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1 Supplementary Information Cobalt analogues of Roussin's red salt esters: a density functional study Menyhárt B. Sárosi and R. Bruce King* Table S1. BP86/6-311G(d) electronic energies and thermodynamic corrections calculated for the singlet Co 2(NO) 4(SCH 3) 2 structures. Total energies in a.u., relative energies in kcal mol 1. Electronic Energies O-ud O-dd O-TS B-d B-u Iso Table S2. BP86/6-311G(d) electronic energies and thermodynamic corrections calculated for the relevant singlet Co 2(NO) 4(SCH 3) 2 structures including corrections for the solvent effects. Total energies in a.u., relative energies in kcal mol 1. Electronic Energies O-ud O-dd B-d B-u Iso Table S3. M06-L/6-311G(d) electronic energies and thermodynamic corrections calculated for the singlet Co 2(NO) 4(SCH 3) 2 structures. Total energies in a.u., relative energies in kcal mol 1. Electronic Energies O-ud O-dd O-uu O-TS B-d B-u Iso

2 Table S4. BP86/6-311G(d) electronic energies and thermodynamic corrections calculated for the singlet Co 2(NO) 4(SCF 3) 2 structures. Total energies in a.u., relative energies in kcal mol 1. Electronic Energies O-ud O-TS O-dd B-u B-d Iso Table S5. BP86/6-311G(d) electronic energies and thermodynamic corrections calculated for the singlet Co 2(NO) 4(SCF 3) 2 structures including corrections for the solvent effects. Total energies in a.u., relative energies in kcal mol 1. Electronic Energies O-ud O-dd B-u B-d Iso Table S6. BP86/6-311G(d) electronic energies and thermodynamic corrections calculated for the relevant Co 2(NO) 4(SC 4H 9) 2 structures. Total energies in a.u., relative energies in kcal mol 1. Electronic Energies O-ud O dd B u B d Iso Table S7. BP86/6 311G(d) electronic energies and thermodynamic corrections calculated for the relevant singlet Co 2(NO) 4(SC 4H 9) 2 structures including corrections for the solvent effects. Total energies in a.u., relative energies in kcal mol 1. Electronic Energies and zero point Energies O ud O dd B d B u Iso

3 O-ud O-dd Iso B-d B-u Figure S1. BP86/6 311G(d) optimized Co 2(NO) 4(SC 4H 9) 2 geometries without corrections for the solvent effects. Hydrogen atoms are not shown for clarity. Table S8. BP86/6-311G(d) structural parameters (Å), HOMO-LUMO gaps (ev), imaginary frequencies (cm 1 ) and point groups of the Co 2(NO) 4(SC 4H 9) 2 structures without corrections for the solvent effects. Co Co Co S a Co N b N O c HOMO-LUMO Imaginary freq. O-ud none C s O-dd none C B-d none C B-u none C a Terminal Co S distances in italics. b Terminal Co N(O) distances are averaged for the butterfly type structures, bridging Co N(O) distances in italics. c Terminal N O distances are averaged for the butterfly type structures, bridging N O distances in italics.

4 Table S9. BP86/6 311G(d) atomic charge distributions from natural population analysis and relative charge differences for O ud 1 Co 2(NO) 4(SR) 2 (R = CH 3, CF 3). Co Co S S Co Co S S N N O O N N O O N N O O N N O O C C C C H F H F H F H F H F H F Table S10. BP86/6 311G(d) atomic charge distributions from natural population analysis and relative charge differences for O dd 1 Co 2(NO) 4(SR) 2 (R = CH 3, CF 3). Co Co S S Co Co S S N N O O N N O O N N O O N N O O C C C C H F H F H F H F H F H F

5 Table S11 BP86/6 311G(d) atomic charge distributions from natural population analysis and relative charge differences for B d 1 Co 2(NO) 4(SR) 2 (R = CH 3, CF 3). Co Co S S Co Co S S N N O O N N O O N N O O N N O O C C C C H F H F H F H F H F H F Table S12 BP86/6 311G(d) atomic charge distributions from natural population analysis and relative charge differences for B u 1 Co 2(NO) 4(SR) 2 (R = CH 3, CF 3). Co Co S S Co Co S S N N O O N N O O N N O O N N O O C C C C H F H F H F H F H F H F

6 Figure S2. BP86/6 311G(d) superimposed theoretical IR spectra of the O ud 1 Co 2(NO) 4(SC 4H 9) 2 structures (shown in black) with the corresponding theoretical IR spectra of O dd 1, B d 1, B u 1 and Iso 1 (shown in red). The spectra of O dd 1, B d 1, B u 1 and Iso 1 have been rescaled 10:1 (according to ref. 7).

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