# Electronic Supplementary Material for CrystEngComm # This journal is (c) The Royal Society of Chemistry 2009 data_global _journal_name_full CrystEngComm _journal_coden_Cambridge 1350 _publ_contact_author_name 'Manuel Almeida' _publ_contact_author_email MALMEIDA@ITN.PT _publ_section_title ; Counterion dimerisation effects in the two chain compound (Per)2Co(mnt)2: Structure and anomalous pressure dependence of the electrical transport properties ; loop_ _publ_author_name 'Manuel Almeida' 'James S. Brooks' 'Vasco Gama' 'David Graf' 'Isabel C. Santos' # Attachment 'PerCo_p21n.cif' data_p21n _database_code_depnum_ccdc_archive 'CCDC 710242' _audit_creation_method SHELXL-97 _chemical_name_systematic ; Per2[Co(mnt)2] ; _chemical_name_common Per2(Co(mnt)2) _chemical_melting_point ? _chemical_formula_moiety '2(C20 H12), C8 Co N4 S4' _chemical_formula_sum 'C48 H24 Co N4 S4' _chemical_formula_weight 843.88 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0033 0.0016 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' H H 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' N N 0.0061 0.0033 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' S S 0.1246 0.1234 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Co Co 0.3494 0.9721 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting monoclinic _symmetry_space_group_name_H-M 'P 21/n' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, y+1/2, -z+1/2' '-x, -y, -z' 'x-1/2, -y-1/2, z-1/2' _cell_length_a 17.5429(4) _cell_length_b 4.06590(10) _cell_length_c 25.0320(5) _cell_angle_alpha 90.00 _cell_angle_beta 92.0160(10) _cell_angle_gamma 90.00 _cell_volume 1784.37(7) _cell_formula_units_Z 2 _cell_measurement_temperature 150(2) _cell_measurement_reflns_used ? _cell_measurement_theta_min ? _cell_measurement_theta_max ? _exptl_crystal_description needle _exptl_crystal_colour black _exptl_crystal_size_max 0.60 _exptl_crystal_size_mid 0.06 _exptl_crystal_size_min 0.05 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.571 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 862 _exptl_absorpt_coefficient_mu 0.760 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.6583 _exptl_absorpt_correction_T_max 0.9630 _exptl_absorpt_process_details 'SADABS; Sheldrick,2004' _exptl_special_details ; ? ; _diffrn_ambient_temperature 150(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker-AXS APEX- CCD area-detector' _diffrn_measurement_method '\f and \w' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 12212 _diffrn_reflns_av_R_equivalents 0.0636 _diffrn_reflns_av_sigmaI/netI 0.1026 _diffrn_reflns_limit_h_min -23 _diffrn_reflns_limit_h_max 23 _diffrn_reflns_limit_k_min -5 _diffrn_reflns_limit_k_max 4 _diffrn_reflns_limit_l_min -33 _diffrn_reflns_limit_l_max 33 _diffrn_reflns_theta_min 3.26 _diffrn_reflns_theta_max 