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nnano.2006.158_149 RH_TDBU.indd
www-g.eng.cam.ac.uk/nms/highlights-press/Nanotechnologygraphene.pdf10 Apr 2007: Although silicon is the conventional hardware on. nnano.2006.158_149 RH_TDBU.indd 160nnano.2006.158_149 RH_TDBU.indd 160 24/11/06 17:12:5024/11/06 ... If citing these articles, please refer to the web version. nnano.2006.158_149 RH_TDBU.indd Sec1:161nnano -
Near‐ and Far‐Field Observation of Phonon Polaritons in Wafer Scale…
www-g.eng.cam.ac.uk/nms/publications/pdf/Calandrini_2023.pdf25 Jul 2023: e,f) Near-field phase images 𝜑3(𝑥, 𝑦) of the 24 and 13 nm. ... layer thickness of 13 nm, where q = 12.6 and vg = 3.24 10-3 c. -
Charge-tuneable biexciton complexes in monolayer WSe2
www-g.eng.cam.ac.uk/nms/publications/pdf/Barbone2018.pdf3 Oct 2018: 24 observed a peak in 1L-molybdenumdiselenide (MoSe2) in the expected energy range, which theylabelled as the neutral biexciton. ... Graphite. hBN. WSe2. 1.728. 1.699. 1.6921.685. 1.679. 1.711. = 1. = 24 K. -
doi:10.1016/j.msec.2003.09.084
www-g.eng.cam.ac.uk/nms/publications/pdf/Piscanec_MSEC2003.pdf28 Nov 2006: 23,24]. Furthermore, electronic Raman scattering introdu-. ces an extra dependence of the lineshape with the excitation. ... 24] N.H. Nickel, P. Lengsfeld, I. Sieber, Phys. Rev., B 61 (2000) 15558. -
nn0c02738 1..15
www-g.eng.cam.ac.uk/nms/publications/pdf/403.pdf24 Sep 2020: with feature sizes <100 nm.15,24,25 Dynamic character-ization is performed up to 67 GHz, showing a flat electro-opticalfrequency response without roll-off. ... 1 42 GHz(RI = 0.36 A W. 1 at 1.2 V bias)24 PTE none CVD RV = 12 V W. -
Conversionless efficient and broadband laser light diffusers for high …
www-g.eng.cam.ac.uk/nms/publications/pdf/396.pdf7 Apr 2020: 24). This. 210. a. y. y. x. x. 10 cm. 10 cm. -
42414.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/Bottani_EPL1998.pdf8 Dec 2006: Our results differ considerably from those reported in [24]. c. e. ... 24] Pailard V., Melinon P., Perez J. P., Dupuis V., Perez A., Loubet J. -
http://www.nanotechwire.com/news.asp?nid=3608&ntid=&pg=41
www-g.eng.cam.ac.uk/nms/highlights-press/nanotechwirenewmethodofgrowingcnt.pdf20 Apr 2007: 8/10/2006 12:24:38 AM. New method of growing carbon nanotubes. to revolutionise electronics. -
Spider silk reinforced by graphene or carbon nanotubes
www-g.eng.cam.ac.uk/nms/publications/pdf/Lepore.pdf22 Aug 2017: 11 0.51 0.05 111 24.3 13.5 0.75 0.29 1969.1 1158.8 764.7 640.5. ... Mater. 24 1482–6. [7] Foelix R F 2011 Biology of Spiders (Oxford: Oxford University Press). -
1.4942778
www-g.eng.cam.ac.uk/nms/publications/pdf/1.4942778.pdf21 Mar 2016: tunnel barrier is centrosymmetric.24 For example, TAMR 3%was recorded25 at 4.2K for an interface between an organic. ... Ballestar, F. Bern, W. Bohlmann, and P. Esquinazi, Nanotechnology 24, 015703 (2013).21S. -
acs_nn_nn-2011-01203s 1..6
www-g.eng.cam.ac.uk/nms/publications/pdf/nn201203s.pdf5 Oct 2011: high-κ gate dielectrics. Electrically active NWshave also been used to gate graphene FETswhile acting at the same time as evaporationmasks to yield channel lengths down to130 nm.24 In all ... 24. Liao, L.; Lin, Y. C.; Bao, M.; Cheng, R.; Bai, J.; Liu, Y. -
Tetrahedral amorphous carbon resistive memories with graphene-based…
www-g.eng.cam.ac.uk/nms/publications/pdf/Ott2018.pdf14 Apr 2020: hetero-atoms, such as oxygen [10, 32], hydrogen [26, 30] and nitrogen [24, 33], even though this makes them not mono-atomic. ... In reference [24] we studied the influ-ence of nitrogen implantation on RS in ta-C. -
RAMAN SIGNATURE OF BONDING AND DISORDER IN CARBONS A ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_mrs99raman.pdf20 Oct 2009: 8. This isvalidated by NMR and EELS data where available [24], as shown in the Figure. ... 1990)23. J. Robertson, Phys Rev B 53, 16302 (1996)24. M. A. -
Graphene modelocked VECSELs C.A. Zaugg1*, V.J. Wittwer2, Z. Sun2, ...
