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Quartet state

Higgins J, Ernst W E, Caiiegari C, Reho J, Lehmann K K, Scoies G and Gutowski M 1996 Spin poiarized aikaii ciusters observation of quartet states of the sodium trimer Phys. Rev. Lett. 77 4532... [Pg.2408]

As discussed in preceding sections, FI and have nuclear spin 5, which may have drastic consequences on the vibrational spectra of the corresponding trimeric species. In fact, the nuclear spin functions can only have A, (quartet state) and E (doublet) symmetries. Since the total wave function must be antisymmetric, Ai rovibronic states are therefore not allowed. Thus, for 7 = 0, only resonance states of A2 and E symmetries exist, with calculated states of Ai symmetry being purely mathematical states. Similarly, only -symmetric pseudobound states are allowed for 7 = 0. Indeed, even when vibronic coupling is taken into account, only A and E vibronic states have physical significance. Table XVII-XIX summarize the symmetry properties of the wave functions for H3 and its isotopomers. [Pg.605]

As with the other sem i-cm pineal methods. HyperGhem s im p le-meiitation of ZINDO/1 is restricted to spin multiplicities up to a quartet state. ZIXDO/1 lets you calculate the energy slates in molecules containing transition metals. [Pg.294]

It only remains to eonstmet the doublet states whieh are orthogonal to these quartet states. Reeall that the orthogonal eombinations for systems having three equal eomponents (for... [Pg.325]

ZINDO/S is an modified INDO method parameterized to reproduce UV visible spectroscopic transitions when used with the Cl singles methods. It was developed in the research group of Michael Zerner of the Quantum Theory Project at the University of Florida. As with the other semi-empirical methods, HyperChem s implementation of ZINDO/S is restricted to spin multiplicities of up to a quartet state. Higher spin systems may not be done using HyperChem. [Pg.296]

Previous expositions of photochemical laws have distinguished ptominentiy between states of singlet and triplet multiplicity (1). This distinction continues to be important with respect to photophysics of smaH organic molecules, but among inorganic and organometaHic compounds, states of other multiplicities, eg, doublet and quartet states (23), play an important role. Spin conservation characterizes electronic molecular excitations and localized... [Pg.388]

The stability of sexivalent chromium, in the chromate ion and related ions, can also be understood. The chromic complexes, involving tervalent chromium, make use of d2sp3 bond orbitals, the three remaining outer electrons of the chromium atom being in three of the 3d orbitals, with parallel spins. The resonance energy of these three atomic electrons in a quartet state helps to stabilise the chromic compounds. However, if all of the nine outer orbitals of the chromium atom were available for bond formation, stable compounds might also be expected... [Pg.229]

The decrease in the contribution of A from 35 % (for cobalt) to 30 % is presumably due in the main to the smaller amount of resonance stabilization for the triplet state than for the quartet state. [Pg.382]

Figure 10. Electron excitations in radicals (a) Collective representation of one-electron transitions of the A, B, and C types if denotes MO (b) LCI energy-level scheme (Jablonski diagram) for doublet and quartet states indicating why with radicals fluorescence (- - -) but not phosphorescence is observed. Spin-forbidden transitions are represented by dashed lines. Figure 10. Electron excitations in radicals (a) Collective representation of one-electron transitions of the A, B, and C types if denotes MO (b) LCI energy-level scheme (Jablonski diagram) for doublet and quartet states indicating why with radicals fluorescence (- - -) but not phosphorescence is observed. Spin-forbidden transitions are represented by dashed lines.
Photoionization can also access excited electronic states of the ion that are difficult to study by optical methods. The photoionization yield of FeO increases dramatically 0.36 eV above the ionzation energy. This result corresponds to the threshold for producing low spin quartet states of FeO. These states had not been previously observed, as transitions to them are spin forbidden and occur at inconveniently low energy. Because the FeO + CH4 reaction occurs via low spin intermediates, accurately predicting the energies of high and low spin states is critical. [Pg.352]

Fig. 4 Esr spectra of high-spin trianthrylene [21a] at 120 K in MTHF/K A, biradical triplet state [21a]2- (labelled O) B, triradical quartet state [21a]3- (labelled ) C, biradical triplet state [21a]4- (labelled ). Fig. 4 Esr spectra of high-spin trianthrylene [21a] at 120 K in MTHF/K A, biradical triplet state [21a]2- (labelled O) B, triradical quartet state [21a]3- (labelled ) C, biradical triplet state [21a]4- (labelled ).
The spin transition in [Fe(salen)(NO)] has been studied by IR [171, 172], 57Fe Mossbauer [169, 173] and EPR spectroscopy [169]. IR spectra have also been recorded at room temperature for various pressures ranging from ambient up to 37 kbar. At 37 kbar conversion to the S=l/2 state is complete [172]. The quartet state is re-populated on relaxation of the pressure. [Pg.313]

Long-lived luminescence. 2. Luminescence involving a change in spin multiplicity (e.g., triplet-to-singlet, singlet-to-triplet, quartet state-to-doublet state, etc.). See Fluorescence Jablonski Diagram... [Pg.556]

The temperature dependence (296-330 K) of the ring methyl proton resonances of these monomeric heme complexes in the hydrophobic micellar cavity shows [22] a small deviation from the Curie law as in the low-spin complexes in organic and simple aqueous solvents [1, 52]. The origin of such deviation has been variously ascribed [3, 1, 53] either to aggregation or second order Zeeman (SOZ) effect or presence of low-lying spin-quartet state. Since these low-spin hemes in micellar solutions are in deaggregated form, the deviation may be due to the SOZ and/or presence of low-lying excited state. [Pg.132]


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Spin-quartet ground state

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