UNUSUAL LUMINESCENCE SPECTRA AND DECAY DYNAMICS IN CRYSTALLINE SUPRAMOLECULAR [(A18C6)(4)MBR4][TLBR4](2) (A = RB, K M = 3D ELEMENT) COMPLEXES

Citation
Ns. Fender et al., UNUSUAL LUMINESCENCE SPECTRA AND DECAY DYNAMICS IN CRYSTALLINE SUPRAMOLECULAR [(A18C6)(4)MBR4][TLBR4](2) (A = RB, K M = 3D ELEMENT) COMPLEXES, Inorganic chemistry, 36(24), 1997, pp. 5539-5547
Citations number
31
Categorie Soggetti
Chemistry Inorganic & Nuclear
Journal title
ISSN journal
00201669
Volume
36
Issue
24
Year of publication
1997
Pages
5539 - 5547
Database
ISI
SICI code
0020-1669(1997)36:24<5539:ULSADD>2.0.ZU;2-U
Abstract
Luminescence and electronic energy transport characteristics of supram olecular cubic F23 [(A18C6)(4)MnBr4][TlBr4](2) complexes (A = Rb, 1; A = K, 2) were studied with the expectation that MnBr42- ions would be effective luminescent probes for solid state 18-crown-6 rotation-confo rmational reorientation motion frequently revealed by NMR methods. Lum inescence and excitation spectra of 1 are normal for complexes of MnBr 42-, but complex 2 features an unusual orange emission (due to crystal defects) with lambda(max) approximate to 570 nm which is sensitized b y MnBr42- ions. Thermal barriers of 8 and 14 kJ mol(-1) (T < 210 K and T > 240 K, respectively) for 1 (MnBr(4)(2-)lambda(em) = 511 nm) and 2 (crystal defect lambda(em) = 610 nm) are attributed to the energy req uired to bridge the Stokes shifted T-4(1)((4)G) emission of the donor MnBr42- ions with the electronic origin of the T-4(1)((4)G) State on t he acceptor MnBr42- during energy migration. That of 26 kJ mol(-1) (21 0 < T < 240 K) exhibited by 1 is attributed to the activation energy f or;he 18C6 solid state motion inferable from the single, broad, featur eless solid state C-13 NMR band of [(K18C6)(4)ZnBr4][TlBr4](2) (3). Cr ystal data for [(K18C6)(4)MBr4][TlBr4](2), where M = Mn (Zn): space gr oup F23 and Z = 4 for both complexes; a = 20.986(7) (20.9682(7)) Angst rom, V = 9242.8(3) (9219.0(3)) Angstrom(3), number of observed data = 672 (668), R-w = 0.037 (0.039), R = 0.062 (0.036).