Photophysics of AgCl doped with [Cl5Ir(N-methylpyrazinium)]-:: I.: EPR, ENDOR and structural calculations

被引:4
作者
Eachus, RS [1 ]
Pawlik, TD [1 ]
Baetzold, RC [1 ]
Crosby, DA [1 ]
McGugle, WG [1 ]
机构
[1] Eastman Kodak Co, Imaging Mat Div, Rochester, NY 14650 USA
关键词
D O I
10.1088/0953-8984/12/11/318
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
By applying a combination of multi-frequency electron paramagnetic resonance spectroscopy, electron nuclear double resonance spectroscopy and advanced computational techniques, an understanding of the effects of [Cl5Ir(NMP)](-) complexes on the photophysics of AgCl dispersions is emerging (NMP = N-methylpyrazinium). There is indirect spectroscopic evidence that this dopant is incorporated intact during AgCl precipitation. Calculations predict its substitution for an (Ag2Cl7)(5-) sub-unit of the host lattice, with the NMP ring rotated 45 degrees with respect to the equatorial chloride ligands. Calculations also shaw that, in grains with edge lengths greater than or equal to 0.05 mu m, the majority of dopant centres will be fully charge compensated by association with four silver ion vacancies. A (101)((1) over bar 01)(<01(1)over bar >)(<0(11)over bar>) geometry is favoured, where the Cl-Ir-(NMP) axis defines z. Photo-EPR experiments suggest a small population of undercompensated {[Cl5Ir(NMP)](-) 3V} centres also exists in most of the dispersions studied. During exposure to actinic light, these dopant centres trap electrons. Since the dopant's LUMO is primarily a pi* NMP orbital, the initial photoproducts are ligand-centred, one-electron donors. Experimental H-1 hyperfine data obtained by powder ENDOR spectroscopy for the favoured vacancy geometry of {[Cl5Ir(NMP)](2-) 4V} are consistent with the unpaired electron distribution calculated by Hartree-Fock methods. Vacancy binding energies are so large that the over-compensated donor ionizes before the extra vacancy diffuses away.
引用
收藏
页码:2535 / 2553
页数:19
相关论文
共 29 条
[1]  
AMOS RD, 1995, CAMBRIDGE ANAL DERIV
[2]   Computational study of iron hexacyanide in silver halide [J].
Baetzold, RC .
JOURNAL OF PHYSICAL CHEMISTRY B, 1997, 101 (07) :1130-1137
[3]  
BAETZOLD RC, 2000, IN PRESS
[4]  
BELL EL, 1992, Patent No. 5132203
[5]   Shallow electron centers in silver halides [J].
Bennebroek, MT ;
Arnold, A ;
Poluektov, OG ;
Baranov, PG ;
Schmidt, J .
PHYSICAL REVIEW B, 1996, 54 (16) :11276-11289
[6]   STRUCTURE OF THE INTRINSIC SHALLOW ELECTRON CENTER IN AGCL STUDIED BY PULSED ELECTRON-NUCLEAR DOUBLE-RESONANCE SPECTROSCOPY AT 95-GHZ [J].
BENNEBROEK, MT ;
POLUEKTOV, OG ;
ZAKRZEWSKI, AJ ;
BARANOV, PG ;
SCHMIDT, J .
PHYSICAL REVIEW LETTERS, 1995, 74 (03) :442-445
[7]  
BERRY CR, 1977, THEORY PHOTOGRAPHIC, pCH3
[8]   A CALCULATION OF DEFECT GIBBS ENERGIES FOR SILVER-CHLORIDE AND SILVER BROMIDE [J].
CATLOW, CRA ;
CORISH, J ;
HARDING, JH ;
JACOBS, PWM .
PHILOSOPHICAL MAGAZINE A-PHYSICS OF CONDENSED MATTER STRUCTURE DEFECTS AND MECHANICAL PROPERTIES, 1987, 55 (04) :481-498
[9]   Spectroscopic and computational studies of [OsCl5(NO)]3- and [RuCl5(NO)]3- donors in AgCl [J].
Eachus, RS ;
Baetzold, RC ;
Pawlik, TD ;
Poluektov, OG ;
Schmidt, J .
PHYSICAL REVIEW B, 1999, 59 (13) :8560-8571
[10]   EPR SPECTROSCOPIC INVESTIGATIONS OF METAL-HALIDES DOPED WITH TRANSITION-METAL IONS .1. RHODIUM(III)-DOPED AGBR [J].
EACHUS, RS ;
GRAVES, RE .
JOURNAL OF CHEMICAL PHYSICS, 1974, 61 (07) :2860-2867