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The Initial State

The coefficients of the 5-fiinction in the sum are called Franck-Condon factors, and reflect the overlap of the initial state with the excited-state i at energy (see figure Al.6.13). Fonnally, equation (A1.6,88i... [Pg.248]

Themiodynamic measurements are possible only when both the initial state and tire final state are essentially at equilibrium, i.e. internally and with respect to the surroundings. Consequently, for a spontaneous themiodynamic change to take place, some constraint—hitemal or external—must be changed or released. [Pg.337]

Thus, the spontaneous proeess involves the release of a eonstraint while the driven reverse proeess involves the imposition of a eonstraint. The details of the reverse proeess are irrelevant any series of reversible steps by whieh one ean go from the final state baek to the initial state will do to measure AS. [Pg.339]

It is possible to write two such equations for the initial state,(corresponding to the reduced aquo-complex... [Pg.605]

Figure A3.9.9. Dissociation probability versus incident energy for D2 molecules incident on a Cu(l 11) surface for the initial quantum states indicated (u indicates the mitial vibrational state and J the initial rotational state) [100], For clarity, the saturation values have been scaled to the same value irrespective of the initial state, although in reality die saturation value is higher for the u = 1 state. Figure A3.9.9. Dissociation probability versus incident energy for D2 molecules incident on a Cu(l 11) surface for the initial quantum states indicated (u indicates the mitial vibrational state and J the initial rotational state) [100], For clarity, the saturation values have been scaled to the same value irrespective of the initial state, although in reality die saturation value is higher for the u = 1 state.
When spectroscopists speak of electronic selection niles, they generally mean consideration of the integral over only the electronic coordinates for wavefiinctions calculated at the equilibrium nuclear configuration of the initial state, 2 = 0,... [Pg.1136]

The second-order nonlinear optical processes of SHG and SFG are described correspondingly by second-order perturbation theory. In this case, two photons at the drivmg frequency or frequencies are destroyed and a photon at the SH or SF is created. This is accomplished tlnough a succession of tlnee real or virtual transitions, as shown in figure Bl.5.4. These transitions start from an occupied initial energy eigenstate g), pass tlnough intennediate states n ) and n) and return to the initial state g). A fiill calculation of the second-order response for the case of SFG yields [37]... [Pg.1274]

Rule B. When the direct coupling from only the initial state to the continuum vanishes, but the couplmg F 0 for n , the transition can then occur via the intennediate states n at the rate... [Pg.2021]

Figure B3.4.6. Reaction probabilities for the initial-state-selected process H2(v = 0,J = 0)+OH(v,y = 0) — H2O+H, for zero total angular momentum. Taken from [75] with pennission. Figure B3.4.6. Reaction probabilities for the initial-state-selected process H2(v = 0,J = 0)+OH(v,y = 0) — H2O+H, for zero total angular momentum. Taken from [75] with pennission.
The methodology presented so far allows the calculations of state-to-state. S -matrix elements. However, often one is not interested in this high-level of detail but prefers instead to find more average infomiation, such as the initial-state selected reaction probability, i.e. the probability of rearrangement given an initial state Uq. In general, this probability is... [Pg.2302]

In an electron scattering or recombination process, the free center of the incoming electron has the functions Wi = ui U u, and the initial state of the free elechon is some function v/ the width of which is chosen on the basis of the electron momentum and the time it takes the electron to aiTive at the target. Such choice is important in order to avoid nonphysical behavior due to the natural spreading of the wavepacket. [Pg.230]

Estimating Relative Free Energies from a Single Simulation of the Initial State... [Pg.149]

Smith, P. E., van Gunsteren, W. F. Predictions of free energy differences from a single simulation of the initial state. J. Chem. Phys. 100 (1994) 577-585... [Pg.161]

As is well known. Molecular Dynamics is used to simulate the motions in many-body systems. In a typical MD simulation one first starts with an initial state of an N particle system F = xi,..., Xf,pi,..., pf) where / = 3N is the number of degrees of freedom in the system. After sampling the initial state one numerically solves Hamilton s equations of motion ... [Pg.299]

Each of the factorized operators are displacement operators and can thus be applied seriatim to the initial state vector to give the final solution. [Pg.302]

Here, we give here a brief outline of the methods as introduced in Refs. 43, 44, and 47. Suppose that the initial state of the system is tpoili, ,<]n) From ipo, the Wigner phase-space distribution D(qi,..., qn pi,. ..,Pn] is computed. This distribution is used to sample initial positions and momenta, . .., for a classical trajectory simulation of the process of... [Pg.368]


See other pages where The Initial State is mentioned: [Pg.236]    [Pg.250]    [Pg.251]    [Pg.263]    [Pg.276]    [Pg.338]    [Pg.390]    [Pg.395]    [Pg.605]    [Pg.686]    [Pg.753]    [Pg.800]    [Pg.900]    [Pg.1008]    [Pg.1162]    [Pg.1162]    [Pg.1274]    [Pg.1326]    [Pg.1855]    [Pg.2206]    [Pg.2216]    [Pg.2299]    [Pg.2303]    [Pg.3011]    [Pg.58]    [Pg.229]    [Pg.261]    [Pg.291]    [Pg.149]    [Pg.151]    [Pg.151]    [Pg.158]    [Pg.187]    [Pg.301]    [Pg.368]   


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Initial state

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