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Graphene Reflectarray Metasurface for Terahertz Beam Steering and…
www-g.eng.cam.ac.uk/nms/publications/pdf/Tamagone2018.pdf8 Jun 2018: Furthermore, highmobility of SLG allows mid infrared plasmon-polaritons,also tuneable by gating[24, 25]. ... From Eq. 22 we get:. γR =(RON ROFF)2(1 ω2τ2). 4 RON ROFF' 0.856 (24). -
doi:10.1098/rspa.2005.1598
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/guest2006.pdf25 Jan 2008: 24. 35 dq. dĈ. " #C/:. ð4:3ÞTo find equilibrium configurations of the structure, we look for points where. ... K̂ Zv2Û=vq2 v2Û=vq vĈ. v2Û=vq vĈ v2Û=vĈ2. 24. 35; ð4:5Þ. is positive definite. -
Identification of Exciton Complexes in Charge-Tunable Janus WSeS…
www-g.eng.cam.ac.uk/nms/publications/pdf/446_Feuer2023.pdf17 Apr 2023: potential landscape due to spatial variations in layer separationand twist angle.23,24. ... Nat.Phys. 2021, 17, 720725.(24) Andrei, E. Y.; Efetov, D. K.; Jarillo-Herrero, P.; MacDonald, A.H.; Mak, K. -
Top-Gated Silicon Nanowire Transistorsin a Single Fabrication…
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_ACSNANO2009.pdf26 Jun 2009: This ensures that RW RC ROX, no matter if conduction is via holes or elec-trons.24 Statistically, we note that our SiO2 gate dielec-tric can exhibit two different responses. ... Silicon-Nanowire Transistors withIntruded Nickel-Silicide Contacts. Nano Lett -
High performance bilayer-graphene terahertz detectors Davide…
www-g.eng.cam.ac.uk/nms/publications/pdf/spirito_APL_2014.pdf14 Feb 2014: reports.10,20,24 This is interpreted as due to the larger gate. length, as predicted by the photo-induced voltage equation:15. ... Teppe, A. Tredicucci, and T. Nagatsuma,. Nanotechnology 24, 214002 (2013).11A. Lisauskas, S. -
Broadband, electrically tunable third-harmonic generation in graphene
www-g.eng.cam.ac.uk/nms/publications/pdf/Soavi2018-Nanotech.pdf9 Jul 2018: Te = 1,000 K. Te = 300 K. THGE. –0.24 eV–0.39 eV–0.42 eV–0.44 eV–0.48 eV. ... 24. Saynatjoki, A. et al. Ultra-strong nonlinear optical processes and trigonal warping in MoS2 layers. -
Machine Learning May Sometimes Simply Capture Literature Popularity…
www-g.eng.cam.ac.uk/nms/publications/pdf/2022.pogna_new.pdf25 Mar 2022: on SMILES-represented reaction and associated reactionconditions,43 and Rel-GAT (Relational Graph AttentionNeural Network) previously evaluated on Suzuki and severalother coupling reactions.24. -
Phonon-Assisted Electroluminescence fromMetallic Carbon Nanotubes and …
www-g.eng.cam.ac.uk/nms/publications/pdf/Essig_nanolett_2010.pdf21 May 2010: The spectra can be deconvo-luted in two Gaussians centered at 1.35 and 1.76 eV, witha full width at half-maximum (FWHM) of 0.28 and 0.24 ... In addi-tion, we observed that controlled oxidation with meta-chloroperbenzoic acid (MCPBA)24 does not increase -
nature nanotechnology…
www-g.eng.cam.ac.uk/nms/publications/pdf/Montblanch_2023SI.pdf25 Jul 2023: Appl. Phys. Lett. 103, 183112 (2013). 24. Sünner, T. et al. -
JSTQE TWINS_Revision2_all changes accepted
www-g.eng.cam.ac.uk/nms/publications/pdf/07748501.pdf25 Nov 2016: nonlinear spectroscopy, in the pump-probe [24] and SRS [23] configurations. Since both techniques use the same experimental approach to extract the differential signal, for the sake of clarity we will ... Express, vol. 23, pp. 25235–25246, 2015. [24] F. -
Renewable Electricity ImpEE IMPRO VIN G ENG INEERIN G ...
