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  2. Femtonewton Force Sensing withOptically Trapped NanotubesO. M.…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_NL2008.pdf
    8 Oct 2008: Phys. ReV. Lett. 1970, 24, 156–159.(2) Ashkin, A.; Dziedzic, J. M.; Bjorkholm, J.E.; Chu, S. ... Phys. ReV.Lett. 2008, 100, 163903. (24) Rohrbach, A. Stiffness of optical traps: Quantitative agreement betweenexperiment and electromagnetic theory.
  3. Intravalley Spin–Flip Relaxation Dynamics in Single-Layer WS2

    www-g.eng.cam.ac.uk/nms/publications/pdf/ZWang2018a.pdf
    21 Nov 2018: We use a 24 24 1 k-grid tocalculate the BetheSalpeter kernel. ... The real-time simulation adoptsa coarse 24 24 1 and a denser 61 61 1 k-grid.
  4. Spider silk reinforced by graphene or carbon nanotubes

    www-g.eng.cam.ac.uk/nms/publications/pdf/Lepore.pdf
    22 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).
  5. Vapor-phase nucleation of individual CdSe nanostructuresfrom…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_APL2008.pdf
    21 Jan 2008: on functionalized substrates;22,24 and c they canbe made of the same material of the final NWs, thus, mini-mizing chemical contaminations.20. ... Although nanocrystal-seeded growth has proven viablefor NWs synthesis,10,20,21,24 many fundamental
  6. doi:10.1016/j.physe.2007.09.161

    www-g.eng.cam.ac.uk/nms/publications/pdf/Hasan_PE2007.pdf
    27 May 2008: Inaddition to dielectric screening [24,25], the presence ofbundles [20,21] contributes to the red shift in theabsorption spectrum compared to sample C1. ... Werecently reported that addition of PVP in a freshlyprepared SWNT dispersion increases the PL
  7. doi:10.1016/j.physe.2007.10.088

    www-g.eng.cam.ac.uk/nms/publications/pdf/Marago_PE2007.pdf
    27 May 2008: References. [1] A. Ashkin, Phys. Rev. Lett. 24 (1970) 156. [2] A. ... Gittes, C.F. Schmidt, Opt. Lett. 23 (1998) 7. [24] A. Rohrbach, Phys.
  8. 7 Apr 2020: 24). This. 210. a. y. y. x. x. 10 cm. 10 cm.
  9. PII: S0925-9635(00)00479-9

    www-g.eng.cam.ac.uk/nms/publications/pdf/MilneDRM2001.pdf
    15 Oct 2009: Recently,a a. Ferrari and Robertson 24 have shown from their workŽ. ... Lett. 76. Ž. Ž. 18 2000 2627. Ž. 24 A.C. Ferrari, J.
  10. doi:10.1016/j.msec.2003.09.084

    www-g.eng.cam.ac.uk/nms/publications/pdf/Piscanec_MSEC2003.pdf
    28 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.
  11. Tetrahedral amorphous carbon resistive memories with graphene-based…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ott2018.pdf
    14 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.
  12. Resistive Switching Crossbar Arrays Based on Layered Materials

    www-g.eng.cam.ac.uk/nms/publications/pdf/501_Lanza2022_2.pdf
    30 Mar 2023: Switching energy <6 nJ 10 pJ 10 pJ 24 nJ. Endurance 4  104 1015 107 106. ... omm. ons License. 2023 Wiley-VCH GmbH2205402 (7 of 24). www.advmat.dewww.advancedsciencenews.com. Adv.
  13. 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: 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,
  14. HBN-Encapsulated, Graphene-based, Room-temperature Terahertz…

    www-g.eng.cam.ac.uk/nms/publications/pdf/397.pdf
    7 Jan 2021: For these, the dominant detectionmechanism can be tailored by design.21 Their ultrafastdynamics22 and the ease of fabrication23,24 and integration25. ... C. Production and processing of graphene and 2dcrystals. Mater. Today 2012, 15, 564589.(24) Ferrari,
  15. RAMAN SIGNATURE OF BONDING AND DISORDER IN CARBONS A ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_mrs99raman.pdf
    20 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.
  16. 1.4937461

