1998
DOI: 10.1016/s0022-2313(97)00260-3
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Dynamical processes between triplet sublevels of metal-organic Pt(II) compounds

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Cited by 14 publications
(22 citation statements)
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“…Moreover, one finds a pronounced diversity with respect to emission wavelengths, decay times, and quantum yields. [9][10][11][12][13][14][15][16][17][18] An enormous variability is also found regarding sizes and patterns of zero-field splittings (ZFSs) of the triplets into the three substates, 18,19 excitation dynamics within the triplet substate system according to different spin-lattice relaxation (SLR) processes, [19][20][21] vibronic coupling properties, 18 spatial extensions of excited-state wave functions, 18,22 etc. These features may systematically be tuned by the variation of the ligands coordinating the Pt(II) central metal ion.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, one finds a pronounced diversity with respect to emission wavelengths, decay times, and quantum yields. [9][10][11][12][13][14][15][16][17][18] An enormous variability is also found regarding sizes and patterns of zero-field splittings (ZFSs) of the triplets into the three substates, 18,19 excitation dynamics within the triplet substate system according to different spin-lattice relaxation (SLR) processes, [19][20][21] vibronic coupling properties, 18 spatial extensions of excited-state wave functions, 18,22 etc. These features may systematically be tuned by the variation of the ligands coordinating the Pt(II) central metal ion.…”
Section: Introductionmentioning
confidence: 99%
“…Of particular significance is the amount of splitting of the triplet into sublevels under zero magnetic field (zero-field splitting, zfs), which in general increases with increasing d character. Also other properties exhibit correspondingly systematic changes, like emission decay times, relaxation properties between the triplet sublevels, radiative rates of the transitions to the ground states, distinctnesses of Franck−Condon progressions, blue shifts of the transition energy upon deuteration, etc. Interestingly, also the spatial extension of the lowest excited states is controlled by the amount of metal or MLCT character in these states, since this property determines crucially the electronic ligand−ligand coupling in these compounds. Thus, in complexes with small metal character in the corresponding states, such as [Rh(bpy) 3 ] 3+ 26 and [Pt(bpy) 2 ] 2+ with zfs values of the order of 0.1 cm -1 , the lowest excited states are ligand centered (LC) and localized on one ligand 26,27,29,31 (left-hand side of Figure ), while for those compounds with distinct MLCT character, the metal induces a strong ligand−ligand coupling.…”
Section: Introductionmentioning
confidence: 99%
“…1 and Refs. [9][10][11][12][13][14]) due to the low density of phonon states corresponding to such zfs patterns.…”
mentioning
confidence: 99%
“…Recently, the processes of spin-lattice relaxation and the decay behavior of excited states have been studied experimentally for such systems in Shpol'skii matrices. [8][9][10][11][12][13][14] Of special importance are compounds with a Pt(II) central ion. Pt(II) systems exhibit many different types of low-lying excited triplets that include metal-centered (MC) dd * states [15,16], metal-to-ligand-charge-transfer (MLCT) states [17][18][19], intra-ligand-charge-transfer (ILCT) states [10,13,20], ligand-ligand ′ -charge-transfer (LL ′ CT) states [6,7], and ligand-centered (LC) states with some MLCT and/or MC contribution [21][22][23].…”
mentioning
confidence: 99%
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