Supply Target Lower-bound Upper-bound Average [Pg.245]

Figure 15.7 Emission from a bound upper state (/ =40) to a repulsive lower state, with the resulting oscillatory continuum emission spectrum (simulated) the inset shows the related potential energy curves. Adapted from Tellinghuisen, Adv. Chem. Phys., 1985, 60 299, with permission of John Wiley Sons Ltd |

PARAMETER ESTIMATE ST.ERROR LONER BOUND UPPER BOUND [Pg.160]

PARAMETER ESTIMATE ST.ERROR LOWER BOUND UPPER BOUND [Pg.180]

IF ES=0 THEN LPRINT "ST. ERROR", LOWER BOUND","UPPER BOUND" [Pg.168]

Nonlinear Optimization (NLP) Solution Lower Bound Upper Bour [Pg.1036]

If n in Eq.(17) equals the quantum number of the upper bound state N, n =N, U is positive, and it determines the energy of a weakly bound (upper) state En [Pg.419]

IF ES=0 THEN LPRINT " ESTIHATE"," ST. ERR","LONER BOUND","UPPER BOUND", LFRINT iLPRINT V [Pg.293]

LPRINT "PARANETER ", "ESTIHATE", "STNRD.ERROR", LONER BOUND", "UPPER BOUND" 4084 LPRINT Vt [Pg.148]

These features were interpreted - in terms of transitions from high vibrational levels of a strongly bound upper state of AX to a much flatter region of the ground state. In Figure 3, which shows more recent calculated potential [Pg.167]

The time-dependent wavepacket constructed in Section 4.1 is not the wavepacket that a laser with finite duration creates in the excited electronic state. It represents the wavepacket created by a pulse with infinitely narrow width in time. In order to construct the real wavefunction of the molecular system we must go back to Section 2.1. For simplicity of presentation, let us consider a diatomic molecule with internuclear separation R. We assume that the excitation takes place from the electronic ground state (index 0) to a bound upper state (index 1). The extension to a dissociative state, several coupled excited states, or several degrees of freedom is formally straightforward. [Pg.368]

See also in sourсe #XX -- [ Pg.104 , Pg.269 ]

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