Excited-state interactions for [Au(CN)(2)(-)](n) and [Ag(CN)(2)(-)](n) oligomers in solution. Formation of luminescent gold-gold bonded excimers and exciplexes
Ma. Rawashdeh-omary et al., Excited-state interactions for [Au(CN)(2)(-)](n) and [Ag(CN)(2)(-)](n) oligomers in solution. Formation of luminescent gold-gold bonded excimers and exciplexes, J AM CHEM S, 123(45), 2001, pp. 11237-11247
Solutions of K[Au(CN)(2)] and K[Ag(CN)(2)] in water and methanol exhibit st
rong photoluminescence. Aqueous solutions of K[Au(CN)(2)] at ambient temper
ature exhibit luminescence at concentration levels of greater than or equal
to 10(-2) M, while frozen methanol glasses (77 K) exhibit strong luminesce
nce with concentrations as low as 10(-5) M. The corresponding concentration
limits for K[Ag(CN)(2)] solutions are 10(-1) M at ambient temperature and
10-1 M at 77 K. Systematic variations in concentration, solvent, temperatur
e, and excitation wavelength tune the luminescence energy of both K[Au(CN)(
2)] and K[Ag(CN)(2)] solutions by > 15 x 10(3) cm(-1) in the UV-visible reg
ion. The luminescence bands have been individually assigned to *[Au(CN)(2)(
-)](n) and *[Ag(CN)(2)(-)](n) excimers and exciplexes that differ in "n " a
nd geometry. The luminescence of Au(I) compounds is related for the first t
ime to Au-Au bonded excimers and exciplexes similar to those reported earli
er for Ag(I) compounds. Fully optimized unrestricted open-shell MP2 calcula
tions for the lowest-energy triplet excited state of staggered [Au(CN)(2)(-
)](2) show the formation of a Au-Au sigma single bond (2.66 Angstrom) in th
e triplet excimer, compared to a weaker ground-state aurophilic bond (2.96
Angstrom). The corresponding frequency calculations revealed Au-Au Raman-ac
tive stretching frequencies at 89.8 and 165.7 cm(-1) associated with the gr
ound state and lowest triplet excited state. respectively. The experimental
evidence of the exciplex assignment includes the extremely large Stokes sh
ifts and the structureless feature of the luminescence bands, which suggest
very distorted excited states. Extended Huckel (EH) calculations for [M(CN
)(2)(-)](n) and *[M(CN)(2)(-)](n) models (M = An, A: n = 2, 3) indicate the
formation of M-M bonds in the first excited electronic states. From the av
erage EH values for staggered dimers and trimers, the excited-state Au-Au a
nd Ag-Ag bond energies are predicted to be 104 and 112 kJ/mol, respectively
. The corresponding bond energies in the ground state are 32 and 25 kJ/mol,
respectively.