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1 n absorption, ORF emission, RRS, and solvent Rayleigh scattering.
2 en near-field SERS enhancement and far-field Rayleigh scattering.
3 y means of Infrared Thermal Diffusion Forced Rayleigh Scattering.
4 olarizabilities beta(0) determined via hyper-Rayleigh scattering and Stark spectroscopy maximize at n
6 hyperpolarizabilities (as measured by hyper-Rayleigh scattering) and high affinities for biological
8 measured in isotropic solution through hyper-Rayleigh scattering as well as estimated from theoretica
9 ses beta have been determined by using hyper-Rayleigh scattering at 800 and 1064 nm and also via Star
10 ses beta have been determined by using hyper-Rayleigh scattering at 800 nm and also via Stark (electr
11 ses beta have been determined by using hyper-Rayleigh scattering at 800 nm and also via Stark (electr
12 e been determined by using femtosecond hyper-Rayleigh scattering at 880 and 800 nm, and depolarizatio
13 Cos(2) theta dependence, as is the case for Rayleigh scattering, but instead scatter light in an inc
14 e report a theoretical analysis showing that Rayleigh scattering could be used to monitor the growth
15 method were demonstrated for quantifying the Rayleigh scattering cross sections of solvents including
18 ass of nanocouplers based on cavity enhanced Rayleigh scattering from nano-scatterer(s) on resonator
21 esponses have been determined by using hyper-Rayleigh scattering (HRS) at 1064 nm, and also via Stark
24 eta of these chromophores, measured by hyper-Rayleigh scattering (HRS) relative to p-nitroaniline are
26 ies beta have been determined by using hyper-Rayleigh scattering (HRS) with an 800 nm laser and also
27 S(-2omega;omega,omega), as measured by Hyper-Rayleigh Scattering (HRS), when corrected to zero-freque
30 ts of guiding light in air derive from lower Rayleigh scattering, lower nonlinearity and lower transm
31 raction measurements of the chiral index and Rayleigh scattering measurements of the optical resonanc
33 ission electron microscopy (TEM), dark-field Rayleigh scattering microscopy, surface-enhanced Raman s
34 all-size atmospheric plasma objects based on Rayleigh scattering of microwaves on the plasma volume.
36 where the feedback is provided by amplified Rayleigh scattering on sub-micron refractive index inhom
37 tic excitation, below the (multiple) Compton/Rayleigh scattering peak region, the XRF spectra obtaine
40 n behavior and to characterize, via absolute Rayleigh scattering ratios, their molecular masses and s
41 n-resonance fluorescence (ORF) and resonance Rayleigh scattering (RRS) is limited and often problemat
43 quantized plasmon quenching dips in resonant Rayleigh scattering spectra by plasmon resonance energy
50 ities beta have been measured by using hyper-Rayleigh scattering with an 800 nm laser, and Stark spec
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