Haruka Koshino, Fumitaka Takeiri, Kunihisa Sugimoto, Tomoyuki Mochida. “Tuning structural order in photogenerated metal-complex solids from ruthenium-containing ionic liquids.” ChemRxiv (). https://doi.org/10.26434/chemrxiv.15007791/v1

The main paper refers to supporting information, but no separate supporting information file was found among the files available from the ChemRxiv record

K[B(C₂H₄CN)(CN)₃]
¹H NMR (400 MHz, DMSO-d₆) δ = 0.75 (t, 2H, BCH₂, J = 8.26 Hz), 2.27 (t, 2H, BCH₂CH₂, J = 8.36 Hz)
¹¹B NMR (128 MHz, DMSO-d₆) δ = −31.14 (s)
FT-IR (cm⁻¹) 563, 571, 636, 851, 891, 950, 984, 1013, 1173, 1223, 1328, 1434, 2224 (CN), 2259 (CN), 2930
Main, p. 16
[RuCp(PhNMeHex)]B(C₂H₄CN)(CN)₃
Identifier 1a
¹H NMR (400 MHz, CDCl₃) δ = 0.91–0.93 (m, 3H, NC₅H₁₀CH₃), 1.02–1.06 (m, 2H, BCH₂CH₂CN), 1.28–1.41 (m, 8H, NCH₂C₄H₈CH₃), 2.39–2.43 (m, 2H, BCH₂CH₂CN), 2.95–2.96 (m, 3H, NCH₃), 3.24–3.28 (m, 2H, NCH₂C₅H₁₁), 5.23 (s, 5H, Cp-H₅), 5.63–5.65 (m, 2H, Ar-H₂), 5.81–5.84 (m, 1H, Ar-H), 5.94–5.96 (m, 2H, Ar-H₂)
¹¹B NMR (128 MHz, CDCl₃) δ = −30.73 (s)
FT-IR (cm⁻¹) 557, 656, 725, 837, 881, 942, 981, 1002, 1089, 1105, 1169, 1197, 1260, 1321, 1372, 1414, 1430, 1474, 1555, 2205 (CN), 2242 (CN), 2858, 2928, 3100
Elemental analysis Calcd. for C₂₄H₃₀N₅RuB: C, 57.60; H, 6.04; N, 14.00. Found: C, 56.95; H, 6.19; N, 13.82
Differential scanning calorimetry Glass transition at 215 K
TG–DTA (3 K min⁻¹, N₂), thermal decomposition Tdec = 458 K, defined at 3 % weight loss; single-step weight loss corresponding to loss of the anion and arene ligand: observed, −52 wt %; calcd, −56 wt %
Raman spectroscopy CN stretching bands at 2245 and 2209 cm⁻¹, assigned to B(CN)₃ and B(CH₂CH₂CN), respectively
Main, pp. 12, 14, 17
Neat [RuCp(PhNMeHex)]B(C₂H₄CN)(CN)₃ during 365 nm irradiation at 293 K and heating at 393 K
FT-IR Upon photoirradiation, CN stretching bands at 2240 and 2205 cm⁻¹ were replaced by a single, more intense band at 2224 cm⁻¹; the arene-ring band at 1553 cm⁻¹ split into bands at 1507 and 1599 cm⁻¹ attributable to the dissociated arene ligand; heating restored the original spectrum
¹H NMR (CDCl₃) During the photoreaction, the Cp signal shifted, the arene signals disappeared, and new signals due to the dissociated ligand appeared
¹H NMR reaction monitoring, conversion 92 % after 5 min of irradiation; 100 % after 1 h
UV–Vis Photoirradiation increased absorbance in the 350–450 nm region; heating decreased this absorption; repeated cycles of 30 min photoirradiation and 30 min heating demonstrated reversible spectral changes
FT-IR, ¹H NMR and UV–Vis spectra during the photo/thermal reaction Image data were not transcribed
Main, pp. 7–8, 16
Neat 1a₀.₇₅1b₀.₂₅ and 1a₀.₅1b₀.₅ during 365 nm irradiation at 293 K and heating at 393 K
FT-IR, ¹H NMR and UV–Vis Spectral changes were essentially the same as those of 1a
Main, p. 8
[RuCp(PhNMeHex)]Tf₂N
Identifier 1b
¹H NMR (400 MHz, (CD₃)₂SO) δ = 0.92 (t, 3H, NC₅H₁₀CH₃, J = 6.84 Hz), 1.27–1.34 (m, 8H, NCH₂C₄H₈CH₃), 1.54–1.59 (m, 2H, NCH₂CH₂C₄H₉), 2.86 (s, 3H, NCH₃), 3.22 (t, 2H, NCH₂C₅H₁₁, J = 7.74 Hz), 5.15 (s, 5H, Cp-H₅), 5.63 (d, 2H, Ar-H₂, J = 6.64 Hz), 5.74 (t, 1H, Ar-H, J = 5.4 Hz), 5.83 (t, 2H, Ar-H₂, J = 6.10 Hz)
¹⁹F NMR (376 MHz, (CD₃)₂SO) δ = −78.7 (s)
Elemental analysis Calcd. for C₂₀H₂₆N₂RuF₆O₄S₂: C, 37.67; H, 4.11; N, 4.39. Found: C, 37.72; H, 4.34; N, 4.65
Differential scanning calorimetry Glass transition at 217 K
TG–DTA (3 K min⁻¹, N₂), thermal decomposition Tdec = 593 K; single-step weight loss
Main, pp. 14, 17
[RuCp(PhNMeHex)]FSA
Identifier 1c
