# Electronic Supplementary Material (ESI) for Chemical Communications # This journal is © The Royal Society of Chemistry 2013 ####################################################################### # # Cambridge Crystallographic Data Centre # CCDC # ####################################################################### # # This CIF contains data from an original supplementary publication # deposited with the CCDC, and may include chemical, crystal, # experimental, refinement, atomic coordinates, # anisotropic displacement parameters and molecular geometry data, # as required by the journal to which it was submitted. # # This CIF is provided on the understanding that it is used for bona # fide research purposes only. It may contain copyright material # of the CCDC or of third parties, and may not be copied or further # disseminated in any form, whether machine-readable or not, # except for the purpose of generating routine backup copies # on your local computer system. # # For further information on the CCDC, data deposition and # data retrieval see: # www.ccdc.cam.ac.uk # # Bona fide researchers may freely download Mercury and enCIFer # from this site to visualise CIF-encoded structures and # to carry out CIF format checking respectively. # ####################################################################### data_IRMOF-3-AM4XL _database_code_depnum_ccdc_archive 'CCDC 906534' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C24 O13 Zn4' _chemical_formula_sum 'C24 H0 N0 O13 Zn4' _chemical_formula_weight 759.72 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' O O 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Zn Zn 0.2839 1.4301 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Cubic _symmetry_space_group_name_H-M Fm-3m loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-y, x, z' '-x, -y, z' 'y, -x, z' 'x, -z, y' 'x, -y, -z' 'x, z, -y' 'z, y, -x' '-x, y, -z' '-z, y, x' 'z, x, y' 'y, z, x' '-y, -z, x' 'z, -x, -y' '-y, z, -x' '-z, -x, y' '-z, x, -y' 'y, -z, -x' 'y, x, -z' '-y, -x, -z' '-x, z, y' '-x, -z, -y' 'z, -y, x' '-z, -y, -x' 'x, y+1/2, z+1/2' '-y, x+1/2, z+1/2' '-x, -y+1/2, z+1/2' 'y, -x+1/2, z+1/2' 'x, -z+1/2, y+1/2' 'x, -y+1/2, -z+1/2' 'x, z+1/2, -y+1/2' 'z, y+1/2, -x+1/2' '-x, y+1/2, -z+1/2' '-z, y+1/2, x+1/2' 'z, x+1/2, y+1/2' 'y, z+1/2, x+1/2' '-y, -z+1/2, x+1/2' 'z, -x+1/2, -y+1/2' '-y, z+1/2, -x+1/2' '-z, -x+1/2, y+1/2' '-z, x+1/2, -y+1/2' 'y, -z+1/2, -x+1/2' 'y, x+1/2, -z+1/2' '-y, -x+1/2, -z+1/2' '-x, z+1/2, y+1/2' '-x, -z+1/2, -y+1/2' 'z, -y+1/2, x+1/2' '-z, -y+1/2, -x+1/2' 'x+1/2, y, z+1/2' '-y+1/2, x, z+1/2' '-x+1/2, -y, z+1/2' 'y+1/2, -x, z+1/2' 'x+1/2, -z, y+1/2' 'x+1/2, -y, -z+1/2' 'x+1/2, z, -y+1/2' 'z+1/2, y, -x+1/2' '-x+1/2, y, -z+1/2' '-z+1/2, y, x+1/2' 'z+1/2, x, y+1/2' 'y+1/2, z, x+1/2' '-y+1/2, -z, x+1/2' 'z+1/2, -x, -y+1/2' '-y+1/2, z, -x+1/2' '-z+1/2, -x, y+1/2' '-z+1/2, x, -y+1/2' 'y+1/2, -z, -x+1/2' 'y+1/2, x, -z+1/2' '-y+1/2, -x, -z+1/2' '-x+1/2, z, y+1/2' '-x+1/2, -z, -y+1/2' 'z+1/2, -y, x+1/2' '-z+1/2, -y, -x+1/2' 'x+1/2, y+1/2, z' '-y+1/2, x+1/2, z' '-x+1/2, -y+1/2, z' 'y+1/2, -x+1/2, z' 'x+1/2, -z+1/2, y' 'x+1/2, -y+1/2, -z' 'x+1/2, z+1/2, -y' 'z+1/2, y+1/2, -x' '-x+1/2, y+1/2, -z' '-z+1/2, y+1/2, x' 'z+1/2, x+1/2, y' 'y+1/2, z+1/2, x' '-y+1/2, -z+1/2, x' 'z+1/2, -x+1/2, -y' '-y+1/2, z+1/2, -x' '-z+1/2, -x+1/2, y' '-z+1/2, x+1/2, -y' 'y+1/2, -z+1/2, -x' 'y+1/2, x+1/2, -z' '-y+1/2, -x+1/2, -z' '-x+1/2, z+1/2, y' '-x+1/2, -z+1/2, -y' 'z+1/2, -y+1/2, x' '-z+1/2, -y+1/2, -x' '-x, -y, -z' 'y, -x, -z' 'x, y, -z' '-y, x, -z' '-x, z, -y' '-x, y, z' '-x, -z, y' '-z, -y, x' 'x, -y, z' 'z, -y, -x' '-z, -x, -y' '-y, -z, -x' 'y, z, -x' '-z, x, y' 'y, -z, x' 'z, x, -y' 'z, -x, y' '-y, z, x' '-y, -x, z' 'y, x, z' 'x, -z, -y' 'x, z, y' '-z, y, -x' 'z, y, x' '-x, -y+1/2, -z+1/2' 'y, -x+1/2, -z+1/2' 'x, y+1/2, -z+1/2' '-y, x+1/2, -z+1/2' '-x, z+1/2, -y+1/2' '-x, y+1/2, z+1/2' '-x, -z+1/2, y+1/2' '-z, -y+1/2, x+1/2' 'x, -y+1/2, z+1/2' 'z, -y+1/2, -x+1/2' '-z, -x+1/2, -y+1/2' '-y, -z+1/2, -x+1/2' 'y, z+1/2, -x+1/2' '-z, x+1/2, y+1/2' 'y, -z+1/2, x+1/2' 'z, x+1/2, -y+1/2' 'z, -x+1/2, y+1/2' '-y, z+1/2, x+1/2' '-y, -x+1/2, z+1/2' 'y, x+1/2, z+1/2' 'x, -z+1/2, -y+1/2' 'x, z+1/2, y+1/2' '-z, y+1/2, -x+1/2' 'z, y+1/2, x+1/2' '-x+1/2, -y, -z+1/2' 'y+1/2, -x, -z+1/2' 'x+1/2, y, -z+1/2' '-y+1/2, x, -z+1/2' '-x+1/2, z, -y+1/2' '-x+1/2, y, z+1/2' '-x+1/2, -z, y+1/2' '-z+1/2, -y, x+1/2' 'x+1/2, -y, z+1/2' 'z+1/2, -y, -x+1/2' '-z+1/2, -x, -y+1/2' '-y+1/2, -z, -x+1/2' 'y+1/2, z, -x+1/2' '-z+1/2, x, y+1/2' 'y+1/2, -z, x+1/2' 'z+1/2, x, -y+1/2' 'z+1/2, -x, y+1/2' '-y+1/2, z, x+1/2' '-y+1/2, -x, z+1/2' 'y+1/2, x, z+1/2' 'x+1/2, -z, -y+1/2' 'x+1/2, z, y+1/2' '-z+1/2, y, -x+1/2' 'z+1/2, y, x+1/2' '-x+1/2, -y+1/2, -z' 'y+1/2, -x+1/2, -z' 'x+1/2, y+1/2, -z' '-y+1/2, x+1/2, -z' '-x+1/2, z+1/2, -y' '-x+1/2, y+1/2, z' '-x+1/2, -z+1/2, y' '-z+1/2, -y+1/2, x' 'x+1/2, -y+1/2, z' 'z+1/2, -y+1/2, -x' '-z+1/2, -x+1/2, -y' '-y+1/2, -z+1/2, -x' 'y+1/2, z+1/2, -x' '-z+1/2, x+1/2, y' 'y+1/2, -z+1/2, x' 'z+1/2, x+1/2, -y' 'z+1/2, -x+1/2, y' '-y+1/2, z+1/2, x' '-y+1/2, -x+1/2, z' 'y+1/2, x+1/2, z' 'x+1/2, -z+1/2, -y' 'x+1/2, z+1/2, y' '-z+1/2, y+1/2, -x' 'z+1/2, y+1/2, x' _cell_length_a 25.543(2) _cell_length_b 25.543(2) _cell_length_c 25.543(2) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 16666(3) _cell_formula_units_Z 8 _cell_measurement_temperature 250(2) _cell_measurement_reflns_used 622 _cell_measurement_theta_min 4.51 _cell_measurement_theta_max 19.51 _exptl_crystal_description 'square block' _exptl_crystal_colour colorless _exptl_crystal_size_max 0.10 _exptl_crystal_size_mid 0.10 _exptl_crystal_size_min 0.05 _exptl_crystal_density_meas 'not measured' _exptl_crystal_density_diffrn 0.604 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 2944 _exptl_absorpt_coefficient_mu 1.159 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.8159 _exptl_absorpt_correction_T_max 0.9187 _exptl_absorpt_process_details SADABS _exptl_special_details ; ? ; _diffrn_ambient_temperature 250(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 