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Quantum mechanical action

The solution of the time-dependent Schrodinger equation (2) with initial condition (3) corresponds to a stationary point of the quantum mechanical action integral... [Pg.89]

The xc potentials in (71) and (72) are formally given by functional derivatives of the xc part of the quantum mechanical action functionals ... [Pg.96]

Once the existence of u,o and A o is assumed, uniqueness follows from the above theorem. Up to this point the time-dependent HKS formalism is quite similar to the case without magnetic fields developed in Sect. 2. The variational representation of Dg,o and As,o, however, turns out to be much more complicated. Following Wacker, Kiimmel and Gross [60] the quantum mechanical action functional... [Pg.104]

As is well-known, the time-dependent variational principle (TDVP) applied to the quantum mechanics action, when fully general variations in state vector space are possible, yields the time-dependent Schrodinger equation. However, when the variations take place in a limited space determined by the choice of an approximate form of wavefunction the result is a set of coupled first-order differentiS equations that govern the time-evolution of the wavefunction parameters (27). [Pg.112]

The time-dependent variational principle in quantum mechanics [9] starts from the quantum mechanical action [10,11]... [Pg.18]

We start from the quantum mechanical action of a many-electron system interacting with an external field [21,26]... [Pg.39]

In time-dependent systems, there is no variational principle on the basis of the total energy for it is not a conserved quantity. There exists, however, a quantity analogous to the energy, the quantum mechanical action... [Pg.148]

The functional derivative of the quantum-mechanical action is, thus, replaced by the much simpler and time-independent functional derivative of the exchange-correlation energy at a particular time f. [Pg.135]

This expression relates the action-at-a-distance forces between atoms to the macroscopic deformations and dominated adhesion theoiy for the next several decades. The advent of quantum mechanics allowed the interatomic interactions giving rise to particle adhesion to be understood in greater depth. [Pg.147]

In Lee s discrete quantum mechanics, the classical action Sc is again replaced by the discrete action (equation 12,33), and, because both x and t are variables, the continuous path [ Dcx t)] is replaced by the discrete path [Dox t)] j] d x ndtji, where is the same as for the continuous case. The parameter n... [Pg.657]

The form of the action principle given above was first applied to quantum mechanics to describe the time evolution of pure states (i.e. [Pg.223]

Section II discusses the real wave packet propagation method we have found useful for the description of several three- and four-atom problems. As with many other wave packet or time-dependent quantum mechanical methods, as well as iterative diagonalization procedures for time-independent problems, repeated actions of a Hamiltonian matrix on a vector represent the major computational bottleneck of the method. Section III discusses relevant issues concerning the efficient numerical representation of the wave packet and the action of the Hamiltonian matrix on a vector in four-atom dynamics problems. Similar considerations apply to problems with fewer or more atoms. Problems involving four or more atoms can be computationally very taxing. Modern (parallel) computer architectures can be exploited to reduce the physical time to solution and Section IV discusses some parallel algorithms we have developed. Section V presents our concluding remarks. [Pg.2]

A key question in the action of enzymes is the understanding of the mechanisms by which they attain their catalytic rate enhancement relative to the uncatalyzed reactions. Some enzymes have been shown to produce rate accelerations as large as 1019 [1], The theoretical determination of the reaction mechanisms by which enzymes carry out the chemical reactions has been an area of great interests and intense development in recent years [2-11], A common approach for the modeling of enzyme systems is the QM/MM method proposed by Warshel and Levitt [12], In this method the enzyme is divided into two parts. One part includes the atoms or molecules that participate in the chemical process, which are treated by quantum mechanical calculations. The other contains the rest of the enzyme and the solvent, generally thousands of atoms, which is treated by molecular mechanics methods. [Pg.58]

Oxidative drug metabolism is extremely complex and possibly the most poorly understood ADME property. Rapid metabolism is unacceptable for drug candidates, except for drugs whose metabolite is the active moiety, because it causes duration of action to be too short. Considerable work has focused on the liver enzyme CYP3A4, which is responsible for the metabolic clearance of approximately 50% of marketed drugs. Recent approaches used to model and understand drug metabolism include database matching, quantum mechanics, QSAR, and structure-based analyses. [Pg.463]

Apart from the operational, wave or action-based pictures of quantum mechanics provided by Heisenberg, Schrodinger, or Feynman, respectively, there is an additional, fully trajectory-based picture Bohmian mechanics [20,23]. Within this picture, the standard quantum formalism is understood in terms of trajectories defined... [Pg.112]


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See also in sourсe #XX -- [ Pg.104 ]




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