www-g.eng.cam.ac.uk/impee/topics/RenewElectricity/files/Renewable%20Electricity%20v4%20PDF.pdf11 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. -
Identification of Exciton Complexes in Charge-Tunable Janus WSeS…
www-g.eng.cam.ac.uk/nms/publications/pdf/446_Feuer2023SI.pdf25 Jul 2023: potential landscape due to spatial variations in layer separationand twist angle.23,24. ... Nat.Phys. 2021, 17, 720725.(24) Andrei, E. Y.; Efetov, D. K.; Jarillo-Herrero, P.; MacDonald, A.H.; Mak, K. -
RAPID COMMUNICATIONS PHYSICAL REVIEW B 89, 121402(R) (2014) Effects…
www-g.eng.cam.ac.uk/nms/publications/pdf/PhysRevB.89.121402.pdf6 Mar 2014: B dependence can beexplained through the Slonczewski-Weiss-McClure (SWM)model [22–24]. ... q̃ = 2mlB V1. kzmV1. cos θ. sin2 θ V 24/V 21 cos. -
Graphene Mode-Locked Ultrafast LaserZhipei Sun,† Tawfique Hasan,†…
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_ACSNANO_2010.pdf23 Feb 2010: passively mode-lock an erbium-doped fiber laser working at 1559 nm, with a 5.24 nm spectral bandwidth and. ... arXiv:0908.0154, 2009. 24. Eberlein, T.; Bangert, U.; Nair, R. R.; Jones, R.; Gass, M.;Bleloch, A. -
st148018.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/PiscanecEPJ2007.pdf15 Oct 2009: This is the Case in graphene, graphite and nanotubes, where γan is much smallerthan γEP [12].The EPC contribution to γqη is given by the Fermi golden rule [24]:. ... 94, 015503 (2005)24. P.B. Allen, Phys. Rev. B 6, 2577 (1972); P.B. -
The Preparation, Characterization and Tribological Properties of…
www-g.eng.cam.ac.uk/nms/publications/pdf/Morrison_PSSA1999.pdf15 Oct 2009: Therefore, to a first order, the effect of neutraland radical species can be neglected and the deposition process may be described by asubplantation model of subsurface growth [24, 25]. ... Mater. 4,. 366 (1995).[23] K. Enke, Thin Solid Films 80, 227 -
Resonant Raman spectroscopy of twisted multilayer graphene
www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms6309.pdf10 Nov 2014: ARTICLE. Received 24 Jan 2014 | Accepted 19 Sep 2014 | Published 10 Nov 2014. ... The G peakcorresponds to the high-frequency E2g phonon at G. The Dpeak is due to the breathing modes of six-atom rings and requiresa defect for its activation16,22–24. -
Graphene-Based Interconnects for Stable Dye-Sensitized Solar Modules
www-g.eng.cam.ac.uk/nms/publications/pdf/414_ACS.pdf26 Jan 2021: 23,24 and subsequently transferredto fluorine-doped Tin Oxide (FTO), the most common. ... in condition to react to lightby the mediation of a light-absorbing molecule, i.e., the dye)21,24. -
Electron-electron interactions and doping dependence of the…
www-g.eng.cam.ac.uk/nms/publications/pdf/basko_PRB2009.pdf20 Oct 2009: 24, 26, 32, 33,and 36. The G peak position, PosG, increases and its fullwidth at half maximum, FWHMG, decreases for both elec-tron and hole doping. ... 24 C. Casiraghi, S. Pisana, K. S. Novoselov, A. K. Geim, and A. -
1.1 Gigahertz Multi-Transistor Graphene Integrated Circuits
www-g.eng.cam.ac.uk/nms/publications/pdf/06724538.pdf4 Feb 2014: Bandgap engineering is usually attempted by patterning into graphene nanoribbons (GNRs) (24,11), but GNRs tend to have low mobilities (<200 cm2V1s1) (27) as a consequence of carrier scattering on disordered ... 6, no. 24, pp. 2822-2825, 2010. (26) X. Yang -
Dynamic Catalyst Restructuring during Carbon Nanotube Growth
www-g.eng.cam.ac.uk/nms/publications/pdf/nn102118y.pdf6 Jan 2011: We alsotested the Ni (001)graphene system because it has been re-ported that a single C atom is strongly attracted to the Ni(001)surface.24 For the graphene ... 24. Borjesson, A.; Zhu, W.; Amara, H.; Bichara, C.; Bolton, K.Computational Studies of -
03/12/2012 It's not exactly HARDware... Nokia and Samsung in ...
