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Direct measurement of the complex refractive index in the ...
https://www.np.phy.cam.ac.uk/system/files/documents/apl08-xray-scattering.pdfNatl. Acad. Sci. U.S.A. 105, 24 2008. 7R. Soufli and E. ... T. Chantler, J. Phys. Chem. Ref. Data 24, 71 1995.12Centre for X-Ray Optics, http://henke.lbl.gov/optical_constants/. -
Coexistence of low threshold lasing and strong coupling in ...
https://www.np.phy.cam.ac.uk/system/files/documents/jap04-mcav-lasing.pdfGuillaume Malpuech and Alexey KavokinLASMEA, UMR-6602, Universit Blaise Pascal, 24 av. ... This dependence has been observed for arange of detuningD! conditions of exciton and cavity modefrom D512 to 24 meV! -
APPLIED PHYSICS LETTERS VOLUME 81, NUMBER 2 8 JULY ...
https://www.np.phy.cam.ac.uk/system/files/documents/apl02-directwrite_0.pdfNouchi, T. Mitsuyu, M. Watanabe, P. G. Kazansky, andHirao, Opt. Lett.24, 646 1999! ... Smith, OLett. 24, 13111999! 8 H. Sun, S. Juodkazis, M. Watanabe, S. -
smll201200546.indd
https://www.np.phy.cam.ac.uk/system/files/documents/small12-januscb.pdf22 , 23 ] Meanwhile, CB[ n ]s have been utilized as stabilizing ligands for noble metal nanoparticles (NPs), such as that of gold, [ 24–27 ] silver, [ 28 , 29 ] and palladium. [ ... 24 mM HCl, and 0.16 mL of a 6 mM AgNO 3 aqueous solution with 0.12 mL -
Trapping plasmonic nanoparticles with MHz electric fields
https://www.np.phy.cam.ac.uk/files/apl22_mhzdielectrophoresis.pdf18 May 2022: The electric field distribution is analytically approximatedas that from two symmetrical hyperbolic 2D conductors,24 allowingthe total potential to be extracted for different separations of NPs[Figs. ... Mater. 24, OP305 (2012). Applied Physics Letters -
6549_13925_67856.dvi
https://www.np.phy.cam.ac.uk/system/files/documents/optexp-05-lx.pdfdrops,” Liq. Crys.24, 117–125 (1998).8. A. Ferńandez-Nieves, D. R. Link, D. ... Similarly, the micromirror surface is treated with a surfactant [24] to produce homeotropicLC alignment. -
Hot electron science in plasmonics and catalysis: what we argue about
https://www.np.phy.cam.ac.uk/system/files/documents/FaradayDisc19_overview.pdfFaraday DiscussionsCite this: DOI: 10.1039/c9fd00027e. PAPER. Publ. ishe. d on. 24. ... n 4/. 24/2. 019. 1:35. :53. PM. View Article Online. 10 F. -
Determination of nonlinear refractive index in a Ta2O5 rib waveguide…
https://www.np.phy.cam.ac.uk/system/files/documents/optexp04-ta2o5spm.pdf24. 2. effdxdy)y,x(F. dxdy)y,x(FA. = (4). where F(x,y) is the modal intensity distribution. ... 12. 14. 16. 18. 20. 22. 24. 26. 28. band. wid. -
Corrugated metallodielectric superlattices via release-rollup…
https://www.np.phy.cam.ac.uk/system/files/documents/optexp11-rollup-grating.pdfLett. 10, 1787–1792 (2010). 24. I.M. Pryce, K. Aydin, Y. A. ... ble electronics [22], flexible plasmonics [23] and flexible metamaterials [24]. By using a PDMS. -
Tuneable polaritonics at room temperature with strongly coupled…
https://www.np.phy.cam.ac.uk/system/files/documents/apl11-tamm300k.pdfMechanical displacement of suspended layers forexploiting polaritonic MEMS can be achieved in such de-vices using bridge- or cantilever-etched structures togetherwith piezoelectric actuation,24 accessing optomechanical po-lariton coupling regimes. -
Shear ordering in polymer photonic crystals D. R. E. ...