APEX-II CCD' _diffrn_measurement_method '\f and \w scans' _diffrn_reflns_number 2430 _diffrn_reflns_av_R_equivalents 0.0326 _diffrn_reflns_av_sigmaI/netI 0.0233 _diffrn_reflns_limit_h_min -19 _diffrn_reflns_limit_h_max 5 _diffrn_reflns_limit_k_min -19 _diffrn_reflns_limit_k_max 24 _diffrn_reflns_limit_l_min -23 _diffrn_reflns_limit_l_max 24 _diffrn_reflns_theta_min 3.19 _diffrn_reflns_theta_max 19.72 _reflns_number_total 430 _reflns_number_gt 284 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker APEX2' _computing_cell_refinement 'Bruker SAINT' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics 'Bruker SHELXTL' _computing_publication_material 'Bruker SHELXTL' _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. Due to weak diffraction, CheckCif reported Alert_A on low theta_max/ wavelength. Due to the severe disorders, we cannot locate the substituents on the ligands. SQUEEZE protocol has found 1304 electrons that can be accounted for the disordered solvents and substituents. ; _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^)+(0.2000P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens constr _refine_ls_hydrogen_treatment constr _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 430 _refine_ls_number_parameters 25 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.1108 _refine_ls_R_factor_gt 0.0900 _refine_ls_wR_factor_ref 0.2908 _refine_ls_wR_factor_gt 0.2624 _refine_ls_goodness_of_fit_ref 1.132 _refine_ls_restrained_S_all 1.132 _refine_ls_shift/su_max 0.000 _refine_ls_shift/su_mean 0.000 loop_ _platon_squeeze_void_nr _platon_squeeze_void_average_x _platon_squeeze_void_average_y _platon_squeeze_void_average_z _platon_squeeze_void_volume _platon_squeeze_void_count_electrons _platon_squeeze_void_content 1 -0.014 -0.007 -0.006 12993 1304 ' ' _platon_squeeze_details ; ; 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 Zn1 Zn 0.79368(5) 0.70632(5) 0.29368(5) 0.1452(19) Uani 1 6 d S . . O13 O 0.7824(4) 0.6343(5) 0.2824(4) 0.229(6) Uani 1 2 d S . . O1 O 0.7500 0.7500 0.2500 0.125(7) Uani 1 24 d S . . C2 C 0.7500 0.6126(8) 0.2500 0.218(11) Uani 1 4 d S . . C1 C 0.7223(8) 0.5238(7) 0.2223(8) 0.308(15) Uani 1 2 d S . . C3 C 0.7500 0.5552(10) 0.2500 0.193(8) Uani 1 4 d S . . 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 Zn1 0.1452(19) 0.1452(19) 0.1452(19) 0.0067(7) -0.0067(7) 0.0067(7) O13 0.264(9) 0.159(10) 0.264(9) -0.020(6) -0.019(8) -0.020(6) O1 0.125(7) 0.125(7) 0.125(7) 0.000 0.000 0.000 C2 0.28(2) 0.094(16) 0.28(2) 0.000 -0.02(3) 0.000 C1 0.39(2) 0.139(14) 0.39(2) -0.026(8) -0.10(3) -0.026(8) C3 0.209(14) 0.16(2) 0.209(14) 0.000 -0.037(15) 0.000 _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 Zn1 O13 1.883(12) . ? Zn1 O13 1.883(12) 86_566 ? Zn1 O13 1.883(12) 61_664 ? Zn1 O1 1.933(2) . ? Zn1 Zn1 3.156(4) 122_565 ? Zn1 Zn1 3.156(4) 75_665 ? Zn1 Zn1 3.156(4) 148_655 ? O13 C2 1.294(11) . ? O1 Zn1 1.933(2) 122_565 ? O1 Zn1 1.933(2) 148_655 ? O1 Zn1 1.933(2) 75_665 ? C2 O13 1.295(11) 57_655 ? C2 C3 1.47(3) . ? C1 C1 1.21(3) 105_565 ? C1 C3 1.28(2) . ? C1 C1 2.00(6) 57_655 ? C3 C1 1.28(2) 57_655 ? 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 O13 Zn1 O13 106.0(4) . 86_566 ? O13 Zn1 O13 106.0(4) . 61_664 ? O13 Zn1 O13 106.0(4) 86_566 61_664 ? O13 Zn1 O1 112.7(4) . . ? O13 Zn1 O1 112.7(4) 86_566 . ? O13 Zn1 O1 112.7(4) 61_664 . ? O13 Zn1 Zn1 77.5(4) . 122_565 ? O13 Zn1 Zn1 125.6(3) 86_566 122_565 ? O13 Zn1 Zn1 125.6(3) 61_664 122_565 ? O1 Zn1 Zn1 35.3 . 122_565 ? O13 Zn1 Zn1 125.6(3) . 75_665 ? O13 Zn1 Zn1 77.5(4) 86_566 75_665 ? O13 Zn1 Zn1 125.6(3) 61_664 75_665 ? O1 Zn1 Zn1 35.3 . 75_665 ? Zn1 Zn1 Zn1 60.0 122_565 75_665 ? O13 Zn1 Zn1 125.6(3) . 148_655 ? O13 Zn1 Zn1 125.6(3) 86_566 148_655 ? O13 Zn1 Zn1 77.5(4) 61_664 148_655 ? O1 Zn1 Zn1 35.3 . 148_655 ? Zn1 Zn1 Zn1 60.0 122_565 148_655 ? Zn1 Zn1 Zn1 59.999(1) 75_665 148_655 ? C2 O13 Zn1 127.9(13) . . ? Zn1 O1 Zn1 109.475(1) . 122_565 ? Zn1 O1 Zn1 109.474(1) . 148_655 ? Zn1 O1 Zn1 109.5 122_565 148_655 ? Zn1 O1 Zn1 109.5 . 75_665 ? Zn1 O1 Zn1 109.468(1) 122_565 75_665 ? Zn1 O1 Zn1 109.468(2) 148_655 75_665 ? O13 C2 O13 129(2) . 57_655 ? O13 C2 C3 115.4(10) . . ? O13 C2 C3 115.4(10) 57_655 . ? C1 C1 C3 128.8(15) 105_565 . ? C1 C1 C1 90.000(3) 105_565 57_655 ? C3 C1 C1 38.8(15) . 57_655 ? C1 C3 C1 102(3) . 57_655 ? C1 C3 C2 128.8(15) . . ? C1 C3 C2 128.8(15) 57_655 . ? _diffrn_measured_fraction_theta_max 0.986 _diffrn_reflns_theta_full 19.72 _diffrn_measured_fraction_theta_full 0.986 _refine_diff_density_max 0.466 _refine_diff_density_min -0.540 _refine_diff_density_rms 0.067 data_IRMOF-3-AM7XL _database_code_depnum_ccdc_archive 'CCDC 906535' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C24 H0 N0 O13 Zn4' _chemical_formula_sum 'C24 H0 N0 O13 Zn4' _chemical_formula_weight 757.72 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' O O 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Zn Zn 0.2839 1.4301 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Cubic _symmetry_space_group_name_H-M Fm-3m loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z' '-x, y, -z' 'x, -y, -z' 'z, x, y' 'z, -x, -y' '-z, -x, y' '-z, x, -y' 'y, z, x' '-y, z, -x' 'y, -z, -x' '-y, -z, x' 'y, x, -z' '-y, -x, -z' 'y, -x, z' '-y, x, z' 'x, z, -y' '-x, z, y' '-x, -z, -y' 'x, -z, y' 'z, y, -x' 'z, -y, x' '-z, y, x' '-z, -y, -x' 'x, y+1/2, z+1/2' '-x, -y+1/2, z+1/2' '-x, y+1/2, -z+1/2' 'x, -y+1/2, -z+1/2' 'z, x+1/2, y+1/2' 'z, -x+1/2, -y+1/2' '-z, -x+1/2, y+1/2' '-z, x+1/2, -y+1/2' 'y, z+1/2, x+1/2' '-y, z+1/2, -x+1/2' 'y, -z+1/2, -x+1/2' '-y, -z+1/2, x+1/2' 'y, x+1/2, -z+1/2' '-y, -x+1/2, -z+1/2' 'y, -x+1/2, z+1/2' '-y, x+1/2, z+1/2' 'x, z+1/2, -y+1/2' '-x, z+1/2, y+1/2' '-x, -z+1/2, -y+1/2' 'x, -z+1/2, y+1/2' 'z, y+1/2, -x+1/2' 'z, -y+1/2, x+1/2' '-z, y+1/2, x+1/2' '-z, -y+1/2, -x+1/2' 'x+1/2, y, z+1/2' '-x+1/2, -y, z+1/2' '-x+1/2, y, -z+1/2' 'x+1/2, -y, -z+1/2' 'z+1/2, x, y+1/2' 'z+1/2, -x, -y+1/2' '-z+1/2, -x, y+1/2' '-z+1/2, x, -y+1/2' 'y+1/2, z, x+1/2' '-y+1/2, z, -x+1/2' 'y+1/2, -z, -x+1/2' '-y+1/2, -z, x+1/2' 