Crystal structure of fac-Ir(ppy)3 and emission properties under ambient conditions and at high pressure

被引:73
作者
Breu, J
Stössel, P
Schrader, S
Starukhin, A
Finkenzeller, WJ
Yersin, H
机构
[1] Univ Bayreuth, Lehrstuhl Anorgan Chem 1, D-95440 Bayreuth, Germany
[2] Covion Organ Semicond GmbH, Res & Dev, D-65926 Frankfurt, Germany
[3] Univ Potsdam, Dept Condensed Matter Phys, Inst Phys, D-14469 Potsdam, Germany
[4] Natl Acad Sci, Inst Mol & Atom Phys, Minsk 220072, BELARUS
[5] Univ Regensburg, Inst Phys Chem, D-93040 Regensburg, Germany
关键词
D O I
10.1021/cm0486767
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Solution and refinement of the crystal structure of fac-Ir(ppy)(3) is severely hampered by systematic twinning and pseudo-symmetry.fac-Ir(ppy)(3) Crystallizes in the centrosymmetric space group P (3) over bar as has been deduced from single-crystal structure refinement and investigations of the second harmonic generation (SHG) of fac-Ir(ppy)(3) powder as compared to two standard materials. The topology of the molecular packing of fac-Ir(ppy)(3) is identical to the packing observed for [Ru(bpy)(3)](0), however, the site symmetry of all Ir(ppy)(3) molecules is necessarily lowered from D-3 to C-3. Packing motifs with intermolecular "pi-pi interactions" of T-shaped and "shifted pi stack" geometry are realized. The systematic twinning leads to the occurrence of crystalline domains with rigorously alternating chirality within the bulk of the domains but with homochiral fac-Ir(ppy)(3) contacts at the domain interfaces. These differences in packing motifs are displayed in the emission spectra and in the high-pressure-induced shifts of the emission. The emission maximum of the bulk material at 18 350 cm(-1) (545 nm) and of the domain interfaces at 19 700 cm-1 (507 nm) experience for p < 25 kbar and T = 295 K red shifts of Delta nu/Delta p = -(12 +/- 2) cm(-1)/kbar, and -(22 +/- 4) cm(-1)/kbar, respectively.
引用
收藏
页码:1745 / 1752
页数:8
相关论文
共 76 条
[1]   Crystal engineering: Strategies and architectures [J].
Aakeroy, CB .
ACTA CRYSTALLOGRAPHICA SECTION B-STRUCTURAL SCIENCE, 1997, 53 :569-586
[2]   How strong is a pi-facial hydrogen bond? [J].
Adams, H ;
Harris, KDM ;
Hembury, GA ;
Hunter, CA ;
Livingstone, D ;
McCabe, JF .
CHEMICAL COMMUNICATIONS, 1996, (22) :2531-2532
[3]  
AGREN H, COMMUNICATION
[4]  
Albrecht G., 1963, Z CHEM, V3, P182
[5]  
Allen F.H., 1993, CHEM AUTOMAT NEWS, V8, P31
[6]   CRYSTAL-STRUCTURE DETERMINATION FOR CRYSTALS WITH TWINNING BY HEMIHEDRY OR PSEUDOHEMIHEDRY [J].
ARAKI, T .
ZEITSCHRIFT FUR KRISTALLOGRAPHIE, 1991, 194 (3-4) :161-191
[7]   THE ROTATIONAL SPECTRUM, STRUCTURE AND DYNAMICS OF A BENZENE DIMER [J].
ARUNAN, E ;
GUTOWSKY, HS .
JOURNAL OF CHEMICAL PHYSICS, 1993, 98 (05) :4294-4296
[8]   High pressure probes of electronic structure and luminescence properties of transition metal and lanthanide systems [J].
Bray, KL .
TRANSITION METAL AND RARE EARTH COMPOUNDS: EXCITED STATES, TRANSITION, INTERACTIONS I, 2001, 213 :1-94
[9]   Crystal engineering as a tool for directed radiationless energy transfer in layered {Λ-[Ru(bpy)3]Δ-[Os(bpy)3]}(PF6)4 [J].
Breu, J ;
Kratzer, C ;
Yersin, H .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 2000, 122 (11) :2548-2555
[10]  
Breu J, 2002, CHEM-EUR J, V8, P4454, DOI 10.1002/1521-3765(20021004)8:19<4454::AID-CHEM4454>3.0.CO