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Matrix element definition

Note in passing that the common model in the theory of diffusion of impurities in 3D Debye crystals is the so-called deformational potential approximation with C a>)ccco,p co)ccco and J o ) oc co, which, for a strictly symmetric potential, displays weakly damped oscillations and does not have a well defined rate constant. If the system permits definition of the rate constant at T = 0, the latter is proportional to the square of the tunneling matrix element times the Franck-Condon factor, whereas accurate determination of the prefactor requires specifying the particular spectrum of the bath. [Pg.24]

Comparing this expression with (3.81), one obtains the formal definition of the quasiclassical tunneling matrix element... [Pg.53]

The orbital energies can be considered as matrix elements of the Fock operator with the MOs (dropping the prime notation and letting 0 be the canonical orbitals). The total energy can be written either as eq. (3.32) or in terms of MO energies (using the definition of F in eqs. (3.36) and (3.42)). [Pg.63]

Fock Space Representation of Operators.—Let F be some operator that neither creates nor destroys particles, and is a known function in configuration space for N particles. In symbols such an operator must by definition have the following matrix elements in Fock space ... [Pg.455]

The ri fiiatrix, due to the tune ordering operator in its definition is not invariant under time inversion. The invariance of the theory under tahi ihversidn has the following important consequence for the S-matrix since this operator s matrix elements axe given by ... [Pg.692]

In the latter expression the matrix element of operator dq> is transformed according to the Wigner-Eckart theorem and the definition used is... [Pg.232]

The F matrix elements in eqs. (15) and (16) are formally the same as for closed-shell systems, the only difference being the definition of the density matrix in eq. (17), where the singly occupied orbital (m) has also to be taken into account. The total electronic energy (not including core-core repulsions) is given by... [Pg.336]

S u P space. If the determinants j> are built on orthogonal orbitals, equation (6) is automatically fulfilled which ensures that equation (5) is also valid due to the definition of H°. The matrix elements of H° are then easily calculated ... [Pg.43]

Our task is now to write out the spin Hamiltonian Hs, to calculate all the energy-matrix elements in Equation 7.11 using the spin wavefunctions of Equation 7.14 and the definitions in Equations 7.15-7.17, and to diagonalize the complete E matrix to get the energies and the intensities of the transitions. We will now look at a few examples of increasing complexity to obtain energies and resonance conditions, and we defer a look at intensities to the next chapter. [Pg.116]

Both of these matrix elements are readily computed analytically (the subscript R denotes integration over the nuclear coordinates and by definition Su and S/y vanish for / / J). In Eq. (2.11), H/y is the full Hamiltonian matrix including both electronic and nuclear terms. Each matrix element of H is written as the sum of the nuclear kinetic energy (7r) and the electronic Hamiltonian (He)... [Pg.448]

The quantities introduced have a number of properties necessary for thermodynamic equilibrium to establish between the subsystem and the reservoir at / - oo. First of all, we note that by virtue of the definition (4.2.30) the summation of the matrix elements Wqq over the first index gives zero. Therefore, summation over q of both sides of Eq. (4.2.31) makes the product Cqv vanish. From... [Pg.100]

Here u(+), w(z) are related to U(z), W(z) through the definitions (31) and Evac stands for the contribution due to the electron vacuum polarization which is added by hand . The results of calculations for the matrix elements determining the energy-label shift are the same as in Ref. (Lyubovitskji and Rusetsky, 2000) ... [Pg.320]

The operators Fk(t) defined in Eq.(49) are taken as fluctuations based on the idea that at t=0 the initial values of the bath operators are uncertain. Ensemble averages over initial conditions allow for a definite specification of statistical properties. The statistical average of the stochastic forces Fk(t) is calculated over the solvent effective ensemble by taking the trace of the operator product pmFk (this is equivalent to sum over the diagonal matrix elements of this product), so that = Trace(pmFk) is identically zero (Fjk(t)=Fk(t) in this particular case). The non-zero correlation functions of the fluctuations are solvent statistical averages over products of operator forces,... [Pg.309]

Definition (5) shows that TJb which is sometimes called the electronic matrix element , represents the residual interaction resulting from the overlap of the wavefunctions v /j and These functions, which describe the initial and final electronic states of the whole system, respectively, depend closely on the nature of the redox centers and of the medium, so that reliable values of T are very difiicult to obtain from ab initio calculations in complex systems. For that reason, some authors have proposed determining T b semi-empirically by using the results of spectroscopic measurements. We begin by a brief presentation of... [Pg.12]

These equations differ from the previous definitions of the X and Y matrix elements since the derivatives of the internal coordinates with respect to vibrational coordinate are considered. [Pg.403]

Using the definition < A > = Tr(pA), we can express all the matrix elements in the density matrix in terms of different spin-spin correlation functions [62] ... [Pg.507]

In the definition of the essential coupling matrix element CCfj... [Pg.276]

Electric field in 10 an, energies in eV, dipole moment matrix elements in Debye, charges Aq in e for the definitions of various quantities, see Table 1 Adapted from [41]... [Pg.54]

An outstanding feature of inorganic mass spectrometry is its determination of precise and accurate isotopic abundances and isotope ratios. Isotopes of the same element (of the same number of protons or atomic number of element, Z) are, by definition, nuclides with different mass m and mass number A (A = Z + N) due to the different number of neutrons (N) in the nucleus. Isotope analyses are of special interest for characterizing the composition of samples with respect to stable and unstable isotopes in quite different concentration ranges - from the analysis of matrix elements down to the trace and ultratrace concentration level.1-9 Of 1700 isotopes, nearly 16 % (264 isotopes) are stable. The chemical elements Tc, Pm, Th, U and the transuranic elements do not possess stable isotopes. [Pg.223]

It may not at first be obvious that the Jahn-Teller theorem applies to transition states (40). The proof rests on the fact that the matrix element of the distortion gives a first-order change in energy and hence is linear in Q. In other words there must be a non-zero slope in some direction and this is incompatible with the definition of a transition point as a saddle point on the potential energy surface. [Pg.111]

Since the selection rule for nonzero Qi and Pi matrix elements in the harmonic oscillator basis is Av = 1, and since the definition of a polyad is such that all pairs of states differing by only one vibrational quantum number... [Pg.477]


See other pages where Matrix element definition is mentioned: [Pg.153]    [Pg.153]    [Pg.448]    [Pg.201]    [Pg.384]    [Pg.235]    [Pg.274]    [Pg.606]    [Pg.706]    [Pg.171]    [Pg.283]    [Pg.202]    [Pg.189]    [Pg.474]    [Pg.273]    [Pg.15]    [Pg.497]    [Pg.249]    [Pg.382]    [Pg.219]    [Pg.353]    [Pg.383]    [Pg.756]    [Pg.243]    [Pg.20]   
See also in sourсe #XX -- [ Pg.4 ]

See also in sourсe #XX -- [ Pg.4 ]




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