ライフサイエンスコーパス: Rayleigh scattering

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