28.41 _reflns_number_total 3576 _reflns_number_gt 2278 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker SMART, (Bruker, 2004)' _computing_cell_refinement 'Bruker SMART, (Bruker, 2004)' _computing_data_reduction 'Bruker SAINT, (Bruker, 2004)' _computing_structure_solution 'SIR97 (Altomare, 1999)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics ORTEP3(Farrugia,1997) _computing_publication_material 'WinGX (Farrugia, 1999)' _refine_special_details ; Refinement of F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > 2sigma(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. The crystals obtained were of poor quality, which results in a weak data set and low fraction (0.795) of measured theta full. Due to problems with substantial anisotropy on the S2 Sulfur atom, disorder model was applied and the S2 atom was refined over two position (S2-S3) with s.o.f. 50:50. ; _refine_ls_structure_factor_coef Fsqd _refine_ls_matrix_type full _refine_ls_weighting_scheme calc _refine_ls_weighting_details 'calc w=1/[\s^2^(Fo^2^)+(0.0221P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens geom _refine_ls_hydrogen_treatment constr _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 3576 _refine_ls_number_parameters 272 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0765 _refine_ls_R_factor_gt 0.0440 _refine_ls_wR_factor_ref 0.0855 _refine_ls_wR_factor_gt 0.0799 _refine_ls_goodness_of_fit_ref 0.822 _refine_ls_restrained_S_all 0.822 _refine_ls_shift/su_max 0.001 _refine_ls_shift/su_mean 0.000 loop_ _atom_site_label _atom_site_type_symbol _atom_site_fract_x _atom_site_fract_y _atom_site_fract_z _atom_site_U_iso_or_equiv _atom_site_adp_type _atom_site_occupancy _atom_site_symmetry_multiplicity _atom_site_calc_flag _atom_site_refinement_flags _atom_site_disorder_assembly _atom_site_disorder_group Co1 Co 0.50064(4) 0.39190(12) 0.49137(2) 0.02124(14) Uani 0.50 1 d P . . S1 S 0.38778(4) 0.46408(17) 0.46245(2) 0.03740(17) Uani 1 1 d . . . S2 S 0.46970(7) 0.2630(7) 0.57121(7) 0.0274(6) Uani 0.505(5) 1 d P . 1 S3 S 0.46652(7) 0.0899(7) 0.55861(6) 0.0221(5) Uani 0.495(5) 1 d P . 2 C1 C 0.33726(14) 0.2526(6) 0.50900(9) 0.0301(5) Uani 1 1 d . . . C2 C 0.37189(15) 0.1297(6) 0.55436(9) 0.0324(5) Uani 1 1 d . . . C3 C 0.25698(17) 0.2072(6) 0.49868(10) 0.0375(6) Uani 1 1 d . . . C4 C 0.33238(16) -0.0534(6) 0.59363(9) 0.0351(6) Uani 1 1 d . . . C10 C 0.54762(12) 0.6856(4) 0.17453(8) 0.0211(4) Uani 1 1 d . . . C11 C 0.54558(12) 0.5995(4) 0.22963(8) 0.0202(4) Uani 1 1 d . . . C12 C 0.60234(13) 0.7217(5) 0.26468(8) 0.0247(5) Uani 1 1 d . . . H12 H 0.6013 0.6649 0.3015 0.030 Uiso 1 1 calc R . . C13 C 0.66032(13) 0.9237(5) 0.24744(9) 0.0267(5) Uani 1 1 d . . . H13 H 0.6978 1.0052 0.2724 0.032 Uiso 1 1 calc R . . C14 C 0.66357(13) 1.0061(5) 0.19428(9) 