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Lett. 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.

24. 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.

Zn-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, signicant Zn-doping ofBiVO4 ... View Article Online. 24 K. P. S. Parmar

Mechanical 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.

4c 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

C) 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.

The 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.

become 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.

platinum,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.

B. Wright, Opt. Lett.24, 1305 (1999).[5] W. Chen, H. J. Maris, Z.