560
V. N. Pustovit and T. V. Shahbazyan
(a)
(b)
(c)
Fig. 15.17 FRET for N = 100 donors on top of spherical core-shell NP with Ag core radius
R c = 30 nm and SiO 2 shell thickness 40 nm (a), 60 nm (b), and 80 nm (c) with acceptor at d = 10 nm
from NP surface. Full calculations for two sets of donors and acceptors with their emission and
absorption bands tuned to dipole and high-l SP resonances are compared to independent donors
approximation.
FRET and of FRET from independent donors with increasing shell thickness show
opposite trends: the normalized cooperative FRET increases for thicker shells while
energy transfer from independent donors is reduced (see Fig. 15.17).
V. N. Pustovit and T. V. Shahbazyan
(a)
(b)
(c)
Fig. 15.17 FRET for N = 100 donors on top of spherical core-shell NP with Ag core radius
R c = 30 nm and SiO 2 shell thickness 40 nm (a), 60 nm (b), and 80 nm (c) with acceptor at d = 10 nm
from NP surface. Full calculations for two sets of donors and acceptors with their emission and
absorption bands tuned to dipole and high-l SP resonances are compared to independent donors
approximation.
FRET and of FRET from independent donors with increasing shell thickness show
opposite trends: the normalized cooperative FRET increases for thicker shells while
energy transfer from independent donors is reduced (see Fig. 15.17).
