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Amplitudes, correspondence

Yes, by filtering only the wave amplitude corresponding to 20 Hz can be measured, thus eliminating the noise. [Pg.954]

Yes, each detector will see only the wave amplitudes corresponding to 20 and 12 Hz. They will be sensitive to their signal only. [Pg.954]

Let < j(k) be the Klein-Gordon amplitude corresponding to a spin zero particle localized at the origin at time t = 0. Since in momentum space the space displacement operator is multiplication by exp (— tk a), the state localized at y at time t = 0 is given by exp (—ik-y) (k). This displaced state by condition (b) above must be orthogonal to (k), i.e. [Pg.501]

More generally, the configuration space amplitude corresponding to a particle localized at time y0 at the spatial point y is given by... [Pg.502]

We shall adopt Eqs. (9-510) and (9-511) as the covariant wave equation for the covariant four-vector amplitude 9ttf(a ) describing a photon. The physically realizable amplitudes correspond to positive frequency solutions of Eq. (9-510), which in addition satisfy the subsidiary condition (9-511). In other words the admissible wave functions satisfy... [Pg.552]

When two or more waves pass through the same region of space, the phenomenon of interference is observed as an increase or a decrease in the total amplitude of the wave (recall Fig. 1.20). Constructive interference, an increase in the total amplitude of the wave, occurs when the peaks of one wave coincide with the peaks of another wave. If the waves are electromagnetic radiation, the increased amplitude corresponds to an increased intensity of the radiation. Destructive interference, a decrease in the total amplitude of the waves, occurs when the peaks of one wave coincide with the troughs of the other wave it results in a reduction in intensity. [Pg.334]

The dissociation of 7 (Scheme 5) from poly[(G-C)] showed three relaxation times and the amplitude corresponded to the total signal, while the dissociation of 7 from poly[(A-T)] was faster and only two relaxation times, corresponding to 70% of the total signal were observed in the stopped-flow experiment. The biological activity of this class of molecules was correlated to the presence of four relaxation times when the dissociation process is measured with DNA, in particular the presence of the long-lived component of hundreds of milliseconds.86,104 105,132 143 The difference in the dissociation kinetics observed with the two polydeoxynucleotides indicates that intercalation into G-C sites is responsible for the biological activity. The dissociation of 7 from ct-DNA led to four relaxation times, a result that is in line with the relaxation times observed with poly[(G-C)] and poly[(A-T)]. [Pg.195]

Turning now back to the single-root MR BWCC approach, we derive the basic equations for the effective Hamiltonian and cluster amplitudes in the spin-orbital form without the use of the BCH formula. We limit ourselves to a complete model space which implies that amplitudes corresponding to internal excitations (i.e. excitations within the model space) are equal to zero. In our derivation we shall work with the Hamiltonian in the normal-ordered-product form, i.e. [Pg.85]

Using time-resolved crystallographic experiments, molecular structure is eventually linked to kinetics in an elegant fashion. The experiments are of the pump-probe type. Preferentially, the reaction is initiated by an intense laser flash impinging on the crystal and the structure is probed a time delay. At, later by the x-ray pulse. Time-dependent data sets need to be measured at increasing time delays to probe the entire reaction. A time series of structure factor amplitudes, IF, , is obtained, where the measured amplitudes correspond to a vectorial sum of structure factors of all intermediate states, with time-dependent fractional occupancies of these states as coefficients in the summation. Difference electron densities are typically obtained from the time series of structure factor amplitudes using the difference Fourier approximation (Henderson and Moffatt 1971). Difference maps are correct representations of the electron density distribution. The linear relation to concentration of states is restored in these maps. To calculate difference maps, a data set is also collected in the dark as a reference. Structure factor amplitudes from the dark data set, IFqI, are subtracted from those of the time-dependent data sets, IF,I, to get difference structure factor amplitudes, AF,. Using phases from the known, precise reference model (i.e., the structure in the absence of the photoreaction, which may be determined from... [Pg.11]

The amplitude of the main-chain angular changes is directly related to the activation energy value a larger amplitude corresponds to a higher activation energy. [Pg.178]