'y+1/2, x, -z+1/2' '-y+1/2, -x, -z+1/2' 'y+1/2, -x, z+1/2' '-y+1/2, x, z+1/2' 'x+1/2, z, -y+1/2' '-x+1/2, z, y+1/2' '-x+1/2, -z, -y+1/2' 'x+1/2, -z, y+1/2' 'z+1/2, y, -x+1/2' 'z+1/2, -y, x+1/2' '-z+1/2, y, x+1/2' '-z+1/2, -y, -x+1/2' 'x+1/2, y+1/2, z' '-x+1/2, -y+1/2, z' '-x+1/2, y+1/2, -z' 'x+1/2, -y+1/2, -z' 'z+1/2, x+1/2, y' 'z+1/2, -x+1/2, -y' '-z+1/2, -x+1/2, y' '-z+1/2, x+1/2, -y' 'y+1/2, z+1/2, x' '-y+1/2, z+1/2, -x' 'y+1/2, -z+1/2, -x' '-y+1/2, -z+1/2, x' 'y+1/2, x+1/2, -z' '-y+1/2, -x+1/2, -z' 'y+1/2, -x+1/2, z' '-y+1/2, x+1/2, z' 'x+1/2, z+1/2, -y' '-x+1/2, z+1/2, y' '-x+1/2, -z+1/2, -y' 'x+1/2, -z+1/2, y' 'z+1/2, y+1/2, -x' 'z+1/2, -y+1/2, x' '-z+1/2, y+1/2, x' '-z+1/2, -y+1/2, -x' '-x, -y, -z' 'x, y, -z' 'x, -y, z' '-x, y, z' '-z, -x, -y' '-z, x, y' 'z, x, -y' 'z, -x, y' '-y, -z, -x' 'y, -z, x' '-y, z, x' 'y, z, -x' '-y, -x, z' 'y, x, z' '-y, x, -z' 'y, -x, -z' '-x, -z, y' 'x, -z, -y' 'x, z, y' '-x, z, -y' '-z, -y, x' '-z, y, -x' 'z, -y, -x' 'z, y, x' '-x, -y+1/2, -z+1/2' 'x, y+1/2, -z+1/2' 'x, -y+1/2, z+1/2' '-x, y+1/2, z+1/2' '-z, -x+1/2, -y+1/2' '-z, x+1/2, y+1/2' 'z, x+1/2, -y+1/2' 'z, -x+1/2, y+1/2' '-y, -z+1/2, -x+1/2' 'y, -z+1/2, x+1/2' '-y, z+1/2, x+1/2' 'y, z+1/2, -x+1/2' '-y, -x+1/2, z+1/2' 'y, x+1/2, z+1/2' '-y, x+1/2, -z+1/2' 'y, -x+1/2, -z+1/2' '-x, -z+1/2, y+1/2' 'x, -z+1/2, -y+1/2' 'x, z+1/2, y+1/2' '-x, z+1/2, -y+1/2' '-z, -y+1/2, x+1/2' '-z, y+1/2, -x+1/2' 'z, -y+1/2, -x+1/2' 'z, y+1/2, x+1/2' '-x+1/2, -y, -z+1/2' 'x+1/2, y, -z+1/2' 'x+1/2, -y, z+1/2' '-x+1/2, y, z+1/2' '-z+1/2, -x, -y+1/2' '-z+1/2, x, y+1/2' 'z+1/2, x, -y+1/2' 'z+1/2, -x, y+1/2' '-y+1/2, -z, -x+1/2' 'y+1/2, -z, x+1/2' '-y+1/2, z, x+1/2' 'y+1/2, z, -x+1/2' '-y+1/2, -x, z+1/2' 'y+1/2, x, z+1/2' '-y+1/2, x, -z+1/2' 'y+1/2, -x, -z+1/2' '-x+1/2, -z, y+1/2' 'x+1/2, -z, -y+1/2' 'x+1/2, z, y+1/2' '-x+1/2, z, -y+1/2' '-z+1/2, -y, x+1/2' '-z+1/2, y, -x+1/2' 'z+1/2, -y, -x+1/2' 'z+1/2, y, x+1/2' '-x+1/2, -y+1/2, -z' 'x+1/2, y+1/2, -z' 'x+1/2, -y+1/2, z' '-x+1/2, y+1/2, z' '-z+1/2, -x+1/2, -y' '-z+1/2, x+1/2, y' 'z+1/2, x+1/2, -y' 'z+1/2, -x+1/2, y' '-y+1/2, -z+1/2, -x' 'y+1/2, -z+1/2, x' '-y+1/2, z+1/2, x' 'y+1/2, z+1/2, -x' '-y+1/2, -x+1/2, z' 'y+1/2, x+1/2, z' '-y+1/2, x+1/2, -z' 'y+1/2, -x+1/2, -z' '-x+1/2, -z+1/2, y' 'x+1/2, -z+1/2, -y' 'x+1/2, z+1/2, y' '-x+1/2, z+1/2, -y' '-z+1/2, -y+1/2, x' '-z+1/2, y+1/2, -x' 'z+1/2, -y+1/2, -x' 'z+1/2, y+1/2, x' _cell_length_a 25.654(19) _cell_length_b 25.654(19) _cell_length_c 25.654(19) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 16884(22) _cell_formula_units_Z 8 _cell_measurement_temperature 250(2) _cell_measurement_reflns_used 568 _cell_measurement_theta_min 4.49 _cell_measurement_theta_max 19.49 _exptl_crystal_description block _exptl_crystal_colour colourless _exptl_crystal_size_min 0.20 _exptl_crystal_size_mid 0.40 _exptl_crystal_size_max 0.40 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 0.596 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 2944 _exptl_absorpt_coefficient_mu 1.144 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.8952 _exptl_absorpt_correction_T_max 0.9432 _exptl_absorpt_process_details SADABS _exptl_special_details ; ? ; _diffrn_ambient_temperature 250(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 APEX-II CCD' _diffrn_measurement_method '\f and \w scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number ? _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 1773 _diffrn_reflns_av_R_equivalents 0.1061 _diffrn_reflns_av_sigmaI/netI 0.0898 _diffrn_reflns_limit_h_min -22 _diffrn_reflns_limit_h_max 24 _diffrn_reflns_limit_k_min -19 _diffrn_reflns_limit_k_max 24 _diffrn_reflns_limit_l_min -18 _diffrn_reflns_limit_l_max 6 _diffrn_reflns_theta_min 2.63 _diffrn_reflns_theta_max 19.70 _reflns_number_total 418 _reflns_number_gt 227 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker APEX2' _computing_cell_refinement 'Bruker SAINT' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics 'Bruker SHELXTL' _computing_publication_material 'Bruker SHELXTL' _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 structure of IRMOF_Az was collected at 250 K because at lower temperature, the diffraction was weak and the resolution was low. The organic linkers are severely disordered and distored, thus we cannot locate the substituents and C1 and C2 have to be refined as isotropically rather than anisotropically.Due to the low resolution and weak diffraction, CheckCif reported Alert_A on low value of theta_max/wavelenght. SQUEEZE protocol has found 2124 electrons that can be accounted for the disordered solvent molecules and substituents. ; _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^)+(0.2000P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens constr _refine_ls_hydrogen_treatment constr _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 418 _refine_ls_number_parameters 21 _refine_ls_number_restraints 1 _refine_ls_R_factor_all 0.1454 _refine_ls_R_factor_gt 0.1074 _refine_ls_wR_factor_ref 0.3421 _refine_ls_wR_factor_gt 0.2889 _refine_ls_goodness_of_fit_ref 1.107 _refine_ls_restrained_S_all 1.119 _refine_ls_shift/su_max 0.000 _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 O1 O 0.2146(4) 0.1334(5) 0.2146(4) 0.188(6) Uani 1 2 d S . . O2 O 0.2500 0.2500 0.2500 0.133(12) Uani 1 24 d S . . C3 C 0.2189(8) 0.0230(7) 0.2189(8) 0.243(14) Uani 1 2 d S . . C1 C 0.2500 0.1152(18) 0.2500 0.187(14) Uiso 1 4 d SD . . C2 C 0.2500 0.0562(19) 0.2500 0.239(18) Uiso 1 4 d SD . . Zn1 Zn 0.20639(7) 0.20639(7) 0.20639(7) 0.124(2) Uani 1 6 d S . . 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 O1 0.200(9) 0.162(12) 0.200(9) -0.015(7) 0.031(10) -0.015(7) O2 0.133(12) 0.133(12) 0.133(12) 0.000 0.000 0.000 C3 0.30(2) 0.127(17) 0.30(2) 0.004(12) 0.00(2) 0.004(12) Zn1 0.124(2) 0.124(2) 0.124(2) -0.0025(10) -0.0025(10) -0.0025(10) loop_ _platon_squeeze_void_nr _platon_squeeze_void_average_x _platon_squeeze_void_average_y _platon_squeeze_void_average_z _platon_squeeze_void_volume _platon_squeeze_void_count_electrons _platon_squeeze_void_content 1 -0.014 -0.007 -0.006 13163 2124 ' ' _platon_squeeze_details ; ; _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 O1 C1 1.367(16) . ? O1 Zn1 1.895(14) . ? O2 Zn1 1.938(4) 28 ? O2 Zn1 1.938(4) 74 ? O2 Zn1 1.938(4) . ? O2 Zn1 1.938(4) 51 ? C3 C3 1.18(4) 99 ? C3 C2 1.41(3) . ? C1 O1 1.367(16) 51 ? C1 C2 1.513(19) . ? C2 C3 1.41(3) 51 ? Zn1 O1 1.895(14) 9 ? Zn1 O1 1.895(14) 5 ? 