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Signal Lorentz

The condition for a time-like difference vector is equivalent to stating that it is possible to bridge the distance between the two events by a light signal, while if the points are separated by a space-like difference vector, they cannot be connected by any wave travelling with the speed c. If the spatial difference vector r i — r2 is along the z axis, such that In — r2 = z — z2, under a Lorentz transformation with velocity v parallel to the z axis, the fourth component of transforms as... [Pg.147]

Use the same series of data and follow the same procedure as before to try out the Lorentz-Gauss convert window type. There is one single parameter LB available to adjust the window. Set the initial value to LB = 0, increment and decrement its value in small steps and inspect the shape of the window using the interactive mode. Note that for LB > 0 the shape of the window is similar to the exponential window (signal-to-noise improvement) whereas for LB < 0 the window shape is similar to the sine-bell squared window. Try out a few values to enhance the signal-to-noise ratio and to improve the resolution, store the results and compare the spectra using the multiple display. [Pg.179]

Curves 2 (Ei E) and 5 (Ei L E) in Fig. 4.15 refer to the uoj Jj/T 1 scale, in which the excited state Hanle effect manifests itself (the ground state Hanle effect is already fully developed and does not manifest itself in this scale). The signal is of Lorentz shape ... [Pg.131]

Lorentz curves with a tail function for the asymmetry of the XPS signals for these transition elements. These sets were kept constant in position, shape and size relative to each other. The XPS spectrum of an actual specimen was described with a least-square fit by variation of the size of the appropriate standard sets [36]. Various standards were prepared and measured for a subsequent data analysis of actual specimens. Only some few examples are mentioned here. Pure metal standards are Ar-sputter cleaned specimens. Fe(III) oxide corresponds to a thick passive layer formed at the positive end of the passive range. For Fe(II), a passive layer formed on Fe5Cr is reduced in 1 M NaOH at ca. = -1.0 V (SHE) [12]. For NiO, oxide grown at 1000 °C on pure Ni in air was used as a standard. For Ni(III)oxyhydroxide, NiOOH was deposited by oxidation of Ni2+ from weakly alkaline solution or formed... [Pg.299]

However, the theory with CPT and Lorentz violation involves spatial components in a celestial frame of reference, and since the laboratory rotates with the earth, these spatial components vary with time, and consequently the experimentally observed 1/42 and P34 may oscillate about a mean value at the earth s sidereal frequency fi = 27t/23 hr 56 rn with amplitudes 81/42 and 81/34. No such signal would be obtained from the standard model. In the non-rotating celestial frame of reference with equatorial axes x, Y,Z where Z is oriented along the earth s rotational North Pole, an experimental constraint on 81/12 implies [4]... [Pg.399]

Figure 4. Schematic arrangement of the TRACER balloon instrument. The nuclear charge Z of traversing cosmic-ray nuclei is determined with plastic scintillators. An acrylic Cherenkov counter determines their Lorentz factor 7 at low energies, and arrays of single-wire proportional tubes measure 7 from the relativistic rise in specific ionization, and from transition radiation signals. Figure 4. Schematic arrangement of the TRACER balloon instrument. The nuclear charge Z of traversing cosmic-ray nuclei is determined with plastic scintillators. An acrylic Cherenkov counter determines their Lorentz factor 7 at low energies, and arrays of single-wire proportional tubes measure 7 from the relativistic rise in specific ionization, and from transition radiation signals.
The third-order nonlinear optical susceptibility x was obtained by comparing the measured signals for the sample with that of carbon disulfide as reference under the same experimental condition. The measured x value is 6.2 x 10 esu for the subphthalocyanine at a concentration 1.25 x 10 M. Considering an isotropic media under the Lorenz-Lorentz approximation, the second hyperpolarizability value was found to be 3.0 x 10 esu. Furthermore, A pirc corresponding to the pure subphthalocyanine 17 was calculated to be 6.9 x 10 esu, about four times higher... [Pg.526]

S(co) is called a complex Lorentz line. Its real and imaginary parts, A(co) and D (o), denote the absorption signal and the dispersion signal, respectively (Fig. 2.2.6) ... [Pg.34]

In general, one might consider the influence of the induced adiabatic vector potential on the mean values of the coordinates, q, these of course directly affect the value of the interference signal. In the 2 = 0 case to which we have specialized, however, the transverse vector potential has vanishing curl except at the origin and therefore does not exert a Lorentz force. For that reason, the effect of in the z = 0 case has been likened to the Aharonov-Bohm effect [1]. In contrast, the repulsive inverse-cubed force arising from the (Aj + A )/2M term will always affect q, through its presence in and... [Pg.17]

Apodization is the process of multiplying the FID prior to Fourier transformation by a mathematical function. The type of mathematical or window function applied depends upon the enhancement required the signal-to-noise ratio in a spectrum can be improved by applying an exponential window function to a noisy FID whilst the resolution can be improved by reducing the signal linewidth using a Lorentz-Gauss function. ID WIN-NMR has a variety of window functions, abbreviated to wdw function, such as exponential (EM), shifted sine-bell (SINE) and sine-bell squared (QSINE). Each window function has its own particular parameters associated with it LB for EM function, SSB for sine functions etc. [Pg.76]

Attempts have been made to simulate the X-ray signal of the ACP in plasma-sprayed hydroxyapatite coatings by a Lorentz function added to the Rietveld refinement algorithm (Hesse et al., 2008). This provides a reasonable fit of the... [Pg.313]

To understand the information conveyed by an ICR signal, one has to solve the equation of motion of an ion under ICR conditions. The effect of collisions on the energy absorption of ions in the ICR cell is described by the Lorentz equation with the inclusion of a term for collisional damping ... [Pg.68]


See other pages where Signal Lorentz is mentioned: [Pg.133]    [Pg.133]    [Pg.733]    [Pg.165]    [Pg.65]    [Pg.74]    [Pg.2]    [Pg.59]    [Pg.290]    [Pg.176]    [Pg.179]    [Pg.144]    [Pg.248]    [Pg.118]    [Pg.118]    [Pg.13]    [Pg.109]    [Pg.273]    [Pg.91]    [Pg.305]    [Pg.48]    [Pg.59]    [Pg.316]    [Pg.71]    [Pg.173]    [Pg.207]    [Pg.211]    [Pg.179]    [Pg.363]    [Pg.366]    [Pg.165]    [Pg.76]    [Pg.162]    [Pg.56]    [Pg.147]    [Pg.159]    [Pg.414]   
See also in sourсe #XX -- [ Pg.76 ]




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