    www-g.eng.cam.ac.uk/nms/publications/pdf/1.4937461.pdf
    19 Feb 2016: air-hole spacing,23 thus offering possibilities for both nonli-. nearity and dispersion management in fiber lasers.24,25. ... persion management,15 nonlinearity management is alsoa)Electronic mail: dp387@cam.ac.uk. 0003-6951/2015/107(24)/241107/4/$30.00
  17. Charge-tuneable biexciton complexes in monolayer WSe2

    www-g.eng.cam.ac.uk/nms/publications/pdf/Barbone2018.pdf
    3 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.
  18. INSTITUTE OF PHYSICS PUBLISHING NANOTECHNOLOGY Nanotechnology 16…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NT2005.pdf
    23 Nov 2006: Rev. Mater. Res.24 83. [2] Duan X, Huang Y, Agarwal R and Lieber C M 2003 Nature421 241.
  19. 42414.dvi

    www-g.eng.cam.ac.uk/nms/publications/pdf/Bottani_EPL1998.pdf
    8 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.
  20. Nonlinear optics: Fibre sources in the deep ultraviolet

    www-g.eng.cam.ac.uk/nms/publications/pdf/nphoton.2011.166.pdf
    29 Jul 2011: St. J. J. Lightwave Technol. 24, 4729–4749 (2006).10. Dudley, J. M., Genty, G. &
  21. 8/1/2016 Graphene based optoelectronics…

    www-g.eng.cam.ac.uk/nms/highlights-press/faster_future_phys.pdf
    1 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.
  22. phb76194d_598

    www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_PSSB2007.pdf
    28 Nov 2007: Nanoruptor ultrasonicator) in presence of sodium dodecylbenzenesulphonate (SDBS) as surfactant [24]. ... 24] M. F. Islam, E. Rojas, D. M. Bergey, A. T.
  23. 1.4942778

    www-g.eng.cam.ac.uk/nms/publications/pdf/1.4942778.pdf
    21 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.
  24. acs_nn_nn-2012-01587b 1..3

    www-g.eng.cam.ac.uk/nms/highlights-press/ACSNANO_April2012.pdf
    2 May 2012: April 24, 2012. C 2012 American Chemical Society. Graphene Electronics, Fresh from the Printer.
  25. LETTERS Breakdown of the adiabaticBorn–Oppenheimer approximationin…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Pisana_NM2007.pdf
    2 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. &
  26. Using APL format

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_APL1999.pdf
    20 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
  27. acs_nn_nn-2011-01203s 1..6

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn201203s.pdf
    5 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.
  28. Renewable Electricity ImpEE IMPRO VIN G ENG INEERIN G ...

    www-g.eng.cam.ac.uk/impee/topics/RenewElectricity/files/Renewable%20Electricity%20v4%20PDF.pdf
    11 Jun 2006: litre. Grid Electricity1 0.43 - -Natural Gas 0.19 - -. Fuel Oil 0.27 3223 -Diesel 0.25 3164 2.63Petrol 0.24 3135 2.30.
  29. Excitonic Emission of Monolayer Semiconductors Near-Field Coupled to…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Galy2018.pdf
    11 May 2018: B.; Turnbull, G. A. How torecognize lasing. Nat. Photonics 2009, 3, 546.(24) Purcell, E. ... Today 1989, 42, 24.(26) Auffev̀es, A.; Gerace, D.; Geŕard, J.-M.; Franca Santos, M.;Andreani, L.
  30. Graphene field-effect transistors as room-temperature terahertz…

    www-g.eng.cam.ac.uk/nms/publications/pdf/nmat3417.pdf
    28 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
  31. Carbon Nanotube Polycarbonate Composites for Ultrafast Lasers

