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Ka values areunaffected by the proportion of direct guest interactions withthe AuNP surface, if any. ... The obtained binding isotherms were used ascalibration curves through G2 = θ/(Ka Kaθ).

KA KA. K A A. [( )( ) ][( )( ) ]. 0. QE 1 11 QE 2 22. 212 21 (2). where ΩQE = ω12 iγ12 is the complex frequency of thetwo-level electronic transition with ω12 being ... KA KA. K A A. [( )( ) ][( )( ) ]. 0. QE 1 11 QE 2 22. 212 21 (9). For a system

Saand S. Kawakami, Phys. Rev. B58, R100961998!; H. Kosaka, T. Ka-washima, A. ... M. Monro, and D. J. Richards, Opt. Lett.24, 12031999!;J. C. Knight, T.

Saand S. Kawakami, Phys. Rev. B58, R100961998!; H. Kosaka, T. Ka-washima, A. ... M. Monro, and D. J. Richards, Opt. Lett.24, 12031999!;J. C. Knight, T.

Received 24 July 2006; published 25 September 2006). A new self-aligned robust method for coupling to whispering gallery modes (WGMs) of submicronmicrospheres utilizes their periodic arrangement without relying on nanopositioned ... Lett. 24, 723(1999).

Wide-angle and low-angle X-raydiffraction (XRD) data were collected using a Siemens D5000 X-ray diffractometer with Cu Ka radiation (k = 1.5406 Å). ... The films were deposited on double-sided pol-ished single crystalline n-type Si (1 0 0) wafers which

Lett. 24, 1416 (1999).6N. N. Lepeshkin, A. Schweinsberg, and G. Piredda, Phys. ... 24, 711 (1999).24H. Monard and F. Sabary, Thin Solid Films 310, 265 (1997).25H.

The Bose glass to superfluid transition was first observedin Josephson junction arrays [22,23] and it has recently beenobserved in thermally equilibrated cold atom lattices [24], butdifferent features emerge for the ... 8). From Eq. (B5), we can see that

22]. Thevalidity of the approximation is further strengthened by recentexperiments and simulation on both condensate pairs [24]and small closed chains [25]. ... MJ = cos (ka)2. J 0 0 00 J 0 00 0 J 00 0 0 J.

metal and void, and the primeindicates differentiation with respect to the argument ka. ... C. Kitson, and J. R. Sambles, Phys. Rev. B 54, 6227 1996.24 P.