www-g.eng.cam.ac.uk/nms/publications/pdf/896607.pdf14 Mar 2014: due to various processes [27, 28], including carrier-carrier and carrier-phonon scattering, as well as radiative electron-hole recombination (non-linear photoluminescence [24, 43, 44]). ... 24] F. Bonaccorso, Z. Sun, T. Hasan, and A. C. Ferrari, -
nl4018463 1..6
www-g.eng.cam.ac.uk/nms/publications/pdf/nl4018463.pdf15 Nov 2013: PGAP) in a form of plasmonhybridization closely analogous to ferromagnetic and anti-ferromagnetic dipolar coupling.24 While the P mode is dipolar-like, the P+ mode is more quadrupolar due to ... Gold Nanoparticles on Polarizable Surfaces as -
LETTERS Breakdown of the adiabaticBorn–Oppenheimer approximationin…
www-g.eng.cam.ac.uk/nms/publications/pdf/Pisana_NM2007.pdf2 Mar 2007: Thedependence of the electronic bands on u can be obtained from theDFT electron–phonon coupling matrix elements (see equation (6)and note 24 of ref. ... Phys. Rev. Lett. 96,. 136806 (2006).24. Moos, G., Gahl, C., Fasel, R., Wolf, M. & -
INSTITUTE OF PHYSICS PUBLISHING NANOTECHNOLOGY Nanotechnology 16…
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NT2005.pdf23 Nov 2006: Rev. Mater. Res.24 83. [2] Duan X, Huang Y, Agarwal R and Lieber C M 2003 Nature421 241. -
Using APL format
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_APL1999.pdf20 Feb 2008: density of 3.24 g/cm3.15 The dispersionrelations depend on the elastic constants of both the olayer (E,G) surf and the inner layer (E,G) bulk. ... Knapp and co-workers3,24 proposed a finite-element modelovercome the limitations of the Oliver–Pharr1,2 -
Quantum Control of the Tin-Vacancy Spin Qubit in Diamond
www-g.eng.cam.ac.uk/nms/publications/pdf/2021Debroux.pdf16 Dec 2021: Box 5046, 2600 GA Delft, Netherlands. (Received 24 May 2021; accepted 16 September 2021; published 30 November 2021). ... state host for scalable fabrication of quantum light-matterinterfaces [23], enabling all-optical control [24–27]. -
Supplementary Note 1 Continuum-model Hamiltonian and cur-rent matrix…
www-g.eng.cam.ac.uk/nms/publications/pdf/SaynatjokiSI.pdf7 Dec 2017: i1,i2,.,in. Π(n)i1i2.in. (ωΣ; ω1,ω2,. ,ωn)Ai1 (ω1)Ai2 (ω2). Ain (ωn) ,. (24)where A(ωi) = iE(ωi)/(ωi iη/) and η is an infinitesimal positive ... Phys.:Condens. Matter 24, 205802 (2012). [13] Rostami, H. & Polini, M. -
phb76194d_598
www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_PSSB2007.pdf28 Nov 2007: Nanoruptor ultrasonicator) in presence of sodium dodecylbenzenesulphonate (SDBS) as surfactant [24]. ... 24] M. F. Islam, E. Rojas, D. M. Bergey, A. T. -
doi:10.1016/j.physe.2007.10.024
www-g.eng.cam.ac.uk/nms/publications/pdf/Mattevi_PE2007.pdf27 May 2008: re-organization of the C atoms in a sp2 network (284.5 eV,CNT growth) [21,24]. ... 24] J.C. Lascovich, R. Giorgi, S. Scaglione, Appl. Surf. Sci. 47 (1991) 17. -