0.0269(5) Uani 1 1 d . . . H14 H 0.7035 1.1439 0.1827 0.032 Uiso 1 1 calc R . . C15 C 0.60811(13) 0.8878(5) 0.15667(9) 0.0236(4) Uani 1 1 d . . . C16 C 0.61134(14) 0.9700(5) 0.10219(9) 0.0287(5) Uani 1 1 d . . . H16 H 0.6517 1.1040 0.0903 0.034 Uiso 1 1 calc R . . C17 C 0.55683(14) 0.8584(5) 0.06627(9) 0.0307(5) Uani 1 1 d . . . H17 H 0.5598 0.9147 0.0296 0.037 Uiso 1 1 calc R . . C18 C 0.49722(14) 0.6638(5) 0.08290(9) 0.0269(5) Uani 1 1 d . . . H18 H 0.4597 0.5902 0.0574 0.032 Uiso 1 1 calc R . . C19 C 0.49119(12) 0.5732(4) 0.13670(8) 0.0203(4) Uani 1 1 d . . . C20 C 0.42878(13) 0.3678(5) 0.15483(8) 0.0215(4) Uani 1 1 d . . . C21 C 0.37111(13) 0.2523(5) 0.11994(9) 0.0267(5) Uani 1 1 d . . . H21 H 0.3724 0.3077 0.0831 0.032 Uiso 1 1 calc R . . C22 C 0.31183(14) 0.0579(5) 0.13762(10) 0.0304(5) Uani 1 1 d . . . H22 H 0.2725 -0.0120 0.1131 0.036 Uiso 1 1 calc R . . C23 C 0.31006(13) -0.0328(5) 0.19027(10) 0.0284(5) Uani 1 1 d . . . H23 H 0.2703 -0.1716 0.2017 0.034 Uiso 1 1 calc R . . C24 C 0.36617(13) 0.0763(5) 0.22761(9) 0.0245(5) Uani 1 1 d . . . C25 C 0.36441(13) -0.0115(5) 0.28195(9) 0.0277(5) Uani 1 1 d . . . H25 H 0.3248 -0.1499 0.2938 0.033 Uiso 1 1 calc R . . C26 C 0.41904(14) 0.0995(5) 0.31811(9) 0.0300(5) Uani 1 1 d . . . H26 H 0.4163 0.0416 0.3548 0.036 Uiso 1 1 calc R . . C27 C 0.47856(14) 0.2971(5) 0.30132(9) 0.0263(5) Uani 1 1 d . . . H27 H 0.5164 0.3695 0.3268 0.032 Uiso 1 1 calc R . . C28 C 0.48387(12) 0.3912(4) 0.24791(8) 0.0206(4) Uani 1 1 d . . . C29 C 0.42702(12) 0.2801(4) 0.20978(8) 0.0198(4) Uani 1 1 d . . . N1 N 0.19268(16) 0.1745(6) 0.49062(9) 0.0563(7) Uani 1 1 d . . . N2 N 0.30318(16) -0.2016(6) 0.62538(9) 0.0531(7) Uani 1 1 d . . . loop_ _atom_site_aniso_label _atom_site_aniso_U_11 _atom_site_aniso_U_22 _atom_site_aniso_U_33 _atom_site_aniso_U_23 _atom_site_aniso_U_13 _atom_site_aniso_U_12 Co1 0.0206(3) 0.0253(3) 0.0178(3) 0.0007(2) 0.0001(2) 0.0006(3) S1 0.0346(4) 0.0568(4) 0.0209(3) 0.0069(3) 0.0031(2) 0.0171(3) S2 0.0279(7) 0.0309(13) 0.0231(7) 0.0052(8) -0.0019(5) -0.0008(5) S3 0.0207(6) 0.0286(12) 0.0170(6) 0.0000(6) -0.0002(4) -0.0008(5) C1 0.0318(14) 0.0344(12) 0.0240(11) -0.0074(9) 0.0002(10) 0.0050(10) C2 0.0329(14) 0.0452(13) 0.0195(11) -0.0036(10) 0.0060(10) 0.0079(11) C3 0.0477(18) 0.0390(13) 0.0252(12) 0.0000(10) -0.0075(12) -0.0072(12) C4 0.0419(16) 0.0406(13) 0.0224(11) -0.0055(10) -0.0044(11) -0.0025(12) C10 0.0222(11) 0.0168(9) 0.0241(10) -0.0022(8) -0.0007(9) 0.0067(8) C11 0.0202(11) 0.0162(9) 0.0241(10) -0.0028(8) -0.0009(9) 0.0065(8) C12 0.0262(12) 0.0223(10) 0.0252(11) -0.0030(8) -0.0047(10) 0.0050(9) C13 0.0217(12) 0.0231(10) 0.0350(12) -0.0056(9) -0.0045(10) 0.0048(8) C14 0.0207(12) 0.0225(10) 0.0378(13) -0.0051(9) 0.0031(10) 0.0021(9) C15 0.0215(11) 0.0200(9) 0.0294(11) -0.0022(8) 0.0031(9) 0.0039(8) C16 