www-g.eng.cam.ac.uk/nms/highlights-press/Independent_20121130.pdf3 Dec 2012: 03/12/2012 It's not exactly HARDware. Nokia and Samsung in race to launch 'flexible' mobile phones during 2013 - News - Gadgets & Tech - The Independent. -
Multi-Valley Superconductivity in Ion-Gated MoS2 Layers
www-g.eng.cam.ac.uk/nms/publications/pdf/Piatti2018-3.pdf5 Sep 2018: When exfoliated frombulk to single layer (1L), they undergo an indirect-to-directgap transition,24 offering a platform for electronic andoptoelectronic applications,1,2,5 such as transistors,68 ... Electric-double-layer field-effecttransistors with ionic -
Strong plasmonic enhancement of photovoltage in graphene
www-g.eng.cam.ac.uk/nms/publications/pdf/2011Etchermeyer_ncomms.pdf30 Aug 2011: 2. 2. 4. 4. 4. 6. 6. 10. 10. 24. 20. ... Appl. Phys. Lett. 91, 063124 (2007).24. Abergel, D. S. L., Russell, A. & -
This content has been downloaded from IOPscience. Please scroll ...
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2013GuestA.pdf6 Feb 2014: received 24 May 2013; accepted in final form 17 June 2013published online 2 July 2013. ... Γ(Tx,Ty) 2 1 1 2 0 0= 24 0 0 0 0 0. -
acs_nn_nn-2013-03323k 1..13
www-g.eng.cam.ac.uk/nms/publications/pdf/nn403323k.pdf11 Nov 2013: Nanotechnology2013, 24, 265102. 10. Liu, Z.; Tabakman, S. M.; Chen, Z.; Dai, H. -
acs_JA_ja-2010-10939a 1..6
www-g.eng.cam.ac.uk/nms/publications/pdf/Zhao_JACS_2011.pdf3 May 2011: Published: March 24, 2011. r 2011 American Chemical Society 5941 dx.doi.org/10.1021/ja110939a |J. ... 2007, 7,2711.(24) Blake, P.; Hill, E. W.; Neto, A. H. C.; Novoselov, K. -
Scalable Microaccordion Mesh for Deformable and Stretchable Metallic…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2015PAR.pdf14 Oct 2015: as a hyperelastic material usingthe Mooney-Rivlin fit with parameters E 1.23 MPa,C1 0.205 MPa, C2 0 MPa (corresponding to a 24-hour cure at 60 C) [49]. ... 24] Z. Xu, Z. Liu, H. Sun, and C. Gao, Highly electricallyconductive Ag-doped graphene fibers as -
sample.tex
www-g.eng.cam.ac.uk/nms/publications/pdf/Pedersen_IEEEPhotonics2012.pdf20 Jun 2012: 0.16. 0.18. 0.2. 0.22. 0.24. 0.26. 0.28. 0.3. 0.32. 1000 1020 1040 1060 1080 1100 1120 1140. ... Mater. 21, 3874-3899 (2009). [24] Z. Sun,T. Hasan and A. C. -
Nano Res (2010) 3: 404–411 404 Ultrafast Stretched-Pulse Fiber ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Sun_naonres_2010.pdf21 Jun 2010: These have been used to mode-lock fiber [8–23], waveguide [24], solid-state [25–27], and semiconductor lasers [28]. ... Langmuir 2008, 24, 5070–5078. [37] Hasan, T; Tan, P. H.; Bonaccorso, F; Rozhin, A. -
doi:10.1016/j.diamond.2003.10.086
www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_DRM2004.pdf27 Nov 2006: Byplotting j vs. time, this givesbya;0.24 w34x. Usingour a value, we find an independent value ofb between0.006 and 0.12. -
nn0c00309 1..11
