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Wavelengths in vacuum

Thus, for electromagnetic radiation of frequency, V, the wavelength in vacuum is longer than in other media. Another unit used to describe the wave properties of electromagnetic radiation is the wavenumber, V, which is the reciprocal of wavelength... [Pg.370]

Note that the wavelength in vacuum has been replaced by the wavelength in the medium, since it is the latter that drives the oscillations in the fluctuation domain. Now what can we say about 6a ... [Pg.680]

Meter (metre) (preferred spelling in U.S. is meter) m 1650763.73 wavelengths in vacuum of the orange-red line of the spectrum of krypton-86... [Pg.970]

After the corrections for the pressure shifts Torii et al. [18] obtained wavelengths in vacuum, which revealed a small discrepancies of several ppm, as shown in Fig. 6. The theoretical values are further corrected for QED effects [9,19,20], yielding excellent agreements to ppm precision. Various QED corrections calculated by Korobov [21] are itemized in Table 1. [Pg.252]

In a transparent medium, /cabs = 0, a plane wave has the form e"Cabs reix where Kabs = (2n /lo), where X0 is the wavelength in vacuum. [Pg.250]

Refractive index is defined as the ratio of the speed of light of a given wavelength in vacuum to the speed of light at the same wavelength in the substance measured. The refractive index of epoxy resins is seldom reported. However, the property is important for cured epoxy adhesives that are used in the assembly of optical devices. [Pg.442]

Here fj(k) is the field amplitude of the light scattered by particle j with its center of mass at the position ry, Nis the number of particles in the scattering volume, K = K/ — K is the transferred momentum, and k = K. For elastic scattering K, = K/ = 2tuis/2q, where is the incident light wavelength in vacuum. Thus,... [Pg.22]

The meter is the length equal to 1650763.73 wavelengths in vacuum of the radiation corresponding to the transition between the levels 2p10 and 5ds of the krypton-86 atom. [Pg.779]

Figure 4. Dependences of the extinction A of gold bispheres in water on the number of multipoles included in the single-particle expansions. Calculations by the T-matrix method for randomly oriented bispheres with touching component spheres (hd = 0 ) and those separated by distances hd = 0.5 nm and hd = 1 nm. Particle diameter equals d = 5 nm the wavelength in vacuum equals A = 515 nm (a) and 550 nm (b). Figure 4. Dependences of the extinction A of gold bispheres in water on the number of multipoles included in the single-particle expansions. Calculations by the T-matrix method for randomly oriented bispheres with touching component spheres (hd = 0 ) and those separated by distances hd = 0.5 nm and hd = 1 nm. Particle diameter equals d = 5 nm the wavelength in vacuum equals A = 515 nm (a) and 550 nm (b).

See other pages where Wavelengths in vacuum is mentioned: [Pg.1385]    [Pg.1388]    [Pg.650]    [Pg.126]    [Pg.147]    [Pg.106]    [Pg.169]    [Pg.400]    [Pg.1644]    [Pg.2]    [Pg.76]    [Pg.106]    [Pg.60]    [Pg.72]    [Pg.394]    [Pg.17]    [Pg.204]    [Pg.251]    [Pg.381]    [Pg.23]    [Pg.37]    [Pg.104]    [Pg.111]    [Pg.170]    [Pg.85]    [Pg.110]    [Pg.563]    [Pg.703]    [Pg.129]    [Pg.2]    [Pg.1385]    [Pg.1388]    [Pg.12]    [Pg.713]    [Pg.962]    [Pg.280]    [Pg.565]    [Pg.176]    [Pg.77]   
See also in sourсe #XX -- [ Pg.7 , Pg.441 , Pg.620 ]




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Vacuum wavelengths

Wavelength of light in vacuum

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