0.0292(13) 0.0255(10) 0.0319(12) 0.0019(9) 0.0078(10) 0.0031(9) C17 0.0376(14) 0.0302(11) 0.0245(11) 0.0020(9) 0.0043(11) 0.0052(10) C18 0.0313(13) 0.0245(10) 0.0245(11) -0.0004(8) -0.0024(10) 0.0047(9) C19 0.0210(11) 0.0186(9) 0.0213(10) -0.0024(8) -0.0005(9) 0.0065(8) C20 0.0214(11) 0.0179(9) 0.0253(11) -0.0036(8) 0.0008(9) 0.0063(8) C21 0.0281(13) 0.0269(11) 0.0248(11) -0.0028(9) -0.0060(10) 0.0036(9) C22 0.0238(12) 0.0263(11) 0.0406(13) -0.0082(10) -0.0055(11) 0.0016(9) C23 0.0212(12) 0.0227(10) 0.0413(13) -0.0031(9) 0.0009(10) 0.0006(9) C24 0.0236(12) 0.0167(9) 0.0333(12) -0.0009(8) 0.0039(9) 0.0055(8) C25 0.0260(13) 0.0220(10) 0.0356(12) 0.0052(9) 0.0069(10) 0.0050(9) C26 0.0332(13) 0.0289(11) 0.0283(11) 0.0056(9) 0.0063(10) 0.0088(10) C27 0.0292(13) 0.0251(10) 0.0244(11) -0.0003(8) -0.0018(10) 0.0047(9) C28 0.0235(12) 0.0156(9) 0.0226(10) -0.0011(7) -0.0011(9) 0.0065(8) C29 0.0181(11) 0.0160(9) 0.0252(10) -0.0018(8) -0.0011(9) 0.0045(8) N1 0.0534(17) 0.0773(17) 0.0369(13) 0.0047(12) -0.0148(13) -0.0259(15) N2 0.0603(17) 0.0604(14) 0.0380(13) 0.0055(12) -0.0070(13) -0.0208(13) _geom_special_details ; All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. ; loop_ _geom_bond_atom_site_label_1 _geom_bond_atom_site_label_2 _geom_bond_distance _geom_bond_site_symmetry_2 _geom_bond_publ_flag Co1 S1 2.1046(9) . ? Co1 S2 2.1540(14) . ? Co1 S2 2.1796(15) 3_666 ? Co1 S3 2.1841(15) . ? Co1 S1 2.3133(9) 3_666 ? Co1 S3 2.405(3) 3_656 ? Co1 S3 2.527(2) 3_666 ? S1 C1 1.719(3) . ? S1 Co1 2.3133(9) 3_666 ? S2 C2 1.834(3) . ? S2 Co1 2.1796(15) 3_666 ? S3 C2 1.668(3) . ? S3 Co1 2.405(3) 3_656 ? S3 Co1 2.527(2) 3_666 ? C1 C2 1.364(3) . ? C1 C3 1.435(4) . ? C2 C4 1.431(3) . ? C3 N1 1.147(4) . ? C4 N2 1.134(3) . ? C10 C19 1.421(3) . ? C10 C11 1.425(3) . ? C10 C15 1.427(3) . ? C11 C12 1.395(3) . ? C11 C28 1.461(3) . ? C12 C13 1.388(3) . ? C13 C14 1.375(3) . ? C14 C15 1.414(3) . ? C15 C16 1.407(3) . ? C16 C17 1.367(3) . ? C17 C18 1.387(3) . ? C18 C19 1.404(3) . ? C19 C20 1.462(3) . ? C20 C21 1.395(3) . ? C20 C29 1.422(3) . ? C21 C22 1.391(3) . ? C22 C23 1.370(3) . ? C23 C24 1.405(3) . ? C24 C25 1.408(3) . ? C24 C29 1.435(3) . ? C25 C26 1.371(3) . ? C26 C27 1.394(3) . ? C27 C28 1.397(3) . ? C28 C29 1.429(3) . ? loop_ _geom_angle_atom_site_label_1 _geom_angle_atom_site_label_2 _geom_angle_atom_site_label_3 _geom_angle _geom_angle_site_symmetry_1 _geom_angle_site_symmetry_3 _geom_angle_publ_flag Co1 Co1 S1 89.46(7) 3_666 . ? Co1 Co1 S2 78.39(11) 3_666 . ? S1 Co1 S2 95.07(4) . . ? Co1 Co1 S2 75.48(10) 3_666 3_666 ? S1 Co1 S2 84.75(4) . 3_666 ? S2 Co1 S2 153.87(3) . 3_666 ? Co1 Co1 S3 98.82(10) 3_666 . ? S1 Co1 S3 93.63(4) . . ? S2 Co1 S3 20.50(4) . . ? S2 Co1 S3 174.06(5) 3_666 . ? Co1 Co1 S1 65.47(7) 3_666 3_666 ? S1 Co1 S1 154.93(3) . 3_666 ? S2 Co1 S1 80.47(6) . 