¹H NMR (400 MHz, CD₃CN) δ = 0.92 (t, 3H, NC₅H₁₀CH₃, J = 6.84 Hz), 1.34 (m, 6H, NC₂H₄C₃H₆CH₃), 1.54–1.57 (m, 2H, NCH₂CH₂C₄H₉), 2.86 (s, 3H, NCH₃), 3.22 (t, 2H, NCH₂C₅H₁₁, J = 7.74 Hz), 5.15 (s, 5H, Cp-H₅), 5.63 (d, 2H, Ar-H₂, J = 6.76 Hz), 5.74 (t, 1H, Ar-H, J = 5.48 Hz), 5.81–5.84 (m, 2H, Ar-H₂)
¹⁹F NMR (376 MHz, CD₃CN) δ = −51.0 (s)
Elemental analysis Calcd. for C₁₈H₂₆N₂RuF₂O₄S₂: C, 40.21; H, 4.87; N, 5.21. Found: C, 40.32; H, 4.89; N, 5.23
Differential scanning calorimetry Solid-state phase transition at 178.0 K: ΔH = 4.74 kJ mol⁻¹, ΔS = 26.2 J mol⁻¹ K⁻¹; melting at 331.6 K: ΔHm = 26.9 kJ mol⁻¹, ΔSm = 80.5 J mol⁻¹ K⁻¹; glass transition at 213 K on cooling; cold crystallization at 267 K on reheating; Tg/Tm = 0.64
Single-crystal X-ray diffraction (223 K) Space group P-1; Z = 2; alternating cation–anion arrangement; intermolecular π···π contacts between Cp rings and between benzene rings of adjacent cations with C···C distances of 3.45 and 3.52 Å, respectively; the hexyl groups of the cations adopted all-trans conformations and were aligned parallel to one another; the central N atom of the anion was disordered over three positions with occupancies of 0.463(3):0.307(3):0.230(3), and the –SO₂F groups were likewise disordered over three positions
Single-crystal X-ray structure image (223 K) Image data were not transcribed
Main, pp. 13–14, 17
Cubane-type complex
Identifier 3
¹H NMR (400 MHz, CDCl₃) δ = 1.09 (t, 2H, BCH₂, J = 7.80 Hz), 2.45 (t, 2H, BCH₂CH₂, J = 7.84 Hz), 4.24 (s, 5H, Cp-H₅)
FT-IR (cm⁻¹) 589, 814, 836, 869, 914, 977, 997, 1100, 1170, 1205, 1293, 1350, 1428, 2223 (CN), 2916, 3101, 3667
Elemental analysis Calcd. for C₄₄H₃₆N₁₆Ru₄B₄: C, 42.74; H, 2.93; N, 18.13. Found: C, 42.39; H, 2.69; N, 17.79
Optical microscopy Aggregates of well-defined, cube-shaped crystalline particles
Raman spectroscopy Single, slightly asymmetric band near 2232 cm⁻¹, likely comprising two unresolved components
Powder X-ray diffraction, heating at 373 K for 1 h Pattern was unchanged
TG–DTA (3 K min⁻¹, N₂), thermal decomposition Tdec = 487 K, defined at 3 % weight loss; single-step weight loss corresponding to elimination of cyanoethyl groups: observed, −17.9 wt %; calcd, −17.5 wt %
Main, pp. 9, 12, 14, 18
3·0.5MeOH
Single-crystal X-ray diffraction (90 K) Space group P-1; Z = 4; two crystallographically independent cubane molecules in the asymmetric unit; one cyanoethyl group in cubane I was disordered over three positions with occupancies of 0.479(3):0.354(3):0.167(3); one cyanoethyl group in cubane II was disordered over two positions with occupancies of 0.548(7):0.452(7); the methanol molecules occupied voids between neighboring cubane molecules along the c axis
Single-crystal X-ray structure image (90 K) Image data were not transcribed
Main, pp. 12–13
Solids 2, 2′ and 2″ and cubane-type complex 3
Optical microscopy and scanning electron microscopy Image data were not transcribed
Optical microscopy, well-defined cube-shaped crystalline particles in 2, 2′ and 2″ Not observed
Powder X-ray diffraction patterns and PXRD- and ¹H NMR-derived fractions Image data were not transcribed
Powder X-ray diffraction, crystalline phase in 2, 2′ and 2″ Assigned to cubane-type complex 3 because its diffraction peaks matched those of 3
Raman spectroscopy, coordination environment in 2, 2′ and 2″ Close similarity to 3 supported the presence of common local Ru–NC–B coordination environments; the data did not establish the overall connectivities
Main, pp. 9–10, 12
Solid from neat-state photoirradiation of 1a
Identifier 2
Elemental analysis Calcd. for C₄₄H₃₆N₁₆Ru₄B₄: C, 42.74; H, 2.93; N, 18.13. Found: C, 43.19; H, 2.80; N, 18.45
Optical microscopy and scanning electron microscopy Densely packed morphology on the quartz plates; peeled samples consisted mainly of irregular plate-like fragments
