Search

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

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.

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.

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

frequencies.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.

60 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.

Guillaume 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!

RAPID COMMUNICATIONS. PHYSICAL REVIEW B 15 DECEMBER 2000-IIVOLUME 62, NUMBER 24.