An ab initio and MNDO-d SCF-MO Computational Study of Stereoelectronic Control in Extrusion Reactions of R2I-F Iodine (III) Intermediates.

Michael A. Carroll, Sonsoles Martin-Santamaria, Victor W. Pike, Henry S. Rzepa* and David A. Widdowson

Department of Chemistry, Imperial College of Science, Technology and Medicine, London, SW7 2AY, UK; Chemistry and Engineering Group, MRC Cyclotron Unit, Imperial College School of Medicine, Hammersmith Hospital, Ducane Road, London, W12 0HS UK.

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This supplemental data (c) H. S. Rzepa and S. Martin-Santamaria, 1999.

Part 1. Coordinates derived from Crystal Structures

Original sources for these coordinates are indicated in the body of the article.

Structures of R2I-X Systems (X=Cl...I)

Structures of R2I-O Systems (X=Cl...I)

Structures of R2Br and R2Cl Systems

Structures of RIZ2 Systems

Structures of R2W-X Systems (W=B...Tl, X=F...I)

Part 2. Coordinates derived from Quantum Mechanically optimised Geometries

Table 1. Energies, Hartree (activation barriers, kcal mol-1) and transition normal mode (cm-1) for the stationary point structures R=RÍ=H.

Table 2. Energies, (activation barriers, kcal mol-1) and transition wavenumber (cm-1) for stationary point structures (RHF/3-21G(d)/Hartree, B3LYP/3-21G(d)/Hartree, MNDOD/kcal mol-1).

Table 3. Energies (activation barriers, kcal mol-1) and first normal mode (cm-1) for the stationary point structures (RHF/3-21G(d)/Hartree, B3LYP/3-21G(d)/Hartree, MNDOD/kcal mol-1).

Table 5. Energies (dimerisation/activation) and first normal mode (cm-1) for stationary point structures (RHF/3-21G(d)/Hartree, B3LYP/3-21G(d)/Hartree, B3LYP/DZVP/Hartree, MNDOD/kcal mol-1).