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Ground state absorption

Two-Photon Absorption, Ground State/Excited State Absorption,... [Pg.184]

Self-absorption ground-state atoms in cooler, outer part of flame absorb emission from excited atoms at center of flame, thereby decreasing overall emission higher analyte concentration gives higher self-absorption and a nonlinear calibration curve... [Pg.447]

There are two fimdamental types of spectroscopic studies absorption and emission. In absorption spectroscopy an atom or molecule in a low-lying electronic state, usually the ground state, absorbs a photon to go to a higher state. In emission spectroscopy the atom or molecule is produced in a higher electronic state by some excitation process, and emits a photon in going to a lower state. In this section we will consider the traditional instrumentation for studying the resulting spectra. They define the quantities measured and set the standard for experimental data to be considered. [Pg.1120]

Most stable polyatomic molecules whose absorption intensities are easily studied have filled-shell, totally synuuetric, singlet ground states. For absorption spectra starting from the ground state the electronic selection rules become simple transitions are allowed to excited singlet states having synuuetries the same as one of the coordinate axes, v, y or z. Other transitions should be relatively weak. [Pg.1137]

So far we have exclusively discussed time-resolved absorption spectroscopy with visible femtosecond pulses. It has become recently feasible to perfomi time-resolved spectroscopy with femtosecond IR pulses. Flochstrasser and co-workers [M, 150. 151. 152. 153. 154. 155. 156 and 157] have worked out methods to employ IR pulses to monitor chemical reactions following electronic excitation by visible pump pulses these methods were applied in work on the light-initiated charge-transfer reactions that occur in the photosynthetic reaction centre [156. 157] and on the excited-state isomerization of tlie retinal pigment in bacteriorhodopsin [155]. Walker and co-workers [158] have recently used femtosecond IR spectroscopy to study vibrational dynamics associated with intramolecular charge transfer these studies are complementary to those perfomied by Barbara and co-workers [159. 160], in which ground-state RISRS wavepackets were monitored using a dynamic-absorption technique with visible pulses. [Pg.1982]

Figure B3.4.7. Schematic example of potential energy curves for photo-absorption for a ID problem (i.e. for diatomics). On the lower surface the nuclear wavepacket is in the ground state. Once this wavepacket has been excited to the upper surface, which has a different shape, it will propagate. The photoabsorption cross section is obtained by the Fourier transfonn of the correlation function of the initial wavefimction on tlie excited surface with the propagated wavepacket. Figure B3.4.7. Schematic example of potential energy curves for photo-absorption for a ID problem (i.e. for diatomics). On the lower surface the nuclear wavepacket is in the ground state. Once this wavepacket has been excited to the upper surface, which has a different shape, it will propagate. The photoabsorption cross section is obtained by the Fourier transfonn of the correlation function of the initial wavefimction on tlie excited surface with the propagated wavepacket.
You can use Cl to predict electronic spectra. Since the Cl wave function provides groun d state an d excited state energies, you can obtain electron ic absorption frequen cies from the dlfferen ces between the energy of the ground state and the excited states. [Pg.39]

Absorption of electromagnetic radiation causes a molecule to be excited from Its most stable state (the ground state) to a higher energy state (an excited state)... [Pg.575]

Use Configuration Interaction to predict the electronic spectra of molecules. The Configuration Interaction wave function computes a ground state plus low lying excited states. You can obtain electronic absorption frequencies from the differences between the energies of the ground state and the excited states. [Pg.117]

The atomic absorption spectrum for Na is shown in Figure 10.19 and is typical of that found for most atoms. The most obvious feature of this spectrum is that it consists of a few, discrete absorption lines corresponding to transitions between the ground state (the 3s atomic orbital) and the 3p and 4p atomic orbitals. Absorption from excited states, such as that from the 3p atomic orbital to the 4s or 3d atomic orbital, which are included in the energy level diagram in Figure 10.18, are too weak to detect. Since the... [Pg.383]


See other pages where Ground state absorption is mentioned: [Pg.132]    [Pg.238]    [Pg.183]    [Pg.132]    [Pg.238]    [Pg.183]    [Pg.200]    [Pg.245]    [Pg.263]    [Pg.264]    [Pg.312]    [Pg.847]    [Pg.1121]    [Pg.1128]    [Pg.1129]    [Pg.1142]    [Pg.1980]    [Pg.1981]    [Pg.1990]    [Pg.2304]    [Pg.304]    [Pg.507]    [Pg.517]    [Pg.5]    [Pg.47]    [Pg.117]    [Pg.216]    [Pg.69]    [Pg.586]    [Pg.47]    [Pg.423]    [Pg.424]    [Pg.426]    [Pg.438]    [Pg.123]    [Pg.124]    [Pg.125]    [Pg.125]    [Pg.127]    [Pg.135]   
See also in sourсe #XX -- [ Pg.422 , Pg.423 , Pg.424 , Pg.425 , Pg.426 , Pg.427 ]




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Charge-transfer absorption band ground state

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