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Rayleigh range

Figure 3. The phase lag produced by the Gouy phase, calculated using the analytic model described in the text for 0)3 + 3t0i excitation, with two additional coi photons in one of the channels. The calculations are performed for various ratios of the molecular beam radius d to the Rayleigh range zr. Figure 3. The phase lag produced by the Gouy phase, calculated using the analytic model described in the text for 0)3 + 3t0i excitation, with two additional coi photons in one of the channels. The calculations are performed for various ratios of the molecular beam radius d to the Rayleigh range zr.
Fig. 13.5. Femtosecond pulse loosely focused into water creates a long filament with a nearly constant diameter that extends over many Rayleigh ranges (left), and generates a broad supercontinuum spectrum (right). This seemingly stationary filament is created by a series of very dynamic multiple pulse splittings illustrated in the following... Fig. 13.5. Femtosecond pulse loosely focused into water creates a long filament with a nearly constant diameter that extends over many Rayleigh ranges (left), and generates a broad supercontinuum spectrum (right). This seemingly stationary filament is created by a series of very dynamic multiple pulse splittings illustrated in the following...
For self-similar particle size distributions, the average particle size can be determined directly by measuring the extinction. Total scattering in the Rayleigh range is... [Pg.140]

For particles smaller than the wavelength of light used, that is, for the Rayleigh range, the scattering intensity is a strong function of the diameter (sixth power), the wavelength (fourth power) and the complex refractive index ratio as described by the equation ... [Pg.216]

Figure 11.10 A plot of w(z) and the corresponding spatial dependence of the two-photon transition probability for an excitation wavelength of 800 nm and a minimum spot size of 1 pm. Approximately 82% of the two-photon absorption takes place within the Rayleigh range Zr about the focal point at Z = 0, leading to an effective focal volume of ca. 32 x 10 litres (32 fl)... Figure 11.10 A plot of w(z) and the corresponding spatial dependence of the two-photon transition probability for an excitation wavelength of 800 nm and a minimum spot size of 1 pm. Approximately 82% of the two-photon absorption takes place within the Rayleigh range Zr about the focal point at Z = 0, leading to an effective focal volume of ca. 32 x 10 litres (32 fl)...
Figure 11.11 A direct comparison between the spatial dependence of two- and single-photon absorption from a fluorescent probe in an isotropic solution contained in a cuvette and viewed at 90° to the excitation direction. Single-photon excitation at 488 nm produces fluorescence throughout the sample, whereas the restriction of two-photon fluorescence (excited at 800 nm) to the Rayleigh range around the laser focus is evident. The photographs were provided courtesy of Dr Mireille Blanchard-Desce (CNRS UMR 6510 Rennes)... Figure 11.11 A direct comparison between the spatial dependence of two- and single-photon absorption from a fluorescent probe in an isotropic solution contained in a cuvette and viewed at 90° to the excitation direction. Single-photon excitation at 488 nm produces fluorescence throughout the sample, whereas the restriction of two-photon fluorescence (excited at 800 nm) to the Rayleigh range around the laser focus is evident. The photographs were provided courtesy of Dr Mireille Blanchard-Desce (CNRS UMR 6510 Rennes)...

See other pages where Rayleigh range is mentioned: [Pg.317]    [Pg.155]    [Pg.158]    [Pg.85]    [Pg.274]    [Pg.147]    [Pg.140]    [Pg.141]    [Pg.142]    [Pg.476]    [Pg.481]    [Pg.481]    [Pg.625]    [Pg.180]    [Pg.124]    [Pg.2716]    [Pg.3]    [Pg.439]    [Pg.440]    [Pg.1639]    [Pg.181]    [Pg.226]    [Pg.260]    [Pg.260]    [Pg.363]    [Pg.1167]    [Pg.1168]    [Pg.269]    [Pg.269]    [Pg.270]    [Pg.270]    [Pg.86]   
See also in sourсe #XX -- [ Pg.3 ]

See also in sourсe #XX -- [ Pg.363 ]




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