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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
5  first hyperpolarizabilities beta0 via hyper-Rayleigh scattering and Stark spectroscopy.
6  hyperpolarizabilities (as measured by hyper-Rayleigh scattering) and high affinities for biological
7                                 Using forced Rayleigh scattering, anomalous self-diffusion is observe
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
16                               We compute the Rayleigh scattering cross sections of the nanoparticles
17                            The laser-induced Rayleigh scattering defects were found to be stable from
18 ass of nanocouplers based on cavity enhanced Rayleigh scattering from nano-scatterer(s) on resonator
19 F has a depolarization close to 1, while its Rayleigh scattering has zero depolarization.
20        Measurement of beta by means of hyper-Rayleigh scattering (HRS) as well as their analysis usin
21 esponses have been determined by using hyper-Rayleigh scattering (HRS) at 1064 nm, and also via Stark
22                                    The hyper Rayleigh scattering (HRS) intensity increases 10 times a
23                                        Hyper-Rayleigh Scattering (HRS) measurements at 800 nm provide
24 eta of these chromophores, measured by hyper-Rayleigh scattering (HRS) relative to p-nitroaniline are
25                                        Hyper-Rayleigh scattering (HRS) studies confirmed that the fir
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
28                However, to date, the role of Rayleigh scattering in FMFs remains elusive.
29  experimentally validate a general model for Rayleigh scattering in FMFs.
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
32 e favorably with values reported from forced Rayleigh scattering measurements.
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.
35                                              Rayleigh scattering off a Bose-Einstein condensate was s
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
38           We find that the resolution of the Rayleigh scattering probe is adequate to detect nanopart
39                                              Rayleigh scattering, Raman scattering, and background fl
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
42               In single-mode optical fibers, Rayleigh scattering serves as the dominant mechanism for
43 quantized plasmon quenching dips in resonant Rayleigh scattering spectra by plasmon resonance energy
44                                              Rayleigh scattering spectra were obtained from individua
45 tubes by combining electron diffraction with Rayleigh scattering spectroscopy.
46                Despite the elastic nature of Rayleigh scattering, the feedback mechanism has been ins
47        Here we use the absolute intensity of Rayleigh scattering to show that single-walled carbon na
48        We also show that forward inter-modal Rayleigh scattering ultimately sets a fundamental limit
49                                           By Rayleigh scattering, we determined that 14S particles ar
50 ities beta have been measured by using hyper-Rayleigh scattering with an 800 nm laser, and Stark spec

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