ライフサイエンスコーパス: Rayleigh scattering

1 y means of Infrared Thermal Diffusion Forced Rayleigh Scattering.

2 n absorption, ORF emission, RRS, and solvent Rayleigh scattering.

3 en near-field SERS enhancement and far-field Rayleigh scattering.

4 ither an external magnetic field or coherent Rayleigh scattering.

5 olarizabilities beta(0) determined via hyper-Rayleigh scattering and Stark spectroscopy maximize at n

6 first hyperpolarizabilities beta0 via hyper-Rayleigh scattering and Stark spectroscopy.

7 hyperpolarizabilities (as measured by hyper-Rayleigh scattering) and high affinities for biological

8 s when free atoms scatter light elastically (Rayleigh scattering) and the final external momentum sta

9 Using forced Rayleigh scattering, anomalous self-diffusion is observe

10 Rayleigh scattering, arising from frozen-in density fluc

11 measured in isotropic solution through hyper-Rayleigh scattering as well as estimated from theoretica

12 ses beta have been determined by using hyper-Rayleigh scattering at 800 and 1064 nm and also via Star

13 ses beta have been determined by using hyper-Rayleigh scattering at 800 nm and also via Stark (electr

14 ses beta have been determined by using hyper-Rayleigh scattering at 800 nm and also via Stark (electr

15 e been determined by using femtosecond hyper-Rayleigh scattering at 880 and 800 nm, and depolarizatio

16 Cos(2) theta dependence, as is the case for Rayleigh scattering, but instead scatter light in an inc

17 d using femtosecond laser-induced artificial Rayleigh scattering centers in single-mode fiber cores.

18 rms of both chiral indices and handedness by Rayleigh scattering circular dichroism.

19 d is based on the background-free feature of Rayleigh scattering collected at an oblique angle, which

20 Rayleigh scattering, Compton scattering, photo-electric

21 e report a theoretical analysis showing that Rayleigh scattering could be used to monitor the growth

22 method were demonstrated for quantifying the Rayleigh scattering cross sections of solvents including

23 We compute the Rayleigh scattering cross sections of the nanoparticles

24 The laser-induced Rayleigh scattering defects were found to be stable from

25 ass of nanocouplers based on cavity enhanced Rayleigh scattering from nano-scatterer(s) on resonator

26 F has a depolarization close to 1, while its Rayleigh scattering has zero depolarization.

27 Measurement of beta by means of hyper-Rayleigh scattering (HRS) as well as their analysis usin

28 esponses have been determined by using hyper-Rayleigh scattering (HRS) at 1064 nm, and also via Stark

29 This work combines hyper-Rayleigh scattering (HRS) experiments performed in the N

30 The hyper Rayleigh scattering (HRS) intensity increases 10 times a

31 Hyper-Rayleigh Scattering (HRS) measurements at 800 nm provide

32 eta of these chromophores, measured by hyper-Rayleigh scattering (HRS) relative to p-nitroaniline are

33 Their hyper-Rayleigh scattering (HRS) responses in solution were acc

34 Hyper-Rayleigh scattering (HRS) studies confirmed that the fir

35 ies beta have been determined by using hyper-Rayleigh scattering (HRS) with an 800 nm laser and also

36 S(-2omega;omega,omega), as measured by Hyper-Rayleigh Scattering (HRS), when corrected to zero-freque

37 However, to date, the role of Rayleigh scattering in FMFs remains elusive.

38 experimentally validate a general model for Rayleigh scattering in FMFs.

39 Their lower than Rayleigh scattering loss in an air-guiding structure off

40 ts of guiding light in air derive from lower Rayleigh scattering, lower nonlinearity and lower transm

41 raction measurements of the chiral index and Rayleigh scattering measurements of the optical resonanc

42 e favorably with values reported from forced Rayleigh scattering measurements.

43 ission electron microscopy (TEM), dark-field Rayleigh scattering microscopy, surface-enhanced Raman s

44 all-size atmospheric plasma objects based on Rayleigh scattering of microwaves on the plasma volume.

45 Here we report the non-resonant Rayleigh scattering of various molecules in liquid phase

46 Rayleigh scattering off a Bose-Einstein condensate was s

47 where the feedback is provided by amplified Rayleigh scattering on sub-micron refractive index inhom

48 ibre cavity ring down spectroscopy probed by Rayleigh scattering optical frequency domain reflectomet

49 tic excitation, below the (multiple) Compton/Rayleigh scattering peak region, the XRF spectra obtaine

50 We find that the resolution of the Rayleigh scattering probe is adequate to detect nanopart

51 Rayleigh scattering, Raman scattering, and background fl

52 ures, where atoms scatter at the single-atom Rayleigh scattering rate.

53 n behavior and to characterize, via absolute Rayleigh scattering ratios, their molecular masses and s

54 n-resonance fluorescence (ORF) and resonance Rayleigh scattering (RRS) is limited and often problemat

55 In single-mode optical fibers, Rayleigh scattering serves as the dominant mechanism for

56 quantized plasmon quenching dips in resonant Rayleigh scattering spectra by plasmon resonance energy

57 Rayleigh scattering spectra were obtained from individua

58 tubes by combining electron diffraction with Rayleigh scattering spectroscopy.

59 Despite the elastic nature of Rayleigh scattering, the feedback mechanism has been ins

60 h evidences the signal-building mechanism of Rayleigh scattering theory.

61 Here we use the absolute intensity of Rayleigh scattering to show that single-walled carbon na

62 We also show that forward inter-modal Rayleigh scattering ultimately sets a fundamental limit

63 By Rayleigh scattering, we determined that 14S particles ar

64 ities beta have been measured by using hyper-Rayleigh scattering with an 800 nm laser, and Stark spec