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 C1 O1 Zn1 119(2) . . ? Zn1 O2 Zn1 109.474(1) 28 74 ? Zn1 O2 Zn1 109.5 28 . ? Zn1 O2 Zn1 109.5 74 . ? Zn1 O2 Zn1 109.5 28 51 ? Zn1 O2 Zn1 109.472(1) 74 51 ? Zn1 O2 Zn1 109.5 . 51 ? C3 C3 C2 127(2) 99 . ? O1 C1 O1 140(4) 51 . ? O1 C1 C2 110(2) 51 . ? O1 C1 C2 110(2) . . ? C3 C2 C3 106(4) 51 . ? C3 C2 C1 127(2) 51 . ? C3 C2 C1 127(2) . . ? O1 Zn1 O1 101.9(6) . 9 ? O1 Zn1 O1 101.9(6) . 5 ? O1 Zn1 O1 101.9(6) 9 5 ? O1 Zn1 O2 116.2(5) . . ? O1 Zn1 O2 116.2(5) 9 . ? O1 Zn1 O2 116.2(5) 5 . ? _diffrn_measured_fraction_theta_max 0.957 _diffrn_reflns_theta_full 19.70 _diffrn_measured_fraction_theta_full 0.957 _refine_diff_density_max 0.718 _refine_diff_density_min -0.744 _refine_diff_density_rms 0.089 data_IRMOF-3-AM3XL _database_code_depnum_ccdc_archive 'CCDC 906536' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety ? _chemical_formula_sum 'C24 H9 N0 O13 Zn4' _chemical_formula_weight 766.79 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0181 0.0091 '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 0.0311 0.0180 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' O O 0.0492 0.0322 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Zn Zn -1.5491 0.6778 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Cubic _symmetry_space_group_name_H-M Fm-3m loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' 'x, -z, y' 'x, z, -y' 'z, y, -x' '-z, y, x' '-y, x, z' 'y, -x, z' 'z, x, y' 'y, z, x' '-y, -z, x' 'z, -x, -y' '-y, z, -x' '-z, -x, y' '-z, x, -y' 'y, -z, -x' 'x, -y, -z' '-x, y, -z' '-x, -y, z' 'y, x, -z' '-y, -x, -z' 'z, -y, x' '-z, -y, -x' '-x, z, y' '-x, -z, -y' 'x, y+1/2, z+1/2' 'x, -z+1/2, y+1/2' 'x, z+1/2, -y+1/2' 'z, y+1/2, -x+1/2' '-z, y+1/2, x+1/2' '-y, x+1/2, z+1/2' 'y, -x+1/2, z+1/2' 'z, x+1/2, y+1/2' 'y, z+1/2, x+1/2' '-y, -z+1/2, x+1/2' 'z, -x+1/2, -y+1/2' '-y, z+1/2, -x+1/2' '-z, -x+1/2, y+1/2' '-z, x+1/2, -y+1/2' 'y, -z+1/2, -x+1/2' 'x, -y+1/2, -z+1/2' '-x, y+1/2, -z+1/2' '-x, -y+1/2, z+1/2' 'y, x+1/2, -z+1/2' '-y, -x+1/2, -z+1/2' 'z, -y+1/2, x+1/2' '-z, -y+1/2, -x+1/2' '-x, z+1/2, y+1/2' '-x, -z+1/2, -y+1/2' 'x+1/2, y, z+1/2' 'x+1/2, -z, y+1/2' 'x+1/2, z, -y+1/2' 'z+1/2, y, -x+1/2' '-z+1/2, y, x+1/2' '-y+1/2, x, z+1/2' 'y+1/2, -x, z+1/2' 'z+1/2, x, y+1/2' 'y+1/2, z, x+1/2' '-y+1/2, -z, x+1/2' 'z+1/2, -x, -y+1/2' '-y+1/2, z, -x+1/2' '-z+1/2, -x, y+1/2' '-z+1/2, x, -y+1/2' 'y+1/2, -z, -x+1/2' 'x+1/2, -y, -z+1/2' '-x+1/2, y, -z+1/2' '-x+1/2, -y, z+1/2' 'y+1/2, x, -z+1/2' '-y+1/2, -x, -z+1/2' 'z+1/2, -y, x+1/2' '-z+1/2, -y, -x+1/2' '-x+1/2, z, y+1/2' '-x+1/2, -z, -y+1/2' 'x+1/2, y+1/2, z' 'x+1/2, -z+1/2, y' 'x+1/2, z+1/2, -y' 'z+1/2, y+1/2, -x' '-z+1/2, y+1/2, x' '-y+1/2, x+1/2, z' 'y+1/2, -x+1/2, z' 'z+1/2, x+1/2, y' 'y+1/2, z+1/2, x' '-y+1/2, -z+1/2, x' 'z+1/2, -x+1/2, -y' '-y+1/2, z+1/2, -x' '-z+1/2, -x+1/2, y' '-z+1/2, x+1/2, -y' 'y+1/2, -z+1/2, -x' 'x+1/2, -y+1/2, -z' '-x+1/2, y+1/2, -z' '-x+1/2, -y+1/2, z' 'y+1/2, x+1/2, -z' '-y+1/2, -x+1/2, -z' 'z+1/2, -y+1/2, x' '-z+1/2, -y+1/2, -x' '-x+1/2, z+1/2, y' '-x+1/2, -z+1/2, -y' '-x, -y, -z' '-x, z, -y' '-x, -z, y' '-z, -y, x' 'z, -y, -x' 'y, -x, -z' '-y, x, -z' '-z, -x, -y' '-y, -z, -x' 'y, z, -x' '-z, x, y' 'y, -z, x' 'z, x, -y' 'z, -x, y' '-y, z, x' '-x, y, z' 'x, -y, z' 'x, y, -z' '-y, -x, z' 'y, x, z' '-z, y, -x' 'z, y, x' 'x, -z, -y' 'x, z, y' '-x, -y+1/2, -z+1/2' '-x, z+1/2, -y+1/2' '-x, -z+1/2, y+1/2' '-z, -y+1/2, x+1/2' 'z, -y+1/2, -x+1/2' 'y, -x+1/2, -z+1/2' '-y, x+1/2, -z+1/2' '-z, -x+1/2, -y+1/2' '-y, -z+1/2, -x+1/2' 'y, z+1/2, -x+1/2' '-z, x+1/2, y+1/2' 'y, -z+1/2, x+1/2' 'z, x+1/2, -y+1/2' 'z, -x+1/2, y+1/2' '-y, z+1/2, x+1/2' '-x, y+1/2, z+1/2' 'x, -y+1/2, z+1/2' 'x, y+1/2, -z+1/2' '-y, -x+1/2, z+1/2' 'y, x+1/2, z+1/2' '-z, y+1/2, -x+1/2' 'z, y+1/2, x+1/2' 'x, -z+1/2, -y+1/2' 'x, z+1/2, y+1/2' '-x+1/2, -y, -z+1/2' '-x+1/2, z, -y+1/2' '-x+1/2, -z, y+1/2' '-z+1/2, -y, x+1/2' 'z+1/2, -y, -x+1/2' 'y+1/2, -x, -z+1/2' '-y+1/2, x, -z+1/2' '-z+1/2, -x, -y+1/2' '-y+1/2, -z, -x+1/2' 'y+1/2, z, -x+1/2' '-z+1/2, x, y+1/2' 'y+1/2, -z, x+1/2' 'z+1/2, x, -y+1/2' 'z+1/2, -x, y+1/2' '-y+1/2, z, x+1/2' '-x+1/2, y, z+1/2' 'x+1/2, -y, z+1/2' 'x+1/2, y, -z+1/2' '-y+1/2, -x, z+1/2' 'y+1/2, x, z+1/2' '-z+1/2, y, -x+1/2' 'z+1/2, y, x+1/2' 'x+1/2, -z, -y+1/2' 'x+1/2, z, y+1/2' '-x+1/2, -y+1/2, -z' '-x+1/2, z+1/2, -y' '-x+1/2, -z+1/2, y' '-z+1/2, -y+1/2, x' 'z+1/2, -y+1/2, -x' 'y+1/2, -x+1/2, -z' '-y+1/2, x+1/2, -z' '-z+1/2, -x+1/2, -y' '-y+1/2, -z+1/2, -x' 'y+1/2, z+1/2, -x' '-z+1/2, x+1/2, y' 'y+1/2, -z+1/2, x' 'z+1/2, x+1/2, -y' 'z+1/2, -x+1/2, y' '-y+1/2, z+1/2, x' '-x+1/2, y+1/2, z' 'x+1/2, -y+1/2, z' 'x+1/2, y+1/2, -z' '-y+1/2, -x+1/2, z' 'y+1/2, x+1/2, z' '-z+1/2, y+1/2, -x' 'z+1/2, y+1/2, x' 'x+1/2, -z+1/2, -y' 'x+1/2, z+1/2, y' _cell_length_a 25.5827(7) _cell_length_b 25.5827(7) _cell_length_c 25.5827(7) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 16743.2(8) _cell_formula_units_Z 8 _cell_measurement_temperature 200(2) _cell_measurement_reflns_used 787 _cell_measurement_theta_min 2.99 _cell_measurement_theta_max 38.78 _exptl_crystal_description block _exptl_crystal_colour colourless _exptl_crystal_size_min 0.15 _exptl_crystal_size_mid 0.15 _exptl_crystal_size_max 0.20 _exptl_crystal_density_meas 'not measured' _exptl_crystal_density_diffrn 0.608 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 3016 _exptl_absorpt_coefficient_mu 1.494 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.8356 _exptl_absorpt_correction_T_max 0.9146 _exptl_absorpt_process_details SADABS _exptl_special_details ; ? ; _diffrn_ambient_temperature 200(2) _diffrn_radiation_wavelength 1.54178 _diffrn_radiation_type