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Operators excitation energy

The first term in the brackets is the expectation value of the square of the dipole moment operator (i.e. the second moment) and the second term is the square of the expectation value of the dipole moment operator. This expression defines the sum over states model. A subjective choice of the average excitation energy As has to be made. [Pg.289]

Here ho is the kinetic energy and nuclear attraction operator while and 1C are the coulomb and exchange operators, respectively. The coefficients X and Y are solutions of the RPA equations, which for the / singlet transition with excitation energy can be written as... [Pg.179]

Equation 17 can be viewed as the general form of a sum rule for an arbitrary one-electron operator O expressed in terms of the square of the transition moment of the operator and its excitation energies. [Pg.181]

Concentration At high concentrations fluorescence emission l ecomes non-linear due to self-absorption by the sample itself or complete absorption of the excitation energy before it reaches the cell center. High fluorescence Intensity may overload the photomultiplier tube which returns slowly to its normal operating conditions and misrepresents the actual fluorescence signal until restabilized. [Pg.809]


See other pages where Operators excitation energy is mentioned: [Pg.2188]    [Pg.2208]    [Pg.380]    [Pg.32]    [Pg.225]    [Pg.402]    [Pg.457]    [Pg.100]    [Pg.35]    [Pg.300]    [Pg.220]    [Pg.510]    [Pg.465]    [Pg.10]    [Pg.267]    [Pg.125]    [Pg.41]    [Pg.113]    [Pg.355]    [Pg.224]    [Pg.10]    [Pg.461]    [Pg.7]    [Pg.189]    [Pg.362]    [Pg.87]    [Pg.89]    [Pg.92]    [Pg.98]    [Pg.166]    [Pg.87]    [Pg.89]    [Pg.92]    [Pg.98]    [Pg.166]    [Pg.319]    [Pg.1223]    [Pg.206]    [Pg.13]    [Pg.583]    [Pg.78]    [Pg.380]    [Pg.140]    [Pg.1223]    [Pg.712]   
See also in sourсe #XX -- [ Pg.80 , Pg.87 , Pg.88 , Pg.89 ]




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Energy operator

Excitation energy

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