3_666 ? S2 Co1 S1 88.68(6) 3_666 3_666 ? S3 Co1 S1 90.42(5) . 3_666 ? Co1 Co1 S3 165.79(9) 3_666 3_656 ? S1 Co1 S3 100.04(4) . 3_656 ? S2 Co1 S3 110.93(7) . 3_656 ? S2 Co1 S3 94.76(7) 3_666 3_656 ? S3 Co1 S3 91.15(7) . 3_656 ? S1 Co1 S3 104.60(4) 3_666 3_656 ? Co1 Co1 S3 58.65(8) 3_666 3_666 ? S1 Co1 S3 86.65(4) . 3_666 ? S2 Co1 S3 137.01(5) . 3_666 ? S2 Co1 S3 16.90(5) 3_666 3_666 ? S3 Co1 S3 157.47(4) . 3_666 ? S1 Co1 S3 80.37(4) 3_666 3_666 ? S3 Co1 S3 111.01(6) 3_656 3_666 ? C1 S1 Co1 101.44(9) . . ? C1 S1 Co1 103.61(9) . 3_666 ? Co1 S1 Co1 25.07(3) . 3_666 ? C2 S2 Co1 97.05(11) . . ? C2 S2 Co1 105.66(9) . 3_666 ? Co1 S2 Co1 26.13(3) . 3_666 ? C2 S3 Co1 101.27(10) . . ? C2 S3 Co1 107.58(15) . 3_656 ? Co1 S3 Co1 88.85(7) . 3_656 ? C2 S3 Co1 97.54(12) . 3_666 ? Co1 S3 Co1 22.53(4) . 3_666 ? Co1 S3 Co1 111.01(6) 3_656 3_666 ? C2 C1 C3 120.6(2) . . ? C2 C1 S1 121.5(2) . . ? C3 C1 S1 117.94(18) . . ? C1 C2 C4 123.4(2) . . ? C1 C2 S3 120.13(19) . . ? C4 C2 S3 114.25(19) . . ? C1 C2 S2 117.96(19) . . ? C4 C2 S2 117.87(18) . . ? S3 C2 S2 24.90(6) . . ? N1 C3 C1 179.2(3) . . ? N2 C4 C2 177.9(3) . . ? C19 C10 C11 121.7(2) . . ? C19 C10 C15 119.00(19) . . ? C11 C10 C15 119.28(19) . . ? C12 C11 C10 118.7(2) . . ? C12 C11 C28 121.99(19) . . ? C10 C11 C28 119.33(19) . . ? C13 C12 C11 122.0(2) . . ? C14 C13 C12 120.1(2) . . ? C13 C14 C15 120.7(2) . . ? C16 C15 C14 120.9(2) . . ? C16 C15 C10 119.7(2) . . ? C14 C15 C10 119.3(2) . . ? C17 C16 C15 120.5(2) . . ? C16 C17 C18 120.6(2) . . ? C17 C18 C19 121.4(2) . . ? C18 C19 C10 118.7(2) . . ? C18 C19 C20 122.02(19) . . ? C10 C19 C20 119.24(18) . . ? C21 C20 C29 118.8(2) . . ? C21 C20 C19 122.20(19) . . ? C29 C20 C19 119.04(19) . . ? C22 C21 C20 121.8(2) . . ? C23 C22 C21 120.1(2) . . ? C22 C23 C24 121.1(2) . . ? C23 C24 C25 121.6(2) . . ? C23 C24 C29 119.1(2) . . ? C25 C24 C29 119.3(2) . . ? C26 C25 C24 121.0(2) . . ? C25 C26 C27 120.3(2) . . ? C26 C27 C28 121.5(2) . . ? C27 C28 C29 119.0(2) . . ? C27 C28 C11 122.26(19) . . ? C29 C28 C11 118.77(18) . . ? C20 C29 C28 121.9(2) . . ? C20 C29 C24 119.16(19) . . ? C28 C29 C24 118.95(19) . . ? _diffrn_measured_fraction_theta_max 0.795 _diffrn_reflns_theta_full 28.41 _diffrn_measured_fraction_theta_full 0.795 _refine_diff_density_max 0.250 _refine_diff_density_min -0.461 _refine_diff_density_rms 0.049 # start Validation Reply Form _vrf_REFLT03_p21n ; PROBLEM: Reflection count < 85% complete (theta max?) RESPONSE:The crystals obtained were of poor quality, which results in a weak data set and low fraction (0.795) of measured theta full. ; _vrf_PLAT029_p21n ; PROBLEM: _diffrn_measured_fraction_theta_full Low ....... 0.80 RESPONSE: The crystals obtained were of poor quality, which results in a weak data set and low fraction (0.795) of measured theta full. ; # end Validation Reply Form