CuK\a _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_standards_decay_% ? _diffrn_reflns_number 374 _diffrn_reflns_av_R_equivalents 0.0000 _diffrn_reflns_av_sigmaI/netI 0.0220 _diffrn_reflns_limit_h_min 0 _diffrn_reflns_limit_h_max 13 _diffrn_reflns_limit_k_min 0 _diffrn_reflns_limit_k_max 16 _diffrn_reflns_limit_l_min 1 _diffrn_reflns_limit_l_max 22 _diffrn_reflns_theta_min 2.99 _diffrn_reflns_theta_max 46.06 _reflns_number_total 374 _reflns_number_gt 231 _reflns_threshold_expression >2sigma(I) _computing_data_collection 'Bruker APEX2' _computing_cell_refinement 'Bruker SAINT' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics 'Bruker SHELXTL' _computing_publication_material 'Bruker SHELXTL' _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 resolution of the crystal was at ~1.0 Angstrom, but we collected and integrated the data upto to 0.83 to ensure if we can locate any substituents on the organic ligand. (CHECKCIF reported Alert A on low completeness and value of sine (theta_max)/wavelength <0.550. Electron density for nitrogen atoms that belong to the cross-linker was found. However, it is severely disordered, and we tried to resolve the disorders but it then unabled us to apply SQUEEZE protocol to the structure (the refinement is unstable/ not convergent). SQUEEZE protocol found 2159 electrons in the structure that can be accounted for the disorders DMF molecules and the cross-linker group. ; _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^)+(0.2000P)^2^+0.0000P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens constr _refine_ls_hydrogen_treatment constr _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_number_reflns 374 _refine_ls_number_parameters 25 _refine_ls_number_restraints 2 _refine_ls_R_factor_all 0.1188 _refine_ls_R_factor_gt 0.1085 _refine_ls_wR_factor_ref 0.3420 _refine_ls_wR_factor_gt 0.3319 _refine_ls_goodness_of_fit_ref 1.329 _refine_ls_restrained_S_all 1.329 _refine_ls_shift/su_max 0.000 _refine_ls_shift/su_mean 0.000 loop_ _platon_squeeze_void_nr _platon_squeeze_void_average_x _platon_squeeze_void_average_y _platon_squeeze_void_average_z _platon_squeeze_void_volume _platon_squeeze_void_count_electrons _platon_squeeze_void_content 1 -0.014 -0.007 -0.006 12763 2159 ' ' _platon_squeeze_details ; ; 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 O2 O 0.2500 0.2500 0.2500 0.174(9) Uani 1 24 d S . . O1 O 0.2191(4) 0.1357(7) 0.2191(4) 0.242(6) Uani 1 2 d S . . C1 C 0.2500 0.1142(16) 0.2500 0.225(12) Uani 1 4 d SD . . C2 C 0.2500 0.0566(16) 0.2500 0.220(10) Uani 1 4 d SD . . C3 C 0.2799(6) 0.0259(9) 0.2799(6) 0.268(11) Uani 1 2 d SD . . H3 H 0.3028 0.0424 0.3028 0.321 Uiso 0.75 2 calc SPR . . Zn1 Zn 0.20630(9) 0.20630(9) 0.20630(9) 0.197(3) Uani 1 6 d S . . 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 O2 0.174(9) 0.174(9) 0.174(9) 0.000 0.000 0.000 O1 0.262(10) 0.201(12) 0.262(10) -0.013(7) 0.003(9) -0.013(7) C1 0.26(2) 0.16(3) 0.26(2) 0.000 -0.02(3) 0.000 C2 0.22(2) 0.22(5) 0.22(2) 0.000 0.00(2) 0.000 C3 0.304(16) 0.20(2) 0.304(16) -0.041(11) -0.049(16) -0.041(11) Zn1 0.197(3) 0.197(3) 0.197(3) 0.0034(13) 0.0034(13) 0.0034(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 O2 Zn1 1.936(4) . ? O2 Zn1 1.936(4) 125 ? O2 Zn1 1.936(4) 171 ? O2 Zn1 1.936(4) 146 ? O1 C1 1.246(14) . ? O1 Zn1 1.865(17) . ? C1 O1 1.246(14) 65 ? C1 C2 1.473(19) . ? C2 C3 1.336(16) . ? C2 C3 1.336(16) 65 ? C3 C3 1.33(4) 113 ? Zn1 O1 1.865(17) 9 ? Zn1 O1 1.865(17) 8 ? 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 Zn1 O2 Zn1 109.5 . 125 ? Zn1 O2 Zn1 109.5 . 171 ? Zn1 O2 Zn1 109.472(1) 125 171 ? Zn1 O2 Zn1 109.5 . 146 ? Zn1 O2 Zn1 109.5 125 146 ? Zn1 O2 Zn1 109.471(1) 171 146 ? C1 O1 Zn1 131(2) . . ? O1 C1 O1 128(4) 65 . ? O1 C1 C2 116.2(18) 65 . ? O1 C1 C2 116.2(18) . . ? C3 C2 C3 108(3) . 65 ? C3 C2 C1 126.0(16) . . ? C3 C2 C1 126.0(16) 65 . ? C3 C3 C2 126.0(16) 113 . ? O1 Zn1 O1 108.0(5) . 9 ? O1 Zn1 O1 108.0(5) . 8 ? O1 Zn1 O1 108.0(5) 9 8 ? O1 Zn1 O2 110.9(5) . . ? O1 Zn1 O2 110.9(5) 9 . ? O1 Zn1 O2 110.9(5) 8 . ? _diffrn_measured_fraction_theta_max 0.901 _diffrn_reflns_theta_full 46.06 _diffrn_measured_fraction_theta_full 0.901 _refine_diff_density_max 0.316 _refine_diff_density_min -0.290 _refine_diff_density_rms 0.071 data_IRMOF-3-AM5XL _database_code_depnum_ccdc_archive 'CCDC 906537' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C24 H6 N0 O13 Zn4' _chemical_formula_sum 'C24 H6 N0 O13 Zn4' _chemical_formula_weight 763.77 loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source C C 0.0181 0.0091 '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 0.0311 0.0180 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' O O 0.0492 0.0322 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Zn Zn -1.5491 0.6778 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Cubic _symmetry_space_group_name_H-M 'F-43m ' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' 'x, -y, -z' '-x, -y, z' '-x, y, -z' 'y, -x, -z' '-y, -x, z' '-y, x, -z' 'y, x, z' 'y, z, x' '-y, -z, x' 'y, -z, -x' '-y, z, -x' 'z, -y, -x' 'z, y, x' '-z, y, -x' '-z, -y, x' 'z, x, y' '-z, x, -y' '-z, -x, y' 'z, -x, -y' 'x, z, y' 'x, -z, -y' '-x, z, -y' '-x, -z, y' 'x, y+1/2, z+1/2' 'x, -y+1/2, -z+1/2' '-x, -y+1/2, z+1/2' '-x, y+1/2, -z+1/2' 'y, -x+1/2, -z+1/2' '-y, -x+1/2, z+1/2' '-y, x+1/2, -z+1/2' 'y, x+1/2, z+1/2' 'y, z+1/2, x+1/2' '-y, -z+1/2, x+1/2' 'y, -z+1/2, -x+1/2' '-y, z+1/2, -x+1/2' 'z, -y+1/2, -x+1/2' 'z, y+1/2, x+1/2' '-z, y+1/2, -x+1/2' '-z, -y+1/2, x+1/2' 'z, x+1/2, y+1/2' '-z, x+1/2, -y+1/2' '-z, -x+1/2, y+1/2' 'z, -x+1/2, -y+1/2' 'x, z+1/2, y+1/2' 'x, -z+1/2, -y+1/2' '-x, z+1/2, -y+1/2' '-x, -z+1/2, y+1/2' 'x+1/2, y, z+1/2' 'x+1/2, -y, -z+1/2' '-x+1/2, -y, z+1/2' '-x+1/2, y, -z+1/2' 'y+1/2, -x, -z+1/2' '-y+1/2, -x, z+1/2' '-y+1/2, x, -z+1/2' 'y+1/2, x, z+1/2' 'y+1/2, z, x+1/2' '-y+1/2, -z, x+1/2' 'y+1/2, -z, -x+1/2' '-y+1/2, z, -x+1/2' 'z+1/2, -y, -x+1/2' 'z+1/2, y, x+1/2' '-z+1/2, y, -x+1/2' '-z+1/2, -y, x+1/2' 'z+1/2, x, y+1/2' '-z+1/2, x, -y+1/2' '-z+1/2, -x, y+1/2' 'z+1/2, -x, -y+1/2' 