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precursor.16,23 The latter was chosen because of our experience in. the templated electrodeposition of nanostructured materials.24–28. ... Plichon, J. Electroanal. Chem., 1998, 444, 247–252.24 G. S. Attard, P.

of Young’s moduli, EPETEgold 7 GPa. 79 GPa 0:1.24 The expected.

24 ] and the I domain was extracted for the fi nite-difference time-domain simulations. ... 24 ] C. A. Tyler , J. Qin , F.

PHYSICAL REVIEW B 15 JUNE 1996-IIVOLUME 53, NUMBER 24. 530163-1829/96/5324!/161404!/$10.00 R16 140 1996 The American Physical Society.

These prepared surfaces,rinsed clean and dried, were then dipped in colloidalsolutions of nanoplatelets in hexane for another 24 h.This gives a homogenous monolayer of platelets lying flatwith a surface ... This was ensuredby a sufficiently sparse

Pikus (BAP) [24]. ... JETP 33, 1053(1971). [24] G. L. Bir, A. G. Aronov, and G.

Box 1385, 71110 Heraklion, Greece. Received 25 October 2010; accepted 3 February 2011; published online 24 February 2011.

Adv. Mater 17(24):3011–3018.8. Pelrine R, Kornbluh R, Pei Q, Joseph J (2000) High-speed electrically actuated elas-. ... Chem Commun (Camb) (18):2571–2573. 24. Karg M, Pastoriza-Santos I, Pérez-Juste J, Hellweg T, Liz-Marzán LM (2007)Nanorod-coated

528 9) nm (3.14 0.26). (525 5) nm (0.24 0.07). BDP. ... Opt. Express 2015, 23,3325533269.(23) Pelton, M.; Bryant, G. W. Introduction to Metal-NanoparticlePlasmonics; Wiley: Hoboken, NJ, 2013.(24) Njoki, P.

Cam. brid. ge o. n 24. /09/. 2014. 17:. 16:3. 5. ... Yang and W. Huang, Macromolecules, 2004, 37,9746. 24 P. J. Flory and J.

Bimberg, Phys. Rev. B 52,11969 (1995). [24] M. A. Cusack, P.

The films were deposited on double-sided pol-ished single crystalline n-type Si (1 0 0) wafers which are opticallytransparent to infrared radiation out to wavelengths beyond 14 lm[24] ... Polisski, F. Koch, Appl. Phys. B 73 (2001) 31. [24] H.

Received 24 February 2003, revised 28 March 2003, accepted 28 March 2003Published online 11 August 2003.

2. The yield stress should depend on the Schmidtfactor for the different possible slip directions that canoperate in the ð111Þ slip plane [24]. ... Ruel, and P. Wiltzius, Nature. (London) 385, 321 (1997).[24] R. E.

a. b. 0.12. 1.0. 0.5. 0.0. 0.16. 0.20. 0.24. 20 30 40 50. ... This is the case even for regularphotonic crystals, where recent experimental and theoretical resultsshow similar discrepancies in transmission spectra5,24 26.

Aligning AuNRs end-to-end using a number of approaches, including supramolecular assembly, [ 18,19 ] solvent interactions, [ 20–23 ] lithography [ 24 ] and other techniques have been presented. ... 24 ] However, large scale solution-phase methods,

Mater. 6, 957–960 (2007).10. S. Colodrero, M. Ocaña, and H. Mı́guez, “Nanoparticle-based one-dimensional photonic crystals,” Langmuir 24,. ... the deflection [24].This can also be seen in the linearity of the maximum strain found at the centre

Received 10 June 2009; accepted 30 June 2009; published online 24 July 2009.

A 50 μm core optical fiber mounted inthe conjugate plane of the focal plane of a 20 objective (NA =0.24) served as a pinhole in the conjugate to the focal ... Wiesner, J. J. Baumberg andU. Steiner, Adv. Mater., 2012, 24, OP23–OP27.

The steady-statecurrent (Is) is achieved when the recombination and chargegeneration reach equilibrium.24,25 In bulk semiconductors, thecharge recombination rate is reduced in the presence ofplasmonic fields26,27 as the ... The surfaces were then