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Spin order

The difference compared to equation B 1.13.2 or equation B 1.13.3 is the occurrence of the expectation value of the operator (the two-spin order), characterized by its own decay rate pjg and coupled to the one-spin longitudinal operators by the tenus 8j aud 5. We shall come back to the physical origin of these tenus below. [Pg.1502]

Many R, Vollenweider J-K and Fischer H 1988 Separation and analysis of CIDNP spin orders for a coupled multiproton system Chem. Rhys. 120 169-75... [Pg.1619]

Longitudinal spin order Extended Solomon equations... [Pg.99]

So far, we have not considered the so-called longitudinal two-spin order, represented by the product operator9 2J ff, a quantity related to the polarization of nuclei A and B. This spin state can be created in different ways. The easiest way is probably to let the system evolve under the sole Jab coupling so as to obtain an antiphase doublet, for instance the B antiphase doublet represented by 2//Vf (corresponding to the two proton-carbon-13 satellites in an antiphase configuration). [Pg.99]

Transfer of the initial proton polarization is not confined to other protons or 13C, but the signals of other heteronuclei (2H, 15N, 29Si, 31P) in the hydrogenation products can also become substantially enhanced, thereby also increasing their receptivity. Accordingly, the transfer of the PHIP-derived high spin order to 19F has been accomplished using a set of chemically similar fluorinated styrene and ethynylbenzene derivatives. [Pg.352]

Determinations of epr fine structure and paramagnetic susceptibilities are most often used. For characterization of higher spin orders, neutron diffraction and other physical methods may be useful. On the other hand, a successful measurement of normal high-resolution nmr spectra would serve as good evidence for singlet ground states of the chemical entities at issue. [Pg.201]

Table 5 Prescriptions for spin-ordered D/A charge-transfer salts."... Table 5 Prescriptions for spin-ordered D/A charge-transfer salts."...
As far as the size of the exchange integral J between the two open-shell centres is concerned, it can become as high as a few tenths of an eV in diradicals (see Section 3). The /-values between radicals are usually smaller than 0.01 eV. Therefore, we cannot readily expect spin-ordering temperatures higher than a few to 20 K for intermolecular spin alignment. [Pg.242]

While rather lengthy synthetic efforts may be necessary for constructing high-spin polyradicals, samples having intermolecular spin order can be prepared by a combination of rather simple components like appropriate donors and acceptors. [Pg.242]

It is relatively common for DFT calculations to not explicitly include electron spin, for the simple reason that this approximation makes calculations faster. In materials where spin effects may be important, however, it is crucial that spin is included. Fe, for example, is a metal that is well known for its magnetic properties. Figure 8.10 shows the energy of bulk Fe in the bcc crystal structure from calculations with no spin polarization and calculations with ferromagnetic spin ordering. The difference is striking electron spins lower the energy substantially and increase the predicted equilibrium lattice constant by 0.1 A. [Pg.188]

Sketch three spin orderings analogous to the one shown in Fig. 8.9d but with nonzero net magnetic moment. [Pg.191]

The DFT calculations shown in Fig. 8.10 are valid for bulk Fe at T 0 K. At temperatures above the so-called Curie temperature, Tc, Fe is no longer ferromagnetic because of thermal effects on the spin order. Find an appropriate reference that tells you what metals in the periodic table are ferromagnetic and what their Curie temperatures are. [Pg.191]

Fig. 6.8 Spin ordering in hematite above and below Tm (Coey, 1988, with permission). Fig. 6.8 Spin ordering in hematite above and below Tm (Coey, 1988, with permission).
Within the Zener approach, and its nuclear spin variant (Frohlich and Nabarro 1940), the degree of spin ordering, Mq, at given temperature T is found by minimizing the total free energy of the spin and carrier subsystems, F[Mq], Here Mq denotes the Fourier... [Pg.48]

Although the basic nature of the charge and associated spin order in cuprates and nickelates has now been fairly well been established, many questions concerning this order remain to be answered. One of our goals here was to elucidate some problems that are under discussion at present. Unquestionable, Raman scattering will continue to be an essential tools as we try to improve our understanding of stripe ordering and other complex correlation effects. [Pg.213]


See other pages where Spin order is mentioned: [Pg.1512]    [Pg.1512]    [Pg.89]    [Pg.83]    [Pg.225]    [Pg.229]    [Pg.205]    [Pg.206]    [Pg.226]    [Pg.242]    [Pg.18]    [Pg.54]    [Pg.99]    [Pg.188]    [Pg.189]    [Pg.68]    [Pg.69]    [Pg.85]    [Pg.105]    [Pg.381]    [Pg.620]    [Pg.84]    [Pg.193]    [Pg.50]    [Pg.276]    [Pg.253]    [Pg.76]    [Pg.76]    [Pg.207]    [Pg.230]    [Pg.144]    [Pg.144]    [Pg.269]   


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Spin ordering

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