'x+1/2, z, y+1/2' 'x+1/2, -z, -y+1/2' '-x+1/2, z, -y+1/2' '-x+1/2, -z, y+1/2' 'x+1/2, y+1/2, z' 'x+1/2, -y+1/2, -z' '-x+1/2, -y+1/2, z' '-x+1/2, y+1/2, -z' 'y+1/2, -x+1/2, -z' '-y+1/2, -x+1/2, z' '-y+1/2, x+1/2, -z' 'y+1/2, x+1/2, z' 'y+1/2, z+1/2, x' '-y+1/2, -z+1/2, x' 'y+1/2, -z+1/2, -x' '-y+1/2, z+1/2, -x' 'z+1/2, -y+1/2, -x' 'z+1/2, y+1/2, x' '-z+1/2, y+1/2, -x' '-z+1/2, -y+1/2, x' 'z+1/2, x+1/2, y' '-z+1/2, x+1/2, -y' '-z+1/2, -x+1/2, y' 'z+1/2, -x+1/2, -y' 'x+1/2, z+1/2, y' 'x+1/2, -z+1/2, -y' '-x+1/2, z+1/2, -y' '-x+1/2, -z+1/2, y' _cell_length_a 25.6341(6) _cell_length_b 25.6341(6) _cell_length_c 25.6341(6) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 16844.3(7) _cell_formula_units_Z 8 _cell_measurement_temperature 250(2) _cell_measurement_reflns_used 2571 _cell_measurement_theta_min 2.99 _cell_measurement_theta_max 67.74 _exptl_crystal_description block _exptl_crystal_colour colourless _exptl_crystal_size_min 0.05 _exptl_crystal_size_mid 0.05 _exptl_crystal_size_max 0.08 _exptl_crystal_density_meas 'not measured' _exptl_crystal_density_diffrn 0.602 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 2992 _exptl_absorpt_coefficient_mu 1.485 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.8458 _exptl_absorpt_correction_T_max 0.9694 _exptl_absorpt_process_details SADABS _exptl_special_details ; ? ; _diffrn_ambient_temperature 250(2) _diffrn_radiation_wavelength 1.54178 _diffrn_radiation_type CuK\a _diffrn_radiation_source 'sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker APEX-II CCD' _diffrn_measurement_method '\f and \w scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number 0 _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 8625 _diffrn_reflns_av_R_equivalents 0.0380 _diffrn_reflns_av_sigmaI/netI 0.0285 _diffrn_reflns_limit_h_min -30 _diffrn_reflns_limit_h_max 29 _diffrn_reflns_limit_k_min -28 _diffrn_reflns_limit_k_max 30 _diffrn_reflns_limit_l_min -9 _diffrn_reflns_limit_l_max 27 _diffrn_reflns_theta_min 2.99 _diffrn_reflns_theta_max 68.33 _reflns_number_total 1489 _reflns_number_gt 1007 _reflns_threshold_expression >2\s(I) _computing_data_collection 'Bruker APEX2' _computing_cell_refinement 'Bruker SAINT' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics 'Bruker SHELXTL' _computing_publication_material 'Bruker SHELXTL' _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^ > 2\s(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 Alert A for high or low Ueq for C2, C3, and C4 are due to distortion of the benzene ring. C2, C3, and C4 have to be carbon atoms due to the structure of the ligand. We cannot locate the substituents of the ligand because of the severe disorder. SQUEEZE protocol found 2071 electrons that belong to the solvent molecules [eg. DMF, CHCl3] and the substituents. The Shelx program suggest the space group as Fm-3m but the structure could not be solved and refined using that space group so F-43m was used. ; _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^)+(0.2000P)^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_abs_structure_details 'Flack H D (1983), Acta Cryst. A39, 876-881' _refine_ls_abs_structure_Flack 0.1(3) _refine_ls_number_reflns 1489 _refine_ls_number_parameters 49 _refine_ls_number_restraints 2 _refine_ls_R_factor_all 0.1087 _refine_ls_R_factor_gt 0.0995 _refine_ls_wR_factor_ref 0.3213 _refine_ls_wR_factor_gt 0.2994 _refine_ls_goodness_of_fit_ref 1.225 _refine_ls_restrained_S_all 1.226 _refine_ls_shift/su_max 0.000 _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 O1 O 0.0000 0.5000 0.0000 0.086(4) Uani 1 24 d S . . O2 O 0.0000 0.5000 0.5000 0.083(4) Uani 1 24 d S . . O3 O 0.0304(4) 0.4696(4) 0.3855(3) 0.178(5) Uani 1 2 d S . . O4 O 0.0302(3) 0.4698(3) 0.1167(4) 0.145(3) Uani 1 2 d SD . . C2 C 0.0000 0.5000 0.3635(6) 0.215(15) Uani 1 4 d S . . C3 C 0.0000 0.5000 0.2995(6) 0.132(6) Uani 1 4 d S . . C4 C 0.0317(13) 0.4683(13) 0.2750(6) 0.39(3) Uani 1 2 d SD . . C1 C 0.0000 0.5000 0.1416(6) 0.112(4) Uani 1 4 d SD . . C5 C 0.0000 0.5000 0.1921(9) 0.142(6) Uani 1 4 d S . . C6 C 0.0306(4) 0.4694(4) 0.2244(5) 0.169(6) Uani 1 2 d SD . . H6 H 0.0534 0.4466 0.2077 0.203 Uiso 1 2 calc SR . . Zn1 Zn 0.04333(5) 0.45667(5) 0.45667(5) 0.1041(8) Uani 1 6 d S . . Zn2 Zn 0.04332(5) 0.45668(5) 0.04332(5) 0.1049(8) Uani 1 6 d S . . 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 O1 0.086(4) 0.086(4) 0.086(4) 0.000 0.000 0.000 O2 0.083(4) 0.083(4) 0.083(4) 0.000 0.000 0.000 O3 0.239(8) 0.239(8) 0.056(3) 0.018(4) -0.018(4) -0.005(10) O4 0.157(4) 0.157(4) 0.120(5) 0.005(3) -0.005(3) 0.040(7) C2 0.30(2) 0.30(2) 0.040(6) 0.000 0.000 -0.12(3) C3 0.159(10) 0.159(10) 0.077(8) 0.000 0.000 0.033(13) C4 0.54(4) 0.54(4) 0.092(10) -0.030(13) 0.030(13) 0.09(5) C1 0.105(5) 0.105(5) 0.127(11) 0.000 0.000 0.005(7) C5 0.157(10) 0.157(10) 0.112(11) 0.000 0.000 -0.019(13) C6 0.189(9) 0.189(9) 0.128(8) 0.001(5) -0.001(5) 0.082(11) Zn1 0.1041(8) 0.1041(8) 0.1041(8) -0.0011(8) 0.0011(8) 0.0011(8) Zn2 0.1049(8) 0.1049(8) 0.1049(8) 0.0041(9) -0.0041(9) 0.0041(9) _geom_special_details ; All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'s involving l.s. planes. ; loop_ _platon_squeeze_void_nr _platon_squeeze_void_average_x _platon_squeeze_void_average_y _platon_squeeze_void_average_z _platon_squeeze_void_volume _platon_squeeze_void_count_electrons _platon_squeeze_void_content 1 -0.006 0.100 0.115 11693 2071 ' ' _platon_squeeze_details ; ; 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 O1 Zn2 1.924(2) . ? O1 Zn2 1.924(2) 3_565 ? O1 Zn2 1.924(2) 2_565 ? O1 Zn2 1.924(2) 4 ? O2 Zn1 1.924(2) 2_566 ? O2 Zn1 1.924(2) . ? O2 Zn1 1.924(2) 4_556 ? O2 Zn1 1.924(2) 3_565 ? O3 C2 1.238(14) . ? O3 Zn1 1.884(8) . ? O4 C1 1.266(12) . ? O4 Zn2 1.941(9) . ? C2 O3 1.238(14) 3_565 ? C2 C3 1.64(2) . ? C3 C4 1.31(4) 3_565 ? C3 C4 1.31(4) . ? C4 C6 1.296(15) . ? C1 O4 1.266(12) 3_565 ? C1 C5 1.29(3) . ? C5 C6 1.39(2) 3_565 ? C5 C6 1.39(2) . ? Zn1 O3 1.884(8) 63 ? Zn1 O3 1.884(8) 60 ? Zn1 Zn1 3.142(4) 2_566 ? Zn1 Zn1 3.142(4) 4_556 ? Zn1 Zn1 3.142(4) 3_565 ? Zn2 O4 1.941(9) 14 ? Zn2 O4 1.941(9) 82 ? Zn2 Zn2 3.141(4) 3_565 ? Zn2 Zn2 3.141(4) 2_565 ? Zn2 Zn2 3.141(4) 4 ? 