Because step 3 will be discussed in great detail in the sections below, it is appropriate to provide a brief summary of how it was discovered, using the T7 DNA polymerase as an example (Donlin et al, 1991 Patel et al., 1991 Wong et al., 1991). The rate-limiting step was observed when the dependence of the burst amplitude (corresponding to the incorporation of the first nucleotide) on nucleotide concentration was examined. This experiment provided kpol of step 3 (Fig. 1), which was lower than all the other... [Pg.407]

In this section we investigate the factors affecting the formation and decay of shape resonances by examining the radial charge density /120/ plots from the Feynman Dyson amplitudes corresponding to the resonant poles identified earlier /22,25,26,40,41/ in sections 3.1 and 3.2 for different atomic and molecular resonances. [Pg.267]

The electron and its charge can hence be identified with a local maximum in the radiation field, embedded in a sea of virtual photons. The amplitude corresponds to the electric potential of the electron and significantly does not become infinite as r — 0, but approaches 4>0. The interference between divergent and convergent waves therefore achieves the same, and more, as renormalization in field theory. [Pg.127]

The first way we have examined the ( -(- 2)s ( , 3) transitions, by varying the microwave field amplitude, corresponds to how we measured the microwave ionization threshold fields, a process explained by a single cycle Landau-Zener description. As noted above, the same (n -t- 2)s ( , 3) transitions can also be... [Pg.135]

To analyze the advantages and drawbacks of each test comparatively, two sets of calibration functions were created. The first one is derived from four functions, representing different levels of stationarity. In each of these cases, three levels of random white noise are added with different amplitudes corresponding to 1, 5 and 10% standard deviations, of the original data. This set of functions is presented in Fig. 1. [Pg.461]

A — —8/2 and A — —38/2. Paths (a) and (b) (constructed with delayed pulses of the same length and peak amplitude) correspond respectively to the intuitive and counterintuitive pulse sequences in A or ladder systems (for which the initial population resides in state 1)). [Pg.229]

Figure 10. Surfaces of eigen-energies (in units of 8) as functions of QP/8 and Us/8 for the case /.] < >.2 < -3, with Ap = 8/2 and As = — 8/2. Paths (a) and (b) (with pulses of the same length and peak amplitude) correspond respectively to the intuitive (transfer to 2)) and counterintuitive (transfer to 13)) pulse sequences in A or ladder systems leading to the selective transfer. Paths (a) and (c) correspond to the selective transfer in V systems (for which the initial population resides in 12)), respectively to 11) and 3). Figure 10. Surfaces of eigen-energies (in units of 8) as functions of QP/8 and Us/8 for the case /.] < >.2 < -3, with Ap = 8/2 and As = — 8/2. Paths (a) and (b) (with pulses of the same length and peak amplitude) correspond respectively to the intuitive (transfer to 2)) and counterintuitive (transfer to 13)) pulse sequences in A or ladder systems leading to the selective transfer. Paths (a) and (c) correspond to the selective transfer in V systems (for which the initial population resides in 12)), respectively to 11) and 3).
Notice that we have said nothing about the amplitude of the oscillation. There really is no amplitude variable in our system. If we had an amplitude as well as a phase variable, we d be in a two-dimensional phase space this situation is more complicated and will be discussed later in the book. (Or if you prefer, you can imagine that the oscillation occurs at some fixed amplitude, corresponding to the radius of our circular phase space. In any case, amplitude plays no role in the dynamics.)... [Pg.95]

The warmest month of the year is July with a mean monthly temperature of about 24 Tl whereas January is the coldest with a mean monthly temperature of about 3 "C. An annual mean temperature variation of about 28 °C is estimated, which classifies Iasi as a region with very a high thermic amplitude corresponding to a severe continental climate. During winter and summer a small difference of the air temperature is observed from one month to another... [Pg.370]


See other pages where Amplitudes, correspondence is mentioned: [Pg.792]    [Pg.449]    [Pg.384]    [Pg.114]    [Pg.117]    [Pg.155]    [Pg.288]    [Pg.128]    [Pg.131]    [Pg.3]    [Pg.86]    [Pg.55]    [Pg.32]    [Pg.522]    [Pg.343]    [Pg.59]    [Pg.372]    [Pg.220]    [Pg.860]    [Pg.233]    [Pg.232]    [Pg.12]    [Pg.198]    [Pg.159]    [Pg.185]    [Pg.462]    [Pg.117]    [Pg.198]    [Pg.277]    [Pg.453]   


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