https://www.np.phy.cam.ac.uk/system/files/documents/pre10-mproptics.pdf4c during “creepingflow” 23,24. Assuming a parabolic flow profile, estimated strains atthe onset of crystal melting yield point, Region B/C tran-sition were essentially constant within error, ranging from60% ... Rheol. 52, 649 2008.24 A. Le Grand and -
doi:
https://www.np.phy.cam.ac.uk/system/files/documents/EnEnvSci14BiVO4opals.pdfZn-doping of BiVO4 could haveoccurred during the annealing process and Zn-doping waspreviously shown to give a negative effect on the photocatalyticperformance of BiVO4.24 However, signicant Zn-doping ofBiVO4 ... View Article Online. 24 K. P. S. Parmar -
rsc_cp_b712144j 6016..6020
https://www.np.phy.cam.ac.uk/system/files/documents/pccp07-serrs.pdfplatinum,24 proving the flexibility of our technique. In our. a School of Chemistry, University of Southampton, Southampton, UKSO17 1BJ. ... E. Russell, Faraday Discuss., 2005, 132,191–199. 24 M. E. Abdelsalam, S. -
Interrogating Nanojunctions Using Ultraconfined Acoustoplasmonic…
https://www.np.phy.cam.ac.uk/system/files/documents/PRL17_bouncingNPoM.pdfbecome deformed by light due to the low cohesive energyof gold [23,24]. ... 24] J. Mertens, A. Demetriadou, R. W. Bowman, F. Benz,M.-E. Kleemann, C. -
acs_NL_nl-2011-02875w 1..5
https://www.np.phy.cam.ac.uk/system/files/documents/nanolett11-secars.pdffrequencies.18,24,2628 The pump resonance seems to have thelargest effect (Supporting Information, Figure S5), which is alsoconsistent with the mechanism of SECARS described later inthe paper. ... R. Anal. Biochem. 2001, 298, 1–24.(8) Koo, T.; Chan, S. -
VOLUME 77, NUMBER 13 P H Y S I ...
https://www.np.phy.cam.ac.uk/system/files/documents/prl96-spin-in-dms.pdfThe QWscontain a single 3-ML barrier of MnSes1 3 3 ML d, threeequispaced single monolayers of MnSes3 3 1 ML d,24 one-eighth ML s24 3 1y8 ML d, ... Figure 1( b) shothe field dependence ofVL and DE in the 24 3 1y8 MLsample at different temperatures. -
Title: font: times; size: 18 point; style: plain; justified: center;…
https://www.np.phy.cam.ac.uk/system/files/documents/optexp10-pbi-mcav_0.pdfC) 2009 OSA 23 November 2009 / Vol. 17, No. 24 / OPTICS EXPRESS 22171. ... Rev. B 42(17), 11099–11107 (1990). 24. P. A. Hobson, W. L. -
USING STANDARD SYSTE
https://www.np.phy.cam.ac.uk/system/files/documents/prb00-rc-mopo.pdfRAPID COMMUNICATIONS. PHYSICAL REVIEW B 15 DECEMBER 2000-IIVOLUME 62, NUMBER 24. -
Strong Coupling between Localized Plasmons and Organic Excitons in ...
https://www.np.phy.cam.ac.uk/system/files/documents/prl06-jagg-plasmons.pdf60 meV) from the strongest plasmon absorption. Thisfurther suggests that the balance between plasmon reab-sorption and radiative coupling controls which moleculesemit PL efficiently [24]. ... Mater. 16, 90 (2004).[24] P. Anger, P. Bharadwaj, and L. -
1.4876475
https://www.np.phy.cam.ac.uk/system/files/documents/APL14_MoS2onAu.pdfq b1 d3 <e eAu eeAu þ e. :. Here, q is the quantum yield of the emitter (around 10%), b1is its decay rate (for which we use the 24 nm linewidth ... Chang, L.-J. Li, and T.-W. Lin, Adv. Mater. 24, 2320 (2012).
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