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Frequency irradiating

Many other pulsed NMR experiments are possible, and some are listed in the final sections. Most can be canied out using the standard equipment described above, but some require additions such as highly controllable, pulsed field gradients, shaped RF pulses for (for example) single-frequency irradiations, and the combined use of pulses at several different frequencies. [Pg.1441]

Overall, it can be summarized that, use of multiple frequency irradiations based on the use of multiple transducers gives much higher cavitational activity in the reactor and hence enhanced results. It is also recommended that a combination of low frequency irradiation (typically 20 kHz) with other frequencies in the range of 50-200 kHz should be used for obtaining maximum benefits from the cavitational reactors. [Pg.52]

Within its orbit, which has some of the characteristics of a molecular orbital because it is shared with electrons on the surrounding atoms, the electron has two possible spin multiplicity states. These have different energies, and because of the spin-multiplicity rule, when an (N-V) center emits a photon, the transition is allowed from one of these and forbidden from the other. Moreover, the electron can be flipped from one state to another by using low-energy radio-frequency irradiation. Irradiation with an appropriate laser wavelength will excite the electron and as it returns to the ground state will emit fluorescent radiation. The intensity of the emitted photon beam will depend upon the spin state, which can be changed at will by radio-frequency input. These color centers are under active exploration for use as components for the realization of quantum computers. [Pg.438]

An alternating magnetic field Bl with frequency irradiating an ensemble of nuclear spins precessing in the static field B0 may overcome the energy difference AE if it meets two conditions The vector of the alternating field B1 must rotate in the plane of precession with the Larmor frequency v0 of the nuclei to be observed (Fig. 1.4(a)). [Pg.4]

Two-frequency irradiation of a two-level atom was proposed by Pomeau et al. (1986). As compared with one-frequency irradiation, a rapid decay of correlations, indicative of true quantum chaos, was observed. However, for the particular choice of parameters in the paper by Pomeau et al. (1986), Badii and Meier (1987) were able to demonstrate that the response is not chaotic, but quasi-periodic, albeit on a very long time... [Pg.196]

The transmitter offset describes the location of the observation frequency and is closely related to the spectral width. With quadrature phase detection of sample signals (Section 5-8), the frequency of the transmitter is positioned in the middle of the spectral width. In so doing, the operator has the best chance of irradiating, with equal intensity, those nuclei whose resonances are both close to and far from the transmitter frequency. Irradiation is not a problem for protons, with their small chemical shift range, but it can be for nuclei with large chemical shift ranges (Chapter 3). [Pg.43]

In principle, NMR utilizes the atomic nuclear transition, induced by radio frequency irradiation, between two quantized nuclear energy levels in a magnetic... [Pg.137]

Thus, it can be said that multiple-transducer and/or multiple-frequency irradiation also results in an enhancement in the cavitational yield and these types of reactors should play a key role in the design of industrial-scale reactors. Another key feature of the flow cells is the possibility of continuous operation, which is another key requirement for the industrial-scale operation. [Pg.256]

This relatively straightforward resonant excitation process is complicated somewhat in a stretched ion trap (see above). Since ion axial secular frequencies increase as an ion approaches an end cap electrode, it is necessary to adopt one of several strategies to maintain resonance and thus ion excitation. There are three such methods of resonant excitation of ions of a selected miz value isolated within an ion trap, namely, single frequency irradiation (SFI), secular frequency modulation (SFM) and multifrequency irradiation (MFI). [Pg.299]

In contrast, MFI involves the application of a resonant excitation waveform consisting of several frequency components while the value of is held constant. The frequency components of the waveform bracket the entire anticipated range of the secular frequency so as to compensate for frequency shifts. Other variants of multi-frequency irradiation (March 1998) include random noise, swept frequency and broadband excitation. A rather different ion activation method (Paradisi 1992, 1992a Curcuruto 1992) is accessible with ion trap instruments equipped with a DC power supply so that non-zero values of U and thus a are available. The method involves moving the working point of a given ion species to either the P,. or the p, boundary of the stability diagram... [Pg.299]

Figure 6.25 Scan function for MS spectrum of the molecular ions of tetrachlorodibenzodioxin (TCDD, or dioxin ) m/z 320 and 320 correspond to the Cl4 and Cl3 Cli isotopologs, respectively. MFI refers to resonance activation using multi-frequency irradiation. The pre-scan for AGC is not shown. Reproduced from March, J. Mass Spectrom. 32, 351 (1997), with permission of John Wiley Sons, Ltd. Figure 6.25 Scan function for MS spectrum of the molecular ions of tetrachlorodibenzodioxin (TCDD, or dioxin ) m/z 320 and 320 correspond to the Cl4 and Cl3 Cli isotopologs, respectively. MFI refers to resonance activation using multi-frequency irradiation. The pre-scan for AGC is not shown. Reproduced from March, J. Mass Spectrom. 32, 351 (1997), with permission of John Wiley Sons, Ltd.
High-power, low-frequency waves are often associated with better mechanical treatment and less importantly with chemical effects. This rule, however, suffers exceptions, and sonochemical switchings can be observed, even in solutions, under low-frequency irradiation. A heterogeneous reaction with a metal was also reported to be improved by the use of a high-frequency irradiation. ... [Pg.303]

Fig. 2.33. Carbon-13 spectra of suvanine (25) in DMSO-dg. a Broad-band proton decoupling b DEPT spectra (0 = 135) with broad-band proton decoupling c selective INEPT sequence with single frequency irradiation of 6H singlet at = 2.94 (-NMe2) (251). (L. V. Manes, P. Crews, MR. Kernan, D.J. Faulkner, F.R. Fronczek, R.D. Candour 1988 J. Org. Chem. S3, 570)... Fig. 2.33. Carbon-13 spectra of suvanine (25) in DMSO-dg. a Broad-band proton decoupling b DEPT spectra (0 = 135) with broad-band proton decoupling c selective INEPT sequence with single frequency irradiation of 6H singlet at = 2.94 (-NMe2) (251). (L. V. Manes, P. Crews, MR. Kernan, D.J. Faulkner, F.R. Fronczek, R.D. Candour 1988 J. Org. Chem. S3, 570)...
Dielectric polarizability depends on the facility of a material to polarize in response to electric fields it is expressed by the permittivity e which, generally speaking, represents a measure of the resistance that is encountered in the dipole or charge reorganization. In fact, the permittivity (resistivity) will almost always be dependent on the frequency of the applied field and on the viscosity of the reactive environment to some extent, thus it has the form of a complex value. When the frequency irradiation is low, dipole/charges re-orientation is regularly in phase with the applied field coherently re-displacing themselves alternatively in the field... [Pg.426]


See other pages where Frequency irradiating is mentioned: [Pg.290]    [Pg.42]    [Pg.11]    [Pg.311]    [Pg.279]    [Pg.202]    [Pg.786]    [Pg.112]    [Pg.31]    [Pg.51]    [Pg.546]    [Pg.98]    [Pg.183]    [Pg.197]    [Pg.358]    [Pg.6]    [Pg.51]    [Pg.6336]    [Pg.270]    [Pg.30]    [Pg.850]    [Pg.252]    [Pg.383]    [Pg.5266]    [Pg.371]    [Pg.221]    [Pg.482]    [Pg.138]    [Pg.16]    [Pg.97]   
See also in sourсe #XX -- [ Pg.191 ]

See also in sourсe #XX -- [ Pg.191 ]

See also in sourсe #XX -- [ Pg.191 ]




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