Carbon Nanotube Polycarbonate Composites for Ultrafast Lasers
www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_AM2008.pdf5 Nov 2008: Published online: September 24, 2008. [1] Y.-C. Chen, N. R. Raravikar, L. ... Appl. Phys. A 2003, 76, 111. [24] S. Singh, Y. Pei, R. -
Electrically Controlled Nano and Micro Actuation in Memristive…
www-g.eng.cam.ac.uk/nms/publications/pdf/Kos2018.pdf5 Sep 2018: mechanical deformations in the underlying structure),[21] and impermeability to gases.[21] Raman spectroscopy is used to monitor the presence of defects,[22] doping,[23,24] and strain[25–28] (see ... KGaA, Weinheim. www.small-journal.com. Small 2018, 14 -
Graphene field-effect transistors as room-temperature terahertz…
www-g.eng.cam.ac.uk/nms/publications/pdf/nmat3417.pdf28 Sep 2012: We also note a further sign switch around VG =0 in all curves.This suggests a contribution to the photoresponse of thermoelectricorigin23,24, arising from the presence of the ungated ... 24. Gabor, N. M. et al. Hot-carrier-assisted intrinsic -
Thermal conductivity of diamond-like carbon filmsM. Shamsa, W. L. ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Shamsha_APL2006.pdf13 Nov 2006: and E by laser induced acoustic waves and/or by surfaceBrillouin scattering.22–24 Visible and UV Raman measure-ments were performed using Renishaw Ramanspectrometers.1,25 Table I summarizes the ... 374 412GLCH 2 24 0.248 379ta-C:H 2.2 30 250 0.77 -
acs_nn_nn-2013-00758r 1..7
www-g.eng.cam.ac.uk/nms/publications/pdf/nn400758r.pdf2 Apr 2013: The properties of multilayer gra-phene (e.g., bilayer, BLG, and trilayer,TLG) vary with stacking order23 andwith relative twist.24 In BLG, a trans-verse electric field can open a ... 24. Latil, S.; Meunier, V.; Henrard, L.Massless Fermions in Multilayer -
Fabrication of graphene nanoribbons via nanowire lithography
www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_PSSB2009.pdf8 Dec 2009: Similar to the case of nanotubes, confinement modifiesthe electronic structure of graphene, when cut intonanoribbons [18–24]. ... Harrison, Phys.Rev. B 75, 064418 (2007). [24] K. Nakada, M. Igami, and M. -
8/1/2016 Graphene based optoelectronics…
www-g.eng.cam.ac.uk/nms/highlights-press/faster_future_phys.pdf1 Aug 2016: Huge, oncehated fish now seen asweapon against Asian carp Jul 29,2016 9. Mars gullies likely not formed by liquidwater Jul 29, 2016 24. -
Photoluminescence Spectroscopy of Carbon Nanotube Bundles:Evidence…
www-g.eng.cam.ac.uk/nms/publications/pdf/Tan_PRL2007.pdf27 Sep 2007: due toits much lower position than previous investigations ofthese tubes [18,19,24,25]. ... 24] H. Htoon et al., Phys. Rev. Lett. 94, 127403 (2005).[25] S. -
http://www.fabtech.org/content/view/1720