www-g.eng.cam.ac.uk/nms/publications/pdf/Trovatello2020.pdf20 Jul 2020: transducers,24 which can be operatedat extremely high frequencies (up to several THz5). ... Continuous wave (CW) optical spectroscopies, like PL andabsorption, revealed signatures of excitonphonon interactionin 1L-TMDs.2326 This gives rise to peculiar -
Graphene: The quest for supercarbon : Nature News & Comment
www-g.eng.cam.ac.uk/nms/highlights-press/quest_for_supercarbon.pdf22 Nov 2013: Ultrashort laser pulses squeezed out of graphene. 24 May 2013. Graphene: The quest for supercarbon : Nature News & Comment http://www.nature.com/news/graphene-the-quest-for-supercarbon-1.14193. -
nn5b05647 1..9
www-g.eng.cam.ac.uk/nms/publications/pdf/acsnano.5b05647.pdf2 Feb 2016: Pos(G), Figure 1e, and FWHM(G), Figure 1f,are 1583 and 24 cm1. ... H.; Seifert, M.; Garrido, J. A. Graphene Transistors forBioelectronics. Proc. IEEE 2013, 101, 17801792.(24) Sanchez, V. -
ISSN:1369 7021 © Elsevier Ltd 2007JAN-FEB 2007 | VOLUME ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_MT2007.pdf8 Jan 2007: These films are usually deposited by plasma-enhanced. chemical vapor deposition (PECVD) at low bias voltage22-24. ... For a 100 nm a-C:H-coated bottle, the OTR is reduced. to 0.0008 cc/package/24 hours from the 0.04 cc/package/24 hours of. -
OE_revised.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/oe-20-22-25077.pdf18 Oct 2012: 24. S. Y. Set, H. Yaguchi, Y. Tanaka, and M. Jablonski, “Ultrafast fiber pulsed lasers incorporating carbon nanotubes,”IEEE J. ... Nanotubes have mode-lockedfiber [18, 24–29], waveguide [30, 31], solid-state [32–34] and semiconductor lasers [35], -
OE_29_final.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/Zaugg-2013-OE.pdf14 Dec 2013: Mater.21, 3874-3899 (2009). 24. Z. Sun, T. Hasan, F. Torrisi, D. ... Dueto its low-cost fabrication and assembly [16, 23, 24], graphene based saturable absorbers haveemerged as a promising saturable absorber (SA) for ultrafast pulse generation. -
phb79640d_540
www-g.eng.cam.ac.uk/nms/publications/pdf/Cervantes-Sodi_PSSb2008.pdf31 May 2011: Rev. Lett. 98, 196803 (2007).[24] B. Huang et al., arXiv:0708.1795v1.[25] H. -
Moiré Modulation of Van Der Waals Potential in Twisted Hexagonal…
www-g.eng.cam.ac.uk/nms/publications/pdf/2022chiodini.pdf17 Jun 2022: producing aspatially modulated interlayer registry, known as moire ́superlattice.24 This can lead to superconductivity5 andMott-like insulator states6 in twisted graphene bilayers, long-lived interlayer excitonic states in monolayer (1L) -
2D Materials ACCEPTED MANUSCRIPT • OPEN ACCESS Graphene-Black…
www-g.eng.cam.ac.uk/nms/publications/pdf/509_Akhavan2023.pdf27 Mar 2023: 123456789101112131415161718192021222324252627282930313233343536373839404142434445464748495051525354555657585960. Acc. epte. d M. anus. crip. t. 2. technology[8]. For applications in the short-wave in-frared (SWIR) (1000-2500nm/1.24-0.5eV), beyond -
acs_nn_nn-2014-00767b 1..12
www-g.eng.cam.ac.uk/nms/publications/pdf/nn500767b.pdf5 Jun 2014: These results arecomparable to those obtained with SWNTs at 1 μm.23,24. ... Opt. Lett. 2009, 34, 3526–3528. 24. Kelleher, E. J. R.; Travers, J. -