    www-g.eng.cam.ac.uk/nms/publications/pdf/Scardaci_AM2008.pdf
    5 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.
  32. doi:10.1016/j.physe.2007.10.024

    www-g.eng.cam.ac.uk/nms/publications/pdf/Mattevi_PE2007.pdf
    27 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.
  33. Coherent anti-Stokes Raman spectroscopy of single and multi-layer…

    www-g.eng.cam.ac.uk/nms/publications/pdf/376.pdf
    7 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.
  34. Electrically Controlled Nano and Micro Actuation in Memristive…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Kos2018.pdf
    5 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
  35. nl4018463 1..6

    www-g.eng.cam.ac.uk/nms/publications/pdf/nl4018463.pdf
    15 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
  36. Thermal conductivity of diamond-like carbon filmsM. Shamsa, W. L. ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Shamsha_APL2006.pdf
    13 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
  37. Supplementary Note 1 Continuum-model Hamiltonian and cur-rent matrix…

    www-g.eng.cam.ac.uk/nms/publications/pdf/SaynatjokiSI.pdf
    7 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.
  38. Fabrication of graphene nanoribbons via nanowire lithography

    www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_PSSB2009.pdf
    8 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.
  39. Effect of the sp2 carbon phase on n-type conduction ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ikeda_JAP2008.pdf
    20 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.
  40. acs_nn_nn-2014-02676g 1..10

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn502676g.pdf
    15 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,
  41. INSTITUTE OF PHYSICS PUBLISHING NANOTECHNOLOGY Nanotechnology 17…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NT2006.pdf
    13 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.
  42. acs_nn_nn-2013-00758r 1..7

    www-g.eng.cam.ac.uk/nms/publications/pdf/nn400758r.pdf
    2 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
  43. Vertically Illuminated, Resonant Cavity Enhanced, Graphene–Silicon…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Casalinos.pdf
    4 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
  44. Photoluminescence Spectroscopy of Carbon Nanotube Bundles:Evidence…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Tan_PRL2007.pdf
    27 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.
  45. 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: 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.
  46. nn-2019-02621n 1..10

    www-g.eng.cam.ac.uk/nms/publications/pdf/380.pdf
    7 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,
  47. The Stiffness of Tensegrity Structures S.D. GuestDepartment of…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2011b.pdf
    22 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.
  48. Nanoscale Cathodoluminescence and Conductive Mode Scanning Electron…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ramsden_2023.pdf
    20 Jul 2023: and doping21,24 of hBN encapsulated TMDs have been assessedthrough correlation with their optical emission.20,21,24 Theseresults have shown that nanoscale heterogeneities in doping andstrain exist in TMD-based ... devices.20,21,24.
  49. Thermionic graphene&sol;silicon Schottky infrared photodetectors

    www-g.eng.cam.ac.uk/nms/publications/pdf/2022doukas.pdf
    17 Mar 2022: Combining the above, we get a transcendental equa-tion [24,74,91]. sF E2F,SLG sF 0E 2F 0,SLG. =. ( ... d,. (24). where = ω iτ 1opt and τopt is the free electron relaxationtime related to charge carrier mobility in SLG [107].
  50. Low-Loss Integrated Nanophotonic Circuits with Layered Semiconductor…

    www-g.eng.cam.ac.uk/nms/publications/pdf/2021NanoLett.pdf
    27 Apr 2021: Dint(μ) = ωμ ω0 μD1 = D2μ2/2 D3μ3/6 D4μ4/24. , is shown in Figure 3b, top. ... Nano Lett.2014, 14, 62316236.(24) Robert, C.; Picard, R.; Lagarde, D.; Wang, G.; Echeverry, J.
  51. Research Graphene means business – two-dimensional materialmoves from …

    www-g.eng.cam.ac.uk/nms/highlights-press/Graphene%20means%20business.pdf
    27 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 

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