www-g.eng.cam.ac.uk/nms/highlights-press/semiconductorfabtechlowtemepraturenanotube.pdf20 Apr 2007: ring oscillator circuit around single carbon nanotube (24/03/2006) > Flexible 'Nano skin' electronics (02/03/2006) > Carbon nanotubes made in Munich (04/02/2005). < -
Vertically Illuminated, Resonant Cavity Enhanced, Graphene–Silicon…
www-g.eng.cam.ac.uk/nms/publications/pdf/Casalinos.pdf4 Dec 2017: modern telecom systems, operation at 1550 nmbenefits from a reduced light absorption in optical fibers.1 Infree-space optical communications (FSO)24 and light-radars(LIDARs),5,6 this minimizes the ... chips using advanced packaging andassembling.24 -
Coherent anti-Stokes Raman spectroscopy of single and multi-layer…
www-g.eng.cam.ac.uk/nms/publications/pdf/376.pdf7 Apr 2020: ωas = ωP ωv.In the biological field21,24, a wealth of studies has demonstrated. ... Annu. Rev. Anal. Chem. 1,883–909 (2008). 24. Evans, C. L. et al. -
Nonlinear optics: Fibre sources in the deep ultraviolet
www-g.eng.cam.ac.uk/nms/publications/pdf/nphoton.2011.166.pdf29 Jul 2011: St. J. J. Lightwave Technol. 24, 4729–4749 (2006).10. Dudley, J. M., Genty, G. & -
INSTITUTE OF PHYSICS PUBLISHING NANOTECHNOLOGY Nanotechnology 17…
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NT2006.pdf13 Nov 2006: of CdSeis only a function of the powder temperature and is independentof the Ar partial pressure [24]. ... 94 6005. [24] Merten U and Bell W E 1967 The Characterization ofHigh-Temperature Vapors (New York: Margrave) chapter 4. -
ELASTIC CONSTANTS OF DIAMOND LIKE CARBON FILMSBY SURFACE BRILLOUIN ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_mrs99.pdf20 Oct 2009: lay. 3.24 63.5ta-C:H 70% 28.4 2.35 70 6 30%ta-C:H 28.4 2.35 43. ... of 3.24 g/cm 3 [11]. -
Few-cycle pulses from a graphene mode-locked all-fiber laser D. ...
www-g.eng.cam.ac.uk/nms/publications/pdf/1.4922397.pdf3 Jul 2015: Downloaded to IP:. 129.169.173.200 On: Mon, 29 Jun 2015 16:19:24. 26F. ... Downloaded to IP:. 129.169.173.200 On: Mon, 29 Jun 2015 16:19:24. -
VOLUME 93, NUMBER 18 P H Y S I ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Piscanec_PRL2004.pdf27 Nov 2006: The EPCs near K between bands [24] allow theaccurate determination of the intensity and shape of theRaman D peak. ... Jianget al., Chem. Phys. Lett. 392, 383 (2004). [24] For the branch near A01 at K, jg2Kk0q0;Kk0j2 hg2KiF1 cos'00. -
acs_nn_nn-2014-02676g 1..10
www-g.eng.cam.ac.uk/nms/publications/pdf/nn502676g.pdf15 Jul 2014: Ref 9measured I(D)/I(G) for irradiated single layer. Address correspondence toacf26@eng.cam.ac.uk. Received for review May 16, 2014and accepted June 24, 2014. ... Lett. 2010, 104, 227401. 24. Kalbac, M.; Reina-Cecco, A.; Farhat, H.; Kong, J.; Kavan, -
320 fs pulse generation from an ultrafast laser inscribed ...