Dielectrophoretic Assembly of High-Density Arrays of Individual…
www-g.eng.cam.ac.uk/nms/publications/pdf/Aravind_ACSNano2009.pdf28 Jul 2009: GO can be subse-quently reduced to graphene,23 but leavesa significant number of defects that disruptthe electronic properties.24 Recently, much. ... Nano Lett. 2008, 8,4283–4287. 24. Mkhoyan, K. A.; Contryman, A. W.; Silcox, J.; Stewart, D. -
Rotation Detection in Light-Driven Nanorotors
www-g.eng.cam.ac.uk/nms/publications/pdf/Jones_ACSNano2009.pdf27 Oct 2009: Gold nanorods (AuNRs) have size-tunable optical properties, facile surfacechemistry, and appropriate scale for manyapplications in biology and medicine.23,24. ... J. Nanobiotechnol. 2004, 2, 3. 24. Kneipp, J. H.; Kneipp, H.; McLaughlin, M.; Brown, -
Subjecting a Graphene Monolayer to Tension and Compression
www-g.eng.cam.ac.uk/nms/publications/pdf/Tsoukleri_small2009.pdf30 Oct 2009: stress transfer[24] and the fracture processes in unidirec-. tional,[25] but also multidirectional,[26] composites. ... H. Hong, Nature 2009, 457, 706.[24] N. Melanitis, C. Galiotis, Proc. -
Using JPF1 format
www-g.eng.cam.ac.uk/nms/publications/pdf/Rodil_JAP2001.pdf4 Dec 2006: For rings containing N a contribu-tion between 1400 and 1500 cm21 from NvN vibrations hasbeen suggested,24 but it seems unphysical at low nitrogecontents. -
Anomalous low-temperature Coulomb drag in graphene-GaAs…
www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms6824.pdf23 Dec 2014: Science 335, 947–950 (2012). 24. Rojo, A. G. Electron-drag effects in coupled electron systems. -
Graphene-based mid-infrared room-temperature pyroelectric bolometers…
www-g.eng.cam.ac.uk/nms/publications/pdf/Sassi17.pdf1 Feb 2017: Avouris, P. Ultrafastgraphene photodetector. Nat. Nanotechnol. 4, 839–843 (2009). 24. -
Hindawi Publishing CorporationJournal of NanomaterialsVolume 2012,…
www-g.eng.cam.ac.uk/nms/publications/pdf/Cole_JNanoMater2012.pdf9 May 2012: alignment. The films demonstrated optoelectroniccharacteristics nearing the ITO benchmark and superiorcharacteristics to competing organic technologies such asTDA and PEG-enhanced PEDOT:PSS [24, 25]. ... 45, no. 5, pp. 913–921,2007. [24] B. D. Martin, N -
Light–matter interaction in a microcavity-controlled…
www-g.eng.cam.ac.uk/nms/publications/pdf/Michael_NatComm2012.pdf20 Jun 2012: Further data analysis reveals that microcavity-controlled thermal radiation is emitted into a narrow lobe with a total angular width of 24 (FWHM) only (see Supplementary Methods and Supplementary Fig. ... 24. Casiraghi, C. et al. Rayleigh imaging of -
Thermal and chemical vapor deposition of Si nanowires:Shape control,…
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_JAP2007.pdf18 Dec 2007: 12b correspond to deviceswith 7, 24, and 10 SiNWs for types I, II, and III, respec-tively. ... Curvescorrespond to devices with 7, 24, and 10 SiNWs for types I, II, and III,respectively.
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