Synchrotron powder X-ray diffraction (λ = 0.49592 Å) Broad halo and sharp diffraction peaks; crystalline cubane-type complex fraction estimated from the integrated areas of the sharp reflections and amorphous halo: approximately 13 %; low-angle peak FWHM = 0.11°; crystallite size estimated using the Scherrer equation: approximately 24 nm
¹H NMR (CD₂Cl₂, immediately after dissolution) Several Cp-H signals indicated multiple coordination species; cubane-type complex 3 gave a singlet at δ 4.24 ppm and had a semiquantitative solution-derived fraction of 63 %; the remaining signals arose from additional components whose structures could not be assigned; limited reorganization during dissolution could not be excluded
¹H NMR (CDCl₃-soluble portion) Semiquantitative cubane-type complex 3 fraction: 73 %
Raman spectroscopy Single, slightly asymmetric band near 2232 cm⁻¹, likely comprising two unresolved components
Powder X-ray diffraction, heating at 373 K for 1 h Pattern was unchanged
Main, pp. 8–12, 18
Solid from neat-state photoirradiation of 1a₀.₇₅1b₀.₂₅
Identifier 2′
Optical microscopy Cracks were more prominent than in 2
Synchrotron powder X-ray diffraction (λ = 0.49592 Å) Broad halo and sharp diffraction peaks; crystalline cubane-type complex fraction estimated from the integrated areas of the sharp reflections and amorphous halo: approximately 19 %; low-angle peak FWHM = 0.10°; crystallite size estimated using the Scherrer equation: approximately 27 nm
¹H NMR (CD₂Cl₂, immediately after dissolution) Several Cp-H signals indicated multiple coordination species; cubane-type complex 3 gave a singlet at δ 4.24 ppm and had a semiquantitative solution-derived fraction of 56 %; the remaining signals arose from additional components whose structures could not be assigned; limited reorganization during dissolution could not be excluded
¹H NMR (CDCl₃-soluble portion) Semiquantitative cubane-type complex 3 fraction: 58 %
Raman spectroscopy Single, slightly asymmetric band near 2232 cm⁻¹, likely comprising two unresolved components
Powder X-ray diffraction, heating at 373 K for 1 h Pattern was unchanged
Main, pp. 8–12, 18
Solid from neat-state photoirradiation of 1a₀.₅1b₀.₅
Identifier 2″
Optical microscopy and scanning electron microscopy Cracks were more prominent than in 2; peeled samples consisted mainly of irregular plate-like fragments; the surface appeared smoother than that of 2, while the overall morphologies were similar
Synchrotron powder X-ray diffraction (λ = 0.79986 Å) Broad halo and sharp diffraction peaks; crystalline cubane-type complex fraction estimated from the integrated areas of the sharp reflections and amorphous halo: approximately 44 %; low-angle peak FWHM = 0.06°; crystallite size estimated using the Scherrer equation: approximately 45 nm
¹H NMR (CD₂Cl₂, immediately after dissolution) Several Cp-H signals indicated multiple coordination species; cubane-type complex 3 gave a singlet at δ 4.24 ppm and had a semiquantitative solution-derived fraction of 39 %; the remaining signals arose from additional components whose structures could not be assigned; limited reorganization during dissolution could not be excluded
¹H NMR (CDCl₃-soluble portion) Semiquantitative cubane-type complex 3 fraction: 54 %
Raman spectroscopy Single, slightly asymmetric band near 2232 cm⁻¹, likely comprising two unresolved components
Powder X-ray diffraction, heating at 373 K for 1 h Pattern was unchanged
Main, pp. 8–12, 18
CD₂Cl₂ solutions of 2, 2′ and 2″
¹H NMR, five days after dissolution The species other than cubane-type complex 3 gradually converted into 3