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 Zn2 O1 Zn2 109.5 . 3_565 ? Zn2 O1 Zn2 109.5 . 2_565 ? Zn2 O1 Zn2 109.5 3_565 2_565 ? Zn2 O1 Zn2 109.5 . 4 ? Zn2 O1 Zn2 109.5 3_565 4 ? Zn2 O1 Zn2 109.5 2_565 4 ? Zn1 O2 Zn1 109.471(1) 2_566 . ? Zn1 O2 Zn1 109.5 2_566 4_556 ? Zn1 O2 Zn1 109.5 . 4_556 ? Zn1 O2 Zn1 109.5 2_566 3_565 ? Zn1 O2 Zn1 109.5 . 3_565 ? Zn1 O2 Zn1 109.5 4_556 3_565 ? C2 O3 Zn1 131.4(9) . . ? C1 O4 Zn2 134.5(8) . . ? O3 C2 O3 126.0(12) 3_565 . ? O3 C2 C3 117.0(6) 3_565 . ? O3 C2 C3 117.0(6) . . ? C4 C3 C4 123(3) 3_565 . ? C4 C3 C2 118.7(13) 3_565 . ? C4 C3 C2 118.7(13) . . ? C6 C4 C3 117(4) . . ? O4 C1 O4 119.5(13) . 3_565 ? O4 C1 C5 120.3(7) . . ? O4 C1 C5 120.3(7) 3_565 . ? C1 C5 C6 126.8(9) . 3_565 ? C1 C5 C6 126.8(9) . . ? C6 C5 C6 106.5(19) 3_565 . ? C4 C6 C5 128(3) . . ? O3 Zn1 O3 108.0(5) 63 . ? O3 Zn1 O3 108.0(5) 63 60 ? O3 Zn1 O3 108.0(5) . 60 ? O3 Zn1 O2 110.9(4) 63 . ? O3 Zn1 O2 110.9(4) . . ? O3 Zn1 O2 110.9(4) 60 . ? O3 Zn1 Zn1 75.6(4) 63 2_566 ? O3 Zn1 Zn1 124.1(4) . 2_566 ? O3 Zn1 Zn1 124.1(4) 60 2_566 ? O2 Zn1 Zn1 35.3 . 2_566 ? O3 Zn1 Zn1 124.1(4) 63 4_556 ? O3 Zn1 Zn1 124.1(4) . 4_556 ? O3 Zn1 Zn1 75.6(4) 60 4_556 ? O2 Zn1 Zn1 35.3 . 4_556 ? Zn1 Zn1 Zn1 60.0 2_566 4_556 ? O3 Zn1 Zn1 124.1(4) 63 3_565 ? O3 Zn1 Zn1 75.6(4) . 3_565 ? O3 Zn1 Zn1 124.1(4) 60 3_565 ? O2 Zn1 Zn1 35.3 . 3_565 ? Zn1 Zn1 Zn1 60.0 2_566 3_565 ? Zn1 Zn1 Zn1 60.0 4_556 3_565 ? O1 Zn2 O4 111.0(3) . 14 ? O1 Zn2 O4 111.0(3) . . ? O4 Zn2 O4 107.9(3) 14 . ? O1 Zn2 O4 111.0(3) . 82 ? O4 Zn2 O4 107.9(3) 14 82 ? O4 Zn2 O4 107.9(3) . 82 ? O1 Zn2 Zn2 35.3 . 3_565 ? O4 Zn2 Zn2 124.2(2) 14 3_565 ? O4 Zn2 Zn2 75.8(3) . 3_565 ? O4 Zn2 Zn2 124.2(2) 82 3_565 ? O1 Zn2 Zn2 35.3 . 2_565 ? O4 Zn2 Zn2 75.8(3) 14 2_565 ? O4 Zn2 Zn2 124.2(2) . 2_565 ? O4 Zn2 Zn2 124.2(2) 82 2_565 ? Zn2 Zn2 Zn2 60.0 3_565 2_565 ? O1 Zn2 Zn2 35.3 . 4 ? O4 Zn2 Zn2 124.2(2) 14 4 ? O4 Zn2 Zn2 124.2(2) . 4 ? O4 Zn2 Zn2 75.8(3) 82 4 ? Zn2 Zn2 Zn2 60.0 3_565 4 ? Zn2 Zn2 Zn2 60.0 2_565 4 ? _diffrn_measured_fraction_theta_max 0.998 _diffrn_reflns_theta_full 68.33 _diffrn_measured_fraction_theta_full 0.998 _refine_diff_density_max 1.115 _refine_diff_density_min -0.288 _refine_diff_density_rms 0.087 data_IRMOF-3-AM6XL _database_code_depnum_ccdc_archive 'CCDC 906538' _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_name_common ? _chemical_melting_point ? _chemical_formula_moiety 'C24 H6 N0 O13 Zn4' _chemical_formula_sum 'C24 H6 N0 O13 Zn4' _chemical_formula_weight 763.77 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' O O 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' Zn Zn 0.2839 1.4301 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting Cubic _symmetry_space_group_name_H-M 'F-43m ' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x, -y, z' '-x, y, -z' 'x, -y, -z' 'z, x, y' 'z, -x, -y' '-z, -x, y' '-z, x, -y' 'y, z, x' '-y, z, -x' 'y, -z, -x' '-y, -z, x' 'y, x, z' '-y, -x, z' 'y, -x, -z' '-y, x, -z' 'x, z, y' '-x, z, -y' '-x, -z, y' 'x, -z, -y' 'z, y, x' 'z, -y, -x' '-z, y, -x' '-z, -y, x' 'x, y+1/2, z+1/2' '-x, -y+1/2, z+1/2' '-x, y+1/2, -z+1/2' 'x, -y+1/2, -z+1/2' 'z, x+1/2, y+1/2' 'z, -x+1/2, -y+1/2' '-z, -x+1/2, y+1/2' '-z, x+1/2, -y+1/2' 'y, z+1/2, x+1/2' '-y, z+1/2, -x+1/2' 'y, -z+1/2, -x+1/2' '-y, -z+1/2, x+1/2' 'y, x+1/2, z+1/2' '-y, -x+1/2, z+1/2' 'y, -x+1/2, -z+1/2' '-y, x+1/2, -z+1/2' 'x, z+1/2, y+1/2' '-x, z+1/2, -y+1/2' '-x, -z+1/2, y+1/2' 'x, -z+1/2, -y+1/2' 'z, y+1/2, x+1/2' 'z, -y+1/2, -x+1/2' '-z, y+1/2, -x+1/2' '-z, -y+1/2, x+1/2' 'x+1/2, y, z+1/2' '-x+1/2, -y, z+1/2' '-x+1/2, y, -z+1/2' 'x+1/2, -y, -z+1/2' 'z+1/2, x, y+1/2' 'z+1/2, -x, -y+1/2' '-z+1/2, -x, y+1/2' '-z+1/2, x, -y+1/2' 'y+1/2, z, x+1/2' '-y+1/2, z, -x+1/2' 'y+1/2, -z, -x+1/2' '-y+1/2, -z, x+1/2' 'y+1/2, x, z+1/2' '-y+1/2, -x, z+1/2' 'y+1/2, -x, -z+1/2' '-y+1/2, x, -z+1/2' 'x+1/2, z, y+1/2' '-x+1/2, z, -y+1/2' '-x+1/2, -z, y+1/2' 'x+1/2, -z, -y+1/2' 'z+1/2, y, x+1/2' 'z+1/2, -y, -x+1/2' '-z+1/2, y, -x+1/2' '-z+1/2, -y, x+1/2' 'x+1/2, y+1/2, z' '-x+1/2, -y+1/2, z' '-x+1/2, y+1/2, -z' 'x+1/2, -y+1/2, -z' 'z+1/2, x+1/2, y' 'z+1/2, -x+1/2, -y' '-z+1/2, -x+1/2, y' '-z+1/2, x+1/2, -y' 'y+1/2, z+1/2, x' '-y+1/2, z+1/2, -x' 'y+1/2, -z+1/2, -x' '-y+1/2, -z+1/2, x' 'y+1/2, x+1/2, z' '-y+1/2, -x+1/2, z' 'y+1/2, -x+1/2, -z' '-y+1/2, x+1/2, -z' 'x+1/2, z+1/2, y' '-x+1/2, z+1/2, -y' '-x+1/2, -z+1/2, y' 'x+1/2, -z+1/2, -y' 'z+1/2, y+1/2, x' 'z+1/2, -y+1/2, -x' '-z+1/2, y+1/2, -x' '-z+1/2, -y+1/2, x' _cell_length_a 25.741(3) _cell_length_b 25.741(3) _cell_length_c 25.741(3) _cell_angle_alpha 90.00 _cell_angle_beta 90.00 _cell_angle_gamma 90.00 _cell_volume 17055(3) _cell_formula_units_Z 8 _cell_measurement_temperature 250(2) _cell_measurement_reflns_used 1264 _cell_measurement_theta_min 2.74 _cell_measurement_theta_max 21.17 _exptl_crystal_description cubic _exptl_crystal_colour colourless _exptl_crystal_size_max 0.10 _exptl_crystal_size_mid 0.10 _exptl_crystal_size_min 0.08 _exptl_crystal_density_meas 'not measured' _exptl_crystal_density_diffrn 0.595 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 2992 _exptl_absorpt_coefficient_mu 1.132 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.8952 _exptl_absorpt_correction_T_max 0.9149 _exptl_absorpt_process_details SADABS _exptl_special_details ; ? ; _diffrn_ambient_temperature 250(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker APEX-II CCD' _diffrn_measurement_method '\f and \w scans' _diffrn_detector_area_resol_mean ? _diffrn_standards_number 0 _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% ? _diffrn_reflns_number 3726 _diffrn_reflns_av_R_equivalents 0.0252 _diffrn_reflns_av_sigmaI/netI 0.0258 _diffrn_reflns_limit_h_min -26 _diffrn_reflns_limit_h_max 18 _diffrn_reflns_limit_k_min -21 _diffrn_reflns_limit_k_max 6 _diffrn_reflns_limit_l_min -21 _diffrn_reflns_limit_l_max 26 _diffrn_reflns_theta_min 1.58 _diffrn_reflns_theta_max 21.68 _reflns_number_total 1018 _reflns_number_gt 739 _reflns_threshold_expression >2\s(I) _computing_data_collection 'Bruker APEX2' _computing_cell_refinement 'Bruker SAINT' _computing_data_reduction 'Bruker SAINT' _computing_structure_solution 'SHELXS-97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 2008)' _computing_molecular_graphics 'Bruker SHELXTL' _computing_publication_material 'Bruker SHELXTL' _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^ > 2\s(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 alert A about the low value of sine(theta_max)/wavelength is caused by weak diffraction of the crystal. We cannot locate the substituents of the ligand because of the severe disorder. SQUEEZE protocol found 6271 electrons that belong to the solvent molecules [eg. DMF, CHCl3] and the substituents. Shelx program suggest the space group as Fm-3m but the structure could not be solved and refined using that space group so F-43m was used. ; loop_ _platon_squeeze_void_nr _platon_squeeze_void_average_x _platon_squeeze_void_average_y _platon_squeeze_void_average_z _platon_squeeze_void_volume _platon_squeeze_void_count_electrons _platon_squeeze_void_content 1 -0.003 0.108 0.350 13091 6271 ' ' _platon_squeeze_details ; ; _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^)+(0.1481P)^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_abs_structure_details 'Flack H D (1983), Acta Cryst. A39, 876-881' _refine_ls_abs_structure_Flack 0.20(17) _refine_ls_number_reflns 1018 _refine_ls_number_parameters 49 _refine_ls_number_restraints 0 _refine_ls_R_factor_all 0.0769 _refine_ls_R_factor_gt 0.0668 _refine_ls_wR_factor_ref 0.2063 _refine_ls_wR_factor_gt 0.1999 _refine_ls_goodness_of_fit_ref 1.100 _refine_ls_restrained_S_all 1.100 _refine_ls_shift/su_max 0.006 _refine_ls_shift/su_mean 0.001 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 Zn1 Zn 0.95662(7) 0.45662(7) 0.04338(7) 0.0508(10) Uani 1 6 d S . . Zn2 Zn 0.95657(7) 0.45657(7) 0.45657(7) 0.0514(10) Uani 1 6 d S . . O1 O 0.9683(5) 0.4683(5) 0.3849(5) 0.105(5) Uani 1 2 d S . . O2 O 1.0000 0.5000 0.5000 0.028(8) Uani 1 24 d S . . O3 O 0.9708(4) 0.4708(4) 0.1169(4) 0.097(5) Uani 1 2 d S . . O4 O 1.0000 0.5000 0.0000 0.056(11) Uani 1 24 d S . . C1 C 1.0000 0.5000 0.1951(11) 0.079(9) Uani 1 4 d S . . C2 C 0.9705(8) 0.4705(8) 0.2285(7) 0.138(12) Uani 1 2 d S . . C3 C 1.0000 0.5000 0.2993(12) 0.089(10) Uani 1 4 d S . . C4 C 0.9677(6) 0.4677(6) 0.2765(5) 0.107(9) Uani 1 2 d S . . H4 H 0.9455 0.4455 0.2942 0.128 Uiso 1 2 calc SR . . C5 C 1.0000 0.5000 0.3607(16) 0.098(12) Uani 1 4 d S . . C6 C 1.0000 0.5000 0.1383(9) 0.063(8) Uani 1 4 d S . . 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 Zn1 0.0508(10) 0.0508(10) 0.0508(10) 0.0017(13) 0.0017(13) -0.0017(13) Zn2 0.0514(10) 0.0514(10) 0.0514(10) -0.0031(13) -0.0031(13) -0.0031(13) O1 0.115(7) 0.115(7) 0.084(9) 0.017(7) 0.017(7) -0.016(12) O2 0.028(8) 0.028(8) 0.028(8) 0.000 0.000 0.000 O3 0.127(8) 0.127(8) 0.035(7) 0.010(5) 0.010(5) -0.047(12) O4 0.056(11) 0.056(11) 0.056(11) 0.000 0.000 0.000 C1 0.110(14) 0.110(14) 0.017(10) 0.000 0.000 -0.024(17) C2 0.178(18) 0.178(18) 0.057(14) 0.012(9) 0.012(9) -0.04(2) C3 0.095(14) 0.095(14) 0.08(2) 0.000 0.000 -0.003(19) C4 0.145(14) 0.145(14) 0.031(11) 0.021(6) 0.021(6) -0.091(16) C5 0.092(16) 0.092(16) 0.11(3) 0.000 0.000 0.00(3) C6 0.084(13) 0.084(13) 0.021(14) 0.000 0.000 0.00(2) _geom_special_details ; All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'s 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 Zn1 O4 1.934(3) . ? Zn1 O3 1.961(12) . ? Zn1 O3 1.961(12) 83_556 ? Zn1 O3 1.961(12) 32_645 ? Zn1 Zn1 3.158(5) 2_765 ? Zn1 Zn1 3.158(5) 3_755 ? Zn1 Zn1 3.158(5) 4_565 ? Zn2 O1 1.894(13) 57_554 ? Zn2 O1 1.894(13) 77_545 ? Zn2 O1 1.894(13) . ? Zn2 O2 1.936(3) . ? O1 C5 1.31(2) . ? O2 Zn2 1.936(3) 4_566 ? O2 Zn2 1.936(3) 2_765 ? O2 Zn2 1.936(3) 3_756 ? O3 C6 1.197(15) . ? O4 Zn1 1.934(3) 2_765 ? O4 Zn1 1.934(3) 3_755 ? O4 Zn1 1.934(3) 4_565 ? C1 C2 1.37(3) 2_765 ? C1 C2 1.37(3) . ? C1 C6 1.46(4) . ? C2 C4 1.240(15) . ? C3 C4 1.31(2) . ? C3 C4 1.31(2) 2_765 ? C3 C5 1.58(5) . ? C4 H4 0.9300 . ? C5 O1 1.31(2) 2_765 ? C6 O3 1.197(15) 2_765 ? 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 O4 Zn1 O3 110.0(5) . . ? O4 Zn1 O3 110.0(5) . 83_556 ? O3 Zn1 O3 108.9(5) . 83_556 ? O4 Zn1 O3 110.0(5) . 32_645 ? O3 Zn1 O3 108.9(5) . 32_645 ? O3 Zn1 O3 108.9(5) 83_556 32_645 ? O4 Zn1 Zn1 35.3 . 2_765 ? O3 Zn1 Zn1 74.7(5) . 2_765 ? O3 Zn1 Zn1 123.4(4) 83_556 2_765 ? O3 Zn1 Zn1 123.4(4) 32_645 2_765 ? O4 Zn1 Zn1 35.3 . 3_755 ? O3 Zn1 Zn1 123.4(4) . 3_755 ? O3 Zn1 Zn1 74.7(5) 83_556 3_755 ? O3 Zn1 Zn1 123.4(4) 32_645 3_755 ? Zn1 Zn1 Zn1 60.0 2_765 3_755 ? O4 Zn1 Zn1 35.3 . 4_565 ? O3 Zn1 Zn1 123.4(4) . 4_565 ? O3 Zn1 Zn1 123.4(4) 83_556 4_565 ? O3 Zn1 Zn1 74.7(5) 32_645 4_565 ? Zn1 Zn1 Zn1 60.0 2_765 4_565 ? Zn1 Zn1 Zn1 60.0 3_755 4_565 ? O1 Zn2 O1 106.6(6) 57_554 77_545 ? O1 Zn2 O1 106.6(6) 57_554 . ? O1 Zn2 O1 106.6(6) 77_545 . ? O1 Zn2 O2 112.2(6) 57_554 . ? O1 Zn2 O2 112.2(6) 77_545 . ? O1 Zn2 O2 112.2(6) . . ? C5 O1 Zn2 131(2) . . ? Zn2 O2 Zn2 109.5 . 4_566 ? Zn2 O2 Zn2 109.5 . 2_765 ? Zn2 O2 Zn2 109.471(1) 4_566 2_765 ? Zn2 O2 Zn2 109.5 . 3_756 ? Zn2 O2 Zn2 109.471(1) 4_566 3_756 ? Zn2 O2 Zn2 109.471(1) 2_765 3_756 ? C6 O3 Zn1 132.7(14) . . ? Zn1 O4 Zn1 109.471(1) 2_765 3_755 ? Zn1 O4 Zn1 109.5 2_765 . ? Zn1 O4 Zn1 109.5 3_755 . ? Zn1 O4 Zn1 109.5 2_765 4_565 ? Zn1 O4 Zn1 109.5 3_755 4_565 ? Zn1 O4 Zn1 109.5 . 4_565 ? C2 C1 C2 103(3) 2_765 . ? C2 C1 C6 128.7(13) 2_765 . ? C2 C1 C6 128.7(13) . . ? C4 C2 C1 133(3) . . ? C4 C3 C4 127(3) . 2_765 ? C4 C3 C5 116.5(13) . . ? C4 C3 C5 116.5(13) 2_765 . ? C2 C4 C3 112(3) . . ? C2 C4 H4 124.1 . . ? C3 C4 H4 124.1 . . ? O1 C5 O1 123(3) . 2_765 ? O1 C5 C3 118.4(16) . . ? O1 C5 C3 118.4(16) 2_765 . ? O3 C6 O3 125(2) . 2_765 ? O3 C6 C1 117.4(11) . . ? O3 C6 C1 117.4(11) 2_765 . ? _diffrn_measured_fraction_theta_max 0.995 _diffrn_reflns_theta_full 21.68 _diffrn_measured_fraction_theta_full 0.995 _refine_diff_density_max 0.518 _refine_diff_density_min -0.753 _refine_diff_density_rms 0.179