Spin direction

Figure Bl.13.2. Spin-lattice and spin-spm relaxation rates (R and/ 2> respectively) for a carbon-13 spin directly bonded to a proton as a fiinction of correlation time at the magnetic fields of 7 and 14 T.

A second type of relaxation mechanism, the spin-spm relaxation, will cause a decay of the phase coherence of the spin motion introduced by the coherent excitation of tire spins by the MW radiation. The mechanism involves slight perturbations of the Lannor frequency by stochastically fluctuating magnetic dipoles, for example those arising from nearby magnetic nuclei. Due to the randomization of spin directions and the concomitant loss of phase coherence, the spin system approaches a state of maximum entropy. The spin-spin relaxation disturbing the phase coherence is characterized by T. ... [Pg.1552]

H = di(Z—iy di are the potential parameters I is the orbital quantum number 3 characterizes the spin direction Z is the nuclear charge). Our experience has show / that such a model potential is convenient to use for calculating physical characteristics of metals with a well know electronic structure. In this case, by fitting the parameters di, one reconstructs the electron spectrum estimated ab initio with is used for further calculations. [Pg.142]

Work on intermolecular energy transfer at low temperature from a donor (D) to an acceptor (A) has indicated that if a donor is prepared such that its triplet state has a unique spin direction, the acceptor will also have a unique and predictable direction when both donor and acceptor are oriented in a single crystal. 27 ... [Pg.444]

Spinning Direction of Bobbin Same for Primary and Secondary Windings... [Pg.251]

The configurational entropy evaluated above omits all mention of electron spin. Because there are two spin directions, a spin degeneracy of 2, these must be included in the possible configurations. When this term is included, the Heikes equation becomes the Chaikin-Beni equation ... [Pg.470]

Beside intra- and interresidue 13C nuclei, the magnetization can be transferred from the 15N spin directly to the 13C nuclei of the preceding... [Pg.255]

In 1925, an Austrian physicist, Wolfgang Pauli, proposed that only two electrons of opposite spin could occupy an orbital. This proposal became known as the Pauli exclusion principle. What the exclusion principle does is place a limit on the total number of electrons that may occupy any orbital. That is, an orbital may have a maximum of two electrons only, each of which must have the opposite spin direction of the other. It may also have only one electron of either spin direction. An orbital may also have no electrons at all. [Pg.140]

From the few examples of electron configurations that you have seen so far, you may have noticed that they do not include information about the spin direction of the electron. Once you have considered the electron configurations for a variety of atoms, you will see that you can safely infer where electrons with opposite spins have been paired together. [Pg.143]

Fig. 2.2 A 7i/2-flipper effecively rotating the spin direction from longitudinal (S) to perpendicular to the path and to the external field. The vertical field B /2 generated inside the flipper adds to the embedding external field...

Uranyl is formed due to o and n bonds of 5/, 6d, 7s electrons of the uranium atom and 2p electrons of two oxygen atoms. Molecular orbitals of uranyl are formed by the interaction of atomic orbitals of uraniiun and oxygen with the same type ofsymmetry and close energy levels. Bonding orbitals la , lag, l7r , iTTg are filled with electrons with antiparallel spin directions. Nonbonding orbitals la, la. In, In and so on are empty and form excitation levels. The... [Pg.229]

Below the Curie temperature Tc, the B-site moments are ferromagnetically coupled, and the mobile-electron spins on the B sites are coupled antiparallel to the B-site majority-spin direction, but parallel to the A-site majority-spin direction. Therefore, below T ... [Pg.14]

The density of states per unit energy range and per unit volume, for given spin direction, is written N(E), where E denotes the energy. Thus from (2), setting 2=1 cm3, we can write... [Pg.6]

The successes of the free-electron model came from combining it with Fermi-Dirac statistics, according to which the number of electrons in each orbital state cannot be greater than two, one for each spin direction. Thus at the absolute zero of temperature all states are occupied up to a maximum energy F given by... [Pg.6]

N0 being defined for a given spin direction. Expanding (22), we find, for small n,... [Pg.100]

Fig. 3.8 Density of states in a magnetic impurity for two spin directions.

Here U is the intra-atomic interaction defined in Chapter 4 and t, the hopping integral, is equal to B/2z, where B is the bandwidth and z is the coordination number. The suffixes i and j refer to the nearest-neighbour sites, and aia is the creation operator for site i. The suffix a refers to the spin direction. Hubbard found that a metal-insulator transition should occur when B/U = 1.15. Hubbard s analysis did not include long-range interactions, and therefore did not predict any discontinuity in the number of current carriers. [Pg.123]

Electron spin has more subtle effects on atomic and molecular energies. The exclusion principle as stated above is really a consequence of a more profound influence of the spin on the way electrons move. Two elections with parallel spins (i.e. having the same value of ms) have a strong tendency to avoid each other in space. Suppose we put two elections into different orbitals. There is then no restriction on the relative spin directions. If they are parallel, however, the electrons keep apart and so the electrostatic repulsion between them is less than if the spins are anti-parallel. The former situation gives a lower total energy. We shall see below that this has consequences for the filling of degenerate orbitals, such as the p and d shells, in the periodic table. [Pg.79]

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