the Raman scat-tering efficiency of the G peak [dS/d(G)] is 200 105m1 Sr1 at 2.41 eV. ... Eq. (12) we get dS/d(G)SLG 200 105 m1Sr1 anddS/d(G)(2D)SLG 1580 105 m1Sr1. -
PHYSICAL REVIEW B 87, 115413 (2013) Raman spectroscopy of ...
www-g.eng.cam.ac.uk/nms/publications/pdf/physrevb87_115413.pdf14 Mar 2013: In the high-frequency region above 200 cm1, theE12g (384 cm1), A1g (409 cm1), 2LA(M) (453 cm1),. ... Although the in-plane modes in 5 and 6L-MoS2above 200 cm1 are almost identical, the C and LB modepositions below 100 cm1 are different. -
SUPPLEMENTARY INFORMATIONDOI: 10.1038/NNANO.2013.46 NATURE…
www-g.eng.cam.ac.uk/nms/publications/pdf/nnano201346si.pdf4 Apr 2013: 6. 0 50 100 150 200 250 300 3500.0. 0.2. 0.4. ... G). 200. (a) (b) (c). φ φ. Figure S2. Polarization.(a) Geometry for polarized measurements. -
PHYSICAL REVIEW B 88, 035430 (2013) Nonequilibrium dynamics of ...
www-g.eng.cam.ac.uk/nms/publications/pdf/PhysRevB_88_035430.pdf16 Jul 2013: The second stage, t 200 fs, isdominated by the emission of optical phonons,98 which ingraphene are associated with an unusually large energy scale(200 meV)88,99 and are moderately ... which act on a much longer time scale(200 fs). -
Mid-infrared Raman-soliton continuum pumped by a nanotube-mode-locked …
www-g.eng.cam.ac.uk/nms/publications/pdf/oe-21-20-23261.pdf25 Sep 2013: 200 -100 0 100 2000.0. 0.2. 0.4. 0.6. 0.8. 1.0 Data Fit. -
MATTOD0612_cover
www-g.eng.cam.ac.uk/nms/publications/pdf/Bonaccorso_MT_2012.pdf16 Jan 2013: 1b), and the glass substrate is then heated (200 C for 10 – 20 mins)49,50. ... On the C-face, larger domains (200 nm) of multilayered, rotationally disordered graphene are produced198,199. -
Raman spectroscopy as a versatile tool for studying the properties of …
www-g.eng.cam.ac.uk/nms/publications/pdf/nnano201346.pdf4 Apr 2013: NATURE NANOTECHNOLOGY | VOL 8 | APRIL 2013 | www.nature.com/naturenanotechnology 235. Graphene is the two-dimensional building block for sp2 carbon allotropes of every other dimensionality. It can be stacked into three-dimensional graphite, rolled
Search history
Recently clicked results
Recently clicked results
Your click history is empty.
Recent searches
Recent searches
Your search history is empty.