www-g.eng.cam.ac.uk/nms/publications/pdf/beecher_apl2010.pdf20 Sep 2010: Single wall carbon nanotubes SWNTs12–22 andgraphene12,13 are promising saturable absorbers SAs formode-locking fiber,12–17 waveguide,6 solid-state,23 and semi-conductor lasers.24 They have several ... complex processes, such as molecular beam epitaxy -
Research Graphene means business – two-dimensional materialmoves from …
www-g.eng.cam.ac.uk/nms/highlights-press/Graphene%20means%20business.pdf27 May 2016: electric energy through heatlike Geothermal source of energy which may provide 24 hrs energy for consumption .I did some research back in 1999 and but unfortunately I wonder today that what ... Walking and cycling good -
Effect of the sp2 carbon phase on n-type conduction ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Ikeda_JAP2008.pdf20 Oct 2008: for further N2 addi-tion up to 20%;22,24 ii electron mobility increases slightlywith N2 10%–20%;. ... 0 TM1/2, following Ref. 24, with VRH0 independent of TM. However, the slopes for. -
1077-260X (c) 2013 IEEE. Translations and content mining are ...
www-g.eng.cam.ac.uk/nms/publications/pdf/06880814.pdf22 Aug 2014: locked pulses has potential applications in nonlinear frequency. conversion [23] and surgery [24]. ... 24 cm-1. larger than in individual flakes [2]. Thus, even if the. -
nn-2019-02621n 1..10
www-g.eng.cam.ac.uk/nms/publications/pdf/380.pdf7 Apr 2020: 0.005 carbon weight% at 1084 C)23 and its catalytic role during growth.24,25. ... The Solubility of C in Solid Cu.Scr. Mater. 2004, 51, 15.(24) Li, X.; Zhu, Y.; Cai, W.; Borysiak, M.; Han, B.; Chen, D.; Piner, R.D.; Colombo, L.; Ruoff, -
doi:10.1016/j.physe.2007.10.044
www-g.eng.cam.ac.uk/nms/publications/pdf/Hsieh_PE2007.pdf27 May 2008: eXerox Research Centre of Canada, Mississauga, Ont., Canada L5K 2L1. Available online 24 October 2007. ... Several groups haverecently considered CNTs for fabrication of TFTs, usingvarious fabrication methods, including spin coating, dropcasting, and -
doi:10.1016/j.diamond.2005.10.049
www-g.eng.cam.ac.uk/nms/publications/pdf/Boutroy_DRM2006.pdf13 Nov 2006: C2H2 60 nm/s 0.002 cc/Package/24 H 20. CH4 4 nm/s 0.030 cc/Package/24 H 1.3. ... C2H4 25 nm/s 0.012 cc/Pckage/24 H 3.3. a BIF: Barrier Improvement Factor is the ratio of a non-coated bottle to a. -
nn5b06488 1..7
www-g.eng.cam.ac.uk/nms/publications/pdf/acsnano.5b06488.pdf14 Sep 2016: the investigation of the carrier dynamics is only at thebeginning.24,29,30. In this work, we assign these features by combining ultrafastTA spectroscopy of exfoliated 1L-MoS2, with selectiveexcitation of ... The irreducible Brillouin zone (IBZ) issampled -
No Job Name
www-g.eng.cam.ac.uk/nms/publications/pdf/Cantoro_NL2006.pdf13 Nov 2006: device operation.50 An optimized (pregrowth)catalyst nanostructuring, a lower C2H2 partial pressure,10,24. ... Small 2005, 1, 1180.(24) Lin, M.; YingTan, J. P.; Boothroyd, C.; Loh, K. -
The Stiffness of Tensegrity Structures S.D. GuestDepartment of…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2011b.pdf22 Jun 2010: It consists of j = 12nodes, and b = 30 members, made up of 24 cables and 6 struts. ... The effect of this is to leave an 24 24 symmetric matrix,for which the eigenvalues are then found. -
First-Principles Prediction of Doped Graphaneas a High-Temperature…
www-g.eng.cam.ac.uk/nms/publications/pdf/Savini_PRL2010.pdf15 Jul 2010: In particular, it was proposed thatfully hydrogenated graphene (graphane) would be stable[24]. ... The main difference between graphene and graphaneis that, while the former is fully sp2 bonded, the latter issp3, as diamond [24].
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